Engineering » Vehicle Engineering » "Electric Vehicles - Modelling and Simulations", book edited by Seref Soylu, ISBN 978-953-307-477-1, Published: September 12, 2011 under CC BY-NC-SA 3.0 license

Chapter 8

Global Design and Optimization of a Permanent Magnet Synchronous Machine Used for Light Electric Vehicle

By Daniel Fodorean
DOI: 10.5772/17741

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Overview

The PM and steel characteristics used as the active part’s materials of the PMSM.
Figure 1. The PM and steel characteristics used as the active part’s materials of the PMSM.
The PMSM: (a) geometry; (b) fractioned type winding configuration; (c) the resultant voltage vectors.
Figure 2. The PMSM: (a) geometry; (b) fractioned type winding configuration; (c) the resultant voltage vectors.
Phasor diagram for PMSM in motor-load conditions.
Figure 3. Phasor diagram for PMSM in motor-load conditions.
The d (a) and q (b) axis equivalent circuits.
Figure 4. The d (a) and q (b) axis equivalent circuits.
Simplified basic scheme of the implemented FOC technique.
Figure 5. Simplified basic scheme of the implemented FOC technique.
Simplified basic scheme of the implemented DTC technique.
Figure 6. Simplified basic scheme of the implemented DTC technique.
PMSM simulation results: (a) electrical performances; (b) mechanical performances.
Figure 7. PMSM simulation results: (a) electrical performances; (b) mechanical performances.
PMSM simulation results: energetic performances.
Figure 8. PMSM simulation results: energetic performances.
Flux-density and field lines for studied PMSM.
Figure 9. Flux-density and field lines for studied PMSM.
FEM results of PMSM in motor regime.
Figure 10. FEM results of PMSM in motor regime.
Optimization results of PMSM: source current and mechanical performances constraints.
Figure 11. Optimization results of PMSM: source current and mechanical performances constraints.
Optimization results of PMSM: evolution of geometrical and energetic parameters.
Figure 12. Optimization results of PMSM: evolution of geometrical and energetic parameters.
Optimization results of PMSM: power density and mass improvement.
Figure 13. Optimization results of PMSM: power density and mass improvement.

Global Design and Optimization of a Permanent Magnet Synchronous Machine Used for Light Electric Vehicle

Daniel Fodorean1

1. Introduction

One of the most commonproblems of modern society, these days, particularly for industrialized countries, is the pollution (Fuhs, 2009;Ehsani et al., 2005; Vogel,2009; Ceraolo et al., 2006; Chenh-Hu& Ming-Yang, 2007; Naidu et al., 2005). According to several studies, the largest share of pollution from urban areas comes from vehicle emissions and because of this explosive growth of the number of cars. The pollution effect is more and more obvious, especially in large cities. Consequently, finding a solution to reduce (or eliminate) the pollution is a vital need. If in public transports (trains, buses and trams) were found non-polluted solutions (electrical ones), for the individual transport the present solutions can not yet meet the current need in autonomy. Even though historically the electric vehicle precedes the thermal engine, the power/fuel-consumption ratio and the reduced time to refill the tank has made the car powered by diesel or gasoline the ideal candidate for private transport. Although lately there were some rumors regarding the depletion of fossil resources, according to recent studies, America's oil availability is assured for the next 500 years (Fuhs, 2009; Ehsani et al., 2005). So, the need of breathing clean air remains the main argument forusing electric vehicles (EV). However, all over the world, one of the current research topics concerns the use of renewable energy sources and EVs.

With regard to automobiles, there have been made several attempts to establish a maximum acceptable level of pollution. Thus, several car manufacturers have prepared a declaration of Partnership for a New Generation of Vehicles (PNGV), also called SUPERCAR. This concept provides, for a certain power, the expected performance of a thermal or hybrid car. Virtually, every car manufacturer proposes its own version of electric or hybrid car, at SUPERCAR standard, see Table 1(Fuhs, 2009).

Of course, at concept level, the investment is not a criterion for the construction of EVs, as in the case of series manufacturing (where profits are severely quantified). For example, nowadays the price of 1 kW of power provided by fuel cell (FC) is around 4,500 €; thus, a FC of 100 kW would cost 450,000 € (those costs are practically prohibitive, for series manufacturing).

By consulting Table 1, it can be noticed the interest of all car manufacturers to get a reduced pollution, with highest autonomy. Nowadays, the hybrid vehicles can be seen on streets. Although the cost of a hybrid car is not much higher than for the classical engine (about 15-25% higher), however, the first one requires supplementary maintenance costs which cannot be quantified in this moment.

