TW201002944A - Sirocco fan and air conditioner using the same - Google Patents
Sirocco fan and air conditioner using the same Download PDFInfo
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- TW201002944A TW201002944A TW097130507A TW97130507A TW201002944A TW 201002944 A TW201002944 A TW 201002944A TW 097130507 A TW097130507 A TW 097130507A TW 97130507 A TW97130507 A TW 97130507A TW 201002944 A TW201002944 A TW 201002944A
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- point
- fan
- air
- suction port
- volute casing
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Classifications
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F04—POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
- F04D—NON-POSITIVE-DISPLACEMENT PUMPS
- F04D29/00—Details, component parts, or accessories
- F04D29/40—Casings; Connections of working fluid
- F04D29/42—Casings; Connections of working fluid for radial or helico-centrifugal pumps
- F04D29/4206—Casings; Connections of working fluid for radial or helico-centrifugal pumps especially adapted for elastic fluid pumps
- F04D29/4213—Casings; Connections of working fluid for radial or helico-centrifugal pumps especially adapted for elastic fluid pumps suction ports
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F04—POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
- F04D—NON-POSITIVE-DISPLACEMENT PUMPS
- F04D29/00—Details, component parts, or accessories
- F04D29/40—Casings; Connections of working fluid
- F04D29/42—Casings; Connections of working fluid for radial or helico-centrifugal pumps
- F04D29/4206—Casings; Connections of working fluid for radial or helico-centrifugal pumps especially adapted for elastic fluid pumps
- F04D29/4226—Fan casings
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F04—POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
- F04D—NON-POSITIVE-DISPLACEMENT PUMPS
- F04D29/00—Details, component parts, or accessories
- F04D29/66—Combating cavitation, whirls, noise, vibration or the like; Balancing
- F04D29/661—Combating cavitation, whirls, noise, vibration or the like; Balancing especially adapted for elastic fluid pumps
- F04D29/667—Combating cavitation, whirls, noise, vibration or the like; Balancing especially adapted for elastic fluid pumps by influencing the flow pattern, e.g. suppression of turbulence
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- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Structures Of Non-Positive Displacement Pumps (AREA)
Abstract
Description
201002944 九、發明說明: 【發明所屬之技術領域】 之空調裝 可風扇及 气發明係有關於西洛可風扇及使用該風扇 置,尤其係有關於作成降低所產生之聲音的西洛 使用該風扇之空調裝置。 【先前技術】 形,自以往’存在一種係多葉片離心式風扇,其具有圓筒 / ’並可對空調對象區域吹出t度寬之帶 ^ ,常利用於構成空㈣置之室内機、或除濕:: ::淨機等。這種西洛可風扇,一般將複數支細長的心 :排列於圓周上而整體上成圓筒形的風扇,收容於 口二吹出出的蜗形殼而構成。而’西洛可風扇從吸入 、工m㈣,並從吹出口側對空調對象 取入的空氣。 所 作為那種西洛可風扇,提議「―種多葉片風扇,包括. :此間:…沿著同一轉轴所連結之複數個多葉片離心 :風扇單元、及用以收容該連結之複數個多葉片離心式風 羽早凡的外殼’該外殼形成用以將從該複數 式風扇單元所排出之空氣向外部吹出的也 出用流路係對該複數個多葉片離心式風扇單元所連續之 共同的流路」(例如,參照專利文獻1 )。 專利文獻1 :特開平1 1 — 324984號公報(頁, 7〜8圖) 昂 2148-9915-PF 5 201002944 ·-【發明内容】 【發明要解決之課題】 在以在之多葉片風扇,在動作點之損失係數小 作點位於比不安定區域更接近開放側的情況,具^ 橫寬窄、在既定風量時所逄吐 扇之 里t所產生之嗶音變大的課題。 這種西洛可風扇,在將既定量之風量供給空調^ 時,從風扇所產生之聲音變大,而成為噪音,並傳至^ 對象區域,令使用者覺得$ # ° 兀侍不舒服。又,若降低既定噪音僅, 則來自西洛可風扇的吹出 人出風$變小,若使吹出風量變大, 則α喿音值變大,而亦且右魏a 〃、有難取付吹出風量和聲音的產生之 適虽的平衡。又,在風扇寬度 了使噪音變小,亦1有係數小的情況,為 丌/、有必須使風扇直徑過度地變大之 題。此外,在將這種西洛 务了風扇用於空調裝置的情況,若 風扇寬度窄,在執交換呙办 „ ”、、換态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 、 變成不均勻,而熱交換器的導熱 性月b降低,亦具有壓縮機 0 〈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 2供西洛可風扇及使用該風扇之空調襄置,而該風扇作成 降低在供給既定量之吹屮 人出風置時所產生的聲音。 【解決課題之手段】 本發明之西洛可魚 ,, ",匕括··蜗形殼,係具有用以取 入空氣的吸入口、用以吹 囬工軋的吹出口、以及從該吸入 口至該吹出口的風政. ,風扇,係被收容於該蜗形殼内,藉201002944 IX. Description of the invention: [Technical field of the invention] The air conditioner fan and the gas invention are related to the sirocco fan and the use of the fan, in particular, the use of the fan for making a sound for reducing the sound generated Air conditioning unit. [Prior Art] Shape, since the past, there is a multi-blade centrifugal fan that has a cylinder/' and can blow a t-wide band to the air-conditioned object area, and is often used in an indoor unit that constitutes an empty (four), or Dehumidification ::::Net machine, etc. Such a sirocco fan generally has a plurality of elongated cores: a fan which is arranged on the circumference and is formed in a cylindrical shape as a whole, and is housed in a volute casing which is blown out from the mouth. And the air that the Sloan fan takes in from the inhalation, the work m (four), and the air-conditioning object from the air outlet side. As a kind of siro fan, it is proposed to "- a multi-blade fan, including: : here: ... a plurality of multi-blade centrifugation connected along the same shaft: a fan unit, and a plurality of multiples for housing the connection An outer casing of a centrifugal fan-shaped wind feather, the casing is formed to continuously blow air discharged from the plurality of fan units to the outside, and the flow path is continuously connected to the plurality of multi-blade centrifugal fan units. The flow path" (for example, refer to Patent Document 1). Patent Document 1: Japanese Laid-Open Patent Publication No. Hei No. Hei No. 1 324 984 (page, 7 to 8) Ang 2148-9915-PF 5 201002944 ·- [Summary of the Invention] In the blade of the blade, The loss coefficient of the operating point is located closer to the open side than the unstable area, and has a problem that the width of the moving point is narrow and the noise generated by the t in the fan is large at a predetermined air volume. When the sirocco fan supplies a certain amount of air to the air conditioner, the sound generated by the fan becomes large, and becomes noise, and is transmitted to the object area, so that the user feels that the ##° is uncomfortable. In addition, if the predetermined noise is reduced, the blower's airflow $ from the sirocco fan becomes small, and if the blown air volume is increased, the α 喿 sound value becomes large, and the right wei a 〃 有 〃 〃 〃 And the balance of the sound is produced. Further, when the width of the fan is small, the noise is small, and if the coefficient is small, the diameter of the fan must be excessively increased. In addition, in the case where such a Xiluo fan is used for an air conditioner, if the fan width is narrow, the speed distribution in the width direction of the heat exchanger in the case where the switching is performed, and the state of the shift is located on the downstream side of the fan. It becomes uneven, and the heat conductivity month b of the heat exchanger is lowered, and the compressor 0 has a problem of increasing power consumption. 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 order to solve the above problems, and the object of the present invention is to provide a sirocco fan and an air conditioner using the same, and the fan is configured to reduce the occurrence of a blown air supply when a predetermined amount is blown. the sound of. [Means for Solving the Problem] The sirloin fish of the present invention, "including a volute casing, has a suction port for taking in air, a blow port for blowing back the work, and The suction port to the outlet of the wind. The fan is contained in the volute casing.
