S5 Physics Practice Paper: Uniformly Accelerated Motion, Newton Laws, Momentum, Work and Energy, Circular Motion and Power
- 2026-11-12
S5 Physics practice paper on accelerated motion, Newton second law with friction, momentum in collisions, energy on an incline, circular motion and power.
Part 1: Uniformly accelerated motion (16 marks)
Four questions. Write the formula used, substitute values and state units to 3 significant figures.
| # | Question | Answer and marking notes |
|---|---|---|
| 1 | A car starts from rest and accelerates at 2.5 m/s2 along a straight line for 8.0 s. Find the velocity at the end of this stage and the displacement covered. | Use v = u + at with u = 0, so v = 0 + 2.5 x 8.0 = 20.0 m/s. The displacement is s = ut + 0.5 a t2 = 0 + 0.5 x 2.5 x 64.0 = 80.0 m. Check: mean velocity = 10.0 m/s times 8.0 s gives 80.0 m. |
| 2 | The car then travels at a constant 20.0 m/s for 5.0 s. Find the displacement. | With a = 0 the displacement is s = v t = 20.0 x 5.0 = 100.0 m. The velocity is constant, so the displacement is proportional to the time. |
| 3 | The car then decelerates uniformly to rest in 4.0 s. Find the acceleration, including its direction. | Use a = (v – u) / t with v = 0, u = 20.0 m/s and t = 4.0 s, so a = (0 – 20.0) / 4.0 = -5.0 m/s2. The minus sign means the acceleration points opposite to the motion, that is a deceleration of 5.0 m/s2. |
| 4 | Find the total displacement and the average velocity for the whole journey. | Total displacement = 80.0 + 100.0 + 40.0 = 220.0 m and total time = 17.0 s, so the average velocity is 220.0 / 17.0 = 12.94 m/s, that is 12.9 m/s to 3 significant figures. The braking displacement is 0.5 x 20.0 x 4.0 = 40.0 m in the same direction. |
Part 2: Newton second law and friction (18 marks)
A block of mass 4.0 kg rests on a horizontal table. A pulling force of 40 N acts at 37 degrees above the horizontal. The coefficient of kinetic friction is 0.25. Take g = 10 m/s2, sin37 = 0.6 and cos37 = 0.8.
| # | Question | Answer and marking notes |
|---|---|---|
| 5 | Find the normal force exerted by the table on the block. | There is no vertical acceleration, so N + F sin37 = m g and therefore N = 40.0 – 24.0 = 16.0 N. The upward component of the pull makes the normal force smaller than the weight of 40.0 N. |
| 6 | Find the friction force acting on the block. | The block slides, so the friction is kinetic: f = mu N = 0.25 x 16.0 = 4.0 N, directed horizontally opposite to the motion. |
| 7 | Find the acceleration of the block. | The net horizontal force is F cos37 – f = 32.0 – 4.0 = 28.0 N, so by Newton second law a = 28.0 / 4.0 = 7.0 m/s2. |
| 8 | If the pull continues, find the speed and displacement of the block after 2.0 s. | Using v = u + at with u = 0 gives v = 7.0 x 2.0 = 14.0 m/s and s = 0.5 a t2 = 0.5 x 7.0 x 4.0 = 14.0 m. The block is already sliding, so kinetic friction applies throughout. |
Part 3: Momentum conservation and collision (18 marks)
Trolley A of mass 2.0 kg moves right at 6.0 m/s on a smooth horizontal track and collides with a stationary trolley B of mass 3.0 kg. The trolleys lock together after the collision.