Concept CarsTechnical DataPerformances
Audi metroproject quattroturbocharged four-cylinder engine and an electric machine of 30 kW; lithium-ion batterymaximum range on electric-only of 100 km; 0-100 km/h in 7.8 s; maximum speed 200 km/h
BMW x5 hybrid SUVfor 1000 rpm, there is a V-8 engine providing 1000 Nm; the electric motor gives 660 Nmfuel economy is improved by an estimated 20%.
Chrysler eco voyager FCVpropulsion of 200 kW; hydrogen is feed to a PEM fuel cell (FC)range of 482 km and a 0–60 km/h in less than 8 s.
Citroën c-cactus hybriddiesel engine provides 52 kW and the electric motor gives 22 kWfuel consumption is 2.0 L/100 km; maximum speed is 150 km/h
Ford hySeries edgeLi-ion battery has maximum power of 130 kW, and the FC provides 35 kWrange of 363 km (limited by the amount of hydrogen for the FC)
Honda FCXelectric vehicle with 80 kW propulsion engine, combining ultracapacitors (UC) and PEM FC55% for overall efficiency, driving range of 430 km
Hyundai I-blue FCVFC stack produces 100 kW; there is a 100 kW electric machine (front wheels) and 20 kW motor for each rear wheelestimated range is 600 km
Jeep renegade diesel–electric1.5 L diesel engine provides 86 kW and is teamed with 4 electric motors (4WD) of 85 kW combined powerthe diesel provides range extension up to 645 km beyond the 64 km electric-only range (diesel fuel tank holds 38 L)
Kia FCVa 100 kW FC suppliss a 100 kW front wheel electric motor, while the motor driving the rear wheels is 20 kWrange is stated to be 610 km
Mercedesbenz s-class direct hybrid3.5 L (V-6) gasoline engine with motor/generator combined power of 225 kW and combined torque of 388 Nmacceleration time from 0-100 km/h in 7.5 s
Mitsubishi pure EVLi-ion battery and wheel-in-motors of 20 kW150 kg Li-ion battery give a range of 150 km (2010 prospective range of 250 km
Opel flextremea series hybrid configuration (with diesel engine) with Li-ion battery; the electric motor has peak power of 120 kWfuel consumption of 1.5 L/100 km; electric only mode has range of 55 km
Peugeot 307 hybridit is diesel/electric hybrid automobilethe estimated fuel economy is 82 mpg; this is a hybrid that matches the PNGV goals
Subaru G4Efive passengers EV, using Li-ion batteriesdriving range is 200 km; the battery can be fully charged at home in 8 h (an 80% charge is possible in 15 min)
Toyota 1/X plug-in hybridthermal engine 0.5 L, with a huge reduction of mass to 420 kg (use of carbon fiber composites, although expensive)low mass also means low engine power and fuel consumption
Volkswagen Blue FCa 12 kW FC mounted in the front charges 12 Li-ion batteries at the rear; The 40 kW motor is located at the rearthe electric-only range is 108 km; top speed is 125 km/h, and the acceleration time from 0-100 km/h is 13.7 s
Volvo rechargeseries hybrid with lithium polymer batteries; the engine is of 4-cylinder type with1.6 L; it has 4 electric wheels motors (AWD)electric-only range is 100 km; for a 150 km trip, the fuel economy is 1.4 L/100 km

Table 1.

Several types of hybrid vehicle concepts.

Some predictions on the EV’s were considered by (Fuhs, 2009). In the nearest future the thermal automobiles number will decrease, while the hybrid ones are taking their place. By 2037 the fully electric vehicle (called kit car) will replace the engine and then, after a fuzzy period all vehicles will be powered based on clean energy sources, when a new philosophy of building and using the cars will be put in place.

So, one of the challenges of individual transport refers to finding clean solutions, with enhanced autonomy (Ceraolo et al., 2006; Chenh-Hu& Ming-Yang, 2007; Naidu et al., 2005). This is the motivation of this research work. For that, an electric scooter will be studied from the motorization, supplying and control point of view. The global steps of the design process will be presented here. Firstly, the considered load and expected mechanical performances will be introduced. The electromagnetic design of the electrical motor, capable to fulfill the mechanical performances, will be presented too. The obtained analytical performances should be validated; for that, the finite element method will be used. Also, the machine optimization will fulfill the global designing process of the electrical machine.

2. Design of studied electrical machine

The research study presented here concerns the design of a three phase permanent magnet synchronous machine (PMSM) used for the propulsion of an electric scooter. It is widely recognized that the common solution, the dc motor, has usually poor performances against ac motor. However, for low small power electrical machines, this advantage is not always obvious. Also, a special attention should be paid for the efficiency and power factor of ac machines. This will be analyzed here. The validation of the obtained results will be made based on finite element method (FEM) analysis. The goal is to increase the autonomy of the light electric vehicle, based on a PMSM, with a proper control, and after the optimization of the designed machine.