2148-9915-PF 201002944 由進行轉動驅動而從与r明 > 勒阳攸这及入口取入空氣並從該吹迚口吹 "氣,以及鈴嘴,係安裝於該堝形殼的該吸入口丨其特 '在於.在5亥吸·入口位於該風扇之轉動中心的延長線上, 並形成於㈣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、該 :扇之轉軸方向的寬度A L[_卜k為常數 '該堝形殼的 巧度為 H=246k[_]、P/Q2 為損失係數 p [pa/(m3/min) 2] 的清況,在0. 1 g k4 f客〇. 4之範圍,作成f (k4 F) = 〇.34947(k^)2- 1.0554(k^) + 1.8> 0.75f(k^)^ L/HS f(k4|:)。 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 政在於.在該吸入口位於該風扇之轉動中心的延長線上, 亚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為Q[mViDin]、該 風扇之轉軸方向的寬度為L[mm]、k為常數、該蜗形殼的 高度為 H = 246k[mm]、P/Q2 為損失係數 g [pa/(m3/min) 2] 的情況,在0.1 S S 0_4之範圍,作成g(k4 ζ )-1.39788( k4^ )2-2. 1108( k4f ) + 1.3 , l.SgQ^^ ^ < L/HS2g(k4f)。 = 又,本發明之空調裝置,其特徵在於:使用上述之西 2148-9915-PF 7 201002944 洛可風扇.。 【發明效果】 右依據本發明之西洛可風扇 決定風扇寬产,以祛n芦 疋根據既疋之數學式 見又以使風扇的動作點位於既定… 可使空氣之吹出風旦* „立 、疋之乾圍,因為 在供^1^和$音取得均衡,所以可有效地降低 、,°既疋置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熊。 第1實施形態 “ 第1圖係透視本發明之第1A ⑽之㈣而声… 感的西洛可風扇 整體/狀Γ 立體圖。第2圖係表示風扇1之 H 第3圖係表示西洛可風扇_之剖面 可二:!縱向剖面圖。根據第1圖〜第3圖,說明西洛 風扇1〇0之整體構造。此西洛可風扇100孫刹田 :氣:或除濕機等之空調裝置的室内機、或於^ =等者。此外,包含第1圖在内,在以下之圖面二 構成構件之尺寸的關係和實際者相異之情況。 :第:圖所示,西洛可風扇m由以下之構件構成, ^ 係將複數支細長的葉片板(葉片)排列於圓周上, =整體變成圓筒形;堝形殼2’係收容風扇卜並在内部 成風路,以及鈴嘴3,係風扇1之轉動中心的延長線上 (以下僅稱為轉轴上),並安裝於堝形殼2之 /、有t動中心’藉由轉動而吸人空氣,並吹出該空氣。 2148-9915-PF 8 201002944 蝎形殼2由以下之構件構成,吸入口 2a,係形成於轉轴上 的開口;吹出口 2b,係向對象區域吹出從吸入口 2a所吸 入的空氣;以及風路2c’係朝向風扇1之轉動圓周方向开> 成蝸形殼形狀(曲線形狀),··並使吸入口 2a和吹出口 2b連 通。 鈴嘴3係加工開口而形成,並安裝於蝸形殼2的吸入 口 2a,作成可將從吸入口 2a所取入之空氣集中增速並供 給風扇1。風扇1能以例如必192ran]構成風扇直徑d,以例 如15〇〜4_m構成寬度尺寸L,以例如4〇片構成葉片板 數。蜗形殼2能以246mm構成蜗形般高度H。此外,未 別:定鈐嘴3的形狀’例如可因應於風扇直徑〇之長度而 決定, 第4圖係表示西洛可涵戸2148-9915-PF 201002944 is driven by the rotation and is taken from the inlet and the inlet of the air, and the air is blown from the mouthpiece, and the bell is attached to the dome. The suction port is characterized by the fact that the inlet is located on the extension line of the center of rotation of the fan and is formed on both sides of the (four) shaped shell, and the ventilation resistance in the air passage is P [Pa], The amount of air taken in from the suction port is: the width AL of the axis of the fan in the direction of the axis of rotation [_b is a constant 'the complexity of the dome-shaped shell is H=246k[_], and P/Q2 is the loss coefficient. The condition of p [pa/(m3/min) 2] is in the range of 0. 1 g k4 f 〇. 4, and is made f (k4 F) = 〇.34947(k^)2- 1.0554(k^) + 1.8> 0.75f(k^)^ L/HS f(k4|:). 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 path from the suction port to the blow port; the fan is fastened Storing in the volute casing, taking in air from the suction port by blowing and blowing air from the air outlet; and the bell mouth is attached to the suction port of the volute casing; In the extension line of the suction port located at the center of rotation of the fan, the one side of the volute casing is sub-formed, and the ventilation resistance in the air path is P [Pa], and the air taken in from the suction port The amount is Q[mViDin], the width of the fan in the direction of the axis of rotation is L[mm], k is constant, the height of the volute is H = 246k [mm], and P/Q2 is the loss coefficient g [pa/( In the case of m3/min) 2], in the range of 0.1 SS 0_4, g(k4 ζ )-1.39788( k4^ )2-2. 1108( k4f ) + 1.3 , l.SgQ^^ ^ < L/HS2g (k4f). Further, the air conditioner of the present invention is characterized in that the above-mentioned West 2148-9915-PF 7 201002944 Rockwell fan is used. [Effect of the Invention] According to the sirocco fan of the present invention, the fan is widely produced, and the 疋n reed is seen according to the mathematical formula of the 疋n, so that the operating point of the fan is located at the predetermined position... the air can be blown out of the wind* In addition, since the balance is provided between the supply and the sound, it is possible to effectively reduce the sound generated when the air volume is blown. In the first embodiment, the first embodiment is a perspective view of the sirocco fan as a whole in the first aspect of the present invention. Fig. 2 shows the H of the fan 1. Fig. 3 shows the cross section of the sirocco fan _. The overall structure of the Xiluo fan 1〇0 will be described based on Fig. 1 to Fig. 3 . This Silo fan 100 Sun Brake: Air: or indoor unit of an air conditioner such as a dehumidifier, or ^^. In addition, the relationship between the dimensions of the constituent members of the following two drawings, including the first drawing, is different from the actual one. : In the figure: the sirocco fan m is composed of the following members, ^ is a plurality of elongated blade plates (blades) arranged on the circumference, = the whole becomes a cylindrical shape; the 埚-shaped case 2' is a receiving fan Bu is internally formed into a wind path, and the bell mouth 3 is an extension line of the center of rotation of the fan 1 (hereinafter simply referred to as a rotating shaft), and is attached to the dome-shaped housing 2, and has a t-moving center' by rotating Inhale the air and blow the air out. 2148-9915-PF 8 201002944 The clamshell 2 is composed of the following members, the suction port 2a is an opening formed on the rotating shaft, and the air outlet 2b blows air sucked from the suction port 2a to the target region; The path 2c' is opened toward the rotational direction of the fan 1 and has a volute shape (curved shape), and the suction port 2a and the air outlet 2b are communicated. The bell mouth 3 is formed by machining an opening, and is attached to the suction port 2a of the scroll case 2, and is configured to increase the speed of the air taken in from the suction port 2a and supply it to the fan 1. The fan 1 can constitute a fan diameter d by, for example, 192 ran, for example, 15 〇 to 4 mm to form a width dimension L, for example, a number of blades to form a blade number. The volute casing 2 can form a volute-like height H of 246 mm. Further, the shape of the nozzle 3 is determined, for example, depending on the length of the fan diameter ,, and Fig. 4 shows the sirocco 戸
胜从 备了風扇100之卜Q特性及KS-Q 特性的圖形。根據第4圖 y 說明西洛可風扇100的P—Q 特性及Ks—Q特性。在此, y [m3/m. 1 v - 不靜壓[Pa],ΰ表示風量Winning from the fan 100's Q characteristics and KS-Q characteristics of the graphics. The P-Q characteristics and Ks-Q characteristics of the sirocco fan 100 are illustrated in accordance with Fig. 4 y. Here, y [m3/m. 1 v - no static pressure [Pa], ΰ indicates air volume
Lm /min] ’ Ks表示比噪音[仙 ^ 學式Ks_SPI 1 n ,比曰Ks係根據數 ^ ^ Ks-SPL- 10 . i0gl〇(p . q2. 示噪音值,使用在從安裝於 者。此外,SPL表 之中心,沿著轉軸上跖觖;° 〃设2之吸入口 2a的鈴嘴3 扇10。所產生之噪音的’勺位置,測量從西洛可風 性,而空白圓記號表示κ :黑圓形記號表示p-Q特 動作點。 寺性。此外’(1)〜(3)表示 p— Q特性係表示在風扇丨 阻力之靜壓Ρ(左側縱轴 ^迷固定的狀態,係通風 〇風篁Q(橫軸)的關係。如第4Lm /min] ' Ks indicates the noise ratio [Xian ^ Ks_SPI 1 n , 曰 Ks is based on the number ^ ^ Ks-SPL - 10 . i0gl 〇 (p. q2.) The noise value is used in the slave installation. In addition, the center of the SPL table, along the axis of rotation; ° 〃 2 the mouth of the suction port 2a of the bell 3 fan 10. The noise generated by the 'spoon position, measured from the Silo wind, and the blank circle mark κ: The black circle symbol indicates the pQ special action point. Temple characteristics. In addition, '(1) to (3) indicate that the p-Q characteristic is expressed in the static pressure of the fan 丨 resistance (the left vertical axis is fixed, The relationship between ventilation hurricane 篁Q (horizontal axis).
