PhMichael
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Homework Statement
So I have this standard problem of a cylinder rolling down an inclined plane, however, this time the plane itself is free to slide on the ground. I need to find the acceleration of that cylinder relative to the plane.
2. The attempt at a solution
[PLAIN]http://img801.imageshack.us/img801/14/rollingf.jpg
V / A - the velocity / acceleration of the plane relative to the ground.
v / a - the velocity / acceleration of the cylinder relative to the plane.
The velocity of the cylinder relative to the ground is:
\vec{u}=\vec{v}+\vec{V}=(vcos \beta -V) \hat{x} - (vsin \beta) \hat{y}
Momentum is conserved conserved in the \hat{x} direction so that:
0=-MV+m(v cos \beta -V) \to V=\frac{m}{M+m} v cos \beta
so the acceleration of the plane relative to the ground is:
A=\frac{dV}{dt}=\frac{m}{m+M}a cos \beta
About point P, we have:
\vec{\tau}_{P}=mR(g sin \beta + A cos \beta) \hat{z}
I_{P}\vec{\alpha}=(0.5MR^{2}+MR^{2})\vec{\alpha}=1.5MR^{2} \frac{a}{R}\hat{z}
Equating the last two equations while using the equation of A yields:
a=gsin\beta\left [ \frac{3}{2}-\left ( \frac{m}{m+M} \right )cos^{2}\beta \right ]
This answer is correct, however, I'm not sure whether what I did is kosher; to be more specific, is linear momentum conserved along the \hat{x} direction? are fictitious forces, like the one we have here on the cylinder as a result of the plane's acceleration, not treated as real forces so that eventhough they exist, we may still use the conservation of momentum principle?
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