The analytical approach, employed here, can be used for any type of electric vehicle. First of all, for a given maximum load, it will be established the necessary power needed for the propulsion of the vehicle. Secondly, the main steps in the design process of the studied machine will be given. Next, the energetic performances and electro-mechanical characteristics will be presented. The validation of the analytical obtained results is made based on finite element method (FEM). By means of numerical computation, it will be demonstrated that a unity power factor control is possible when using ac machines, by employing a field oriented control strategy. The optimization of the studied machine will be realized based on gradient type algorithm and the obtained results will show the benefits of using a PMSM for the propulsion of the light electric vehicle.

2.1. The needed mechanical performances

The maximum speed and weight of the vehicle are 12 km/h and 158 kg, respectively. The considered vehicle has 4 tires of 11 inches in diameter. The vehicle dimensions are: 1290 mm in length, 580 mm in width and 1150 mm in height. The vehicle will be supplied from a battery of 24 Vcc.

First of all, it is needed to compute the output power of the electric motor which is capable to run the vehicle. Since the mechanical power is the product between the mechanical torque and angular speed, it is possible to establish the speed of the vehicle at the wheel:

nt=v60/(πDt)
(1)

where nt is the velocity measured at the vehicle’s wheels (measured in min-1), v is the vehicle speed (in m/s), Dt is the outer diameter of the wheel (the tire height included, in m). The resulted velocity is nt=244.4 min-1. From mechanical and controllability considerations, it is desirable to have an electric motor operating at higher speed, so it is considered a gear ratio of 6.1 to 1. Thus the electric motor rated speed is imposed at 1500 min-1.

Next, the rated torque has to be established. Since the motor torque is proportional to the wheel radius and the force acting on it, one should determine the force involved by the vehicle’s weight and rolling conditions. The electric motor has to be capable to produce a mechanical force to balance all other forces which interfere in vehicle’s rolling. Thus, the motor force is:

Fm=Facc+Fh+Fd+Fw+Fr
(2)

where Facc is the acceleration force, Fh is the climbing force, Fd is the aerodynamic drag force, Fw is a resistive force due to the wind, and Fr is the rolling force.

Since the vehicle studied here is not for racing, and will be controlled to start smoothly, no acceleration constraints are imposed.

When the vehicle goes hill climbing, based on angle of incline θ, the climbing force is:

Fh=Mtotgsin(θ)
(3)

where Mtot, is the total mass of the vehicle (in kg), g is the gravitational constant (9.8 m/s2).

Usually, the degree of incline is given in percentage. For this special electric scooter it is considered a maximum 8% degree of incline. 1% degree of incline represents the ratio of 1 meter of rise, on a distance of 100 meters. Thus, 1%=atan(0.01)=0°34’ (zero degrees and 34 minutes). For an incline of 8%, the angle is 4°34’ (or 4.57 degrees).

The drag force takes into account the aerodynamics of the vehicle. This force is proportional with the square of the speed, the frontal area of the vehicle (Afr, here 0.668 m2) and the aerodynamic coefficient, kd, (empirically determined, for each specific vehicle (Vogel,2009)):

Fd=Afrv2gkd
(4)

The resistant force due to wind, cannot be precisely computed. It depends on various conditions, like (for common automobiles) the fact that windows are entirely or partially open etc... Also, the wind will never blow at constant speed. However, an expression, determined empirically, which will take into account the speed of wind, vw, can be written as (Vogel,2009):

Fw=((0.98(vw/v)2+0.63(vw/v))krw0.4(vw/v))Fd
(5)

where krw is the wind relative coefficient, depending on the vehicle’s aerodynamics, (here is1.6).

The resistant force due to rolling depends on the hardness of the road’s surface, being proportional with the weight of the vehicle and the angle of incline:

Fr=krMtotgcos(θ)
(6)

(here, the road surface coefficient, kr, is 0.011).

A more precise computation of the rolling resistant force could take into account also the shape and the width of the tires, but these elements are not critical at low speeds, like in this case.

After the computation of the resistant forces, it can be determined the needed torque at the wheel, see Table 2, and finally the rated torque of the electrical machine.

For this specific value of the torque at the wheel, a power of 505.1 W is required. Nevertheless, for small power electrical traction systems, the efficiency is quite poor. Here, the efficiency is estimated at 75%. This means that the output power of the electrical motor, capable to operate in the specified road/mechanical conditions, it has to be at least of 673.5 W. Thus, rounding the power, it is obtained a 700 W electrical machine.

