An Ultimate Guide to Axial Flux Motors
Axial flux motors (AFMs) have surged from research labs into real products—from robotics and e-mobility to aerospace and distributed generation. Their disc-like geometry packs high torque in a short axial length, enabling thin, pancake-style machines that fit where traditional cylindrical (“radial flux”) motors struggle. What is an Axial Flux Motor? In an axial flux machine, magnetic flux travels parallel to the shaft (axially) across a flat air gap between a rotor disc with permanent magnets (or a wound field) and a flat stator disc with windings. By contrast, radial flux machines guide flux radially, across a cylindrical air gap between an inner rotor and outer stator. The axial configuration creates a large effective lever arm (mean radius), so for a given air-gap shear stress the torque scales roughly with the cube of radius and only linearly with axial length. That’s why AFMs tend to offer excellent torque density for a given mass and especially for limited axial space. Common AFM topologies Single-stator, single-rotor (SS-SR): Simplest build; unbalanced axial magnetic forces must be handled structurally. Double-rotor, single-stator (DR-SS): Rotors on both sides of one stator balance axial forces and double the active area for the same diameter. Double-stator, single-rotor (DS-SR): A central rotor sandwiched by two stators; also balances axial forces and doubles active copper. Yokeless and segmented armature (YASA-type): Segmented tooth modules without a continuous back iron reduce iron mass and eddy losses, thereby improving torque density. Coreless (air-core) stator: Eliminates iron teeth to remove cogging and iron losses virtually; great for smoothness and partial-load efficiency, but lower flux density and higher copper mass. PCB stator (very low power): Spiral copper traces on FR-4 or polyimide; exceptional thinness and precision for fans/micro-drives at low torque. Why Choose (or Not Choose) an AFM? Strengths High torque density at modest diameter; thin “pancake” packaging with short axial length. Low cogging potential (especially with coreless or yokeless designs), yielding smooth motion and low acoustic noise. Scalability in disc area: Large-diameter, low-speed direct-drive generators/motors (e.g., wind, flywheels, test benches). Short end-turns with concentrated windings (in many AFMs) reduce copper loss. Limitations Tighter air-gap control required: the flat faces must remain parallel under load and temperature. Thermal paths can be tricky: Large, thin discs need thoughtful heat extraction to avoid hot spots. Higher pole counts lead to higher electrical frequency at a given rpm (impacts inverter and losses). Manufacturing complexity for segmented stators, magnet fixtures, and rotor banding—especially at high rpm. Typical Performance Ranges (Indicative) Real performance depends on materials, cooling, control, duty cycle, and safety margins. The following ranges are conservative but useful for initial screening: Peak air-gap flux density (NdFeB): 0.6–0.9 T (teethed), 0.3–0.5 T (coreless) Specific electric loading (A, RMS): 20–60 kA/m (air-cooled), up to ~80 kA/m (aggressive liquid cooling) Continuous torque density: ~8–25 N·m/kg (well-cooled designs); peak can exceed 30–60 N·m/kg for short bursts Continuous power density: ~1–3 kW/kg; peak ~2–6 kW/kg (brief) Peak efficiency: 92–97% (properly optimized) Air gap: 0.3–1.5 mm typical (smaller at lower diameter/lower runout) Pole pairs: 6–40 (higher for large diameters/low speed) These are not hard limits; specialized designs, advanced cooling (spray/oil jet, cold plates), and premium magnets can exceed them. Losses and Efficiency Copper (I²R) losses: Dominant at high torque. Reduce via larger conductor cross-section, lower winding temperature, and higher fill factor (35–55% is typical with round or rectangular wire). Iron losses (hysteresis + eddy): Significant in teethed stators; reduce via thin laminations (0.1–0.35 mm), low-loss grades, or Soft Magnetic Composites (SMC) in 3D flux regions. Proximity & skin effect: Grow with electrical frequency and conductor geometry; mitigated by litz wire (low-power) or shaped bar conductors (higher power). Mechanical & windage: Rotating discs can incur windage; shrouding and smooth surfaces help. Inverter (switching + conduction) losses: Rise with electrical frequency (which rises with pole count at a given rpm). Correct device choice (SiC/MOSFET/IGBT), optimal PWM, and appropriate switching frequency are key. Thermal Management AFMs are thin and wide, so heat must be moved radially and axially out of copper and iron: Conduction paths: From teeth/tooth-coils to back-iron to housing; or directly from slot/coil to a liquid-cooled plate. Cooling options: Air convection over stator faces, with finned housings Liquid cold plates behind the stator Spray/oil-jet cooling directly on windings (advanced) Heat flux ballparks: ~5–15 kW/m² (forced air), ~30–100 kW/m² (liquid plates), and higher for direct oil impingement with careful insulation. Materials and Manufacturing Magnets NdFeB (N42–N52, H/EH grades): Highest energy density; watch max temperature (80–180 °C depending on grade). SmCo: Lower remanence but far better thermal stability (200–300 °C); excellent for high-temp or demag-robust designs. Ferrite: Cheap and stable but low energy density; viable with flux concentration structures. Stator iron Electrical steel laminations (0.1–0.35 mm) for teethed stators; SMC for complex 3D flux; or none for coreless. Windings Round-wire coils, rectangular “hairpin-style” (less common in AFM but possible), or litz for high frequency/small machines. PCB windings for micro-AFMs at low torque. Rotor integrity Magnets bonded to a steel or composite carrier; at higher rpm use non-magnetic banding (e.g., carbon fiber sleeves) to contain hoop stress and prevent magnet throw. Tolerances Flatness and parallelism matter. Air-gap uniformity within tens of microns improves efficiency and lowers acoustic noise. Dynamic balance typically to ISO 21940 G2.5 (or better) for quiet operation. AFM vs Radial Flux vs Transverse Flux Below is a practical comparison. Values are indicative—not absolutes—and assume competent cooling and modern materials. Attribute Axial Flux (AFM) Radial Flux (RFM) Transverse Flux (TFM) Packaging Thin “pancake”, short axial length Longer axial length, smaller diameter Bulky, complex magnetic paths Continuous torque density High (8–25 N·m/kg, higher with liquid cooling) Moderate–High (6–20 N·m/kg) Potentially very high but hard to realize Power density 1–3 kW/kg (cont.), 2–6 kW/kg (peak) 1–2.5 kW/kg (cont.), up to ~4 kW/kg (peak) High potential; complex manufacturing Pole count (typ.) Medium–High (6–40 pairs) Low–Medium (3–12 pairs) High Electrical frequency at given rpm Higher (due to more poles) Lower Higher Cogging & ripple Very low with coreless/yokeless Low–moderate (mitigation required) Depends on design; often challenging Cooling Needs careful planar