The Mystery of Inclined Plane Motion: Analyzing a Block's Acceleration

AI Thread Summary
The discussion revolves around analyzing the motion of a block on an inclined plane fixed to a rotating turntable. Participants are trying to understand the components of the block's acceleration, particularly why the acceleration appears to be directed opposite to the position vector and the implications for the z-axis component. Clarifications are made regarding the definitions of the coordinate system, emphasizing the need to accurately define the radial and vertical components in relation to the wedge. There is debate about whether the vertical component of acceleration is zero, given that the block's position on the wedge remains constant. Ultimately, the focus is on applying Newton's laws to resolve the acceleration into its respective components.
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A wedge with face inclined at an angle theta to the horizontal is fixed on a rotating turntable. A block of mass m rests on the inclined plane and the coefficient of static friction between the block and the wedge is μ. The block is to remain at position R from the center of the turntable, as shown in the attachment. Find the components of the block's acceleration parallel and vertical to the inclined plane.

a=-Rω^(2)\hat{r}

I have been struggling to get to grips with this question for a while now. I don't understand how the acceleration is pointing in the opposite direction of the position vector r, which has a z axis component although there is no displacement in that direction. Have I interpreted the polar coordinates wrongly? Any insight would be greatly appreciated. Thanks.
 

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yeah \hat{r} is the unit vector in radial direction. So your problem is to find how much this given acceleration points(the projection of) parallel and vertical to the wedge i.e. change basis
Also you have to express omega as something you know a general wedge problem.
Edit:
The r coordinate points from the axis of revolution(z) and out to. Thats why it is negative, cause the block is accelerated in the opposite direction
And in fact there is an acceleration in z direction. Try to draw the situation where the polar coordinates(They look cylindrical to me) are defined by the axis in the middle.
 
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also omega is \omega = \dot{\theta} the azimutal angle differentiated in time.
 
Thanks for the reply. I still can't understand how there is an acceleration in the z direction. Surely its z coordinate does not change as its position on the wedge is locked?
 
No but try to be strict when defining your coordinate system. This pre-defined is seen from the bottom and close to the vertical axis. When you define yours you should try to get a usual centripetal acceleration. So the z-component is maybe zero? Which would make sense considering that the object dosen't accelerate vertical.
So my point is: Their definition looks like it is seen from the axis in the middle and your job is to use Newtons laws to find the components of a in 2 directions.
 
thanks I'm nearly there!
when they say vertical component of the inclined plane, do they mean perpendicular to it or parallel to the z-axis? sorry if this seems obvious but it's pretty vital to answering the question!
 
Sorry for the late answer, but vertical is parallel to their z-axis(probably also yours). Maybe it is 0 and maybe not.
 
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