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That is dimensionally wrong. You forgot something.Fibo112 said:the childs weight creates a torque of R/2*30kg * sin(b)
But please, let us do it the safe way, with free body diagrams, ΣF=ma etc.
That is dimensionally wrong. You forgot something.Fibo112 said:the childs weight creates a torque of R/2*30kg * sin(b)
yes I forgot gharuspex said:That is dimensionally wrong. You forgot something.
Right... and please see my edit above.Fibo112 said:yes I forgot g
Yes.Fibo112 said:Ok. So since the child remains motionless in an Inertial system we have a=0. The forces on the child are the Gravitational force, the normal force of the disc and the friction force of the disc. The component of the Gravitational force which is perpendicular to the disk will cancel out with the discs normal force. The remaining forces on the child are 30kg*g*sin(b) for the remaining gravitational force and a frictional force of equal magnitude and opposite direction to compensate the gravitational force. By Newtons third law the child enacts an equal and opposite force on the disk. The normal component causes no torque. The frictional component causes a torque of T= R/2 30kg*g*sin(b). This causes an angular acceleration of T/Moment of Intertia. The acceleration of the disk at the point of the child is R/2*T/Moment of inertia.?
as meaning relative to the tangential acceleration of the disc, not an acceleration of magnitude a relative to the reference frame of the disc. I think you have the right reading.Fibo112 said:positive y-direction with constant acceleration a relative to the disk
The question states that the child is to stay in the same place in the laboratory frame. That is enough to determine the force the child must exert on the disc, and the disc's consequent acceleration.Fibo112 said:I am still bothered by this questions notion of acceleration, it just doesn't make any sense to me to be talking about acceleration without a clear frame of reference as to where this acceleration is taking place...