It is now possible to identify the mechanical characteristics of the electrical machines. Two traction motors are considered, with a gear ratio of 6.1 to 1. Thus, the rated mechanical characteristics for one motor are: 350 W, 1500 rpm, 2.2 N.m.

Fh (N)Fd (N)Fw (N)Fr (N)Fm (N)torque at the wheel (N.m)
123.50.0260.66716.98141.219.73

Table 2.

Computed resistant forces and the torque at the wheel.

2.2. Electromagnetic design of the PMSM

The permanent magnet synchronous machine (PMSM) has to provide a maximum power density. For that, good quality materials should be used. The permanent magnet (PM) material is of Nd-Fe-B type, with 1.25 T remanent flux density. The steel used for the construction of PMSM is M530-50A. The material characteristics are presented in Fig. 1.

media/image7.png

Figure 1.

The PM and steel characteristics used as the active part’s materials of the PMSM.

For the PM, the N38SH material was use. This rear earth magnet can be irreversible demagnetized starting from 120°C. The 1.25 T remanent flux density (at 20°C) is however affected with the temperature increase. In order to compute the real value of the PM’ s remanent flux density, for a temperature derivative coefficient of 0.1% and for an increase in temperature of 110 K, the rated operating point of the PM is 1.11 T (based on the mathematical expressionX20°C+ΔT=X20°C(1αxΔT)).

In order to obtain a smooth torque wave, a fractioned winding type is used. Thus, the PMSM has 8 pair of poles and 18 slots. The geometry of the PMSM, the winding configuration and the obtained phase resultant vectors are shown in Fig. 2.

The design approach is based on the scientific literature presented in (Pyrhonen et al., 2008; Fitzgerald et al., 2003; Huang et al., 1998). The output power (measured in W) of an electric machine, when the leakage reactance is neglected, is proportional with the number of phases of the machine, nph, the phase current, i(t), and the inducted electromotive force (emf), e(t):

Pout=ηnphT0Te(t)i(t)dt=ηnphkpEmaxImax
(7)

where T is the period of one cycle of emf, Emax, and Imax represent the peak values of the emf and phase current, kp is the power coefficient, and η is the estimated efficiency.

The peak value of the emf is expressed by introducing the electromotive force coefficient, kE:

Emax=kENtBgapDgapLmfsp
(8)

where Nt is the number of turns per phase, Bgap and Dgap are the air-gap flux density and diameter, Lm is the length of the machine, fs is the supplying frequency and p is the number of pole pairs.

By introducing a geometric coefficient, kL=Lm/Dgap, and a current coefficient (related to its wave form) ki=Imax/Irms, and defining the phase load ampere-turns,

Ath=2/πNtIrms/Dgap
(9)

it is possible to define the air-gap diameter of the machine:

Dgap=2pPoutπnphAtkekikpkLηBgapfs3
(10)

Based on the type of the current wave form, it is possible to define the current and power coefficients (Huang et al., 1998). Thus, for sinusoidal current wave form, ki=2,kp=0.5, for rectangular current wave ki=1,kp=1 and for trapezoidal current waveki=1.134,kp=0.777.

All the other geometric parameters will be computed based on this air-gap diameter. The designer has to choose only the PMs shape and stator slots.

The air-gap flux density is computed based on the next formula:

Bgap=hmBrmDgap2(ln(RsigapRcr)+ln(RsiRsigap))
(11)

where, hm and Brm are the PM length on magnetization direction (in m) and the remanent flux-density (in tesla), respectively, Rsi and Rcr are inner stator radius and rotor core radius, respectively.

media/image17.png

Figure 2.

The PMSM: (a) geometry; (b) fractioned type winding configuration; (c) the resultant voltage vectors.

The saturation factor, ks, has to be computed in order to take into account the non-linearity of the steel. ks depends on the equivalent magnetomotive force, Fm, in each active part of the machine and in the air-gap:

ks=(2Fmt+Fmy+Fmr+2Fmg)/(2Fmg)
(12)

where ‘t’, ‘y’, ‘r’ and ‘g’ indices refer to the stator teeth and yoke, rotor core and air-gap, respectively. Each magnetomotive force is computed based on the magnetic field intensity (H) and the length (l) of the active part of the machine, on the flux direction:

Fmx=Hxlx
(13)

Equation (13) is general and used for the computation of the magnetomotive force in each active part of the machine, while ‘x’ replaces ‘t’, ‘y’, ‘r’ and ‘g’ indices. The parameter lx can be easily expressed. Further on, the magnetic field intensity is computed. The Hx value can be chosen from the supplier B(H) magnetic characteristic (for each computed value of the flux density).

