Crispy Vegetable Spring Rolls | Vegetable Roll Recipe | Easy Snacks Recipe #Shorts

Consider the situation in which one end of a massless spring of spring constant k is connected to a cylinder of mass m and the other to a rigid support. When cylinder is given a gentle push in horizontal direction it starts oscillating on the rough horizontal surface. During the oscillation cylinder rolls without slipping. When calculated, motion of cylinder is found to be S.H.M. with time period T=2pisqrt((3m)/(2K)) and equation of SHM is x=Asinomegat , where symbols have their usual meaning. At a distance x_(1) from the equilibrium position, kinetic energy of the oscillating system becomes equal to potential energy then, x_(1) is equal to:

A batsman hits a cricket ball which then rolls on a level ground. After covering a short distance, the ball comes to rest. The ball slows to a stop because (a) the batsman did not hit the ball hard enough, (b) velocity is proportional to the force exerted on the ball, (c ) there is a force on the ball opposing the motion ,(d) there is no unbalanced forcr on the ball, so the ball would want to come to rest.

Consider the situation in which one end of a massless spring of spring constant k is connected to a cylinder of mass m and the other to a rigid support. When cylinder is given a gentle push in horizontal direction it starts oscillating on the rough horizontal surface. During the oscillation cylinder rolls without slipping. When calculated, motion of cylinder is found to be S.H.M. with time period T=2pisqrt((3m)/(2K)) and equation of SHM is x=Asinomegat , where symbols have their usual meaning. At a distance x_(1) from the equilibrium position, kinetic energy of the oscillating system becomes equal to potential energy then, x_(1) is equal to: Q The equation which correctly shows the variation in friction as a function of time is-

Consider the situation in which one end of a massless spring of spring constant k is connected to a cylinder of mass m and the other to a rigid support. When cylinder is given a gentle push in horizontal direction it starts oscillating on the rough horizontal surface. During the oscillation cylinder rolls without slipping. When calculated, motion of cylinder is found to be S.H.M. with time period T=2pisqrt((3m)/(2K)) and equation of SHM is x=Asinomegat , where symbols have their usual meaning. At a distance x_(1) from the equilibrium position, kinetic energy of the oscillating system becomes equal to potential energy then, x_(1) is equal to: Q The minimum value of coefficient of friction such that the cylinder does not slip on the surface is: