

I am a bit stuck on this question, particularly part b. I have found that air resistance is equal to 689N from part a (though I am not sure that this is correct) So far for part b, I have used suvat to find the deceleration of the car to be 6.05ms^2 and then used F=ma to find the force to be 13007.5 N but I don't know what this force is or if these steps are necessary.
In the first situation, the forces involved are the following:
Applying the second Newton's law in the directions perpendicular and parallel to the motion:
$$ N - m\,g\,\cos\alpha = 0\,, \; \; \; F_d + m\,g\,\sin\alpha - F_a = m\,a $$
and given that $a = 0$, we get:
$$ N = m\,g\,\cos\alpha = 20771.1\,N\,, \; \; \; F_a = F_d + m\,g\,\sin\alpha = 4362.5\,N\,. $$
In the second situation, the forces involved are the following:
Applying Newton's second law parallel to motion:
$$ m\,g\,\sin\alpha - F_a - \mu\,N = m\,a $$
i.e.
$$ m\,g\,\sin\alpha - \left(F_d + m\,g\,\sin\alpha\right) - \mu\left(m\,g\,\cos\alpha\right) = m\,a $$
from which:
$$ a = - \frac{F_d + \mu\,m\,g\,\cos\alpha}{m}\,. $$
On the other hand, the stopping time is equal to:
$$ 0 = v_0 + a\,t \; \; \; \Leftrightarrow \; \; \; t = -\frac{v_0}{a} $$
and given that the stopping distance is equal to $L$, we have:
$$ L = 0 + v_0\,t + \frac{1}{2}\,a\,t^2 = - \frac{v_0^2}{2\,a} \; \; \; \Leftrightarrow \; \; \; a = - \frac{v_0^2}{2\,L}\,. $$
Well, all that remains is to match the two expressions of acceleration:
$$ - \frac{F_d + \mu\,m\,g\,\cos\alpha}{m} = - \frac{v_0^2}{2\,L} $$
from which it's possible to obtain the friction coefficient:
$$ \mu = \frac{m\,v_0^2 - 2\,F_d\,L}{2\,m\,g\,L\,\cos\alpha} = 0.592531\,. $$