Next, the electromagnetic parameters of the PMSM should be determined. The phase resistance depends on: copper resistivity, ρco, length of series turns, lt, and conductor cross section, Sc:

Rph=ρcolt/Sc
(14)

The d-q axis reactances are computed based on magnetizing (Xm) and leakage (Xσ) reactances:

Xd,q=Xσ+Xm_d,qka_d,q/ks
(15)

where d-q magnetizing reactances depend on the saliency coefficient, ka_d,q, (which equals unity for surface mounted PM machines: Xm_d = Xm_q):

Xm_d,q=4nphfsτpLm(Ntkws)2μ0kad,q/(πpgap)
(16)
Xσ=4πfs(Nt)2μ0Λσ/(pq)
(17)

where τp is the polar pitch, kws is the winding factor, q is the number of slots per pole and per phase, and Λσ is the sum of leakage permeances. The saliency ratios (for saliency rotors) are:

ka_d=παmp+sin(παmp)4sin(αmpπ/2)ka_q=παmpsin(παmp)+2/3cos(αmpπ/2)4sin(αmpπ/2)
(18)

where αmp is a coefficient representing the percentage of magnet covering the rotor pole.

For motor operation of PMSM (with magnetic anisotropy), we can use the typical load phasor diagram, in d-q reference frame, Fig. 3. From this phasor diagram one will get the d-q axis reactances equations, function of phase voltage, Uph, phase electromotive force, Eph, phase resistance, Rph, d-q axis currents and internal angle, δ:

media/image26.png

Figure 3.

Phasor diagram for PMSM in motor-load conditions.

Xd=(Uphcoscos(δ)ERphIq)/IdXq=(Uphsinsin(δ)+RphId)/Iq
(19)

Also, it is possible to compute the source current, Is=Id2+Iq2, knowing that the direct and quadrature current are obtainedby developing (19):

Id=Uph(Xqcos(δ)Rphsin(δ))EphXqRph2+XdXqIq=Uph(Xdcos(δ)+Rphsin(δ))EphRphRph2+XdXq
(20)

The electromotive force is proportional with the frequency, the number of turns, the air-gap flux per pole and a demagnetization coefficient, kd (given by the PMs material supplier, usually between 0.8 – 0.9 for rare earth PMs):

Eph=2πfsNtkwsΨgapkd
(21)

Next, the common electromechanical characteristics can be also computed, namely:

the input power:

Pin=nphUph(Iqcos(δ)Idsin(δ))
(22)

the output power (function of the sum of losses) and axis torque:

Pout=PinLosses
(23)
Tm=Pout/
(24)

the energetic performances (power factor and efficiency, respectively):

cosφ=Pin/(nphUphIs)η=Pin/Pout
(25)

The sum of losses contains the copper (the product between the phase resistance and square current), iron, mechanical (neglected here) and supplementary (estimated to 0.5% of output power) losses.

After the designing process, the following results have been obtained, see Table 3. The reader’s attention is now oriented towards the energetic performances of the PMSM.

ParameterPMSM
Output power (W)350
Rated speed (rpm)1500
Rated torque (N.m)2.2
Battery voltage (V)24
Number of phases ( - )3
Number of pole pairs ( - )8
Number of slots ( - )18
Outer diameter (mm)98.7
Machine length (mm)43.5
Airgap length (mm)1
Airgap flux density (T)0.83
Phase resistance (Ω)0.0424
d axis inductance (mH)0.30515
q axis inductance (mH)0.30515
Phase emf (V)9.058
Rated current (A)16.64
Losses (W)71.4
Power factor (%)60.9
Efficiency (%)83.06
Active part costs (€)27.15
Active part mass (kg)2.69
Power/mass (W/kg)130.1

Table 3.

Comparison of obtained results for the designed PMSM.

2.3. Drive modeling for controlling the PMSM

The power factor for the PMSM is quite reduced (as it can be seen in Table 3). In order to increase the power factor, it is possible to use capacitor battery connected to stator winding. This solution is expensive and non-reliable. On the other hand, the current, and finally the power factor are depending on angle δ and φ (see Fig. 3).

It is possible to rewrite the d,q-axis currents by imposingβ=(δφ). Thus, the currents are Id=Issin(β) andIq=Iscos(β). If one will choose the q axis as phase origin, in Fig. 2, the electric motor will operate to unity power factor (coscosφ=1) ifβ=δ.

The purpose of this subsection is to introduce the control modeling of a PMSM and the controllability of the motor at unity power factor.

First of all, the motor model will be presented. After a short review of the vector control technique, the results of the PMSM control are presented.

