The acceleration(a) of the suitcase along the slide is the
acceleration due to gravity times the sine of the incline angle,
or a=32.2*sin(30)=16.1f/s/s. Starting
with zero velocity, the suitcase distance(d) from the top of the
slide is
d=1/2*a*t2.
At d=20ft,
40=16.1*t2, or t2=2.48s2, or t=1.58s.
Neglecting the dimensions of the suitcase so we do not have to
deal with the rotation that occurs when the leading edge of the
suitcase clears the slide by 1/2 its length, the velocity at the
instant the suitcase leaves the slide is
16.1f/s/s*1.58s=25.44 f/s directed 30 degrees below
horizontal. The vertical component of that velocity is
Vv=25.44*sin(30)=12.72f/s.
The horizontal component is
Vh=25.44*cos(30)=22.03f/s.
The vertical distance(Dv) fallen in time, t, after leaving the
slide is
Dv=12.72*t+16.1*t2=4.
The time to hit the floor then is given by
4=12.72*t+16.1*t2, or 16.1*t2+12.72*t-4=0.
Solving the quadratic equation,
t=(-12.72(+/-)(12.722-4*16.1*(-4)).5)/32.2,
or
t=(-12.72(+/-)20.48)/32.2, or t=0.2425,
taking the positive value of t.
The total time to go from the top of the slide to the floor is
1.58+0.2425=1.82s.
The horizontal distance covered after leaving the slide will
be the horizontal velocity times the fall time or
Dh=22.03f/s*0.2425s=5.34ft.
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