2148-9915-PF 201002944 圖之黑圓形記號所々,靜壓愈小在風& 2e風愈易流動, 而靜塵愈大在風路2e風愈難流動。即,在動作點⑺,易 得到風量,在動作點⑴,料到風量。因此,靜壓愈小 風量愈大,而靜壓愈大風量愈小。此外,在以下的說明, 將高靜壓且低風量側稱為關閉側(圖形的左上側),而將低 靜壓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,靜壓 亦變小的區域。將此區域稱為不安定(surging)區域(在^ 4圖所示之虛線包圍區域)。在這種不安定區域,在風路 2c内之空氣的流動易變成不安定。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)如第4圖之空白圓記號所 不,風量Q增加時變大。此比噪音Ks係考慮到靜壓p和 風量Q的°喿音值。 第5圖係表示西洛可風扇1〇〇之L()/H。和損失係數^ 的關係之圖形。根據第5圖,說明西洛可風扇1 〇〇之 和知失係數的關係。此第5圖,係將蝸形殼高度Η。固 定為246mm ’使風扇寬度尺寸l。在150 ~ 50 Omm之間變化, 使用對損失係數I:。= p。/ Q。2 [ p a / ( m 3 / m i n ) 2 ],比π喿音K s變 成最小之寬度尺寸L。,表示Lo/Ho和損失係數f d的關係。 在此第5圖’縱軸表示“/Η。,橫軸表示損失係數I: 0。 損失係數f D= pe/Qa2,在第4圖所示之P— Q特性上, 表不損失係數f °愈大愈接近關閉側,損失係數f 〇愈小愈 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 201002944 的位置而求得的值。又,L()/H。表示將蝸形殼高度h固定, 而改緩:見度尺寸L。之情況的比例。從第5圖得知,根據損 失係數f。,可知比噪音Ks變成最小之寬度尺寸L。產生變 化。亦即,愈是損失係數g。小之開‘側,比噪音Ks變成 最小之覓度尺寸L。愈長。因此,自第5圖,在將損失係數 芕〇 δ又為〇· 1 $ f各0. 4之範圍的情況,設f ( f ) = 〇. 34947 f —l‘0554 f+l,8,Lci/Hd= f ( p )時,比噪音 Ks 變成最 J 此外’ $(^) = 0.34947^2 — 1.0554^+1.8 係從第 5 圖 所示之圖形所算出的式子。 其次,說明比噪音Ks因損失係數g ^及寬度尺寸L〇 而變化的理由。 第6圖係表不將寬度尺寸L。設為230或30 0匪,通過 :作點A之情況的西洛可風肩“〇。之p—Q特性及Ks—q ^ &的圖形°又’黑圓形記號表示寬度尺寸L。為230mm之 情況的P—q特性,而空白圓記號表示寬度尺寸L。為 V:-: 之情況的P—Q特性,黑三角形記號表示寬度尺寸L。為 __之情況的Ks—Q特性,而空白三角形記號表示寬度 尺寸L°為300_之情況的Ks— Q特性。此外,在此所說明 之動作點係根據單元之設計風量、及設計靜壓(熱交換器 抑k風阻力、或單%的風路、管之風路的通風阻力、過淚 器等之通風阻力)而決定。 ’。、 字1度尺寸L。设為230mm、300mm的情況,比較通 I動作點八之^特性時,得知寬度尺寸比較長的 _,不女疋區域移至p— Q特性之圖形的右下(開放2148-9915-PF 201002944 The black round mark of the figure shows that the smaller the static pressure is, the more wind and the wind become easier to flow, and the more the static dust is, the more difficult it is to flow in the wind 2e. That is, at the operating point (7), the air volume is easily obtained, and at the operating point (1), the air volume is expected. Therefore, the smaller the static pressure, the larger the air volume, and the larger the static pressure, the smaller the air volume. Further, in the following description, the high static pressure and low air volume side will be referred to as the closing side (the upper left side of the figure), and the low static pressure and high air volume side will be referred to as the open side (the lower right side of the figure). However, as shown in Fig. 4, there is a localized area where the static pressure is small even if the amount of wind is small. This area is referred to as a surging area (the dotted line enclosed area shown in Fig. 4). In this unstable area, the flow of air in the wind path 2c tends to become unstable. That is, the 'unstable area is a region where the possibility of abnormal noise is high due to the instability of air flow. Further, the specific noise Ks (right vertical axis) is not as long as the blank circular mark of Fig. 4, and becomes larger when the air volume Q is increased. This specific noise Ks takes into account the hysteresis value of the static pressure p and the air volume Q. Figure 5 shows the L()/H of the sirocco fan. A graph of the relationship with the loss factor ^. According to Fig. 5, the relationship between the sirocco fan 1 and the loss factor is explained. In the fifth figure, the volute casing is highly sturdy. Fix it to 246mm ' to make the fan width size l. Change between 150 and 50 Omm, using the loss factor I:. = p. / Q. 2 [ p a / ( m 3 / m i n ) 2 ], which becomes the smallest width dimension L than the π 喿 K s. , represents the relationship between Lo/Ho and the loss coefficient f d . In Fig. 5, the vertical axis represents "/Η., the horizontal axis represents the loss coefficient I: 0. The loss coefficient f D = pe / Qa2, and in the P-Q characteristic shown in Fig. 4, the loss coefficient f is shown. The larger the temperature is, the closer it is to the closing side, and the smaller the loss coefficient f is, the closer it is to the open side. Further, the loss coefficient is a value obtained from the position of the operating point (p, Q) 2148-9915-PF 10 201002944 described later. , L()/H, which means that the height h of the volute casing is fixed, and the ratio of the case of the visibility dimension L is changed. From the fifth figure, according to the loss coefficient f, it is known that the specific noise Ks becomes the smallest. The width dimension L. changes, that is, the more the loss coefficient g. The smaller the opening side, the longer the noise size Ks becomes the smallest dimension L. Therefore, from Fig. 5, the loss coefficient 芕〇δ In the case of 〇·1 $f each of the range of 0.4, let f (f) = 〇. 34947 f —l'0554 f+l,8,Lci/Hd= f ( p ), the specific noise Ks becomes The most J is '$(^) = 0.34947^2 - 1.0554^+1.8 is the equation calculated from the graph shown in Fig. 5. Next, the ratio of the noise Ks due to the loss coefficient g^ and the width dimension L〇 is explained. The reason for the change. Fig. 6 shows that the width dimension L is not set to 230 or 30 匪, and the sirlo wind shoulder of the case of the point A is "〇. The p-Q characteristic and the pattern of Ks_q^ & and the 'black circle mark' indicate the width dimension L. The P-q characteristic is the case of 230 mm, and the blank circle mark indicates the width dimension L. The P-Q characteristic for the case of V:-:, the black triangle mark indicates the width dimension L. The Ks-Q characteristic is the case of __, and the blank triangle mark indicates the Ks-Q characteristic of the case where the width dimension L° is 300_. In addition, the operating points described here are based on the design of the unit's air volume, and the design of static pressure (heat exchanger k wind resistance, or single% of the wind path, ventilation of the duct air duct, tears, etc.) Resistance). ’. , word 1 degree size L. When it is set to 230mm or 300mm, when the characteristic of the I-operation point is compared, the _ of the width dimension is longer, and the non-female area is moved to the lower right of the graph of the p-Q characteristic (open
