Analysis of a Permanent Magnet Synchronous Machine

This is a summary of a project completed along with two fellow students at Lund University in 2016. The full paper can be found here, the paper is based on preparation assignments 1, 2, 3, 4, & 5

Introduction

This project is a technical feasability study on magnetic rotors, their qualities and restrictions. When I first started the study it was the first time I had encountered most of the mechanical terms, equations and methods laid out in the assignments for this module, including the Finite Element Method.

Our aims for the project are to design a magnetic machine that would deliver enough torque for an electric bike application, while maintaining appropriate size, weight, and efficiency. This is to be achieved through:

  1. Calculation
  2. Equivalent circuit analysis with MATLAB
  3. Finite Element Method analysis with FEMM

Initial Calculation

The first stage is to lay out some fundamental assumptions about the application of the machine. In this case it was to be used within a bicycle wheel; this imposes restrictions on size and weight. We also assume a rider weight of 80Kg and bicycle weight of 20Kg with 0mph wind speed. We show that the required power and torque are dependent on the various forms of resistance.

\[Power=((Fdrag + Froll + Fgrav) * v)/0.8\] \[Torque = P/w\]

Input into MATLAB while varying inlination and speed gives the output shown by figure 1.

Bicycle speed dependence on inclination angle and torque
Figure 1: Bicycle speed dependence on inclination angle and torque
Bicycle speed dependence on inclination angle and power
Figure 2: Bicycle speed dependence on inclination angle and power

Equivalent Circuit

The output of the initial simulations is fed back into MATLAB using the equivalent circuit method to find the required machine sizes for different torque outputs. The output of these secondary simulations is shown in Figures 2 & 3.

Power contour for width and diameter
Figure 2: Power contour for width and diameter
Output efficiency for width and diameter
Figure 3: Output efficiency for width and diameter

The equivalent circuit method is much less accurate than finite element but it helped us narrow down the choices for machine size. Our aim for power output is 250W, therefore it was judged to use a diameter of 90mm, width of 80mm going forward.

After more equivalent circuit simulations it can be shown that the effect of the number of magnetic poles on the output power is much greater than size or magnetic air gap. Figure 3 shows the result of varying air gap and number of poles on output power for a 90mm by 80mm machine.

Machine power contour for poles and air gap
Figure 4: Machine power contour for poles and air gap
Output efficiency for poles and air gap
Figure 5: Output efficiency for poles and air gap

It has been determined from the equivalent circuit simulations that power and number of poles are the most important factors as a gear can be used to adjust our torque if there is enough power. A new script is run to determine the optimal size for a 200W, 6 pole machine with a planetary gear. The output is shown in Figure 6, it has a diameter of 75mm and width of 47.5mm.

Equivalent circuit optimal machine with planetary gear
Figure 6: Equivalent circuit optimal machine with planetary gear

Finite Element Method

The finite element method was applied via the FEMM program, called from MATLAB and applied to the inner and outer rotors seperately.

Outer rotor machine heat loss contour for width and diameter
Figure 7: Outer rotor machine heat loss contour for width and diameter
Outer rotor machine power contour for width and diameter
Figure 8: Outer rotor machine power contour for width and diameter

Figure 6 shows one of the output diagrams and shows significant variation from the equivalent circuit diagrams. We conclude that this variation is due to the FEM being purely 2D and not accounting for losses in the third dimensions which would grow proportionally larger with a lower diameter.

The next stage is to compare the inner and outer rotor topologies for temperature distribution and flux density.

Inner machine rotor flux density
Figure 9: Inner machine rotor flux density
Outer machine rotor flux density
Figure 10: Outer machine rotor flux density

The inner rotor seems to display a better spread of flux density compared to the outer. For the heat distribution it is the opposite so the differences in design choice may not be very different. The harmonics are also analysed and judged to be satisfactory.

Conclusion

The results from all the simulations are processed and digested to inform the decision of the final design parameters. The final design drawing is shown in figure 11.

Width Diameter Poles Air Gap Rotor Position Weight
80mm 120mm 6 0.8mm Outer 3.5kg
Final machine geometry
Figure 11: Final machine geometry

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