Suppose that the air resistance a car encounters is independent of its speed. When the car travels at $15\mathrm{~m/s}$, its engine delivers $20\mathrm{~hp}$ to its wheels. (a) What is the power delivered to the wheels when the car travels at $30 \mathrm{~m/s}$? (b) How much energy does the car use in covering $10\mathrm{~km}$ at $15\mathrm{~m/s}$? At $30\mathrm{~m/s}$? Assume that the engine is $25\text{%}$ efficient. (c) Answer the same questions if the force of air resistance is proportional to the speed of the automobile. (d) What do these results, plus your experience with gasoline consumption, tell you about air resistance?
The answer key says
a. $40\mathrm{~hp}$; b. $39.8\mathrm{~MJ}$, independent of speed; c. $80\mathrm{~hp}$, $79.6\mathrm{~MJ}$ at $30\mathrm{~m/s}$; d. If air resistance is proportional to speed, the car gets about $22\mathrm{~mpg}$ at $34\mathrm{~mph}$ and half that at twice the speed, closer to actual driving experience.
I understand parts (a) and (b). But in part (c), why does the power delivered to the wheels double again? Is the problem implying that all of the power delivered to the wheels is used to overcome air resistance?
It seems to me like some share of it must be used to overcome internal friction, friction between the wheels and road, and other inefficiencies—quantities that would remain constant even if the air resistance increased.
If the answer to the question in bold is simply yes, then I'd be happy to accept a one-word answer. But I'm wondering if there's something more subtle going on, e.g. if those other forces also have a linear relationship to air resistance.