2024 A/L Physics Past Paper · Question 03 (English Medium)

Angle of projection from the kinetic energy at the top

The kinetic energy of a projectile at its maximum height is one-fourth (14\dfrac{1}{4}) of its initial kinetic energy. What is the angle of projection of the projectile with the horizontal? (Neglect air resistance.)

  1. (1) 10∘10^{\circ}
  2. (2) 20∘20^{\circ}
  3. (3) 30∘30^{\circ}
  4. (4) 45∘45^{\circ}
  5. (5) 60∘60^{\circ}
Answer and explanation

Answer: (5) 60∘60^{\circ}

Given information

What we know:

At the maximum height the kinetic energy is 14\dfrac{1}{4} of the initial kinetic energy.

The air resistance is neglected.

What the question asks

We want: the angle of projection θ\theta.

What each letter means:

uu (m s−1\text{m s}^{-1}): the speed of projection.

θ\theta: the angle of projection with the horizontal.

mm (kg\text{kg}): the mass of the projectile.

K0K_0 and KK (J\text{J}): the kinetic energy at the start and at the top.

Relevant theory

Considering the effect on the horizontal component, →ucos⁡θ\rightarrow u\cos\theta, Since horizontally, Acceleration = 0 v=u+atv = u + at v1=ucos⁡θv_1 = u\cos\theta

Horizontal component remains constant.

Vertical component of velocity decreases.

This decreases until it reaches zero.

Translational kinetic energy of the body, W=12mv2W = \frac{1}{2}mv^2

The first quote says that the horizontal component of the velocity stays at ucos⁡θu\cos\theta. The second says that the vertical component falls to zero at the top. So at the maximum height the speed is ucos⁡θu\cos\theta. The third quote gives the kinetic energy, 12mv2\dfrac{1}{2}mv^2.

For example, a stone thrown over a wall rises, slows down and reaches the top. At the top it is not going up or down any more. It is moving sideways, and this sideways speed is the same as it had at the start.

Required equations

K0=12mu2K_0 = \dfrac{1}{2}mu^2

v=ucos⁡θv = u\cos\theta

K=12m(ucos⁡θ)2K = \dfrac{1}{2}m(u\cos\theta)^2

KK0=cos⁡2θ\dfrac{K}{K_0} = \cos^2\theta

Applying it to this question

Divide KK by K0K_0. The factor 12mu2\dfrac{1}{2}mu^2 is in both, so it cancels.

KK0=cos⁡2θ\dfrac{K}{K_0} = \cos^2\theta

0.250.25

cos⁡2θ=14\cos^2\theta = \dfrac{1}{4}

0.50.5

cos⁡θ=14\cos\theta = \sqrt{\dfrac{1}{4}}

6060

θ\theta

Reasoning and calculation

cos(t∗pi/180)2cos(t * pi / 180) ^ 2

Now match it with the five options.

Option (5) is 60∘60^{\circ}. It matches.

The others give a ratio cos⁡2θ\cos^2\theta of about 0.970.97, 0.880.88, 34\dfrac{3}{4} and 12\dfrac{1}{2}. None of them is 14\dfrac{1}{4}.

Checks

Check the units. KK and K0K_0 are both in joules, so their ratio is a plain number, and cos⁡2θ\cos^2\theta is a plain number too.

Does it make sense?

If the ball is thrown straight up, θ=90∘\theta = 90^{\circ}, it stops at the top and its kinetic energy there is 00. If it is thrown flat, θ=0∘\theta = 0^{\circ}, it keeps the whole of its kinetic energy.

60∘60^{\circ} lies between these two, and it keeps a quarter. That fits.

Conclusion

θ=60∘\theta = 60^{\circ}

The angle of projection is θ=60∘\theta = 60^{\circ}.

The answer is (5).

At the top of the path just the horizontal speed ucos⁡θu\cos\theta is left. So the kinetic energy there is cos⁡2θ\cos^2\theta times the first.

Set this equal to the given fraction and solve for θ\theta.

Exam tip

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