Formula1 Journal

The motor was cooled by engine oil and the PCU was cooled by a dedicated coolant loop. The 106-cell lithium-ion battery pack was mounted in the forward section of the vehicle’s keel to preserve the vehicle’s center of gravity and take advantage of draft air cooling.

 

Given the light weight (minimum 620 kg/1,367 pounds) and compact design of Formula One cars, Honda calculated that the motor would have to be no more than 100 mm (4 inches) in diameter, 200 mm in length, and produce approximately 8 kilowatts (kW) per kilogram (almost 5 hp per pound) of motor weight. By comparison, a typical mass production hybrid or electric vehicle motor produces between 1.0 and 2.5 kW per kilogram.

 

Stator Core. A three-phase, four-pole, twelve-tooth design with a double lap-wound stator and permanent magnet rotor was selected. Operating motor speed would be roughly equivalent to engine speed, with a range of 13,000 to 21,000 rpm (engine speed was limited to 18,000 rpm during the 2009 F1 season).

 

An initial concern, particularly given the high motor speed, was the effect of iron losses in the stator core, which is typically an AC motor’s heaviest component. Conventional grain-oriented silicon steel was not efficient enough to be used in a motor that would meet the project’s motor size and weight targets, and an iron-cobalt alloy (49Fe-49Co-2V) was used to produce the motor’s stator core laminations. This yielded a 30% increase in flux density and a 15% increase in torque.

 

Relative magnetic flux densities of 49Fe-49Co-2V iron-cobalt alloy, as compared to more common silicon steel. Click to enlarge. The iron-cobalt alloy’s iron losses were further reduced via a combination of technologies. A post-rolling heat treatment reduced core hysteresis losses, and an ultra-thin oxidized insulation coating was developed, which allowed the engineers to reduce stator core lamination thickness to a tenth of a millimeter per lamination while preserving the desired iron-to-insulation ratio. These refinements reduced the alloy’s iron losses by a further 60%.

 

The magnetic flux density of Honda’s iron- cobalt alloy was increased through multiple refinements. Click to enlarge. Although Honda has not released details of the motor control strategy, the maximum current frequency for a 21,000 rpm four-pole motor is 42 kHz, and pulse width modulated voltages driving a motor at such a speed must inherently use extremely fast transients, creating voltage stresses within the winding. Not surprisingly, the stator winding was wound with scratch-resistant inverter duty wire to reduce the possibility of pinholes created during the manufacturing and/or winding process, and therefore reduce the possibility of winding failure.

 

Rotor Design - Honda developed a high-coercivity magnet with an intrinsic coercivity of at least 1.1 Ma/m at 160ºC (320ºF), and tuned the magnetization angles for maximum torque. To minimize temperature increases and resultant eddy current losses, 448 magnets (28 axially, 16 circumferentially) were used in the rotor’s interior PM configuration.

 

Rotor diameter was reduced by employing the rotor’s shaft as part of the rotor flux circuits. A high tensile filament winding made of organic high-strength fibers encloses the rotor, preventing magnet burst at the centrifugal forces produced at the rotor’s 21,000 rpm redline. The rotor’s ceramic ball bearings were lubricated by high-temperature grease rather than oil, to simplify the oil circuit and reduce losses.

 

Section view of motor, showing rotor and stator coolant flow paths; engine oil is used as coolant. A water-cooled motor was initially developed, but could not meet Honda’s size/performance targets. The final motor was cooled by engine oil, with stator cooling passages around the circumference of the rotor and the rotor cooled by oil passing through its hollow shaft. A thin cylindrical resin sleeve structure was mounted in the motor’s rotor-stator air gap to isolate stator cooling oil from the rotor and eliminate windage losses.

 

Motor torque was delivered to the engine’s crankshaft via a front-mounted five-gear gearbox. Vehicle testing commenced in April 2008 with straight course accelerations, and progressed into circuit tests at Silverstone the following month. Additional circuit tests were conducted at full load in September, at the Jerez circuit in Spain, yielding the following results:

•Lap times were reduced by ~0.4 seconds per lap at full assist;

•Speed was increased by 7 km/h, resulting in a gain of 7.8 meters (1.6 car lengths) on a straightaway with a continuous 324 kJ of assist.

The final design achieved 7.8 kW (10.46 hp) of power per kilogram, close to Honda's design goal of 8 kilowatts per kilogram. Peak motor efficiency was 99% and peak generator efficiency during regen was 93%. Motor weight was 6.9 kilograms.

 

KERS systems were introduced to Formula One during the 2009 racing season, and were key to several race wins, but were subsequently withdrawn due to development issues. KERS is expected to return to F1 in 2013 (Editor's note:2011), concurrent with the introduction of new engine regulations. Honda sold its Formula One team to Brawn GP Limited in 2009.

Source

•Development of F1 KERS motor, November 2010 Tamotsu Kawamura, Hirofumi Atarashi, and Takehiro Miyoshi, Automobile R & D Center, Honda R & D Co., Ltd.