Looking at the graph shown, it is quite clear, by looking at the current curve vs the power curve, that the electric motor efficiency is pretty much independent of motor speed. Which is what I would expect.
This means that the power consumption will depend almost entirely on the resistance to movement of the vehicle and internal drag. The internal drag will be mainly from the bearings, seals, and gears in the transmission (plus at high speeds aerodynamic drag mainly from prop shafts). These will generally be more or less fixed for bearings and seals, but I'm not sure about gears - in the case of gears, I suspect power consumption will depend on the amount of power transmitted, and the number of gears used. (This suggests that gears should only be used where you need more torque than the maximum the motor can provide, and to match maximum speed to maximum power)
The big one though is rolling and aerodynamic resistance to the movement of the vehicle. And hill climbing.
Rolling resistance is the the power turned into heat in the tyres and shock absorbers, and would seem to be proportional to the the speed but also depends on the surface conditions.
Hill climbing will use the same amount of energy regardless of speed, so its power use (power is energy/time) is proportional to speed. And if you have regenerative braking, you get most of it back when you go back downhill!)
So these two factors will not depend, as a first approximation, on the speed of travel.
The big one! Aerodynamic drag, however, depends on the square of the speed. Doubling the speed quadruples the power needed, but you get there in half the time, so the energy used is only double. But this is still the really big factor for realistic highway speeds, no matter how streamlined the vehicle or how small the frontal area. Crawling along offroad at <40k, it will be pretty small, but once above about that speed it becomes the dominant power requirement.
Hope this analysis helps.
John
JDNSW
1986 110 County 3.9 diesel
1970 2a 109 2.25 petrol
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