TW508595B - Magnetic core insulation - Google Patents

Magnetic core insulation Download PDF

Info

Publication number
TW508595B
TW508595B TW089109728A TW89109728A TW508595B TW 508595 B TW508595 B TW 508595B TW 089109728 A TW089109728 A TW 089109728A TW 89109728 A TW89109728 A TW 89109728A TW 508595 B TW508595 B TW 508595B
Authority
TW
Taiwan
Prior art keywords
core
layers
scope
iron
patent application
Prior art date
Application number
TW089109728A
Other languages
Chinese (zh)
Inventor
Richard Lathlaen
Richard Wood
William Beckham
Original Assignee
Nat Arnold Magnetics
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nat Arnold Magnetics filed Critical Nat Arnold Magnetics
Application granted granted Critical
Publication of TW508595B publication Critical patent/TW508595B/en

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F41/00Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
    • H01F41/02Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C26/00Coating not provided for in groups C23C2/00 - C23C24/00
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C8/00Solid state diffusion of only non-metal elements into metallic material surfaces; Chemical surface treatment of metallic material by reaction of the surface with a reactive gas, leaving reaction products of surface material in the coating, e.g. conversion coatings, passivation of metals
    • C23C8/02Pretreatment of the material to be coated
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C8/00Solid state diffusion of only non-metal elements into metallic material surfaces; Chemical surface treatment of metallic material by reaction of the surface with a reactive gas, leaving reaction products of surface material in the coating, e.g. conversion coatings, passivation of metals
    • C23C8/06Solid state diffusion of only non-metal elements into metallic material surfaces; Chemical surface treatment of metallic material by reaction of the surface with a reactive gas, leaving reaction products of surface material in the coating, e.g. conversion coatings, passivation of metals using gases
    • C23C8/08Solid state diffusion of only non-metal elements into metallic material surfaces; Chemical surface treatment of metallic material by reaction of the surface with a reactive gas, leaving reaction products of surface material in the coating, e.g. conversion coatings, passivation of metals using gases only one element being applied
    • C23C8/10Oxidising
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
    • H01F1/14Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
    • H01F1/147Alloys characterised by their composition
    • H01F1/153Amorphous metallic alloys, e.g. glassy metals
    • H01F1/15333Amorphous metallic alloys, e.g. glassy metals containing nanocrystallites, e.g. obtained by annealing
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
    • H01F1/14Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
    • H01F1/147Alloys characterised by their composition
    • H01F1/153Amorphous metallic alloys, e.g. glassy metals
    • H01F1/15383Applying coatings thereon
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
    • H01F1/14Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
    • H01F1/16Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys in the form of sheets
    • H01F1/18Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys in the form of sheets with insulating coating
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y40/00Manufacture or treatment of nanostructures
    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21DMODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
    • C21D8/00Modifying the physical properties by deformation combined with, or followed by, heat treatment
    • C21D8/12Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties
    • C21D8/1277Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties involving a particular surface treatment
    • C21D8/1283Application of a separating or insulating coating

Abstract

Disclosed herein is an insulating material between adjacent metal layers of a soft magnetic core, and a process for forming this insulating material. The insulating material is composed of the native metal oxides of the metallic core material. A method of providing dielectric isolation between adjacent metal layers of a laminated magnetic assembly, comprising: providing a laminated magnetic assembly having a plurality of layers, wherein the layers are formed in part of iron; and oxidizing the layers to produce an insulative coating comprising iron oxide between the layers, the resulting oxidized magnetic assembly exhibiting power losses reduced by at least 15% in comparison to a substantially identically dimensioned assembly without the insulative coating at an operating frequency of 10 kHz to 20 kHz.

Description

508595 A7508595 A7

經濟部智慧財產局員工消費合作社印製 五、發明說明() 發明領媸: 本發明大致關係於一種於一磁心之相鄰金屬層間之 絕緣的方法,及有關於由此方法所生產之軟磁心。特別 是’本發明關於相鄰金屬磁心層間之自然金屬氧化物之形 成與使用,以作為於層間之絕緣,以限制電流流量。較隹 地,本發明之方法可以被用以調整使用本發明所形成之鐵 心之磁特性。 發明背景: 磁性材料至少有兩種形式,硬或軟。硬磁性材料為永 久磁鐵,其於激能磁場移開後,仍保持其磁特性。一硬磁 材料例是一般冰箱磁鐵。相反地’軟磁材料之磁場於激能 場移開後即消失。例如,軟磁材料包含電磁鐵。軟磁材料 係大量被使用於例如變壓器’電感器,反相器,轉換式電 源及其他應用之邵件中之電路。軟磁材料同時用以作成磁 心,其提供高能量儲存,快速能量儲存及有效能量回復。 於這些應用中,磁心可以用於各種不同操作頻率中,典刑 係由50Hz至20kHz或更高。 多數磁心係由將一很薄磁金屬帶緊繞於一基材上,以 形成多層之積層。所繞之金屬鐵心係然後受到被稱為,,回 火之加熱步驟,以藉由感熱排序於金屬中之磁轉,而使 其效能最佳化。於回火步驟後,基材可以被移開及磁心可 以被以黏結劑處理,以將相鄰金屬層接在一起,使得鐵心 不會散開。如熟習於本技藝者所知,此黏結劑可以包含具 -------» I--- u I (請先閱讀背面之注意事項再填寫本頁) %- 第2頁Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs 5. Description of the invention () Invention collar: The present invention relates generally to a method for insulating between adjacent metal layers of a magnetic core, and a soft magnetic core produced by the method . In particular, the invention relates to the formation and use of natural metal oxides between adjacent metal magnetic core layers as insulation between the layers to limit the current flow. Rather, the method of the present invention can be used to adjust the magnetic characteristics of a core formed using the present invention. BACKGROUND OF THE INVENTION: Magnetic materials come in at least two forms, hard or soft. Hard magnetic materials are permanent magnets that retain their magnetic properties even after the excitatory magnetic field is removed. An example of a hard magnetic material is a general refrigerator magnet. Conversely, the magnetic field of the 'soft magnetic material' disappears after the excitation energy field is removed. For example, soft magnetic materials include electromagnets. Soft magnetic materials are a large number of circuits used in components such as transformers' inductors, inverters, switching power supplies, and other applications. The soft magnetic material is also used as a magnetic core, which provides high energy storage, fast energy storage and effective energy recovery. In these applications, the core can be used in a variety of different operating frequencies, ranging from 50Hz to 20kHz or higher. Most magnetic cores are formed by tightly winding a thin magnetic metal strip around a substrate to form a multilayer stack. The wound metal core is then subjected to a heating step called tempering to optimize its performance by thermally sequencing magnetic turns in the metal. After the tempering step, the substrate can be removed and the magnetic core can be treated with an adhesive to join adjacent metal layers together so that the core does not fall apart. As known to those skilled in the art, this adhesive can contain ------- »I --- u I (Please read the precautions on the back before filling this page)%-Page 2

508595 A7 B7 五、發明說明() 有一或兩部份之環氧樹脂,例如由三邦公司之H y s ο 1 # 4 2 4 2 樹脂及#340 1硬化劑,或#2076浸潰環氧樹脂。以黏結劑 之處理同時允許鐵心能藉由切割處理以形成C形或E形鐵 心,如此命名係因為如熟習於本技藝者所知,切割鐵心形 成一 C或E。 作成磁心之金屬帶或層係很簿,典型形成約〇 · 〇 1至 0.3毫米厚。對於大於400Hz之高頻應用時,一繞線磁心 之個別金屬層同時必須彼此電氣絕緣,以適當地操作。沒 有了上絕緣,於高頻時,磁心具有類似於大金屬塊之電氣 特性,並將由於滿流之故而造成大量功率損失。 為了於層間提供絕緣’先前技藝均教導於繞帶形成鐵 心前,以一絕緣材料塗覆金屬帶。絕緣材料係典型覆於帶 之兩侧,並作用以絕緣開於纏繞積層中之相鄰金屬層。一 種常用塗覆方法係由史高夫所述之美國專利第2,796,364 號案中,其揭示一種於金屬帶表面形成作為絕緣層之氧化 鎂層的方法。如於該案所述,甲基鎂係溶解於一有機溶液 中,該溶液係施加至金屬帶表面。該金屬帶係然後被加熱 至一高溫,以形成一強黏結氧化鎂於金屬帶表面上。金屬 帶可以被纏繞以形成磁心。 經濟部智慧財產局員工消費合作社印製 --------------LI (請先閱讀背面之注意事項再填寫本頁) 對於甲基鍰處理有幾項不利缺點。首先,甲基鎂必須 於其被繞成鐵心别被施加至金屬帶上。於將金屬帶解開, 將帶浸入一槽中,以形成塗層,加熱及固化該塗層,及纏 繞帶以形成鐵心,使得處理緩慢及淨貴。因此,甲基鎂並 不適用以低成本高體積提供對鍰鐵心之絕緣。第二,這很 第3頁 本紙張尺度適用中國國家標準(CNS)A4規袼(21〇 X 297公髮) 508595 A7 B7 五、發明說明( 難控制所得氧化鎂絕緣層之厚度。這對某些磁心應用會有 問題’例如脈衝鐵心,*具有很難完成之高效能規定:除 非所塗覆甲基鑊層是很薄。形成薄甲基鍰塗層需要很快及 很難控制之特殊處理。對於這些應用之施加甲基鎂係特別 昂貴的,i所得心係易碎的。再者,於可以接受厚絕緣 層之應用中,當過量非導電絕緣材料使用時,佔用了昂音 之磁心空間。這降低了積層之空間因素,使得由磁材料所 佔用之鐵心之百分比隨著鐵心效率減少。最後,因為甲基 鎂必須於回火步驟前被塗覆,所以其同時藉由於塗層及2 磁材料間建立應力,而干擾於回火時磁疇之排列。 甲基鎂處理同時不能用以形成某些類型之鐵心之絕 緣層。南溫係需要以適當固化於金屬帶上之甲基鎂。典型 地,甲基鎂塗層必須被加熱至至少843°C (1 550T ),或更 高溫,以形成一氧化鎂膜,其穩固地黏著至金屬帶上。然 而,例如非晶金屬合金之一些軟磁材料並不能被加熱至高 於449t (840T )之溫度,而不會破壞其想要之磁特性。當 甲基鎂:用以作為一這些金屬合金之絕緣材料時,其被加熱 至一較低溫,及所得氧化鎂只是鬆結合至金屬帶上。結 果,這些類型之鐵心並不能被切割以形成C或E鐵心,因 為強力切割動作將使得鬆結合絕緣塗層分開。只有未切割 鐵心,例如環帶可以由以甲基鎂處理塗覆之非晶金屬合金 形成。再者,本發明人知道另一方法可以用以形成非晶金 屬合金之C或E磁心。該處理涉及於纏繞前形成薄非連續 氧化鎂塗層於帶上,因為塗層並不連續,造成於鐵心中於 第4頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) (請先閱讀背面之注意事項再填寫本頁) 訂: 經濟部智慧財產局員工消費合作社印製 508595 經濟部智慧財產局員工消費合作社印製 A7 B7 五、發明說明() 高頻時具有較高功率耗散。 因此,有需要改良方法以形成薄介電絕緣於用以作成 磁心之軟磁金屬帶上。同時,也有需要一絕緣,以允許# 晶金屬鐵心處理,以形成可以用於高頻之c及E鐵心。 目的及概述: 本發明有利地克服了先前技藝之缺點,其藉由提供一 處理以於鐵心繞成後’形成絕緣層於一磁心之相鄭金屬層 間。該處理可以用以提供對各種用以作為磁心之金屬及金 屬合金之絕緣,諸金屬包含非晶金屬合金。由本發明之處 理所形成之絕緣材料係固定地結合至形成鐵心之金屬帶 的表面,以及加入此絕緣材料之鐵心可以被切割以形成c 或E鐵心,或其他為熟習於本技藝者所知之切割鐵心。結 果’對於第一次,C及E鐵心可以由非晶金屬合金下被完 成’該合金係由絕緣膜所保護,並適用於高頻應用。 於本發明之一方面中,有一種提供介電絕緣於一積層 磁組件之相鄰金屬層間之方法。該方法包含第一步驟為氧 化一積層磁組件,其中該組件為多數部份由鐵作成之層。 氧化產生一包含氧化鐵混合之塗層。所得磁組件具有一大 於約5 0 0歐姆-公分之電阻率。氧化步驟可以包含將多數 層曝露至有氧之蒸汽,於約至少260°C (550°F )之溫度。較 佳地’諸層可以被加熱至由約2 6 0 °C至4 2 7 C (5 0 0 F至8 0 〇 T )間之一溫度。當諸層為非晶金屬合金時,較佳地’諸 層被加熱於約3 54°c至427°C(670°F至800°F)間’其中若 第5頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) (請先閱讀背面之注意事項再填寫本頁) 裝 經濟部智慧財產局員工消費合作社印製 508595 A7 -_________ 五、發明說明() 想要正方環鐵心,則較佳由約354°C至379°C (670°F至715 卞)。於該方法之較佳實施例中,氧化積層磁組件展現減 少至少15。/。之功率損失’於10-20kHz之操作頻率,相較 於曝露至蒸汽及空氣前之磁組件。 於本發明之另一方面,有一製作介電絕緣軟磁組件之 方法。該方法包含將一含鐵之非晶金屬合金帶捲成一多層 鐵心之第一步驟。然後,該鐵心被加熱於水及氧之中,以 氧化於非晶金屬合金帶之鐵,以形成包含鐵氧化物之塗 層。塗層係至少約0.0 3微米厚。 於本發明之另一方面中,提供有一包含長形非晶金屬 帶之軟磁组件。該帶係至少約40%鐵。該帶具有第一側及 第二側。第一侧具有小突出部及第二側係大致平滑。該帶 係被纏繞以形成一積層,使得於第一側上之突出部接觸平 滑之第二表面。一包含鐵氧化物之塗層大致覆蓋平滑第二 面及接觸平滑第二面之至少突出部之一部份。該塗層較佳 具有0.03微米厚或更多。於一些實施例令,塗層之75% 以上包含鐵(ΙΠ )氧化物及鐵(IV )氧化物(即 Fe2〇3~FeO,其 被稱為磁鐵礦及鐵(Π ΙΠ )氧化物)。較佳地,該被塗覆軟磁 組件具有大於500歐姆-公分之電阻率,更妤是大於1000 歐姆-公分,最好是大於1 0000歐姆-公分。 於本發明之一方面中,於一軟磁组件之相鄰金屬層之 接觸點間有一介電絕緣塗層。該塗層主要包含足夠量之鐵 (瓜)氧化物,以降低於組件中之功率損失至少1 5 %。較佳 地,介電絕緣塗層係足夠量,以減少於組件*中之功率損失 第6頁 冢紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 魏 (請先閱讀背面之注意事項再填寫本頁)508595 A7 B7 V. Description of the invention () One or two parts of epoxy resin, such as Hyss 1 # 4 2 4 2 resin and # 340 1 hardener, or # 2076 impregnated epoxy resin . The treatment with an adhesive also allows the core to be formed into a C-shaped or E-shaped core by cutting treatment, so named because the cutting core forms a C or E as known to those skilled in the art. The metal strip or layer used as the magnetic core is very thin, and is typically formed to a thickness of about 0.1 to 0.3 mm. For high frequency applications greater than 400Hz, the individual metal layers of a wound core must be electrically insulated from each other at the same time for proper operation. Without upper insulation, at high frequencies, the magnetic core has electrical characteristics similar to large metal blocks and will cause a large amount of power loss due to full current. In order to provide insulation between layers, the prior art teaches that the metal tape is coated with an insulating material before the core is wound around the tape. Insulating materials are typically applied to both sides of the tape and act to insulate adjacent metal layers in the wound laminate. A common coating method is described in U.S. Patent No. 2,796,364 described by Schiff, which discloses a method of forming a magnesium oxide layer as an insulating layer on the surface of a metal strip. As described in the case, methylmagnesium is dissolved in an organic solution, and the solution is applied to the surface of the metal strip. The metal band is then heated to a high temperature to form a strongly bonded magnesium oxide on the surface of the metal band. The metal strip can be wound to form a magnetic core. Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs -------------- LI (Please read the notes on the back before filling this page) There are several disadvantages to the treatment of methyl hydrazone. First, methylmagnesium must be applied to the metal strip before it is wound into a core. After the metal strip is unraveled, the strip is immersed in a groove to form a coating, the coating is heated and cured, and the strip is wound around to form a core, making processing slow and noble. Therefore, methylmagnesium is not suitable for providing low-frequency, high-volume insulation to the plutonium iron core. Second, it is very p. 3 This paper is in accordance with Chinese National Standards (CNS) A4 regulations (21OX 297) 508595 A7 B7 5. Description of the invention (It is difficult to control the thickness of the obtained magnesium oxide insulation layer. Some magnetic core applications have problems, such as pulsed iron cores, * which have very high performance requirements that are difficult to accomplish: unless the applied methylfluorene layer is very thin. Forming a thin methylfluorene coating requires special treatment that is fast and difficult to control. For For these applications, the application of methylmagnesium is particularly expensive, and the core obtained is fragile. Furthermore, in applications that can accept thick insulating layers, when excessive non-conductive insulating materials are used, the magnetic core space of Angstrom is occupied. This reduces the space factor of the laminate, so that the percentage of the core occupied by the magnetic material decreases with the efficiency of the core. Finally, because methylmagnesium must be coated before the tempering step, it is also due to the coating and 2 magnetic Stresses are established between materials and interfere with the alignment of magnetic domains during tempering. Methyl magnesium treatment cannot be used to form some types of iron core insulation at the same time. South temperature systems need to be properly cured on metal strips Methylmagnesium. Typically, the methylmagnesium coating must be heated to at least 843 ° C (1 550T) or higher to form a magnesium oxide film that firmly adheres to the metal strip. However, for example, non- Some soft magnetic materials of crystalline metal alloys cannot be heated to a temperature higher than 449t (840T) without destroying their desired magnetic properties. When methylmagnesium is used as an insulating material for these metal alloys, it is Heat to a lower temperature and the resulting magnesium oxide is only loosely bonded to the metal strip. As a result, these types of cores cannot be cut to form C or E cores, because the strong cutting action will separate the loosely bonded insulating coatings. The cutting core, for example, the endless belt may be formed of an amorphous metal alloy coated with a methylmagnesium treatment. Furthermore, the inventors know that another method can be used to form a C or E magnetic core of an amorphous metal alloy. The process involves A thin non-continuous magnesium oxide coating was formed on the tape before winding, because the coating was not continuous and was caused in the iron core on page 4. This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) ( (Please read the notes on the back before filling this page) Order: Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs 508595 Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs A7 B7 5. Description of the invention () High power consumption at high frequencies Therefore, there is a need for improved methods to form thin dielectric insulation on soft magnetic metal strips used as magnetic cores. At the same time, there is also a need for insulation to allow #crystalline metal cores to be processed to form high-frequency c and E iron core. Purpose and summary: The present invention advantageously overcomes the shortcomings of the prior art by providing a process to form an insulating layer between the core and the metal layers of a magnetic core after the core is wound. This process can be used to provide Insulation of various metals and metal alloys used as magnetic cores, including amorphous metal alloys. The insulating material formed by the treatment of the present invention is fixedly bonded to the surface of the metal strip forming the core, and the core added with this insulating material can be cut to form a c or E core, or other known to those skilled in the art. Cutting iron core. Result 'For the first time, the C and E cores can be completed under an amorphous metal alloy. The alloy is protected by an insulating film and is suitable for high frequency applications. In one aspect of the present invention, there is a method for providing dielectric insulation between adjacent metal layers of a laminated magnetic component. The method comprises a first step of oxidizing a laminated magnetic component, wherein the component is a layer made of a majority of iron. Oxidation produces a coating containing a mixture of iron oxides. The resulting magnetic module has a resistivity greater than about 500 ohm-cm. The oxidation step may include exposing a plurality of layers to an aerobic vapor at a temperature of at least about 260 ° C (550 ° F). More preferably, the layers can be heated to a temperature between about 260 ° C and 4 2 7 C (50 ° F to 800 ° T). When the layers are amorphous metal alloys, it is preferred that the layers be heated between about 3 54 ° C and 427 ° C (670 ° F and 800 ° F). Where page 5 of this paper applies to Chinese countries Standard (CNS) A4 specification (210 X 297 mm) (Please read the precautions on the back before filling out this page) Installed by the Intellectual Property Bureau of the Ministry of Economic Affairs and printed by the Consumer Cooperatives 508595 A7 -_________ V. Description of Invention The ring core is preferably from about 354 ° C to 379 ° C (670 ° F to 715 卞). In a preferred embodiment of the method, the oxide laminated magnetic component exhibits a reduction of at least 15. /. The power loss' is at an operating frequency of 10-20kHz, compared to magnetic components before exposure to steam and air. In another aspect of the present invention, there is a method of manufacturing a dielectrically insulated soft magnetic component. The method includes a first step of winding an iron-containing amorphous metal alloy ribbon into a multilayer core. Then, the iron core is heated in water and oxygen to oxidize iron in the amorphous metal alloy strip to form a coating including iron oxide. The coating is at least about 0.0 3 microns thick. In another aspect of the present invention, a soft magnetic assembly including an elongated amorphous metal strip is provided. The band is at least about 40% iron. The belt has a first side and a second side. The first side has a small protrusion and the second side is substantially smooth. The tape is wound to form a laminate so that the protrusions on the first side contact the smooth second surface. An iron oxide-containing coating substantially covers the smooth second surface and at least a portion of the protrusion that contacts the smooth second surface. The coating preferably has a thickness of 0.03 microns or more. In some embodiments, more than 75% of the coating contains iron (II) oxide and iron (IV) oxide (ie, Fe203 ~ FeO, which is called magnetite and iron (II)) . Preferably, the coated soft magnetic component has a resistivity of more than 500 ohm-cm, more preferably more than 1000 ohm-cm, and most preferably more than 10,000 ohm-cm. In one aspect of the invention, a dielectric insulating coating is provided between the contact points of adjacent metal layers of a soft magnetic component. The coating mainly contains a sufficient amount of iron (melon) oxide to reduce the power loss in the component by at least 15%. Preferably, the dielectric insulation coating is a sufficient amount to reduce the power loss in the module * Page 6 The paper size of the mound is applicable to the Chinese National Standard (CNS) A4 specification (210 X 297 mm) Wei (Please read the back first (Notes for filling in this page)

