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A ski jumper travels down a slope and leaves
the ski track moving in the horizontal direc-
tion with a speed of 28 m/s as in the figure.
The landing incline below her falls off with a
slope of 0 = 36º.
The acceleration of gravity is 9.8 m/s.

Respuesta :

Question seems to be missing. Found it on google:

a) How long is the ski jumper airborne?

b) Where does the ski jumper land on the incline?

a) 4.15 s

We start by noticing that:

- The horizontal motion of the skier is a uniform motion, with constant velocity

[tex]v_x = 28 m/s[/tex]

and the distance covered along the horizontal direction in a time t is

[tex]d_x = v_x t[/tex]

- The vertical motion of the skier is a uniformly accelerated motion, with initial velocity [tex]u_y = 0[/tex] and constant acceleration [tex]g=9.8 m/s^2[/tex] (where we take the downward direction as positive direction). Therefore, the vertical distance covered in a time t is

[tex]d_y = \frac{1}{2}gt^2[/tex]

The time t at which the skier lands is the time at which the skier reaches the incline, whose slope is

[tex]\theta = 36^{\circ}[/tex] below the horizontal

This happens when:

[tex]tan \theta = \frac{d_y}{d_x}[/tex]

Substituting and solving for t, we find:

[tex]tan \theta = \frac{\frac{1}{2}gt^2}{v_x t}= \frac{gt}{2v_x}\\t = \frac{2v_x}{g}tan \theta = \frac{2(28)}{9.8} tan 36^{\circ} =4.15 s[/tex]

b) 143.6 m

Here we want to find the distance covered along the slope of the incline, so we need to find the horizontal and vertical components of the displacement first:

[tex]d_x = v_x t = (28)(4.15)=116.2 m[/tex]

[tex]d_y = \frac{1}{2}gt^2 = \frac{1}{2}(9.8)(4.15)^2=84.4 m[/tex]

The distance covered along the slope is just the magnitude of the resultant displacement, so we can use Pythagorean's theorem:

[tex]d=\sqrt{d_x^2+d_y^2}=\sqrt{(116.2)^+(84.4)^2}=143.6 m[/tex]