TW200841364A - High-voltage transformer with adjustable magnetic leakage - Google Patents
High-voltage transformer with adjustable magnetic leakage Download PDFInfo
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200841364 九、發明說明: 【發明所屬之技術領域】 本發明是有關於一種變壓器,特別是指一種可降低初 級線圈溫升及可調整線圈茂漏磁束以使左右磁阻對稱的高 壓可調漏磁變壓器。 【先前技術】 依據美國案專利號第us 7015785 B2號及日本案特開第 2001-148318號之專利案所揭露之變壓器,一次側磁阻是等 於二次側磁阻,可減少磁芯的磁束洩漏。若要增加磁芯的 磁束Λ漏了在-人側與二次側之間增加一個控制磁芯。 但是’此控制磁芯必須以非常精密的加工(通常是〇 . 〇1匪 以下的公差)來達成洩漏磁束的調整,並且符合交貨規格在 漏電感±7.5%的條件内,進而用分類的方式,將漏電感以土 2/〇为類元成’然後放在同一片驅動電路板上,以符合最後 成品的電氣需求。 此種控制浪漏磁束的方式,是以控制鐵芯吸引中柱鐵 芯的磁线漏方式來達成,在中柱磁芯中的磁束必須通過空 氣隙到達控制磁芯,且因為空氣與鐵芯的導磁係數(# ) 差異南達2000倍,導致控制磁芯不易將中柱磁芯中的磁束 吸出而形成漏磁。所以在人工組裝時,只要有些微的組裝 决差’就會導致產品不良,無法符合大量製造時所要求的 穩定度。 由於該初級線圈是同時驅動兩個次級線圈,所以該初 級線圈的繞線徑度等於該二次級線圈的繞線徑度的和,使 5 200841364200841364 IX. Description of the Invention: [Technical Field] The present invention relates to a transformer, and more particularly to a high-voltage adjustable leakage magnetic flux which can reduce the temperature rise of the primary coil and adjust the magnetic flux leakage of the coil to make the left and right magnetic reluctance symmetrical. transformer. [Prior Art] According to the transformer disclosed in the U.S. Patent No. US Pat. No. 7,150, 785, and the Japanese Patent Application No. 2001-148318, the primary side reluctance is equal to the secondary side reluctance, and the magnetic flux of the magnetic core can be reduced. leakage. To increase the magnetic core of the magnetic core, a control core is added between the human side and the secondary side. However, 'this control core must be adjusted to a very precise machining (usually 〇. 〇1匪 tolerance) to achieve leakage magnetic beam adjustment, and meet the delivery specifications within ±7.5% of the leakage inductance, and then with the classification In this way, the leakage inductance is made of soil 2/〇 as 'class' and then placed on the same drive circuit board to meet the electrical requirements of the final product. The way to control the magnetic flux leakage is achieved by controlling the magnetic flux leakage mode of the iron core to attract the middle pillar iron core. The magnetic flux in the middle pillar magnetic core must reach the control magnetic core through the air gap, and because the air and the iron core The magnetic permeability coefficient (#) is 2000 times different from that of the south, which causes the control core to not easily suck out the magnetic flux in the middle column core to form magnetic flux leakage. Therefore, in the case of manual assembly, as long as there is a slight assembly failure, the product may be defective and cannot meet the stability required for mass production. Since the primary coil drives the two secondary coils at the same time, the winding diameter of the primary coil is equal to the sum of the winding diameters of the secondary coil, so that 5 200841364
得該初級線圈的繞線截面積等於該二次級線圈的繞線截面 積的和。在此條件下,一次側的總磁阻約等於兩個二次側 的總磁阻的和,也就是磁力線並沒有因為磁阻改變而被強 制洩漏形成漏磁。根據已知公式^ = ,可知電感量L 與繞線截面積A呈正比,因此,藉由增加該初級線圈的繞 線截面積A使該初級線圈的電感量[增加,進而增加初級 線圈的有效磁通,有效地控制初級線圈溫度的上升。The winding cross-sectional area of the primary coil is equal to the sum of the winding cross-sectional areas of the secondary coil. Under this condition, the total magnetic reluctance of the primary side is approximately equal to the sum of the total reluctances of the two secondary sides, that is, the magnetic lines of force are not forced to leak due to the change in magnetoresistance to form a magnetic flux leakage. According to the known formula ^ = , the inductance L is proportional to the cross-sectional area A of the winding. Therefore, by increasing the winding cross-sectional area A of the primary coil, the inductance of the primary coil is increased, thereby increasing the effectiveness of the primary coil. Flux, effectively controlling the rise in temperature of the primary coil.
