A wooden block of mass $M$ resting on a rough horizontal surface is pulled with a force $F$ at an angle $\phi $ with the horizontal. If $\mu $ is the coefficient of kinetic friction between the block and the surface, then acceleration of the block is
$\frac{F}{M}\left( {\cos \,\phi + \mu \,\sin \,\phi } \right) - \mu g$
$F\,\sin \,\phi /M$
$\mu F\,\cos \,\phi $
$\mu F\,\sin \,\phi $
A block of mass $5\, kg$ is on a rough horizontal surface and is at rest. Now a force of $24\, N $is imparted to it with negligible impulse. If the coefficient of kinetic friction is $0.4$ and $g = 9.8\,m/{s^2}$, then the acceleration of the block is ........ $m/s^2$
The limiting friction between two bodies in contact is independent of
As shown in the figure a block of mass $10\,kg$ lying on a horizontal surface is pulled by a force $F$ acting at an angle $30^{\circ}$, with horizontal. For $\mu_{ s }=0.25$, the block will just start to move for the value of $F..........\,N$ : $\left[\right.$ Given $\left.g =10\,ms ^{-2}\right]$
The coefficient of friction $\mu $ and the angle of friction $\lambda $ are related as
Static friction between two surfaces