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DOI -10.32743/UniTech.2022.105.12.14726
DETERMINATION OF THE MAIN PARAMETERS OF THE ASYNCHRONOUS TRACTION MOTOR OF THE ELECTRIC LOCOMOTIVE OF THE "O'ZBEKISTON" SERIES
Tulagan Nazirkhonov
PhD (Phd), acting Docent, Department of "Electric rolling stock", Tashkent State Transport University, Republic of Uzbekistan, Tashkent E-mail: [email protected]
Dilshod Yuldashev
Master,
Tashkent State Transport University, Republic of Uzbekistan, Tashkent E-mail: yuldawev1998@,gmail. com
ОПРЕДЕЛЕНИЕ ОСНОВНЫХ ПАРАМЕТРОВ АСИНХРОННОГО ТЯГОВОГО ЭЛЕКТРОДВИГАТЕЛЯ ЭЛЕКТРОВОЗА СЕРИИ "O'ZBEKISTON"
Назирхонов Тулаган Мансурхон угли
канд. техн. наук (Phd), и.о. доц. кафедры «Электроподвижной состав»,
Ташкентский государственный транспортный университет,
Республика Узбекистан, г. Ташкент
Йулдашев Дилшод Илхом угли
магистр,
Ташкентский государственный транспортный университет,
Республика Узбекистан, г. Ташкент
ABSTRACT
Target. Determining the parameters of asynchronous traction motors (ATM) is necessary to create a computer simulation model that allows you to reproduce electromagnetic processes in the traction drive and converters, as well as the processing functions of the obtained simulation results, adequate to the real conditions of use on electric rolling stock of converters with various control algorithms in traction and regenerative braking. To determine the parameters of the ATD in relation to the T-shaped equivalent circuit, the idle, short circuit and rated load modes are used using the motor loss separation method. Analytical expressions are obtained for calculating the main parameters of the ATD in relation to the T-shaped equivalent circuit. The main design parameters and electrical quantities are given, The results obtained can be used in a computer simulation model designed to reproduce electromagnetic processes in a traction electric drive and converters, when determining the energy characteristics of an electric locomotive series "O'zbekiston".
АННОТАЦИЯ
Цель. Определение параметров асинхронных тяговых двигателей (АТД) необходимо для создания компьютерной имитационной модели, позволяющей воспроизводить электромагнитные процессы в тяговом электроприводе и преобразователях, а также функции обработки полученных результатов моделирования, адекватные реальным условиям применения на электрическом подвижном составе преобразователей с различными алгоритмами управления в режимах тяги и рекуперативного торможения. Для определения параметров АТД применительно к T - образной схеме замещения используются режимы холостого хода, короткого замыкания и номинальной нагрузки с помощью метода разделения потерь в двигателе. Получены аналитические выражения для расчета основных параметров АТД применительно к T-образной схеме замещения. Приведены основные расчетные параметры и электротехнические величины, характеризующие режимы работы АТД серии 1TB 2KF2624 - 3EA00 электровоза серии «O'zbekiston». Полученные результаты могут быть использованы в компьютерной имитационной модели, предназначенной для воспроизведения электромагнитных процессов в тяговом электроприводе и преобразователях, при определении энергетических характеристик электровоза серии «O'zbekiston».
Библиографическое описание: Nazirkhonov T., Yuldashev D. DETERMINATION OF THE MAIN PARAMETERS OF THE ASYNCHRONOUS TRACTION MOTOR OF THE ELECTRIC LOCOMOTIVE OF THE "O'ZBEKISTON" SERIES // Universum: технические науки : электрон. научн. журн. 2022. 12(105). URL: https://7universum. com/ru/tech/archive/item/14726
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Keywords: asynchronous traction motor, method for calculating parameters, active and inductive resistances of windings, determination of ATD parameters.
Ключевые слова: асинхронный тяговый электродвигатель, метод расчета параметров, активные и индуктивные сопротивления обмоток, определение параметров АТД.
Introduction
Asynchronous electric motors are widely used in the traction drive of rail transport due to their greater reliability and lower manufacturing and operation costs compared to collector motors.
Six-axle AC electric locomotives of the "O'zbekiston" series (Picture. 1) are designed taking into account the latest trends in the field of electric locomotive construction. The characteristic features of an electric locomotive include the use of an asynchronous traction electric drive, traction converters, axis-by-axis regulation of traction and braking force, and a microprocessor control system [6].
