Electri c Machines and Control Vol. 21 No. 7 Jul totally enclosed fan-cool TEFC 55 kw DOI 10.

Similar documents
34 22 f t = f 0 w t + f r t f w θ t = F cos p - ω 0 t - φ 1 2 f r θ t = F cos p - ω 0 t - φ 2 3 p ω 0 F F φ 1 φ 2 t A B s Fig. 1

p = n p ei = n 1. 15k a qb f ei ( ) Gei 1 50 n p W p e - 12 W B e T q B = 1 T f = 50 Hz G e kg a

4 16 SRM J z J z B x B y SRM J. M. Stephenson J. Corda 1 SRM 6 T. J. E. Miller McGilpM Table 1 The basic parameter o

Fig. 1 1 The sketch for forced lead shear damper mm 45 mm 4 mm 200 mm 25 mm 2 mm mm Table 2 The energy dissip

u GW 1-2 x + v y + w z = 0 1 u v w x y z ρuu + ρuv + ρuw = 3-4 x y z x( μ u x ) + y( μ u y ) + z ( μ u ) - p z x 2 ρvu + ρvv + ρ

CARDSM 3 1 CARDSM 1. 1 CARDSM 9 /6 1 CARDSM CARDSM axial coil assisted reluctance doubly salient motor CARDSM CARD

2 ( 自 然 科 学 版 ) 第 20 卷 波 ). 这 种 压 缩 波 空 气 必 然 有 一 部 分 要 绕 流 到 车 身 两 端 的 环 状 空 间 中, 形 成 与 列 车 运 行 方 向 相 反 的 空 气 流 动. 在 列 车 尾 部, 会 产 生 低 于 大 气 压 的 空 气 流

1 2 Z θ. 1 T z = 3 mm (b) 轴向气隙磁密 2 Fig. 2 Air gap flux density when rotor aligns with stator with trapezoidal P

JOURNAL OF EARTHQUAKE ENGINEERING AND ENGINEERING VIBRATION Vol. 31 No. 5 Oct /35 TU3521 P315.

Electri c Machines and Control Vol. 22 No. 11 Nov DOI /j. emc

LaDefense Arch Petronas Towers 2009 CCTV MOMA Newmark Hahn Liu 8 Heredia - Zavoni Barranco 9 Heredia - Zavoni Leyva

u d = R s i d - ωl q i q u q = R s i q + ωl d i d + ωψ 1 u d u q d-q i d i q d q L d L q d q ψ f R s ω i 1 i 5th i th 5 θ 1 θ θ 3 5 5

[1-3] (Smile) [4] 808 nm (CW) W 1 50% 1 W 1 W Fig.1 Thermal design of semiconductor laser vertical stack ; Ansys 20 bar ; bar 2 25 Fig

11 : 1345,,. Feuillebois [6]. Richard Mochel [7]. Tabakova [8],.,..,. Hindmarsh [9],,,,,. Wang [10],, (80 µm),.,. Isao [11]. Ismail Salinas [12],. Kaw

/MPa / kg m - 3 /MPa /MPa 2. 1E ~ 56 ANSYS 6 Hz (a) 一阶垂向弯曲 (b) 一阶侧向弯曲 (c) 一阶扭转 (d) 二阶侧向弯曲 (e) 二阶垂向弯曲 (f) 弯扭组合 2 6 Hz

3 6 permanent magnet synchronous motor LSPMSM G A x( μ ) + A x y( μ ) = - J y s + σ A t 7-8 Γ A = LSPMSM A Γ 2 ν n - ν A 2 n = δ c LSPMSM A J s μ σ v

KUKA W. Polini L. Sorrentino Aized Shirinzadeh 6 7 MF Tech Pitbull Fox Taniq Scorpo Scorpo Compositum Windows KUKA 1 P 1 P 2 KU

P ID,, P ID P ID ; k P ; k I ; k D ; e ( k) k [ 10, 11 ], P ID ; e ( k), 2 e ( k) P ID, e ( k) P ID, P ID P I D, ( k P, k I, k D ), P ID P ID [

