How much time do I have to catch a coin?

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SUMMARY

The discussion centers on the physics of a coin's motion as perceived from two different frames of reference: a stationary observer (Philipp) and a moving observer. Philipp asserts that the coin's initial velocity is zero, leading to a misunderstanding of kinetic energy and distance traveled. The resolution reveals that while acceleration and time are consistent across frames, the distance the coin travels must account for the relative motion, resulting in the equation ##\frac 12 l + vt## in the moving frame. This clarifies the relationship between the two perspectives and confirms the equivalence of the equations.

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Lotto
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Homework Statement
When riding up the inclined moving walkway of inclination ##α## and length ##l## a coin drops out of Philipp’s pocket when he is exactly in the middle of it. It falls into one of the grooves on the walkway and starts rolling down without slipping. How much time does Philipp have to catch the coin before it falls under the bottom edge of the walkway? The velocity of the moving walkway is ##v##.
Relevant Equations
I would use an euqation for a rotational kinetic energy ##\frac 12 I{\omega}^2## and an equation for a transfer kinetic energy ##\frac 12 mv^2##. ##I=\frac 12 mR^2##.
I am a bit confused with velocities in this problem. From Philipp's view, the coin's initial velocity is zero, so its transfer kinetic energy is also zero. When I am standing on a non-moving ground, is the coin's initial velocity ##v## in direction the walkway is moving? But won't I get then different times?

From Philipp's view: ##\frac 12 l=\frac 12 at^2##
From my view: ##\frac12 l=\frac 12 at^2-vt##

Where do I do a mistake?
 
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There are four quantities there. You've assumed correctly that ##a## and ##t## are the same in both frames. And, that ##v## is different in the two frames (##v = 0## in Philipp's frame). What about ##l##? Is that the same in both frames?
 
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PeroK said:
There are four quantities there. You've assumed correctly that ##a## and ##t## are the same in both frames. And, that ##v## is different in the two frames (##v = 0## in Philipp's frame). What about ##l##? Is that the same in both frames?
Now I understand, in Philipp's frame, the total way the coin must travel is ##\frac 12 l+vt##, so then the equations are equivalent.
 
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