Mastering Projectile Motion: Practice Problems and Solutions

Expert reviewed 22 November 2024 7 minute read


Revision of the key Concepts in Projectile Motion

Before diving into practice problems, let’s review the essential concepts:

  • Two-dimensional motion: Projectile motion combines horizontal and vertical components.
  • Constant horizontal velocity: Neglecting air resistance, the horizontal velocity remains constant.
  • Vertical motion: Affected by gravity, causing acceleration in the vertical direction.
  • Parabolic trajectory: The path of a projectile forms a symmetrical parabola.

Essential Equations

The following equations are crucial for solving projectile motion problems:

  • Horizontal position:
x0=x+vxtx_0=x+v_xt
  • Vertical position:
y=y0+vy0t12gt2y = y_0 + v_{y0}t - \frac{1}{2}gt^2
  • Horizontal velocity:
vx=v0cosθv_x=v_0cos\theta
  • Vertical velocity:
vy=v0sinθgtv_y=v_0sin\theta-gt
  • Time of flight:
tflight=2v0sin(θ)gt_{flight} = \frac{2v_0 \sin(\theta)}{g}
  • Maximum height:
hmax=v02sin2(θ)2gh_{max} = \frac{v_0^2 \sin^2(\theta)}{2g}
  • Horizontal range:
R=v02sin(2θ)gR = \frac{v_0^2 \sin(2\theta)}{g}

Where:

  • v0v_0 is the initial velocity
  • θ\theta is the launch angle
  • gg is the acceleration due to gravity (approximately 9.8 m/s²)
  • tt is time

Practice Question 1

A ball is launched from ground level with an initial velocity of 20 m/s at an angle of 30° above the horizontal. Calculate:

  • The maximum height reached by the ball
  • The horizontal range of the ball
  • Maximum height:

    Using the equation: hmax=v02sin2(θ)2gh_{max} = \frac{v_0^2 \sin^2(\theta)}{2g}

    hmax=(20)2sin2(30°)2(9.8)hmax=400×0.2519.65.10 mh_{max} = \frac{(20)^2 \sin^2(30°)}{2(9.8)} \\h_{max} = \frac{400 \times 0.25}{19.6} \\\approx 5.10 \text{ m}
  • Horizontal range:

    Using the equation: R=v02sin(2θ)gR = \frac{v_0^2 \sin(2\theta)}{g}

    R=(20)2sin(60°)9.8R=400×0.8669.835.3 mR = \frac{(20)^2 \sin(60°)}{9.8 } \\R = \frac{400 \times 0.866}{9.8} \\\approx 35.3 \text{ m}

\therefore The ball reaches a maximum height of 5.10 m and travels a horizontal distance of 35.3 m.

Practice Question 2

A projectile is fired from a cliff 100 m above sea level with an initial velocity of 50 m/s at an angle of 45° above the horizontal. How long does it take for the projectile to hit the water?

We need to use the vertical position equation and solve for time:

y=y0+vy0t12gt2y = y_0 + v_{y0}t - \frac{1}{2}gt^2

Where:

  • y=0y = 0 is sea level
  • y0=100my_0 = 100 m is the initial height
  • vy0=50sin(45°)=35.36m/sv_{y0} = 50sin (45°) = 35.36 m/s
  • g=9.8m/s2g = 9.8 m/s^2

Substituting these values:

0=100+35.36t4.9t20 = 100 + 35.36t − 4.9t^2

This quadratic equation can be solved using the quadratic formula:

t=b±b24ac2at = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}

Where, a =  − 4.9, b = 35.36, and c = 100

  • a=4.9a=-4.9
  • b=35.36b=35.36
  • c=100c=100

Solving this gives us two solutions:

t18.54sandt22.38st_1 ≈ 8.54 s \quad \text{and}\quad t_2 ≈− 2.38 s

We discard the negative solution as time cannot be negative. Therefore, the projectile hits the water after approximately 8.54 seconds.

Practice Question 3

A baseball is hit at an angle of 40° above the horizontal. It reaches a maximum height of 30 m. What was the initial velocity of the baseball?

We can use the maximum height equation and solve for v0v_0:

hmax=v02sin2(θ)2gh_{max} = \frac{v_0^2 \sin^2(\theta)}{2g}

Rearranging for v0v_0:

v0=2ghmaxsin2(θ)v_0 = \sqrt{\frac{2gh_{max}}{\sin^2(\theta)}}

Substituting the values:

v0=2(9.8)(30)sin2(40°)v0=5880.41337.7 m/sv_0 = \sqrt{\frac{2(9.8 )(30 )}{\sin^2(40°)}} \\v_0 = \sqrt{\frac{588}{0.413}} \\\approx 37.7 \text{ m/s}

The initial velocity of the baseball was approximately 37.7 m/s.

Return to Module 5: Advanced Mechanics