可是,因為第一鐵芯與第二鐵芯組立完畢之後,鐵芯 的結構跟繞線的配置已經決定了線圈茂漏磁束的大小,並 ’又有〃他可行的結構可以進行調整。再加上鐵芯是由粉末 U成,因$燒結尺寸會因熱服冷縮產生燒結公差及上 下鐵芯會有結合公差,左右磁阻通常不相等,導致次級線 圈進入諧振工作時,尤亡&、息 1左右兩邊所產生的功率轉移有差異, 導致其他電氣上的品質問題發生。 另外,依據美國案專利號第US7〇1578sb2號專利案所 揭露之變壓器,在實抨麻 ^ 貝際研磨製造時,受限於第二鐵心的外 型设計’研磨程序十分繫* ^ 繁負使業者無法針對此變壓器進 行量產。 ° 【發明内容】 溫升因二!發明之目的,即在提供一種可降低初級線圈 _磁:的大::可漏磁束的鐵心結構來調整線 心的接觸面二而=用:分移動的方式改變二次侧鐵 右磁阻對稱,同時側磁阻做對稱調整,以使左 j 了具有可ϊ產性的變壓器。 200841364 於是’本發明變壓器是包含一繞線架單元,一初級線 圈,二次級線圈,及一鐵芯單元。 該繞線架單元包括一形成一初級線圈段的初級線圈架 ,及二各形成一次級線圈段的次級線圈架,該初級線圈段 的繞線徑度大於該二次級線圈段的繞線徑度的兩倍。 該初級線圈是繞設於該初級線圈段,該二次級線圈是 分別繞設於該二次級線圈段。 該鐵芯單元是組設於該繞線架單元,包括一穿設於該 繞線架單元的第一鐵芯,一連接於該第一鐵芯的第二鐵芯 ,一形成於該第一鐵芯與該第二鐵芯之間並靠近該初級線 圈的初級磁通區,及二形成於該第一鐵芯與該第二鐵芯之 間並靠近該二次級線圈的次級磁通區,該第一鐵芯具有一 牙设於该初級線圈架的初級段,二自該初級段延伸並相間 隔地穿設於該二次級線圈架的次級段,二形成於該二次級 段内側並相對设置的第一内面,及二相反於該二第一内面 的第一側面,該第二鐵芯具有二分別連接該二次級段的次 級端部,二分別形成於該二次級端部内側並相對設置的第 二内面,二相反於該二第二内面的第二側面,及二分別形 成於該一次級端部並與該二次級段連接的次級接觸面。 本發明的有益效果在於:因為該初級線圈段的繞線徑 度大於該次級線圈段的繞線徑度的兩倍,使磁束因為中柱 磁芯磁阻的改變而產生磁力線強制洩漏,使得控制磁芯得 以控制洩漏電感(磁束)的大小,並使該初級線圈的電感量匕 立曰加,進而增加初級線圈的有效磁通,有效地控制初級線 200841364 圈溫度的上升。 此外,由於一次側繞線區的磁阻不等於二次側繞線區 磁臂的磁阻,使得一次側線圈產生的磁力線因磁阻的改變 而被強制擠壓到空氣中形成洩漏磁束。然而,控制此浪漏 磁束的最佳區域,即磁阻改變的區域附近,、是位於初級磁 通區與兩個次級磁通區之間。 因此,更在初級磁通區與兩個次級磁通區之間增加一However, after the first core and the second core are assembled, the structure of the core and the configuration of the winding have determined the size of the magnetic flux leakage of the coil, and the structure that can be adjusted can be adjusted. In addition, the iron core is made of powder U, because the sintering size will result in sintering tolerance due to shrinkage of the hot clothes and the upper and lower iron cores will have combined tolerances, and the left and right magnetic reluctances are usually not equal, resulting in the secondary coil entering the resonance work, especially There is a difference in the power transfer between the dead & and the left and right sides of the interest, causing other electrical quality problems to occur. In addition, the transformer disclosed in the U.S. Patent No. US Pat. No. 7,78, sb2, is limited in the design of the second core when the ramie is manufactured by the ramie, and the grinding process is very complicated. The manufacturer is unable to mass produce this transformer. ° [Summary of the content] Temperature rise due to two! The object of the invention is to provide a core structure capable of reducing the large:: magnetic flux leakage of the primary coil to adjust the contact surface of the core; and to change the secondary magnetic resonance symmetry of the secondary side by means of sub-movement At the same time, the side reluctance is symmetrically adjusted so that the left j has a switchable transformer. 200841364 Thus, the transformer of the present invention comprises a bobbin unit, a primary coil, a secondary coil, and a core unit. The bobbin unit includes a primary bobbin forming a primary coil segment, and two secondary bobbins each forming a primary coil segment, the primary coil segment having a winding diameter greater than the winding of the secondary coil segment Double the diameter. The primary coil is wound around the primary coil segment, and the secondary coil is wound around the secondary coil segment. The core unit is assembled on the bobbin unit, and includes a first iron core disposed on the bobbin unit, and a second iron core connected to the first iron core, one formed on the first core a primary magnetic flux region between the iron core and the second core adjacent to the primary coil, and a secondary magnetic flux formed between the first core and the second core and adjacent to the secondary coil a first core having a primary segment disposed on the primary bobbin, two extending from the primary segment and spaced apart from the secondary segment of the secondary coil former, and two formed in the secondary segment a first inner surface opposite to the inner side of the step, and a second inner surface opposite to the first inner surface, the second core has two secondary ends respectively connected to the second