TWI354735B - - Google Patents

Download PDF

Info

Publication number
TWI354735B
TWI354735B TW097130507A TW97130507A TWI354735B TW I354735 B TWI354735 B TW I354735B TW 097130507 A TW097130507 A TW 097130507A TW 97130507 A TW97130507 A TW 97130507A TW I354735 B TWI354735 B TW I354735B
Authority
TW
Taiwan
Prior art keywords
point
fan
air
suction port
mouth
Prior art date
Application number
TW097130507A
Other languages
Chinese (zh)
Other versions
TW201002944A (en
Inventor
Okazawa Hiroki
Tsutsumi Hiroshi
Yamatani Takahiro
Nishimiya Kazunobu
Kawanori Yukihiko
Original Assignee
Mitsubishi Electric Corp
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
Family has litigation
First worldwide family litigation filed litigation Critical https://patents.darts-ip.com/?family=41506762&utm_source=google_patent&utm_medium=platform_link&utm_campaign=public_patent_search&patent=TWI354735(B) "Global patent litigation dataset” by Darts-ip is licensed under a Creative Commons Attribution 4.0 International License.
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Publication of TW201002944A publication Critical patent/TW201002944A/en
Application granted granted Critical
Publication of TWI354735B publication Critical patent/TWI354735B/zh

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F04POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
    • F04DNON-POSITIVE-DISPLACEMENT PUMPS
    • F04D29/00Details, component parts, or accessories
    • F04D29/40Casings; Connections of working fluid
    • F04D29/42Casings; Connections of working fluid for radial or helico-centrifugal pumps
    • F04D29/4206Casings; Connections of working fluid for radial or helico-centrifugal pumps especially adapted for elastic fluid pumps
    • F04D29/4213Casings; Connections of working fluid for radial or helico-centrifugal pumps especially adapted for elastic fluid pumps suction ports
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F04POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
    • F04DNON-POSITIVE-DISPLACEMENT PUMPS
    • F04D29/00Details, component parts, or accessories
    • F04D29/40Casings; Connections of working fluid
    • F04D29/42Casings; Connections of working fluid for radial or helico-centrifugal pumps
    • F04D29/4206Casings; Connections of working fluid for radial or helico-centrifugal pumps especially adapted for elastic fluid pumps
    • F04D29/4226Fan casings
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F04POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
    • F04DNON-POSITIVE-DISPLACEMENT PUMPS
    • F04D29/00Details, component parts, or accessories
    • F04D29/66Combating cavitation, whirls, noise, vibration or the like; Balancing
    • F04D29/661Combating cavitation, whirls, noise, vibration or the like; Balancing especially adapted for elastic fluid pumps
    • F04D29/667Combating cavitation, whirls, noise, vibration or the like; Balancing especially adapted for elastic fluid pumps by influencing the flow pattern, e.g. suppression of turbulence

Description

1^54735 九、發明說明: 【發明所屬之技術領域】 本發明係有關於西洛可風扇及使㈣ 尤其係有關於作成降低所產生之聲音的西各工調裝 使用該風扇之空調裝置。 的西洛可風扇及 【先前技術】 自以往,存在—種係多葉片離心 ^並可對空調對象區域吹出寬度寬之帶狀的風具有圓筒 I:扇’常利用於構成空調裝置之室内 二西洛 虱清淨機等。這種 次除濕機、空 板排列於圓周上而敕俨卜士間& 支,、田長的葉片 吸入口及吹出出/ 圓靖形的風扇,收容於已形成 及人出出的竭形殼而構成。而, 城 口將空氣吸入内邛,计…曲〜可風扇從吸入 N 口!5並攸吹出口側對空胡#4_ & 取入的空氣。 。對象區域吹出所 作為那種西洛可風扇’提議「一種 彼此間以空間沿著 葉片風扇,包括: 式風斧… 轉軸所連結之複數個乡葉片離心 式風扇早兀、及用以收容該連結之複數個^ 4 扇單元的外超,h 數個夕葉片離心式風 式風戶二 該外殼形成用以將從該複數個多葉片離心 八風扇早元所排屮命# 7示 ^ 出用β ^吹出用流路’該吹 共同的、、,路,二複數個多葉片離心式風扇單元所速續之 门的机路」(例如,參照專利文獻丨)。 專利文獻1 :特開平1 1 — 324984 π、 ^ 7^8圖) .4唬公報(第5貢,第1^54735 IX. Description of the Invention: [Technical Field of the Invention] The present invention relates to a sirocco fan and a (4) air conditioner which uses the fan in particular for the purpose of making a sound for reducing the sound generated. The sirocco fan and the [prior art] Since the past, there has been a multi-blade centrifugation of the seed system, and it is possible to blow a wide strip of wind to the air-conditioned object area. The cylinder I: the fan is often used in the interior of the air-conditioning apparatus. Second Xiluojing cleaning machine and so on. The sub-dehumidifier and the empty plate are arranged on the circumference, and the 敕俨士间& 支, the Tian Chang's blade suction port and the blow-out/round-shaped fan are housed in the formed and human out-out shape. Composed of shells. However, the city mouth draws air into the inner sputum, count... ~ fan can suck in from the N port! 5 and blew the outlet side to the air hu #4_ & . The object area is blown out as the kind of Syracuse fan 'proposal'. A plurality of township blade centrifugal fans connected to each other by space along the blade fan, including: a wind axe... The outer plurality of ^ 4 fan units, h the number of eve leaves centrifugal wind type wind house two, the outer casing is formed to be used for the plurality of multi-blade centrifugal eight fans The β ^ blowout flow path 'the common path of the door of the two-blade centrifugal fan unit of the common multi-blade centrifugal fan unit is blown by the flow path' (for example, refer to the patent document 丨). Patent Document 1: Special Kaiping 1 1 - 324984 π, ^ 7^8 Figure) . 4唬 Bulletin (5th Gong, No.

2148-9915-PF 5 1354735 【發明内容】 【發明要解決之課題】 在以往之多葉片風扇,在動作點之損失係數小,且動 於比不安定區域更接近開放側的情況,具有風扇之 :寬乍、在既定風量時所產生之噪音變大的課題。即在 這種西洛可風扇’在將既定量之風量供給2148-9915-PF 5 1354735 [Problem to be Solved by the Invention] In the conventional multi-blade fan, the loss coefficient at the operating point is small, and the fan is moved closer to the open side than the unstable region. : The problem that the noise generated when the air volume is large and the volume is increased. That is, in this kind of siro fan, the air volume is supplied in a quantitative manner.

時,從風扇所產生之聲音變大,而成為噪音,並傳 對象區域,令使用者覺得不舒服。又,若降低既定啤音值, 則來自西洛可風扇的吹出風量變,卜若使吹出風量變大, 則噪音值變大’而亦具有難取得吹出風量和聲音的產生之 適當的平衡。X,在風扇寬度窄、損失係數小的情況,為 了使噪音變小’亦具有必須使風扇直徑過度地變大之課 題。此外,在將這種西洛可風扇用於空調裝置的情況,若 風扇寬度窄,在熱交換器位於風扇下游側的情況,熱交換 器之寬度方向的速度分布變成不均勻,而熱交換器的導熱 性能降低,亦具有壓縮機之耗電力增加的課題。又,亦具 有損失係數和風扇寬度之關係不明確的課題。 本發明係為了解決上述之問題而開發者,其目的在於 提供西洛可風扇及使用該風扇之空調裝置,而該風扇作成 降低在供給既定量之吹出風量時所產生的聲音。 【解決課題之手段】 本發明之西洛可風扇,包括:蝸形殼,係具有用以取 入空氣的吸入口、用以吹出空氣的吹出口、以及從該吸入 口至該吹出口的風路;風扇,係被收容於該蝸形殼内,藉 2148-9915-PF 6 1354735 由進行轉動驅動而從該吸入口取入空氣並從該吹出口吹 出空氣;以及鈴嘴,係安裝於該蝸形殼的該吸入口;其特 徵在於:在該吸入口位於該風扇之轉動中心的延長線上, 並形成於該蜗形殼的兩側面者’設在該風路内之通風阻力 為P[Pa]、從該吸入口所取入之空氣的量為Q[mVmin]、該At this time, the sound generated from the fan becomes large, and becomes noise, and the object area is transmitted, making the user feel uncomfortable. Further, when the predetermined beer sound value is lowered, the amount of blown air from the sirocco fan is changed, and if the blown air volume is increased, the noise value is increased, and it is difficult to obtain an appropriate balance between the blown air volume and the sound. X, in the case where the fan width is narrow and the loss coefficient is small, the noise is made small, and there is a problem that the fan diameter must be excessively increased. Further, in the case where such a sirocco fan is used for an air conditioner, if the fan width is narrow, when the heat exchanger is located on the downstream side of the fan, the speed distribution in the width direction of the heat exchanger becomes uneven, and the heat exchanger The thermal conductivity is reduced, and the power consumption of the compressor is also increased. Moreover, there is also a problem that the relationship between the loss coefficient and the fan width is not clear. The present invention has been made in an effort to solve the above problems, and an object of the invention is to provide a sirocco fan and an air conditioner using the same, and the fan is configured to reduce sound generated when a predetermined amount of blown air is supplied. [Means for Solving the Problem] The sirocco fan of the present invention includes: a volute casing having a suction port for taking in air, a blow port for blowing air, and a wind from the suction port to the blow port. a fan; the fan is housed in the volute casing, and is driven by the rotation of 2148-9915-PF 6 1354735 to take in air from the suction port and blow air from the air outlet; and the bell mouth is mounted on the The suction port of the volute casing; characterized in that: the suction port is located on an extension line of the center of rotation of the fan, and the ventilation resistance formed in the air path of the two sides of the volute casing is P [ Pa], the amount of air taken in from the suction port is Q [mVmin], the

