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IPM and SPMInductionEESMSynRMHairpin windings

Every traction motor has essentially the same stator: three-phase windings in a laminated steel bore. The interesting choice — cost, efficiency, supply-chain exposure, controller complexity — is what spins inside it.

7.1Five rotors, one stator

VIPMmagnets buried in Vrare earthSPMmagnets on surfacerare earthInductioncast conductor cageno magnetsSynRMflux barriers onlyferrite optionalEESMwound field polesno magnetsNSconductor
Figure 7.1Simplified quarter-symmetry views. The V-shaped magnet arrangement in the IPM rotor is doing two jobs at once — it holds the magnets against 20,000 rpm centrifugal load, and it deliberately creates the flux barriers that generate reluctance torque.

The V-shaped magnet arrangement in the IPM rotor is doing two jobs at once: it holds the magnets against 20,000 rpm centrifugal load, and it deliberately creates the flux barriers that generate the reluctance torque of chapter 6.

7.2What each topology commits you to

TopologyWhat it gives youWhat it costs
IPM — interior permanent magnetPeak efficiency 96–97 %, the highest torque density available, mechanical retention and reluctance torque from the same buried geometry, and a wide field-weakening range. The incumbent.1–2 kg of NdFeB per motor, with heavy rare earths for temperature. Back-EMF is always present, so an inverter fault at high speed produces uncontrolled generation and braking torque.
SPM — surface permanent magnetSimple to model, near-sinusoidal back-EMF, very low torque ripple. Common in servos and industrial drives.L_d ≈ L_q, so no reluctance torque at all and poor field weakening. Magnets need a retaining sleeve above modest speeds. Rarely used in traction.
Induction — IMA shorted cage of aluminium or copper bars. Robust, cheap, no magnets, no supply exposure, and it free-wheels harmlessly when de-energised.Rotor I²R loss exists by definition — the rotor has to carry current to work — so efficiency runs 2–4 points below IPM, worst at light load, which is most of a drive cycle. Rotor heat is hard to remove.
EESM — externally excited synchronousThe rotor is an electromagnet fed through slip rings or a rotating transformer, so field strength becomes an independent control variable: full flux for launch, weak flux at cruise. No back-EMF when de-excited, so no uncontrolled generation. Zero rare earths.Rotor copper loss, brushes or a contactless exciter to maintain, and a more complex inverter. BMW and Renault ship it at scale, so the objections are engineering rather than fundamental.
SynRM and ferrite-assisted SynRMPure reluctance torque from a rotor of stamped flux barriers. No magnets, no rotor current, no rotor loss, and very cheap. Adding low-cost ferrite into the barriers lifts torque density substantially without touching a rare earth.Low power factor drives up inverter VA rating, and torque ripple is high. The ferrite variant inherits ferrite’s cold-demagnetisation behaviour from chapter 5.
Axial fluxFlux runs parallel to the shaft in a pancake geometry. Because torque scales as D²L, a large-diameter short-axial machine is intrinsically torque-dense — 2–3× the N·m/kg of a comparable radial motor.Large axial magnetic attraction forces demand stiff structures and precise gaps. Harder to manufacture and to cool. Genuinely excellent for in-wheel and space-constrained installations.

7.3Why hairpins replaced round wire

Slot fill factor is the fraction of the slot occupied by copper rather than air, insulation and varnish. Randomly wound round wire reaches 40 to 45 per cent. Rectangular hairpin conductors — pre-formed U-shaped bars inserted and laser-welded — reach 65 to 75.

  • More copper in the same slot means lower resistance, which means less I²R loss and better continuous rating from the same volume.
  • It also gives a far better thermal path from conductor to stator iron, because rectangular bars sit flat against the slot wall instead of touching it at points.

Important

The catch appears at high speed. A large solid conductor in a slot suffers skin and proximity effects. At 800 Hz electrical the current crowds into the outer few millimetres of the bar — and a hairpin bar is a few millimetres. The AC resistance can be several times the DC value exactly where the motor spends its highway life.

