Kinematics: Question 8

Syllabus 2.1

Structured AS 10 marks

A footballer kicks a ball from ground level on a horizontal pitch. The ball leaves her foot with an initial speed of 18.0 m s118.0\text{ m s}^{-1} at an angle of 35.0°35.0° above the horizontal. Air resistance is negligible. Take g=9.81 m s2g = 9.81\text{ m s}^{-2}.

(a) Calculate the horizontal component and the vertical component of the ball's initial velocity. [2]

(b) Calculate the time taken for the ball to reach its maximum height. [2]

(c) Calculate the maximum height reached by the ball above the pitch. [2]

(d) Calculate the total time of flight before the ball lands back on the pitch. [2]

(e) Calculate the horizontal distance travelled by the ball before it first lands. [2]

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Worked solution

Setting up the problem

The horizontal and vertical motions of the ball are independent: the horizontal component of velocity stays constant (no horizontal force, air resistance negligible), while the vertical component is uniformly decelerated (then accelerated) by gravity, g=9.81 m s2g=9.81\text{ m s}^{-2} downwards.

Part (a): Components of the initial velocity

Resolving the initial velocity u=18.0 m s1u=18.0\text{ m s}^{-1} at 35.0°35.0° above the horizontal: ux=ucos35.0°=18.0×0.8192=14.7 m s1(3 s.f.)u_x = u\cos35.0° = 18.0 \times 0.8192 = 14.7\text{ m s}^{-1} (3\text{ s.f.}) uy=usin35.0°=18.0×0.5736=10.3 m s1(3 s.f.)u_y = u\sin35.0° = 18.0 \times 0.5736 = 10.3\text{ m s}^{-1} (3\text{ s.f.})

Part (b): Time to reach maximum height

At maximum height the vertical velocity is momentarily zero. Taking upwards as positive, a=g=9.81 m s2a=-g=-9.81\text{ m s}^{-2}. Using vy=uy+atv_y = u_y + at with vy=0v_y=0: 0=10.3249.81tup0 = 10.324 - 9.81\,t_{up} tup=10.3249.81=1.05 s(3 s.f.)t_{up} = \frac{10.324}{9.81} = 1.05\text{ s} (3\text{ s.f.})

Part (c): Maximum height reached

Using vy2=uy2+2ahmaxv_y^2 = u_y^2 + 2ah_{max} with vy=0v_y=0 and a=9.81 m s2a=-9.81\text{ m s}^{-2}: 0=(10.324)22(9.81)hmax0 = (10.324)^2 - 2(9.81)h_{max} hmax=106.5919.62h_{max} = \frac{106.59}{19.62} hmax=5.43 m(3 s.f.)h_{max} = 5.43\text{ m} (3\text{ s.f.})

Part (d): Total time of flight

Since the ball lands back at the same height (ground level) from which it was launched, the time to fall from maximum height back to the ground equals the time taken to rise to maximum height. So the total time of flight is: T=2tup=2(1.0524)T = 2\,t_{up} = 2(1.0524) T=2.10 s(3 s.f.)T = 2.10\text{ s} (3\text{ s.f.})

Part (e): Horizontal range

The horizontal component of velocity is constant throughout the flight, so: x=uxT=14.745×2.1049x = u_x T = 14.745 \times 2.1049 x=31.0 m(3 s.f.)x = 31.0\text{ m} (3\text{ s.f.})

Check: using the range formula R=u2sin(2θ)g=(18.0)2sin70.0°9.81=324×0.93979.81=31.0 mR=\dfrac{u^2\sin(2\theta)}{g}=\dfrac{(18.0)^2\sin70.0°}{9.81}=\dfrac{324\times0.9397}{9.81}=31.0\text{ m}, which agrees.

Final answers

  • (a) ux=14.7 m s1u_x = \boxed{14.7}\text{ m s}^{-1}, uy=10.3 m s1u_y = \boxed{10.3}\text{ m s}^{-1}
  • (b) Time to maximum height =1.05 s= \boxed{1.05}\text{ s}
  • (c) Maximum height =5.43 m= \boxed{5.43}\text{ m}
  • (d) Total time of flight =2.10 s= \boxed{2.10}\text{ s}
  • (e) Horizontal range =31.0 m= \boxed{31.0}\text{ m}