風扇之轉軸方向的寬度為L[mm]、k為常數、該蝸形殼的 咼度為 H = 246k[mm]、P/Q2 為損失係數 f [pa/(m3/min) 2] 的情況,在0. 1 S k4 f各〇. 4之範圍,作成f(k4 F ) = 〇. 34947(k4 f )2 - I - 〇554(k4 ^ ) + ι, 8 , 〇. 75f (k4 ^ L/HS f (k4 f )。 本發明之西洛可風扇’包括:蝸形殼,係具有用以取 入空氣的吸入口 1以吹出空氣的吹出口、以及從該吸入 口至忒π人出口的風路,風扇,係被收容於該蝸形殼内,藉 由進行轉動驅自而從該吸A口取入$氣並從該吹出口吹 出空氣;以及鈴嘴,係安裝於該蝸形殼的該吸入口;其特 徵在於:在該吸人口位於該風扇之轉動中心的延長線上, 並形成於該蜗形殼的單側面者,設在該風路内之通風阻力 為P[Pa]、從該吸入口所取入之空氣的量為Q[mVmin]、該 風扇之轉軸方向的見度$ L[mm]、k為常數 '該蝸形殼的 高度為 H = 246k[mm]、P/q2 為損失係數 f [pa/(m3/min) 2] 的凊况,在〇. 1 - k4 t客〇· 4之範圍,作成g(k4 ^)-1. 3 9788(k4 ξ )2- 2. ll〇8(k4 ^) + 1.8- 1. 5g(k4 ^ ) ^ L/H S 2g(k4 f )。 又,本發明之空調裝置,其特徵在於^使用上述之西The width of the fan in the direction of the rotation axis is L [mm], k is constant, the vortex case has a twist of H = 246 k [mm], and P/Q2 is the loss factor f [pa/(m3/min) 2]. , in the range of 0. 1 S k4 f 〇. 4, made f(k4 F ) = 〇. 34947(k4 f )2 - I - 〇554(k4 ^ ) + ι, 8 , 〇. 75f (k4 ^ L/HS f (k4 f ). The sirocco fan of the present invention includes: a volute casing having a suction port 1 for taking in air to blow out air, and from the suction port to the 忒π person The outlet air passage and the fan are housed in the volute casing, and the air is taken from the suction port A by blowing and the air is blown from the air outlet; and the bell mouth is attached to the worm The suction port of the casing; characterized in that: the suction resistance is located on an extension line of the center of rotation of the fan, and is formed on one side of the volute casing, and the ventilation resistance in the air passage is P[Pa ], the amount of air taken in from the suction port is Q [mVmin], the visibility of the fan in the direction of the axis of rotation is $ L [mm], and k is a constant 'the height of the volute case is H = 246 k [mm] , P/q2 is the loss coefficient f [pa/(m3/min) 2] In the case of 〇. 1 - k4 t客〇·4, make g(k4 ^)-1. 3 9788(k4 ξ )2- 2. ll〇8(k4 ^) + 1.8- 1. 5g( K4 ^ ) ^ L/HS 2g(k4 f ). Further, the air conditioner of the present invention is characterized in that the above-mentioned west is used

2148-9915-PF 7 1354735 洛可風扇。 【發明效果】 若依據本發明之西洛可風扇,只是根據既定之數學式 決定風扇寬度,以使風扇的動作點位於既,因為 可使空氣之吹出風量和噪音取得均衡,所以可有效地降低 在供給既定量之吹出風量時所產生的聲音。 【實施方式】 以下,根據圖面說明本發明之實施形態。 第1實施形態 第1圖係透視本發明之第1實施形態的西洛可風扇 1。〇之内部而表示的透視立體圖。第2圖係表示風扇工之 整體形狀的立體圖。第3圖係表 一 固V'衣不西洛可風扇1 〇〇之剖面 構造的示意縱向剖面圖。根據第 低爆弟i圖〜第3圖,說明西洛 可風扇100之整體構造。此西洛 合J風扇10 〇係利用於構成 冷氣機或除濕機等之空調裝詈的 门展罝的至内機、或除濕機、空氣 >月淨機等者。此外,包含第1 ” 已3弟1圖在内,在以下之圖面,有 各構成構件之尺寸的關係和實際者相異之情況。 如第1圖所示,西洛可涵彦1Λ 西洛了風扇100由以下之構件構成, 風扇1 ’係將複數支細長的荦片柘f K W茱片板(業片)排列於圓周 而整體變成圓筒形,·蝸形殼2 風扇1,並在内部 元成風路;以及鈴嘴3,係風们之轉動中心 (以下僅稱為轉軸上),並安裝 、線上 之兩側面。風扇 "有轉動中心’藉由轉動而吸人空氣,並吹出該空氣。2148-9915-PF 7 1354735 Roco fan. [Effect of the Invention] According to the sirocco fan of the present invention, the width of the fan is determined according to a predetermined mathematical formula so that the operating point of the fan is located, and the air volume and noise of the air can be equalized, so that the fan can be effectively reduced. The sound produced when a certain amount of air is blown out. [Embodiment] Hereinafter, embodiments of the present invention will be described based on the drawings. (First Embodiment) Fig. 1 is a perspective view of a sirocco fan 1 according to a first embodiment of the present invention. A perspective perspective view of the inside of the cymbal. Fig. 2 is a perspective view showing the overall shape of the fan. Figure 3 is a schematic longitudinal section of the structure of a solid V' 衣西西洛可可11. According to the second low-fidelity i-Fig. 3, the overall structure of the sirocco fan 100 is illustrated. This Xiluo J Fan 10 is used in an internal air conditioner, a dehumidifier, an air, a moon cleaner, etc., which constitutes an air conditioner of an air conditioner or a dehumidifier. In addition, in the following drawings, the relationship between the dimensions of the respective constituent members and the actual ones is included in the following drawings. As shown in Fig. 1, Siro Khanhiko 1Λ The fan 100 is composed of the following members, and the fan 1' is formed by arranging a plurality of elongated 柘 柘 茱 茱 茱 业 业 而 而 而 而 而 排列 , , , , , , , , , , , · · · · · · · · 蜗 蜗 蜗In the inner element, the wind path; and the bell mouth 3, the center of rotation of the winds (hereinafter referred to as the rotating shaft only), and the two sides of the line are installed. The fan "the center of rotation' attracts air by turning, And blow out the air.