From the PMSM equivalent circuit (Fig. 4), one can obtain the machine’s mathematical model. The model takes into account the iron loss. The voltage equations, as a matrix, are:

media/image40.png

Figure 4.

The d (a) and q (b) axis equivalent circuits.

[VdVq]=Rph[IdIq]+(1+RphRir)[0ωLqωLd0][I0dI0q]+[0ωλf]
(26)

where: Vd,q, Ld,q are the d-q axis voltages and inductances, respectively; λf represents the excitation flux produced by the PMs; Rir, is the resistance corresponding to the iron loss.

The phase voltage and total torque equations are:

V2=(ωλf+ωLdI0d+RphIq)2+(ωLqI0q+RphId)2
(27)
T=p[λfI0q+(LdLq)I0dI0q]
(28)

with I0d=Id -Iird and I0q=Iq -Iirq ; representing the d,q axis equivalent currents.

The copper and iron losses are:

Pph=Rph(Id2+Iq2)
(29)
Pir=Rir(Iird2+Iirq2)=(ωLqI0q)2+(ωλf+ωLdI0d)Rir
(30)

The motor speed equation is:

s=V2p(λfLdId)2+(LqIq)2
(31)

Vector-controlled drives were introduced about 30 years ago (as was stated in Buja & Kazmierkowski, 2004) and they have achieved a high degree of maturity, being very popular in a wide range of applications in our days. It is an important feature of various types of vector controlled drives that they allow dynamic performance of AC drives to match or sometimes even to surpass that of the DC drive. At the present, the main trend is to use sensorless vector drives, where the speed and position information is obtained by monitoring input voltages or currents.

The vector control (VC) consists in controlling the spatial orientation of the electromagnetic field and has led to the name of field orientation. The FOC usually refers to controllers which maintain a 90° electrical angle between the rotor d-axis and the stator field components. Thus, with a FOC strategy, the field and armature flux are held orthogonal; moreover, the armature flux does not affect the field flux and the motor torque responds immediately to a change in the armature flux (or armature current). Hence, the AC motor behaves like a DC one.

A basic scheme of the FOC technique was used for the PMSM control. Having a speed and direct axis current as references and using PI controllers, one can obtain the needed stator voltage components for the motor supply. The employed simplified FOC scheme for our simulations is given in Fig. 5.

Direct torque control (DTC) technique was introduced about 20 years ago (as was stated in Bae et al., 2003). The principle of DTC is to directly select voltage vectors according to the difference between the reference and the actual value of the torque and the flux linkage. Thus, the torque and flux errors are compared in hysteresis comparators. Depending on the comparators a voltage vector is selected from the well known switching table of the DTC technique.

In general, compared to the conventional FOC scheme, the DTC is inherently a sensorless control method; it has a simple and robust control structure (however, the performances of DTC strongly depends on the quality of the estimation of the actual stator flux and torque).

The implemented simplified DTC scheme is given in Fig. 6. Here, from the current and speed controllers, it is possible to get the flux and torque references The reference values are compared with the measured ones.From the obtained errors, one can get the voltage vector selection in order to assure the PMSM supply after an abc=>dq transformation.

In contrast to induction motors the initial value of the stator flux in PMSM is not zero and depends on the rotor position. In motion-sensorless PMSM drives the initial position of the rotor is unknown and this often causes initial backward rotation and problems of synchronization. Otherwise, the DTC system possesses good dynamic performances, but in steady state regime the torque-current-flux ripples present high levels.

media/image47.png

Figure 5.

Simplified basic scheme of the implemented FOC technique.

media/image48.png

Figure 6.

Simplified basic scheme of the implemented DTC technique.

Both techniques can be used for controlling the PMSM at unity power factor. Here, the FOC was employed.

The internal angle of the PMSM can be expressed function of d,q axis voltages:tan δ= – Vd/Vq. Then, in stationary regime (derivate terms are suppressed), one will get:

tanδ=RphIssinβ+ωLqIscosβRphIphcosβ ωLdIssinβ+ωΨm
(32)

Neglecting the phase resistance, the internal angle tangent becomes:

tanδ=ωLqIscosβ ωLdIssinβ+ωΨm
(33)

For unity power factor, β equals δ and the following expression is obtained:

sinβcosβ=ωLqIscosβ ωLdIssinβ+ωΨm
(34)

One will get, after calculation, a second degree equation which solution is:

sinβ=1±14LdLqIs2Ψd(1LqLd)2LdIsΨm(1LqLd)
(35)

In this way, the d,q currents will be computed for unity power factor.