7.3.1The tension is structural

The hairpin’s fill-factor win and its AC-loss penalty come from the same property: a large solid conductor. Chapter 8 works through the skin-depth arithmetic and the geometric mitigations.

Quick check: test yourself

1.An inverter faults at 15,000 rpm. What happens in an IPM motor that does not happen in an EESM?

Show answer
Uncontrolled generation. An IPM’s magnets are always there, so a rotating rotor keeps inducing back-EMF into a faulted inverter, producing generation and braking torque you cannot switch off. An EESM can simply de-excite its rotor field, after which there is no back-EMF at all — which is one of the strongest arguments for it beyond rare earth avoidance.

2.Induction motors are 2 to 4 points less efficient. Why is that worse than it sounds?

Show answer
Because the gap is largest at light load, and light load is where a vehicle spends most of a drive cycle. Rotor I²R loss exists by definition since the rotor must carry current to work, and rotor heat is hard to remove. Cycle-weighted efficiency suffers more than the peak-efficiency comparison suggests.

3.Hairpin windings raise slot fill from 45 to 70 per cent. Why is that not a straightforward win?

Show answer
Because the same large solid conductor that carries more copper also suffers skin and proximity effects. At 800 Hz — 4 pole pairs at 12,000 rpm — skin depth in copper is about 2.3 mm, the same order as the bar thickness, so AC resistance climbs well above DC exactly during highway cruising.

Chapter summary

Frequently asked questions

Why is IPM the default traction motor?+

Because burying the magnets does three jobs at once: it gives peak efficiency of 96 to 97 per cent and the highest torque density available, it retains the magnets mechanically against centrifugal load, and it creates the flux barriers that generate reluctance torque. It also gives a wide field-weakening range. The costs are 1 to 2 kg of NdFeB per motor with heavy rare earths for temperature, and back-EMF that is always present — an inverter fault at high speed produces uncontrolled generation and braking torque.

What is EESM and why is it growing?+

An externally excited synchronous machine makes the rotor an electromagnet, fed through slip rings or a rotating transformer. Field strength becomes an independent control variable — full flux for launch torque, weak flux at cruise — and with no permanent magnets there is no back-EMF when de-excited, so no uncontrolled generation, and zero rare earth exposure. The costs are rotor copper loss, brushes or a contactless exciter to maintain, and a more complex inverter. BMW and Renault ship it at volume, so the objections are engineering rather than fundamental.

Why is induction less efficient than IPM?+

Because the rotor has to carry current to work, so rotor I²R loss exists by definition. Efficiency runs 2 to 4 points below IPM, and the gap is worst at light load — which is where a vehicle spends most of a drive cycle. Rotor heat is also hard to remove. In exchange you get no magnets, no supply exposure, mechanical robustness, and harmless free-wheeling when de-energised.

Why did hairpin windings replace round wire, and what is the catch?+

Slot fill factor. Randomly wound round wire reaches 40 to 45 per cent copper in the slot; rectangular hairpin bars, pre-formed and laser-welded, reach 65 to 75. More copper means lower resistance, less I²R loss and better continuous rating from the same volume, plus a far better thermal path because flat bars sit against the slot wall rather than touching at points. The catch is AC loss: at 800 Hz electrical the skin depth in copper is about 2.3 mm, which is the same order as a hairpin bar’s thickness, so current crowds to the surface exactly where the motor spends its highway life.

Reviewed by

SG

Sahil Goyal

Co-founder, Wingzman

LinkedIn
SG

Sourabh Goyal

Co-founder, Wingzman

LinkedIn

Magnets and Motors is an original educational series on permanent magnets and electric machines. Datasheet ranges, temperature coefficients and efficiency figures are representative standard-condition literature values, not measurements of a specific product, and sources differ on several. Always verify against the specific magnet and lamination datasheets in use before making design, procurement or certification decisions.