stage, and two are respectively formed on the second end a second inner surface opposite to the second secondary end, opposite to the second side of the second inner surface, and two secondary contact surfaces respectively formed at the end of the primary stage and connected to the secondary stage . The invention has the beneficial effects that: because the winding diameter of the primary coil segment is greater than twice the winding diameter of the secondary coil segment, the magnetic flux is forced to leak due to the change of the magnetic resistance of the central pillar core, so that the magnetic flux is forced to leak. The control core controls the size of the leakage inductance (magnetic flux) and increases the inductance of the primary coil, thereby increasing the effective magnetic flux of the primary coil and effectively controlling the rise of the temperature of the primary line 200841364. Further, since the magnetic resistance of the primary side winding region is not equal to the magnetic resistance of the magnetic arm of the secondary winding portion, the magnetic lines of force generated by the primary side coil are forcibly pressed into the air to form a leakage magnetic flux due to the change in magnetic resistance. However, the optimum area for controlling this leakage magnetic flux, i.e., near the region where the magnetoresistance changes, is located between the primary magnetic flux region and the two secondary magnetic flux regions. Therefore, one more is added between the primary magnetic flux region and the two secondary magnetic flux regions.
洩漏磁路調整結構,此結構可以根據最後鐵芯燒結的特性 結果,以研磨鐵心深度的方式來調整變壓器整體的洩漏磁 束的大小,藉此控制洩漏磁束進而控制洩漏電感,減少因 鐵心燒結所引起尺寸變化所造成的後製程分類,降低量產 時所需之成本。並將上下鐵芯結合的部份,以不同尺寸的 組裝方式,以部份的結合磁阻面積來調整磁臂上的差異, 進而使左右磁臂對稱。 另外,藉由研磨鐵心深度的方式將研磨公差控制在+ 0.05賴以符合電氣上的交貨規格,且漏電感均位於±2%的條 件内,不需要再加以分類即可放在同一片驅動電路板上, 以符合最後成品的電氣需求。 所以,以中柱磁芯強制、、由、货r义土 ^ u強制次漏磁束的方法,可使控制 Γ加=的公差放寬到可以大量製造的水準,並符合客戶 嚴袼父貨要求。以目前的 尤一 ㈣機械研磨加工要求來說,本發 =可以達到大量製造的目的,而且可 要求’大大的降低生產成本,同時增加產品的良率。 而且’該第二鐵心的結構較習知單純,可降低實際 8 200841364 ==費的成本,可降低實際大量 ’ k成不良率、出貨成本及庫存增加等。 【實施方式】 、有關本發明之前述及其他技術内容、特點與功效,在 以下配口參考圖式之六個較佳實施例的詳細說明中,將可 清楚的呈現。Leakage magnetic circuit adjustment structure, which can adjust the leakage magnetic flux of the whole transformer according to the characteristics of the final core sintering, thereby controlling the leakage magnetic flux and controlling the leakage inductance, thereby reducing the sintering caused by the core sintering. The post-process classification caused by dimensional changes reduces the cost of mass production. The parts of the upper and lower iron cores are combined in different sizes, and the difference in the magnetic arms is adjusted by the combined magnetic reluctance area, so that the left and right magnetic arms are symmetrical. In addition, by grinding the core depth to control the grinding tolerance to +0.05 to meet the electrical delivery specifications, and the leakage inductance is within ±2% of the conditions, no need to classify can be placed in the same drive On the board to meet the electrical requirements of the final product. Therefore, with the method of forcing the magnetic core of the middle column, and forcing the magnetic flux leakage, the tolerance of the control 放 plus = can be relaxed to a level that can be mass-produced, and meets the strict requirements of the customer. In the current U.S. (4) mechanical grinding processing requirements, this hair = can achieve a large number of manufacturing purposes, and can require 'significantly reduce production costs, while increasing product yield. Moreover, the structure of the second core is simpler than conventional, and the cost of the actual 8 200841364 == fee can be reduced, and the actual large amount of defective rate, shipping cost, and inventory increase can be reduced. The above and other technical contents, features and effects of the present invention will be apparent from the following detailed description of the preferred embodiments of the accompanying drawings.