508595 經濟部智慧財產局員工消費合作社印製 A7 B7 五、發明說明( 至少30%,較佳係至少45%。 發gj目的及概述: 於本發明之另一方面中,提供有一軟磁組件,其具有 一絶緣塗覆材料於組件之相鄰金屬層間,該塗覆基本上包 含鐵之氧化物,該組件具有至少1〇〇〇歐姆-公分之電阻 率0 於本發明之另一方面中,其中有-種於非晶金屬合金 帶之表面上形成一絕緣塗層之方法。該方法包含提供一非 晶金屬合金帶,其中鐵之百分比超出於該合金中之任何其 他兀素义百分比。然後,該帶係被加熱至合金回火之溫 度。該帶然後曝露至有氧之蒸汽中,以形占钟、_ …、/飞τ 以形成鐵(氧化物塗 層於大部份之帶上。或者,於將該帶加熱至回火溫度前, 該帶可以被繞成一鐵心。 於本發明之另一方面中,其中提供一磁鐵0形鐵心。 *亥鐵心具有多數非晶金屬合金帶形成一積層,其形狀上係 為半圓形’半橢圓形或半矩形。金屬氧化物絕緣塗層係於 積層内之相鄰帶間。該氧化物係由鐵之氧化所形成。去 曷鐵 心用於1 0 k Η z或更高之操作頻率時’絕緣塗層降低认 中之功率損失至少1 5 %。 圖式簡單說明: 第1圖為一圓環磁鐵心之立體圖。 第2圖為第1圖之磁心之剖面圖。 第7頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐). (請先閱讀背面之注意事項再填寫本頁)508595 Printed by A7 B7, Consumer Cooperative of Intellectual Property Bureau of the Ministry of Economic Affairs 5. Description of the invention (at least 30%, preferably at least 45%. Purpose and summary of the invention: In another aspect of the present invention, a soft magnetic component is provided. There is an insulating coating material between adjacent metal layers of the component, the coating substantially comprises an oxide of iron, and the component has a resistivity of at least 1000 ohm-cm. In another aspect of the invention, wherein There is a method of forming an insulating coating on the surface of an amorphous metal alloy strip. The method includes providing an amorphous metal alloy strip in which the percentage of iron exceeds any other percentage of the element in the alloy. Then, The belt is heated to the tempering temperature of the alloy. The belt is then exposed to aerobic steam to form bells, _, ... // τ to form iron (oxide coating on most of the belts). Alternatively, before heating the strip to a tempering temperature, the strip may be wound into a core. In another aspect of the present invention, a magnet 0-shaped core is provided. * The core has a majority of amorphous metal alloy strips to form a core. Laminated, its shape is semi-circular 'semi-elliptical or semi-rectangular. Metal oxide insulation coating is between adjacent bands in the laminate. The oxide is formed by the oxidation of iron. At an operating frequency of 10 k Η z or higher, the insulation coating reduces the recognized power loss by at least 15%. The diagram is briefly explained: Figure 1 is a perspective view of a toroidal magnetic core. Figure 2 is the first Cross section of the magnetic core shown in the figure. Page 7 This paper size is applicable to China National Standard (CNS) A4 (210 X 297 mm). (Please read the precautions on the back before filling this page)

A7A7

五、發明說明() 經濟部智慧財產局員工消費合作社印製 當 Λ % J圖為於形成本發明之絕緣材料前,被繞成一積層之非 曰曰金屬帶之剖面圖。 第4圖為第3圖之非晶金屬積層之剖面圖,其示出本發明 之氧化物絕緣材料。 第5圖為使用由具有鹼性pH之給水產生之蒸汽之塗層之 改良效能比較圖。 第6圖為用以執行環形脈衝測試之脈衝測試器設備圖。 第7圖為適用以提供氧化鐵之遷移基質之矽酸鋁矩陣之孔 頻譜圖。 第8圖為適用以提供氧化鐵之遷移基質之矽酸鋁基質之吸 著/脫除等溫線。 第9圖為用於未塗覆浸潰鐵心之鐵心通量對驅動位準圖。 第1 0圖為用於未塗覆浸潰鐵心之導磁率對功率消散(瓦/ )圖。 第11圖為用於已塗覆浸潰鐵心之鐵心通量對驅動位準 圖。 第1 2圖為用於已塗覆浸潰鐵心之導磁率對功率消散(瓦/ 磅)圖。 第1 3圖為未塗覆鐵心之導磁率對回火溫度圖。 第1 4圖為已塗覆鐵心之導磁率對回火溫度圖。 第15圖為巡迴條件下以690及725°c處理〇1磅鐵心之鐵 心通量對驅動位準圖。 第1 6圖為用於未塗覆未浸潰鐵心之鐵心通量對驅動位準 第8頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) (請先閱讀背面之注意事項再填寫本頁)V. Description of the Invention () Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs When the Λ% J picture is a cross-sectional view of a non-Yellow metal band wound before forming the insulating material of the present invention. Fig. 4 is a sectional view of the amorphous metal laminate of Fig. 3, which shows the oxide insulating material of the present invention. Figure 5 is a comparison of the improved performance of a coating using steam generated from feed water having an alkaline pH. Fig. 6 is a diagram of a pulse tester device for performing a ring pulse test. Figure 7 is a spectrum of pores of an aluminum silicate matrix suitable to provide a migration matrix for iron oxide. Figure 8 is an adsorption / removal isotherm of an aluminum silicate matrix suitable to provide a migration matrix for iron oxide. Figure 9 is a graph of core flux versus drive levels for an uncoated impregnated core. Figure 10 is a plot of permeability versus power (watts / watt) for an uncoated impregnated core. Fig. 11 is a flux-to-drive level diagram of a core for a coated impregnated core. Figure 12 is a plot of permeability versus power (watts / pounds) for coated impregnated cores. Figure 13 shows the permeability versus tempering temperature of an uncoated core. Figure 14 shows the permeability versus tempering temperature of the coated core. Figure 15 shows the flux vs. drive level of a 0.01-pound iron core processed at 690 and 725 ° C under roving conditions. Figure 16 shows the core flux vs. drive level for the uncoated and unimpregnated core. Page 8 This paper is sized for China National Standard (CNS) A4 (210 X 297 mm) (Please read the back (Please fill in this page again)

508595 A7 B7 五、發明說明() 第1 7圖為用糸未塗覆未浸潰鐵心之導磁率對功率消散(瓦 /磅)圖。 第1 8圖為用於已塗覆未浸潰鐵心之鐵心通量對驅動位準 圖。 第1 9圖為用於已塗覆未浸潰鐵心之導磁率對功率消散(瓦 /磅)圖。 第20圖為用於表1 2之資料之退回分析之視在導磁率對以 公分表示之指示器間隙圖。 第21及22圖為藉由本發明之塗覆於約68〇卞至8〇〇下之 溫度範圍所提供之功率損失改良之資料圖。 <請先閱讀背面之注意事項再填寫本頁) 圖號對照說明: 10 磁心 20 金屬帶 30 心軸 40 絕緣材料 120 帶 121 平滑面 122 粗糖面 130 間隙 150 小點 明 說 細 詳 明 發 - 經濟部智慧財產局員工消費合作社印製 可 其 份 成 緣 絕 物 化 氧 金 合 屬 金 然 於 關 致 大 明 發 本 鐵 磁 於 成 形,-,主 後為 繞心 纏鐵 被磁 心形 鐵環 於繞 以纏 以 可 應 但 以了 係所 述者 所藝 下技 以本 然於 β $習 。熟 上% G為 之本 明, 發如 本例 > 〇 解心 教 發 磁形 之以 寸, 尺份 及部 狀一 形之 種理 各處 ί 有 具 至 用 應 以 可 導 為 用 應 14 迅 以 可 明 9 第 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 Α7 Β7 五、發明說明( 成C磁鐵心,E磁鐵,及其他為熟習於本技藝者所知之積 層磁組件。再者,本發明可以應用至包含積層之磁組件,' 該積層可以未被纏繞者,例如用以藉由堆疊連續層而形成 一磁積層組件。 參考第1圖,其中示出加入本發明之纏繞環磁心ι〇 之示意圖。磁心10係藉由將一薄金屬帶20繞於一心軸3〇 而形成,以形成一積層。心軸30只是一硬體基材,其周 圍繞有帶’例如長形金屬條或棒。心軸30係於後續鐵心 處理中被去除’其並不是最終磁心1 〇之一部份。心軸3 〇 可以具有各種大小及形狀,例如圓形,矩形,正方形等, 其可以被選擇以形成具有不同形狀及尺寸之鐵心。金屬帶 20係繞於心軸3 0旁一足夠圈數,以形成想要集合厚度之 多層積層。為了本發明之目的,金屬帶2 0可以被繞以形 成為市場上可得之大小,尺寸及重量之鐵心。於纏繞完成 後,磁心1 0可以被回火,以如熟習於本技藝者所知最佳 化其效能。 金屬帶20係為一軟磁金屬或具有鐵為主金屬之合 金。金屬帶20較佳為薄的,厚度範圍由約0.01毫米至〇·3 毫米。金屬帶20可以由0.1至約25公分之寬度。為了減 少於高頻率之功率損失,絕緣材料40係提供於金屬帶20 之相鄰層間。如於第2圖中所示,磁心1 〇具有絕緣材料 40之塗層於金屬帶20之層間。絕緣材料40係至少形成於 金屬帶2 0之部份上,該部份係接觸相鄰金屬層者,因此’ 抵抗於相鄰金屬層間之電流量。於一些實施例中,金屬帶 第10頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) (請先閱讀背面之注意事項再填寫本頁) 訂· 經濟部智慧財產局員工消費合作社印製 508595 A7 _— _ B7__ 五、發明說明() (請先閱讀背面之注意事項再填寫本頁} 20可以是一非晶金屬合金,較佳鐵為主過渡金屬為主類金 屬’具有TM-M公式’其中TM為至少8〇0/〇鐵,c〇或犯 或其混合’其餘20%包含Μ,其中Μ為由包含B,c,Si, P或Ai或其混合之群組中選出。於其他實施例中,金屬帶 20可以是細結晶材料。 較佳地,本發明提供一特有處理,其可以用以形成絕 緣材料40於金屬τ 20之相鄰金屬層間,於金屬帶2〇被 繞於碗心1 0之後。因此’先前技藝之時間消耗及昂貴之 塗覆程序可以避免。再者’本發明之特有絕緣材料4〇係 很薄並固定黏著至金屬帶20上。因此,當絕緣材料4〇形 成於由非晶金屬合金之磁心上時,鐵心可以被切割,以來 成先前無法完成之軟磁组件,例如非晶金屬合金之c及£ 鐵心。 丨線 經濟部智慧財產局員工消費合作社印製 一般而T ’絕緣材料4 0係藉由氧化金屬帶2 〇加以米 成’以形成金屬之自然金屬氧化物或合金金屬成為很薄塗 層於金屬帶20之表面上。多數用以形成鐵心之金屬之自 然金屬氧化物具有相當高電阻率,並特別適用以作為於相 鄰金屬層間之絕緣。因為多數金屬及於合金中可以形成金 屬帶20之金屬可以被氧化,以形成一金屬氧化物,其具 有一足夠電阻抗以形成一適當絕緣材料4 0 ’本發明係可$ 泛用於今日所用之軟磁心材料中。表1說明可以用於本發 明之金屬及金屬合金之代表例,及可以由氧化金屬 < 人金 所創造之絕緣材料之相關化學成份。 第11頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 A7B7 五、發明說明() 表1 _軟磁材料之部份明細 元素金屬 合金成份 商品名 自然金屬氧化 物絕緣材料 F e,N i 40%Fe,38%Ni, 18%B,4%Mo METGLAS Alloy2828MB FeO,Fe2〇3, Fes 〇4 Fe,B 81%Fe, 13.5%B,3%Si, 2%C METGLAS Alloy2605SC FeO,Fe203, Fe3 〇4 F e,C ο, Ni T(70-80%) ’ M(30-20%) 非晶及細結晶 FeO,Fe2〇3, F e 3 0 4 Fe,B 70%Fe,9%B, 3%Nb,2%Cu, Mo,Co,Si 細結晶 FeO , Fe2〇3 , Fes 〇4 Fe,Co 67%Fe, 18%Co,14%B, l%Si METGLAS Alloy 2605CO FeO,Fe2〇3, F e 3 0 4 Fe,Co 49%Fe, 49%Co,2%V SUPERMENDUR FeO,Fe2〇3, F e 3 0 4 (請先閱讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製 T=Fe , Co , Ni M = B,C,Si,P,A1 其中鐵為合金中之主金屬,例如於METGLAS合金 2005SA1中,絕緣材料係主要由氧化鐵(Fe2〇3)所形成,其 他為多數氧化鐵(II-III)。例如,對於以690T之蒸汽及空 第12頁 * 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 經濟部智慧財產局員工消費合作社印製 508595 Α7 _Β7 五、發明說明() 氣處理一鐵心6小時’雷門光譜顯示絕緣層係由约80-90%Fe2O3 及磁心 1〇-1::>%Fe3〇4(即鐵(II-III)氧化物),具小 量FeO構成。該層具有〇·15微米厚之氧化鐵混合。 可以為熟習於本技勢者所了解’前述之代表合金及金 屬係為例示,本發明之教導可以應用至由所述以外之成份 之鐵為主合金。例如’本發明可以容易地應用至只改變成 份百分比之合金,或引入新金屬或元素之合金而沒有改變 予以氧化以形成絕緣氧化鐵之鐵為主合金。 絕緣材料4 0應形成夠厚並具有足夠電阻,以有效地 絕緣金屬帶20之過量層與層間之電流。若絕緣材料4〇係 太厚,則磁心1 〇將含過量非導電絕緣材料,及磁心1 〇將 具有一低空間因數’由磁材料所佔用之磁心1 〇之百分比 相當地低,減少鐵心效率。較佳地,絕緣材料40係形成 以具有於0.01及5微米,較佳係於〇·〇3·至2微米間,最 好是0·03至0.5微米。當然,應為熟習於本技藝者所了解 的,絕緣材料40之其他厚度可以提供,藉由改變如下述 之處理條件。例如’當絕緣材料40係主要由一具有相當 兩黾阻率之金屬氧化物所形成’薄膜可以用以增加空間因 數及鐵心效率。再者,對於一些應用,更多量之絕緣材料 40可以是想要於相鄰金屬層間,例如對於很高頻及脈衝功 率應用。較佳地,絕緣材料40係足夠薄,使得所得鐵心 具有至少70%之空間因數,較佳8〇%及最好是85%或更 高。 加入本發明之積層之電阻係為由絕緣材料4 〇之波形 第13頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) (請先閱讀背面之注意事項再填寫本頁)508595 A7 B7 V. Description of the invention (1) Figure 17 shows the magnetic permeability versus power dissipation (watts / pounds) of uncoated and unimpregnated iron cores. Figure 18 shows the core flux versus drive level for a coated unimpregnated core. Figure 19 is a plot of permeability versus power (watts / pounds) for a coated, unimpregnated core. Figure 20 is a graph of apparent permeability versus indicator clearance expressed in centimeters for the return analysis of the data in Table 12. Figures 21 and 22 are data graphs of power loss improvement provided by the application of the present invention at a temperature range of approximately 6800 to 800 ° C. < Please read the notes on the back before filling in this page) Drawing number comparison description: 10 Magnetic core 20 Metal belt 30 Mandrel 40 Insulating material 120 Belt 121 Smooth surface 122 Coarse sugar surface 130 Clearance 150 Dot detailing-Ministry of Economic Affairs Printed by the Intellectual Property Bureau's Consumer Cooperatives, which can be part of the pre-existing chemical oxygen alloy is Jin Ran Yu Guan Zhiming's hair ferromagnetic forming,-, the core and the core are wrapped around the core by the magnetic core iron ring Yi Keying but the technique described by those who are based on the nature of β $ learning. The% G is familiar with it, and it is issued as in this example. 〇 Xie Xin teaches that the magnetic shape is based on the inch, the size and the shape of the shape. There is a guide to use. The Chinese paper standard (CNS) A4 (210 X 297 mm) is applicable to the 9th paper size of the clarifiable paper. 508595 A7 B7 5. Description of the invention (C magnet core, E magnet, and others are known to those skilled in the art Laminated magnetic components. Furthermore, the present invention can be applied to magnetic components including laminated layers, 'the laminated layers can be unwound, for example, to form a magnetic laminated layer component by stacking continuous layers. Refer to FIG. 1, which shows The schematic diagram of the winding ring magnetic core ι0 added to the present invention is shown. The magnetic core 10 is formed by winding a thin metal strip 20 around a mandrel 30 to form a laminated layer. The mandrel 30 is only a hard substrate, and Surrounded by a band, such as an elongated metal bar or rod. The mandrel 30 is removed in subsequent core processing. It is not part of the final magnetic core 10. The mandrel 3 can have various sizes and shapes, such as circular , Rectangle, square, etc., which It can be selected to form iron cores with different shapes and sizes. The metal strip 20 is wound around the mandrel 30 for a sufficient number of turns to form a multilayer stack of desired thickness. For the purpose of the present invention, the metal strip 20 can It is wound to form a core of size, size and weight available on the market. After the winding is completed, the magnetic core 10 can be tempered to optimize its performance as known to those skilled in the art. Metal belt 20 series It is a soft magnetic metal or an alloy with iron as the main metal. The metal strip 20 is preferably thin and has a thickness ranging from about 0.01 mm to 0.3 mm. The metal strip 20 may have a width of 0.1 to about 25 cm. For high frequency power loss, the insulating material 40 is provided between adjacent layers of the metal strip 20. As shown in Figure 2, the magnetic core 10 has a coating of the insulating material 40 between the layers of the metal strip 20. The insulating material 40 is Formed on at least a portion of the metal strip 20, which is in contact with adjacent metal layers, and therefore 'resistance to the amount of current between adjacent metal layers. In some embodiments, the metal strip on page 10 of this paper applies Chinese national standard (CNS) A4 specification (210 X 297 mm) (Please read the notes on the back before filling out this page) Order · Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 508595 A7 _ — _ B7__ V. Description of the invention () ( Please read the notes on the back before filling in this page} 20 can be an amorphous metal alloy, preferably iron is the transition metal and the main metal is 'with the TM-M formula' where TM is at least 80/0 iron, The remaining 20% of 〇 or criminal or its mixture 'contains M, where M is selected from the group consisting of B, c, Si, P or Ai or a mixture thereof. In other embodiments, the metal strip 20 may be finely crystalline material. Preferably, the present invention provides a special treatment which can be used to form the insulating material 40 between adjacent metal layers of the metal τ 20, after the metal strip 20 is wound around the bowl core 10. Therefore, the time consumption of the prior art and the expensive coating process can be avoided. Furthermore, the unique insulating material 40 of the present invention is thin and fixedly adhered to the metal tape 20. Therefore, when the insulating material 40 is formed on a magnetic core made of an amorphous metal alloy, the core can be cut to form a soft magnetic component that could not be previously completed, such as the c and £ cores of the amorphous metal alloy.丨 Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs, and T 'Insulating material 40 is formed by oxidizing the metal strip 20 to form a natural metal oxide or alloy metal of the metal to become a very thin coating on the metal On the surface of the band 20. The natural metal oxides of most metals used to form iron cores have a relatively high resistivity and are particularly suitable as insulation between adjacent metal layers. Because most metals and metals in the alloy that can form the metal strip 20 can be oxidized to form a metal oxide, which has a sufficient electrical impedance to form a suitable insulating material. 40 'The present invention is generally applicable to today's use Soft magnetic core material. Table 1 shows representative examples of metals and metal alloys that can be used in the present invention, and the relevant chemical composition of insulating materials that can be created by oxidized metals < Renjin. Page 11 This paper size applies Chinese National Standard (CNS) A4 specification (210 X 297 mm) 508595 A7B7 V. Description of the invention () Table 1 _ Part of the detailed elements of soft magnetic materials Metal alloy composition Trade name Natural metal oxide insulation Material F e, Ni 40% Fe, 38% Ni, 18% B, 4% Mo METGLAS Alloy2828MB FeO, Fe203, Fes 04Fe, B 81% Fe, 13.5% B, 3% Si, 2% C METGLAS Alloy2605SC FeO, Fe203, Fe3 〇4 F e, C ο, Ni T (70-80%) 'M (30-20%) Amorphous and fine crystalline FeO, Fe203, Fe 3 0 4 Fe, B 70% Fe, 9% B, 3% Nb, 2% Cu, Mo, Co, Si Fine crystalline FeO, Fe203, Fes 04Fe, Co 67% Fe, 18% Co, 14% B, 1% Si METGLAS Alloy 2605CO FeO, Fe2〇3, F e 3 0 4 Fe, Co 49% Fe, 49% Co, 2% V SUPERMENDUR FeO, Fe2 03, F e 3 0 4 (Please read the notes on the back before filling (This page) Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs T = Fe, Co, Ni M = B, C, Si, P, A1, where iron is the main metal in the alloy, for example, in METGLAS alloy 2005SA1, the insulation material system Mainly formed from iron oxide (Fe2〇3) The others are most iron oxides (II-III). For example, for 690T steam and air page 12 * This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) Printed by the Employees' Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 508595 Α7 _Β7 V. Description of the invention ( ) Gas treatment of an iron core for 6 hours. The Raman spectrum shows that the insulation layer is composed of about 80-90% Fe2O3 and magnetic core 10-1 ::>% Fe304 (ie, iron (II-III) oxide), with a small amount FeO composition. This layer has a 0.15 micron thick iron oxide mix. It can be exemplified by those skilled in the art that the aforementioned representative alloys and metals are examples, and the teachings of the present invention can be applied to iron-based alloys composed of components other than those described above. For example, the present invention can be easily applied to an iron-based alloy in which only a percentage of the alloy is changed, or an alloy of a new metal or an element is introduced without change to oxidize to form an insulating iron oxide. The insulating material 40 should be formed to be sufficiently thick and sufficiently resistive to effectively insulate the excess layers of the metal strip 20 and the current between the layers. If the insulating material 40 is too thick, the magnetic core 10 will contain an excessive amount of non-conductive insulating material, and the magnetic core 10 will have a low space factor. The percentage of the magnetic core 1 occupied by the magnetic material is quite low, reducing the core efficiency . Preferably, the insulating material 40 is formed to have a thickness of 0.01 to 5 m, more preferably 0.03 to 2 m, and most preferably 0.03 to 0.5 m. Of course, it should be understood by those skilled in the art that other thicknesses of the insulating material 40 can be provided by changing the processing conditions as described below. For example, when the insulating material 40 is mainly formed of a metal oxide having a relatively high resistivity, a thin film can be used to increase the space factor and core efficiency. Furthermore, for some applications, a greater amount of insulating material 40 may be desired between adjacent metal layers, such as for very high frequency and pulsed power applications. Preferably, the insulating material 40 is sufficiently thin so that the resulting core has a space factor of at least 70%, preferably 80% and most preferably 85% or more. The resistance added to the laminated layer of the present invention is the waveform of insulating material 40. Page 13 This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) (Please read the precautions on the back before filling this page )

經濟部智慧財產局員工消費合作社印製 Α7 _—... _^ 一 五、發明說明() 因數乘以金屬氧化物之電阻率之函數,該絕 e,‘豕何枓配合以 由磁心1 0金屬材料所創造之邊緣電阻。對 一 τ万;夕數應用, 較佳地,磁心10具有500歐姆-公分有效電阻率及較圭為 1000歐姆-公分’最好是10000歐姆-公分。 乃 备然,應可以 為熟習於本技藝者所了解,本發明可以容易適用以創造具 有積層電阻大於或小於所述值之積層之絕緣材料4〇 ,藉 由改變如下所述之處理條件。使用本發明所形成之磁積層 可以被支撐由至少約2至1 〇伏積層之每層。 一般說來,絕緣材料40係由控制於金屬帶2〇中之鐵 之氧化加以形成。現行氧化之較佳方法係將磁心1 〇曝露 至空氣(約2 0 %氧)之高溫中。蒸汽及空氣擴散進入纏繞磁 心10中並與金屬帶20之受熱層表面接觸,造成金屬帶20 表面之加速氧化,形成一薄金屬氧化物塗層或層於金屬帶 20表面上。於帶合金之金屬與氧反應時,蒸汽及熱量加速 電子遷移率形成氧化鐵。處理條件可以變化,以進一步加 速於部份或所有反應時之電子遷移,例如引入以下所詳述 之觸媒,或溫度增加以降低蒸汽粒子大小。 再者,可以為熟習於本技藝者所知,加速電子遷移於 金屬及氧間以形成自然金屬氧化物之不同處理條件可以 替換或補充蒸汽/空氣組合。這些其他處理條件可以包含將 積層組件曝露至高濃度高反應氧化分子,例如臭氧’氧化 氮,及氮之其他高反應氧化物中。吾人想要若這些高反應 分子係以可控制方式配合所述處理加以引入,反應速率將 被加速以形成絕緣金屬氧化物。 第14頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公髮) (請先閱讀背面之注意事頊蒋填窵本貢>Printed by the Consumers ’Cooperative of Intellectual Property Bureau of the Ministry of Economic Affairs A7 _—... _ ^ 15. Explanation of the invention () Factor multiplied by the resistivity of the metal oxide as a function of the absolute e, '豕 何 豕0 Edge resistance created by metallic materials. For a τ 10,000 digit application, it is preferred that the magnetic core 10 has an effective resistivity of 500 ohm-cm and is more preferably 1000 ohm-cm ', more preferably 10,000 ohm-cm. However, it should be understood by those skilled in the art that the present invention can be easily applied to create an insulating material 40 having a laminate having a laminate resistance greater than or less than the stated value, by changing the processing conditions described below. The magnetic buildup layer formed using the present invention can be supported by each layer of at least about 2 to 10 volt buildup layers. Generally, the insulating material 40 is formed by the oxidation of iron controlled in the metal strip 20. The current preferred method of oxidation is to expose the magnetic core 10 to the high temperature of air (about 20% oxygen). Steam and air diffuse into the wound core 10 and come into contact with the surface of the heated layer of the metal strip 20, which causes accelerated oxidation of the surface of the metal strip 20 to form a thin metal oxide coating or layer on the surface of the metal strip 20. When an alloyed metal reacts with oxygen, steam and heat accelerate the electron mobility to form iron oxide. Processing conditions can be varied to further accelerate electron migration during some or all reactions, such as introducing catalysts detailed below, or increasing temperature to reduce steam particle size. Furthermore, as is known to those skilled in the art, different processing conditions that accelerate electron migration between metals and oxygen to form natural metal oxides can replace or supplement the steam / air combination. These other processing conditions may include exposing the laminate to high concentrations of highly reactive oxidizing molecules, such as ozone ' nitrogen oxides, and other highly reactive oxides of nitrogen. I would like that if these highly reactive molecules are introduced in a controlled manner in conjunction with the treatment, the reaction rate will be accelerated to form insulating metal oxides. Page 14 This paper size is in accordance with China National Standard (CNS) A4 (210 X 297) (Please read the note on the back first 顼 江 窎 窎 本 贡 >