| # | Question | Answer and marking notes |
|---|---|---|
| 9 | Find the common velocity of the trolleys after the collision. | External forces are negligible, so momentum is conserved: 2.0 x 6.0 = 12.0 kg m/s = 5.0 v, giving v = 2.4 m/s to the right. |
| 10 | State the total momentum of the system before the collision. | Total momentum = 2.0 x 6.0 + 3.0 x 0.0 = 12.0 kg m/s to the right, and it is unchanged by the collision. |
| 11 | Calculate the kinetic energy lost in the collision. | Before: 0.5 x 2.0 x 6.0 squared = 36.0 J. After: 0.5 x 5.0 x 2.4 squared = 14.4 J. The loss is 21.6 J, that is 60 per cent of the initial kinetic energy, appearing as heat, sound and deformation. |
| 12 | What type of collision is this? Explain in terms of momentum and kinetic energy. | Momentum is conserved but kinetic energy decreases, so this is a perfectly inelastic collision. The trolleys move together with zero relative velocity, so the coefficient of restitution is zero and the kinetic energy loss is the largest possible. |
Part 4: Work and energy on an incline (16 marks)
A block of mass 5.0 kg slides from rest down an incline of height 4.0 m and slope length 5.0 m. Friction does 40 J of work during the slide. Take g = 10 m/s2.
| # | Question | Answer and marking notes |
|---|---|---|
| 13 | Find the decrease in gravitational potential energy. | The loss of potential energy is m g h = 5.0 x 10.0 x 4.0 = 200.0 J. Only the height change matters, not the path taken. |
| 14 | Find the magnitude of the friction force. | Friction does work f L, so f = 40.0 / 5.0 = 8.0 N acting up the incline. |
| 15 | Find the kinetic energy of the block at the bottom. | By energy conservation the loss of potential energy equals the gain in kinetic energy plus the energy dissipated by friction, so the kinetic energy is 200.0 – 40.0 = 160.0 J. |
| 16 | Find the speed at the bottom, and the speed if the incline were smooth. | From KE = 0.5 m v2, v = sqrt(2 x 160.0 / 5.0) = 8.0 m/s. Without friction, v = sqrt(2 x 10.0 x 4.0) = 8.9 m/s, which is larger. |
Part 5: Horizontal circular motion (16 marks)
A ball of mass 0.5 kg moves at 2.0 m/s in a circle of radius 0.8 m on a smooth horizontal table, held by a string through a hole at the centre.
| # | Question | Answer and marking notes |
|---|---|---|
| 17 | Find the centripetal acceleration of the ball. | a = v squared over r = 2.0 x 2.0 / 0.8 = 5.0 m/s2 directed towards the centre of the circle. |
| 18 | Find the tension in the string. | The tension alone provides the centripetal force, so T = m a = 0.5 x 5.0 = 2.5 N. The string length is fixed, so the ball moves in a circle in the horizontal plane. |
| 19 | Find the time taken for one complete revolution. | The period is 2 pi r / v = 2 pi x 0.8 / 2.0 = 2.51 s. The angular speed is v / r = 2.5 rad/s and 2 pi divided by it gives the same period. |
| 20 | If the speed increases to 4.0 m/s at the same radius, what is the required centripetal force? | F = 0.5 x 4.0 squared / 0.8 = 10.0 N. Doubling the speed makes the centripetal force four times larger, since it varies with the square of the speed. |
Part 6: Power and efficiency (16 marks)
A pump lifts 60 kg of water through a height of 5.0 m in 20 s. The efficiency of the pump is 75 per cent. Take g = 10 m/s2.
| # | Question | Answer and marking notes |
|---|---|---|
| 21 | Find the useful work done by the pump. | Useful work = m g h = 60.0 x 10.0 x 5.0 = 3000.0 J, all of it stored as gravitational potential energy of the water. |
| 22 | Find the output power of the pump. | P = 3000.0 / 20.0 = 150.0 W. |
| 23 | Find the input power of the pump. | Efficiency = output over input, so the input power is 150.0 / 0.75 = 200.0 W. |
| 24 | Find the energy dissipated as heat and friction in 20 s. | Input energy = 200.0 x 20.0 = 4000.0 J, so the dissipated energy is 4000.0 – 3000.0 = 1000.0 J, that is 25 per cent of the input. |
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