标题

Fig. Distribution model of axial magnetic bearing air gap permeance G 6 ~ G 8 G G G ' 7-8 G 3 G 4 G ' 3 G ' 4 G 5 G 6 G 5 G

2 193 EMAT F a λ 1 a λ 1 /2 EMAT 8 9 EMAT H = J C 1 B = μh EMAT E = - B 3 t J = γe F = J B + B S 5 H J C B μ EMAT E EMAT EMAT γ J ANSYS B

Vol. 22 No. 4 JOURNAL OF HARBIN UNIVERSITY OF SCIENCE AND TECHNOLOGY Aug GPS,,, : km, 2. 51, , ; ; ; ; DOI: 10.

#4 ~ #5 12 m m m 1. 5 m # m mm m Z4 Z5

<4D F736F F D20B8DFB9B0B0D3B0D3F5E0D3A6C1A6CAB5B2E2D3EBBCC6CBE3BDE1B9FBB2EED2ECD4ADD2F2B7D6CEF62DD5C5B9FAD0C22E646F6378>

cm /s c d 1 /40 1 /4 1 / / / /m /Hz /kn / kn m ~

mm ~

* CUSUM EWMA PCA TS79 A DOI /j. issn X Incipient Fault Detection in Papermaking Wa

8 : 731 Key words : narrow annular gap ; curvat ure ; critical heat flux ; annular flow,,,,,,,, ( ),, [122 ] kg/ (m 2 s) MPa

85% NCEP CFS 10 CFS CFS BP BP BP ~ 15 d CFS BP r - 1 r CFS 2. 1 CFS 10% 50% 3 d CFS Cli

Fig. 1 Frame calculation model 1 mm Table 1 Joints displacement mm

EL ECTR IC MACH IN ES AND CON TROL Vol113 No11 Jan. 2009,, (, ) :, X 2Y,,,,,,, P ID P ID P ID,, : ; ; ; P ID : TM33 : A : X

ELECTRI C MACHINES AND CONTROL Vol. 16 No. 10 Oct TM 77 A X Electromagnet

f 2 f 2 f q 1 q 1 q 1 q 2 q 1 q n 2 f 2 f 2 f H = q 2 q 1 q 2 q 2 q 2 q n f 2 f 2 f q n q 1 q n q 2 q n q n H R n n n Hessian

4 155 earthquake resilient structure 1 Yahya Kurama 2 Bulent Erkmen 3 Jose Restrepo 4 Brian Smith C40 HRB mm mm 125 mm 2

untitled

Maup re,,,,,, ;,,,,,,,,,, PC 1985 Cognac,, 80, [ 526 ], 420m 160m [ 728 ], PC,,,,,,,,, , [ 3 ] 3008mm, 488mm, 222mm, ( ) 2880mm , 4914, 6

Y m G C I IMC C II IMC R Y = + C I IMC F f G - G^ + - F f G^ C I IMC D + C I IMC F f G - G^ 9 D() R() C IMC() Ⅱ CIMC() U() Ⅰ G() Y() Y m() - G

p 3 p 4 p 5 p 6 p 7 p 8 p 9 p 10 p 11 θ 1 θ 2 θ 3 θ 4 θ 5 θ 6 θ 7 θ 8 θ 9 θ d 1 = 0 X c 0 p 1 p 2 X c 0 d pi p j p i p j 0 δ 90

Electri c Machines and Control Vol. 21 No. 12 Dec :,,,,,,,, 15 kw r /min, : ; ; ; DOI:

[1] Nielsen [2]. Richardson [3] Baldock [4] 0.22 mm 0.32 mm Richardson Zaki. [5-6] mm [7] 1 mm. [8] [9] 5 mm 50 mm [10] [11] [12] -- 40% 50%