在本發明被詳細描述之前,要注意的是,在以下的說 明内容中’類似的元件是以相同的編號來表示。 如圖1所示,本發明變壓器之第一較佳實施例包含一 繞線架單元1 ’ 一初級線圈2,二次級線圈3,及一鐵芯單 元4 〇 5亥繞線架單元1包括一形成一初級線圈段11的初級線 圈架15 ’及一各形成一次級線圈段12的次級線圈架16, —該初級線圈段11的繞線徑度是大於該二次級線圈段丨2的 繞線徑度的兩倍。 該初級線圈2是繞設於該初級線圖段11,該二次級線 圈3是分別繞設於該二次級線圈段12。 該鐵芯單元4包括一穿設於該繞線架單元1的第一鐵 芯41,一連接於該第一鐵芯41的第二鐵芯42,一形成於 該第一鐵芯41與該第二鐵芯42之間並靠近該初級線圈2 的初級磁通區43,二形成於該第一鐵芯41與該第二鐵芯 42之間並靠近該二次級線圈3的次級磁通區44,及一位於 該初級線圈2與該二次級線圈3之間的漏磁區45,該第二 9 200841364 鐵芯42與該第一鐵芯41形成一連接該初級線圈2與該二 次級線圈3的磁通路。 該第一鐵芯41具有一穿設於該初級線圈架15的初級 段411 ’二自該初級段4Π延伸並相間隔地穿設於該二次級 線圈架16的次級段412,二形成於該二次級段412内側並 相對設置的第一内面414,及二相反於該二第一内面414的 第一側面413 ’該第二鐵芯42具有二分別連接該二次級段 412的次級端部423,二分別形成於該二次級端部423内側 並相對设置的第二内面425,二相反於該二第二内面425的 第一側面424 ’ 一對應該漏磁區45的調磁端部426,及二 分別形成於該二次級端部423並與該二次級段412連接的 次級接觸面422。 除了圖1所示的鐵心組成方式外,如圖2所示,該調 磁端部426也可以形成於該第一鐵心41上。如圖3所示, w亥一次級端部423之間的開口也可以是呈半圓形。如圖· 4 所示’該第二鐵心42相背於該二次級端部423的一端也可 以向内縮減成一初級端部427。如圖5所示,該第一鐵芯 41與該第二鐵心42也可以是一 γ型鐵芯。而且該初級線圈 架15除了是沿一 X軸方向套設於該第一鐵芯ο之外,也 可以是沿一與X軸方向垂直的γ軸設置於該第一鐵心41與 该第二鐵心42之間。如圖6所示,該初級段411是沿一與 X轴方向垂直的γ軸設置,該二次級段412是由該二次級端 4 423末端朝向該初級段411沿X轴方向延伸形成。 值得注意的是,如圖7(a)所示,該二第二側面424間的 10 200841364 巨_專於該一第一侧面413間的距離,該二次級接觸面422 的面積是分別大於該二次級磁通區44的有效截面積。 如圖7(b)所示,當該第二鐵芯42往左移動時,位於左 侧的該次級磁通區44的有效截面積不變,位於右侧的該次 級磁通區44的有效截面積改變。如圖7(c)所示,當該第二 鐵心42往右移動時,位於左側的該次級磁通區44的有效 截面積改變,位於右側的該次級磁通區44的有效截面積不 變。因此,使用者可藉此改變通過該二次級磁通區44的磁 通里以调整左右兩邊的磁通量對稱,同時使電氣上的功率 轉移對稱。此調整方式是以改變接觸面積的調整方式來達 到磁通量的調整目的。 使用時,因為該初級線圈段u的繞線徑度大於該二次 、、及線圈4又12的繞線徑度,可使該初級線圈2的電感量l增 加,進而增加該初級線圈2的有效磁通,有效地控制溫度 的上升。另外,藉由可調整洩露磁通的結構控制漏電感, 以部份的結合磁阻面積來調整磁臂的差異,進而使左右磁 臂對稱’有效地改善左右磁臂對稱不均的問題。 此外,如圖8(a)所示,以下將更進一步說明本發明變 壓器之第二較佳實施例,該第二較佳實施例與該第一較佳 實施例大致相同,其不同處在於該二第二内面425間的距 離等於該二第一内面414間的距離,該二次級接觸面422 的面積是分別大於該二次級磁通區44的有效截面積。 如圖8(b)所示,該第二鐵芯42往左移動時,位於左側 的該次級磁通區44的有效截面積改變,位於右側的該次級 11 200841364 磁通區44的右i “ 有政戴面積不變。如圖8(c)所示,當該第二鐵 心^右移動時,位於左侧的該次級磁通區 面積不變,位你m ^ ^ 於右側的該次級磁通區44的有效戴面積改變 。因此’使用者可藉此改變通過該二次級磁通區44的磁通 量0 使用時,該第二較佳實施例具有與該第一較佳實施例 相同的功效’可同時降低初級線圈溫升並調整線㈣漏磁 束以使左右磁阻對稱。Before the present invention is described in detail, it is to be noted that in the following description, similar elements are denoted by the same reference numerals. As shown in FIG. 1, a first preferred embodiment of the transformer of the present invention comprises a bobbin unit 1 'a primary coil 2, a secondary coil 3, and a core unit 4 〇5 a primary bobbin 15' forming a primary coil section 11 and a secondary bobbin 16 each forming a primary coil section 12, the winding diameter of the primary coil section 11 being greater than the secondary coil section 丨2 The winding diameter is twice as large. The primary coil 2 is wound around the primary line segment 11, and the secondary coil 3 is wound around the secondary coil segment 12, respectively. The core unit 4 includes a first core 41 that is disposed on the bobbin unit 1 , and a second core 42 that is coupled to the first core 41 , and is formed on the first core 41 . The second core 42 is adjacent to the primary magnetic flux region 43 of the primary coil 2, and is formed between the first core 41 and the second core 42 and adjacent to the secondary magnetic pole of the secondary coil 3. a pass region 44, and a magnetic flux leakage region 45 between the primary coil 2 and the secondary coil 3, the second 9 200841364 core 42 and the first core 41 form a connection between the primary coil 2 and the The magnetic path of the secondary coil 3. The first core 41 has a primary section 411' extending through the primary bobbin 15 and extending from the primary section 4Π and spaced apart from the secondary section 412 of the secondary coil former 16 to form a first inner surface 414 disposed opposite the second stage 412 and opposite to the first side 413 ′ of the two first inner surfaces 414. The second core 42 has two second stages 412 respectively connected to the second stage 412 The second end portion 423 is formed on the inner side of the second-stage end portion 423 and opposite to the second inner surface 425, and opposite to the first side surface 424 ′ of the second second inner surface 425. The magnetically permeable end portions 426, and two are respectively formed on the secondary end portion 423 and connected to the secondary contact portion 422. In addition to the core composition shown in Fig. 1, as shown