Question #49674

A tennis player wishes to return the ball so it just passes over the top of
the net at a point where the net is 1.0 m high. He can return the ball at a
speed of 14 ms-1
from a position that is 0.4 m vertically below the top of
the net and is 8.0 m from the point where he intends the ball to cross the
net.
a. At what angles to the horizontal could the player strike the ball in
order to do this?
b. In each case what will be the total horizontal distance travelled by
the ball before it strikes the ground on the other side of the net?
c. Without further calculation, sketch the trajectories in each case.
1

Expert's answer

2015-01-21T10:56:29-0500

Answer on Question#49674 - Physics - Mechanics - Kinematics - Dynamics

A tennis player wishes to return the ball so it just passes over the top of the net at a point where the net is H=1.0mH = 1.0\mathrm{m} high. He can return the ball at a speed of v0=14msv_{0} = 14\frac{\mathrm{m}}{\mathrm{s}} from a position that is Δh=0.4m\Delta h = 0.4\mathrm{m} vertically below the top of the net and is l0=8.0ml_{0} = 8.0\mathrm{m} from the point where he intends the ball to cross the net.

a. At what angles to the horizontal could the player strike the ball in order to do this?

b. In each case what will be the total horizontal distance travelled by the ball before it strikes the ground on the other side of the net?

c. Without further calculation, sketch the trajectories in each case.

Solution:

The initial position is h0=HΔh=0.6mh_0 = H - \Delta h = 0.6\mathrm{m} high. Assuming that the ball was struck at angle φ\varphi to the horizontal, dependences of the height hh and horizontal displacement ll of the ball on time are


{l=v0cosφth=h0+v0sinφtgt22\left\{ \begin{array}{c} l = v _ {0} \cos \varphi \cdot t \\ h = h _ {0} + v _ {0} \sin \varphi \cdot t - \frac {g \cdot t ^ {2}}{2} \end{array} \right.


When the ball passes over the net these equations give us the following


{l0=v0cosφtH=h0+v0sinφtgt22\left\{ \begin{array}{c} l _ {0} = v _ {0} \cos \varphi \cdot t \\ H = h _ {0} + v _ {0} \sin \varphi \cdot t - \frac {g \cdot t ^ {2}}{2} \end{array} \right.


Expressing tt from the first equation and substituting it into the second we obtain


{t=l0v0cosφH=h0+v0sinφl0v0cosφgl022(v0cosφ)2\left\{ \begin{array}{c} t = \frac {l _ {0}}{v _ {0} \cos \varphi} \\ H = h _ {0} + v _ {0} \sin \varphi \frac {l _ {0}}{v _ {0} \cos \varphi} - \frac {g \cdot l _ {0} ^ {2}}{2 (v _ {0} \cos \varphi) ^ {2}} \end{array} \right.


It's known that


1cos2φ=1+tan2φ\frac {1}{\cos^ {2} \varphi} = 1 + \tan^ {2} \varphi


So the second equation can be rewritten in the following way


H=h0+l0tanφgl022v02(1+tan2φ)H = h _ {0} + l _ {0} \tan \varphi - \frac {g \cdot l _ {0} ^ {2}}{2 v _ {0} ^ {2}} (1 + \tan^ {2} \varphi)


or


tan2φ2v02gl0tanφ+2v02Δhgl02+1=0\tan^ {2} \varphi - \frac {2 v _ {0} ^ {2}}{g \cdot l _ {0}} \tan \varphi + \frac {2 v _ {0} ^ {2} \Delta h}{g \cdot l _ {0} ^ {2}} + 1 = 0


Substituting all given parameters and assuming that g=10ms2g = 10\frac{\mathrm{m}}{\mathrm{s}^2} we obtain


tan2φ4.9tanφ+1.245=0\tan^2 \varphi - 4.9 \tan \varphi + 1.245 = 0


This equation has two roots


tanφ=[4.630.27]\tan \varphi = \begin{bmatrix} 4.63 \\ 0.27 \end{bmatrix}


Since we are only interested in angles which lie in the interval [0,π2]\left[0, \frac{\pi}{2}\right], we have only two possible angles


φ1=\atan4.63=77.8\varphi_1 = \atan 4.63 = 77.8{}^\circφ2=\atan0.27=15.0\varphi_2 = \atan 0.27 = 15.0{}^\circ


Let's first consider the case when φ1=77.8\varphi_1 = 77.8{}^\circ.

To find the total horizontal distance travelled by the ball before it strikes the ground we should find the time it took the ball to reach the ground (h=0h = 0). To do this we have to solve the second equation of the system (1) with respect to time tt.


h0+v0sinφ1tgt22=0h_0 + v_0 \sin \varphi_1 \cdot t - \frac{g \cdot t^2}{2} = 0


or


t22v0sinφ1gt2h0g=0t^2 - \frac{2 v_0 \sin \varphi_1}{g} t - \frac{2 h_0}{g} = 0


Substituting given parameters and φ1=77.8\varphi_1 = 77.8{}^\circ we obtain


t22.74t0.12=0t^2 - 2.74 t - 0.12 = 0


This equation has only one physical root (not negative)


t=2.78st = 2.78 \mathrm{s}


Using the first equation of the system (1) we obtain the total horizontal distance


L1=v0cosφ1t=8.3mL_1 = v_0 \cos \varphi_1 \cdot t = 8.3 \mathrm{m}


Let's now consider the case when φ2=15.0\varphi_2 = 15.0{}^\circ.

We have to solve a similar equation


t22v0sinφ2gt2h0g=0t^2 - \frac{2 v_0 \sin \varphi_2}{g} t - \frac{2 h_0}{g} = 0


Substituting given parameters and φ1=15.0\varphi_1 = 15.0{}^\circ we obtain


t20.72t0.12=0t^2 - 0.72 t - 0.12 = 0


This equation has only one physical root (not negative)


t=0.86st = 0.86s


Using the first equation of the system (1) we obtain the total horizontal distance


L2=v0cosφ2t=11.6mL_2 = v_0 \cos \varphi_2 \cdot t = 11.6m


**Answer:**

a. φ1=77.8\varphi_1 = 77.8{}^\circ

φ2=15.0\varphi_2 = 15.0{}^\circ

b. L1=8.3mL_1 = 8.3m

L2=11.6mL_2 = 11.6m

c.



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