Microsoft PowerPoint - Aqua-Sim.pptx

定稿

JOURNAL OF EARTHQUAKE ENGINEERING AND ENGINEERING VIBRATION Vol. 31 No. 6 Dec

附件4

; 3/2, Buck-Boost, 3 Buck-Boost DC-DC ; Y, Fig. 1 1 BBMC The topology of three phase-three phase BBMC 3 BBMC (Study on the control strategy of

ANSYS在高校《材料力学》教学中的应用

一次辽宁暴雨过程的诊断及风场反演分析

11 25 stable state. These conclusions were basically consistent with the analysis results of the multi - stage landslide in loess area with the Monte

g 100mv /g 0. 5 ~ 5kHz 1 YSV8116 DASP 1 N 2. 2 [ M] { x } + [ C] { x } + [ K]{ x } = { f t } 1 M C K 3 M C K f t x t 1 [ H( ω )] = - ω 2

Ansys /4 Ansys % 9 60% MU10 M m 1 Fig. Actual situation of measured building 1 Fig. 1 First floor plan of typical r

Microsoft Word - 刘 慧 板.doc

1, : FLUENT 81 CA4113Z,,,,.,,. [ ] : :, 9 9t (<) + div (u<) = div ( < grad<) + S < (1) t, u, <, <, < S <,, 1., u i i, E,. k - RNG, () (3) [ 3-4 ],. 5

by industrial structure evolution from 1952 to 2007 and its influence effect was first acceleration and then deceleration second the effects of indust


% GIS / / Fig. 1 Characteristics of flood disaster variation in suburbs of Shang

VLBI2010 [2] 1 mm EOP VLBI VLBI [3 5] VLBI h [6 11] VLBI VLBI VLBI VLBI VLBI GPS GPS ( ) [12] VLBI 10 m VLBI 65 m [13,14] (referen

km km mm km m /s hpa 500 hpa E N 41 N 37 N 121

m m m ~ mm

Microsoft Word tb 赵宏宇s-高校教改纵横.doc

H 2 SO ml ml 1. 0 ml C 4. 0 ml - 30 min 490 nm 0 ~ 100 μg /ml Zhao = VρN 100% 1 m V ml ρ g

1602 CHEMICAL INDUSTRY AND ENGINEERING PROGRESS TQ A Prospect of the structure of oxygen generating

θ 1 = φ n -n 2 2 n AR n φ i = 0 1 = a t - θ θ m a t-m 3 3 m MA m 1. 2 ρ k = R k /R 0 5 Akaike ρ k 1 AIC = n ln δ 2

T K mm mm Q345B 600 mm 200 mm 50 mm 600 mm 300 mm 50 mm 2 K ~ 0. 3 mm 13 ~ 15 mm Q345B 25

1.0 % 0.25 % 85μm % U416 Sulfate expansion deformation law and mechanism of cement stabilized macadam base of saline areas in Xinjiang Song

doc

Mnq 1 1 m ANSYS BEAM44 E0 E18 E0' Y Z E18' X Y Z ANSYS C64K C70C70H C /t /t /t /mm /mm /mm C64K

[1] Liu Hongwei,2013, Study on Comprehensive Evaluation of Iron and Steel Enterprises Production System s Basic Capacities, International Asia Confere

( permanent magnet linear synchronous motor, PMLSM ), [ 1-3 ] PMLSM,, PMLSM PMLSM,, SPWM : 2 Hz; 018; 017 khz; JUNG Insoung [ 4 ] V PM

(L d L q ). i d = 0,, [8].,,,,, / (maximum torque per ampere, MTPA) [9],. MTPA [9] [10],,,. MTPA, MTPA.,,,. MTPA,,,.,. 2 (Model of PMSM) d-q, :

Technical Acoustics Vol.27, No.4 Aug., 2008,,, (, ) :,,,,,, : ; ; : TB535;U : A : (2008) Noise and vibr