in Fig. 2, the magnetically permeable end portion 426 may be formed on the first core 41. As shown in FIG. 3, the opening between the primary ends 423 of the whai may also be semi-circular. As shown in Fig. 4, the end of the second core 42 opposite to the secondary end portion 423 can also be reduced inwardly to a primary end portion 427. As shown in Fig. 5, the first core 41 and the second core 42 may also be a γ-type iron core. Moreover, the primary bobbin 15 may be disposed on the first core 41 and the second core in a y-axis perpendicular to the X-axis direction. Between 42. As shown in FIG. 6, the primary segment 411 is disposed along a γ-axis perpendicular to the X-axis direction, and the secondary segment 412 is extended from the end of the secondary terminal 4 423 toward the primary segment 411 in the X-axis direction. . It should be noted that, as shown in FIG. 7( a ), the distance between the two second side faces 424 10 200841364 is greater than the distance between the first side faces 413 , and the area of the second-level contact faces 422 is greater than The effective cross-sectional area of the secondary magnetic flux region 44. As shown in FIG. 7(b), when the second core 42 is moved to the left, the effective cross-sectional area of the secondary magnetic flux region 44 on the left side is constant, and the secondary magnetic flux region 44 on the right side is unchanged. The effective cross-sectional area changes. As shown in FIG. 7(c), when the second core 42 is moved to the right, the effective sectional area of the secondary magnetic flux region 44 on the left side is changed, and the effective sectional area of the secondary magnetic flux region 44 on the right side is changed. constant. Therefore, the user can thereby change the magnetic flux passing through the secondary magnetic flux region 44 to adjust the magnetic flux symmetry of the left and right sides while making the electrical power transfer symmetrical. This adjustment method is to adjust the contact area to achieve the purpose of adjusting the magnetic flux. In use, since the winding diameter of the primary coil segment u is greater than the winding diameter of the secondary coil and the coils 4 and 12, the inductance l of the primary coil 2 can be increased, thereby increasing the primary coil 2 Effective flux to effectively control the rise in temperature. In addition, the leakage inductance is controlled by the structure of the leakage flux, and the difference of the magnetic arms is adjusted by the combined magnetic reluctance area, so that the left and right magnetic arms are symmetrically effective to improve the symmetry unevenness of the left and right magnetic arms. In addition, as shown in FIG. 8(a), a second preferred embodiment of the transformer of the present invention will be further described below. The second preferred embodiment is substantially the same as the first preferred embodiment except that the The distance between the second inner faces 425 is equal to the distance between the two first inner faces 414, and the area of the secondary contact faces 422 is greater than the effective cross-sectional area of the secondary magnetic flux regions 44, respectively. As shown in FIG. 8(b), when the second core 42 is moved to the left, the effective cross-sectional area of the secondary magnetic flux region 44 on the left side is changed, and the secondary portion 11200841364 on the right side is the right of the magnetic flux region 44. i “The area of the political wear is unchanged. As shown in Fig. 8(c), when the second core moves to the right, the area of the secondary magnetic flux area on the left side does not change, and you are m ^ ^ on the right side. The effective wearing area of the secondary magnetic flux region 44 is changed. Therefore, when the user can change the magnetic flux 0 passing through the secondary magnetic flux region 44, the second preferred embodiment has the first preferred embodiment. The same effect of the embodiment can simultaneously reduce the temperature rise of the primary coil and adjust the line (4) leakage flux to make the left and right magnetoresistance symmetrical.