508595 經濟部智慧財產局員工消費合作社印製 A7 B7 五、發明說明() 再者,對於一應用,吾人想要形成金屬硫化物作為絕 緣材料。為了完成這目的,硫化氫(HJ)可以替代於蒸汽中 之水’以形成自然金屬硫化物作為本發明之絕緣材料。其 他類似之氧及硫,例如硒可以用以作為電子受體,以形成 於相鄰金屬層間之絕緣化合物。 可以迅速了解的疋’彳妨助元成及加快受熱積廣組件之 所有層間之蒸汽或2氣穿透的處理條件或材料之變化,例 如鐵心1 0將造成更快處理時間及更均勻塗層或絕緣材料 4 0於帶2 0上。本案發明人已經帶2 0之表面介面形態可以 加以選擇以最佳化於層間之蒸汽及空氣擴散或穿透。參考 第3圖,其中示出一由軟磁材料作成之纏繞鐵心1 〇 〇之剖 面放大圖。鐵心1 0 〇可以是由表1中所揭示之任一金屬或 合金,及其變化所作成。鐵心1 00具有多層金屬帶1 20, 其中四個120a-d係描繪於第3圖中。相鄰金屬層120a-d 係於其間提供以一絕緣材料,因此,導電電流讦以流動於 接觸點。如於第3圖所示,帶1 20具有一相當平滑表面1 2 1 及較粗表面122。較粗面122係特徵於突出物或小點150, 其係由表面突出一段相較於層120a-d之厚度的小距離,於 金屬帶122表面之分散點處。當帶122係繞以形成一積層 時,如於第3圖所示,小點15 0與平滑面121接觸,藉以 建立於相鄰金屬層1 20a-d間之電流流動路徑。〆很小間隙 130係建立於相鄰金屬層間,其係由表面突出之小點150 距離所界定。較佳地,間隙1 3 0提供一路徑,以於本發明 之處理中,完成蒸汽或空氣穿透進入纏繞鐵心1 0〇之内 第15頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) (請先閱讀背面之注咅?事項再填寫本頁}508595 Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs A7 B7 V. Description of Invention () Furthermore, for an application, I want to form metal sulfides as an insulating material. To accomplish this, hydrogen sulfide (HJ) can be substituted for water 'in steam to form natural metal sulfides as the insulating material of the present invention. Other similar oxygen and sulfur, such as selenium, can be used as electron acceptors to form insulating compounds between adjacent metal layers. You can quickly understand the changes in processing conditions or materials that help Yuan Cheng and accelerate the penetration of steam or 2 gas between all layers of the heated component, such as iron core 10 will result in faster processing time and more uniform coating Or insulating material 40 on the belt 20. The inventors of the present case have chosen a surface interface shape of 20 that can be selected to optimize the diffusion or penetration of steam and air between layers. Referring to FIG. 3, there is shown an enlarged sectional view of a wound core 100 made of a soft magnetic material. The iron core 100 may be made of any one of the metals or alloys disclosed in Table 1, and variations thereof. The iron core 100 has multiple layers of metal strips 120, of which four 120a-d are depicted in Figure 3. Adjacent metal layers 120a-d are provided with an insulating material therebetween, so that a conductive current flows through the contact point. As shown in FIG. 3, the belt 1 20 has a relatively smooth surface 1 2 1 and a rougher surface 122. The rougher surface 122 is characterized by protrusions or small dots 150 which protrude from the surface by a small distance compared to the thickness of the layers 120a-d at the scattered points on the surface of the metal strip 122. When the belt 122 is wound to form a laminate, as shown in FIG. 3, the small point 150 is in contact with the smooth surface 121, thereby establishing a current flow path between the adjacent metal layers 120a-d. 〆The small gap 130 is established between adjacent metal layers, and it is defined by the distance of the small point 150 protruding from the surface. Preferably, the gap 130 provides a path for the penetration of steam or air into the winding core 100 in the process of the present invention. Page 15 This paper is applicable to the Chinese National Standard (CNS) A4 specification ( 210 X 297 mm) (Please read the note on the back? Matters before filling out this page}

)⑽ 595 A7 B7) ⑽ 595 A7 B7

五、發明說明( 部。 具有上述間隙及小點之金屬帶係可以由例如由 威所發售之非晶金屬合金,名為細皿仏。對於 METGLAS 帶,全屬罄 > τ Fi 主 、 金屬τ 120之不冋表面介面形態係為用以 建屬"Τ 120〈處理條件之加工品。Metglas帶係由喷 熔融金屬合金至具液體冷卻之旋轉鼓的表面加以形成。、熔 融金屬係被以每秒約1GG()帆或更快之速度加以冷卻。: 金於原子有機會分離或結晶前固化。所得固體金屬合金: 有非印玻璃狀原子結構。接觸該鼓的固體帶表面係較 粗,因為=鼓表面引入較小缺點,而造成了小點15〇。乂 參考第4圖’其中不出一第3圖積層之剖面圖,其已 經提供有本發明之絕緣材料“Ο纟。如於第4圖所示:、_ 包含絕緣材料14G之金屬氧化物材料已經形成於相鄰層 12〇a-d之間。絕緣材料14〇係形成於相當平滑表面 粗面122 1,特別是蓋住了小點15Q。絕緣㈣i4〇係位 於相鄰金屬層12〇a-d之金屬接點間,及先前 流路徑係被中斷。結果,積層對電流路徑顯現 本發明較佳處理條件以氧化金屬,形成金屬氧化物絕 緣材料係取決於鐵心金屬,及想要磁特性而定。例如,當 Fe/Si/C/B非晶金屬合金被處理時,較佳地加熱該磁心至 由約26(TC至427°C之溫度(500T至800卞),更好是354 C至365 C (670 F至690 F )’ g己合上施加長形磁場。當想 要扁平環特性時,加熱較佳於大於约399t (75〇下)至約 416°C(780°F)。當想要圓環特性時’加熱較佳係於約⑺ 第16頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公髮) I I--------------* ΙΓ (請先閱讀背面之注意事項再填寫本頁) 訂·5. Description of the invention (Department. Metal belts with the above-mentioned gaps and small dots can be made of, for example, amorphous metal alloys sold by Wei, called thin dishes. For METGLAS belts, all belong to the > τ Fi main and metal. The morphology of the surface interface of τ 120 is a processed product used to build "T 120" processing conditions. The Metglas belt is formed by spraying a molten metal alloy to the surface of a rotating drum with liquid cooling. The molten metal is Cool at a rate of about 1 GG () sail or faster per second .: Gold solidifies before the atoms have a chance to separate or crystallize. The resulting solid metal alloy: has a non-printed glass-like atomic structure. The surface of the solid belt contacting the drum is more Thick, because of the small defects introduced on the drum surface, resulting in a small point of 150. 乂 Refer to Figure 4 ', which does not show a cross-sectional view of the laminate of Figure 3, which has been provided with the insulating material of the present invention. As shown in Figure 4: The metal oxide material containing the insulating material 14G has been formed between the adjacent layers 120a. The insulating material 14o is formed on a relatively smooth surface with a rough surface 122 1, especially covering Got a little 15Q. The edge 4i40 system is located between the metal contacts of the adjacent metal layer 120ad, and the previous flow path system is interrupted. As a result, the lamination shows the preferred processing conditions of the present invention for the current path to oxidize the metal to form a metal oxide insulation material system. Depends on the core metal and the desired magnetic properties. For example, when Fe / Si / C / B amorphous metal alloys are processed, it is preferable to heat the core to a temperature of from about 26 (TC to 427 ° C ( 500T to 800 卞), more preferably 354 C to 365 C (670 F to 690 F) 'g, and apply a long magnetic field. When flat ring characteristics are desired, heating is preferably greater than about 399t (75 ° C) ) To about 416 ° C (780 ° F). When the characteristics of the ring are desired, the heating is preferably about ⑺ page 16 This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297) I -------------- * ΙΓ (Please read the notes on the back before filling this page) Order ·

經濟部智慧財產局員工消費合作社印製 508595 A7 B7 五、發明說明() °C 及 388°C (71〇°F 至 730°F )。 對於非晶金屬合金,良好結果已經藉由加熱鐵心至其 回火溫度並同時於回火時形成金屬氧化物加以完成。對於 多數非晶金屬合金,回火溫度係於354。(:至365(67〇下 至6 9 0 °F ),但幾項此合金具有超出此範圍之回火溫度。作 為磁心之金屬合金帶之回火溫度已經為熟習於本技藝者 所知。例如,用於非晶金屬合金METGLAS之回火條件已 經於阿來信號及漢尼威先進材料技術公告所報告過。 吾人已觀察到形成絕緣材料之處理係更有效,若纏繞 磁心被以一循環爐處理的話。一適用於此處理之爐係由美 國伊利諾州藍島型號AGC7-1406G。空氣/蒸汽混合之循環 於爐中以保持爐之均勻溫度,以使空氣帶入爐中建立氧化 反應。於此處理完成後,爐被冷卻。 鐵心應曝露至蒸汽一足夠長時間,以形成用於鐵心應 用之絕緣材料4 0層。吾人發現由0 · 5至1 2小時或更久之 時間段可以使用。良好結果已經觀察到當曝露時間為1至 6小時時,較佳係2至6小時’及最好是4 - 6小時。蒸汽 壓力應足以造成蒸汽穿透進入積層組件中。吾人發現蒸汽 壓力約0.1至2.5psi,較佳係1至2psi,係足夠用於此目 的。然而,其他蒸汽壓力也可以使用’並係由熟習於此技 藝者所知。例如,蒸汽廢力範圍由0 · 1至1 〇 〇 〇 s丨或更多也 可以使用。更者,引入瀘中之蒸汽流必須足夠以允許塗層 之形成。較佳地,流量係至少〇 · 2 2加俞/小時每立方叹之 爐空間,更好是至少0 · 2 5加侖/小時每立方无,最妤是至 第17頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) ---------------· ΙΓ (清先閱讀背面之注意事項再填寫本頁) · 卜線' 經濟部智慧財產局員工消費合作社印製 508595 經濟部智慧財產局員工消費合作社印製 A7 B7 五、發明說明() 少0.26加命/小時每立方叹。可以用以控制蒸汽進入之流 量的流限制器包含具有直徑範圍由约1/18吋至5/8叶之圓 形孔插座。 於金屬帶上之塗層的加強成長及厚度係被觀察,當蒸 汽係加入[Fex〇y]+z陽離子時’其中於此化學式中之x,y, 2因數是,1$)^2,1$)^3,1$2^3。[1^(^广陽離子 之鐵部份係被認為很活躍以完成於Μ E T g l A S 2 6 0 5 S A 1之 多數鐵表面上之氧化’以及,其他富鐵非晶合金及其他金 屬可以用於本發明。由於氧化狀態考量,鐵陽離子啟始所 需電化學反應,並容易搞合至鐵鍵。也可能部份溶解於蒸 汽中之Fe:2〇3被限定於成長塗層氧化物於金屬之表面上, 藉以增加其厚度及絕緣特性。 鐵陽離子之適當源可以是簡單為用以產生蒸汽之鐵 鍋爐中之氧化鐵殘留。較佳源係包圍[FexOy] + z陽離子成為 一遷移基質’具有已知濃度之鐵陽離子,其係被放於蒸汽 路徑中。用此一遷移基質改良於塗層處理中之均勻性,造 成具有對於非晶金屬合金及非結晶材料之更均勻磁效 能。較佳地,加至基質之Fe2〇3([FexOy] + z陽離子之源)係 被包裝,即被吸收,基質具有很高表面積及表面特性,^ 完成[Fex〇y] + z陽離子之釋放及可能Fe2〇3分子進入蒸汽 中。基質應具有高表面積,並被分佈於一多模型孔分稀, 配合以強分解特性。本案發明人已經發現適當基質可以II 由將矽酸鋁浸泡於一稀釋氯化鐵溶液中(其已經以HC1加 以澄清),並混合以MH4〇H,並加熱以吸收所產生之氧化 第18頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) (請先閱讀背面之注意事項再填寫本頁)Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs 508595 A7 B7 V. Description of Invention () ° C and 388 ° C (71 ° F to 730 ° F). For amorphous metal alloys, good results have been achieved by heating the core to its tempering temperature and simultaneously forming metal oxides during tempering. For most amorphous metal alloys, the tempering temperature is 354. (: To 365 (67 ° to 690 ° F), but several of this alloy have tempering temperatures outside this range. The tempering temperature of metal alloy strips as magnetic cores is already known to those skilled in the art. For example, the tempering conditions used for amorphous metal alloy METGLAS have been reported in Alai Signal and Hannover Advanced Materials Technology Bulletin. I have observed that the processing system for forming insulating materials is more effective. If the winding core is wound in a cycle If the furnace is used for treatment, a furnace suitable for this treatment is a model of AGC7-1406G from Blue Island, Illinois, USA. The air / steam mixture is circulated in the furnace to maintain the uniform temperature of the furnace, so that air is brought into the furnace to establish an oxidation reaction. After this treatment is completed, the furnace is cooled down. The iron core should be exposed to steam for a long enough time to form 40 layers of insulating material for iron core applications. I have found that it can be used for a period of 0.5 to 12 hours or more Good results have been observed when the exposure time is from 1 to 6 hours, preferably from 2 to 6 hours, and most preferably from 4 to 6 hours. The steam pressure should be sufficient to cause steam to penetrate into the laminated components. The current steam pressure is about 0.1 to 2.5 psi, preferably 1 to 2 psi, which is sufficient for this purpose. However, other steam pressures can also be used and are known to those skilled in the art. For example, the steam waste force range is given by 0 · 1 to 1 000 s or more can also be used. Furthermore, the steam flow introduced into the thorium must be sufficient to allow the coating to form. Preferably, the flow rate is at least 0.2 2 plus sho / hour Furnace space per cubic sigh, more preferably at least 0 · 25 5 gallons per hour without cubic per cubic meter, the most up to page 17 This paper size applies Chinese National Standard (CNS) A4 (210 X 297 mm)- ------------- · ΙΓ (Read the notes on the back before filling in this page before Qing) · Bu Xian 'Printed by the Intellectual Property Bureau Employee Cooperatives of the Ministry of Economic Affairs 508595 Employee Consumption of the Intellectual Property Bureau of the Ministry of Economic Affairs Cooperative printed A7 B7 V. Description of the invention () Less 0.26 plus life / hour per cubic sigh. A flow restrictor that can be used to control the flow of steam ingress includes a circle with a diameter ranging from about 1/18 inch to 5/8 leaves Hole-shaped socket. The enhanced growth and thickness of the coating on the metal strip are observed When steam is added based [Fex〇y] + z cation 'of the formulas herein wherein x, y, 2 factor is 1 $) $ 2,1 ^) ^ 3 ^ 3, $ 2. [1 ^ (^ The iron part of the broad cation is considered to be very active to complete the oxidation on most iron surfaces of MET gl AS 2 6 0 5 SA 1 ', and other iron-rich amorphous alloys and other metals can be used. In the present invention, due to the consideration of the oxidation state, the iron cation starts the required electrochemical reaction and is easily coupled to the iron bond. It may also be partially dissolved in the steam Fe: 203 is limited to the growth of the coating oxide on On the surface of metal, to increase its thickness and insulation characteristics. A suitable source of iron cations can be simply iron oxide residues in iron boilers used to generate steam. A preferred source is to surround [FexOy] + z cations as a migration matrix 'Iron cations with a known concentration are placed in the steam path. The use of this migration matrix improves the uniformity in the coating process, resulting in a more uniform magnetic performance for amorphous metal alloys and amorphous materials. Preferably, the Fe2O3 (source of [FexOy] + z cations) added to the matrix is packaged, that is, absorbed, the matrix has a high surface area and surface characteristics, and ^ completes the release of [Fex〇y] + z cations And possibly Fe 203 molecules enter the steam. The matrix should have a high surface area and be distributed in a multi-model pore to dilute and cooperate with strong decomposition characteristics. The inventors of the present case have found that a suitable matrix can be obtained by immersing aluminum silicate in a diluted chlorine Iron solution (which has been clarified with HC1), mixed with MH4〇H, and heated to absorb the generated oxidation. Page 18 This paper applies China National Standard (CNS) A4 (210 X 297 mm). (Please read the notes on the back before filling this page)

508595 A7 B7 五、發明說明() (請先閱讀背面之注意事項再填寫本頁) 鐵加以形成。一具有鐵1 〇%w/w基質應供給足夠氧化鐵陽 離子。此一基質係可以由美國加州黑絲匹利之A m o r p h i c 〇 所購得。相較於鐵心未曝露至由矽酸鋁基質之氧化鐵陽離 子,於由本案處理所完成之使用矽鋁基質之用於磁心之功 率損失之降低係典型不少於30%,對於METGLAS2606SA1 會至50%,本案已相較於由鍋爐片或硬水之效能改良了均 勻性。 參考第7及8圖,其中示出一可以用作為Fe2〇3基質 之適當矽酸鋁之吸收及分解等溫分佈及頻譜圖。第7圖繪 出一具有高内部孔表面積(超出200米平方每克)及由20 至1000埃之廣孔大小分布之材料。第8圖繪出一用於緩 釋放[FexOy] + z陽離子進入噴氣蒸汽,以實際時間段,用於 很多連續批次塗層執行之接近理想等溫圖。簡言之,矽酸 鋁完成用於[FexOy] + z離子之可接受時間釋放基質。 經濟部智慧財產局員工消費合作社印製 為第7及8圖繪之矽酸鋁顯示高表面積之組合及接近 理想分解特性創造了 一基質,該基質釋放濃度之[FexOy] + z 陽離子及Fe2〇3分子成為一低壓蒸汽源。”摻雜"蒸汽依序 傳送於衝擊帶鐵心之積層間之[Fex〇y;| + z陽離子及Fe203分 子。沉積Fe2〇3及鐵離子陽離子加強了於金屬合金中之鐵 的氧化,藉以完成有效絕緣塗層。大約2 0立方吋之矽酸, 鐵錯基質具有至少每生產流程20-44小時之有用壽命,即 矽酸鐵鋁之4 - 8小時每立方吋。基質可以供給1 5 0至 2OOppm氧化鐵/氧化鐵離子至進入室中之蒸汽並生產可接 受之塗層。 第19頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐)508595 A7 B7 V. Description of the invention () (Please read the notes on the back before filling this page) Iron to form. A substrate with 10% w / w iron should be supplied with sufficient iron oxide cations. Such a matrix system is commercially available from Amorp h i c 〇, Hessipyl, California. Compared with the iron core which is not exposed to the iron oxide cations from the aluminum silicate matrix, the reduction in power loss for the core using the silicon aluminum matrix completed by the treatment of this case is typically not less than 30%, and for METGLAS2606SA1 it will be 50 %, This case has improved the uniformity compared with the efficiency of the boiler plate or hard water. Referring to Figures 7 and 8, there is shown an absorption and decomposition isotherm distribution and spectrum diagram of a suitable aluminum silicate that can be used as a Fe203 matrix. Figure 7 depicts a material with a high internal pore surface area (exceeding 200 meters squared per gram) and a wide pore size distribution ranging from 20 to 1000 Angstroms. Figure 8 depicts a near-ideal isotherm for the slow release of [FexOy] + z cations into the jet steam for practical time periods for many consecutive batches of coatings. In short, aluminum silicate completes an acceptable time release matrix for [FexOy] + z ions. The Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs printed a combination of aluminum silicates shown in Figures 7 and 8 showing a combination of high surface area and near-ideal decomposition characteristics to create a matrix that releases [FexOy] + z cations and Fe2. 3 molecules become a low-pressure steam source. "Doped" steam is sequentially transmitted between the [Fex〇y; | + z cations and Fe203 molecules between the cores of the impact zone. The deposition of Fe203 and iron ion cations enhances the oxidation of iron in the metal alloy, thereby Complete effective insulation coating. Approximately 20 cubic inches of silicic acid, iron-copper matrix has a useful life of at least 20-44 hours per production process, that is, 4-8 hours per cubic inch of ferric aluminum silicate. The matrix can supply 1 5 0 to 2OOppm of iron oxide / iron oxide ions into the steam entering the chamber and produce an acceptable coating. Page 19 This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm)

