Answer:
On the hill, (a) the centripetal force is [tex]\mathbf{932.70N}[/tex], approximately and on the top of the hill, (b) the normal force exerted on the cycle is [tex]\mathbf{4411.14N}[/tex].
Explanation:
In this case, uniform circular movement equations are suitable, then (a) the centripetal force is given by
[tex]F_c=\frac{mv^2}{r}=\frac{324kg\times\left(22.7\frac{m}{s}\right)^2}{179m} \approx \mathbf{932.70N}.[/tex]
Now, (b) at the top of the fill, where weight alligns with the centripetal force and the normal, by applying Newton's second law, we have
[tex]N-w-F_c=0\\N=w+Fc=324kg\times 9.81\frac{m}{s^2}+932.70N \approx \mathbf{4411.14N}.[/tex].