The simulations results are presented in Fig. 7-Fig. 8. After 0.5 seconds, a reference speed is imposed. The measured speed follows the reference one, and in a very short time it reaches the desired value. This acceleration is accompanied by a current supply, from the electric source. Since the motor is of orthogonal type (a Park transformation was used to transform the 3 phase equation system in a 2 phase one), we will exploit the direct and quadrature axis currents to produce de torque and to evaluate the active and reactive power. To maximize the torque, the Id should be imposed to zero. Thus, the Iq is the image of the axis torque.

The active and reactive powers are computed based on direct and quadrature currents and voltages, respectively. From those values, one can compute the energetic performances of the designed PMSM, Fig. 8. For a load torque of 2.2 N.m, the absorbed electric power (corresponding to the active power P) is of 379 W, meaning that an efficiency of 92.3% is obtained through this vector control strategy. The reactive power is used for the computation of the power factor.

media/image53.png

Figure 7.

PMSM simulation results: (a) electrical performances; (b) mechanical performances.

media/image54.png

Figure 8.

PMSM simulation results: energetic performances.

Based on the obtained simulation results, it can be said that the analytical approach was validated. The unity power-factor control strategy has been successfully employed since the simulated results show a power factor over 99%!

3. Numerical validation of the designed PMSM

In order to prove the electromagnetic design validity, it has been employed a numerical computation based on finite element method (FEM). This analysis has been carried out by using Flux2D. The FEM analysis of PMSM in motor operation regime is employed at rated speed (1500 min-1), while the stator is fed with three currents delayed in time by 120°.

The saturation level can be observed in Fig. 9. In Fig. 10 have been plotted the air-gap flux density, the 3-phase sinusoidal currents, axis torque and iron loss. It can be observed that the air-gap flux-density value is very close to the one obtained from analytical approach, 0.826 T. On the other hand, the rated torque is obtained based on rated current. Also, thanks to the proper winding-slots-poles configurations, the torque ripples are significantly reduced. In fact, the ratio of torque ripple is of 0.8% (maximum at 2.222 N.m and minimum at 2.204 N.m)! For the computed iron loss (average value) a supplementary explanation is needed.

It has been observed that from analytical approach the iron loss is of 34.42 W. From FEM analysis, the average value of iron loss is 27.573 W, meaning that an improved efficiency is obtained. This difference can be explained regarding Fig. 9, where the flux density is depicted in the machine’s active part. Here, the flux density varies significantly in the stator iron, while in the analytical approach a fixed maximum flux density was used. Since the FEM analysis has more credit, it can be said that 2% improved efficiency is obtained!

4. Optimization of the designed PMSM

After the design process and numerical validation, the optimization approach of the studied electrical machine will be presented. Since we want to obtain a specific power for the PMSM, we could say that our optimization objective will be to reduce the volume of the machine (consequently the mass of the active parts of the machine), while the output power is maintained constant (or very close to the desired value). Thus, the objective function is to minimize the mass of the active parts of the PMSM. This mass, called mtot is defined by the mathematical expression:

mtot=mcopper+mrs+mss+mpm
(36)

where mcopper refers to the mass of the winding copper, mrs is the mass of the rotor steel, mss is the mass of the stator steel and mpm is the mass of the permanent magnet.

4.1 The optimization method

The optimization of studied electrical machine is based on gradient algorithm, (Tutelea& Boldea, 2007). The main steps in the optimization algorithm are:

  1. Choose the optimization variables (which will be modified in the process; starting value and boundariesof the optimization variables are imposed).

  2. Impose special limitations of other variables which can be altered during process.

  3. Define the objective function.

  4. Set initial and final value of global increment. The objective values will be initially modified with larger increment, which will be further decreased in order to refine the search space.

  5. Compute geometrical dimensions, the electromagnetic parameters and the characteristics (given in section 2.c), and evaluate the objective function.

  6. Make a movement in the solution space and recompute the objective function and its gradient. Use partial derivative to find the worse and the track points.

  7. Move to the better solution, while the objective function is decreasing.

  8. Reduce the variation step and repeat the previous steps. The algorithm stops when the research movement cannot find better solution, even with smallest variation step. The found value represents a local minimum; a different value can be found by changing the initial starting point.

media/image56.png

Figure 9.

Flux-density and field lines for studied PMSM.

media/image57.png

Figure 10.

FEM results of PMSM in motor regime.

The goal of the optimization process is to maximize the power density (power/mass ratio) – this is our objective function. The parameters to be varied, in the optimization process, are: the length of the machine, the air-gap length, the PM length (on the magnetization direction), the inner stator diameter, the stator slot’s height, the tooth width, the stator yoke height and isthmus height.The initial values and the boundaries are given in Table 4.

parameterInitial valueBoundaries
inner stator diameter (mm)59[30 …80]
slot height (mm)13.4[8 …18]
isthmus height (mm)1.5[0.7 …3]
height of the stator yoke5[3 …9]
width of stator tooth (mm)4[3 …8]
air-gap length (mm)1[0.5 …1.5]
height of the PM on magnetization direction (mm)3[2 …6]
length of the machine (mm)43.5[20 …60]

Table 4.