2l48-99i5-pF 201002944 而接近動作點A。從第6-圖所示之p—q 简 v叫厂"/f、〜y付性及Ks — Q将性侍去比絮音Ks變成最小的動作點位於不安定區域 附近。但,動作點位於不安定區域或不安定區域附近時, 流動變成不安定,發生逆 a立 變動變大。SI&如 或兴吊曰,或者風量之時間 ㈣:屬實地形成安定之流動的情況,需要 使動作點位於屮X6 ^ 而要 比不女定區域更接近開放側。 即’對某動作ΙΉ P π π < ",),使風扇的容積變大時,在ρ__ Q特性圖,不安定區 不安定區域離開開放側(即動作點比 兪易發生昱當立 Q知·14圖之右下側)愈遠, 遍生異"。此原因係,在外殼 示之2M)、或鈐喈以在第3圖所 π紫之和風扇的距離短之區 大。在本發明,作成對所預 & _動變 積變大,使不安定區域移動 乍』,藉由使風扇的容 量接近’使所產生之噪音變少。作點和不安定區域儘 在此,為了使風扇的容積變大 大’或使風扇的寬度變寬。可是,二到使風扇直徑變 元高度變成過高。在本發明,可得:―:扇直捏變大,單 單元高度變成過高’以風扇的寬度:二其不會使 用以可使動作點和不安定區域^的方式構成, 設置限制少,而且可降低劈音。“成最佳之單元的 弟7圖係表示風扇1的每-片葉片拓 葉片板的位置之關係的圖形。根據之:片間風量和 可風扇1 00之風扇丨的每— θ,3兄明構成西洛 板的位置之關係的圖形二之茱片間風量和葉片 圖’縱軸表示每-片葉2l48-99i5-pF 201002944 and close to action point A. From the p-q simplifications shown in Fig. 6 to the factory, "/f, ~y, and Ks - Q, the action point that becomes the smallest than the smack Ks is located near the unstable area. However, when the operating point is located in an unstable area or in the vicinity of an unstable area, the flow becomes unstable, and the fluctuation becomes large. SI& If the hoisting, or the time of the wind (4): In the case of a steady flow of stability, the action point needs to be located at 屮X6^ and closer to the open side than the non-female area. That is, for a certain action ΙΉ P π π <",), when the volume of the fan is increased, in the ρ__ Q characteristic map, the unstable region of the unstable zone leaves the open side (that is, the operating point is more likely to occur. Q knows the lower right side of the 14th map. The farther it is, the more different it is. The reason for this is that the area shown in the outer casing is 2M), or the distance between the fan and the fan in the third figure is short. In the present invention, the pre- & _ motion is made larger, and the unstable area is moved. By making the capacity of the fan close to 'the noise generated is small. The point of the operation and the unstable area are here, in order to make the volume of the fan large, or to widen the width of the fan. However, the second is to make the fan diameter change height too high. In the present invention, it is obtained that: - the fan is straightened and the height is increased, and the height of the single unit becomes too high 'to the width of the fan: the second is not used to make the operating point and the unstable area ^, and the setting limit is small. And it can reduce the arpeggio. "The figure 7 of the best unit represents the relationship between the position of each blade of the fan 1 and the position of the blade. According to this: the air volume between the sheets and the fan of the fan 100 丨, θ, 3 brothers The relationship between the position of the sill plate and the position of the blade. The vertical axis indicates the per-leaf
214 8-9915-PF 201002944 片板之葉片間周. 在第7 (m/min),橫軸表示葉片板的位置。又, _ "'“、圓形記號表示在動作點(1)的每一 # _ 之葉片間風量和葦Hs 片茱片板 在動作點⑵的: 置之關係,空白菱形記號表示 乍』(2)的母—片葉片板之葉片 置之關係,里二& r 里子某片板的位 -角形纪號表示在動作點(3)的每一片苹 板之茱片間風量和葉片板的位置之關係。 某片 片板I:片圖’對於縱軸所示之風扇1的每-片葉 往外周側之流動二m3葉片(葉片板)的内周側 内周側H 示風從葉片的外周側往 間倒之•動的情況。又,在第7圖 橫軸所示之葉片板的位置。即,將荦片板的二 達 。時〇分~12時。分之時… 板的位置置換成在 第7圖所- _的短針之位置來表達。此外, 圖所不之動作點⑴〜動作點⑻,表示和第 之動作點⑴〜動作點⑻相同的動作點。 不 附,:7圖所示’得知在葉片板的位置位於Π)時30分 附近的情況’愈往開放側葉片間風量命大一 葉片間風量愈小。又,^ / 〇里愈大’而愈在關閉側 的巴域9時30分士時30分以外 的£域,葉片間風量未 μ(在葉片板片㈣心的情Γ麵。設葉片間風量為 肌、風扇輸入值[大致以二兄’,’關於噪音值 ⑺式)成立。 ^下所不之數學式(第⑴式及第 第⑴式 sm〇. log!eQl6 第⑺式 W 〇: Σ Q i 3 因此’葉片間風量Qi的分布愈均勾,噪音值肌及214 8-9915-PF 201002944 Inter-blade circumference of the sheet. At 7th (m/min), the horizontal axis indicates the position of the blade. Further, _ "'", the circular mark indicates the relationship between the air volume between the blades of each # _ at the operating point (1) and the position of the 苇Hs piece 在 plate at the operating point (2), and the blank diamond symbol indicates 乍(2) The relationship between the blade of the mother blade and the blade of the blade, the position of the blade of the second & r ri is the volume of the blade and the blade of the blade at the action point (3). The relationship between the positions of the sheets I: the sheet image 'the inner circumference side of the inner circumference side of the inner side of the two m3 blades (blade plates) of the fan 1 on the outer peripheral side of the fan 1 shown on the vertical axis The outer peripheral side of the blade is turned upside down. In addition, the position of the blade plate shown on the horizontal axis of Fig. 7 is that the two pieces of the cymbal plate are divided by ~12 hours. The position of the plate is replaced by the position of the short needle in Figure 7 - _. The operation points (1) to (8) of the figure indicate the same operating point as the first action point (1) to the action point (8). Attached,: Figure 7 shows that the situation near the 30 points when the position of the blade plate is located is 'the more the air volume between the blades on the open side The smaller the amount of wind between the sheets, the larger the ^ / 〇 ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' ' Γ 。 。 。 。 。 。 。 。 。 。 。 。 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌 肌eQl6 Equation (7) W 〇: Σ Q i 3 Therefore, the distribution of the air volume Qi between the blades is more uniform, the noise value of the muscle and
2148-9915-PF 13 201002944 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的分布係岣 勻,所以比噪音Ks變成最小值,在此,如上述所示,反 之動存點愈接近不安定區域,即愈接近Le/He= f ( $ ),雖 然比噪音Ks變成愈小,但是超過L()/H()= 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, 動作點比不安定區域愈遠離開放側,在殼之舌部(在第3 圖所示之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,設0<nS :l、nxf( f。),在損失係數小之 條件(風量大,通風阻力小)的情況,即在4 之範圍,求不產生異常音之最小的n時,係n = 〇75。因而, 在損失係數小之條件(風量大,通風阻力小)的情況,即在 可形成比噪音Ks小、不會產生異常音的流動。 在上述的說明,說明螞形殼高度η^246μ的情況,接 著說明將螞形般高度之尺寸一般化的情況…為常數, H、Ln=kDQq尺寸變化的情況,自相似法則, :於P及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 整理後,得到第(5) 第(4)式 Q=Q°(D/D〇)3(N/N。) 從第(3)式及第(4)式’消去N/n。 式。 2148-9915-pp 14 201002944 第(5)式 P°/Q°2= P/Q2(D/D。)3 將n/Q2、D,。代入 第(6)式式而得到第U)式 使用第(6)式及H = kH8、L = kLe,可將 〇·ΐ44〇·4 —般化成。 。力价。)“。/…“。) 〇、 L/HS f(k4|:)。 战 〇. 75f(k4f )s 即,在將風扇i用於在風扇之下 空調裝置之情況,在損 匕括熱交換器的 丄、 相失係數小之條件(風旦i 力小)的情況’藉由使風扇寬度變寬:丨’通風阻 而且熱交換器之寬度方向的速度分布接為/音變小, 會不必要地增加屢縮機的耗電力。 —L所以可不 其次,說明西洛可風扇1〇〇為單吸入式 將上述之L置換成L/2iQ置換成Q/可。 若設 卿2)2},則此η = 1.3978;α^22148-9915-PF 13 201002944 The smaller the fan input value w. That is, as shown in Fig. 4, in the case of the operating point (1) close to the unstable area, since the distribution of the air volume Qi between the blades is uniform, the specific noise Ks becomes the minimum value, and as shown above, On the contrary, the closer the moving point is to the unstable area, the closer to Le/He= f ( $ ), although the smaller the noise Ks becomes, the more the L()/H()= f ( $ ) is exceeded. Located in an unstable area, it is worse than the noise Ks. On the other hand, the action point is farther away from the open side than the unstable area, in the tongue of the shell (2bl shown in Fig. 3), or the distance between the bell mouth and the fan is short, because the static change becomes larger. Therefore, it is easy to generate abnormal sounds. Therefore, it is assumed that 0 < nS : l and nxf ( f.), when the loss coefficient is small (the air volume is large and the ventilation resistance is small), that is, in the range of 4, when the minimum n of the abnormal sound is not generated, n = 〇75. Therefore, in the case where the loss coefficient is small (the air volume is large and the ventilation resistance is small), it is possible to form a flow that is smaller than the noise Ks and does not generate an abnormal sound. In the above description, the case where the height of the anatomical shell is η^246μ will be described. Next, the case where the size of the eagle-like height is generalized will be described as a constant, and the case where the size of H, Ln=kDQq changes, the law of self-similarity, :P And Q, the mathematical formulas shown below (Formula (3) and (4)) are established. Here, the N system speed. After the formula (3) is sorted, the (5)th (4) formula Q=Q°(D/D〇)3(N/N.) is obtained. The equations (3) and (4) are eliminated. /n. formula. 