sArGe99
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Homework Statement
Prism 1 with bar 2 of mass m placed on it gets a horizontal acceleration \omega directed to the left. At what maximum value of this acceleration \omega will the bar be still stationary relative to the prism, if the coefficient of friction between them k < cot\alpha
Homework Equations
mg sin \alpha - m \omega cos \alpha = Force trying to move the body along the prism.
k (m\omega sin \alpha + mg cos \alpha) = Frictional force.
The Attempt at a Solution
Since the prism is accelerating to the left, the bar experiences a pseudo force m\omega directed to the right. Resolving it has components
m \omega cos \alpha opposed to mg sin \alpha and the component m\omega sin \alpha acting along the direction of mg cos \alpha
At equilibrium, the frictional force equals the force which acts along the prism.
Equating, mg sin \alpha - m\omega cos\alpha = k (m\omega sin \alpha + mg cos \alpha)
Further simplifying,
\omega = \frac {g (sin \alpha - k cos \alpha)}{cos \alpha + k sin \alpha}
This is not the correct answer. Can you please point out where I've made a mistake?