Identification of a 7-phase claw-pole starter-alternator for a micro-hybrid automotive application Antoine Bruyère, Thomas Henneron, Eric Semail, Fabrice Locment, Alain Bouscayrol, J.M Dubus„ Jean-Claude Mipo
To cite this version:
Antoine Bruyère, Thomas Henneron, Eric Semail, Fabrice Locment, Alain Bouscayrol, et al.. Iden- tification of a 7-phase claw-pole starter-alternator for a micro-hybrid automotive application. Inter- national Congress on Electrical Machines, Sep 2008, Vilamoura, Portugal. pp.1-6, 10.1109/ICEL- MACH.2008.4800046. hal-01107781
HAL Id: hal-01107781 https://hal.archives-ouvertes.fr/hal-01107781 Submitted on 3 Feb 2015
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This is an author-deposited version published in: http://sam.ensam.eu Handle ID: .http://hdl.handle.net/10985/9255
To cite this version : Antoine BRUYÈRE, Thomas HENNERON, Fabrice LOCMENT, Eric SEMAIL, Alain BOUSCAYROL, Jean-Marc DUBUS, Jean-Claude MIPO - Identification of a 7-phase claw-pole starter-alternator for a micro-hybrid automotive application - In: International Congress on Electrical Machines, Portugal, 2008-09-06 - International Congress on Electrical Machines - 2008
Any correspondence concerning this service should be sent to the repository Administrator : [email protected] Identification of a 7-phase claw-pole starter-alternator for a micro-hybrid automotive application
A. Bruyère1,2, T. Henneron1, E. Semail1, F. Locment1 A. Bouscayrol1, J.M. Dubus2, J.C. Mipo2
1Laboratoire d’Electrotechnique et d’Electronique de Puissance de Lille (L2EP), 2Valeo Electrical System, Arts et Métiers ParisTech, 8, boulevard Louis XIV, 2, rue André Boulle, BP 150, 59046 Lille, FRANCE 94017 Créteil Cedex, FRANCE Tel. +33 (0)3-20-62-15-61, Tel. +33 (0)1-48-98-84-37 Fax. +33 (0)3-20-62-27-50 Email: [email protected] Email: [email protected]
Abstract- This paper deals with the identification of a new high to develop the torque during the short duration of the start. In power starter-alternator system, using both: a Finite Element section II, the predeterminations obtained by a Finite Element Method (FEM) modeling and an experimental vector control. The drive is composed of a synchronous 7-phase claw-pole machine Method (FEM) modeling are compared with experimental supplied with a low voltage / high current Voltage Source Inverter results for the electromotive forces and for the torque per (VSI). This structure needs specific approaches to plan its Ampere. electrical and mechanical behaviors and to identify the In section III, resistive and inductive parameters of the parameters needed for control purpose. At first, a Finite Element whole drive are determined. These parameters are needed for Method (FEM) modeling of the machine is presented. It is used for the predetermination of the electromotive forces and of the controlling the starter-alternator, in its both functioning modes: torque. Experimental results are in good accordance with in motor mode (for the ICE start) and in alternator mode. As numerical results. In a second part, resistive and inductive the voltage is low (12V), the resistive and inductive electrical parameters of the drive are determined by an original parameter values of the battery and VSI are not negligible in experimental approach that takes into account each component of comparison with those of the machine. At first, results obtained the drive: the battery, the VSI and the machine. with classical determination approach are given and discussed. Secondly, an experimental approach based on an elementary I. INTRODUCTION vector control of the machine is developed to find directly the Claw-pole synchronous machines with separate excitation six characteristic time constants needed for controlling the are commonly used to achieve the alternator function in seven-phase drive. Automotive. This is due to their low cost and their ability to II. DETERMINATION OF EMF AND TORQUE BY FINITE work in a very large speed range. With the studied belt driven ELEMENT METHOD starter-alternator system [1], starting the car Internal Combustion Engine (ICE) is made with this claw-pole This kind of claw-pole structure is known to be sensitive to machine. This kind of system is used to bring the micro-hybrid modeling with a numerical method as FEM [4] because of their Stop-Start function, without major modifications of the car 3D characteristics, a thin airgap (about 0.3% of the external powertrain. The new needed starter function adds a new diameter) and highly saturated