2148-9915-PF 8 蜗形殼2由以下之槎件错^、 „ 0 .卜之構件構成,吸入口 2a,係形成於轉軸上 、開口丄吹出口 2b,係向對象區域吹出從吸入口 “所吸 入的空氣;以及風路2c,係朝向風扇1之轉動圓周方向形 成蜗形殼形狀(曲線形狀),並使吸入口 2a和吹出口 铃嘴3係加工開口而形成,並安裝於堝形殼2的吸入 口 2a’作成可將從吸人σ 2a所取人之空氣集巾增速並供 給風扇1。風扇i能以例如“92mm構成風扇直徑D,以例 如15〇〜偏咖構成寬度尺寸l,以例如4Q片構成葉片板 數蝸形殼2能以246mm構成螞形殼高度η。此外,未特 別限疋鈴嘴3的形狀’例如可因應於風扇直徑D之長度而 決定, 第4圖係表示西洛可風扇1〇〇之p—Q特性及Ks—q 特性的圖形。根據第4圖,說明西洛可風扇100的P—q 特f及KS—Q特性。在此,P表示靜l[Pa],Q表示風量 [m /min] ’ Ks表不比噪音[dB]。又,比嗓音Ks係根據數 學式Ks=SPL—10Μ吻。(P.Q2 5)所算出者。此外,SPL表 示噪音值,使用在從安裝於蝸形殼2之吸入口 2a的鈴嘴3 之中心’沿著轉軸上距_ lm心立i,測量從西洛可風 扇1 00所產生之噪音的值。又,黑圓形記號表示p— Q特 性’而空白圓記號表示Ks— Q特性。此外⑴~⑺表示 動作點。 P— Q特性係表示在風扇丨之轉速固定的狀態,係通風 阻力之靜壓P(左側縱軸)和風量Q(橫轴)的關係。如第4 2148-9915-PF 9 1354735 圖之黑圓形記號所示,静摩合丨士 ^. ^ 靜麼愈小在風路2c風愈易流動, 而靜壓愈大在風路2c風俞錐、丈t /0、 θ L剪難々丨L動。即,在動作點(3 ),易 得到風量,在動作點Μ彳 热π (1)難侍到風量。因此,靜壓愈小 風量愈大,而靜愿愈大風量愈小。此外,在以下的說明, 將回靜壓且低風里側稱為關閉側(圖形的左上側),而將低 靜虔且高風量側稱為開放側(圖形的右下側)。 但,如第4圖所示,局部性存在即使風量變小,靜屢 亦變小的區域。將此區域 + 场稱马不女疋(surging)區域(在第 4圖所示之虛線包圍區域)。 x ; 在;^種不安定區域,在風路 2c内之空氣的流動易變赤尤立^ 视勿受成不文心。即,不安定區域係因空 氣的流動不安定而成為異常音之原因的可能性高之區 域此外,比噪音Ks(右側縱軸)如帛4圖之空白圓記號所 示,風量Q增加時變大。此比„品立 j文八此比本音Ks係考慮到靜壓P和 風量Q的噪音值。 第5圖係表示西洛可風扇1〇〇之L。爪和損失係數^ 的關係之圖形。根據第5圖,說明西洛可風扇j 〇 〇之l。/^ :損失係數的關係。此第5目,係將蝸形殼高度汛固 定為246關,使風扇寬度尺寸L()在15〇5〇〇關之間變化, 使用對損失係數奪[叫3/1^)2],比噪音“變 成最,之寬度尺寸L。,表示WH。和損失係數^的關係。 在此第5圖,縱軸表示Ld/h。,橫軸表示損失係數铲〇。 損失係數f D= pD/QD2 ’在第4圖所示之p〜Q特性上, 表示損失係數I:。愈大愈接近關閉側,損失係數t。愈小愈 接近開放側。此外,損失係數係根據後述之動作點(p Q) 2148-9915-PF 10 的位置而求侍的值。又,L(>/h。表示將蝸形殼高度Η。固定, 而改變寬度尺寸L。之情況的比例。從第5圖得知,根據損 失係數可知比噪音Ks變成最小之寬度尺寸產生變 ^亦即,愈疋知失係數^ °小之開放側,比噪音Ks變成 句J之I度尺寸L。愈長。因此,自第5圖,在將損失係數 2 »又為0. 1 $ $ $ 〇_ 4之範圍的情況,設f ( f ) = 〇. 34947 L〇/H〇= f(g)時,比噪音 Ks 變成最 _此外 f(f)-〇.34947f2-i.〇554m.8 係從第 5 圖 所示之圖形所算出的式子。 其次,說明比噪f Ks因損失係數卜及寬度尺寸L。 而變化的理由。 第6圖係表示將寬度尺寸L。設為230或30〇mm,通過 動作點A之情況的西洛可風们〇〇之P-Q特性及Ks-Q 特性的圖形。又,黑圓形記號表示寬度尺寸匕為23〇咖之 障况的P—Q特性,而空白圓記號表示寬度尺寸L。為3〇〇咖 之凊況的P—Q特性’黑三角形記號表示寬度尺寸L〇為 23〇mm之情況的Ks—主u· _ ^ S y特性,而空白三角形記號表示寬度 尺寸^為300_之情況的Ks—Q特性。此外,在此所說明 之動作點係根據單%之設計風量、及設計靜壓(熱交換器 之通風阻力、或單元的風路、管之風路的通風阻力、過濾 器等之通風阻力)而決定。 在字寬度尺寸L〇 β又為23 〇mm、3 0 0ram的情況,比較通 過動作點A之P—Q特性時,得知寬度尺寸L。比較長的 300mm,不女定區域移至p— Q特性之圖形的右下(開放2148-9915-PF 8 The volute casing 2 is composed of the following components: 构件 0. The suction port 2a is formed on the rotating shaft, and the opening 丄 blowing port 2b is blown out from the suction port to the target area. "The air to be sucked; and the air passage 2c are formed in a spiral shape (curved shape) toward the circumferential direction of the rotation of the fan 1, and the suction port 2a and the outlet bell 3 are formed by machining openings, and are attached to the crucible. The suction port 2a' of the casing 2 is formed to increase the speed of the air collecting towel taken from the suction σ 2a and supply it to the fan 1. The fan i can constitute a fan diameter D of, for example, "92 mm", and a width dimension l of, for example, 15 Å to 255. The volute case 2 can be formed by 246 mm, for example, by a 4Q piece. The shape of the bell mouth 3 can be determined, for example, according to the length of the fan diameter D, and Fig. 4 is a graph showing the p-Q characteristics and Ks-q characteristics of the sirocco fan. According to Fig. 4, Explain the P-q special f and KS-Q characteristics of the Silo fan 100. Here, P denotes static l[Pa], Q denotes air volume [m /min] 'Ks is not better than noise [dB]. Ks is calculated according to the mathematical formula Ks=SPL—10Μ. (P.Q2 5). In addition, SPL indicates the noise value, which is used along the center of the bell mouth 3 attached to the suction port 2a of the scroll case 2. On the axis of the rotation, the distance from the _lm heart is measured, and the value of the noise generated from the sirocco fan 100 is measured. Further, the black circle mark indicates the p-Q characteristic' and the blank circle mark indicates the Ks-Q characteristic. In addition (1)~ (7) indicates the operating point. P-Q characteristic indicates the static pressure P (left vertical axis) and air volume Q of the ventilation resistance in the state where the fan speed is fixed. The relationship of the axis. As shown in the black circle mark of the 4 2148-9915-PF 9 1354735, the static and the gentleman ^. ^ The quieter the smaller the wind, the wind is more likely to flow, and the static pressure is larger. In the wind road 2c wind Yu cone, Zhang t / 0, θ L cut difficult to move L. That is, at the operating point (3), easy to get the air volume, hot point π (1) at the operating point is difficult to serve air volume. Therefore, the smaller the static pressure is, the larger the air volume is, and the smaller the static air volume is, the smaller the air volume is. In addition, in the following description, the static pressure and the low wind side are referred to as the closing side (the upper left side of the figure), and the static is low. The high air volume side is called the open side (the lower right side of the figure). However, as shown in Fig. 4, there is a localized area where the air volume becomes smaller and the static frequency becomes smaller. The surging area (the area enclosed by the dotted line shown in Fig. 4). x ; In the unstable area, the flow of air in the wind path 2c is liable to change. The heart, that is, the area where the unstable area is highly likely due to the instability of the air flow and becomes the cause of the abnormal sound. In addition, the noise than the noise Ks (right vertical axis) is as shown in Fig. 4 When the mark becomes larger as shown, the wind amount Q increases. This ratio "j Li Wen eight this product than Ks this sound system and taking into account the static pressure P of the air flow rate Q noise value. Fig. 5 shows the L of the sirocco fan. A graph of the relationship between the claw and the loss factor ^. According to Fig. 5, the sirocco fan j 〇 〇 l is illustrated. /^ : The relationship of the loss factor. In the fifth item, the height of the snail shell is fixed to 246, and the fan width dimension L() is changed between 15 and 5, and the loss coefficient is used to call [3/1^) 2]. The specific noise "becomes the most, the width dimension L., which represents the relationship between WH and the loss coefficient ^. In Fig. 5, the vertical axis represents Ld/h. The horizontal axis represents the loss coefficient shovel. Loss factor f D = pD /QD2 'In the p to Q characteristics shown in Fig. 4, the loss coefficient I is shown. The larger the closer to the closing side, the smaller the loss coefficient t. The smaller the closer to the open side, the more the loss coefficient is based on the action point described later. (p Q) The value of the position of 2148-9915-PF 10. Further, L(>/h. indicates the ratio of the case where the height of the volute case is fixed, and the width dimension L is changed. It can be seen from Fig. 5 that according to the loss coefficient, it is known that the width dimension which becomes smaller than the noise Ks is changed, that is, the open side where the smaller the gain coefficient is smaller than the noise Ks becomes the I degree dimension L of the sentence J. The longer the length is. Therefore, from Figure 5, in the case where the loss factor 2 » is in the range of 0. 1 $ $ $ 〇 _ 4, let f ( f ) = 〇. 34947 L〇/H〇 = f(g), ratio The sound Ks becomes the most _ in addition f(f)-〇.34947f2-i.〇554m.8 is the equation calculated from the graph shown in Fig. 5. Secondly, the noise ratio f Ks due to the loss coefficient and the width dimension is explained. L. Reasons for the change. Fig. 6 is a graph showing the PQ characteristics and the Ks-Q characteristics of the sirloin of the case where the width dimension L is 230 or 30 〇 mm and the action point A is passed. Further, the black circular mark indicates the P-Q characteristic of the width dimension 〇 23 ,, and the blank circle mark indicates the width dimension L. The P-Q characteristic of the 3 〇〇 凊 condition 'black triangle mark indicates The Ks-main u· _ ^ S y characteristic in the case where the width dimension L 〇 is 23 〇 mm, and the blank triangle mark indicates the Ks-Q characteristic in the case where the width dimension ^ is 300 _. Further, the action point explained here It is determined according to the design air volume of single %, and the design static pressure (ventilation resistance of the heat exchanger, or the air path of the unit, the ventilation resistance of the air passage of the pipe, the ventilation resistance of the filter, etc.). When β is 23 〇mm or 300 ram, the width is known when the P-Q characteristic of the operating point A is compared. L. inch longer 300mm, female given region do not move to Q characteristic pattern of p- lower right (open

2148-9915-PF 1354735 侧),而:近動作點A。從第6圖所示之卜 Q特ϋ得知比臂音Ks變成最小的動作點位於不安定 =二旦’動作點位於不安定區域或不安定區域附近:: -動丈成不安定,發生逆吸入或異常音, =大。因此,在確實地形成安定之流動的情況: 使動作點位於比不安定區域更接近開放側。 即,對某動作點(p,Q),使風扇的容積 Q特性圖,不安定區域逐漸向右下移動。此時時動作在二 ―、或鈐嘴之和風:的在//圖* 大。在本發明,作成掛所^ 之£域,靜慶變動變 積變大,使不安定…動作點’藉由使風扇的容 量接近,使所使動作點和不安定 在此,a 了使風扇的容積變Α, 大,或使風扇的寬度變寬。可 ^至羽直控變 元高度變成過高。在本發明,可得::=直徑:大,單 單元高度變成過高,以風扇的寬度& ===不會使 用以可使動作點和不安定區域的關寬的方' 構成, 設置限制少,而且可降低•音。 變成最佳之早元的 第7圖係表示風扇2的每一片 ^ 葉片板的位置之關係的圖形。根據 《葉片間風量和 可風扇1 00之風扇!的每一片葉目’祝明構成西洛 板的位置之關係的圖形。在此第之葉片間風量和葉片 弟7圖,縱軸表示每—片葉2148-9915-PF 1354735 side), and: near action point A. It is known from the Bu Q special diagram shown in Fig. 6 that the action point that becomes smaller than the arm sound Ks is located in the unstable position = two denier's action point is located in the unstable area or the unstable area:: - The movement becomes unstable, occurs Reverse inhalation or abnormal sound, = large. Therefore, in the case where the steady flow is surely formed: the operating point is located closer to the open side than the unstable area. That is, for a certain operating point (p, Q), the volume Q characteristic map of the fan is gradually moved to the lower right side of the unstable area. At this time, the action is in the second, or the slap in the mouth: the // figure is large. In the present invention, the field of the opening is made, the static change variable becomes larger, and the rest is unstable... the action point 'by making the capacity of the fan close, so that the action point and the instability are made here, a The volume becomes louder, larger, or widens the width of the fan. The height of the direct control variable can be too high. In the present invention, it is possible to:: = diameter: large, the height of the single unit becomes too high, and the width of the fan & === is not used to make the action point and the square of the unstable area of the unstable area, Less restrictions, and can reduce the sound. Fig. 7 showing the optimum early element is a graph showing the relationship of the position of each blade of the fan 2. According to "the air volume between the blades and the fan of the fan 100! Each leaflet's figure shows the relationship between the positions of the West Plate. In this first blade air volume and blade 7 diagram, the vertical axis represents each leaf

2148-9915-PF 12 1354735 片板之葉片間風量(mVinin),橫軸表示葉片板的位置。又, 在第7圖,黑圓形記號表示在動作點(〇的每一片葉片板 之葉片間風量和葉片板的位置之關係,空白菱形記號表示 在動作點(2)的每一片葉片板之葉片間風量和葉片板的位 置之關係,黑三角形記號表示在動作點(3)的每一片葉片 板之葉片間風量和葉片板的位置之關係。2148-9915-PF 12 1354735 The air flow between the blades (mVinin), and the horizontal axis represents the position of the blade. Further, in Fig. 7, the black circular mark indicates the relationship between the air volume between the blades of each blade of the blade and the position of the blade plate at the operating point, and the blank diamond symbol indicates each blade blade at the operating point (2). The relationship between the air volume between the blades and the position of the blade plate, the black triangle symbol indicates the relationship between the air volume between the blades of each blade plate at the operating point (3) and the position of the blade plate.