2148-9915-pp 14 201002944 Equation (5) P°/Q°2= P/Q2(D/D.)3 will be n/Q2, D,. Substituting the equation (6) to obtain the formula U) By using the equation (6) and H = kH8 and L = kLe, 〇·ΐ44〇·4 can be generalized. . Price. ) "./...". ) 〇, L/HS f(k4|:). 〇. 75f(k4f )s that is, in the case where the fan i is used for the air conditioner under the fan, the condition of the enthalpy and the phase loss coefficient of the heat exchanger is small (the wind force is small) By widening the width of the fan: 通风 'ventilation resistance and the speed distribution in the width direction of the heat exchanger is reduced to a small sound, the power consumption of the repeater is unnecessarily increased. - L, so the second is that the sirocco fan 1 is a single suction type. The above L is replaced by L/2iQ and replaced with Q/. If you set 2) 2}, then η = 1.3978; α^2
'2-H〇8(k^)H.8^ 1.5g(k4n^L/H^2g(k,f )〇 J 在:洛可風扇i〇〇為單吸入式的情況,在01^β〇 4 之粑圍’藉由作成15g(k4|: )SL/H‘2g(k4F ),而可形 成比噪音Ks小、不會產生異常音的單元。 在上述的§尤明,雖然說明西洛可風扇i 〇 〇單體的情 况仁疋對於將西洛可風扇1 〇 Q骏載於空調機、或除濕機、 空氣清淨機等之單元的情況之動作點,亦可一樣地決定。 匕隋况求單元之轉速N1、及單元的風量Qi’再從西洛 可風扇100單體的P一q特性,使用轉速Νι及風量I,求 2148-9915-PF 15 201002944 靜£ P,即可。在此,在單元裴載m個風扇的情況,嗖1個 風扇的風量為Ql/m、靜壓為L,求損失係數即可。 产、兄由得知’在西洛可風扇^為雙吸入型的 .=f=〇.4之範圍,藉由作成〇 =咖’而可形成比…小、安定:I: / Τ風扇10。為單吸入型的情況,在〇1 :::立:由作成1她咖離…而―可形 成比朱S Ks小、安定的流動。 第9第:圖係表示鈴嘴3之縱向剖面構造的示意剖面圖。 圖第;n不鈐嘴3之區域α的西洛可風扇1。。之立體 圖。弟10圖係表示兰+广, ,…奴差之區域α的部分在壁面上之兽 :二::rms值之區域“部分的放大圖。 11圖係表示 域二==部分在壁面上之_動的·值之區 == 根據第8圖〜第11圖,-面比較以將 &差形成於堝形殼2之側面的方式Μ鈴嘴3者, ι.., ? 形级2之側面未形成段差之 容护於界、々_^ 、文扶鈐嗝3者,一面說明 裝於西洛可風扇1⑽之鈴嘴3的特徵。 在第8圖所示之鈐嘴3的縱向 扇100側之端點(在铃嘴3 ^ ’设西各可風 ^ A' ^ 、開口 °p的端點)為點A及 :為對鈴嘴3之中心和點A,點對稱的點)、另一方 的端點(在鈐嘴3之最大開口部的端 為對浐喈q為點β及點B,(成 =1 繼點對稱的點)、設從點Β向風扇】 之方向所拉的直線和蝸形殼2側面 β ’向厨戶彳 又點為點C、設從點 羽之方向所拉的直線和蜗形殼2側面的交㈣ 2148-9915-PF 16 201002944 點C 、設爲段AA’和風扇1之轉軸延長線的交點為點〇 加以說明。 即’ BC>〇時以段差形成於蜗形殼2側面之方式安裝鈐 嘴3, BC =。時以在蝸形殼2側面未形成段差之方式安裴鈐 觜^此外,以BC>0時BC之長度為5[mm]、區域α以外 之靜壓變動的rms值大約〇[Pa]為例。在第9圖〜第11圖, 如第8圖所示根據鈴嘴3的安裝法,比較並表示在蝸形殼 2侧面形成段差者之靜壓變動、和在螞形殼2侧面未形成 段差者的靜壓變動。 以下,表示靜壓變動之]~11^值的定義式。 第(Ό式 Ps(t)= ps + ps, 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1Q圖及第n圖得知,㈣形殼2側面形 成段差者之靜壓變動比在則彡殼2側面未形成段差者的靜 壓變動小。因&,在„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1⑽之示意剖面構造的縱 向剖面圖’第13圖係透視西洛可風们〇〇而表示的透視 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nns值大之區域。又,在第12圖,在從構 成西洛可風扇1〇〇之蝸形殼2的風路&至吹出口㉛之弯 曲部分,將最接近風扇i之外周部的部位圖示為舌部卜 2148-9915-PF 17 201002944 在第13圖,在通過第8圖所 的平面和舌邱4夕六始 之點A、點〇以及點A’ 4 4:之父線上,將和風爲 ▲ 點圖示為n 2 " 之距離變成最小的 馬”'、i D、和铃嘴3之勤;η田 於以點。友士 ,點D取近的點圖示為點Ε、位 ”.、占〇為中心從點E之風扇丨的反 為點F、位於以赴η & * 衫方向65之點圖示 方、U點0為中心從點F之風戶 。夕Et固- 風扇1的反轉方向4 0 之點圖不為點G、位於以點〇為中心 動方南η。 处‘."έ F之風扇1的轉 動方向40之點圖示為點H、'2-H〇8(k^)H.8^ 1.5g(k4n^L/H^2g(k,f )〇J In the case of Luo Ke fan i〇〇 is a single suction type, at 01^β By making 15g(k4|: )SL/H'2g(k4F ), it is possible to form a unit that is smaller than the noise Ks and does not generate abnormal sounds. The situation of the Luo Ke fan i 〇〇 〇〇 疋 疋 疋 疋 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西 西隋 求 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 单元 N 单元 单元 单元 N N N N N N N N N N N N N Here, in the case where the unit is loaded with m fans, the air volume of one fan is Ql/m, the static pressure is L, and the loss coefficient can be obtained. The production, brother knows that 'in the West Loko fan ^ The range of .=f=〇.4 of the double suction type can be made smaller than that by making 〇=咖': I: / Τ fan 10. For the single suction type, in 〇1 ::: Li: Made by her, her coffee is away from... and can be formed smaller than Zhu S Ks The flow of stability. The ninth: the figure shows a schematic cross-sectional view of the longitudinal cross-sectional structure of the bell mouth 3. Fig. 1 is a perspective view of the sirocco fan 1 of the area α without the mouth 3; Lan + Guang, , ... the part of the area of the slave's alpha on the wall of the beast: two:: the area of the rms value "partial enlargement. 11 map shows the domain two == part of the wall on the _ moving value Area == According to Fig. 8 to Fig. 11, the surface comparison is performed in such a manner that the & difference is formed on the side of the dome 2, the ι.., ? The features of the bell mouth 3 mounted on the sirocco fan 1 (10) are described on the side of the vertical fan 100 side of the squirrel 3 shown in Fig. 8. Point (in the bell mouth 3 ^ 'set west each wind ^ A ' ^, the end of the opening °p) point A and: point to the center of the bell mouth 3 and point A, point symmetry point), the other side The end point (the end of the largest opening of the mouth 3 is a line which is the point β and the point B for 浐喈q, (the point which is =1 point symmetry), and the direction drawn from the point Β to the fan] Spiral shell 2 side β 'to the kitchen The point is point C, the line drawn from the direction of the point feather and the side of the volute casing 2 (4) 2148-9915-PF 16 201002944 point C, the intersection of the section AA' and the extension of the shaft of the fan 1 is the point ' 。 即 即 即 即 即 即 即 即 即 即 即 即 即 即 即 即 即 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤 钤The rms value of the static pressure fluctuation other than the area α at time 5% is about 5 [mm], and rm [Pa] is taken as an example. In Fig. 9 to Fig. 11, as shown in Fig. 8, according to the mounting method of the bell mouth 3, the static pressure variation of the step formed on the side of the scroll case 2 is compared and the step difference is not formed on the side of the petal case 2. The static pressure of the person changes. Hereinafter, the definition formula of the ~11^ value of the static pressure fluctuation is shown. ((P)(ps) = ps + ps, rms value of (8) = {( Σ ps' (t) 2)}0.5 Here, ps represents the time average, and Ps, (t) represents the static pressure The larger the rms value of the static pressure change on the wall, the greater the noise generated from the wall surface. From the 1st and nth figures, the static pressure variation ratio of the side surface of the shape of the shell 2 is In the case where the step of the clamshell 2 