Figure 1. electric locomotive "O'zbekiston "
The use of ATD as a traction drive is impossible without a semiconductor converter. In this case, the shape of the voltage and current of the stator winding is far from sinusoidal.
Currently, there is an urgent problem of increasing the energy efficiency of railway transport, which is associated with an increase in the energy performance of electric rolling stock (EPS). An important step in this direction is the creation of a computer simulation model that makes it possible to reproduce electromagnetic processes in the traction electric drive and converters, as well as the functions for processing the obtained simulation results that are adequate to the real conditions for using converters with various control algorithms in traction and regenerative braking modes on the ERS [1-3].
Energy consumption of EPS in operating modes is recorded by measuring instruments - electricity meters.
The components of the consumption and losses of electricity for the movement of ERS can be taken into account only by analytical methods. For an adequate analysis of the energy balance, it is necessary to determine the parameters, as well as the energy performance of the converters and units of the traction electric drive.
The parameters and energy characteristics of traction converters and traction motors have an unambiguous relationship in terms of voltage level, switching frequency of power electronic devices, and current ripples.
Experimental determination of the parameters of the ATD windings in most cases is complicated by the technical conditions for the implementation of test modes. Analytical determination of the ATD parameters - active resistance and leakage inductance of the windings, the magnitude of mechanical losses and losses in the steel can be performed on the basis of no-load and short circuit modes using the loss separation method in the rated load mode [4-7].
The resistance of the stator phase windings in this case is determined by the power loss ^PSMH in copper at rated load, (Ohm)
_ apsm.H rs 3/2. '
(1)
where is the stator phase current in the nominal mode 7sh.
Let's determine the power loss in the copper of the stator at rated load by the formula (W)
PH • 103
A^M.H = —-(1 - (^ + *H)) m
^H (2)
(APMex.H+A^s ct.H + APs AM),
Where sh - rotor slip in the rated load mode, ph - power of the rated mode, - coefficient of performance (efficiency) of the rated mode, APS cth - power of losses in the stator steel in the rated load mode, A^Mex.H - power of mechanical losses in the rated load mode, APS gM - power of additional losses in the stator copper, due to the spatial harmonics of the stator current.
The power of mechanical losses in the rated load mode can be taken as APMexH = 0,002 — • 103 W [6],
^h
the power of additional losses from spatial harmonics of the current APS gM = 0,005 — • 103 W [7].
^H
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The power loss in steel in the rated load mode is almost equal to the power loss in steel for the % rated load mode. The latter can be determined from the condition of equality of the main losses in the steel and copper of the stator at the maximum motor efficiency corresponding to the mode of % of the rated load (Picture. 3), (W)
ДР.
3 ph-IO;
s ст.3/4
4-2 rç,
- (Д^мех.3/4 + Д^дм
(1 - ^max)
(3)
Mechanical losses at the rated rotor speed are practically independent of the load, therefore, with sufficient accuracy, we can assume that APMex3/4 = APMex.H .
The rotor resistance, reduced to the stator phase resistance, can be calculated from the power losses in the rotor at rated slip and reduced rotor current /'rH (ohm):
3/' 2
(4)
Let's find the rotor current, reduced to the stator current, for the rated load mode according to the formula
(A), [6]
^ гн ^sh
1 -
f^so\ _ 4o \LJ L..2L
sh 2 ^H
(5)
Wherein /s0 - no-load current of ATD at rated voltage and rated frequency of the stator current, - multiplicity of the highest electromagnetic torque.
The value is determined by the rated load mode and the inductive resistance of the motor short circuit :
h =
^2н(1 - sh)
h Т3^2с1(Рн^103+АРмех.н)^к
(6)
Where cx - the coefficient of reduction of the parameters of the ATD windings to the r - shaped equivalent circuit
The short-circuit impedance for the stator phase of the ATD is conditioned by the multiplicity of the short-circuit current tf/K3 = 7-8 (ohm) equal to
^к = V*K2 + (CirJ2 =
u.
(7)
Here rK - motor short circuit resistance, rK = rs +r'r. Short circuit inductive reactance can be determined from the formula (Ohm)
= zkv1 -cos2^K3,
(8)
Where incos^K3 - engine power factor for the modeshort circuit, pre-accept cos ^K3 = 0,15 — 0,2. Idle mode current ATD (A) [6-7]
40 ~ 4h ( Sin ^SH
COS фsн 2b..