1、^风领丄的母一片茱 片板之葉片間風量,以正表示風從葉片(葉片板)的内周側 在外周側之流動的情況’而以負表示風從葉片的外周側往 ^側第^ ’以時鐘的短針表達 ::斤:之葉:板的位置,,將葉片板的位置置換成在 刀分之時鐘的短針之位置來表達。此外, :二圖所示之動作點⑴,作點(3),表示和第彳圖所示 之動作點(1)〜動作點相同的動作點。 如第7圖所示,得知在葉片板的位置位於 附近的情況’愈往開放側葉片間風量愈大,刀 葉片間風量愈小。又,得知在9時30分〜U時〜。 的區域,葉片間風量未出現顯著 、77以外 ^ 左兵设葉片間Μ吾盔 ;“板片數為40片的情況’ i = 1, 值 饥、風扇輸入值W,大致以下所示之 ;J曰值 (2)式)成立。 予式(第(1)式及第 第⑴式 SPLd 1〇 · log.6 第(2)式 w〇c2 Qi3 噪音值SPL及 因此,葉片間風量Qi的分布愈均句 2148-99is-pr 13 1354735 風扇輸入值w愈小。即,如第4圖所示,在接近不安定區 域之動作點(1)的情況,因為葉片間風量Qi的分布係均 勻所以比噪音Ks變成最小值。在此,如上述所示,反 之動作點愈接近不安定區域,即愈接近h/IU= f(p),雖 d比噪音Ks變成愈小,但是超過f ( f )時,動作 點就位於不安定區域,比噪音Ks反而變差。另一方面, 動作點比不女疋區域愈遠離開放側,在殼之舌部(在第3 圖所不之2bl)、或鈴嘴之和風扇的距離短之區域,因為靜 屢變動變大,所以易產生異常音。 因此,设0<nS 1 ' L〇/He= nxf( I:。),在損失係數小之 條件(風量大,通風阻力小)的情況,即在〇1‘ $ 4 0.4 之範圍,求不產生異常音之最小的η時,係了5。因而, 在知失係數小之條件(風量大,通風阻力小)的情況,即在 0.1^60.4 之範圍,若是 〇75f(D^ L。/^ f (卜), 可形成比臂音Ks小、不會產生異f音的流動。 “、在上述的說明,說明蝸形殼高度Hd = 246觀的情況,接 著說明將蝸形设咼度之尺寸一般化的情況。設k為常數, H kH〇 L-kL〇、D = kD。。在尺寸變化的情況,自相似法則, 關於P & Q,以下所示之數學式(第(3)式及第⑷式)成 立。在此,N係轉速。 第(3)式 P = P〇(D/D〇)2(N/N〇)2 第(4)式 Q = Qd(D/D〇3(N/N。) 攸第(3)式及第(4)式,消去N/n。,整理後,得到第(5) 式。1. The air volume between the blades of the female slab of the wind collar is positively indicating the flow of wind from the inner peripheral side of the blade (blade plate) on the outer peripheral side, and negatively indicating the wind from the outer peripheral side of the blade ^ Side ^ ^ Expressed by the short needle of the clock:: Jin: The leaf: the position of the plate, the position of the blade plate is replaced by the position of the short needle of the clock of the knife. Further, the operating point (1) and the point (3) shown in the second figure indicate the same operating point as the operating point (1) to the operating point shown in the second drawing. As shown in Fig. 7, it is found that the position of the blade plate is located nearby. The larger the air volume between the blades on the open side, the smaller the air volume between the blades. Also, it is known that at 9:30 to U. In the area, the air volume between the blades did not appear significant, except 77. The left armor set the blade between the blades; the case of "the number of plates is 40" i = 1, the value of the hungry, the fan input value W, roughly as shown below; J 曰 (2) Formula is established. Formula (1) and Equation (1) SPLd 1〇·log.6 Equation (2) w〇c2 Qi3 Noise value SPL and, therefore, the air volume between the blades Qi The more uniform the distribution sentence 2148-99is-pr 13 1354735 The smaller the fan input value w is, that is, as shown in Fig. 4, in the case of the action point (1) close to the unstable zone, the distribution of the air volume Qi between the blades is uniform. Therefore, the specific noise Ks becomes the minimum value. Here, as shown above, the closer the action point is to the unstable region, the closer to h/IU=f(p), although d becomes smaller than the noise Ks, but exceeds f ( f), the action point is located in the unstable area, which is worse than the noise Ks. On the other hand, the action point is farther away from the open side than the non-female area, at the tongue of the shell (2bl in Fig. 3) Or the area where the distance between the bell mouth and the fan is short, because the static change becomes large, it is easy to generate abnormal sound. Therefore, let 00&n;nS 1 ' L〇/He= nxf( I:.), in the case where the loss coefficient is small (the air volume is large and the ventilation resistance is small), that is, in the range of 〇1' $ 4 0.4, the minimum η of the abnormal sound is not generated. It is 5. Therefore, in the case where the loss-of-loss coefficient is small (the air volume is large and the ventilation resistance is small), that is, in the range of 0.1^60.4, if 〇75f (D^L./^f (b), it can be formed. It is smaller than the arm sound Ks and does not cause the flow of the different f sounds. "In the above description, the case where the volute case height Hd = 246 is described, and the case where the size of the snail shape is generalized will be described. k is a constant, H kH 〇 L-kL 〇, D = kD. In the case of dimensional change, the self-similarity rule, about P & Q, the mathematical formula shown below (paragraphs (3) and (4)) Established here. N series speed. Equation (3) P = P〇(D/D〇)2(N/N〇)2 Equation (4) Q = Qd(D/D〇3(N/N .) 攸 Equations (3) and (4), eliminate N/n. After finishing, get the formula (5).

2148-9915-PF 14 1354735 第(5)式 P〇/Q〇2= p/q2(d/d。)3 將^ Ρ/(ΤΉΙ)β代人該第⑸式’而得到第⑻式。 第(6)式 f〇 = k4f 使用第(6)式及H = kH〇、L=kL❶,可將 0.1S f。客 0.4 —般化成 o.isvi;各 〇 4、 O.HfCfOsLo/HdfCf。)一 般化成 〇 75f(k $ L/HSf(k4f)。 — 即,在將風扇1用於在風扇之下游側包括熱交換写的 空調裝置之情況’在損失係數小之條件(風量大通風阻 力小)的情況’藉由使風扇寬度變寬,而因為噪音變小, 而且熱交換器之寬度方向的速度分布接近均勻,所以可不 會不必要地增加壓縮機的耗電力。 其次,說明西洛可風扇100為單吸入式的情況。 2. 1108(k4^ ) + 1.8^ 1. 5g(k4F )^L/H^ 2g(k^ 在西洛可風扇100為單吸入式的情況,在 之範圍’藉由作成,而—可升: 成比噪音Ks小、不會產生異常音的單元。 v 在上述的說明,雖然說明西洛可風扇1〇〇單 但疋對於將西洛可風扇⑽裝載於空調機 空氣清淨機等之單元的情況之動作點,亦可一樣地::: 在此情況’求單元之轉速N|、及單元的風量h,再從 可風扇1GG單體的p—Q特性,使用轉速&及風量q"求 將上述之L置換成l/2、將Q置換成Q/2即可。而, 若設 f{ P/(Q/2” },則 g(k彳)=139? ;2 )。即2148-9915-PF 14 1354735 Equation (5) P〇/Q〇2= p/q2(d/d.)3 The equation (8) is obtained by substituting ^ Ρ / (ΤΉΙ) β for the equation (5). Equation (6) f〇 = k4f Using Equation (6) and H = kH〇, L=kL❶, 0.1S f can be used. Guest 0.4 is generalized into o.isvi; each 〇 4, O.HfCfOsLo/HdfCf. Generalized into 〇75f (k $ L/HSf(k4f). - that is, in the case where the fan 1 is used for an air conditioner including a heat exchange write on the downstream side of the fan', the condition with a small loss coefficient (large air flow resistance) In the case of "small", the width of the fan is widened, and since the noise is reduced, and the velocity distribution in the width direction of the heat exchanger is nearly uniform, the power consumption of the compressor can be prevented from being unnecessarily increased. The case where the fan 100 is a single suction type. 2. 1108(k4^ ) + 1.8^ 1. 5g(k4F )^L/H^ 2g(k^ In the case where the sirocco fan 100 is a single suction type, The range 'by making, and - can be raised: into a unit that is smaller than the noise Ks and does not produce abnormal sounds. v In the above description, although the siro fan 1 is single, but for the siro fan (10) The operation point of the unit mounted on the unit of the air conditioner, such as the air conditioner, can also be the same:: In this case, 'the rotation speed N| of the unit and the air volume h of the unit, and then the p- of the fan 1GG alone Q characteristics, use the speed & and the air volume q " to replace the above L with l/2, replace Q It can be Q/2. However, if f{ P/(Q/2" } is set, then g(k彳)=139? ;2 ).

2148-9915-PF 15 靜壓Pi即可。在此,在單元裝 風扇的風量A0/匕 個風扇的情況,設J個 風讓、靜壓Μ,求損失 情況,帥…之範7::=^ ‘L/HSf("),而可形成比豐音Ks :5f(k Β 在西洛可風扇_為單吸入型的情況動二 之範圍,藉由作成匕㈣乂)。/ 成比噪音Ks小、安定的流動。 ㈠,而可形 第8圖係表示龄嘴3之縱 第9圖係表示鈴嘴3之 的示意剖面圖。 圖…。圖係表示無段差之區 := 壓變動的rms值之卩托A 丨刀在壁面上之靜 值之£域《部分的放大圖 有段差之區域α的部分在壁面上之 ^ 域α部分的放大κ 靜i父動的rms值之區 ]孜大圖。根據第8圖〜 段差形成於蝸形殼2之 圖,一面比較以將 成Z之側面的方式安裝鈴 形殼2之側面未形成段差之方式安裝鈴嘴3者二蜗 安裝於西洛可風扇1〇〇之鈴嘴3的特徵。’ --明 在第8圖所示之鈴嘴3的縱向剖面構造, 扇1〇〇側之端點(在鋒嘴3之最小 :點二 點A (成為對私趣。 丨)和點)為點A及2148-9915-PF 15 Static pressure Pi can be used. Here, in the case where the air volume A0 of the unit-mounted fan/one fan is set, J winds and static pressures are set, and the loss situation is obtained, which is handsome 7::=^ 'L/HSf("), and It can form a ratio of abundance Ks : 5f (k Β in the case of the sirocco fan _ is a single-inhalation type, by making 匕 (four) 乂). / The flow is smaller and stable than the noise Ks. (1), and the shape is shown in Fig. 8 is a vertical sectional view of the mouthpiece 3. Fig. 9 is a schematic sectional view showing the bell mouth 3. Figure... The graph indicates the area without step: = the rms value of the pressure change is the value of the static value of the boring tool on the wall. The enlarged part of the section has the section of the section α on the wall surface. Enlarge the area of the rms value of the κ static i parent's motion] 孜 big picture. According to Fig. 8 - the figure in which the step is formed in the volute casing 2, the side of the bell-shaped casing 2 is mounted on the side of the Z-shaped side to form a bell mouth. The characteristics of the bell mouth 3 of 1 inch. ' -- The longitudinal section structure of the bell mouth 3 shown in Fig. 8, the end point of the fan 1〇〇 side (the smallest at the front end 3: point 2 A (becoming a private interest. 丨) and points) For point A and