通 过 厂 变 带 电, 这 种 设 计 减 少 了 机 组 自 带 厂 用 电 负 荷 能 力, 降 低 了 锅 炉 满 足 FCB 时 最 低 稳 燃 工 况, 同 时 造 成 燃 烧 调 整 量 加 大 本 电 厂 在 FCB 试 验 时, 电 泵 不 联 启, 始 终 保 持 汽 泵 运 行

标题

718 30,. [8],,,,,,. PMSM, (q ) (d ).,,,,. 2 IPMSM (Mathematical model of IPMSM and analysis of the flux-weakening control operation) 2.1 IPMSM (Mathem

(1) ( 1965 ),, 1952 [9] 2.1 (2) 1 53 (E i ), 2 (P i ) (G E (G P, 31 (Q i ) 3, : G E (x,y)= (E i Q(x i, y i )) E i G P (x,y)=

实 践 探 讨 高 丽 : 从 少 数 民 族 大 学 生 的 阅 读 需 求 看 民 族 院 校 图 书 馆 的 资 源 建 设 有 区 域 性 和 民 族 性 很 强 的 传 统 学 科 特 色 学 科 及 优 势 学 科, 因 此 图 书 馆 的 资 源 建 设 也 要 顺 应 这 一 特 性

12-1b T Q235B ML15 Ca OH Table 1 Chemical composition of specimens % C Si Mn S P Cr Ni Fe

13-15 Lagrange 3. 1 h t + hu + hv = 0 1 x y hu + t x hu gh 2 ( ) + y huv = - gh z 0 ( + x u u 2 2 槡 + v + W C ) 2 x + fhv + z h x 2hv u ( t x )

T e = K 1 Φ m I 2 cosθ K 1 Φ m I cosθ 2 1 T 12 e Φ / 13 m I 4 2 Φ m Φ m 14 I 2 Φ m I 2 15 dq0 T e = K 2 ΦI a 2 16

~ a 3 h NCEP ~ 24 3 ~ ~ 8 9 ~ km m ~ 500 m 500 ~ 800 m 800 ~ m a 200

0 1 / m m 2 ~ 3. 9m 3. 2m 1 / m 23. 6m mm 3 300mm 32. 1% 38. 1% 250mm C60 ~ C50 ~ C40 C

第二部分

System Design and Setup of a Robot to Pass over Steps Abstract In the research, one special type of robots that can pass over steps is designed and se

标题

Microsoft Word 任 辉_new_.doc

1 引言

微软用户

Thesis for the Master degree in Engineering Research on Negative Pressure Wave Simulation and Signal Processing of Fluid-Conveying Pipeline Leak Candi

CFDesign 2 1 CFDesign CFDesign CAD ~ r /min mm 1

m m m

2 3. 1,,,.,., CAD,,,. : 1) :, 1,,. ; 2) :,, ; 3) :,; 4) : Fig. 1 Flowchart of generation and application of 3D2digital2building 2 :.. 3 : 1) :,

第 1 期 常 壮 等 : 基 于 RS-485 总 线 的 舰 船 损 管 训 练 平 台 控 系 统 研 究 87 能 : 1) 损 管 基 本 理 论 的 学 习 帮 助 舰 员 熟 悉 舰 艇 舱 室 相 关 规 章 制 度 损 管 施 分 布 和 使 用 不 沉 性 文 件 等 ) 损 管

~ 4 mm h 8 60 min 1 10 min N min 8. 7% min 2 9 Tab. 1 1 Test result of modified

TI 3 TI TABLE 4 RANDBIN Research of Modern Basic Education

Microsoft PowerPoint - TOHO Dust core and material.ppt

mm 5 1 Tab 1 Chemical composition of PSB830 finishing rolled rebars % C Si Mn P S V 0 38 ~ 1 50 ~ 0 80 ~ ~


Microsoft Word - 专论综述1.doc

2009 年第 54 卷第 12 期 : 1779 ~ csb.scichina.com SCIENCE IN CHINA PRESS,,, ;, , 200

基于因子分析法对沪深农业类上市公司财务绩效实证分析

5 551 [3-].. [5]. [6]. [7].. API API. 1 [8-9]. [1]. W = W 1) y). x [11-12] D 2 2πR = 2z E + 2R arcsin D δ R z E = πr 1 + πr ) 2 arcsin