五、發明說明() 使用第7及8圖之矽酸鐵鋁基質所形成之鐵心之效能 資料係示於以下之表2中。示於表2及第9圖中之資料係 使用5至lOpsi蒸汽源,以〇125吋直徑及具有20立方吋 體積之罐’於蒸汽源及塗層室爐間具矽酸鐵鋁加以建立。 於塗覆室爐中之蒸汽壓力係典型由〇·5至2pSi,及塗層係 藉由將曝露至蒸汽4小時於690T至700卞加以產生。 表 2--6 i% 3月之Meglas2605SAl生產之磁心重對功率損失 磁心重(磅) 低功率損(瓦/磅) 中功率損(瓦/碡) 高限(瓦/碡) •05 9.8 11.9 14.0 •08 10.2 10.5 10.7 •22 9.0 丨 9.0 9.0 •31 9.6 10.5 11.5 .36 10.8 12.1 13.4 .41 8.1 8.8 9.6 •43 9.3 12.7 ----- 16.1 .435 16.2 18.7 21.1 •58 9.3 11.9 —---- 14.5 •70 14.1 14.6 15.1 .705 9.3 11.5 13.7 •77 10.6 12.6 14.6 .83 10.2 15.3 ---- 20.3 1.06 1.3 16.1 ----- 18.9 2.41 13.9 13.9 13.9 第20頁 經濟部智慧財產局員工消費合作社印製 (請先閱讀背面之注意事項再填寫本頁} 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 A7 B7 五、發明說明( 2.42 10.3 12.5 14.8 4.50 9.1 10.3 11.4 5.2 8.5 9.2 10.0 5.73 1.5 1.5 1.5 5.97 11.2 15.4 19.5 6.37 7.5 7.9 8.3 6.57 11.4 14.3 17.1 8.32 10.1 10.2 10.2 8.6 9.5 9.5 9.5 功率量測於20KHz及〇·2泰斯拉。磁心平均重量以計算瓦/磅 (請先閱讀背面之注意事項再填寫本頁) 較佳地’磁心係被氧化處理前或時所回火,該氧化處 理係用以形成絕緣材料於金屬帶表面上。如熟習於本技# 者所知,回火降低了於磁心中之磁不連續量並可以給予磁 心想要之磁特性。於磁心層間之全層絕緣金屬氧化物之出 現藉由應力之建立干擾了回火處理。這係藉由於磁心被纏 繞後然後於回火時或之後,以形成絕緣材料,以處理磁心 加以避免。因為本發明之處理於回火溫度或以下之溫度生 產金屬氧化物絕緣材料’所以此較佳順序可以用於多數類 型之磁心。 一已取得良好結構之實施例係在磁場下被回火一非 晶金屬合金鐵心(含鐵作為主要金屬)於約365它之空氣溫 度中,以對齊於鐵心中之磁疇。於將鐵心曝露至蒸汽以形 成氧化鐵絕緣層前,爐溫然後被降低至3〇5至329t(58〇 第21頁 訂·· 卜線_ 經濟部智慧財產局員工消費合作社印製 508595 A7 B7 五、發明說明() 至625 F )。即使回火係、被完成於空氣中以高於由本發明處 理形成絕緣層之^,但於帶之表面上並未有U金屬氧 化物以提供於層間之介電絕緣。 另一產生特别好之結果的實施例係於鐵心被回火 時”乂蒸汽及2氣處理非晶金屬合金鐵心,令鐵作為主要 金屬。換句話說,絕緣氧化鐵塗層之形成及回火同時發 生。非晶金屬合金之回火溫度將指定處理之精確溫度,如 以上所述。 、本發明之塗層同時藉由引入或釋放機械應力而完成 優良效能。如同於熟習於本技藝者所知,於軟磁心之功率 損失具有兩成份。第—成份為渦電流,其係由於引入基材 層中《電壓之磁通變化所產生。渦流損失係直接有關於感 應線圈之操作頻率,並JL,於4⑽Ηζ或更低之低操作頻率 中係為小角色,特別是於非晶及細結晶材料中是如此。 經濟部智慧財產局員工消費合作社印製 (請先閱讀背面之注意事項再填寫本頁) 卜線 功率損失 < 第二成份為磁滯效應所造成,其係為當磁 材料重覆一磁化循環時之能量損失量。置於磁材料上之應 力可以增加磁滯損失,藉由影響形成於磁材料中之磁疇活 動。特別是,應用於大磁化限制,例如非晶金屬合金時, 之材料磁滯循環係特別不想要的。當同時應用金屬帶回火 時,本發明之塗層允許於下層金屬帶之減少之應力。吾人 相仏塗層之氧化鐵之軟性構成此效應。因為塗層可以於典 型回火溫度中移動,所以於金屬帶上之應力被降低,因為 塗層於回火時,作為於金屬帶上之潤滑釋放應力,而改良 其效能。例如,於低頻操作條件下,當渦流損失很小 第22頁 508595 A7 B7 五、發明說明() 本發明之同時回火塗層鐵心相較於未塗覆鐵心改良了效 能。見以下之表3。此改良效能將不被期望由相鄰金屬層 之介電絕緣改變效能,並可以部份建立降低磁滯損之金屬 帶上之應力。再者,釋放於下層金屬帶之應力的效應可以 由以顯微鏡分斷於塗廣中之線斷加以完成。 再者,本發明之塗層並未引入任何於磁心上不想要之 壓縮應力,由於熱膨脹之故。吾人知道METGLAS2605SA1 及2605SC之膨服係數分別為7.6及5.9ppm每。C。一般傳 統用作為絕緣之材料例如氧化錳及MYLAR分別具有8及 絕緣材料40-9Oppm每。C之膨脹係數。因為絕緣之膨脹係 數超出金屬者,所以使用MgO或MYLAR作為絕緣引入了 於操作溫度範圍中壓縮應力。吾人相信鐵心之應力增加功 率損失二之因數。然而’本發明塗層並未引入壓縮應力’ 而大大地改良了效能。 以下表 3 所示的是由處理 METGLAS2605SA1 及 2605 SC以設計以消除應力所形成之鐵心之資料比較。特 別是,由加熱纏繞鐵心至670-690 °F四小時所形成之塗 層,同時將鐵心外露至0.1至0.5psi之壓力之蒸汽。這些 鐵心之資料係比較於為錳甲基處理(MgO)所形成之鐵心。 結果係示於表3中,及對於非晶材料之塗層鐵心2及4相 較於標準錳甲基塗層之鐵心1及3減少了 5 0%之損失。 第23頁 本紙張尺度適用中國國家標準(CNS)A4規格(210^297公釐) (請先閱讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製V. Description of the invention () The performance data of the iron core formed by using the ferrous aluminum silicate matrix of Figs. 7 and 8 is shown in Table 2 below. The data shown in Tables 2 and 9 were created using a steam source of 5 to 10 psi, a tank with a diameter of 0125 inches and a volume of 20 cubic inches, and an iron silicate between the steam source and the coating chamber furnace. The vapor pressure in the coating chamber furnace is typically from 0.5 to 2 pSi, and the coating is generated by exposing to steam for 4 hours at 690T to 700 Torr. Table 2--6 i% March core weight produced by Meglas 2605SAl versus power loss core weight (lbs.) Low power loss (W / lb) Medium power loss (W / 碡) High limit (W / 碡) • 05 9.8 11.9 14.0 • 08 10.2 10.5 10.7 • 22 9.0 丨 9.0 9.0 • 31 9.6 10.5 11.5 .36 10.8 12.1 13.4 .41 8.1 8.8 9.6 • 43 9.3 12.7 ----- 16.1 .435 16.2 18.7 21.1 • 58 9.3 11.9 ----- -14.5 • 70 14.1 14.6 15.1 .705 9.3 11.5 13.7 • 77 10.6 12.6 14.6 .83 10.2 15.3 ---- 20.3 1.06 1.3 16.1 ----- 18.9 2.41 13.9 13.9 13.9 Page 20 Intellectual Property Bureau Staff Consumer Cooperatives, Ministry of Economic Affairs Printed (Please read the precautions on the back before filling in this page) This paper size applies to China National Standard (CNS) A4 (210 X 297 mm) 508595 A7 B7 V. Description of the invention (2.42 10.3 12.5 14.8 4.50 9.1 10.3 11.4 5.2 8.5 9.2 10.0 5.73 1.5 1.5 1.5 5.97 11.2 15.4 19.5 6.37 7.5 7.9 8.3 6.57 11.4 14.3 17.1 8.32 10.1 10.2 10.2 8.6 9.5 9.5 9.5 9.5 The power was measured at 20KHz and 0.2 Tesla. The average core weight was calculated in watts per pound ( Please read the notes on the back before filling (Page) Preferably, the magnetic core is tempered before or at the time of the oxidation treatment, which is used to form an insulating material on the surface of the metal strip. As known to those skilled in the art, tempering is reduced in the magnetic core. The magnetic discontinuity can give the magnetic core the desired magnetic properties. The appearance of a full-layer insulating metal oxide between the core layers interferes with the tempering process by the establishment of stress. This is because the core is wound and then tempered. At or after, the insulating material is formed to avoid the processing of the magnetic core. Because the process of the present invention produces metal oxide insulating materials at or below the tempering temperature, this preferred sequence can be used for most types of magnetic cores. An example of achieving a good structure is to temper an amorphous metal alloy core (containing iron as the main metal) in a magnetic field at an air temperature of about 365 to align the magnetic domains in the core. The core is exposed to steam Before the iron oxide insulating layer is formed, the furnace temperature is then lowered to 305 to 329t (58 ° page 21 order.… Line _ Printed by the Ministry of Economic Affairs Intellectual Property Bureau Staff Consumer Cooperatives 508595 A7 B7 5. Description of the invention () to 625 F). Even though the tempering system is completed in the air to be higher than the insulating layer formed by the process of the present invention, there is no U metal oxide on the surface of the tape to provide dielectric insulation between the layers. Another example that produces particularly good results is when the iron core is tempered. "Rhenium steam and 2-gas treatment of amorphous metal alloy cores, with iron as the main metal. In other words, the formation and tempering of an insulating iron oxide coating Simultaneous. The tempering temperature of the amorphous metal alloy will specify the precise temperature of the treatment, as described above. The coating of the present invention simultaneously achieves excellent performance by introducing or releasing mechanical stress. As is familiar to those skilled in the art It is known that the power loss in the soft magnetic core has two components. The first component is the eddy current, which is caused by the change in the magnetic flux of the voltage introduced into the substrate layer. The eddy current loss is directly related to the operating frequency of the induction coil, and JL It is a small role in low operating frequency of 4⑽Ηζ or lower, especially in amorphous and fine crystalline materials. Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs (please read the precautions on the back before filling in this (Page) The power loss of the wire < The second component is caused by the hysteresis effect, which is the amount of energy loss when the magnetic material repeats a magnetization cycle. Put on the magnetic material The stress can increase the hysteresis loss by affecting the magnetic domain activity formed in the magnetic material. In particular, when applied to large magnetization restrictions, such as amorphous metal alloys, the hysteresis cycle of the material is particularly undesirable. When applying metal band tempering, the coating of the present invention allows for reduced stress on the underlying metal band. The softness of the iron oxide of our coatings constitutes this effect. Because the coating can move at typical tempering temperatures, it is The stress on the metal strip is reduced because the coating, when tempered, releases stress as a lubricant on the metal strip and improves its performance. For example, under low frequency operating conditions, when the eddy current loss is small Page 22 508595 A7 B7 V. Description of the invention () The simultaneous tempered coated core of the present invention has improved performance compared to the uncoated core. See Table 3 below. This improved performance will not be expected to be changed by the dielectric insulation of adjacent metal layers. , And can partially establish the stress on the metal strip that reduces the hysteresis loss. Furthermore, the effect of the stress released on the lower metal strip can be broken by the microscope to the line of Tu Guangzhong. In addition, the coating of the present invention does not introduce any unwanted compressive stress on the magnetic core due to thermal expansion. I know that the expansion coefficients of METGLAS 2605SA1 and 2605SC are 7.6 and 5.9 ppm each. C. General tradition Materials used as insulation such as manganese oxide and MYLAR have an expansion coefficient of 8 and insulation materials of 40-9Oppm per C. Because the expansion coefficient of insulation exceeds that of metal, the use of MgO or MYLAR as insulation has introduced compression in the operating temperature range. I believe that the stress of the core increases the power loss factor by two. However, 'the coating of the present invention does not introduce compressive stress' and greatly improves the performance. Table 3 below is designed by processing METGLAS 2605SA1 and 2605 SC to eliminate Comparison of data on cores formed by stress. In particular, the coating is formed by heating and winding the core to 670-690 ° F for four hours while exposing the core to steam at a pressure of 0.1 to 0.5 psi. The data of these cores are compared with those formed by manganese methyl treatment (MgO). The results are shown in Table 3, and the coated cores 2 and 4 for the amorphous material reduced the loss by 50% compared to the standard manganese methyl coated cores 1 and 3. Page 23 This paper size is in accordance with Chinese National Standard (CNS) A4 (210 ^ 297 mm) (Please read the precautions on the back before filling out this page) Printed by the Employees ’Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs

508595 A7 B7 五、發明說明()508595 A7 B7 V. Description of the invention ()

表 3 : METGLAS2605SA1&2605SC : 5.25”UDX4.0"IDX2,,SW # 材料處理條件 鐵心千瓦 開始安培 設定安培 脈衝Jim3 1 2605SA1,標準(MgO) 95.3 25 42 810 2 2605SA1,塗層,零應力△ B=2.BT,2#s 57.7 10 20 490 3 2605SC,標準(MgO)Z\B=2.6T,2 /2S 102 25 40 867 4 2605SC,塗層,零應力△ B=3.05T,2/zs 61 10 20 518 條件:5.35-5.8千伏施加至鐵心上使用6圈,lOpps,及2#秒脈衝寬,通量2.8-3.05T (請先閱讀背面之注意事項再填寫本頁)Table 3: METGLAS2605SA1 & 2605SC: 5.25 "UDX4.0 " IDX2 ,, SW # Material processing conditions core kW start ampere set ampere pulse Jim3 1 2605SA1, standard (MgO) 95.3 25 42 810 2 2605SA1, coating, zero stress △ B = 2.BT, 2 # s 57.7 10 20 490 3 2605SC, standard (MgO) Z \ B = 2.6T, 2 / 2S 102 25 40 867 4 2605SC, coating, zero stress △ B = 3.05T, 2 / zs 61 10 20 518 Conditions: Apply 5.35-5.8 kV to the core and use 6 turns, lOpps, and 2 # second pulse width, flux 2.8-3.05T (Please read the precautions on the back before filling this page)

處理加強以改變磁特性 塗層可以發生之處理溫度可以加以調整,以調整所得 鐵心之基本磁特性。對於例如METGLAS2605SA1之非晶 金屬合金,曝露至蒸汽至由約3 88°C (730°F )至427t (800 °F )之溫度傾向於產生圓及扁平環特性。當一縱長磁場係 於塗層形成時被施加時,於3 7 9 °C (7 1 5 °F )以下之溫度傾向 於產生正方形環特性。於379°C至3 88°C (715至730°F )間 之溫度傾向於產生具有圓環磁特性之鐵心。 例如想要一用於環形之扁平環特性時,應用可以用以 間隙以限制有效導磁率。然而,間隙需要其他處理步驟, 典型相較於沒有間隙之環造成相當大之功率消散。等效扁 平環特性可以替代具有較低所得功率消散之例子(因為其 中並沒有間隙)及潛在上係較易製造(因為不需切割一間 第24頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 卜線· 經濟部智慧財產局員工消費合作社印製 經濟部智慧財產局員工消費合作社印製 五、發明說明( 隙) 雖然有可能以使用傳統處理及於橫向磁場出現時,產 生一扁平磁滞環,但這是較困難。理由是橫向磁場係垂直 於圓周方向方向)’因此,需要-特殊磁場產生器。 磁场產:器係典型為一載電流多圈螺線管,其係由包在爐 或成之很大線所建互或是_放置在具間隙之大C 形鐵心電磁鐵外之電場’該間隙係通過有一適當定向鐵心 (受熱通道。於後例中’爐必須被特殊設計,以用於棒向 場回火,並特別受限於很特定之鐵心大小。螺線管殼通常 很限制可以被橫放之元件量’並容易受到過量處理變化。 然而’當本發明配合適當回火溫度時,扁平磁滯環係更容 易形成。 更明確地說,當METGLAS2605A1被加熱於715卞之 蒸汽四小時或使用縱向磁場以定位磁疇時,則一直得到一 般正方形環特性。這已經於生產中加以驗證,於由丨磅至 超出40镑之鐵心。於接近715Τ-73〇ΐ或更高溫度中,於 正方形’圓形及扁平環狀態間之轉換並沒有尖銳變化,因 為塗層時間及溫度以合成方式與上述作動溫度互動。當鐵 心很小,即少於1磅時,4小時之塗層或超出73〇τ之蒸 汽可以造成扁平鐵心。雖然所述溫度可能略有不同,但例 如METGLAS2605SC之其他非晶金屬也可以類似地動作。 磁性非晶合金有兩項技術重要等級:過渡金屬(ΤΜ). 類金屬(Μ)合金及稀土過渡金屬合金。METGLAS2605SA1 及其等效商品係為過渡金屬類金屬合金,其廣泛地說包含 第25頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 x 297公釐) (請先閱讀背面之注意事項再填寫本頁)Processing enhancements to change the magnetic properties The processing temperature at which the coating can occur can be adjusted to adjust the basic magnetic properties of the resulting core. For amorphous metal alloys such as METGLAS 2605SA1, exposure to steam to temperatures from about 3 88 ° C (730 ° F) to 427t (800 ° F) tends to produce round and flat ring characteristics. When a longitudinal magnetic field is applied when the coating is formed, temperatures below 37 ° C (71.5 ° F) tend to produce a square ring characteristic. Temperatures between 379 ° C to 3 88 ° C (715 to 730 ° F) tend to produce iron cores with toroidal magnetic properties. For example, if you want a flat ring feature for a toroid, the application can be used with a gap to limit the effective magnetic permeability. However, gaps require additional processing steps, which typically result in considerable power dissipation compared to loops without gaps. Equivalent flat ring characteristics can replace the example of lower power dissipation (because there is no gap) and the potential upper line is easier to manufacture (because there is no need to cut a room) Page 24 This paper applies Chinese National Standard (CNS) A4 Specifications (210 X 297 mm) Printed by the Consumers ’Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs, printed by the Employees’ Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs. When a flat hysteresis ring is generated, this is more difficult. The reason is that the transverse magnetic field is perpendicular to the circumferential direction) 'Therefore, a special magnetic field generator is needed. Magnetic field generation: The device is typically a multi-turn solenoid with a current carrying current, which is built by a large wire enclosed in a furnace or an electric field placed outside a large C-shaped iron core electromagnet with a gap. The gap is passed through an appropriately oriented core (heated channel. In the following example, the furnace must be specially designed for rod field tempering and is particularly limited by very specific core sizes. Solenoid shells are usually very limited. The amount of elements placed horizontally 'is susceptible to excessive processing changes. However, when the present invention is matched with an appropriate tempering temperature, a flat hysteresis ring system is easier to form. More specifically, when METGLAS 2605A1 is heated to 715 ° F. When the vertical magnetic field is used to locate magnetic domains for hours or less, the general square ring characteristics are always obtained. This has been verified in production and applied to iron cores from 丨 pounds to over 40 pounds. At temperatures close to 715T-73 ° C or higher There is no sharp change in the transition between the square 'round and flat ring states, because the coating time and temperature interact with the above-mentioned operating temperature in a synthetic manner. When the core is small, that is, less than 1 pound, it takes 4 hours. Layers or steam exceeding 73〇τ can cause flat iron cores. Although the temperature may be slightly different, other amorphous metals such as METGLAS 2605SC can also behave similarly. Magnetic amorphous alloys have two technically important grades: transition metals ( TM). Metal-like (M) alloys and rare-earth transition metal alloys. METGLAS2605SA1 and its equivalent are transition metal-based metal alloys, which are broadly included on page 25. This paper applies Chinese National Standard (CNS) A4 specifications ( 210 x 297 mm) (Please read the notes on the back before filling out this page)

508595 A7 B7 五、發明說明() 約80原子量%之一或多數Fe,Co或Ni及20原子量%之 B,C ’ Si,P 或 A1。#2805 合金係為 80%Fe 及 20%B,其 (請先閱讀背面之注意事項再填寫本頁) 係用於現在METGLAS2605xxx合金之前幾代。類金屬成 份係為要以降低溶點’使得合金可以迅速經由其玻璃轉移 溫度加以快速淬火。同樣類金屬同時也穩定所得淬火非晶 相’並相對於可比結晶合金降低了飽和磁化及玻璃轉移溫 度。 這些主要想要合金因為其預想等向特徵已經被顯示 造成很低矯頑磁性及磁滯損失反很高導磁性,其組合對於 高頻應用係很重要的。然而,其弱點係在於亞穩態,其可 以造成取後結晶’而不管類金屬穩定劑出現否。因此,相 當多之研究係針對於TM-M非晶合金穩定性及結晶時間常 數。這是因為有關於磁應用之壽命結束係被認為相對於結 晶化之設定。對於很小溫度增加,於結晶溫度範圍中,矯 頑磁性力及功率損失增加及剩磁及導磁率降低,均呈很快 速之速率。這是METGLAS2605SA1連續服務溫度定於相 當保守150 °C之理由之一。同樣地,因為此作用,有可能 以藉由將鐵心回火於結晶溫度範圍中一控制量之時間加 以調整導磁率。 經濟部智慧財產局員工消費合作社印製 TM-M合金之穩定性已經被發現係相關於結晶設定溫 度及玻璃轉移溫度間之差。於熔化溫度及玻璃轉移溫度間 Tg,當接近Tg時,結晶快速增加。另一方面,當結晶設 定溫度低於Tg時,結晶快速減少。因此,對於結晶設定 時間常數之討論,玻璃轉移溫度為一重要參數。對於#2605 第26頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) A7508595 A7 B7 V. Description of the invention () One or most of Fe, Co or Ni at about 80 atomic% and B, C 'Si, P or A1 at 20 atomic%. # 2805 alloys are 80% Fe and 20% B, which (please read the precautions on the back before filling this page) are used in the previous generations of the METGLAS2605xxx alloy. The metalloid component is to reduce the melting point 'so that the alloy can be rapidly quenched through its glass transition temperature. At the same time, the same metal also stabilizes the obtained quenched amorphous phase 'and lowers the saturation magnetization and glass transition temperature relative to comparable crystalline alloys. These mainly wanted alloys have been shown to cause very low coercivity and hysteresis loss and very high magnetic permeability because of their expected isotropic characteristics. The combination is important for high frequency applications. However, its weakness lies in the metastable state, which can cause crystallization after removal ' regardless of the presence of metal-like stabilizers. Therefore, a considerable amount of research has focused on the stability and crystallization time constants of TM-M amorphous alloys. This is because the end of life for magnetic applications is considered relative to the setting of crystallization. For a small temperature increase, in the crystallization temperature range, the coercive force and power loss increase, and the remanence and magnetic permeability decrease, all at a rapid rate. This is one of the reasons why the continuous service temperature of METGLAS2605SA1 is set at a relatively conservative 150 ° C. Also, because of this effect, it is possible to adjust the magnetic permeability by tempering the core for a controlled amount of time in the crystallization temperature range. The stability of the TM-M alloy printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs has been found to be related to the difference between the crystallization set temperature and the glass transition temperature. Between the melting temperature and the glass transition temperature, Tg, when approaching Tg, the crystallization increases rapidly. On the other hand, when the crystallization setting temperature is lower than Tg, the crystallization decreases rapidly. Therefore, for the discussion of setting the time constant of crystallization, the glass transition temperature is an important parameter. For # 2605 page 26 This paper size applies Chinese National Standard (CNS) A4 (210 X 297 mm) A7

