I was asking a similar question about general energy consumption. The approach I took is presented below. I hope some of you could verify this in terms of physics, specifically in regard to the Law of conservation of energy.
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The mass of a car equals 1000 kg. Its frontal area is $2x1,5 = 3 m^2$ and the aerodynamic coefficient is 0,3. The average rolling coefficient is 0,01. Let’s assume the drive-chain is 100% efficient and there is no AC nor heating. The brakes use no recuperation unfortunately, for ease of calculation.
This took me quite a while to find the right formula to calculate this. I hope it is convincing:
$$E_{el} = E + E_l$$
Where: $E_el$ – is total energy consumed by the motor, $E$ – energy consumption of the motion, $E_l$ – drive train and idling losses [ $E_l = 0$ in our case ]
$$E = E_{rr} + E_{air} + E_{gr} + E_k$$
Where: $E_{rr}$ – energy lost to rolling resistance, $E_{air}$ – energy lost to air resistance, $E_{gr}$ – enrgy lost to climb grades = 0 as assumed, $E_k$ – energy used to increase kinetic energy.
$$E = ½ mv^2$$ - during acceleration only
$$E_{rr} = mgC_{rr}(L_a + L_d)$$ and $$E_{rr} = m g C_{rr} L_{avg}$$
Where $m$ is mass, $g$ – gravity, $C_{rr}$ – rolling resistance coefficient, $L$ - distance covered, $a$ – acceleration, $d$ – deceleration, $avg$ – average velocity for the steady case.
$$E_{air} = AC_d(V_{avg}^2L_a + V_{avg}^2L_d)$$ and $$E_{air} = AC_d V_{avg}^2L_{avg}$$
Where $A$ - frontal area, $C_d$ - air friction coefficient [ $\rho = 1$, negligible ]