magnetic materials. Moreover, constraint on the electrical machine: the ability to develop a the studied machine is a synchronous 7-phase claw pole large torque during the start. Starter-alternators already equip machine with permanent magnets between the claws. Sixteen small cars, with a small 1.4 ICE. The major interest of this poles and a number of slots per pole and per phase equal to simple system concerns the limited extra cost for the final car 0.25 imply a modelling of a quarter of the structure at least [1], when the hybridization operation is achieved. (Fig. 2). The aim of the modeling is not only to plan the To take up this challenge for powerful Internal Combustion voltage output, in generator mode, but also to determine the Engine (ICE) without changing the classical (12 Volts) DC- maximum available torque in motor mode, during the start of Bus voltage level [1], a new claw-pole starter-alternator with the car ICE. The first step in order to validate the 3D-modeling seven phases and permanent magnets between the claws has is to compare the experimental electromotive forces (emf) with been developed [2]-[3] (Fig. 1). The obtained torque density the calculated ones. The second step is to obtain, for a defined (Nm/m3) allows keeping the economical benefits of using a 12- repartition of the currents among the phases, the maximum Volts battery [1]. possible torque. In order to carry out the starter function, a modeling of the The thin airgap leads to a mesh composed of 380000 machine is at first necessary to plan the ability of the machine tetrahedral elements, the air-gap being meshed with two layers
of elements. The resolution is made using the magnetostatic stator (3/4), assumption and the scalar potential formulation, with with concentrated windings CARMEL, a software developed at the L2EP. Fig.2 gives rotor front claw-pole wheel results of the numerical simulation, related to the magnetic flux permanent magnets density B under no load condition and a 5A current IF (between the claws) supplying the excitation coil. The highest flux density values (in yellow) are obtained under the stator teeth. Fig. 3 compares the electromotive force waveform named e(t), calculated under no load condition, at a rotation speed N = 1800rpm and IF = 5A, with an experimental measurement in the same conditions. These results validate the numerical model good accuracy, at the first order, for the determination of the voltage outputs. Fig. 4 gives the calculated torque T as function of the rotor excitation coil position θ, when the machine currents are imposed to be the rotor rear claw-pole wheel same as in an experimental test (Square Wave Voltage supply), for which the torque is maximized. The maximal numerical Fig.1. Exploded view of the multiphase claw pole starter-alternator torque value is Tcalculated = 62.4 Nm, to be compared with the experimental maximum measured torque: Tmeasured = 66.5 Nm, that shows a difference of about 6 %. For the determination of the inductive parameters, numerical FEM leads to too large durations of computation in the present case. It is due to the 3D characteristics of the machine and its thin air-gap (which implies a high number of 380000 elements). Moreover, the magnetic materials being highly saturated for this application, the simulation has to take into account the non-linear characteristics of the materials. In Fig. 5, the magnetic flux density is represented for a 2D slice of the whole structure (rotor and stator); z-coordinate of the slice is at the middle of the structure. This figure points out the magnetic saturation areas under no load conditions, with iF = 5 A. These Permanent saturated areas evolve with the rotor position and the currents magnet
(excitation coil current iF, and stator windings currents). They Fig. 2. Rotor magnetic flux density B under no-load condition with iF=5A are at the origin of variable magnetic air-gap effects. As consequence, the inductances depend on the rotor position and 15 on the currents. Finite Element modeling to calculate the 10 inductive parameters for every rotor position, and for every 5 supplying situation, would lead to huge computation and analysis times. 0 0,002 0,0025 0,003 0,0035 0,004 0,0045 0,005 0,0055 0,006 0,0065
As consequence, experimental methods have been developed -5 for the determination of the machine inductive parameters. (V) voltage EMF -10 experimental measurement Numerical calculation -15