獨595 五、發明說明() 合金之Tg被公開為441 X:或825· 8T。漢尼威並未公開用 於METGLAS2605SA1之Tg或用於任一 METGLAS合金之 事項。然而,其確實公告用於2605SA1及其他metglas 合金之結晶溫度’對於2 6 0 5 S A 1為9 4 5 °F,其係高於用於 # 2 6 0 5合金之T g約1 2 0 °F。假設漢尼威結晶溫度為τ g,, 對於回火一已知時間之#2605合金之公開結晶設定溫度為 可能或120°F低於用於2805SA1非晶成份者。這大量差之 理由是2605SA1係大大不同於#2605合金在於其在化學上 加入其他元素。 基於此基礎及於窩法拉著之”鐵磁材料”(北荷蘭出版 社)之第6章中所示之表,顯示對於#2605合金,結晶化調 整發生於6 0 0 - 6 1 0 °F 2至5小時後。因此,估計對於2至5 小時之回火時間,結晶化可能調整2605SA1合金於720-730°F範圍中超出690°F,基於於690卞及730°F之導磁性 及功率損失量測之比較。此觀察係相當符合於#2605合金 T g,及2 6 0 6 S A 1合金公開結晶溫度間之差。 於以下表格及相關圖中之資料係藉由選擇兩標準漢 尼威元件號加以累積’以測試標準及非標準塗層溫度,保 持塗覆溫度時間定為4小時,具有外加一小時之溫度設定 時間。為了此測試,所選擇部件係為由具有一標準1密耳 規及約0.75镑重之METGLAS2605SA1所製造之”c”鐵 心,其他則為具有約2.5磅重。較大鐵心於窗尺寸,剖面 積,路徑長度係大約1 · 8至2倍大於較小心,該較小鐵心 具有成比例增加之窗面積及質量。兩鐵心之帶寬均約1 .2 5 第27頁 本紙張尺度適用中國國家標準(CNS)A4規格(21〇 X 297公髮) (請先閱讀背面之注意事項再填寫本頁) 訂- 經濟部智慧財產局員工消費合作社印製 508595 五、發明說明( 經 濟 部 智 慧 財 產 局 員 工 消 費 合 作 社 印 製 A7 B7 吋。用於大鐵心之長條資料及圖跟隨用於小鐵心之結果。 因此,為了簡明起見,只有較小鐵心之資料被示出。如於 此及圖中所示,名詞,,已塗覆”表示一鐵心,該鐵心已緩被 以熱及蒸汽組合以形成氧化鐵絕緣材料於積層之間。名詞 ”未塗覆”表示一鐵心,其未被以蒸汽處理,並沒有足夠氧 化鐵絕緣於積層之間。 於這些測試中,資料係使用前述四小時處理加以累 计,一小時設足處理作為一用於回火之熱模型,除了不同 度係被替代 6 9 0 F 外,即 7 1 5 °F,7 3 0 °F,7 5 0 T,7 6 0 卞, 770F , 780 F或800卞之一外。標準69〇下處理也完成於 相同測試群中,以比較特別回火溫度結果與標準處理之結 果。為了更佳觀察於所列溫度之塗層之作用,由89〇卞開 始及範圍由總數8階段至8〇〇卞,測試係被以或不以塗覆 處理完成。當塗覆提供時,處理係使用上述之鐵鋁矽酸鹽 遷移基質加以完成。對於沒有施加塗層之測試,熱處理時 間係被保持於5小時,以完全複製一小時穩定化之回火時 間條件及4小時之曝露至蒸汽及加熱,或5小時總回火時 間。測試係被以三個主要處理步驟加以完成:(1)於回火 後’(2)於以環氧樹脂浸潰後,及(3)於最終處理後。縱長 磁場係被施加,其中可以完成最大飽和磁化。當一縱長磁 場被使用時,名詞正方形(Sq)出現於以下表中。當未使用 磁場時,名詞圓(Rd)出現。因此,對於多數磁場未使用超 出約765卞之居里溫度,用於這些回火條件下。以下密集 測試係完成於8個不同溫度,一很小” c”鐵心係處理於較 第28頁 :297公釐) C請先閱讀背面之注意事項再填寫本頁)Du 595 V. Description of the invention () The Tg of the alloy is disclosed as 441 X: or 825.8T. Hannover does not disclose the use of Tg for METGLAS 2605SA1 or for any METGLAS alloy. However, it does announce that the crystallization temperature for 2605SA1 and other metglas alloys is 9 4 5 ° F for 2 6 0 5 SA 1, which is about 1 2 0 ° higher than the T g for # 2 6 0 5 alloy. F. Assuming Hanniway's crystallization temperature is τ g, the public crystallization set temperature for # 2605 alloy tempered for a known time is possible or 120 ° F is lower than those used for the 2805SA1 amorphous component. The reason for this large difference is that the 2605SA1 series is very different from the # 2605 alloy in that it chemically adds other elements. Based on this basis and the table shown in Chapter 6 of "Ferromagnetic Materials" (North Holland Press) by Wofar, it is shown that for # 2605 alloy, the crystallization adjustment occurs at 6 0 0-6 1 0 ° F After 2 to 5 hours. Therefore, it is estimated that for the tempering time of 2 to 5 hours, the crystallization may adjust the 2605SA1 alloy to exceed 690 ° F in the range of 720-730 ° F, based on the comparison of the permeability and power loss measurements at 690 卞 and 730 ° F. . This observation is quite consistent with the difference between the # 2605 alloy T g and the published crystallization temperature of the 2 6 6 S A 1 alloy. The data in the following table and related figures are accumulated by selecting two standard Hannover component numbers to test the standard and non-standard coating temperature. The time for maintaining the coating temperature is set to 4 hours, with an additional temperature setting of one hour. time. For this test, the selected component was a "c" core made of METGLAS 2605SA1 with a standard 1 mil gauge and a weight of approximately 0.75 pounds, and the others were approximately 2.5 pounds. The larger core has a window size, cross-sectional area, and path length of approximately 1.8 to 2 times larger than the smaller core, which has a proportionally increased window area and mass. The bandwidth of both iron cores is about 1.2 5 Page 27 This paper size applies the Chinese National Standard (CNS) A4 specification (21〇X 297) (Please read the precautions on the back before filling this page) Order-Ministry of Economic Affairs Printed by the Intellectual Property Bureau employee consumer cooperative 508595 V. Description of the invention (The Intellectual Property Bureau employee consumer cooperative of the Ministry of Economic Affairs printed A7 B7 inches. The bar data and diagrams for the large iron core follow the results for the small iron core. Therefore, for simplicity For the sake of simplicity, only the information of the smaller core is shown. As shown here and in the figure, the noun, "coated" means an iron core that has been slowly combined with heat and steam to form an iron oxide insulating material. Between the layers. The term "uncoated" means an iron core that has not been treated with steam and does not have enough iron oxide to insulate between the layers. In these tests, the data was accumulated using the four-hour process described above, and one hour was set. As a heat model for tempering, foot treatment is replaced by 6 9 0 F, that is, 7 1 5 ° F, 7 3 0 ° F, 7 5 0 T, 7 6 0 卞, 770F, 780 F or 800 卞In addition, the treatment under the standard 690 is also completed in the same test group to compare the results of the special tempering temperature with the results of the standard treatment. In order to better observe the effect of the coatings at the listed temperatures, starting from 890 ° and the range from For a total of 8 stages to 800, the test is done with or without coating treatment. When coating is provided, the treatment is done using the iron-aluminosilicate migration matrix described above. For tests without a coating applied, The heat treatment time is maintained at 5 hours to completely replicate the one hour stabilized tempering time condition and 4 hours of exposure to steam and heating, or 5 hours of total tempering time. The test is completed in three main processing steps : (1) after tempering '(2) after impregnation with epoxy resin, and (3) after final treatment. The longitudinal magnetic field is applied, in which the maximum saturation magnetization can be completed. When a longitudinal magnetic field is applied When used, the noun square (Sq) appears in the following table. When the magnetic field is not used, the noun circle (Rd) appears. Therefore, for most magnetic fields, the Curie temperature exceeding approximately 765 ° C is not used for these tempering conditions. The following intensive tests are performed at 8 different temperatures, a very small "c" core is processed more than page 28: 297 mm) C Please read the precautions on the back before filling this page)

508595 A7B7 五、發明說明() (請先閱讀背面之注意事項再填寫本頁) 大量於690-7 1 0°F及73 0-745 °F之中,以確保以第一群完成 之觀察。該鐵心具有约0.1磅之毛重。很小鐵心之隨後測 試確認以較小群測試於較大溫度範圍所完成之重要結 論。 導磁參數為由於磁化曲線上之零驅動,零通量點至所 定義之通量位準之斜率。 表4. 磁化曲線鐵心通量(KG)-浸以0.75#鐵心未 塗覆 驅動 690 715 730 750 750 760 770 780 800 800 T T °F Τ °F T T °F °F °F 0. 1 0.79 0.58 0.30 0.25 0.25 0.12 0.08 0.04 0.04 0.04 0.5 4.9 4.52 j . J Ζ 2.9 1 2.66 1.74 1.08 0.50 0.08 0.08 1.0 6.52 6.3 1 5.02 4.73 4.36 3.24 2.4 1 1.29 0.25 0.25 2.0 8.18 8.22 6.72 6.72 6.35 5.15 4.14 2.66 0.7 1 0.7 1 3.0 9.25 9.46 7.80 7.93 7.64 6.43 5.35 3.74 1.3 3 1.12 4.0 10.00 10.29 8.47 8.76 8.4 7 7.35 6.23 4.6 1 1.58 1.49 5.0 10.62 10.96 9.09 9.55 9.30 8.09 7.06 5.35 1.99 1.87 (De) 正方 正方 正方 正方 圓 圓 圓 圓 正方 圓 經濟部智慧財產局員工消費合作社印製 於表4中所示之所有量測係使用磁金屬定電流通量重 置測試機(CCFR)加以完成,其係調整適當鐵心剖面積及路 徑長度,以完成一校正通量位準,單位為千高斯及驅動單 位為奥斯特。另外,通量密度係被調整與1 5.9千高斯飽和 位準配合,除了 METGLAS2605SA1之塗覆及未塗覆處理 第29頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) B7 五、發明說明() 結果外。 (請先閱讀背面之注意事項再填寫本頁) 表4及相關第9圖示出大致下減之磁化曲線成為由 690至800 °F增加之回火溫度。再者,於此資料中並沒有 其他正方環作用係很明顯的,除了 690T,71 5卞及730卞 資料被使用作為縱長”正方環”磁化鐵心。這結果係為浸泡 應力之結果,因為正方形係強烈證明於預浸資料中,即鐵 心通量範圍由不少於15KG至15.9KG,由30e至最大驅動 5〇e對於上述溫度。見第16圖,其示出用於未浸潰0.75 磅未覆蓋以690卞至800T範圍之磁化曲線。 吾人相信此作用之理由是應力降低導磁率。見波窩所 著’’鐵磁’’IEEE公告(第13章,應力及磁化)。所應用等式 為-l=Bls2/gs,其中〇為啟始導磁率,Is為飽和時每單位體 積之磁化量,其係成比例於飽和磁通密度,s為飽和磁限 制,及i為單一區域中之内部應力。因為用於2605SA1之 飽和磁限制為大,即27ppm,所以更小浸潰應力之作可能 相當大。 表5-導磁率及功率損失2KG磁通密度,浸0.75#鐵心-未塗覆 因數 690〇F 715〇F 730T 750T 750°F 760T 770〇F 780T 800°F 80G°F 瓦# 16.73 10.38 26.99 16.48 10.83 17.50 16.42 17.51 20.56 26.36 導磁 9.176 8.198 6.096 5.499 5.115 3.413 2.362 1.315 398 374 經濟部智慧財產局員工消費合作社印製 於表5中之導磁率係計算於2千高斯磁通,由表4中 之資料計算出。鐵心損失係以20KHz及2KG加以量得’ 第30頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 五、發明說明() (請先閱讀背面之注意事項再填寫本頁) 使用於以下所述之測試機及第6圖。用於此鐵心之2KG 之功率量測之測試條件為··使用1 〇圈螺線管線圈之4 3 · 9 伏。用於此測試之資料被繪於第1 0圖中。 功率損失典型高於未浸潰鐵心。第1 7圖為等效於第 10圖,用於未浸潰0.75#鐵心690至800下。注意對於已 浸潰未切割鐵心之功率消散增加。 表6.磁化曲線鐵心通量(KG)-浸以0.75#鐵心塗覆 驅動 690T 715°F 730°F 750〇F 760°F 760T 760T 770T 780T 800°F 0.1 0.54 0.58 0.37 0.12 0.12 0.12 0.08 0.08 0.04 0.04 0.5 4.15 4.15 3.40 1.70 1.33 1.86 1.04 0.83 0.37 0.08 1.0 5.81 5.93 5.10 3.07 2.49 3.07 2.24 1.87 1.04 0.29 2.0 7.60 7.80 6.97 4.77 4.23 4.86 3.88 3.49 2.28 0.71 3.0 8.76 8.96 8.13 5.93 5.48 6.06 5.06 4.69 3.28 1.12 4.0 9.55 9.79 8.96 6.81 6.39 6,97 5.89 5.56 4.07 1.49 5.0 10.21 10.42 9.67 7.51 7.39 7.72 6.64 6,35 4.81 1.91 (De) 正方 正方 正方 正方 正方 正方 圓 圓 圓 圓 經濟部智慧財產局員工消費合作社印製 用於表4之說明同樣也適用於表6。本發明之塗覆似 乎較未塗覆鐵心具有略大作用於作出圓形或平坦化上’這 是取決於溫度。然而,該差異係太小而不會被經歷浸潰鐵 心之應力所注意。用於未浸潰鐵心之等效資料同時也顯示 於塗覆及未塗覆鐵心間沒有重大不同。只有當導磁率及功 率損失被認為一結晶作用時,差異出現。於第1 8 i中之 第31頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 A7 B7 五、發明說明() 未浸潰已塗覆鐵心係很”正方形’’對於低於75〇卞以下之溫 度’及於7 6 0 F或以上溫度係”爲平"。用於塗覆鐵心之浸 潰作用大量降低用於每一回火溫度之導磁率,除了 8〇〇下 以外。較佳地,相同作用係可以於未塗覆鐵心看到,除了 7 15°F回火溫度造成一較高飽和磁通外(較690°F回火溫度 高),相較於未浸潰已塗覆鐵心與未塗覆鐵心。於6 9 0 T及 7 1 5 °F間之差,對於未浸潰鐵心並不是很大。 表7-導磁率及功率損失2KG磁通密度,浸0.75#鐵心-塗覆 因數 690〇F 715〇F 730°F 750〇F 750〇F 760〇F 760〇F 770°F 780°F 800T 瓦# 8.66 7.19 7.99 11.11 9.56 9.97 11.28 10.5 11.84 22.87 導磁 7.639 7.721 6.354 3.284 2.534 3.223 2.233 1.849 1.128 382 用於表5之說明也適用於表7。然而,表7(本發明之 塗覆)及表3 (未塗覆)之比較顯示一清楚差異,其係由其等 效圖看得明’即第12及10圖看出。這些圖顯示功率損失 對於塗覆鐵心係減少’及對於已塗覆鐵心相較於未塗覆鐵 心時,導磁率對2KG功率損失較少之消散。因為導磁率及 功率損失應相反於結晶區之關係’所以當觀察塗覆鐵心 時,用於未塗覆鐵心之其他功率損失及消散係由於其他事 項。 這些差異對於已塗覆及未塗覆鐵心於浸潰前並不明 顯,可以比較第1 7圖(未塗覆)及第1 9圖(已塗覆)看出。 第1 7及1 9圖顯示大約等於鐵心損及消散。只有當浸漬應 第32頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) ---11 ----^ I ------I · LI (請先閱讀背面之注意事項再填寫本頁) . 經濟部智慧財產局員工消費合作社印製 508595 A7 B7_ 五、發明說明() 力出現時,除了差異出現之結晶成份外。 若多數功率損失於溫度增加時是因為增加之結晶,則 未塗覆導磁對功率損失應顯示平滑向下趨勢。然而,因為 於未塗覆資料係相較於可以形成簡單結晶作用有更多消 散,所以由於相較於已塗覆鐵心之較大浸潰應力,其他功 率損失必定較大。 結論是符合於未浸潰鐵心間之差異的缺少及當回火 溫度增加時,對於已浸潰鐵心之差異更小。於浸潰應力保 持不變而不管回火溫度時,應力之結晶分量隨著回火溫度 增加而變大。因此,對於已浸潰鐵心,差異緩慢移動至對 功率損失較高之結晶,於較高之回火溫度。注意的是,對 於已塗覆及已浸潰鐵心,於800°F沒有大量改良。 (請先閱讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製 表8-導磁&回火溫度CF)-浸潰0.75#鐵心未塗覆 溫度°F 0.1 Oe O.SOe l.OOe 2.0Oe 3.0Oe 4.0Oe S.OOe 平均 690 7885 9794 6516 4088 3085 2500 2125 5142 715 5810 9047 6308 4109 3154 2573 2191 4742 730 2490 6640 5022 3362 2601 2117 1818 3435 750 2490 5561 4544 3268 2594 2153 1884 3213 760 1245 3486 3237 2573 2144 1836 1619 3306 770 830 2158 2407 2075 1785 1556 1411 1746 780 415 996 1287 1328 1245 1152 1071 1070 800 415 166 249 353 408 384 386 337 第33頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 A7 B7___ 五、發明說明() (請先閱讀背面之注意事項再填寫本頁) 於表8中之導磁率係由表4之中資料計算,對於每一 溫度及驅動位準之組合成為量測為已知驅動位準之磁通 密度。注意於第 13 圖之 73 0 °F之下凹。對於 METGLAS2605SA1,730°F為5小時回火之結晶設定之估 計理論溫度。第13圖顯示由O.lOe至5.0Oe之相當穩定 導磁範圍轉換至相當陡斜坡,由約 75 0 °F或略高溫度開 始。該平均值係相當線性於超出750°F時,於對數導磁率 對溫度圖中。導磁率同時改變相當缓慢於超出〇. 1 〇e至 5.OOe範圍及750°F以上,除了於很低O.lOe位準之異常 夕卜。磁化曲線係由”圓”改變為”扁平"環於730至750°F範 圍中。表4及第9圖顯示此相同作用。 表9-導磁&回火溫度(°F)-浸潰0.75#鐵心塗覆 溫度。F O.lOe O.50e l.OOe 2.0Oe 3.0Oe 4.0Oe 5.0Oe 平均 690 5395 8300 5810 3818 2919 2386 2042 4381 715 5810 8300 5935 3901 2988 2449 2083 4494 730 3735 6806 5106 3486 2711 2241 1934 3717 750 1245 3403 3071 2386 1978 1702 1502 2184 760 1107 2684 2601 2158 1844 160 1450 1921 770 830 1660 1878 1743 1563 1390 1270 1475 780 414 747 1038 1141 1093 1017 963 916 800 415 166 291 353 374 374 382 336 經濟部智慧財產局員工消費合作社印製 於表9中之導磁率係由表6之資料所計算出,用·於每 第34頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 A7 B7 五、發明說明() 一溫度及驅動位準之組合’於磁通密度對已知驅動位準之 比。於表8中注意,7 3 0 F之下凹’已經被於表9中之有 限傾向向下所替換。見第14圖。本發明之塗覆係協助以 於略低溫度遷移。於第1 4圖中之對數-導磁率對溫度圖之 隔阿瑞尼本質係較於第13圖中明顯,並開始較快些,即 740T。所有其他觀察係由表8完成均適用於表9中。 較大2 · 5 #鐵心顯示相同於較小〇 · 7 5 #鐵心之傾向,略 不同飽和電感及導磁規格作用。 表1Q配合於2〇KHz及2KG,及用於資料收集點之$ 個溫度所取之功率損失資料’其係由6 9 0 °F開始,結束於 800T。〇·75磅(#)鐵心被使用。2.5磅鐵心係顯示類似之 結果。 -n ϋ In n n n an Mmmmatm lap emm§ emmmmm I 一 0 mmm— el (請先閱讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製508595 A7B7 V. Description of the invention () (Please read the notes on the back before filling this page) A large number of 690-7 1 ° F and 73 0-745 ° F to ensure the observations completed by the first group. The core has a gross weight of about 0.1 pounds. Subsequent testing of small cores confirms the important conclusions achieved by testing in smaller groups over a larger temperature range. The magnetic permeability parameter is the slope from the zero flux point to the defined flux level due to the zero drive on the magnetization curve. Table 4. Magnetization curve core flux (KG)-immersed with 0.75 # core uncoated drive 690 715 730 750 750 760 770 780 800 800 TT ° F Τ ° FTT ° F ° F ° F 0. 1 0.79 0.58 0.30 0.25 0.25 0.12 0.08 0.04 0.04 0.04 0.5 4.9 4.52 j. J Z 2.9 1 2.66 1.74 1.08 0.50 0.08 0.08 1.0 6.52 6.3 1 5.02 4.73 4.36 3.24 2.4 1 1.29 0.25 0.25 2.0 8.18 8.22 6.72 6.72 6.35 5.15 4.14 2.66 0.7 1 0.7 1 3.0 9.25 9.46 7.80 7.93 7.64 6.43 5.35 3.74 1.3 3 1.12 4.0 10.00 10.29 8.47 8.76 8.4 7 7.35 6.23 4.6 1 1.58 1.49 5.0 10.62 10.96 9.09 9.55 9.30 8.09 7.06 5.35 1.99 1.87 (De) Cube Cube Cube Cube Cube Circle Cube Circle Cube Circle Cube Circle Smart Property All measurements shown in Table 4 printed by the Bureau ’s Consumer Cooperative are done using a magnetic metal constant current flux reset tester (CCFR), which adjusts the appropriate core cross-sectional area and path length to complete a calibration pass Measurement level, unit is thousand Gauss and drive unit is Oster. In addition, the flux density is adjusted to match the saturation level of 1 5.9 thousand Gauss, except for the coated and uncoated treatment of METGLAS 2605SA1 on page 29. This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) B7 V. Explanation of the invention () Except the result. (Please read the precautions on the back before filling out this page) Table 4 and related Figure 9 show that the approximate decreasing magnetization curve becomes the tempering temperature increasing from 690 to 800 ° F. Furthermore, there are no other square-ring interaction systems in this data that are obvious, except for 690T, 71 5 卞 and 730 卞 data which are used as longitudinal "square-ring" magnetized cores. This result is the result of the immersion stress, because the square system is strongly proved in the prepreg data, that is, the core flux range is from not less than 15KG to 15.9KG, from 30e to the maximum drive 50e for the above temperature. See Figure 16, which shows the magnetization curve for an unimpregnated 0.75 pound uncovered range of 690 卞 to 800T. I believe the reason for this effect is that stress reduces the permeability. See Bo Wo's' 'Ferromagnetism' IEEE Bulletin (Chapter 13, Stress and Magnetization). The applied equation is -l = Bls2 / gs, where 0 is the initial permeability, Is is the magnetization per unit volume when saturated, which is proportional to the saturation magnetic flux density, s is the saturation magnetic limit, and i is Internal stress in a single area. Because the saturation magnetic limit for the 2605SA1 is large, i.e., 27 ppm, a work with smaller immersion stress may be quite large. Table 5 Magnetic permeability and power loss 2KG magnetic flux density, immersion 0.75 # iron core-uncoated factor 690F 715〇F 730T 750T 750 ° F 760T 770〇F 780T 800 ° F 80G ° F Watt # 16.73 10.38 26.99 16.48 10.83 17.50 16.42 17.51 20.56 26.36 Magnetic permeability 9.176 8.198 6.096 5.499 5.115 3.413 2.362 1.315 398 374 The magnetic permeability printed in Table 5 by the Consumers' Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs is calculated in the 2 thousand Gauss magnetic flux, based on the information in Table 4 Calculate. The core loss is measured at 20KHz and 2KG. Page 30 This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 508595 5. Description of the invention () (Please read the precautions on the back before filling This page) is used in the testing machine described below and Figure 6. The test conditions for the 2KG power measurement of this iron core are: 4 3 · 9 volts using a 10-turn solenoid coil. The information used for this test is plotted in Figure 10. The power loss is typically higher than the unimpregnated core. Figure 17 is equivalent to Figure 10 for 690 to 800 unimpregnated 0.75 # cores. Note the increased power dissipation for immersed uncut cores. Table 6. Magnetization curve core flux (KG)-immersion 0.75 # core coating drive 690T 715 ° F 730 ° F 750 ° F 760 ° F 760T 760T 770T 780T 800 ° F 0.1 0.54 0.58 0.37 0.12 0.12 0.12 0.08 0.08 0.04 0.04 0.04 0.5 4.15 4.15 3.40 1.70 1.33 1.86 1.04 0.83 0.37 0.08 1.0 5.81 5.93 5.10 3.07 2.49 3.07 2.24 1.87 1.04 0.29 2.0 7.60 7.80 6.97 4.77 4.23 4.86 3.88 3.49 2.28 0.71 3.0 8.76 8.96 8.13 5.93 5.48 6.06 5.06 4.69 3.28 1.12 4.0 9.55 9.79 8.96 6.81 6.39 6,97 5.89 5.56 4.07 1.49 5.0 10.21 10.42 9.67 7.51 7.39 7.72 6.64 6,35 4.81 1.91 (De) Fang Fang Fang Fang Fang Fang Fang Fang Yuan Fang Yuan Yuan YuanThe Ministry of Economic Affairs Intellectual Property Bureau Employee Consumption Cooperatives printed the instructions for use in Table 4 The same applies to Table 6. The coating of the present invention seems to have a slightly greater effect on making a circle or flattening than an uncoated core, depending on the temperature. However, the difference is too small to be noticed by the stress experienced by the core. Equivalent data for unimpregnated cores also show no significant differences between coated and uncoated cores. The difference appears only when the permeability and power loss are considered a crystallization. On page 31 in page 18, the paper size is in accordance with Chinese National Standard (CNS) A4 (210 X 297 mm) 508595 A7 B7 V. Description of the invention () Uncoated and coated iron core is very "square" 'For temperatures below 75 ° F and below' and temperatures at 760 ° F or above are "flat". The impregnation effect used to coat the iron core substantially reduces the magnetic permeability for each tempering temperature, except for 800 ° C. Preferably, the same effect system can be seen on the uncoated core, except that a higher saturation magnetic flux is caused by the tempering temperature of 15 ° F (higher than the tempering temperature of 690 ° F), compared to the unimpregnated temperature. Coated and uncoated cores. The difference between 690 T and 715 ° F is not so great for unimpregnated cores. Table 7- Permeability and power loss 2KG magnetic flux density, immersed 0.75 # iron core-coating factor 690F 715F 730 ° F 750F 750F 760F 760F 770 ° F 780 ° F 800T watts # 8.66 7.19 7.99 11.11 9.56 9.97 11.28 10.5 11.84 22.87 Magnetic permeability 7.639 7.721 6.354 3.284 2.534 3.223 2.233 1.849 1.128 382 The instructions used in Table 5 also apply to Table 7. However, the comparison between Table 7 (coated according to the present invention) and Table 3 (uncoated) shows a clear difference, which can be seen from its isograms, that is, Figs. 12 and 10. These graphs show that the power loss is reduced for the coated core system 'and for the coated core compared to the uncoated core, the permeability is less dissipated for the 2KG power loss. Because the permeability and power loss should be inverse to the relationship of the crystalline region ', other power losses and dissipations for the uncoated core when observing the coated core are due to other things. These differences are not obvious for coated and uncoated cores before immersion, and can be seen by comparing Figure 17 (uncoated) and Figure 19 (coated). Figures 17 and 19 show approximately equal core loss and dissipation. Only when impregnated should be on page 32. The paper size applies Chinese National Standard (CNS) A4 (210 X 297 mm) --- 11 ---- ^ I ------ I · LI (Please read the back first (Notes on this page, please fill out this page).. Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 508595 A7 B7_ V. Description of the invention () Except for the crystalline components where the differences appear. If most of the power loss is due to increased crystallization as the temperature increases, the power loss of the uncoated magnetically permeable pair should show a smooth downward trend. However, because uncoated materials dissipate more than simple crystals can form, other power losses must be greater due to the greater immersion stress compared to the coated core. The conclusion is that it is consistent with the lack of differences between unimpregnated cores and the smaller the difference between the impregnated cores as the tempering temperature increases. When the immersion stress remains constant regardless of the tempering temperature, the crystalline component of the stress becomes larger as the tempering temperature increases. Therefore, for immersed cores, the difference slowly moves to crystals with higher power loss and higher tempering temperatures. Note that for coated and impregnated cores, there is not much improvement at 800 ° F. (Please read the precautions on the back before filling out this page) Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 8-Magnetic permeability & tempering temperature CF) -Immersion 0.75 # Uncoated temperature of iron core ° F 0.1 Oe O .SOe l.OOe 2.0Oe 3.0Oe 4.0Oe S.OOe average 690 7885 9794 6516 4088 3085 2500 2125 5142 715 5810 9047 6308 4109 3154 2573 2191 4742 730 2490 6640 5022 3362 2601 2117 1818 3435 750 2490 5561 4544 3268 2594 2153 1884 3213 760 1245 3486 3237 2573 2144 1836 1619 3306 770 830 2158 2407 2075 1785 1556 1411 1746 780 415 996 1287 1328 1245 1152 1071 1070 800 415 166 249 353 408 384 386 337 Page 33 This paper is applicable to the Chinese National Standard (CNS) A4 specifications (210 X 297 mm) 508595 A7 B7___ 5. Description of the invention () (Please read the notes on the back before filling this page) The magnetic permeability in Table 8 is calculated from the data in Table 4. For each The combination of temperature and drive level becomes a magnetic flux density measured as a known drive level. Note the depression at 73 ° F in Figure 13. For METGLAS2605SA1, 730 ° F is the estimated theoretical temperature set by the 5-hour tempered crystallization. Figure 13 shows a fairly stable permeability range from 0.1Oe to 5.0Oe, transitioning to a fairly steep slope, starting at about 75 ° F or slightly higher. This average is reasonably linear over a logarithmic permeability versus temperature plot above 750 ° F. At the same time, the permeability changes quite slowly beyond the range of 0.10e to 5.OOe and above 750 ° F, except for abnormalities at very low 0.1Oe levels. The magnetization curve was changed from "circle" to "flat" ring in the range of 730 to 750 ° F. Table 4 and Figure 9 show the same effect. Table 9-Magnetic permeability & tempering temperature (° F)-immersion 0.75 # iron core coating temperature. F O.lOe O.50e l.OOe 2.0Oe 3.0Oe 4.0Oe 5.0Oe average 690 5395 8300 5810 3818 2919 2386 2042 4381 715 5810 8300 5935 3901 2988 2449 2083 4494 730 3735 6806 5106 3486 2711 2241 1934 3717 750 1245 3403 3071 2386 1978 1702 1502 2184 760 1107 2684 2601 2158 1844 160 1450 1921 770 830 1660 1878 1743 1563 1390 1270 1475 780 414 747 1038 1141 1093 1017 963 916 916 800 415 166 291 353 374 374 382 336 Economy The magnetic permeability printed in Table 9 by the Consumers ’Cooperative of the Ministry of Intellectual Property Bureau is calculated from the data in Table 6, and it is used in accordance with the Chinese National Standard (CNS) A4 specification (210 X 297) per page 34. (Centi) 508595 A7 B7 V. Description of the invention (1) A combination of temperature and driving level 'in the ratio of magnetic flux density to a known driving level. Note in Table 8 that the concave under 7 3 0 F' has been used in The limited tendency in Table 9 is replaced downward See Figure 14. The coating system of the present invention assists in migrating at slightly lower temperatures. The logarithmic-permeability versus temperature map in Figure 14 shows that the Arrhenian nature is more apparent than in Figure 13 and begins Faster, that is, 740T. All other observations completed from Table 8 are applicable to Table 9. The larger 2 · 5 # iron core shows the same tendency as the smaller 0 · 7 5 # iron core, with slightly different saturation inductance and magnetic permeability. Specifications and functions: Table 1Q is used at 20KHz and 2KG, and the power loss data taken from the $ temperature used for the data collection point, which starts at 690 ° F and ends at 800T. 0 · 75 pounds (# ) Iron core is used. 2.5 pound iron core shows similar results. -N ϋ In nnn an Mmmmatm lap emm§ emmmmm I-0 mmm — el (Please read the precautions on the back before filling out this page) Staff of the Intellectual Property Bureau of the Ministry of Economic Affairs Printed by Consumer Cooperatives