—如圖9所示’以下將更進—步說明本發明之第三較佳 實施例。為了使必要的特徵能夠清楚地呈現,初級線圈架 與-人級線圈架以及繞設於其上的初級線圈與次級線圈均以- As shown in Fig. 9, a third preferred embodiment of the present invention will be described hereinafter. In order to enable the necessary features to be clearly presented, the primary bobbin and the human-stage bobbin and the primary and secondary coils wound thereon are
假想線表示D 該第三較佳實施例與該第一較佳實施例大致相同,其 不同處在於該繞線架單$ i包括二各形成—初級線圈段U 的初級線圈架15,及四各形成-次級線圈段12的次級線圈 架16。該鐵芯單元4包括二相對設置並穿設於該繞線架單 元1的第一鐵芯41,一連接於該二第一鐵芯41的第二鐵怒 42,二形成於該第一鐵芯41與該第二鐵芯42之間並靠近 該初級線圈架15的初級磁通區43,及二形成於該二第一鐵 心41與該第二鐵芯42之間並靠近該次級線圈架16的漏磁 區45。该第二鐵芯42具有二分別對應於該二漏磁區托的 調磁端部426。 另外,該等次級線圈架16也可以是一體成型,使原本 的四個次級線圈架16縮減為兩個。而且該初級線圈架15 12 200841364 與該第一較佳實施例相同,也可以是沿一與X軸方向垂直 的Y軸設置於該第一鐵心41與該第二鐵心42之間。 使用時,該第三較佳實施例具有與該第一較佳實施例 相同的功效,可同時降低初級線圈溫升並調整線圈泡漏磁 束以使左右磁阻對稱。此外,藉由調整該調磁端部與 該漏磁區45的接觸面積,可調整洩漏磁通量以達成所需的 電感值。 如圖ίο、11所示,以下將更進一步說明本發明之第四 車乂佳實施例,包含一繞線架單元1,一初級線圈2,一次級 線圈3及鐵芯單元4。該繞線架單元1包括一初級線圈 段11,及一次級線圈段12,該初級線圈段u的繞線徑度 大於該次級線圈段12的繞線徑度。該鐵芯單元4是組設於 該繞線架單元1,包括一穿設於該繞線架單元i的第一鐵芯 41 ’ 一連接於該第一鐵芯ο的第二鐵芯42,一形成於該第 一鐵芯41與該第二鐵芯42之間並靠近該初級線圈2的初 級磁通區43,及一形成於該第一鐵芯41與該第二鐵芯42 之間並罪近邊次級線圈3的次級磁通區44,該第二鐵芯42 /、“弟鐵〜41形成一連接該初級線圈2與該次級線圈3 的磁通路。 / 使用守本只施例與該第一較佳實施例相同,該初級 線圈段11的繞線徑度大於該次級線圈段12的繞線植度, 因此可以#到與該第—較佳實施例相同的降溫效果。 囷12 13所示,以下將更進一步說明本發明之第五 較佳實施例,該第五較佳實施例與上述第四較佳實施例大 13 200841364 致相同,其不同處在於該繞線架單元i還包括一穿孔i3, 及-氣隙14 °該第一鐵芯41是穿設於該穿孔,且該第 -鐵怎41的徑度小於該穿孔13的徑度並與該穿孔之間形 成該氣隙14。在本實施例中,該第—鐵芯41的截面積與該 穿孔13的截面積的比例為1.6。該氣隙14可供該第三 鐵芯45穿置,藉此得到更好的導磁效果。 使用恰,本實施例與該第一較佳實施例相同,該初級 線圈段11的繞線徑度大於該次級線圈段12的繞線徑度, 因此可以得到與該第—較佳實施例相同的降溫效果。 —如圖14所示’以下將更進_步說明本發明之第六較佳 實施例’該第六較佳實施例與上述第四較佳 同’其不同處在於該第二鐵芯42具有二分別形成於該第: 鐵芯之相反兩端部並與該第一鐵& 41接觸的初級接觸面 42卜次級接觸面422,該初級接觸面421、次級接觸面似 的面積是不小於該初級磁通區43、次級磁通區44的有效截 面積。 使用時,本實施例與該第一較佳實施例相@,該初級 線圈段11的繞線徑度大於該次級線圈段12的繞線徑度, 因此可以得到與該第一較佳實施例溫效果。2外 ’將該第-鐵芯41相對該第二鐵芯42做橫向移動時,可 改變該初級磁通區43、次級磁通區44的有效截面積,藉此 控制通過該初級磁通區43、次級磁通區44的磁通量的^小 〇 由以上數個實施例可知,本發明不但可降低初級線圈 14 200841364 溫升,並藉由一個可以控制洩漏磁束的結構以使左右磁阻 對稱,同時降低實際製造時所需耗費的成本,增加可量產 性。 惟以上所述者,僅為本發明之數個較隹實施例而已, 當不能以此限定本發明實施之範圍,即大凡依本發明申請 專利範圍及發明說明内容所作之簡單的等效變化與修飾, 皆仍屬本發明專利涵蓋之範圍内。 【圖式簡單說明】 圖1是本新型變壓器一第一較佳實施例的一分解立體 圖; 圖2是一第一鐵心與一第二鐵心的分解立體圖,說明 該第一鐵心與該第二鐵心的不同組成形狀; 圖3是該第一鐵心與該第二鐵心的分解立體圖,說明 該第一鐵心與該第二鐵心的不同組成形狀; 圖4是該第一鐵心與該第二鐵心的分解立體圖,說明 該第一鐵心與該第二鐵心的不同組成形狀; 圖5是該第一鐵心與該第二鐵心的分解立體圖,說明 該第一鐵心與該第二鐵心的不同組成形狀; 圖6是該第一鐵心與該第二鐵心的分解立體圖,說明 該第一鐵心與該第二鐵心的不同組成形狀; 圖7疋該第一較佳實施例的一組合側視圖,說明移動 該第二鐵芯後的狀態; 圖8是本新型變壓器一第二較佳實施例的一缸合側視 圖,說明移動該第二鐵芯後的狀態; 15 200841364 圖9是本新型變壓器一第三較佳實施例的一分解立體 圖; , 圖10是是本新型變壓器一第四較佳實施例的一分解立 體圖; 、 圖11是該第四較佳實施例的一組合俯視圖; 圖12是本新型變壓器一第五較佳實施例的一組合側視 圖, 圖13是該禁五較佳實施例的一分解立體圖;及 圖14是本新型變壓器一第六較佳實施例的分解立體圖The imaginary line indicates that the third preferred embodiment is substantially the same as the first preferred embodiment, except that the bobbin unit $i includes two primary bobbins 15 forming the primary coil segment U, and four Each of the secondary bobbins 16 forming the secondary coil section 12 is formed. The core unit 4 includes two first cores 41 disposed opposite to the bobbin unit 1 , a second iron anger 42 connected to the two first cores 41 , and two formed on the first iron a primary magnetic flux region 43 between the core 41 and the second core 42 adjacent to the primary bobbin 15, and two formed between the two first cores 41 and the second core 42 and adjacent to the secondary coil The magnetic flux leakage region 45 of the shelf 16. The second core 42 has two magnetically permeable ends 426 respectively corresponding to the two magnetic flux barriers. Alternatively, the secondary bobbins 16 may be integrally formed to reduce the original four secondary bobbins 16 to two. Further, the primary bobbin 15 12 200841364 is the same as the first preferred embodiment, and may be disposed between the first core 41 and the second core 42 along a Y axis perpendicular to the X-axis direction. In use, the third preferred embodiment has the same effect as the first preferred embodiment, and can simultaneously lower the temperature rise of the primary coil and adjust