I成為對鈐嘴3之中心和點A 的端點(在鈴嘴3之最大開口部的:點)另-方 為對餘嘴3之中心和點:點)為及點B (成 之方向所拉的直線和設從點B向風扇1 B’向風扇1之方向所 貝1面的父點為點C、設從點 。斤拉的直線和蝸形殼2側面的交點為I becomes the center of the mouth 3 and the end point of the point A (the point at the maximum opening of the bell mouth 3), the other is the center and the point of the remaining mouth 3: the point is the point B and the direction The straight line drawn and the parent point from the point B to the fan 1 B' to the direction of the fan 1 are point C, and the point is set. The intersection of the straight line of the thrust and the side of the volute casing 2 is

2148-9915-PF 16 1354735 點c’ 、設線段AA,和風扇!之轉軸延長線的交點為點〇, 加以說明。 … 即,BC>0時以段差形成於蝸形殼2側面之方式安裝鈴 嘴3, BC=0 ef以在蜗㈣2側自未形成段差之方式安裝龄 嘴3。此外’以BC>0時BC之長度為5[随]、區域“二 之靜壓變動的nns值大約0[Pa]為例。在第9圖第u圖, 如第8圖所示根據鈐嘴3的安裝法,比較並表示在蜗形殼 2側面形成段差者之靜壓變動、和在堝形殼2側面未形成 * 段差者的靜壓變動。 以下,表示靜壓變動之rms值的定義式。 第(7)式 Ps(t)= ps + ps,=(t) 第(8)式 rms 值={ ( ς ps, (t)2) }0 5 在此,ps表示時間平均值,ps’ (t)表示靜壓的變動值。 在壁面上之靜壓變動的rms值愈大,從壁面所產生之 噪音愈大。從第1〇圖及第u圖得知,在蜗形殼2側面形 φ 成段差者之靜壓變動比在蝸形殼2側面未形成段差者的靜 >£變動小。因此,在蝸形殼2側面形成段差者可降低所產 生之噪音》 第12圖係表示西洛可風扇1 〇 〇之示意剖面構造的縱 向剖面圖,第13圖係透視西洛可風扇1〇〇而表示的透視 立體圖。根據第12圖及第13圖,說明在西洛可風扇1〇〇 之靜壓變動的rms值大之區域。又,在第12圖,在從構 成西洛可風扇1〇〇之蜗形殼2的風路仏至吹出口 2b之彎 曲部分’將最接近風扇!之外周部的部位圖示為舌部4。2148-9915-PF 16 1354735 Point c', line AA, and fan! The intersection of the extension of the shaft is a point, which is explained. That is, at the time of BC > 0, the bell mouth 3 is attached so that the step is formed on the side of the scroll case 2, and BC = 0 ef to mount the mouthpiece 3 on the side of the worm (4) 2 since no step is formed. In addition, 'the length of BC when BC>0 is 5 [following], and the nns value of the static pressure variation of the region is about 0 [Pa]. In the figure 9 of the figure u, as shown in Fig. 8 The mounting method of the nozzle 3 compares and shows the static pressure fluctuation of the step formed on the side surface of the scroll case 2 and the static pressure fluctuation of the case where the * segment difference is not formed on the side surface of the dome case 2. Hereinafter, the rms value of the static pressure variation is shown. Formula (7) Ps(t)= ps + ps,=(t) Equation (8) rms value={ ( ς ps, (t)2) }0 5 Here, ps represents the time average , ps' (t) indicates the variation value of the static pressure. The larger the rms value of the static pressure fluctuation on the wall surface, the greater the noise generated from the wall surface. From the first map and the u-th diagram, the snail shape is obtained. The static pressure variation of the side surface shape φ of the shell 2 is smaller than that of the static side of the volute casing 2, so that the noise generated on the side of the volute casing 2 can reduce the noise generated. 12 is a longitudinal sectional view showing a schematic sectional structure of a sirocco fan 1 , and a 13 is a perspective perspective view showing a perspective view of a sirocco fan. According to FIG. 12 and FIG. The area where the rms value of the static pressure change of the sirocco fan is large. Also, in Fig. 12, the bending from the wind path of the volute casing 2 constituting the siro fan 1 to the blowout port 2b The portion 'will be closest to the fan! The outer peripheral portion is illustrated as the tongue 4.

