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AHL 4.25

Projectiles: launch angle, launch height and clearing a wall

AHL 4.25

Projectiles: launch angle, launch height and clearing a wall

Target: I can find the time to the ground and the horizontal distance for an object thrown horizontally from a height. (+5 more)

By the end of this section

Key points

Setting up

  • Take \(\mathbf{i}\) horizontal and \(\mathbf{j}\) vertically up. The acceleration is \(\begin{pmatrix} 0 \\ −9.8 \end{pmatrix}\) m s⁻² and air resistance is ignored.
  • Launch at speed \(u\) and angle \(\theta\) above the horizontal: \(\mathbf{v}(0) = \begin{pmatrix} u\cos\theta \\ u\sin\theta \end{pmatrix}\). Thrown horizontally: \(\theta = 0\), so the vertical component is zero.
  • Horizontal motion has constant velocity. Vertical motion has acceleration \(−9.8\). Put the launch height in as the starting value of \(y\).
  • Position: \(x = u\cos\theta\, t\), \(y = y_{0} + u\sin\theta\, t − 4.9t^{2}\).

The classic questions

  • Highest point: vertical velocity zero, \(u\sin\theta − 9.8t = 0\). Put that time into \(y\).
  • Landing: solve \(y = 0\) with the calculator and take the positive time. Launched from a height, the time up and the time down are not equal, so do not double the time to the top.
  • Range: horizontal speed × landing time.
  • Speed and direction on landing: put the landing time into \(\mathbf{v}\), then \(|\mathbf{v}| = \sqrt{v_{x}^{2} + v_{y}^{2}}\) and \(\tan\theta = \dfrac{|v_{y}|}{v_{x}}\) for the angle below the horizontal.

Clearing a wall

  • Find the time when \(x\) equals the distance to the wall. Use the horizontal component only.
  • Put that time into \(y\). If \(y\) is greater than the height of the wall, the ball clears it. Otherwise it hits the wall.
  • Check the sign of \(v_{y}\) at that time to say whether the ball is rising or falling.
  • To find the least speed that clears the wall, write the height at the wall in terms of the speed, set it equal to the height of the wall and solve.

On the calculator

Landing time

  • Enter the vertical position as an equation equal to zero.
  • Solve for t, or use the polynomial solver.
  • Take the positive solution. The negative one is before the launch.

Screenshot and video to come

Degrees and radians

  • A launch angle in degrees needs the calculator in degree mode.
  • Work out the two components and store them if you use them again.
  • Return the calculator to radian mode for sin and cos of t in other questions.

Screenshot and video to come

Explore: a projectile under gravity

The velocity is (p, q − 9.8t). Drag the tip of the orange launch arrow to set p and q, and drag the launch point up to give a height. Move the time slider to follow the object. Before you press "Show the landing point", type your prediction of the range.

i is horizontal and j is upward. The acceleration is (0, −9.8). The black dot is the object. The orange arrow is the launch velocity and the teal arrow the velocity now, both to the same scale; the dashed lines are the components.

Move the time slider to follow the object.

  1. Set the launch height to 0. How does the time of flight compare with the time to the top? Why?
  2. Move the time slider. Which part of the velocity changes and which part stays the same? What in the acceleration explains this?
  3. Raise the launch point. Is the landing time still twice the time to the top? Is the landing speed still the launch speed?
  4. Choose "Speed and angle" with θ = 45° and add the wall. Change u until the object only just clears the wall. What is the least speed? Check it by solving for u.

Worked examples

Problems like the ones in class. Pick one, try it, then open the working.
Thrown horizontally from a cliff

A stone is thrown horizontally at 15 m s⁻¹ from the top of a cliff 30 m high, over level ground. Take \(\mathbf{i}\) as horizontal, away from the cliff, and \(\mathbf{j}\) as vertically up, with the origin at the foot of the cliff. Find (a) the time it takes to reach the ground, (b) how far from the foot of the cliff it lands, (c) its speed and its direction as it lands.

xy
Working
  1. Position

    \(\mathbf{r} = \begin{pmatrix} 15t \\ 30 − 4.9t^{2} \end{pmatrix}\)

    Horizontally the speed is constant. Vertically it starts with speed 0 and falls under gravity, starting at height 30.

  2. Time to land

    \(30 − 4.9t^{2} = 0\), \(t = 2.47\) s

    On the ground the height is zero. Take the positive solution.

  3. Distance

    \(x = 15 \times 2.474 = 37.1\) m

    Horizontal distance = horizontal speed × time.

  4. xy
    Velocity on landing

    \(\mathbf{v} = \begin{pmatrix} 15 \\ −9.8t \end{pmatrix}\), so \(\mathbf{v} = \begin{pmatrix} 15 \\ −24.2 \end{pmatrix}\) m s⁻¹

    Differentiate the position. Put the landing time into the vertical component.