Fig. 3. Electromotive force under no load condition; N=1800rpm, IF = 5A and comparison with an experimental measurement 80 60 40 20 0 0 50 100 150 200 250 300 350 -20
Torque (Nm) -40 Numercal calculated torque -60 Experimental maximal torque reference value -80 Fig. 4. Calculated torque as function of the position θ and comparison with an experimental maximal torque reference value with [Flux] the seven-dimensional vector of flux linked by the seven stator phases, [Is] the associated current vector and [LSS] the 7X7 stator inductance matrix. Several assumptions are made. At first, the magnetic characteristic of the materials is considered to be linear. Secondly, whereas for a seven-phase machine the [LSS] stator inductance matrix contains 49 values, only 7 different values, one self inductance and six mutual inductances, are considered taking into account standard assumptions of regularity, symmetry and circularity properties for this matrix. These seven inductances lead to six cyclic inductances and one homopolar inductance (or zero-sequence inductance). This last one is omitted since a wye-coupling of the machine implies that the homopolar inductance has no impact on the control. Fig. 5. Magnetic flux density repartition at the middle of the machine The procedure of measurement is the following for different under no load condition and iF=5A values of the rotor position, which is imposed and kept constant by a motion controller: III. INDUCTIVE AND RESISTIVE PARAMETERS IDENTIFICATION a magnetic state is imposed by a choice of a value BY EXPERIMENTAL VECTOR CONTROL for the excitation current iF; sinusoidal current at chosen frequency is imposed In order to control the drive during transient operations, such in phase n°1 by using a VSI with a control of the as starts, the electrical time constants are relevant parameters currents; since they imply the choice of the carrier frequency of the voltage is measured across each phase successively; Pulse Width Modulation (PWM) for the Voltage Source measured voltage is integrated. Flux and Inverter (VSI). For a wye-connected three-phase machine with corresponding inductance are then deduced using reluctance effects, only two time constants are sufficient to (1). characterize the drive. As the resistance is the same in the two The following measurements are made for several fixed axis, the various values of the time constants are directly positions. Then, Table 1 gives average values of inductances. associated with those of the cyclic inductances. In comparison Considering average values is in accordance with the with conventional methods [5], more recent methods have been circularity assumption used for this first method. presented using current controls, either in the stator frame [6], Practically, it has been chosen a 120 Hz frequency with a 17 or in the dq-reference frame [7]-[9]: determination of the A RMS sinusoidal current, around a constant 18 A current. cyclic inductances L and L can be thus obtained either d q Table I gives the average values (in µH) versus for two indirectly or directly. values of excitation currents. For a 7-phase machine, three different dq-reference frames, or “subspaces S1, S2 and S3”, can be determined. TABLE I INDUCTANCES VALUES (µH) IN THE STATOR FRAME Consequently, six time constants can be then evaluated, depending on the importance of the reluctance effects. These
L0 0 0 0 0 0 0 approach it is possible to determine directly the cyclic 0 L 1dS 0 0 0 0 0 inductances in conditions closed to the working ones. 00 L 1qS 0 0 0 0 (2) B. Direct determination of time constants in dq-frames 00 0 L 2dS 0 0 0 00 0 0 L 0 0 In the studied case, since the values of resistances and 2qS 00 0 0 0 L 3dS 0 inductances are very low, it is then preferable to consider a 00 0 0 0 0 L 3qS direct method of identification that takes into account 1 C LSS )( C implicitly the complete drive and gives directly the time constants [10]. The experimental method is based on an TABLE II CYCLIC INDUCTANCE VALUES (µH) elementary vector control for a seven-phase machine. The control is a generalization of classical vector control in dq- I
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A1: SEVEN-DIMENSIONAL CONCORDIA TRANSFORMATION MATRIX:
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A2: EXPERIMENTAL SET-UP DESCRIPTION:
(a) (b) (c) (a): Seven-phase starter-alternator (rear of the picture) mechanically connected to a brushless synchronous machine (front of the picture) (b): Seven-leg Voltage Source Inverter (c): Programmable Electrical source and load