2148-9915-PF 17 的平面和…之=第8圖所示之點A、點0以及點A, 點圖示為點D、和二將和風扇1之距離變成最小的 於以點〇為中心從最近的點圖示為點Ε'位 為/ ·-之風扇1的反轉方向65。之iiS_ ’點F'位於以赴〇 、却圖不 、乂點〇為中心從點F之風扇1的 之點圖示為點G、位於以點〇 向4〇 動方向40。之玷圖_ & 從點F之風扇1的轉 '圖不為點H、位於以'點〇為中心從點 ^的轉動方向180。之點圖示為點丨。 ' 如此地疋義區域的情況,復y* jr 壓變動M g 兄付知在西洛可風扇1G0之靜 =動的㈣值大之區域,係連接點H、點f以及點 大致圓弧HFG的區域。因此,π在 長产Ax h 匕δ又在圓弧HFG之線段BC的 …、在大致圓弧HIG(連接點^點】以及點G之圓 線段BC的長度為¥時,在L/HSfU)或心价) :::圍’若係成為mu的鈴嘴3,可使靜壓變動之㈣ 值关小,而可使噪音變小。 如第10圖及第11圖所示,在蝸形殼2側面未形成段 差的情況,在圓弧肌的區域之靜壓變動的㈣值最大係 他’而在蜗形殼2側面形成段差的情況,在圓弧帆的 區域之靜壓變動的rms值最大變成心以下。即,藉由在 蜗形殼2側面形成段差,而降低以鈐嘴3為音源的;音。 認為其理由係由於’和風扇i之距離僅長了形成段差的 量,即線BC之長度’而抑制因風扇】的轉動所產生之 靜壓變動。 第14圖係表示通過動作點B之情況的西洛可風扇ι〇〇 2148-9915-PF 18 1354735 之P~ Q特性的圖形。根據第14圖,說明在蝸形殼2側面 形成段差之西洛可風扇丨〇〇通過點B的情況之p— Q特性 及在蜗形殼2側面未形成段差之西洛可風扇100通過點B 的情況之P— Q特性。在第14圖,黑圓形記號表示在蝸形 殼2側面形成段差之西洛可風扇丨〇〇的p_ Q特性,空白 圓形記號表示在蝸形殼2側面未形成段差之之西洛可風扇 1〇〇的p—q特性。又,在第14圖,縱軸表示靜壓p[Pa], 橫軸表示風量Q[m3/min]。 如帛14目所示’在蜗形殼2彻j面形成段差之西洛可 .風扇1〇0和在蝸形殼2側面未形成段差之西洛可風扇1〇〇 比較不安定區域時,得知前者位於開放側。在將在蝸形殼 2側面形成段差之西洛可風扇1〇〇裝載於空調裝置、或除 濕機、空氣清淨機等之單元的情況,由於單元之尺寸限 制,可能無法使西洛可風扇100的寬度尺寸變長。即,因 為寬度尺寸短,ίΗ乍‘點比比脅音變成“、之不技區域更 接近開放側的情況’因為可使不安定區域接近動作點,所 以對低噪音化有效。 第15圖係表示裝载西洛可風扇1〇〇之懸吊式室内機 110的示意整體構造之平面圖。第16圖係表示懸吊式室内 機11〇之縱向剖面構造的剖面圖。根據第15圖及第16圖, 說明將在蜗形殼2側面形成段差之西洛可風扇_装載於 懸吊式室内機110的情況之靜壓 圖示裝載2台西洛可風扇1〇〇, 變動。此外’在第15圖, 並將吸入空間5形成於各 自之寬度方向側面的情況 又,在第16圖,以箭號表示 2148-9915-PF 19 1354735 空氣的流動。 將在蝸形殼2侧面形成段差之西洛可風扇1〇〇裝載於 懸吊式室内機11 0的情況,由於所形成的段差,吸入空間 5僅減少段差的量,而有成為使噪音增大之要因的情況。 自上述的說明,靜壓變動之rms值大的區域係圓弧hfg, 在其他的區域,靜壓變動irms值受到和風扇】之距離的 影響小。因此,若將在圓弧HFG的區域形成段差之西洛可 風扇100裝載於懸吊式室内機110,可使段差位於吸入口 2a的下游側,而可使吸入空間5的減少量變小。 第17圖係表示在懸吊式室内機11〇之噪音值的表。 根據第1 7圖,說明從裝載在蜗形殼2側面形成段差之西 洛可風扇1 〇〇的懸吊式室内機i丨〇所產生之噪音值、從裝 載在蝸形殼2側面未形成段差之西洛可風扇丨〇〇的懸吊式 室内機110所產生之噪音值.此外,假設段差形成於圓弧 HFG的區域。又,各自表示在吹出風量為16 m3/min之情 況的噪音值。 如第17圖所示,得知在吹出風量為16 m3/min之情 況,在圓弧HFG之區域形成段差者的噪音值係42.4[dB], 在圓弧HFG之區域未形成段差者的噪音值係44〇[dB]。如 此’藉由在圓弧HFG之區域形成段差,而可使噪音值變小。 自以上,藉由在圓弧HFG之區域設置段差,而抑制吸入空 間5的減少’而且可使臂音值變小。 第2實施形態 第18圖係表示本發明之第2實施形態的空調裴置丄5〇 2148-9915-PF 20 1354735 之示意構造的示意構造圖。根據第18圖,說明空調裝置 150之構造。此空調裝置ι5〇係裝載第1實施形態的西洛 可風扇100者。此西洛可風扇1〇〇用以對構成空調裝置15〇 之室内機(室内單元)裝載於熱交換器的附近。此外,在本 第2實施形態’主要說明和上述之第1實施形態的相異 點’而對和第1實施形態相同的部分,賦予同一符號並省 略說明。 此空調裝置150以冷媒配管依序連接凝結式熱交換器 152、節流裝置153以及蒸發式熱交換器154而構成。其 中’對設置凝結式熱交換器152或蒸發式熱交換器154之 室内機,設置第1實施形態的西洛可風扇1 〇〇。即,西洛 可風扇100設置於室内機所設置之凝結式熱交換器152或 蒸發式熱交換器1 54的附近’具有將空氣供給凝結式熱交 換器152或蒸發式熱交換器154之功能。 壓縮機151吸入在冷媒配管流動的冷媒,將該冷媒壓 縮而變成高溫、高壓之狀態。凝結式熱交換器1 5 2係在空 氣和冷媒之間進行熱交換,而使該冷媒凝結或液化者。節 流裝置1 53係將冷媒降壓而使膨脹者。蒸發式熱交換器 154係在空氣和冷媒之間進行熱交換’而使該冷媒蒸發或 氣化者。藉由對構成此空調裝置1 50之設置凝結式熱交換 器152或蒸發式熱交換器154的室内機,裝載第1實施形 態的西洛可風扇1〇〇,而可降低向室内傳達的噪音。 在此,簡單地說明空調裝置150的動作。第i 8圖所 示之箭號’表示冷媒的流向。被壓縮機151壓縮而變成.高 2148-9915-PF 21 1354735 恤、南壓之冷媒氣體流入凝結式熱交換器152。在此凝结 式熱交換器152,冷媒和空氣進行熱交換而凝結,變成低 咖兩壓之液體冷媒或氣液二相冷媒。從凝結式熱交換器 1 5 2所流出的冷媒,然後,在節流裝置丨5 3降壓變成低 溫、低壓之液體冷媒或氣液二相冷媒,再流入蒸發式熱交 換器154。在蒸發絲交換胃154,冷媒和线進行熱交 換而蒸發’變成高溫、低麼之冷媒氣體,再被虔縮機151 吸入。在暖房運轉時’將蒸發式熱交換器154裝載於室内 機。 在損失係數小、風扇寬度寬的情況,熱交換器之寬产 方向的速度分布接近均自,和風扇寬度窄、速度分布不均 勾的情況相比’可有效地使用熱交換器的導熱面積。因 =,得到既定之空調性能所需的空氣和冷媒之温差變小, 絲機輸入功率變小,而且變成低噪音。χ,在損 小的情況’即使風扇直徑沒有變大 、:'、數 寬,可使噪音變小。此外,在包括福:;八扇寬度變 仕包括複數個風扇寬声 扇的空調裝置,藉由置換成風灵X乍之風 1供风風扇見度寬的風扇,而 :風扇的個數,亦可使在既定動作點之空調農置…減 變小,而且可使熱交換器之寬产 本曰值 句。 莧度方向的速度分布接近均 明說 單 簡式 圖 ΙΛί' Τ/ϋ ^ ^ 而表示的透視立體圖 214B'9915-pf 22 1354/33 Ϊ;=Γ扇之整體形狀的立體圖。 圖。 丁西洛可風扇之示意縱向剖面構造的剖面 第4圖作矣- 口1糸表不西洛可風扇 的圖形。 Q特性及Ks〜Q特性2148-9915-PF 17 plane and ... = point A, point 0 and point A shown in Fig. 8, the point is shown as point D, and the distance between the two and the fan 1 is minimized. The center is illustrated from the nearest point as the reverse direction 65 of the fan 1 whose position is /. The point where the iiS_ 'point F' is located at the point of the fan 1 which is located at the point F, is shown as the point G, and is located at the point 4 in the direction of the click. _ _ & The rotation of the fan 1 from point F is not the point H, and is located 180 degrees from the point ^ in the direction of the point. The point is shown as a point. In the case of such a derogatory area, the complex y* jr pressure change M g brother pays to know that in the area of the Silo fan 1G0 static = moving (four) value, the connection point H, the point f and the point roughly circular arc HFG region. Therefore, π is in the long-term production Ax h 匕δ and in the line BC of the arc HFG..., when the length of the circular arc HIG (connection point ^ point) and the round line segment BC of the point G is ¥, at L/HSfU) Or the price of ::): If it is the bell mouth 3 of mu, the (4) value of the static pressure change can be made small, and the noise can be made smaller. As shown in Fig. 10 and Fig. 11, in the case where no step is formed on the side of the volute casing 2, the value of the static pressure variation in the region of the arc muscle is the largest, and the step on the side of the volute casing 2 is formed. In the case, the rms value of the static pressure fluctuation in the area of the circular sail is maximum below the center. That is, by forming a step on the side surface of the volute casing 2, the sound of the mouthpiece 3 as a sound source is lowered. The reason is considered to be because the distance from the fan i is only increased by the amount of the step, that is, the length of the line BC, and the static pressure fluctuation caused by the rotation of the fan is suppressed. Fig. 14 is a graph showing the P~Q characteristics of the sirocco fan ι〇〇 2148-9915-PF 18 1354735 as it passes through the operating point B. According to Fig. 14, the p-Q characteristic of the case where the sirocco fan 形成 passing through the side of the volute casing 2 is passed, and the sirocco fan 100 passing through the point on the side of the volute casing 2 is not shown. P-Q characteristics of the case of B. In Fig. 14, the black circular mark indicates the p_Q characteristic of the sirocco fan 形成 which forms a step on the side of the volute casing 2, and the blank circular mark indicates that the sirocco is not formed on the side of the volute casing 2 The p-q characteristic of the fan 1〇〇. Further, in Fig. 14, the vertical axis represents the static pressure p [Pa], and the horizontal axis represents the air volume Q [m3 / min]. As shown in Fig. 14 'When the volute shell 2 forms a step difference, the sirocco fan 1 〇 0 and the snail shell 1 side of the snail shell 2 do not form a step difference, the sirocco fan 1 〇〇 relatively unstable area, I learned that the former is on the open side. In the case where a sirocco fan 1 having a step formed on the side surface of the scroll case 2 is mounted on a unit such as an air conditioner or a dehumidifier or an air cleaner, the siro fan 100 may not be possible due to the size limitation of the unit. The width of the width becomes longer. In other words, since the width dimension is short, the Η乍 Η乍 点 点 点 胁 胁 胁 胁 胁 胁 胁 胁 ' 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为 因为A plan view showing a schematic overall structure of a suspended indoor unit 110 carrying a sirocco fan. Fig. 16 is a cross-sectional view showing a longitudinal sectional structure of a suspended indoor unit 11 。. According to Figs. 15 and 16 In the case of the sirocco fan which is formed on the side of the volute casing 2, the static pressure diagram of the case where it is mounted on the suspended indoor unit 110 is loaded with two sets of sirocco fans, and the change is made. Fig. 15 shows the case where the suction space 5 is formed on the side surfaces of the respective width directions. In Fig. 16, the flow of air of 2148-9915-PF 19 1354735 is indicated by an arrow. The west of the step is formed on the side of the scroll case 2. When the Luoke fan 1 is mounted on the suspended indoor unit 110, the suction space 5 is reduced by the amount of the step difference due to the step formed, and there is a case where the noise is increased. Zone with large rms value of static pressure variation The field system arc hfg, in other areas, the static pressure fluctuation irms value is less affected by the distance from the fan. Therefore, if the sirocco fan 100 that forms a step in the arc HFG region is placed in the suspended room The machine 110 can make the step difference on the downstream side of the suction port 2a, and can reduce the amount of decrease in the suction space 5. Fig. 17 is a table showing the noise value of the suspended indoor unit 11 。. The noise value generated from the suspended indoor unit i丨〇 of the sirocco fan 1 形成 which is formed on the side of the volute casing 2, and the sirocco fan which is not formed on the side of the volute casing 2 The noise value generated by the suspended indoor unit 110. In addition, it is assumed that the step is formed in the area of the circular arc HFG, and each represents a noise value in the case where the blown air volume is 16 m3/min. As shown in the figure, when the air volume is 16 m3/min, the noise value of the step in the area of the arc HFG is 42.4 [dB], and the noise value of the step is not formed in the area of the arc HFG. [dB]. So 'by making a step in the area of the arc HFG, the noise can be made The sound value is reduced. From the above, by providing a step in the area of the circular arc HFG, the decrease in the suction space 5 is suppressed, and the arm sound value can be made small. Fig. 18 is a second embodiment of the present invention. A schematic structural view of a schematic structure of an air conditioner 丄 5〇 2148-9915-PF 20 1354735 according to the embodiment. The structure of the air conditioner 150 will be described based on Fig. 18. The air conditioner ι5 is loaded with the Siro of the first embodiment. The sirocco fan 1 is used to mount an indoor unit (indoor unit) constituting the air conditioner 15 in the vicinity of the heat exchanger. In addition, in the second embodiment, the main description and the above are described. In the first embodiment, the same portions as those in the first embodiment are denoted by the same reference numerals and will not be described. The air conditioner (150) is configured by sequentially connecting the condensation heat exchanger (152), the expansion device (153), and the evaporative heat exchanger (154) with a refrigerant pipe. Here, the sirocco fan 1 第 of the first embodiment is provided for the indoor unit in which the condensing heat exchanger 152 or the condensing heat exchanger 154 is provided. That is, the sirocco fan 100 is disposed in the vicinity of the condensing heat exchanger 152 or the evaporative heat exchanger 154 provided in the indoor unit, and has a function of supplying air to the condensing heat exchanger 152 or the evaporative heat exchanger 154. . The compressor 151 sucks in the refrigerant flowing through the refrigerant pipe, and compresses the refrigerant to a high temperature and a high pressure state. The condensing heat exchanger 15 2 is a heat exchange between air and refrigerant to cause the refrigerant to condense or liquefy. The throttle device 1 53 depressurizes the refrigerant to expand the person. The evaporative heat exchanger 154 is a type in which heat is exchanged between air and a refrigerant to evaporate or vaporize the refrigerant. By mounting the sirocco fan 1 of the first embodiment to the indoor unit in which the condensing heat exchanger 152 or the evaporative heat exchanger 154 is installed in the air conditioner 150, the noise transmitted to the room can be reduced. . Here, the operation of the air conditioner 150 will be briefly described. The arrow ' shown in Fig. 8' indicates the flow of the refrigerant. The compressor 151 is compressed to become a high 2148-9915-PF 21 1354735 shirt, and the refrigerant gas of the south pressure flows into the condensing heat exchanger 152. In the condensing heat exchanger 152, the refrigerant and the air exchange heat by condensation, and become a liquid refrigerant or a gas-liquid two-phase refrigerant which is low in pressure and pressure. The refrigerant flowing out of the condensing heat exchanger 152 is then depressurized into a low-temperature, low-pressure liquid refrigerant or a gas-liquid two-phase refrigerant at the expansion device 丨5 3, and then flows into the evaporative heat exchanger 154. The evaporation wire exchanges the stomach 154, and the refrigerant and the wire are heat-exchanged to evaporate into a high-temperature, low-temperature refrigerant gas, which is then sucked by the retort 151. When the greenhouse is in operation, the evaporative heat exchanger 154 is mounted on the indoor unit. In the case where the loss coefficient is small and the fan width is wide, the velocity distribution in the wide production direction of the heat exchanger is nearly uniform, and the heat transfer area of the heat exchanger can be effectively used compared with the case where the fan width is narrow and the speed distribution is unevenly hooked. . Because of the =, the temperature difference between the air and the refrigerant required to obtain the predetermined air-conditioning performance becomes small, the input power of the wire machine becomes small, and it becomes low noise. χ, in the case of small damage, even if the fan diameter does not become large, : ', the number is wide, the noise can be made smaller. In addition, in the inclusion of Fu:; eight widths change the air-conditioning device including a plurality of fan wide-sound fans, by replacing the fan with the wind fan X wind 1 wide fan visibility, and: the number of fans, It can also make the air-conditioning farms at a given operating point less variable, and can make the heat exchanger's wide-ranging value. The velocity distribution in the direction of the twist is close to that of the single figure ΙΛί' Τ/ϋ ^ ^ and the perspective view is 214B'9915-pf 22 1354/33 Ϊ; = the perspective view of the overall shape of the fan. Figure. The cross-section of the schematic longitudinal section of the Dingsilo fan is shown in Figure 4 as a 矣-port 1 糸 not a graph of the siro fan. Q characteristics and Ks~Q characteristics