is not formed, the static pressure fluctuation is small. Because of &, the noise generated on the side of the casing 2 can reduce the noise generated. Fig. 12 shows the schematic cross-sectional structure of the sirocco fan 1 (10). The longitudinal section view 'Fig. 13 is a perspective perspective view showing the Xiluo winds. According to Fig. 12 and Fig. 13, the area of the nns value of the static pressure change of the Xiluo fan is shown. Further, in Fig. 12, the portion closest to the outer circumference of the fan i is illustrated as a tongue from the curved portion of the air passage & to the air outlet 31 which constitutes the scroll casing 2 of the sirocco fan 1部卜2148-9915-PF 17 201002944 In Figure 13, the point A, the point 〇 and the point A' 4 4: the parent line passing through the plane and tongue of the figure 8 , the wind is ▲ point is shown as n 2 " the distance becomes the smallest horse "', i D, and the mouth of the bell 3; η Tian is at the point. Friends, point D is close to the point shown as Point Ε, bit "., occupying the center as the center from the point E of the fan 丨 is the point F, located in the η & * shirt direction 65 point of the graphic side, U point 0 as the center from the point F of the wind夕Et solid - the point of view of the reverse direction of the fan 1 is not the point G, and is located at the point 〇 centered on the south η. The point of the rotation direction 40 of the fan 1 of '."έ F For point H,
Ml戶1 aa ^ 1於以點〇為中心從點F之 風扇1的轉動方向180。之點圖示為點卜 如此地疋義區域的情況 壓變動的r ^兄仔知在西洛可風扇100之靜 主芰勖的rms值大之區域,係遠 ,^ ^ ^ 你運接點Η、點F以及點G之 大致固弧HFG的區域。因此,抓名 具 °又在圓弧HFG之線段BC的 度為Χ、在大致圓弧HIG(連接駄Η叫τ Λ 逆接點Η、點I以及點G之圓 弧)之線段BC的長度為γ時,在 ^ ^ m 了任 L/H$ f( f )或 L/HS g( f ) 之乾圍,若係成為χ>γ 2 〇The M1 household 1 aa ^ 1 is in the direction of rotation 180 of the fan 1 from the point F centered on the point 〇. The point is shown as the point where the pressure of the situation in the derogatory area is r ^ brothers know that the rms value of the static main sill of the sirocco fan 100 is large, ^ ^ ^ your contact point The area of the substantially fixed arc HFG of Η, point F, and point G. Therefore, the length of the line segment BC of the line BC in the circular arc HFG is Χ, and the length of the line segment BC in the approximate arc HIG (the arc connecting the τ τ Λ reverse point Η, the point I and the point G) is In the case of γ, the dry circumference of L/H$ f( f ) or L/HS g( f ) is obtained as ^χ>γ 2 〇
估坪, 7幹令3,可使靜壓變動之MS 值央小’而可使噪音變小。 如第10圖及第11圖如- 丄 H斤不,在蝸形殼2側面未形成段 差的情況,在圓弧HFG的區域 之靜壓變動的rms值最大係 I’而㈣㈣2側面形成段差的情況’在圓弧HFG的 區域之靜壓變動的㈣值最大變成心以下 蜗形殼2側面形成段差,而隊7 、 、 曰 、 降低以鈴嘴3為音源的噪音。 :為其理由係由於’和風看"之距離僅長了形成段差的 里’即線段BC之長度,而抑制因風扇1的轉動所產生之 靜壓變動。 弟1 4圖係表示通過動你肌^ 乍點Β之情況的西洛可風扇1 0 0Estimated ping, 7 dry orders 3, the MS 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, for example, 丄H jin does not form a step difference on the side of the volute casing 2, and the rms value of the static pressure fluctuation in the region of the circular arc HFG is the largest I' and the (4) (4) 2 side faces are formed with a step difference. In the case of the 'fourth value of the static pressure fluctuation in the region of the circular arc HFG, the maximum value becomes a step on the side of the volute casing 2, and the team 7 , , 曰, and the noise of the bell mouth 3 are reduced. The reason for this is that the length of the line segment BC is long because the distance between the 'wind and the wind' is longer than the length of the line segment BC, and the static pressure fluctuation due to the rotation of the fan 1 is suppressed. Brother 1 4 shows the siro fan 1 0 0 by moving your muscles ^ 乍 Β
2148-9915-PF 18 201002944 之P Q特性的圖形.·。炸姑黎, 根據第14圖,說明在堝形殼2側面 形成段差之西洛可風爲1 ΓΪ、S、ra t η L羽1 0 0通過點B的情況之p — Q特性2148-9915-PF 18 201002944 P Q characteristics of the graphics.炸姑黎, According to Fig. 14, the p-Q characteristics of the case where the sirloin of the scorpion shell 2 is 1 ΓΪ, S, ra t η L feathers pass through the point B
及在蜗形殼2側面未形杰❾兰+ ^ AAnd on the side of the volute shell 2 is not shaped as a jasmine + ^ A
不办成#又差之西洛可風扇丨0〇通過點B 的情況之P— Q特性。*楚1 回 在第14圖’黑圓形記號表示在蜗形 殼2側面形成段差之西、、夂a ra e ,n n 〜了風扇100的p — Q特性,空白 0 §己5(¾表不在形句 9仇丨-J- 4* TTy» 1 f 办成2側面未形成段差之之西洛可風扇 100的P — Q特性。又,太贫id π 在第14圖’縱轴表示靜壓P[Pa], 橫軸表示風量Q[m3/min;|。 士第14 ®所示’在蝎形殼2側面开^成段差之西洛可 風扇1 0 0和在蝸形< 2側面未形成段差之西洛可風扇i 〇 〇 比較不安定區域時’得知前者位^開放側。在將在蜗形殼 2側面形成段差之西洛可風扇} 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1〇〇的寬度尺寸變長。即,因 為寬度尺寸短,動作點比比噪音變成最小之不安定區域更The P-Q characteristic of the case of passing the point B is not the result of the #西洛可扇丨0〇. * Chu 1 back in Figure 14 'black circle mark indicates that the west side of the volute case 2 is formed, 夂a ra e , nn ~ the p-Q characteristic of the fan 100, blank 0 § 5 (3⁄4 table) Not in the sentence 9 丨 丨 - J - 4 * TTy» 1 f The P-Q characteristics of the sirocco fan 100 that does not form a step on the side of the 2 sides. Also, too poor id π In the 14th figure, the vertical axis represents static The pressure P[Pa], the horizontal axis represents the air volume Q [m3/min; |. The 14th ® shown in the side of the 蝎-shaped shell 2 is a section of the West Loco fan 1 0 0 and in the volute < 2 When the side is not formed, the sirocco fan i 〇〇 is relatively unsettled, and the 'the open side of the snail shell 2 is slid into the air conditioner, or In the case of a unit such as a dehumidifier or an air cleaner, the size limit of the unit may not be able to lengthen the width of the siro fan 1 。. That is, because the width dimension is short, the operating point is less stable than the noise. More regional
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圖係表不裝载西洛可風扇1〇〇之懸吊式室内機 110的不意整體構造之平面圖。第16圖係表示懸吊式室内 機110之縱向剖面構造的剖面圖。根據第15圖及第丨6圖, 況月將在蝸形设2側面形成段差之西洛可風扇i 〇 〇裝載於 石吊式至内機11 〇的情況之靜壓變動。此外,在第1 5圖, 圖不裝載2台西洛可風扇丄〇〇,並將吸入空間5形成於各 自之足度方向側面的情況。又,在第丨6圖,以箭號表示In the case of approaching the open side, since the unstable area can be brought close to the operating point, it is effective for low noise. Fig. 15 is a plan view showing the unintentional overall configuration of the suspended indoor unit 110 in which the sirocco fan 1 is not loaded. Fig. 16 is a cross-sectional view showing the longitudinal sectional structure of the suspended indoor unit 110. According to Fig. 15 and Fig. 6, the static pressure variation in the case where the sirocco fan i 〇 形成 is placed on the side of the snail-shaped device to the rocker to the inner machine 11 〇. Further, in Fig. 15, there is no case where two sirocco fan blades are loaded and the suction space 5 is formed on the side of each of the sufficient directions. Also, in Figure 6, it is indicated by an arrow
