A daring 510-N swimmer dives off a cliff with a running horizontal leap, as shown in Fig. E3.10. What must her minimum speed be just as she leaves the top of the cliff so that she will miss the ledge at the bottom, which is 1.75 m wide and 9.00 m below the top of the cliff?

A daring 510-N swimmer dives off a cliff with a running horizontal leap, as shown in Fig. E3.10.  What must her minimum speed be just as she leaves the top of the cliff so that she will miss the ledge at the bottom, which is 1.75 m wide and 9.00 m below the top of the cliff?



SOLUTION
Place your frame of reference at the edge of the cliff where the -y-direction points downward.

The moment the swimmer takes the leap it becomes a projectile. Specifically, it is half of a parabolic path thus at max height the following applies:

$x=1.75m$ and $y=9.00m$
$v_{0y}=0$
$a_x = 0$
Using the equation, $v_x=v_{0x}+a_xt=v_{0x}+0$
$v_x=v_{0x}$

$a_x=0$  and $a_y=-g$
At the point of origin $x_0=y_0=0$

Since -y direction is pointed below then $y=-9.00m$ and $x=1.75 \ m$ then you may solve using the equation $x=x_0+v_{0x}t+\frac{1}{2}a_xt^2$  or $y=y_0+v_{0y}t+\frac{1}{2}a_yt^2$.

Let us start with using the x-variable.
$x=x_0+v_{0x}t+\frac{1}{2}a_xt^2$
$x=0+v_{0x}t+0$

so

 $v_{0x}=v_x=\frac{x}{t}$   [equation 1]

Let us find for time t, using
$y=y_0+v_{0y}t+\frac{1}{2}a_yt^2$
$y=0+0+\frac{1}{2}a_yt^2$

$t=\sqrt{\frac{2y}{-g}}$
$t=\sqrt{\frac{2(-9.00m)}{-9.8m/s^2}}$
$t= 1.36 s$

Substitute our time t=1.36 seconds to equation 1
 $v_{0x}=\frac{x}{t}$
 $v_{0x}=\frac{1.75m}{1.36s}$
$v_{0x}=v_x=1.29 \ m/s$

Thus, the swimmer must have a minimum speed of at least 1.29 m/s in order not to die from crashing on the ledge.

Reference: Young, H. D. et al. 2012. Sear’s and Zemansky’s University Physics with Modern Physics. NY: Pearson Education Inc.