第5圖係矣+ I 你夕同 、'^、西洛可風扇之U/H。和損失俜砮 係之圖形。 貝天知數t。的關 第6圖係、表示通過動 卜Q特性及Ksm 』a之情況的西洛可風扇之 y特性的圖形。 二= :::每,一葉一葉 =向剖面構造的示意剖面圖。 …係表:Γ;差區域α的西洛可風扇之立體圖。 壓變動的⑽值之巴域W的部分在壁面上之靜 m i &域0:部分的放大圖。 11圖係表示有段差之區域α的部分在壁面上之靜 ㈣動的㈣之區域α部分的放大圖。 知 第12圖係表示西、、欠π ^ _ 面圖。 ,可風扇之示意剖面構造的縱向剖 第13圖係透視西洛可風扇而表示的透視立體圖。 :14圖係表不通過動作點b之情況的西洛可風 p—Q特性的圖形。 〈 弟15圖係表·•并 咅 、裝載西洛可風扇之懸吊式室内機的示 思整體構造之平面圖。 丁 2148-9915-pf 23 1354735 第1 6圖係表示懸吊式室内機之縱向剖面構造的剖面 圖。 第17圖係表示在懸吊式室内機之噪音值的表。 第18圖係表示本發明之第2實施形態的空調裝置之 不意構造的不意構造圖。 【主要元件符號說明】 1 風扇、 2 蝸形殼、 2 a吸入口、 2b吹出口、 2M舌部、 2c風路、 3 鈐嘴、 4 舌部、 5 吸入空間、 1 0 0西洛可風扇、 110懸吊式室内機、 150空調裝置、 1 51壓縮機、 152凝結式熱交換器、 1 5 3節流裝置、 154蒸發式熱交換器Figure 5 is the system 矣 + I you Xitong, '^, Xiluo fan U / H. And the pattern of loss. Bei Tian knows the number t. The figure of Fig. 6 shows a graph showing the y characteristic of the sirocco fan by the action of the Q characteristic and the Ksm 』a. Two = ::: each, one leaf and one leaf = a schematic sectional view of the cross-sectional structure. ...the table: Γ; the perspective view of the sirocco fan of the difference area α. The portion of the bar field W of the pressure variation (10) is static on the wall m i & field 0: a magnified view of the portion. Fig. 11 is an enlarged view showing a portion of the region α of the static (four) moving (four) portion of the region having the step α in the step. It is understood that the 12th figure shows the west and the π ^ _ surface map. Longitudinal section of the schematic cross-sectional structure of the fan. Fig. 13 is a perspective perspective view showing the sirocco fan. : 14 The graph shows the graph of the sirocco p-Q characteristics in the case where the action point b is not passed. 〈 15 图 图 图 · · 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 Ding 2148-9915-pf 23 1354735 Fig. 16 is a cross-sectional view showing the longitudinal sectional structure of the suspended indoor unit. Figure 17 is a table showing the noise values of the suspended indoor unit. Fig. 18 is a schematic structural view showing an unintentional structure of an air-conditioning apparatus according to a second embodiment of the present invention. [Main component symbol description] 1 fan, 2 volute casing, 2 a suction port, 2b air outlet, 2M tongue, 2c air path, 3 mouth, 4 tongue, 5 suction space, 1 0 0 siro fan , 110 suspended indoor unit, 150 air conditioner, 1 51 compressor, 152 condensing heat exchanger, 1 5 3 throttling device, 154 evaporative heat exchanger

2148-9915-PF 242148-9915-PF 24

Claims (1)

1354735 十、申請專利範圍: 1· 一種西洛可風扇’包括: 蜗形殼,係具有用以取入空氣的吸入口、用以吹出空 氣的吹出口、以及從該吸入口至該吹出口的風路; 風扇,係被收容於該蝸形殼内,藉由進行轉動驅動而 從該吸入口取入空氣並從該吹出口吹出空氣;以及 鈴嘴,係安裝於該堝形殼的該吸入口;1354735 X. Patent application scope: 1. A sirocco fan' includes: a volute casing having a suction port for taking in air, a blow port for blowing air, and a blow port from the suction port to the blow port. a wind passage; the fan is housed in the volute casing, and is driven by rotation to take in air from the suction port and blow air from the air outlet; and the bell mouth is attached to the suction cup mouth; 其特徵在於· 隹該吸入口位於該風扇之轉動中心的延長線上,並 成於該蜗形殼的兩側面者, 設在該風路内之通風阻力為p[pa]、從該吸入口所 入之空氣的量為Q[mvmin]、該風扇之轉軸方向的寬度 L[_]、k為常數、該竭形殼的高度為η,·]: 為損失係數|:[Pa/(mVmin) 2]的情況, 在〇.l$k4f $〇_4之範圍,作成 W H = 0.3494W h 〇.75f(k^)^L/H^f(k4n〇 ΗΗ.8 2·如申請專利範圍第Μ之西洛 該堝形殼之該風路至該吹出口的彎曲 二”中係在 風扇之外周部的部位作為舌部, “刀,將最接近 在該鈐嘴的縱向剖面, 在該鈐嘴之最小開口部的端 設成為對鈐嘴之中心和點八點對二點八, 設在該玲嘴 ··' 、冉的點為點Α,, 嘴之最大開口部的端點, 2148-9915-PF 25 為對鈴嘴之中^和點對稱的點為點B,, 設從該點β向風扇之方向所拉 的交點為點c, 的直線和該蝸形殼侧面 设從該點Β,向風扇之方向所㈣ 面的交點為點c,, 々茨蝸形忒側 »又線奴ΑΑ,和該風扇之轉軸延長線的交點為點〇, 在通過該點Α、該點〇以及該點Α,的 之交線上,將釦坊门昏 和該舌。ρ ^ 將和該風扇之距離變成最小的點設為點D, 設和該鈴嘴之點D最近的點為點E, 設位於以該點〇為 65。之點為點F, 〜點E之該風扇的反轉方向 設位於以該點〇為中 切。之點為點G,為中4該點F之該風扇的反轉方向 ^於以該點。為中'。從該點F之該風扇的轉動方 之點為點H’設位於以該點〇為中心從該點 二 的轉動方向180。之點為點】, ^屬 «又在連接該點H、該點F以及該點G之大 的線段BC之長度4χ, HFG °又在連接該點H、該點I以及該點G之大致圓弧H 的線段BC之長度為¥時, 弧HIG 在L/HS f(k4p )之範圍,作成 X〉γ — 〇 〇 3.-種西洛可風扇,包括: 蜗殼,传月, ’、-、有用以取入空氣的吸入口、用以吹出办 2148-9915-PF 26 1354735 氣的吹出口、以及從該吸入口至該吹出口的風路; 風扇,係被收容於該蜗形殼内,藉由進行轉動驅動而 從該吸入口取入空氣並從該吹出口吹出空氣;以及 鈴嘴,係安裝於該蝸形殼的該吸入口; 其特徵在於: 在該吸入口位於該風扇之轉動中心的延長線上,並形 成於該蝸形殼的單側面者, 設在該風路内之通風阻力為P[Pa]、從該吸入口所取 入之空氣的量I Q[mVmin]、該風扇之轉軸方向的寬度為 L[〇m]、k為常數、該蝸形殼的高度為H = 246k[mm]、p/Q2 為損失係數f [pa/(m3/min) 2]的情況, 在〇. IS k4f $ 〇· 4之範圍,作成 ) = 1.39788(k^ 2.H〇8(k^ ) + 1 g , 1. 5g(k4f hL/HS 2g(k4f )。 4.如申請專利範圍第3項之西洛可風扇,苴中 v係在從該堝形殼之該風路至該吹出口的彎曲之部 为,將最接近該風扇之外周部的部位作為舌部, 在該鈐嘴的縱向剖面, 〇又在該鈐嘴之最小開口部的端點為點A, =為對铃嘴之中心和點A點對稱的點為點A,, 〇又該鈐嘴之最大開口部的端點為點B, 對鈴嘴之中心和點"對稱的點為點B,, s又攸該點Β向風扇之方向所拉 的交點為點C, &直線和該蝸形殼側面 2Ί 2148-9915-PF 設從該點B,& g! # A i 兩的交點為點C,,·向所拉的直線和該蝸形殼側 : 又線段“,和該風扇之轉轴延長線的交點為點〇, < =通過該點A、該點0以及該點A、平面和該舌部 ’將和該風扇之距離變成最小的點設為點D, 設和該鈴嘴之點D最近的點為點E, 5又位於以該點〇為中 Re。 從該點E之該風扇的反轉方向 G b之點為點F, 設位於以該點〇為中心從該點F之該風扇的反轉方向 40之點為點G, «又位於以該點〇為中心從該點f之該風扇的轉動 4 Π。 、 ν 之點為點Η,没位於以該點〇為中心從該點F之該風扇 的轉動方向180。之點為點j, °又在連接該點H、該點F以及該點G之大致圓弧HFG 的線段BC之長度為X, s又在連接該點Η、該點I以及該點g之大致圓弧η I (J 的線段BC之長度為γ時, 在L/HS g(k4 f )之範圍,作成 X>Y$ 0。 5. 一種空調裝置’其特徵在於:使用如申請專利範圍 第1至4項中任一項之西洛可風扇。 2148-9915-PF 28The utility model is characterized in that: the suction port is located on an extension line of the rotation center of the fan, and is formed on both sides of the spiral case, and the ventilation resistance in the air path is p[pa], from the suction port The amount of air entering is Q [mvmin], the width of the fan in the direction of the axis of rotation L[_], k is constant, the height of the dome is η, ·]: is the loss coefficient |: [Pa / (mVmin) In the case of 2], in the range of 〇.l$k4f $〇_4, create WH = 0.3494W h 〇.75f(k^)^L/H^f(k4n〇ΗΗ.8 2· as in the scope of patent application The wind road of the 西 洛 埚 埚 至 至 至 至 至 至 至 的 的 的 ” ” ” ” ” ” ” ” ” ” ” ” ” ” ” ” ” ” ” “ “ “ “ “ “ “ “ “ “ “ “ “ “ “ The end of the smallest opening of the mouth is set to be the center of the mouth and the point is eight o'clock, and the point at the point of the mouth is Α, the point of the largest opening of the mouth, 2148 -9915-PF 25 is a point B which is symmetrical with respect to the point and the point in the bell mouth, and a line from the point β to the direction of the fan is a point c, and the side of the scroll case is set from the side Point In the direction of the fan, the intersection point of the (four) plane is point c, the snail shackle side » the line slave, and the intersection of the fan's shaft extension line is point 〇, at the point of passing the point, the point 〇 and the On the intersection line of the point, the door will be fainted and the tongue. ρ ^ The point at which the distance from the fan becomes the minimum is set to point D, and the point closest to the point D of the bell is set to point E, The point at which the point is 65 is the point F, and the direction of the reverse direction of the fan of the point E is set to be the center cut at the point 。. The point is the point G, which is the fan of the point F at the point 4 The reverse direction is at this point. It is in the middle. The point of the rotation of the fan from the point F is the point H' located at the point 180 from the point of rotation of the point two. 】, ^ is « is connected to the point H, the point F and the length of the line BC of the point G is 4 χ, HFG ° is connected to the point H, the point I and the point of the general arc H of the point G When the length of the line segment BC is ¥, the arc HIG is in the range of L/HS f(k4p), and is made into X>γ-〇〇3.-Sirocco fan, including: volute, moon, ',-, useful a suction port for taking in air, an air outlet for blowing 2148-9915-PF 26 1354735 gas, and a wind passage from the suction port to the air outlet; the fan is housed in the spiral case, Driving the air from the suction port and blowing air from the air outlet; and the bell mouth is attached to the suction port of the scroll case; and the suction port is located at the center of rotation of the fan The extension line is formed on one side of the volute casing, the ventilation resistance in the air passage is P [Pa], the amount of air taken in from the suction port IQ [mVmin], the fan The width in the direction of the rotation axis is L[〇m], k is constant, the height of the scroll case is H = 246k [mm], and p/Q2 is the loss factor f [pa/(m3/min) 2]. 〇. IS k4f $ 〇·4 range, made) = 1.39788(k^ 2.H〇8(k^ ) + 1 g , 1. 5g(k4f hL/HS 2g(k4f ). 4. The sirocco fan of claim 3, wherein the v is in the curved portion from the air passage of the clamshell to the air outlet, and the portion closest to the outer circumference of the fan is used as The tongue, in the longitudinal section of the mouth, the point at the end of the smallest opening of the mouth is point A, = the point which is pointy to the center of the bell mouth and the point A is point A, and The end point of the largest opening of the mouth is point B, and the point of the center of the bell mouth and the point symmetry is point B, and the point where the point is pulled toward the fan is point C, & The straight line and the side of the volute casing 2Ί 2148-9915-PF are set from the point B, & g! # A i the intersection of the two points is point C,, · the straight line drawn to the side of the scroll and the side of the scroll: And the intersection of the fan's axis extension line is point 〇, < = the point at which the point A, the point 0, and the point A, the plane, and the tongue 'the minimum distance with the fan are set to a point D, the point closest to the point D of the bell mouth is point E, and 5 is located at the point Re in the point Re. From the point E, the point of the reverse direction G b of the fan is point F, set The point from the point F in the reverse direction 40 of the fan from the point F is the point G, and «the rotation of the fan from the point f centered on the point 4 is 4 Π. Point Η, is not located in the direction of rotation of the fan from the point F centered at the point F. The point is point j, ° is connected to the point H, the point F and the substantially circular arc HFG of the point G The length of the line segment BC is X, and s is in the range of L/HS g(k4 f ) when the point Η, the point I, and the approximate arc η I of the point g (the length of the line segment BC of J is γ) , X>Y$0. 5. An air conditioning apparatus characterized by using a sirocco fan as claimed in any one of claims 1 to 4. 2148-9915-PF 28
TW097130507A 2008-07-10 2008-08-11 Sirocco fan and air conditioner using the same TW201002944A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
PCT/JP2008/062442 WO2010004628A1 (en) 2008-07-10 2008-07-10 Sirocco fan and air conditioner using the same