2148-9915-PF 19 201002944 空氣的流動。 將在堝形殼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110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、大之要因的情況。 自上述的#兒明’靜壓變動之rms值大的區域係圓弧hfg, 在其他的區域’靜壓變動之rms值受到和風扇1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17圖,說明從裝載在蝸形殼2侧面形成段差之西 洛可風扇1 00的懸吊式室内機丨丨〇所產生之噪音值、從I 載在蝸形殼2側面未形成段差之西洛可風扇i 〇〇的懸吊式 室内機U0所產生之噪音值。此外,假設段差形成:圓弧 HFG的區域。又,各自表示在吹出風量為16 之情 況的噪音值。 如第17圖所示’得知在吹出風量為16之情 況,在圓弧HFG之區域形成段差者的噪音值係42 4_, 在圓弧HFG之區域未形成段差者的噪音值係44〇_。如 此’藉由在圓請 <區域形成段差,而可使噪音值變小。 自以上’#由在圓弧HFG之區域設置段差,而抑制吸入空 間5的減少,而且可使噪音值變小。 第2實施形態2148-9915-PF 19 201002944 The flow of air. In the case where the sirocco fan 1 形成 which forms a step on the side of the dome 2 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 difference formed, and the noise is large. The cause of the cause. The region where the rms value of the above-mentioned static pressure fluctuation is large is the arc hfg, and the rms value of the static pressure fluctuation in other regions is less affected by the distance from the fan 1. Therefore, when the sirocco fan 100 having a step in the region of the circular arc HFG is mounted on the suspended indoor unit 110, the step can be positioned on the downstream side of the suction port 2a, and the amount of decrease in the suction space 5 can be made small. Fig. 17 is a table showing the noise value of the suspended indoor unit 11〇. According to Fig. 17, the noise value generated from the suspended indoor unit of the sirocco fan 100 which is formed on the side of the volute casing 2 is shown, and the step is not formed on the side of the volute casing 2 from I. The noise value generated by the suspension indoor unit U0 of the West Rock Fan i. In addition, it is assumed that the step difference is formed: the area of the circular arc HFG. Further, each represents a noise value when the air volume is 16. As shown in Fig. 17, it is known that the noise value of the step is 42 4_ in the region where the arc HFG is formed when the air volume is 16, and the noise value is 44 〇 in the region of the arc HFG. . Thus, the noise value can be made small by forming a step in the circle < From the above, ## is set by the step in the area of the circular arc HFG, and the decrease in the suction space 5 is suppressed, and the noise value can be made small. Second embodiment
第18圖係表示本發明之第2實施形態的空調農置15〇 2148-9915-PF 20 201002944 之示意構造的示意構造圖。根.據第1 8圖,說明空調裝置 1 5 0之構造。此空β周裝置1 5 0係裝載第1實施形態的西洛 可風扇1 0 0者。此西洛可風扇1 〇 〇用以對構成空調裝置1 5 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1 5 0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’對设置凝結式熱父換器15 2或蒸發式熱交換器1 $ 4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154的附近’具有將空氣供給凝結式熱交 換器1 52或蒸發式熱交換器1 54之功能。 &細機 ..........册碌令媒壓 縮而變成高溫、高壓之狀態。凝結式熱交換器152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153係將冷媒降壓而使膨脹者。蒸發式熱交換= 154係在空氣和冷媒之間進行熱交換,而使該冷媒^發Ζ 氣化者。藉由對構成此空調裝置150之設置凝結式熱^換 器152或蒸發式熱交換器154的室内機,裝載第}〒於來 態的西洛可風扇10 0,而可降低向室内傳達的噪音。 第18圖所 縮而變成高 在此,簡單地說明空調裝置1 50的動作^ 示之箭號,表示冷媒的流向。被壓縮機1 5丨壓 2148-9915-PF 21 201002944 溫、高壓之冷媒氣體流入凝結式熱交換器1 5 2。在此凝結 式熱交換器1 5 2,冷媒和空氣進行熱交換而凝結,變成低 溫、高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1 5 3降i,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。在蒸發式熱交換器154,冷媒和空氣進行熱交 換而蒸發,變成高溫、低壓之冷媒氣體,再被壓縮機1 51 吸入。在暖房運轉時,將蒸發式熱交換器1 54裝載於室内 機。 在損失係數小、風扇寬度寬的情況,熱交換器之寬度 方向的速度分布接近均勻,和風扇寬度窄、速度分布不均 勻的情況相比,可有效地使用熱交換器的導熱面積。因 而,得到既定之空調性能所需的空氣和冷媒之温差變小, 壓縮機輸入功率變小,而且變成低噪音。又,在損失係數 小的情況,即使風扇直徑沒有變大,只要使風扇寬度變 寬,可使噪音變小。此外,在包括複數個風扇寬度窄之風 扇的空調裝置,藉由置換成風扇寬度寬的風扇,而即使減 少風扇的個數,亦可使在既定動作點之空調裝置的噪音值 變小,而且可使熱交換器之寬度方向的速度分布接近均 勻。 【圖式簡單說明】 第1圖係透視本發明之實施形態的西洛可風扇之内部 而表示的透視立體圖。 2148-9915-PF 22 201002944 第2圖係表 斤〇 、風扇之整體形狀的立髂圖 第3圖係表示 J见•體圖。 下西洛可風扇之示意縱向 圖。 欠叼剖面構造的剖面 弟4圖係表示 四洛可風扇之P— Q特妞 的圖形。 寸生及K S — Q特性 第5圖係表示西、、& y q $ 〆π , 洛可風扇之Lo/H〇和損失t , 係之圖形。 々谓天係數f。的關 苐6圖係表示通沾叙从 p-Q特性及Ksi特神 A之情況的西洛可風屬之 y特性的圖形。 第7圖係表示風戶 > ^ u ^ ¥ 羽的母—片葉片板之葉片間風量和苹 片板的位置之關係的圖形。 茱 弟8圖係矣+ h 嘴之縱向剖面構造的示意剖面圖。 第9圖係表示鈐嘴 薄t b域(2的西洛可風扇之立體圖。Fig. 18 is a schematic structural view showing a schematic structure of an air conditioning agricultural plant 15 〇 2148-9915-PF 20 201002944 according to a second embodiment of the present invention. Root. According to Fig. 18, the structure of the air conditioner 150 will be described. This empty beta device 150 is loaded with the sirocco fan 100 of the first embodiment. The sirocco fan 1 〇 is used to mount an indoor unit (indoor unit) constituting the air conditioner 1 5 于 in the vicinity of the heat exchanger. In the second embodiment, the differences from the above-described first embodiment will be mainly described, and the same portions as those in the first embodiment will be denoted by the same reference numerals and will not be described. The air conditioner (150) is configured by sequentially connecting a condensing heat exchanger 152, a throttle device 153, and an evaporative heat exchanger 154 with a refrigerant pipe. Here, the sirocco fan 1 of the first embodiment is provided for the indoor unit in which the coagulation type heat exchanger 15 2 or the evaporative heat exchanger 1 4 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 the air supplied to the condensing heat exchanger 152 or the evaporative heat exchanger 154. Features. & fine machine .......... The book is compressed and becomes a state of high temperature and high pressure. The condensing heat exchanger 152 is a heat exchange between air and refrigerant to cause the refrigerant to condense or liquefy. The throttle device 153 depressurizes the refrigerant to expand the person. Evaporative heat exchange = 154 is a heat exchange between air and refrigerant, and the refrigerant is vaporized. By installing the sirocco fan 100, which is the condensed heat exchanger 152 or the evaporative heat exchanger 154, which constitutes the air conditioner 150, the sirocco fan 100 is placed in the air supply unit 150, thereby reducing the communication to the room. noise. Fig. 18 is abbreviated to become high. Here, the arrow indicating the operation of the air conditioner 505 will be briefly described, indicating the flow of the refrigerant. Pressurized by the compressor 15 2148-9915-PF 21 201002944 The warm and high-pressure refrigerant gas flows into the condensing heat exchanger 1 52. In the condensing heat exchanger 152, the refrigerant and the air exchange heat to be condensed, and become a low-temperature, high-pressure liquid refrigerant or a gas-liquid two-phase refrigerant. The refrigerant flowing out of the condensing heat exchanger 152 is then lowered by the throttling device 1 5 3 to become a low-temperature, low-pressure liquid refrigerant or a gas-liquid two-phase refrigerant, and then flows into the evaporative heat exchanger 154. In the evaporative heat exchanger 154, the