本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 訂·This paper size applies to China National Standard (CNS) A4 (210 X 297 mm).

508595 A7 B7 五、發明說明() 770圓 4.63 4.54 10.5 16.42 10.7一一_ 16.18 34% 780圓 7.52 5.74 11.84 17.51 — 11.36 18.19 38% 800正方 21.24 20.56 一----- 13.63 16% 800圓 23.21 21.24 22.87 26.36 ——---- 13.29 17.87 被標示為正方之回火條件表示7 5安培直流係流經鐵 心窗口,藉以創造一實質縱長磁場於"JE方”磁化曲線回 火。回火條件被標示為圓,表示於電流流經鐵心之窗口, 沒有磁場作回火用。於完成730卞回火條件之”無資料,,係 由損失鐵心造成。用於每一回火溫度範園之指示百分比改 良係圓及正方條件之平均,若兩者都有的話。若以6 9 0 T 至8 0 0 °F範圍作為全部的話,有總數3 0 %之改良。 鐵心之視在導磁率係為間隙(若有間隙的話)之尺寸所 強烈影響如下: Ι/a丨f=l/i + g/p,其中aff=鐵心有效或量得導磁率,1 =測 試條件下,鐵心材料之固有導磁率,即磁通及頻率,g =總 間隙,p =於鐵心内磁通方向之平均路徑長度。注意alf=i, 當間隙為零時。於CGS系統中導磁率係無單位。公式降低 至alf^i/^l+g/pXi),其中g及p為具有相同大小。則等於alt、 Ρβ,當 g/p>>l 時。508595 A7 B7 V. Description of invention () 770 round 4.63 4.54 10.5 16.42 10.7 one one _ 16.18 34% 780 round 7.52 5.74 11.84 17.51 — 11.36 18.19 38% 800 square 21.24 20.56 one ----- 13.63 16% 800 round 23.21 21.24 22.87 26.36 -------- 13.29 17.87 The tempering conditions marked as square indicate that the 75 ampere DC system flows through the core window, thereby creating a substantially longitudinal magnetic field tempered on the "JE square" magnetization curve. Tempering conditions It is marked as a circle, which means that the current flows through the window of the iron core, and there is no magnetic field for tempering. The "no data" at the completion of the tempering condition of 730 卞 is caused by the loss of the iron core. The percentage of indication used for each tempering temperature Fan Yuan is the average of the round and square conditions, if both are available. If the range of 6 9 0 T to 8 0 ° F is taken as the whole, there is a total improvement of 30%. The apparent permeability of the core is strongly influenced by the size of the gap (if there is a gap) as follows: Ι / a 丨 f = l / i + g / p, where aff = core is effective or the permeability is measured, 1 = test Under the conditions, the inherent permeability of the core material, that is, the magnetic flux and frequency, g = total gap, p = average path length in the direction of the magnetic flux in the core. Note that alf = i, when the gap is zero. Permeability in the CGS system is unitless. The formula is reduced to alf ^ i / ^ l + g / pXi), where g and p have the same size. Is equal to alt, pβ, when g / p > &l; l.

假設此間隙不確定性,用以量測未切割鐵心之導磁率 之CCFR儀器組對於已切割鐵心並不適當。同時,CCFR 並未對相當於2KG及20KHz之功率損失測試點之20KHz 頻率作校正。為了克服這些問題,一通用無線電1 630-AV 第36頁 本紙張尺度適用中國國家標準(CNS)A4規格(21G X 297公爱) --------r---·---裝 LI (請先閱讀背面之注意事項再填寫本頁) 訂* - 經濟部智慧財產局員工消費合作社印製 經濟部智慧財產局員工消費合作社印製 508595 - ~~——___- 五、發明說明() 電感量測組件係用以量測具有很小心控制間隙尺寸之小 塗覆C鐵心 < 電感。然而’於CCFR及電感橋間並沒有激 勵差。CCFR使用正弦波電流,及電感橋使用正弦波電壓。 於兩測试機盜間之激勵差將影響導磁率比較。橋量測導磁 率4略大於C C F R。然而,這些差並不認為足夠大以影響 由這些測試所得到結果之本質。 以下公式係用以計算給定電感及已知間隙之# ··Assuming this gap uncertainty, the CCFR instrument set used to measure the permeability of the uncut core is not appropriate for the cut core. At the same time, CCFR has not corrected the 20KHz frequency equivalent to the power loss test points of 2KG and 20KHz. In order to overcome these problems, a general radio 1 630-AV page 36 This paper standard applies to China National Standard (CNS) A4 specification (21G X 297 public love) -------- r --- · --- Install LI (Please read the notes on the back before filling this page) Order *-Printed by the Employees 'Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs Printed by the Employees' Cooperatives of the Ministry of Economics and Intellectual Property Bureau Printed by 508595-~~ ——___- V. Description of the Invention () Inductance measurement module is used to measure small coated C core < inductance with carefully controlled gap size. However, there is no excitation difference between CCFR and the inductor bridge. CCFR uses a sine wave current and the inductor bridge uses a sine wave voltage. The difference in excitation between the two testers will affect the comparison of permeability. The magnetic permeability 4 measured by the bridge is slightly larger than C C F R. However, these differences are not considered large enough to affect the nature of the results obtained from these tests. The following formula is used to calculate the given inductance and the known gap #

Al/(4x1(^XN2xAgif/-g),其中 n 為圈轉數,Agif 為鐵〜有效面積,單位平方公分,# =鐵心之電感,單位 為予利’及g(先前定義)以公分表示。如前所述,i於CGS 系統中沒有單位尺寸,以報告該資料。 用以计弄各間隙之公式包含配合表面間隙。所有導磁 率計算係完成於2KG及20KHz,使用50圈線圈,對稱地 放置於兩間隙上,以減少發火效應。因此,結果係可以比 較於相同條件下之鐵心損失量測。所得導磁之計算值係使 用回歸技術被套用至直線,以估計材料導磁率作為”yn阻 斷’相當於零間隙。隨附功率損失資料係被如上量測。以 下資料顯示用於〇 · 1磅” c ”鐵心之結果。 表11比較芜成〇 · 1磅,,C ”鐵心之導磁率及功率損失, 該鐵心係被回火及塗覆於6 9 0 T四小時,使用用於,,正方環 π要件之標準處理條件。該表比較標準”正方環”及”圓環”。 於表1 1中之導磁率估計係於切割後,使用一回歸技術加 以取得’並應用所計算導磁率對所量出之間隙。導磁率計 算係完成於各種間隙,並使用一標準公式配合一線性回歸 第37頁 V紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 〜 --------iM 裝 II (請先閲讀背面之注意事項再填寫本頁) « ·Al / (4x1 (^ XN2xAgif / -g), where n is the number of revolutions, Agif is iron ~ effective area, in square centimeters, # = inductance of the iron core, the unit is Yuli 'and g (previously defined) is expressed in centimeters As mentioned earlier, i does not have a unit size in the CGS system to report this information. The formula used to calculate each gap includes the mating surface gap. All magnetic permeability calculations are completed at 2KG and 20KHz, using 50 turns of the coil, symmetrical It is placed on the two gaps to reduce the ignition effect. Therefore, the result can be compared with the core loss measurement under the same conditions. The calculated value of the magnetic permeability is applied to a straight line using regression technology to estimate the magnetic permeability of the material as " yn blocking 'is equivalent to zero clearance. The accompanying power loss data was measured as above. The following data shows the results for a 0.1 pound "c" core. Table 11 compares Wu to 0.1 pound, C "core Magnetic permeability and power loss, the core is tempered and coated at 690 T for four hours, using the standard processing conditions for the square ring π requirements. The table compares the standard "square ring" and "ring" "At Table 1 1 The permeability estimation is obtained after cutting, using a regression technique to obtain the calculated permeability, and applying the calculated permeability to the measured gap. The permeability calculation is completed in various gaps, and a standard formula is used in conjunction with a linear regression. V paper size applies Chinese National Standard (CNS) A4 specification (210 X 297 mm) ~ -------- iM Pack II (Please read the precautions on the back before filling this page) «·

508595 A7 B7 五、發明說明() 線。所得回歸線係被外插至零間隙,以提供用於圓及正方 環之導磁率估計(於切割後)如於表1 1所示。注意,於切割 處之導磁率施加至平均5鐵心,用於每群中,以改良估計 準確性。 於表1 2中之間隙量測係捨去三個地方。正確性是必 要的,使得可以產生由回歸分析計算最接近值。諸間隙係 使用一光比較器實際檢查至 0.0001 "。所得資料係被回歸 技術所調整,而不大於正確性限制。此調整係被完成以取 得最佳可能配合。第20圖示出所得回歸線及相當於表1 2 之資料。 ---------ί---ί — --- (請先閱讀背面之注意事項再填寫本頁) 表11.於切割前後導磁率及功率損失比較-0.1#鐵心 條件 導磁率 鐵心損失(瓦) 切割前 切割後 切割前 切割後 正方形環 5142 ±847 4782 8.55±1.20 8.91 ±4.04 圓形環 4914±1193 4298 8.82±0.81 9.13±1.59 · !線. 經濟部智慧財產局員工消費合作社印製 於切割前之導磁率及鐵心損資料係於浸潰後取得,每 一條件為1 0鐵心之平均值。於切割後導磁率資料係於完 成鐵心階段,並且每一條件為5鐵心之平均值。於切割前 之導磁資料係使用CCFR測試機於400HZ加以取得。於切 割後之導磁資料係使用電感橋於20KHz加以取得。±xxxx 為3x(標準偏差)。所有鐵心被以標準690°F回火條件下之 南萊處理。 第 38"M* 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 經濟部智慧財產局員工消費合作社印製 五、發明說明(508595 A7 B7 V. Description of the invention () line. The obtained regression lines are extrapolated to zero gap to provide the permeability estimates (after cutting) for circles and square rings as shown in Table 11. Note that the permeability at the cut is applied to an average of 5 cores and used in each cluster to improve the estimation accuracy. The gap measurements in Table 12 are rounded down to three places. Correctness is necessary so that the closest value calculated by regression analysis can be generated. The gaps are actually checked to 0.0001 " using an optical comparator. The information obtained is adjusted by regression techniques and is not greater than the limit of accuracy. This adjustment is done to get the best possible fit. Figure 20 shows the obtained regression line and the data corresponding to Table 12. --------- ί --- ί — --- (Please read the notes on the back before filling this page) Table 11. Comparison of Permeability and Power Loss Before and After Cutting -0.1 # Permeability of Iron Core Condition Core Loss (Watts) Before Cutting After Cutting After Cutting Before Cutting After Cutting Square Ring 5142 ± 847 4782 8.55 ± 1.20 8.91 ± 4.04 Round Ring 4914 ± 1193 4298 8.82 ± 0.81 9.13 ± 1.59 ·! Line. Intellectual Property Bureau, Ministry of Economic Affairs, Consumer Consumption Cooperative The magnetic permeability and core loss data printed before cutting are obtained after immersion, and each condition is the average of 10 cores. The magnetic permeability data after cutting are at the core completion stage, and each condition is the average of 5 cores. The magnetic permeability data before cutting were obtained using a CCFR tester at 400HZ. The magnetic permeability data after cutting were obtained at 20KHz using an inductive bridge. ± xxxx is 3x (standard deviation). All cores were treated in Nanlai under standard tempering conditions of 690 ° F. Article 38 " M * This paper size applies to China National Standard (CNS) A4 (210 X 297 mm) 508595 Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs

調璧 量測間隙(密 耳) 突出沒有間 隙 0.6 5 (配合間 隙) 2.4 (琥珀片 2_ 3.2 (紫片)璧 Measurement gap (mil) Protruding without gap 0.6 5 (fitting gap) 2.4 (amber 2_ 3.2 (purple)

用於圓環,正 突出沒間隙資料裔 段。注意對調整間 誤差。 第20圖以圖, 鼻得之材料導磁率 A7 B7It is used in the circle, and it highlights the gapless data segment. Note the error between adjustments. Figure 20 shows the magnetic permeability of the material obtained from the nose A7 B7

视在; 时料導磁率-0 .丨#鐵心 g ^) 調整間隙(公分) 圓環 正方環 0 4298 4 7 82 0.00165 5490 8692 一 0.00608 一…_ 1 1 1 0823 1 8 3 3 9 0.00806 1 3224 2 1808 0.00940 ------- 1 2322 26757 万環之回歸係數分別為0.92及〇·99。 用以導磁率估計於表1之”切割後,,階 隙未超出0·1密耳之回歸變動也是量測 /方式再生表12,示出回歸重疊。所計 並不保持不變,因為有兩個間隙改變之 理由。首先,用於好土,% / 、材枓導磁率計算係如先前所討論特別敏 感於間隙尺寸。因為不可能量測間隙至所需精確度,所以 回歸史動技術係用以調整間隙之不確定性。第二,邊緣磁 通傾向於造成’於間隙成比例於增加時,電感成比例增 加。這是一已有記錄之作用,電感器設計者必須加以考量 的。 然而,用以計算於表12中之導磁率之簡單公式並未 將複雜之邊緣磁通作用列入考慮。因為邊緣磁通之作用係 增加電感值’並當當間隙加大時,也有增加計算材料導磁 率之作用。這就是為何需要回歸分析之主要理由,因為否 第39頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) (請先閱讀背面之注意事項再填寫本頁)Apparent; Magnetic permeability of the material-0. 丨 # 铁心 g ^) Adjust the gap (cm) Ring square ring 0 4298 4 7 82 0.00165 5490 8692 One 0.00608 One ..._ 1 1 1 0823 1 8 3 3 9 0.00806 1 3224 2 1808 0.00940 ------- 1 2322 26757 The regression coefficients of the ring are 0.92 and 0.99, respectively. The magnetic permeability is estimated in Table 1 after "cutting, and the regression variation in which the step gap does not exceed 0 · 1 mil is also measured / reproduced in Table 12, showing the regression overlap. The calculation does not remain the same, because there is Two reasons for the gap change. First, for good soils, the% /, material permeability calculation system is particularly sensitive to the gap size as previously discussed. Because it is not possible to measure the gap to the required accuracy, historical regression techniques It is used to adjust the uncertainty of the gap. Second, the edge magnetic flux tends to cause 'the inductance increases proportionally when the gap is proportional to the increase. This is a documented effect that inductor designers must consider. However, the simple formula used to calculate the permeability in Table 12 does not take into account the complex edge magnetic flux effect. Because the effect of the edge magnetic flux is to increase the inductance value, and it is also increased when the gap is increased. The role of magnetic permeability of materials. This is the main reason why regression analysis is needed, because no. The paper size on page 39 applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) (Please read first Note the surface to fill out this page)