Transcription:

21 7 2017 7 Electri c Machines and Control Vol. 21 No. 7 Jul. 2017 1 2 1 3 1. 200031 2. 210000 3. 150080 totally enclosed fan-cool TEFC 55 kw DOI 10. 15938 /j. emc. 2017. 07. 012 TM 15 A 1007-449X 2017 07-0087- 07 Calculation of 3D whole domain steady temperature fields for TEFC motor FENG Hai-jun 1 DING Shu-ye 2 ZHOU Pu 1 LI Guan-nan 3 1. No. 704 Research Institute of CSIC Shanghai 200031 China 2. Nari School of Electrical and Automation Nanjing Normal Univerisity Nanjing 210000 China 3. College of Electrical and Electronic Engineering Harbin University of Science and Technology Harbin 150080 China Abstract In order to research the temperature field of the TEFC induction motor under rated load conditions a 55 kw asynchronous motor was taken as an example. The motor real structure was simplified using equivalent method and the equivalent model of the actual windings was established by the method of insulation equivalent. Based on the basic law of heat conduction and steady-state heat conduction equation the simulation model of the temperature field was established and the steady temperature field was calculated with finite-element method. The problem of rotor rotation and air flow in motor was solved by using the concept of equivalent coefficient of heat conductivity. Temperature distribution characteristics of the motor was obtained. Temperature field of different positions of the stator core was studied in detail. The temperature distribution inside the rotor was analyzed and temperature rise of single winding and the windings a- long the circumferential direction was also numerically analyzed. At last the experimental test was carried out on the prototype comparing the calculated results with the experimental value and accuracy of the calculation method was verified. 2017-03 - 02 2016RAXXJ026 1254 - NCET006 1982 1978 1982 1988

88 21 Keywords totally enclosed fan-cool induction motor 3D temperature field finite elements method numerical analysis loss characteristic 0 1. 2 TEFC 1 14 TEFC 1-11 1 Fig. 1 Structural schematic of electrical machine 2 2 a 2 b 856. 4 Y2-250M - 4 55 kw 1 1. 1 2 Fig. 2 Physical model and interior 12-13 1. 3 x λ T x x + y λ T y y + z λ T z = - q } z - λ T n = α T - T f T λ x λ y λ z q 1 α T f x y z 3 n 15 λ eff λ eff

7 89 1 Table 1 Heat flux density of each part Re = uδ γ 2 u δ γ R i Re er = 41. 2 槡 δ 3 506 182. 5 Re > Re er 2. 1 λ eff = 0. 001 9 η -2. 908 4 Re 0. 4614ln 3. 333 61η 3 4 η = r 0 /R i R i r 0 λ eq = n δ i / n δ i /λ i 5 i = 1 i = 1 λ eq δ i i = 1 2 3 n λ i 1. 4 α 16 α = 9. 37 + 14v 0. 62 v 6 17 / W /m 3 39 582. 853 218 884. 526 452 272. 375 236. 918 80 998. 64 α 1 = 20 + 14. 3u 0. 6 0 7 3 α 2 = 20 + 2. 6u 0. 6 Fig. 3 Temperature rise of motor casing 0 8 u 0 4 2 1

90 21 2. 2 5 62 K 58 K a b c AB 66 K BC CD 62 K DE 61 K 57 K 5 0. 9 mm 86 K 1 /4 76 K 63 K 3 Fig. 6 6 Temperature change of tooth top in axial length Fig. 4 4 Temperature rise inside of the motor 7 Fig. 5 5 Temperature change in the middle of the axial along radial direction 6 a b c 7 Fig. 7 7 Temperature change of windings along the circumferential direction

