Solve 2D Motion Q: Wiley E Coyote & Roadrunner

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The discussion revolves around a physics problem involving Wiley E. Coyote and the Roadrunner, focusing on 2D motion with constant horizontal acceleration. The key points include calculating the minimum speed the Roadrunner must maintain to reach the cliff before the Coyote, as well as determining where the Coyote lands after falling off the cliff and his velocity just before impact. The equations of motion are applied to derive time and velocity parameters, although some attempts to solve for time resulted in complications. The trajectory of the Coyote is analyzed in two parts: the initial fall and the subsequent motion with jet-powered skates. The conversation emphasizes the need to carefully apply kinematic equations to resolve the problem accurately.
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Homework Statement



wiley e coyote is out once more to try to capture the elusive roadrunner. the coyote wears a pair of acme jet powered roller skates, which provide a constant horizontal acceleration ac. the coyote starts off at rest D meters from the edge of a cliff at the instant the roadrunner zips by in the direction of the cliff. the cliff is H meters above the canyon floor. given [ac, D, H], determine:

if the roadrunner moves at constant speed, what should the roadrunners min speed be in order to reach the cliff before the coyote?

as usual the roadrunner is saved by making a sudden turn at the cliff. determine where the coyote lands in the canyon. (assume skates still on)

the velocity of the coyote just before hitting the canyon floor

Homework Equations



vx=v0x+at
x=x0+v0x*t+1/2*a*t^2
vx^2=v0x^2 + 2a(x - x0)

and y equivilents



The Attempt at a Solution




for a, i solved for time(t1) as t1= sqrt(2D/ac), which i then use for velocity of roadrunner(Vr) as Vr= D/sqrt(2D/ac)

for b & c, i used info from solving things in a as info to parameters:

from D to bottom of cliff

x0= D
x= D2
Vx0= acsqrt(2D/ac)
Vx= ?
a = ac

y0=0
y= H
Vy0 = 0
Vy = ?
a = g

t=t2

trying to use my y-based equations to solve for t2 results in them collapsing

Vy= 0 + gt2
Vy^2 = 0^2 + 2gH

g^2*(t2)^2 = 2gH

H = (g*t2^2)/2

(g*t2^2)/2 = 0 + 0 + 1/2*g*(t2)^2

everything cancels :<
 
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The trajectory will have two distinct parts. Find the velocity at the end of the first part. The second part, due to the jets still on, will be accelerated both horizontally and vertically. Use the final velocity of part one to find what is required.
 
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