By the end of this chapter you should be able to:
Describe the doubly salient construction of the switched reluctance motor (SRM).
Derive the torque from the co-energy and the inductance profile \(L(\theta)\).
Compute stroke angle, strokes per revolution and switching frequencies.
Explain the asymmetric half-bridge converter and the motoring and generating regions.
List the merits, problems and applications of the SRM.
Construction
Both stator and rotor have salient poles — the machine is doubly salient. Only the stator carries windings: concentrated coils on diametrically opposite poles are connected in series to form a phase. The rotor is simply a stack of shaped laminations, with no windings, no magnets and no cage.
Common configurations: 6/4 (three-phase), 8/6 (four-phase), 12/8 (three-phase).
\(N_s \ne N_r\) so that some rotor pole is always approaching alignment with an excitable stator pole.
Torque Production
Exciting a phase pulls the nearest rotor poles towards alignment, where the reluctance is minimum and the inductance maximum. From the co-energy method of Part 1, with a linear magnetic circuit,
\(dL/d\theta > 0\) (poles approaching): motoring torque.
\(dL/d\theta < 0\) (poles separating): generating/braking torque.
Since torque ∝ \(i^2\), current is unidirectional.
Each phase must be switched on as its inductance starts to rise and off before it starts to fall — hence a rotor-position sensor (or a sensorless estimator) is essential.
Stroke Angle and Frequencies
One stroke is the rotation produced by one phase excitation. With \(m\) phases and \(N_r\) rotor poles:
Problem. A three-phase 6/4 SRM has aligned and unaligned inductances of 60 mH and 8 mH; the inductance rises linearly over 30° of rotation. Find (a) the stroke angle, (b) the average torque during the rising region at a constant 10 A, and (c) the phase-current and stroke frequencies at 3000 rev/min.
The linear-inductance result is optimistic: real SRMs operate deep in saturation, where the co-energy, not \(\tfrac12 i^2 dL/d\theta\), must be used.
The Asymmetric Half-Bridge Converter
Each phase is fed by two switches and two diodes. Turning both switches on applies \(+V_\text{dc}\) to build up current; turning one off lets current freewheel at zero volts; turning both off forces the current through the diodes against \(-V_\text{dc}\), returning the stored magnetic energy to the DC link and collapsing the current quickly before \(dL/d\theta\) turns negative.
Phases are electrically independent: a fault in one leaves the others working — valuable in aerospace and safety-critical drives.
There is no shoot-through risk, since each switch is in series with a phase winding.
At low speed the current is regulated by chopping (hysteresis or PWM); at high speed the back-EMF limits current, and control is by advancing the turn-on and turn-off angles (single-pulse mode).
Merits, Problems and Applications
Simplest, cheapest and most rugged rotor; very high speed capability; no magnets (no rare-earth cost, works at high temperature); losses mainly in the stator; fault tolerant; high starting torque.
High torque ripple; acoustic noise and vibration from radial forces; needs position sensing; non-linear magnetics make control harder; requires a special converter.
Applications: washing machines and vacuum cleaners, high-speed compressors and fans, mining and textile drives, aerospace starter-generators, and research prototypes for magnet-free EV traction.
Summary and Common Mistakes
Doubly salient; windings only on the stator; rotor is plain iron.
\(T = \tfrac12 i^2\,dL/d\theta\): sign set by the slope of \(L\), not by current direction.
Stroke angle \(\varepsilon = 360^\circ/(mN_r)\).
Asymmetric half-bridge: independent phases, energy return through the diodes.
Using the number of stator poles instead of rotor poles in the stroke-angle formula.
Leaving a phase energised into the falling-inductance region — it produces braking torque.
Using degrees instead of radians in \(dL/d\theta\).
Chapter Review
P91.1 Find the stroke angle and strokes per revolution of a four-phase 8/6 SRM.
Show answer
\(\varepsilon = 360/(4 \times 6) = 15^\circ\); 24 strokes/rev.P91.2 In Example 91.1, what current gives 10 N·m in the rising region?
Show answer
\(i = \sqrt{2T/(dL/d\theta)} = \sqrt{20/0.0993} = 14.2\) A.
MCQ 1. The rotor of an SRM carries:
(a) a cage (b) magnets (c) a field winding (d) none of theseShow answer
(d)MCQ 2. Reversing the current in an SRM phase:
(a) reverses torque (b) does not change torque (c) doubles torque (d) gives zero torqueShow answer
(b) — torque depends on \(i^2\).
Why must \(N_s \ne N_r\) in an SRM?
Why is the SRM considered fault tolerant?
What causes the acoustic noise of an SRM?
The final chapter covers two machines built for specialised duties: the servo motor, designed for fast, accurate response inside a feedback loop, and the linear induction motor, which unrolls the induction motor to produce straight-line thrust.