Optimization variables: initial values and boundaries.

Supplementary constraints were considered for the mechanical outputs (torque and power) and electrical (supplied current) characteristics, see Table 5.

parameterBouderies
Axis torque (N.m)[2.1 … 2.3]
Output power (W)[340 … 360]
Supplied current (A)[13 … 18]

Table 5.

Optimization variables: supplementary constraints.

4.2 Obtained results

The optimization procedure was lunched. The iterative process has reached its optimum after 672 steps, the simulation time being 5.58 seconds on an Intel Core 2 of 2Ghz processor, 2 Gb RAM.

In Fig. 11 have been plotted the current source, the output power and axis torque, to prove that the supplementary constraints were satisfied. The current reaches its upper limit after 672 steps, thus the optimization process is stopped. It is true, the copper loss will increase a little bit, but will not affect drastically the efficiency.

Next, the evolution of the geometric and energetic parameters is plotted in Fig. 12. Not all the geometric parameters are shown. Here, only the stator tooth width, the PM’s height and stator yoke’s height are presented as a sample. It can be seen that some parameters are maintained constant, while others are varied. The gradient type optimization algorithms are sometimes limited and they do not exploit every possible solution (meaning that a local optimum was reached, and the algorithm cannot exit from this local optimum). In order to see other possible geometrical solutions, the user needs to change the starting values; thus, new solution could appear.

It is obvious that, if the current source will increase, the copper loss will increase too. This is a normal behavior, since we want to keep the same number of turns per phase, and not to increase the copper volume. On the other hand, since the geometry volume was reduced, the iron loss is decreased too. Thus, there is compensation on the efficiency.

Practically, the efficiency of the machine has, globally, increased with 1.6%. The power factor has kept the starting value. Thus, with a proper control, this parameter can be optimized.

Finally, the objective function evolution, and the power density ratio are plotted in Fig. 13. If the initial mass of the active parts of the machine was 2.6 kg, the optimized PMS has only 1.93 kg, meaning a mass gain of 28%.

The resume of the optimized results of the PMSM are given in Table 6.

parameterPMSM-RFGain (%)
Rated current (A)18-7.6
Losses (W)67.4+5.6
Power factor (%)59.8-1.8
Efficiency (%)84.4+1.6
Active part costs (€)22.79+16.1
Active part weight (kg)1.93+28.3
Power/weight (W/kg)194.3+33.1

Table 6.

Main optimization results, at rated operating point, of the PMSM.

(In order to validate the obtained optimization results, the author has introduced again the modified parameters into the FEM software to re-compute the performances of the designed machine. The optimization results have been confirmed by the FEM analysis, like the results presented in Section 3.)

media/image58.png

Figure 11.

Optimization results of PMSM: source current and mechanical performances constraints.

media/image59.png

Figure 12.

Optimization results of PMSM: evolution of geometrical and energetic parameters.

media/image60.png

Figure 13.

Optimization results of PMSM: power density and mass improvement.

5. Conclusions

The paper presents the main steps to be followed in the design process of a permanent magnet synchronous machine used for light electric vehicles. Even if the analytical approach is not completely detailed, it contains the major elements which need to be discussed. Detailed equations are presented for the calculation of the desired output characteristics, based on certain mechanical performances. Thus, for a specific load and taking into account the vehicle’s weight and the road profile, it is possible to get the needed output power which will be capable to run the vehicle.

Usually, the traction of light electric vehicles is employed with dc motors. The disadvantage of such a motor is related to its poor efficiency and power density. The permanent magnet synchronous machine (PMSM) has the best power/mass ratio, and very high efficiency. Nevertheless, two problems need to be solved for the PMSM: one is related to the poor power factor and the other one to the torque ripples. The first problem is solved with a proper vector control technique, while the second issue is solved with a proper winding configuration. A fractioned type winding configuration was used for the PMSM, and a very smooth torque was obtained: the torque ripples are of 0.8%.

The design of the PMSM is completed with the optimization of the motor, based on gradient type algorithm. The objective function of the problem is the minimization of the machine’s active parts mass, while the output power is kept practically constant. After the optimization process, the mass of the PMSM was reduced with 28%, at the same energetic performances (efficiency and power factor). This mass decrease involves also an investment decrease of 16%.

Acknowledgements

This research work was supported by CNCSIS-UEFISCDI, project type TE-250, contract number 32/28-07-2010.

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