A2 June 2019 Q4

EdexcelCurrent spec12 marksPowerWork-Energy Principle

4. A car of mass 600 kg pulls a trailer of mass 150 kg along a straight horizontal road. The trailer is connected to the car by a light inextensible towbar, which is parallel to the direction of motion of the car. The resistance to the motion of the trailer is modelled as a constant force of magnitude 200 N. At the instant when the speed of the car is \(v\ \text{m s}^{-1}\), the resistance to the motion of the car is modelled as a force of magnitude \((200 + \lambda v)\) N, where \(\lambda\) is a constant.

When the engine of the car is working at a constant rate of 15 kW, the car is moving at a constant speed of \(25\ \text{m s}^{-1}\)

(a) Show that \(\lambda = 8\) (4)

Later on, the car is pulling the trailer up a straight road inclined at an angle \(\theta\) to the horizontal, where \(\sin\theta = \dfrac{1}{15}\)

The resistance to the motion of the trailer from non-gravitational forces is modelled as a constant force of magnitude 200 N at all times. At the instant when the speed of the car is \(v\ \text{m s}^{-1}\), the resistance to the motion of the car from non-gravitational forces is modelled as a force of magnitude \((200 + 8v)\) N.

The engine of the car is again working at a constant rate of 15 kW.

When \(v = 10\), the towbar breaks. The trailer comes to instantaneous rest after moving a distance \(d\) metres up the road from the point where the towbar broke.

(b) Find the acceleration of the car immediately after the towbar breaks. (4)
(c) Use the work-energy principle to find the value of \(d\). (4)