Block and acceleration of wedge

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Homework Help Overview

The problem involves a block resting on a wedge inclined at an angle, with friction between the block and the wedge. The wedge is subjected to horizontal acceleration, and the task is to determine the minimum acceleration required for the block to remain stationary on the wedge without sliding.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the forces acting on the block, including normal force, friction, and gravity. There is uncertainty about the physical reasoning behind the derived expression for minimum acceleration. Questions arise regarding the direction of acceleration and the choice of coordinate axes. The distinction between static and kinetic friction is also explored.

Discussion Status

Participants are actively questioning the assumptions made in the problem setup and the implications of the derived equations. Some guidance has been offered regarding the physical conditions necessary for the block to remain stationary, and there is an ongoing exploration of the relationship between friction and acceleration.

Contextual Notes

There is a need to clarify the conditions under which the friction force is at its maximum and the implications of the coefficient of friction in the context of the problem. The discussion highlights potential ambiguities in the problem statement and the assumptions regarding the direction of forces.

Mr Davis 97
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Homework Statement


A block rests on a wedge inclined at angle ##\theta##. The coefficient of friction between the block and plane is ##\mu##. The wedge is given a horizontal acceleration ##a##. Assuming that ##\tan \theta > \mu##, find the minimum acceleration from the block to remain on the wedge without sliding

Homework Equations


Newton's second law
Law of static friction

The Attempt at a Solution


So essentially, I feel as though I have the correct solution, but I am not sure why it is the solution, physically.

So we have three forces acting on the block. the normal force, friction, and gravity.
If we define our coordinate system so that the y-direction is up and the x-direction is down, then we have the following equations:

y-direction: ##N \sin \theta + f \sin \theta - mg = 0##
x-direction: ##N \sin \theta - f \cos \theta = ma##

then
##N \cos \theta + f \sin \theta = mg##

Since ##\tan \theta > \mu##
we know that ##f = \mu N##

Then
##N (\cos \theta + \mu \sin \theta) = mg##
##N (\sin \theta - \mu \cos \theta) = ma##

##\displaystyle a = \frac{g(\sin \theta - \mu \cos \theta)}{\cos \theta + \mu \sin \theta}##

I think that this is the expression for the minimum, but I am not sure why this is the minimum. What is the condition that makes this expression the minimum, rather than just some acceleration?
 
Last edited:
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In what direction is the acceleration? Horizontal could be to the left or to the right. This will affect whether the friction is up the incline or down the incline. However, there are two coefficients of friction, static and kinetic. Which one is equal to tanθ and which one should appear in the answer? How did you choose your coordinate axes? I cannot tell from the equations you show.
 
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The friction in this case would be static. Also, acceleration is to the right, so right is positive and up is positive. The friction will be towards the top of the inclined plane.
 
Which way is downhill for the incline? To the right or to the left?
 
To the right
 
Mr Davis 97 said:
Assuming that ##\tan \theta = \mu##, find the minimum acceleration from the block to remain on the wedge without sliding
Did you mean to type "Assuming that ##\tan \theta > \mu## ...?
 
TSny said:
Did you mean to type "Assuming that ##\tan \theta > \mu## ...?
Oops, yes.
 
So essentially, I feel as though I have the correct solution, but I am not sure why it is the solution, physically.
It's not surprising, your working does not seem to involve anything physical. The maths needs to be motivated from your understanding of the physics... this also helps you check your answer.
You should make a statement at the start about the physical conditions needed for the block to not slide down the wedge (hint: talk in terms of the sum of forces).

If I define x to be horizontal, and y upwards, and do my working in the lab frame, then to stop the block falling I need to provide an upwards force equal and opposite gravity. That way, provided there was no initial vertical component, the only non-zero acceleration will be horizontal. I can do this by directly pushing upwards on the block, with force mg, and so have no net acceleration at all ... but that option is not available ... instead I am forced to push on the block at an angle... that help?

This is the same sort of physics as a sailboat tacking at an angle to the wind.
 
I assume that when the problem says "the weight is given a horizontal acceleration a" this means that a horizontal force F is acting on the block. This force is necessary since the block is initially at rest. You need to include that force in your equations because ma is not a force. Also, since the block is moving, which of the two coefficients of friction do you think should appear in the equations? That's why I asked which one is given. Finally, you need to consider that the acceleration has both an x and a y component in the horizontal-vertical coordinate system.
 
  • #10
To understand why your answer gives you the minimum acceleration, you need to understand why you wrote ##f = \mu N## for the friction force. Under what condition does this formula give the static friction force?
 
  • #11
TSny said:
To understand why your answer gives you the minimum acceleration, you need to understand why you wrote ##f = \mu N## for the friction force. Under what condition does this formula give the static friction force?
##f = \mu N## when the static friction force is at a maximum, and relative motion ensues, right?
 
  • #12
Mr Davis 97 said:
##f = \mu N## when the static friction force is at a maximum
Yes
and relative motion ensues, right?
Relative motion need not happen, but ##f = \mu N## does indicate that the object is "on the verge of slipping".
 

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