A7A7

五、發明說明() 則將不可能知道邊緣錯誤作用之斜率。回歸技術允許材料 導磁率之估計,藉由減少之作用大小之突出至零間隙。 書霜處理以改良效能 由本發明所提供之改良係主要在於功率損失降低,其 係漸進地發生。沒有塗層就不會有改良。一薄塗層造成較 佳功率損失改良於"沒塗層”狀態,由於略微渦流降低之 故。當塗層漸進地增加時’首先由於塗層厚度快速增加, 其他改良快速發生。於此階段,渦流快速消失,當塗層電 阻隨厚度增加時。然而,於一些點上,塗層厚度較慢速增 加。當此發生時效能改良也同時變緩,因為厚度不再增加 及渦流到達一平衡狀態。這是用於成長處理之取決於基材 之一般” Sπ曲線。於此時,金屬材料提供鐵給塗層作為絕 緣氧化鐵。 結晶作用係同時與時間有關的,因為”設定作用”。因 此,若回火係於塗覆處理範圍足夠長,則結晶開始。一旦 結晶開始,於所得效能負面作用,即導磁率降低,矯頑磁 性力及功率損失增加前,只是一時間問題。 因為塗層成長及結晶係由溫度所驅動,所以當溫度降 低至較佳低於500-600Τ之某一位準時,兩處理均減緩或 停止。此”冷凍,,一給定位準之改良成為塗覆產品,允許冷 康處理狀態之效能量測。這假設結晶未開始。 因此,利益首先增加,然後隨著時間及溫度之增加而 降低,依據於這些競爭作用間之複雜關係。例如’塗層可 第40頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) -------卜丨1丨1·裝.卜丨 (請先閱讀背面之注意事項再填寫本頁) 訂: 經濟部智慧財產局員工消費合作社印製 508595 A7 ---------— B7_____ 五、發明說明() 以漸地施加,藉由曝露至蒸汽及熱中,一第一時間段,隨 後及或多數後續蒸汽/加熱處理。導磁率及功率損 失之I測可以完成於連續塗層步驟之間。首先,將會有改 良,然後,當渦流減少之競爭力減少時,及結晶工作彼此 相對抗。這是清楚地可決定對於已知導磁率之安全時間及 度範圍,功率損失要件。因為主要限制因數為結晶設 疋,所以於任一給定溫度之處理時間量可以加以由圖中估 計出。例如690-7 1 5 T,使用窩法第6章中之表,可以估 計於METGLAS2605SA1開始之結晶設定前,有1〇-15小 時回火可用。這允許丨至2次一般處理條件重覆5小時功 率損失之”爬昇”,用於正方環處理。 結果,右因為材料變化,一第一塗覆處理並不產生具 有想要特性之鐵心,一或多數其他處理時間有時可以用以 改良塗覆鐵心之效能至想要程度。當然,如上所注意,每 一額外處理應於材料之限制内,以使得結晶作用並未超出 其他處理足利盈所在。量測及重覆處理必須發生於浸潰 前。 以下表示出此減少係如何實現。該資料係取於磅 環形,由METGLAS2605SA1作成,並設計以用於很高功 率變壓器組件中。資料報告堆疊電阻改良為69〇τ進行六 小時之第一塗層之結果,隨後,冷卻及電阻量測,然後, 第二塗覆處理於690Τ6小時,或包含原始處理之總數12 小時。增加堆疊電阻係大致相關於帶鐵心之改良。 第41頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) ,裝 (請先閱讀背面之注意事項再填寫本頁) ·. 經濟部智慧財產局員工消費合作社印製 508595 A7B7 五、發明說明() 表13-40磅METGLAS2605SA1環之直流堆疊電阻 鐵心號 第一-6小時塗覆處理堆疊 第二-6小時(總數12小時)塗覆處理堆疊 24 314 880+180% 26 267 347+30% 29 295 841+185% 30 130 546+320% 31 356 836+135% 32 1456 1295-11% 33 814 1603+97% 34 965 2031+110% 35 869 1485+71% 36 996 2192+120% 38 769 1596+108% 39 715 1704+138% 40 915 2645+189% 41 534 2095+292% 42 721 2218+2-8% 43 530 885+29% 44 1200 1490+24% 45 1238 1413+14% 平均變化 + 124%淨平均改良 (請先閱讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製 1 2 4%淨平均改良係重大的。於1 8個再處理中只有1 部份略微降低,即-1 1 %。 第42頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 A7 B7 五、發明說明() 例子 以下例子示出本發明,於鐵心之優良特性可以由本發 明處理加以產生。 對於以下例子中,於C鐵心中之功率消散係藉由連 接,一電壓電流瓦(v - A - W)表(紐約之克拉克賀氏數位公司) 及一 2MHz之函數產生器(芝加哥,麥克特國際公司,型號 BK Presion 3011B)’至一千瓦放大器(由加州聖地牙哥之 儀器公司型號LB)以控制輸出,整形及振幅頻率及將之量 測。具有可變大小及頻率之正弦波然後經由兩可能多圈之 一被施加至該C鐵心。諸線圈繞於C鐵心並連接至千瓦放 大器之輸出接面。施加至鐵心之典型量測條件係取決於想 要通量,及代表例係如下: (請先閲讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製 用於C鐵心功率量測之電氣設定條件 頻率(KHz) 激勵電壓(伏) 所需通量(KG) 所需圈數 0.4 14.6 2.0 50T 0.4 36.6 5.0 50T 0.4 72.6 10.0 50T 0,4 109 15 50T 1.0 3.6 2.0 5T具有降壓變壓器 1.0 9.26 5.0 5T具有降壓變壓器 10.0 36.6 2.0 5T ______ —«—-- 20.0 73 2.0 5T _ 上述組合並不是特有的,其必須加以選擇&達到所需磁通量位準 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 A7 ----_---— B7 ____ 五、發明說明() "一 ' ^ 這些位準係使用精確函數產生器,加以設定,藉由使 7函數產生器之讀出值,mw I之電壓讀取顯示設 疋加以,又疋V_A-W錶直接量測鐵心功率損失及激勵電 >瓦’使用功率量測及電流量測設定。 為了量測脈衝環之功率消散,一脈衝產生器(惠普型 214A),一高功率脈衝產生器(史丹佛之庫柏電子公司之型 號6〇8))及一調整電源(紐澤西州,巴克利高地之哈利森^ 驗1:型號814A)係被連接至一真空管脈衝器,以控制其輸 出上升時間,工作週期及用於重覆脈衝條件之振幅。真空 管脈衝器係連接至高安培纜線之3圈線圈,其係被繞於 環形件上。設定被絕緣,因為產生高壓。一示波器(菲利 普型號PM3323 50DMS/S具有30kv探針)係被用以記綠脈 衝形狀,鐵心激勵分佈及整合功率反應於記憶體中。對於 脈衝寬度典型量測範圍由1.5至3.〇微秒,於直流重置上 之15-20安培轉,具有脈衝器調整,以完成1-4泰斯拉磁 通於鐵心中。脈衝測試設備係例示於第6圖中。 例子1 降低功率損失 例如具有約大於70%鐵之METGLAS2605SA1之非晶 金屬合金之纏繞鐵心係同時回火,然後,被以蒸汽(pH8) 及3 65。(69 0°F )空氣處理6小時,以於鐵心之相鄰金屬帶 層間形成鐵金屬氧化物絕緣材料。兩群鐵心被形成。第一 群包含每一重约5磅之鐵心,及第二群包含每一重約1磅 第44頁 本紙張尺度翻巾目目家鮮(CNS)A4祕(21G X 297公釐) '' I-----------ί ^ * l· I (請先閱讀背面之注意事項再填寫本頁} 訂··5. Description of the invention () It will be impossible to know the slope of the edge error effect. The regression technique allows the estimation of the permeability of the material to be reduced to zero clearance by reducing the magnitude of the effect. Book frost treatment to improve performance The improvement provided by the present invention is mainly due to a reduction in power loss, which occurs gradually. There is no improvement without a coating. A thin coating results in better power loss improvement in the "uncoated" state due to a slight decrease in eddy current. When the coating gradually increases' first because the coating thickness increases rapidly, other improvements occur quickly. At this stage The eddy current quickly disappears when the resistance of the coating increases with the thickness. However, at some points, the thickness of the coating increases slowly. When this occurs, the performance improvement also slows down at the same time, because the thickness no longer increases and the eddy current reaches a balance. State. This is the general "Sπ curve" of the substrate used for the growth process. At this time, the metallic material provides iron to the coating as the insulated iron oxide. Crystallization is also time-dependent because of "setting effect". Therefore, if the tempering is sufficiently long in the coating treatment range, crystallization starts. Once crystallization has begun, it is only a matter of time before the negative effects of the obtained efficiency, that is, the decrease in magnetic permeability and the increase in coercive force and power loss. Because coating growth and crystallization are driven by temperature, when the temperature is lowered to a level that is preferably below 500-600T, both processes are slowed or stopped. This "freezing," a modification of the positioning accuracy into a coated product, allows the performance measurement of the cold treatment state. This assumes that crystallization has not started. Therefore, the benefits increase first, and then decrease with time and temperature increase. The complex relationship between these competing effects. For example, 'The coating can be page 40. The paper size is applicable to the Chinese National Standard (CNS) A4 specification (210 X 297 mm). . Bu 丨 (Please read the notes on the back before filling this page) Order: Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 508595 A7 ---------— B7_____ V. Description of the invention () Application, by exposure to steam and heat, for a first time period, followed by or most subsequent steam / heating treatments. Measurements of permeability and power loss can be completed between successive coating steps. First, there will be improvements Then, when the eddy current decreases, the competitiveness decreases, and the crystallization work opposes each other. This is clearly to determine the safety time and degree range and power loss requirements for the known permeability. Because the main limiting factor is the crystallization design Therefore, the amount of processing time at any given temperature can be estimated from the graph. For example, 690-7 1 5 T, using the table in Chapter 6 of the method, it can be estimated that there is 1 before the crystallization setting at the beginning of METGLAS2605SA1. 〇 15 hours of tempering is available. This allows 丨 to 2 times of general processing conditions to repeat the "climbing" of power loss for 5 hours for square ring processing. As a result, because of the material change, the first coating treatment does not occur For iron cores with desired properties, one or most other processing times can sometimes be used to improve the effectiveness of the coated core to the desired level. Of course, as noted above, each additional treatment should be within the limits of the material to allow crystallization It does not exceed the other processing margins. Measurement and repeated processing must occur before immersion. The following shows how this reduction is achieved. The data is taken from the pound ring, made by METGLAS2605SA1, and designed to be used for very high In the power transformer assembly, the data report shows that the stacking resistance was improved to 69〇τ for the first coating of six hours. Then, the cooling and resistance measurements were performed, and then, the second coating was applied. 690T 6 hours, or a total of 12 hours including the original processing. Increasing the stacking resistance is roughly related to the improvement with a core. Page 41 This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm). (Please read the precautions on the back before filling this page) ·. Printed by 508595 A7B7, Employee Cooperative of Intellectual Property Bureau of the Ministry of Economic Affairs 5. Description of the invention () Table 13-40 lbs. METGLAS2605SA1 ring DC stacking resistor core No. 1-6 Hours of coating treatment stack 2-6 hours (total 12 hours) Coating treatment stack 24 314 880 + 180% 26 267 347 + 30% 29 295 841 + 185% 30 130 546 + 320% 31 356 836 + 135% 32 1456 1295-11% 33 814 1603 + 97% 34 965 2031 + 110% 35 869 1485 + 71% 36 996 2192 + 120% 38 769 1596 + 108% 39 715 1704 + 138% 40 915 2645 + 189% 41 534 2095 + 292% 42 721 2218 + 2-8% 43 530 885 + 29% 44 1200 1490 + 24% 45 1238 1413 + 14% average change + 124% net average improvement (please read the notes on the back before filling this page) Printed by the Consumer Property Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs of the 1 2 4% net average improvement is significant. Only one part of the 18 reprocessings decreased slightly, namely -1 11%. Page 42 This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 508595 A7 B7 V. Description of the invention () Examples The following examples show the invention. The excellent characteristics of the iron core can be produced by the treatment of the invention. . For the following example, the power dissipation in the C iron core is connected by a voltage and current watt (v-A-W) meter (Clark and Hess Digital of New York) and a 2MHz function generator (Chicago, McTe International company, model BK Presion 3011B) 'to one kilowatt amplifier (model LB from San Diego, Calif., Inc.) to control output, shaping and amplitude frequency and measure it. A sine wave having a variable size and frequency is then applied to the C core via one of two possible turns. The coils are wound around the C iron core and connected to the output connection of the kilowatt amplifier. The typical measurement conditions applied to the iron core depend on the desired flux, and the representative examples are as follows: (Please read the precautions on the back before filling this page) Printed for the C iron core by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs Electrical setting conditions for measurement Frequency (KHz) Excitation voltage (volts) Required flux (KG) Required turns 0.4 14.6 2.0 50T 0.4 36.6 5.0 50T 0.4 72.6 10.0 50T 0,4 109 15 50T 1.0 3.6 2.0 5T Voltage transformer 1.0 9.26 5.0 5T with step-down transformer 10.0 36.6 2.0 5T ______ — «—-20.0 73 2.0 5T _ The above combination is not unique, it must be selected & achieve the required magnetic flux level. This paper scale applies to China Standard (CNS) A4 specification (210 X 297 mm) 508595 A7 ----_---- B7 ____ V. Description of the invention () " 一 '^ These levels are set using precise function generators, By reading the value of the 7-function generator, the voltage reading and display settings of mw I are added, and the V_A-W meter directly measures the core power loss and the excitation power> Watt's use of power measurement and current measurement set up. In order to measure the power dissipation of the pulse ring, a pulse generator (HP type 214A), a high power pulse generator (Stanford Cooper Electronics Co., Ltd. model 608)) and an adjustment power supply (New Jersey, Harrison at Buckley Heights ^ Test 1: Model 814A) is connected to a vacuum tube pulsator to control its output rise time, duty cycle and amplitude for repeated pulse conditions. The vacuum tube pulsator is a three-turn coil connected to a high-amp cable, which is wound on a ring. The setting is insulated because high voltage is generated. An oscilloscope (Philip model PM3323 50DMS / S with 30kv probe) is used to record the green pulse shape, the core excitation distribution and integrated power are reflected in the memory. The typical measurement range for pulse width is from 1.5 to 3.0 microseconds, 15-20 amps on DC reset, with pulser adjustment to complete 1-4 Tesla magnetic flux in the core. The pulse test equipment is illustrated in FIG. 6. Example 1 Reduced power loss For example, a wound core of an amorphous metal alloy of METGLAS 2605SA1 with about 70% iron is tempered at the same time, and then steamed (pH 8) and 3 65 are used. (69 0 ° F) air treatment for 6 hours to form an iron metal oxide insulating material between the adjacent metal strips of the core. Two clusters of iron cores were formed. The first group contains iron cores weighing approximately 5 pounds each, and the second group contains iron cores weighing approximately 1 pound each. Page 44 Paper-size Folding Order Household Products (CNS) A4 (21G X 297 mm) '' I- ---------- ί ^ * l · I (Please read the notes on the back before filling this page} Order ··

經濟部智慧財產局員工消費合作社印製 508595 A7 B7 五、發明說明() 之鐵心。功率損失係正規化於兩群之間,藉由將功率損失 除以鐵心重量。 第二組鐵心包含兩群,其係由上述所完成,但並未受 到蒸汽及空氣處理。結果,此組鐵心缺乏氧化鐵絕緣,並 用以作為比較已處理鐵心功率損失之基礎。 正規化資料係示於以下表1 4中。 表14 > n n n n n (ϋ I^> am· MW 麵 · Hi I (請先閱讀背面之注意事項再填寫本頁) 比較已處理及未處理非晶鐵心之 功率損失為頻率之函數 已處理未處理鐵心之功率損失(瓦/磅) 頻率(KHz) 未處理 已處理 改良% 0.4 1.9 1.3 14 1.0 3.9 2.7 17 10.0 13 9.9 30 16.0 27 19 33 20.0 17 9.0 45 . %- 經濟部智慧財產局員工消費合作社印製 表1 4之資料展現以本發明方法處理之非晶鐵合金之 鐵心產生之鐵心,於高頻時具有較未處理鐵心低1 4-45% 之改良。即,於已處理鐵心中之功率損失減少由1 4 %至減 少45%。再者,於效能之改良隨著頻率增加而增加,如以 上所述。 一類似實驗係以由細結晶材料,例如70%Fe,9%B, 第45頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 五、發明說明() 3%Nb,2%Cu 及少量 Μ〇,。 、、她 C 〇及S加以形成之鐵心力ρ以執 行。這些鐵心係被回火於約53 8。〇(1〇〇〇下),冷卻至室溫, 然後,被處理以形成氧化鐵絕緣層。這些鐵心於功率上之 損失之減少係比較於未處理細結晶鐵心係類似於表14之 非晶金屬合金鐵心所看到者。 例子2 於脈衝測試中被以蒸汽及空氣處理之 鐵心與以甲基錳處理之鐵心之比較 磁心係由約1密耳厚非晶鐵帶,例如 METGLAS2605SA1所形成,作為環脈衝鐵心,具有19 7 公分(7· 75”)外徑,10.8公分(4.25”)内徑,及51.1公分(2,,) 厚。於纏繞前’鐵心係被塗覆以甲基錳,或於纏繞後以芙 汽/空氣處理,以形成氧化鐵絕緣層,或者都採用,如於表 1 5所述。 鐵心係藉由施加約8.6千伏,使用很低頻工作週期, 5圈一次,lOpps及由3微秒脈寬以2.85Τ磁通計算之脈衝 能量加以測試。脈衝資料量測包含鐵心功率(由鐵心所消 散之功率量),開始電流,及飽和電流。脈衝能量係然後 由脈衝曲線乘以電壓之面積加以計算,以取得功率之焦耳 量。於所有量測中,數量愈低,鐵心愈佳。再者,較佳地, 開始電流儘可能地接近飽和電流。測試結果係如於表1 5 所示。 第46頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) Γ清先閱讀背面之注音?事項再填寫本頁} 訂.· 經濟部智慧財產局員工消費合作社印製 508595 A7 B7 五、發明說明() —-Ϊm" 4u"·錳-5今汽/空氣處理之鐵心之脈衝資料 測試 處理 鐵心功率(千 瓦) 開始電流(安) 飽和電流(安) 脈衝能量 (焦耳) 1 浸油,甲基,蒸汽/空氣 201 20 38 0.75 2 甲基,蒸汽/空氣 204 20 40 0.77 3 光樹脂浸潰 287 30 50 1.0 4 重樹脂浸漬,蒸汽/空氣 331 30 60 1.2 5 浸油,蒸汽/空氣 196 22 32 0.7 6 甲基錳 200 20 40 0.8 --------.---.---裝·!.1 (請先閱讀背面之注意事項再填寫本頁) 所有π於表1 5之鐵心均非晶金屬合金,含鐵作為主 要金屬。對於測試1之鐵心,非晶金屬帶係被塗以很薄之 甲基錳,帶係被形成為積層鐵心,及蒸汽及空氣被施加, 藉由首先回火於約366t (69(TF)兩小時,然後,以蒸汽 (pH8)及空氣於304 C至316°C (580-600T )處理六小時,以 形成氧化鐵絕緣層。鐵心然後浸油。於脈衝測試時,鐵心 振動,及油係被加入,以於測試時協助保護鐵心。於鐵心 之測試2時,帶係被塗覆以很薄甲基錳,並被繞成積層鐵 心,鐵心然後被以例子1中之蒸汽/空氣處理。鐵心測試3 係藉由將一非晶金屬帶繞成一積層鐵心,並以示於例子1 中之%汽及$氣加以處理。已處理鐵心然後以光樹脂加以 浸潰。鐵心測試4係以鐵心測試相同方式形成並以重樹脂 加以浸潰。鐵心測試5係將非晶金屬合金繞成一積層鐵心 第47貰 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱) -----Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 508595 A7 B7 V. The iron core of the invention description (). The power loss is normalized between the two groups by dividing the power loss by the core weight. The second group of cores consisted of two groups, which were completed as described above, but were not treated with steam and air. As a result, this group of cores lacked iron oxide insulation and was used as a basis for comparing the power loss of the processed cores. The normalized information is shown in Table 14 below. Table 14 > nnnnn (^ I ^ > am · MW face · Hi I (please read the notes on the back before filling this page) Compare the power loss of treated and untreated amorphous iron cores as a function of frequency Power loss of processing core (W / lb) Frequency (KHz) Unprocessed processed improvement% 0.4 1.9 1.3 14 1.0 3.9 2.7 17 10.0 13 9.9 30 16.0 27 19 33 20.0 17 9.0 45.%-Consumption by employee of Intellectual Property Bureau, Ministry of Economic Affairs The data printed in Table 14 of the cooperative shows that the iron core generated by the iron core of the amorphous iron alloy treated by the method of the present invention has an improvement of 1 to 45% lower than that of the untreated iron core at high frequencies. That is, the The power loss is reduced from 14% to 45%. Furthermore, the improvement in performance increases with increasing frequency, as described above. A similar experiment was performed with fine crystalline materials, such as 70% Fe, 9% B, Page 45 This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 508595 V. Description of the invention () 3% Nb, 2% Cu and a small amount of Mo,. The formed core force ρ is performed. These cores are Tempered at about 58.0 (under 1000), cooled to room temperature, and then processed to form an iron oxide insulating layer. The reduction in power loss of these cores is compared to that of untreated fine crystalline core systems. Similar to what is seen in the amorphous metal alloy cores in Table 14. Example 2 Comparison of iron cores treated with steam and air and iron cores treated with methyl manganese in a pulse test The magnetic core consists of about 1 mil thick amorphous iron A belt, such as METGLAS2605SA1, is formed as a ring pulse iron core with an outer diameter of 197 cm (7 · 75 ”), an inner diameter of 10.8 cm (4.25”), and a thickness of 51.1 cm (2 ,,). It is coated with methyl manganese, or treated with steam / air after winding to form an iron oxide insulating layer, or both, as described in Table 15. The iron core is used by applying about 8.6 kV. Low frequency duty cycle, once every 5 cycles, lOpps and pulse energy calculated from 3 microsecond pulse width and 2.85T magnetic flux. Pulse data measurement includes core power (the amount of power dissipated by the core), starting current, and saturation Current, pulse energy The area of the pulse curve multiplied by the voltage is calculated to obtain the Joule amount of power. In all measurements, the lower the number, the better the core. Furthermore, preferably, the starting current is as close to the saturation current as possible. Test results This is shown in Table 15. Page 46 This paper is sized to the Chinese National Standard (CNS) A4 (210 X 297 mm). Γ Qing first read the note on the back? Please fill in this page again} Order. · Printed by 508595 A7 B7, Consumer Cooperatives of Intellectual Property Bureau of the Ministry of Economic Affairs 5. Description of the invention () --- Ϊm " 4u " · Manganese-5 Jinqi / Air treatment core pulse data test processing Core power (kW) Starting current (A) Saturation current (A) Pulse energy (Joule) 1 Immersion in oil, methyl, steam / air 201 20 38 0.75 2 Methyl, steam / air 204 20 40 0.77 3 Photoresin impregnation 287 30 50 1.0 4 heavy resin impregnation, steam / air 331 30 60 1.2 5 oil impregnation, steam / air 196 22 32 0.7 6 methyl manganese 200 20 40 0.8 --------.---.-- -Packing ·! .1 (Please read the notes on the back before filling this page) All the iron cores in Table 15 are amorphous metal alloys, and iron is the main metal. For the core of Test 1, the amorphous metal ribbon was coated with very thin methyl manganese, the ribbon was formed as a laminated core, and steam and air were applied, by first tempering at about 366t (69 (TF)) Hours, and then treated with steam (pH8) and air at 304 C to 316 ° C (580-600T) for six hours to form an iron oxide insulation layer. The core is then immersed in oil. During the pulse test, the core vibrates, and the oil system It was added to help protect the core during the test. At test 2 of the core, the band was coated with very thin methyl manganese and wound into a laminated core. The core was then treated with steam / air in Example 1. Core test 3 is made by winding an amorphous metal strip into a laminated iron core and treated with% vapor and $ gas as shown in Example 1. The treated iron core is then impregnated with photoresin. Iron core test 4 is the same as iron core test Formed and impregnated with heavy resin. Iron core test 5 is a series of amorphous metal alloy wound into a laminated iron core. The paper size is applicable to China National Standard (CNS) A4 (210 X 297 public love) -----