the bubble bubble of the coil to make the left and right magnetoresistances symmetrical. Further, by adjusting the contact area of the magnetically permeable end portion with the magnetic flux leakage region 45, the leakage magnetic flux can be adjusted to achieve a desired inductance value. As shown in Figs. 11, the fourth embodiment of the present invention will be further described, including a bobbin unit 1, a primary coil 2, a primary coil 3 and a core unit 4. The bobbin unit 1 includes a primary coil section 11 and a primary coil section 12, the primary coil section u having a winding diameter greater than the winding diameter of the secondary coil section 12. The core unit 4 is assembled to the bobbin unit 1 and includes a first core 41 ′, which is connected to the bobbin unit i, and a second core 42 connected to the first core ο. a primary magnetic flux region 43 formed between the first core 41 and the second core 42 and adjacent to the primary coil 2, and a gap between the first core 41 and the second core 42 In addition, the second magnetic core 42/, "the young iron 41" forms a magnetic path connecting the primary coil 2 and the secondary coil 3. Only the embodiment is the same as the first preferred embodiment, the winding diameter of the primary coil segment 11 is greater than the winding implant of the secondary coil segment 12, so that it can be the same as the first preferred embodiment. The cooling effect is as shown in FIG. 12, and the fifth preferred embodiment of the present invention will be further described below. The fifth preferred embodiment is the same as the above-mentioned fourth preferred embodiment 13200841364, the difference being that The bobbin unit i further includes a through hole i3, and an air gap 14°. The first core 41 is disposed through the through hole, and the diameter of the first iron 41 is smaller than The air gap 14 is formed between the diameter of the through hole 13 and the through hole. In the embodiment, the ratio of the cross-sectional area of the first core 41 to the cross-sectional area of the through hole 13 is 1.6. The air gap 14 is available. The third core 45 is pierced, thereby obtaining a better magnetic permeability. The use of the embodiment is the same as the first preferred embodiment, and the winding diameter of the primary coil segment 11 is larger than the secondary coil. The winding diameter of the segment 12, so that the same cooling effect as that of the first preferred embodiment can be obtained. - As shown in Fig. 14, the following will describe the sixth preferred embodiment of the present invention. The sixth preferred embodiment is different from the fourth preferred embodiment described above in that the second core 42 has two primary portions respectively formed at opposite ends of the first core and in contact with the first iron & 41 The contact surface 42 is a secondary contact surface 422. The area of the primary contact surface 421 and the secondary contact surface is not less than the effective sectional area of the primary magnetic flux region 43 and the secondary magnetic flux region 44. In this embodiment, the embodiment In contrast to the first preferred embodiment, the winding diameter of the primary coil segment 11 is greater than that of the secondary coil segment 12. The wire diameter can be obtained, so that the temperature effect of the first preferred embodiment can be obtained. When the second core 41 is laterally moved relative to the second core 42, the primary magnetic flux region 43 can be changed. The effective cross-sectional area of the level magnetic flux region 44, thereby controlling the magnetic flux passing through the primary magnetic flux region 43 and the secondary magnetic flux region 44, is known from the above several embodiments, and the present invention can not only reduce the primary coil 14 200841364 Temperature rise, and by a structure that can control the leakage magnetic flux to make the left and right magnetic reluctance symmetrical, while reducing the cost required in actual manufacturing, and increasing mass productivity. However, the above is only a few of the present invention. The scope of the present invention is not limited by the scope of the invention, and the simple equivalent changes and modifications made by the present invention are still within the scope of the present invention. