The condition in which the fictional force will be equal to weight of the car is when the car moves at constant speed.
The horizontal component of the force on the car moving on the inclined plan is given as;
[tex]\Sigma F_x = 0\\\\Wsin(\theta) - F_k = ma[/tex]
where;
when the speed of the car is constant, the acceleration of the car will be zero.
[tex]Wsin(\theta) - F_k = m(0)\\\\Wsin(\theta) = F_k[/tex]
Thus, we can conclude that the condition in which the fictional force will be equal to weight of the car is when the car moves at constant speed.
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