  5. Speed and direction

    \(|\mathbf{v}| = \sqrt{15^{2} + 24.2^{2}} = 28.5\) m s⁻¹, \(\tan\theta = \dfrac{24.2}{15}\), \(\theta = 58.3\)° below the horizontal

    The vertical component is negative, so the stone is moving downwards.

Video walkthrough coming
Kicked from the ground at an angle

A ball is kicked from level ground with speed 22 m s⁻¹ at an angle of 35° above the horizontal. Take \(\mathbf{i}\) as horizontal and \(\mathbf{j}\) as vertically up, with the origin at the point of the kick. Find (a) the velocity of the ball at time \(t\) seconds, (b) the greatest height it reaches, (c) the distance from the kick to where it lands.

xy
Working
  1. Components

    \(\mathbf{v}(0) = \begin{pmatrix} 22\cos 35^\circ \\ 22\sin 35^\circ \end{pmatrix} = \begin{pmatrix} 18.02 \\ 12.62 \end{pmatrix}\)

    Horizontal part \(u\cos\theta\), vertical part \(u\sin\theta\). Calculator in degrees.

  2. Velocity

    \(\mathbf{v} = \begin{pmatrix} 18.02 \\ 12.62 − 9.8t \end{pmatrix}\) m s⁻¹

    Gravity changes only the vertical component.

  3. Top of the flight

    \(12.62 − 9.8t = 0\), \(t = 1.29\) s

    At the highest point the vertical velocity is zero.

  4. Greatest height

    \(y = 12.62(1.288) − 4.9(1.288)^{2} = 8.12\) m

    Put the time of the top into the vertical displacement.

  5. Range

    \(t_{land} = 2 \times 1.288 = 2.575\) s, \(x = 18.02 \times 2.575 = 46.4\) m

    On level ground the time up equals the time down. Horizontal distance = horizontal speed × total time.

Video walkthrough coming
Thrown from a height at an angle

A shot is released from a point 2 m above level ground with speed 14 m s⁻¹ at 40° above the horizontal. Take \(\mathbf{i}\) as horizontal and \(\mathbf{j}\) as vertically up, with the origin on the ground directly below the release point. Find (a) the time it takes to land, (b) the horizontal distance of the landing point from the origin, (c) the greatest height above the ground, (d) its speed and direction when it lands.

xyrelease
Working
  1. Position

    \(\mathbf{r} = \begin{pmatrix} 10.72t \\ 2 + 8.999t − 4.9t^{2} \end{pmatrix}\)

    The vertical position starts at 2, not 0.

  2. Time to land

    Polynomial solver: \(2 + 8.999t − 4.9t^{2} = 0\), \(t = 2.04\) s

    The other solution is negative: it is before the release.

  3. Distance

    \(x = 10.72 \times 2.037 = 21.8\) m

    Horizontal speed × time in the air.

  4. Greatest height

    \(8.999 − 9.8t = 0\), \(t = 0.918\), \(y = 2 + 8.999(0.9183) − 4.9(0.9183)^{2} = 6.13\) m

    Find the time of the top, then the height. Add the 2 m that it started with.

  5. Landing velocity

    \(\mathbf{v}(2.037) = \begin{pmatrix} 10.72 \\ 8.999 − 9.8(2.037) \end{pmatrix} = \begin{pmatrix} 10.72 \\ −11.0 \end{pmatrix}\)

    Put the landing time into the velocity.

  6. Speed and direction

    \(|\mathbf{v}| = 15.3\) m s⁻¹, \(\tan\theta = \dfrac{11.0}{10.72}\), \(\theta = 45.6\)° below the horizontal

    Its speed is greater than 14 m s⁻¹ because it lands lower than it started.

Video walkthrough coming
Does the ball clear the wall?

A ball is kicked from level ground with speed 20 m s⁻¹ at 30° above the horizontal, towards a wall 3 m high. The wall is 28 m away, measured along the ground from the kick. Take \(\mathbf{i}\) as horizontal and \(\mathbf{j}\) as vertically up, with the origin at the kick. (a) Find the height of the ball when it is above the wall. (b) Does the ball clear the wall? (c) Is the ball rising or falling as it passes the wall?

xykickwall
Working
  1. Position

    \(\mathbf{r} = \begin{pmatrix} 17.32t \\ 10t − 4.9t^{2} \end{pmatrix}\)

    Components: \(20\cos 30^\circ = 17.32\) and \(20\sin 30^\circ = 10\).

  2. Time at the wall

    \(17.32t = 28\), \(t = 1.617\) s

    Use the horizontal component to find when the ball is 28 m away.

  3. Height then

    \(y = 10(1.617) − 4.9(1.617)^{2} = 3.36\) m

    Put that time into the vertical displacement.

  4. xykickwall
    Compare

    \(3.36 > 3\)

    The ball is 0.360 m above the top of the wall, so it clears the wall.

  5. Rising or falling

    \(v_{y} = 10 − 9.8(1.617) = −5.84\)

    The vertical velocity is negative, so the ball is on its way down as it goes over.

Video walkthrough coming