Publications (2)

Publication Number Publication Date
TW201002944A TW201002944A (en) 2010-01-16
TWI354735B true TWI354735B (en) 2011-12-21

Family

ID=41506762

Family Applications (1)

Application Number Title Priority Date Filing Date
TW097130507A TW201002944A (en) 2008-07-10 2008-08-11 Sirocco fan and air conditioner using the same

Country Status (8)

Country Link
EP (1) EP2314880B1 (en)
JP (1) JP4660634B2 (en)
KR (1) KR101045750B1 (en)
CN (1) CN102066771B (en)
AU (1) AU2008359151B2 (en)
ES (1) ES2402790T3 (en)
TW (1) TW201002944A (en)
WO (1) WO2010004628A1 (en)

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5717046B2 (en) * 2010-11-12 2015-05-13 日本電産株式会社 Blower fan
CN102977856A (en) * 2012-11-21 2013-03-20 青岛文创科技有限公司 Acrylic ester dust suppressant
CN103835997B (en) * 2014-03-06 2017-05-03 珠海格力电器股份有限公司 Air conditioner indoor unit and volute thereof
KR102240314B1 (en) 2015-02-16 2021-04-14 삼성전자주식회사 Scroll for air conditioner and Air conditioner having the same
US11319961B2 (en) * 2016-05-20 2022-05-03 Mitsubishi Electric Corporation Centrifugal blower, air conditioner, and refrigeration cycle apparatus
WO2018225217A1 (en) * 2017-06-08 2018-12-13 三菱電機株式会社 Sirocco fan and air conditioner using same
EP4194764A4 (en) * 2020-08-07 2024-01-03 Daikin Ind Ltd Fan unit and air-handling system provided with same

Family Cites Families (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1875881A (en) * 1931-01-27 1932-09-06 American Blower Corp Fan housing construction
JPS61229999A (en) * 1985-04-03 1986-10-14 Matsushita Refrig Co Blower
JPH07208396A (en) * 1994-01-27 1995-08-08 Nippondenso Co Ltd Centrifugal blower
JPH08312592A (en) * 1995-05-19 1996-11-26 Akaishi Kinzoku Kogyo Kk Opening part structure of casing for blower
JP3700217B2 (en) * 1995-10-31 2005-09-28 株式会社デンソー Centrifugal blower
JPH09195978A (en) * 1996-01-17 1997-07-29 Matsushita Electric Ind Co Ltd Blower designing method
JPH11324984A (en) 1998-05-06 1999-11-26 Toto Ltd Multi-blade fan
JP2001115997A (en) * 1999-10-14 2001-04-27 Matsushita Seiko Co Ltd Multi-blade fan
JP2004169579A (en) * 2002-11-18 2004-06-17 Sanden Corp Centrifugal blower
JP2006233835A (en) * 2005-02-24 2006-09-07 Matsushita Electric Ind Co Ltd Blower
CN2937888Y (en) * 2006-02-21 2007-08-22 松下电器产业株式会社 Pipeline type air conditioner

Also Published As

Publication number Publication date
JP4660634B2 (en) 2011-03-30
WO2010004628A1 (en) 2010-01-14
JPWO2010004628A1 (en) 2011-12-22
ES2402790T3 (en) 2013-05-09
EP2314880A1 (en) 2011-04-27
CN102066771B (en) 2012-12-12
AU2008359151B2 (en) 2011-07-28
EP2314880B1 (en) 2013-01-09
KR20100134684A (en) 2010-12-23
CN102066771A (en) 2011-05-18
KR101045750B1 (en) 2011-06-30
AU2008359151A1 (en) 2010-01-14
EP2314880A4 (en) 2011-08-10
TW201002944A (en) 2010-01-16

Similar Documents

Publication Publication Date Title
TWI354735B (en)
JP4906555B2 (en) Sirocco fan and air conditioner
US10436496B2 (en) Indoor unit for air-conditioning apparatus
TWI352779B (en)
JP4831707B2 (en) Cross-flow fan, molding die and fluid feeder
JP4678327B2 (en) Air conditioner
JP6304441B1 (en) Cross flow type blower and indoor unit of air conditioner equipped with the blower
CN108138798A (en) Air blower and the conditioner for having the air blower
CN105091087B (en) There are two the air conditioner indoor unit of heat exchanger for tool
JP6671469B2 (en) Centrifugal blower, air conditioner and refrigeration cycle device
JP2008051035A (en) Method for designing additional blades of axial flow fan
JP2006336935A (en) Outdoor unit for refrigeration air conditioner
JP4785670B2 (en) Air conditioner indoor unit
JP4889716B2 (en) Air conditioner indoor unit
JP5359727B2 (en) Air conditioner indoor unit
CN105091088B (en) A kind of air conditioner indoor unit with air-supply arrangement
JP6375132B2 (en) Air conditioner
EP3064777A1 (en) Cross-flow fan and air conditioner
JP2010236426A (en) Sirocco fan
JPH09229403A (en) Air conditioner
CN211261014U (en) Volute tongue structure of through-flow air duct, air duct system and air conditioner indoor unit
CN217357111U (en) Air supply assembly applied to air conditioner indoor unit and air conditioner indoor unit
CN209557335U (en) Spiral case, blower and air conditioner
JP2002276585A (en) Indoor unit and air conditioner
JP2010242598A (en) Axial blower and air conditioner