經濟部智慧財產局員工消費合作社印製 A7 B7 五、發明說明( 加以形成’然後以示於例子1中之蒸心空氣加以處理。鐵 ’、终後“ ’類似於測試!之鐵心。鐵心之測# 6係藉由 將非晶金屬帶塗覆以很薄甲基 心。 I々邻V成為積層鐵 如以上所示,於脈衝測試中被以蒸汽及空氣處理之 形成乳化鐵絕緣層大致執行如同由以甲基 帶所形成之鐵心之功率或f好。 更好然而’以蒸/汽空氣完成之 、-、、“係更快並較以薄層甲基錳塗覆花較低成本。 再者八有以甲基錳塗覆然後以樹脂浸潰之脈衝鐵心 於測試時破裂,為此並未示於表3之中…,如同資料 所不’於處理中以以由自然金屬氧化%,例如氧化鐵形成 〈絕緣層之脈衝鐵心較以甲基錳塗層形成之脈衝鐵心具 有更多彈性。如於測試3及4中以樹脂塗覆鐵心模擬結合 剑處理,將於切割鐵心形成C鐵心前加以完成。即使浸樹 月E1鐵心足以蒸汽/空氣處理鐵心所備製之鐵心之功率損失 係4 0 - 5 0南於未浸以樹脂之鐵心,浸潰之優點於一些硬性 疋很重要的應用中,可以超出於功率消散之增加。 效能對處理溫度 以下表1 6顯示具有鐵作為主要金屬於不同溫度條件 下之處理非晶金屬鐵心之效能作用。所用之鐵心係均約5 磅重,具有約5 · 1公分(2")寬帶。所以鐵心以蒸汽於空氣 中加以處理4小時,並回火2小時,除了鐵心同時回火及 私紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公麓 --------一---裝.L1 (請先閱讀背面之注意事項再填寫本頁) 訂: 經濟部智慧財產局員工消費合作社印製 508595 A7 __B7__ 五、發明說明() (請先閱讀背面之注意事項再填寫本頁) 處理外。後者係被同時回火並蒸汽處理4小時。一相同組 鐵心被處理及回火,但並不曝露至蒸汽/空氣,以形成氧化 鐵絕緣塗層。每一組鐵心之功率損失係被量測並比較如 下0 表1 6.氧化鐵塗層於C鐵心上比較未塗覆架構之相對效能 處理條件 頻率(kHz) 0.4 1.0 10.0 20.0 500°F處理690°F回火 9.0% 4 3.9% 2 1.1% 19.8% 550°F處理690°F回火 -19.5% 12.9% -71.5% -77.0% 590°F處理690°F回火 -5.7% 2 2.2% -53.1% -57.3% 625 °F處理690°F回火 -1.0% 3 8.1% 18.2% 17.8% 650°F處理690TF回火 -4.3% 3 1.2% -12.7% -18,5% 6 9 0 °F處理同時回火 2 2.8% 5 2.2% 5 0.2% 52.7% 鐵心損失表示為%改良(減少)比較於可比較未塗覆架構 經濟部智慧財產局員工消費合作社印製 表1 6反應由使用pH加強蒸汽所取自鐵心之資料,該 p Η加強蒸汽係大約p Η 8 -1 0,由一蒸汽產生器,用來自一 逆滲透系統之給水。為了比較目的,第5圖(表14)顯示由 未純作為約8之pH給水所處理得之相同鐵心架構。 例子4 示於表1 7是各種重量之未切割環形鐵心之比較。鐵 心係由例如METGLAS2605SA1之非晶金屬合金所形成。 第49頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 508595 A7 B7 五、發明說明() 主要元素金屬。鐵心係回火於3Μ C (690 F )2小時’然後 以蒸汽/氣體於戀3 0 4 °C至3 1 6 C (5 8 0 °F -6 0 0 °F )加以處理 2-6小時。可以由表5所看出,對於較高20kHz頻率,具 有本發明之絕緣塗層之鐵心展現大量減少之功率損失。 表17-有沒有蒸汽/空氣之功率損失未切割鐵心架構之比齡 低頻400Hz 高頻20KHz 400Hz ------- 一 20KHz 重(碎) 未處理 已處理 未處理 已處理 阻抗 阻抗 0.83 2.2 瓦/# 2.9 瓦/# -31% 0.92 1.8 瓦/# 2.2 瓦/# is m 7.2 瓦/# -19% 46% 1.24 1.4 瓦/# 2.0 瓦/# -41% 2.68 29 瓦/# 5.8 瓦/# 80% ££5 1.9 瓦/# 2.2 瓦/# 58 瓦/# 18 瓦/# -21% 69% λ24 1.4 瓦/# 2.0 瓦/# 13 瓦/# 10 瓦/# -44% 23% ----------裝 l· — (請先閱讀背面之注意事項再填寫本頁) 訂: 例子 METGLAS2605SA1鐵心係於690°F回火2小時,然 後,以約3 0 4。(:至3 1 8 °C (5 8 0 °F - 6 0 0 °F )蒸汽/氣體處理2,4 或6小時。如於表18所示,所看到功率損失大致隨著蒸 汽/.氣體處理時間由2增加至6小時而降低。 第50頁 用中國國家標準(CNS)A4規格(210 X 297公釐)Printed by the Consumers ’Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs A7 B7 V. Description of the invention (formed 'and then treated with the steaming air shown in Example 1. Iron', and finally" 'similar to the test! Iron core. Iron core Test # 6 is made by coating an amorphous metal strip with a very thin methyl core. I々V becomes a laminated iron. As shown above, the emulsified iron insulation layer treated with steam and air during the pulse test is roughly performed as The power or f of the iron core formed by the methyl band is better. Better, however, '-,,,' completed with steam / steam air is faster and costs less than coating with a thin layer of methyl manganese. Eight pulse iron cores coated with methyl manganese and impregnated with resin ruptured during the test, for which reason it is not shown in Table 3 ..., as the data does not show in the processing to oxidize by natural metals%, for example The pulse iron core formed by the iron oxide is more flexible than the pulse iron core formed with a methyl manganese coating. If the resin-coated iron core is used in tests 3 and 4 to simulate the combination with the sword treatment, it will be cut before the core is formed into a C iron core. To complete. Even dip The power loss of Shuyue E1 iron core is enough for the steam / air treatment iron core. The power loss of the iron core is 40-50% lower than that of the iron core not impregnated with resin. Increased power dissipation. Efficiency vs. processing temperature Table 16 below shows the effectiveness of iron as the main metal in the treatment of amorphous metal cores under different temperature conditions. The cores used are all about 5 pounds and have about 5.1 cm (2 ") Broadband. So the iron core is treated with steam in the air for 4 hours and tempered for 2 hours, except that the iron core is tempered at the same time and the private paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 male feet- ------ One --- install.L1 (Please read the notes on the back before filling this page) Order: Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 508595 A7 __B7__ 5. Description of the invention () (please first Read the notes on the reverse side and fill in this page again) Treatment outside. The latter is tempered and steam treated for 4 hours at the same time. The same set of cores are treated and tempered, but not exposed to steam / air to form an iron oxide insulation coating The power loss of each group of cores is measured and compared as follows. Table 1 6. Relative performance of iron oxide coatings on C cores compared to uncoated structures. Processing condition frequency (kHz) 0.4 1.0 10.0 20.0 500 ° F processing 690 ° F tempered 9.0% 4 3.9% 2 1.1% 19.8% 550 ° F tempered 690 ° F tempered -19.5% 12.9% -71.5% -77.0% 590 ° F tempered 690 ° F tempered -5.7% 2 2.2% -53.1% -57.3% 625 ° F treatment 690 ° F tempering -1.0% 3 8.1% 18.2% 17.8% 650 ° F treatment 690TF tempering -4.3% 3 1.2% -12.7% -18, 5% 6 9 0 ° Simultaneous tempering of F treatment 2 2.8% 5 2.2% 5 0.2% 52.7% Core loss is expressed as% improvement (reduced) compared to comparable uncoated architecture Printed by Employee Consumer Cooperatives of Intellectual Property Bureau of the Ministry of Economic Affairs Table 1 6 Response by using pH The data of the enhanced steam taken from the iron core, the p 系 enhanced steam system is about p Η 8 -10, and a steam generator uses feed water from a reverse osmosis system. For comparison purposes, Figure 5 (Table 14) shows the same core architecture treated with impure water as a pH of about 8. Example 4 shown in Table 17 is a comparison of uncut toroidal cores of various weights. The core is formed of an amorphous metal alloy such as METGLAS 2605SA1. P.49 This paper size is in accordance with Chinese National Standard (CNS) A4 (210 X 297 mm) 508595 A7 B7 5. Description of the invention () Main element metal. The iron core is tempered at 3M C (690 F) for 2 hours' and then treated with steam / gas at 3 0 4 ° C to 3 1 6 C (5 8 0 ° F -6 0 0 ° F) for 2-6 hours. . As can be seen from Table 5, for higher frequencies of 20 kHz, the core with the insulating coating of the present invention exhibits a significant reduction in power loss. Table 17-Is there a power loss of steam / air? The age of the uncut core structure is low frequency 400Hz high frequency 20KHz 400Hz ------- 20KHz heavy (broken) untreated processed untreated processed impedance impedance 0.83 2.2 watts / # 2.9 watt / # -31% 0.92 1.8 watt / # 2.2 watt / # is m 7.2 watt / # -19% 46% 1.24 1.4 watt / # 2.0 watt / # -41% 2.68 29 watt / # 5.8 watt / # 80% ££ 5 1.9 W / # 2.2 W / # 58 W / # 18 W / # -21% 69% λ24 1.4 W / # 2.0 W / # 13 W / # 10 W / # -44% 23%- -------- Install l · — (Please read the precautions on the back before filling in this page) Order: Example METGLAS2605SA1 iron core is tempered at 690 ° F for 2 hours, and then it is about 3 0 4. (: To 3 1 8 ° C (5 8 0 ° F-6 0 0 ° F)) steam / gas treatment for 2, 4 or 6 hours. As shown in Table 18, the power loss seen roughly follows steam /. The gas treatment time is increased from 2 to 6 hours and reduced. Page 50 Uses Chinese National Standard (CNS) A4 (210 X 297 mm)

經濟部智慧財產局員Η消費合作社印製 一尺 J張 /紙 ί本 508595 A7B7 五、發明說明() 表1 8-於兩頻率對處理時間之功率消散(瓦#) # 處理時間(分) 消散(400Hz) 消散20kHz 1 120 1.9 18 2 120 1.6 17 3 120 1.5 16 4 120 1.5 16 5 120 2.1 22 6 120 1.9 19 7 120 3.0 12 8 120 2.2 20 9 240 1.3 15 10 240 1.5 13 11 240 1.6 17 12 360 10 13 360 17 結果反映各種鐵心架構重量由少於1磅增加至略超出7磅 之正規化資料 (請先閱讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製 雖然,本發明及其優點已經參考其特定實施例加以詳 細說明,但應了解的是,各種變化,替換及改變可以在不 脫離本發明之範圍及精神下加以完成,本發明之範圍係由 以下之申請專利範圍所定義。 第51頁 本紙張尺度適用申國國家標準(CNS)A4規格(210 X 297公釐)Printed by a member of the Intellectual Property Bureau of the Ministry of Economic Affairs / Consumer Cooperative, one sheet of J / paper 508595 A7B7 V. Description of the invention () Table 1 8- Power dissipation of processing time at two frequencies (Watt #) # Processing time (minutes) Dissipation (400Hz) dissipation 20kHz 1 120 1.9 18 2 120 1.6 17 3 120 1.5 16 4 120 1.5 16 5 120 2.1 22 6 120 1.9 19 7 120 3.0 12 8 120 2.2 20 9 240 1.3 15 10 240 1.5 13 11 240 1.6 17 12 360 10 13 360 17 The results reflect the normalized information that the weight of various core structures has increased from less than 1 pound to slightly more than 7 pounds (please read the notes on the back before filling out this page) The present invention and its advantages have been described in detail with reference to specific embodiments thereof, but it should be understood that various changes, substitutions and alterations can be made without departing from the scope and spirit of the invention. The scope of the invention is determined by the following As defined by the scope of patent application. P.51 This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)

Claims (1)

508 508 |8胗9异8^正 臀& 屻m词慨矛、 槪專罐罐+|、辨抑和 六、申請專利範圍 1 ·種提供介電絕緣於一積層磁組件之相鄰金屬層間之方 法,該方法至少包含步驟: 提供一積層磁組件,其具有多數層,其中諸層之部 份係藉由鐵所形成;及 氧化諸層,以產生一絕緣塗層,該塗層包含氧化鐵 於諸層間,該所氧化磁組件於WkHz至2〇kHz之操作頻 率中,展現降低至少1 5%之功率損失,相較於以實質相 同大小組件而沒有絕緣塗層者。 2·如申請專利範圍第丨項所述之方法,其中上述之氧化步 驟包含將多數層曝露至蒸汽中,於氧出現於至少5〇〇卞 之溫度中。 3·如中請專利範圍第2項所述之方法,其中上述之諸層係 曝露至由500°F至800Τ之溫度。 4·如申請專利範圍第丨,2或3項所述之方法,其中上述之 多數層包含一非晶金屬合金。 5·如申請專利範圍第1,2或3項所述之方法,其中上述之 多數層包含一細結晶材料。 6·如申清專利範圍第1項所述之方法,其中上述之積声磁 組件為纏繞鐵心。 第52貰 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) I ---------It--------- (請先閱讀背面之注意事項再填寫本頁) i §88508595508 508 | 8 胗 9 异 8 ^ Positive buttocks & 屻 m words, spears, cans and cans + |, discrimination and six, patent application scope 1 · Adjacent metals that provide dielectric insulation in a laminated magnetic component An interlayer method, the method comprising at least the steps of: providing a laminated magnetic component having a plurality of layers, wherein portions of the layers are formed of iron; and oxidizing the layers to produce an insulating coating, the coating comprising Iron oxide is between the layers. The oxidized magnetic component exhibits a power loss reduction of at least 15% at an operating frequency of WkHz to 20kHz, compared to those having substantially the same size component without an insulating coating. 2. The method according to item 丨 of the scope of patent application, wherein the above-mentioned oxidation step includes exposing a plurality of layers to steam, and the presence of oxygen at a temperature of at least 500 ° F. 3. The method as described in item 2 of the patent scope, wherein the above-mentioned layers are exposed to a temperature from 500 ° F to 800T. 4. The method as described in claims 1, 2 or 3, wherein most of the above layers include an amorphous metal alloy. 5. The method according to claim 1, 2 or 3, wherein most of the above layers contain a fine crystalline material. 6. The method as described in item 1 of the scope of patent application, wherein the above-mentioned acoustic magnetic component is a wound core. Chapter 52: This paper size applies to China National Standard (CNS) A4 (210 X 297 mm) I --------- It --------- (Please read the precautions on the back first (Fill in this page again) i §88508595 經濟部智慧財產局員工消費合作社印製 7·如申請專利_ i項所述之方法,其中上述之積層磁 組件包含堆疊金屬層。 8·如申請專利範圍帛i項所述之方法,其中上述之氧化磁 組件展現至少30%之功率損失上之減少。 9·如申請專利範圍帛i項所述之方法,其中上述之氧化磁 組件展現至少45%之功率損失上之減少。 ι〇·如申請專利範圍第i項所述之方法,更包含由外部來源 提供氧化鐵陽離子給積層磁組件,於氧化積廣磁組件 時。 11.如申請專利範圍第i項所述之方法,更包含經由蒸汽提 供氧化鐵(Fe2〇3)給積廣磁組件,於諸層被氧化之同時β 12_如申請專利範圍第i項所述之方法,更包含將積層磁組 件曝露至其回火溫度至少2小時之時間段。 13. 如申請專利範圍第1項所述之方法,更包含將積層磁組 件曝露至其至少結晶設定溫度’至少兩小時之時間段。 14. 如申請專利範圍第丨項所述之方法,更包含量測氧化磁 組件之磁或電氣特性’然後’更進一步氧化已氧化磁件 illlllllllu I I--*· ---I ^« — — — — — 1 — . (請先閲讀背面之注意事項再填寫本頁) 第53頁Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 7. The method as described in the patent application item i, wherein the laminated magnetic component described above includes stacked metal layers. 8. The method as described in item (i) of the scope of patent application, wherein the above-mentioned oxidized magnetic component exhibits a reduction in power loss of at least 30%. 9. The method as described in item (i) of the scope of patent application, wherein the above-mentioned oxidized magnetic component exhibits a reduction in power loss of at least 45%. ι〇. The method described in item i of the scope of patent application, further comprising supplying iron oxide cations to the laminated magnetic component from an external source, when the laminated magnetic component is oxidized. 11. The method described in item i of the scope of patent application, further comprising supplying iron oxide (Fe2O3) to the magneto-optical component through steam, while the layers are being oxidized while β 12 The method further includes exposing the laminated magnetic component to its tempering temperature for a period of at least 2 hours. 13. The method as described in item 1 of the scope of patent application, further comprising exposing the laminated magnetic component to a time period of at least two hours of at least its crystallizing set temperature '. 14. The method described in item 丨 of the scope of patent application, further comprising measuring the magnetic or electrical characteristics of the oxidized magnetic component 'then' further oxidizes the oxidized magnetic part illlllllllu I I-* · --- I ^ «— — — — — 1 —. (Please read the notes on the back before filling this page) Page 53 508595 A8 B8 C8 D8 9L 8. 2,^ 年.月κ *· 經濟部智慧財產局員工消費合作社印製 申請專利範圍 之諸層,以增加絕緣塗覆之量。 15·—種軟磁組件,包含複數層金屬層,其中該複數層金屬 層之相鄰層間有一絕緣塗層,且該絕緣塗層基本上由氧 化諸層上之鐵所形成之氧化物所組成。 1 6 ·如申請專利範圍第1 5項所述之軟磁組件,更包含: 一長形非晶金屬帶,包含該組#,該帶係為至少40% 鐵,該帶具有第一侧及一第二側,該第一側更具有小突 出物及第二側係大致平滑; 一帶被繞以形成包含相鄰金屬層之積層,使得於第 一側上之突出物接觸該平滑第二面; 該絕緣塗層大致覆蓋平滑第二面並覆蓋至少突出物 之至少一部份,其接觸該平滑第二面者,該塗層具〇.〇 有微米或更多之厚度。 17 ·如申請專利範圍第16項所述之軟磁組件,其中上述之 7 5%以上之塗層包含氧化鐵(111)及氧化鐵(11-111)。 18·如申請專利範圍第16項所述之軟磁組件,具有大於500 歐姆公分之電阻率。 19.如申睛專利範圍第16項所述之軟磁組件,具有一大於 i 0 0 0歐姆公分之電阻率。 第54頁 ......餐......…、玎:;------S (請先閲讀背面之注意事項再填寫本頁) 508595508595 A8 B8 C8 D8 9L 8. 2, ^ year. Month κ * · Printed by the Consumers' Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs, the layers of the scope of patent application to increase the amount of insulation coating. 15 · A soft magnetic component comprising a plurality of metal layers, wherein an insulating coating is formed between adjacent layers of the plurality of metal layers, and the insulating coating is basically composed of an oxide formed by oxidizing iron on the layers. 1 6 · The soft magnetic component described in item 15 of the scope of patent application, further comprising: a long amorphous metal belt including the group #, the belt is at least 40% iron, the belt has a first side and a On the second side, the first side has small protrusions and the second side is substantially smooth; a strip is wound to form a laminate including adjacent metal layers, so that the protrusions on the first side contact the smooth second surface; The insulating coating substantially covers the smooth second surface and covers at least a part of the protrusions, and if the insulating coating contacts the smooth second surface, the coating has a thickness of 0.00 μm or more. 17 · The soft magnetic component according to item 16 of the scope of the patent application, wherein more than 75% of the above coatings include iron oxide (111) and iron oxide (11-111). 18. The soft magnetic component described in item 16 of the scope of patent application, has a resistivity greater than 500 ohm centimeters. 19. The soft magnetic component as described in item 16 of Shenyan's patent scope has a resistivity greater than 100 ohm centimeters. Page 54 ...... Meal ............ 、 玎 :; ------ S (Please read the notes on the back before filling this page) 508595 A8 BB C8 __—__D8 六、申請專利範圍 20·如申請專利範圍第16項所述之軟磁組件,具有一大於 10000歐姆公分之電阻率。 2 1 ·如申請專利範圍第1 6項所述之軟磁組件,其中上述之 金屬層包含一非晶金屬合金。 22·如申請專利範圍第16項所述之軟磁組件,其中上述之 金屬層包含一細結晶材料。 23. —種介電絕緣塗層,於一軟磁組件之相鄰金屬層之接觸 點間,該塗層包含足夠量之主要之氧化鐵,以能降低組 件中之功率損失至少15%,於10kHz或更高之操作頻率 時。 24·如申請專利範圍第23項所述之介電絕緣塗層,其中足 夠量係足以降低於組件中之功率損失至少30%。 經濟部智慧財產局員工消費合作社印製 25·如申請專利範圍第24項所述之介電絕緣層,其中足夠 量係足以降低於組件中之功率損失至少45%。 第55頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐)A8 BB C8 __—__ D8 6. Scope of patent application 20 · The soft magnetic component described in item 16 of the scope of patent application has a resistivity greater than 10,000 ohm cm. 2 1 · The soft magnetic component according to item 16 of the scope of patent application, wherein the metal layer comprises an amorphous metal alloy. 22. The soft magnetic component according to item 16 of the scope of patent application, wherein said metal layer comprises a fine crystalline material. 23. — A dielectric insulation coating between the contact points of adjacent metal layers of a soft magnetic component. The coating contains a sufficient amount of the main iron oxide to reduce the power loss in the component by at least 15% at 10 kHz. Or higher. 24. The dielectric insulation coating according to item 23 of the scope of the patent application, wherein a sufficient amount is sufficient to reduce the power loss in the module by at least 30%. Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 25. The dielectric insulation layer as described in item 24 of the scope of patent application, where a sufficient amount is sufficient to reduce the power loss in the module by at least 45%. Page 55 This paper is sized for China National Standard (CNS) A4 (210 X 297 mm)
TW089109728A 1999-05-20 2000-06-22 Magnetic core insulation TW508595B (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US31554999A 1999-05-20 1999-05-20
US14120999P 1999-06-25 1999-06-25

Publications (1)

Publication Number Publication Date
TW508595B true TW508595B (en) 2002-11-01

Family

ID=26838895

Family Applications (1)

Application Number Title Priority Date Filing Date
TW089109728A TW508595B (en) 1999-05-20 2000-06-22 Magnetic core insulation

Country Status (7)

Country Link
EP (1) EP1101229A1 (en)
JP (1) JP2003500850A (en)
KR (1) KR100701902B1 (en)
AU (1) AU5273600A (en)
CA (1) CA2337653A1 (en)
TW (1) TW508595B (en)
WO (1) WO2000072334A1 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102006019613B4 (en) * 2006-04-25 2014-01-30 Vacuumschmelze Gmbh & Co. Kg Magnetic core, process for its preparation and its use in a residual current circuit breaker
US11715591B2 (en) 2020-03-27 2023-08-01 Proterial, Ltd. Method for manufacturing a wound magnetic core

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CA1205725A (en) * 1982-09-06 1986-06-10 Emiko Higashinakagawa Corrosion-resistant and wear-resistant amorphous alloy and a method for preparing the same
JPS59169109A (en) * 1983-03-16 1984-09-25 Hitachi Ltd Electromagnetic iron core
JPH079057B2 (en) * 1985-04-26 1995-02-01 株式会社東芝 Amorphous alloy magnetic core manufacturing method

Also Published As

Publication number Publication date
CA2337653A1 (en) 2000-11-30
AU5273600A (en) 2000-12-12
JP2003500850A (en) 2003-01-07
KR20010085295A (en) 2001-09-07
WO2000072334A1 (en) 2000-11-30
KR100701902B1 (en) 2007-04-02
EP1101229A1 (en) 2001-05-23

Similar Documents

Publication Publication Date Title
US5032947A (en) Method of improving magnetic devices by applying AC or pulsed current
US4268325A (en) Magnetic glassy metal alloy sheets with improved soft magnetic properties
JPH0777167B2 (en) Magnetic core parts
KR20050084640A (en) Bulk amorphous metal inductive device
JP2002530854A (en) Magnetic core suitable for use in current transformer, method for manufacturing magnetic core, and current transformer
US5256211A (en) Rapid annealing method using shorted secondary technique
JP2011171772A (en) Gapped amorphous metal-based magnetic core
TW511104B (en) High performance bulk metal magnetic component
US7077919B2 (en) Magnetic core insulation
US4834816A (en) Metallic glasses having a combination of high permeability, low coercivity, low ac core loss, low exciting power and high thermal stability
TW508595B (en) Magnetic core insulation
US5284528A (en) Metallic glasses having a combination of high permeability, low coercivity, low ac core loss, low exciting power and high thermal stability
JP5702632B2 (en) Magnetic article using magnetic metal ribbon coated with insulator
US5110378A (en) Metallic glasses having a combination of high permeability, low coercivity, low ac core loss, low exciting power and high thermal stability
JPS5851403B2 (en) Manufacturing method of iron core for switching transformer
GB2233828A (en) Improving magnetic properties of ferromagnetic material
US7132018B2 (en) Magnetic core insulation
JP6759458B2 (en) A transformer core for a cut-and-stack type transformer and a transformer equipped with it
JPH06346219A (en) Magnetic material using amorphous magnetic alloy, method for producing the same and device therefor
JP2760561B2 (en) Magnetic core
JPH0689438B2 (en) Iron-rich metallic glass with high saturation magnetic induction and excellent soft ferromagnetism at high magnetization rates
KR100209438B1 (en) Magnetic cores utilizing metallic glass ribbons and mica paper interlaminar insulation
GB2233829A (en) Improving magnetic properties of ferromagnetic alloys
JPH02260612A (en) Laminated iron core
JPH0296306A (en) Amorphous magnetic thin-band winding core

Legal Events

Date Code Title Description
GD4A Issue of patent certificate for granted invention patent
MM4A Annulment or lapse of patent due to non-payment of fees