(9)
where cos - motor power factor for nominal mode.
After performing the calculations according to formulas (1) - (9), the values should be clarified and the refined calculation of the active and inductive resistances of the stator and rotor of the ATD should be
repeated r'r,^K, ^ ~ 1 + —.
220
From the experience of designing ATD with a power of 1-1.3 MW, the ratio of the leakage inductance of the stator phase and the reduced leakage inductance of the rotor phase in relative units is 1: 0.8.
Stator phase leakage inductance , N)
£ __—K
5 a = 1,8-2я-Ген'
(10)
Where - frequency of the stator voltage in the nominal mode.
r r =
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Leakage inductance rotor phase (L'ra, H), reduced to the stator phase is equal to
1-l^fT -
Хк-0.8
1.8-2ÏÏ-/SH
Motor phase impedance at idle (Z0, 0 m)
у _ ^SH ¿n — —
(11)
(12)
The active component of the no-load current of the stator phase, (7s0a ,A)
мех.н
/s0a - vf^H .
Stator phase magnetization current, (7„ ,A)
^д - V^s02 " (
2 'n 2
s0a ■
(13)
(14)
Mutual inductance resistance , Ohm) of the windings of the stator and rotor phases are calculated by the formula
v _ USH v
(15)
In which is the resistance of the - leakage inductance of the stator phase, = .
Mutual inductance of the stator and rotor phase windings, reduced to the stator (LM, H) is
ß 2^/SH
(16)
Based on formulas (10)-(16), the calculation of the main parameters of the ATD "1TB 2KF2624-3EA00" used on "O'zbekiston" electric locomotives. Passport data, design parameters and electrical values characterizing the operating modes of ATD 1TB 2KF2624 - 3EA00, are given in table. 1, and 2 [6-7].
Table 1.
Passport data ATD "1TB 2KF2624 - 3EA00"
Options Designation Meaning
Rated power, kW ^H 1020
Rotation frequency, rpm Пн 1450
Rated line voltage, V ^н 2100
Rated current, A ^SH 344
Power factor at 100% load COS ^SH 0.85
efficiency ^H 0.94
Rated stator current frequency, Hz /SH 50
Number of pole pairs V 2
Rated rotor slip sh 0.015
Table 2.
Design parameters and basic electrical quantities of ATD "1TB 2KF2624 - 3EA00"
Parameters and data Designation Meaning
Power loss in stator copper at rated load, W ЛТ^м.н 28484
Power of mechanical losses in the mode of rated load, W L-XL мех.н 2170
Power of additional losses from spatial current harmonics, W ^S дм 5425
Power loss in steel in % rated load mode, W àPs ст.3/4 12750
Power loss in rotor copper at rated load, W ЛР 20345
Stator phase winding resistance, Ohm 0.079
Rotor resistance reduced to stator phase resistance, Ohm r'r 0.046
Multiplicity of the greatest electromagnetic moment Ьн 1.9
Short circuit impedance, Ohm 2к 0.499
short circuit inductive reactance, Ohm 0.483
Inductive reactance of leakage fluxes of the stator phase, Ohm 0.268
The inductive resistance of the leakage fluxes of the rotor, reduced to the phase of the stator, Ohm 0.214
Stator phase leakage inductance, H 0.00085335
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Parameters and data Designation Meaning
Leakage inductance of the rotor phase, reduced to the stator phase, H Lr(J 0.00068268
Motor phase impedance at idle, Ohm Zo 12.321
The coefficient of reduction of the parameters of the windings to the L-shaped equivalent circuit Cl 1.023
Rotor current reduced to stator current for rated load mode, A I гн 332
Idle mode current, A 4o 98.4
Active component of the no-load current of the stator phase, A 4o a 5.8
Magnetization current of the stator phase, A V 98.2
Inductive resistance of mutual inductance of the windings of the stator and rotor phases, Ohm 12.074
Mutual inductance of the stator and rotor, reduced to the stator (magnetizing inductance), H 0.038
Conclusion
A method is proposed for calculating the parameters of the ATD based on the experiments of idling and short circuit using the method of loss separation in the rated load mode. Analytical expressions for calculating the
parameters and the main characteristic data of ATD are obtained in relation to the t-shaped equivalent circuit. The main design parameters and electrical quantities characterizing the operating modes of the ATD series are given. 1TB 2KF2624-3EA00 electric locomotive of the O'zbekiston series.
Reference:
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