7 91 5 K 18 K 85 K 4 K π /2 3π /4 1 /2 8 8 9 9 Fig. 9 Temperature rise distribution of the single winding 10 104 K 120. 9 K 8 Fig. 8 Schematic diagram of temperature rise distribution and extraction path 9 11 K 2 K 8 K 4 K 3 8. 5 11

92 21-0. 5 K - 0. 6% PT100 Fig. 12 12 Embedding location of the sensor Fig. 10 10 Temperature rise distribution of rotor section 11 Fig. 11 Experimental test platform 13 Fig. 13 Contrast of measured temperature and calculated temperature 12 15 15 4 U D G 1 20 K 13 2 17 K 15 10 5 K 1 5. 8 K 3 6. 5% 9 3. 6 K 7 0. 3 5 4-2. 8 K - 3%

7 93 2 K 1 GNACINSKI P PEPLINSKI M SZWEDA M. The effect of subharmonics on induction machine heating C / /13th International Power Electronics and Motion Control Conference September 1-3 2008 Poznań Poland. 2008 826-829. 2 VONG P K RODGER D. Coupled electromagnetic thermal modeling of electrical machines J. IEEE Transactions on Magnetics 2003 39 3 1614. 3 XYPTERAS J HATZIATHANASSIOU V. Thermal analysis of an electrical machine taking into account the iron losses and the deepbar effect J. IEEE Transactions on Energy Conversion 1999 14 4 996. J. Proceedings of the CSEE 2012 32 3 137. 4. 12 BOGLIETTI A CAVAGNINO A LAZARRI M et al. A simplified J. 2015 20 5 1. DING Shuye GUAN Tianyu CUI Guanghui. The research on temperature field of asynchronous motor for ship drive J. Journal of Harbin University of Science and Technology 2015 20 5 1. 5 BASTOS J P CABREIRA M F R R. A thermal analysis of induction motors using a weak coupled modeling J. IEEE Transactions on Magnetics 1997 3 2 1714. 6 STATON D BOGLIETTI A CAVAGNINO A. Solving the more difficult aspects of electric motor thermal analysis in small and medium size industrial induction motors J. IEEE Transactions on Energy Conversion 2005 20 3 620. 7. J. 2016 20 1 52. KONG Han LIU Jinglin. Study of rotor eccentricity effect on permanent magnet servo motor performance J. Electric Machines and Control 2016 20 1 52-59. 8. 16. M. J. 2012 32 24 74. DING Shuye GE Yunzhong SUN Zhaoqiong et al. Numerical research on temperature and fluid field for high-altitude wind power generator J. Proceedings of the CSEE 2012 32 24 74. 9. J. 2016 21 4 59. LU Yiping LI Huilan HAN Jiade et al. Three dimensional flow field numerical simulation for some axial ventilation brushless exciter J. Journal of Harbin University of Science and Technology 2016 21 4 59. 10. J. 2012 16 3 83. DING Shuye GE Yunzhong CHEN Weijie et al. Coupling calculation and analysis of three-dimensional temperature field for doubly-fed wind generator J. Electric Machines and Control 2012 16 3 83. 11. 3 MW J. 2012 32 3 137. DING Shuye SUN Zhaoqiong XU Dianguo et al. Numerical investigation of heat transfer for 3MW doubly-fed wind generator thermal model for variable-speed self-cooled induction motor J. IEEE Transactions on Industry Applications 2003 39 4 945. 13 BOGLIETTI A CAVAGNINO A STATON D. TEFC induction motors thermal models a parameter sensitivity analysis J. IEEE Transactions on Industry Applications 2005 41 3 756. 14. J. 2015 51 14 152. CHEN Weijie DING Shuye MIAO Lijie. Research on temperature field non-uniformly distributive heat source coupled investigation of ventilator-driving motor J. Journal of Mechanical Engineering 2015 51 14 152. 15 YABIKU R FIALHO R TERAN L et al. Use of thermal network on determining the temperature distribution inside electric motors in steady-state and dynamic conditions J. IEEE Transactions on Industry Applications 2010 46 5 1787. 2007 377-389. 17. M. 1998 1-12.