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is an exploded perspective view of a first preferred embodiment of the present invention; FIG. 2 is an exploded perspective view of a first core and a second core illustrating the first core and the second core FIG. 3 is an exploded perspective view of the first core and the second core, illustrating different shapes of the first core and the second core; FIG. 4 is an exploded view of the first core and the second core 3 is a perspective view showing a different composition of the first core and the second core; FIG. 5 is an exploded perspective view of the first core and the second core, illustrating different shapes of the first core and the second core; An exploded perspective view of the first core and the second core, illustrating different shapes of the first core and the second core; FIG. 7 is a combined side view of the first preferred embodiment, illustrating moving the second Figure 8 is a side view of a second preferred embodiment of the transformer of the present invention, illustrating the state after moving the second core; 15 200841364 Figure 9 is a third preferred embodiment of the present invention. FIG. 10 is an exploded perspective view of a fourth preferred embodiment of the present invention; FIG. 11 is a combined top view of the fourth preferred embodiment; FIG. A side view of a fifth preferred embodiment, FIG. 13 is an exploded perspective view of the fifth preferred embodiment; and FIG. 14 is an exploded perspective view of a sixth preferred embodiment of the novel transformer.
16 200841364 【主要元件符號說明】 1 ·……· …·繞線架單元 413… •-…弟一侧面 11…… …·初級線圈段 414… ••…第 内面 12…… •…次級線圈段 42"… …··第二鐵芯 13…… •…穿孔 42卜· …··初級底面 14 氣隙 422… •…·次級接觸面 15…… 初級線圈架 423··· ••…次級端部 16·"·" …·次級線圈架 424… ••…第二側面 2.......* •…初級線圈 425… …··第二内面 3*……· …·次級線圈 426… ••…調磁端部 4 •…鐵芯單元 427… …··初級端部 41…… …··第一鐵芯 43"··. •…·初級磁通£ 411 ------初級段 44·.··· •…·次級磁通區 412… 次級段 45·* … •…·漏磁Εΐ16 200841364 [Description of main component symbols] 1 ······The bobbin unit 413... •-...The younger side 11... The primary coil section 414... ••...The inner surface 12... •...Secondary coil Segment 42"...the second core 13...•...perforation 42b...the primary bottom surface 14 air gap 422...•...·secondary contact surface 15... primary coil frame 423··· ••... Secondary end portion 16·"·" .... secondary bobbin 424... ••...second side 2.......* •...primary coil 425... ..... second inner surface 3*... ·...·Secondary coil 426... ••...Magnetizing end 4 •...core unit 427...···primary end 41.........··First core 43"··. £ 411 ------ Primary section 44·.···•...·Second flux zone 412... Secondary section 45·* ... •...·Leakage magnet
1717
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Publication number | Priority date | Publication date | Assignee | Title |
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CN110221159A (en) * | 2019-07-18 | 2019-09-10 | 杭州电力设备制造有限公司 | A kind of fault detection method, system and the equipment of the transformer based on iron core leakage field |
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Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
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CN110221159A (en) * | 2019-07-18 | 2019-09-10 | 杭州电力设备制造有限公司 | A kind of fault detection method, system and the equipment of the transformer based on iron core leakage field |
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