refrigerant and the air are thermally exchanged and evaporated to become a high-temperature, low-pressure refrigerant gas, which is then sucked into the compressor 1 51. When the greenhouse is in operation, the evaporative heat exchanger 1 54 is loaded in the indoor unit. In the case where the loss coefficient is small and the fan width is wide, the velocity distribution in the width direction of the heat exchanger is nearly uniform, and the heat transfer area of the heat exchanger can be effectively used as compared with the case where the fan width is narrow and the speed distribution is uneven. Therefore, the temperature difference between the air and the refrigerant required to obtain the predetermined air-conditioning performance becomes small, the input power of the compressor becomes small, and it becomes low noise. Further, in the case where the loss coefficient is small, even if the fan diameter does not become large, the noise can be made small as long as the fan width is made wider. Further, in an air conditioner including a plurality of fans having a narrow fan width, by replacing the fan having a wide fan width, even if the number of fans is reduced, the noise value of the air conditioner at a predetermined operating point can be reduced, and The velocity distribution in the width direction of the heat exchanger can be made nearly uniform. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a perspective perspective view showing the inside of a sirocco fan according to an embodiment of the present invention. 2148-9915-PF 22 201002944 Fig. 2 is a vertical diagram of the overall shape of the fan. Fig. 3 shows the J figure. A schematic portrait of the lower sirocco fan. The section of the under-section structure is shown in Figure 4, which shows the figure of the P-Q special girl of the Siluo fan. Inch and K S - Q characteristics Fig. 5 shows the graph of the west, , & y q $ 〆 π , Lo / H 洛 and loss t of the Loco fan. 々 is the day coefficient f. The diagram of Fig. 6 shows the graph of the y characteristic of the genus sylvestris from the p-Q characteristics and the case of Ksi. Fig. 7 is a graph showing the relationship between the air volume between the blades of the mother-slice blade of the wind and the ^ u ^ ¥ feather and the position of the panel. A schematic cross-sectional view of the longitudinal section structure of the 矣 + h nozzle. Figure 9 is a perspective view of a sirocco fan with a thin t b domain (2).
第1 0圖係表示I 丁…^又差之區域α的部分在壁面上之靜 壓變動的rms值之f祕 . 值气區域α部分的放大圖。 第 11圖係表干亡 有丰又差之區域α:的部分在壁面上之靜 壓變:的值之區域鳴的放大圖。 第 圖係表示西洛可風扇之示意别面構造的縱向剖 面圖。 第1 3圖係透視西洛可風扇而表示的透視立體圖。 第14圖係表示通過動作點β之情況的西洛可風扇之 Ρ — Q特性的圖形。 第15圖係表示裝載西洛可風扇之懸吊式室内機的示 意整體構造之平面圖。Fig. 10 is a view showing the rms value of the static pressure fluctuation of the portion of the area α which is inferior to the area of the difference α. The enlarged view of the α portion of the value gas region. Figure 11 is a magnified view of the area where the value of the area is abruptly and poorly. The figure is a longitudinal cross-sectional view showing the schematic configuration of the sirocco fan. Fig. 13 is a perspective perspective view showing the sirocco fan. Fig. 14 is a graph showing the 特性-Q characteristic of the sirocco fan passing through the operating point β. Fig. 15 is a plan view showing the schematic overall construction of a suspended indoor unit equipped with a sirocco fan.
2148-9915-PF 23 201002944 ·· 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1 7圖係表示在懸吊式室内機之噪音值的表。 磬· 第1 8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、 f ' 2 堝形殼、 2 a吸入口、 2b吹出口、 2bl舌部、 2c風路、 3 鈴嘴、 4 舌部、 5 吸入空間、 、 1 0 0西洛可風扇、 11 0懸吊式室内機、 1 5 0空調裝置、 1 51壓縮機、 152凝結式熱交換器、 153節流裝置、 1 5 4蒸發式熱交換器 2148—9915-PF 242148-9915-PF 23 201002944 ·· 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, f' 2 埚-shaped shell, 2 a suction port, 2b air outlet, 2 bl tongue, 2c wind road, 3 bell mouth, 4 tongue, 5 suction space, 1 0 0 west Rocko fan, 110 floating indoor unit, 150 air conditioner, 1 51 compressor, 152 condensing heat exchanger, 153 throttling device, 1 5 4 evaporative heat exchanger 2148-9915-PF 24
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PCT/JP2008/062442 WO2010004628A1 (en) | 2008-07-10 | 2008-07-10 | Sirocco fan and air conditioner using the same |
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TW201002944A true TW201002944A (en) | 2010-01-16 |
TWI354735B TWI354735B (en) | 2011-12-21 |
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TW097130507A TW201002944A (en) | 2008-07-10 | 2008-08-11 | Sirocco fan and air conditioner using the same |
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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) |
Cited By (1)
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TWI454619B (en) * | 2010-11-12 | 2014-10-01 | Nidec Corp | Air supply fan |
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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 |
CN109247023B (en) * | 2016-05-20 | 2021-01-22 | 三菱电机株式会社 | Centrifugal blower, air conditioner, and refrigeration cycle device |
WO2018225217A1 (en) * | 2017-06-08 | 2018-12-13 | 三菱電機株式会社 | Sirocco fan and air conditioner using same |
CN116075672B (en) * | 2020-08-07 | 2024-02-02 | 大金工业株式会社 | Fan unit and air treatment system comprising same |
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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 |
-
2008
- 2008-07-10 JP JP2010519591A patent/JP4660634B2/en active Active
- 2008-07-10 KR KR1020107023511A patent/KR101045750B1/en active IP Right Grant
- 2008-07-10 CN CN200880129867.XA patent/CN102066771B/en active Active
- 2008-07-10 WO PCT/JP2008/062442 patent/WO2010004628A1/en active Application Filing
- 2008-07-10 EP EP08791016A patent/EP2314880B1/en active Active
- 2008-07-10 ES ES08791016T patent/ES2402790T3/en active Active
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Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
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TWI454619B (en) * | 2010-11-12 | 2014-10-01 | Nidec Corp | Air supply fan |
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CN102066771A (en) | 2011-05-18 |
AU2008359151A1 (en) | 2010-01-14 |
JP4660634B2 (en) | 2011-03-30 |
WO2010004628A1 (en) | 2010-01-14 |
KR101045750B1 (en) | 2011-06-30 |
CN102066771B (en) | 2012-12-12 |
TWI354735B (en) | 2011-12-21 |
AU2008359151B2 (en) | 2011-07-28 |
EP2314880A4 (en) | 2011-08-10 |
EP2314880B1 (en) | 2013-01-09 |
KR20100134684A (en) | 2010-12-23 |
ES2402790T3 (en) | 2013-05-09 |
EP2314880A1 (en) | 2011-04-27 |
JPWO2010004628A1 (en) | 2011-12-22 |
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