Solving a Stationary Block on a Frictionless Wedge

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Homework Help Overview

The problem involves a block of mass m resting on a frictionless wedge of mass M, inclined at an angle theta. The task is to determine the conditions under which the block remains stationary relative to the wedge, both when the wedge is accelerating and when an external force F is applied to it.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss free body diagrams (FBD) and the forces acting on the block and wedge, questioning how horizontal acceleration affects vertical motion.
  • There are inquiries about the normal force and its relationship with the acceleration of the wedge.
  • Some participants attempt to derive equations based on Newton's laws for both vertical and horizontal components of forces.
  • Questions arise regarding the correct representation of forces and the components of the normal force.

Discussion Status

The discussion is ongoing, with participants exploring various interpretations of the forces involved. Some have provided guidance on how to approach the problem using Newton's laws, while others are clarifying the roles of different forces. There is no explicit consensus yet, but productive dialogue continues around the equations and concepts involved.

Contextual Notes

Participants are navigating the complexities of the problem, including the effects of acceleration and the definitions of forces in a non-horizontal setup. There are indications of confusion regarding the relationship between the normal force and the gravitational force acting on the block.

postfan
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Homework Statement


This is a 2 part question.

A block of mass m rests on a frictionless wedge that has an inclination of theta and mass M.
a) Find the acceleration of the wedge M to the right such that the block m remains stationary relative to the wedge.
c) You now find out that a force of magnitude F was exerted (say, by somebody's hand) on the wedge as shown in the picture below. What is the magnitude F for which the block m remains stationary relative to the wedge? Use m, M, g, and theta.


Homework Equations


F=ma


The Attempt at a Solution


I drew a FBD but I can't fathom how acceleration in the horizontal will cause a block not to move in the vertical.
 

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postfan said:
I drew a FBD but I can't fathom how acceleration in the horizontal will cause a block not to move in the vertical.
What force does the wedge exert on the block? How is that affected by the acceleration?

Do a FBD of the block.
 
The force is the normal force which is m*g*cos(theta) but I don't get how the acceleration affects it.
 
postfan said:
The force is the normal force which is m*g*cos(theta) but I don't get how the acceleration affects it.
Yes, the force is the normal force. But no, the normal force does not equal m*g*cos(theta) when the wedge is accelerating. (It does when the wedge is fixed.) The greater the acceleration, the harder the wedge presses against the block.

Just call the normal force "N" and apply Newton's laws to the block for vertical and horizontal components.
 
Is the normal force m*(g+a)*cos(theta)?
 
postfan said:
Is the normal force m*(g+a)*cos(theta)?

That would look right if g and a were in the same direction, but they're not. Stop guessing: resolve forces and apply ƩF=ma in the vertical and horizontal directions in the usual way. What equations do you get?
 
In the vertical I get mg-mg*cos(theta)=ma a=g-g*cos(theta).
In the horizontal I get m*g*sin(theta)=m*a*sin(theta) a=g.

Is that right?
 
postfan said:
In the vertical I get mg-mg*cos(theta)=ma a=g-g*cos(theta).
In the horizontal I get m*g*sin(theta)=m*a*sin(theta) a=g.

Is that right?
Again, just call the normal force "N" (or any symbol of your choice). Rewrite those equations.

What must be the acceleration in the vertical direction if the block is not to slide down the wedge?
 
In the vertical I get mg-N=ma a=(mg-N)/m.
In the horizontal I get m*g*sin(theta)=m*a*sin(theta) a=g.

Is that right?
 
  • #10
postfan said:
In the vertical I get mg-N=ma a=(mg-N)/m.
In the horizontal I get m*g*sin(theta)=m*a*sin(theta) a=g.

Is that right?
No. First, let's get the set of forces right.
1. List the forces, giving their directions.
2. Write out the horizontal and vertical components of each force.
Then, and only then, should you try to write out the equations.
 
  • #11
Iin the vertical you have the normal force . In the horizontal you have gravity and the force pushing the block (to have acceleration you need a force) Is that right?
 
  • #12
postfan said:
Iin the vertical you have the normal force .
A normal force means a force that is normal to (i.e. at right angles to) the surface. The surface is not horizontal, so the normal force is not vertical.
In the horizontal you have gravity
Last time I checked, gravity acts vertically.
and the force pushing the block (to have acceleration you need a force) Is that right?
Yes, F is horizontal.
 
  • #13
postfan said:
In the horizontal you have gravity and the force pushing the block (to have acceleration you need a force) Is that right?
Careful. The force pushing the block is the normal force. Only two forces act on the block.
 
  • #14
So in the vertical you have gravity and in the horizontal you have the force that is pushing the block. Is that right?
 
  • #15
NO. That's what Doc Al has been trying to get you to see. gravity is vertical but the normal force, due to the wedge, is NOT horizontal. It is normal to the surface of the wedge. Separate it into normal and horizontal forces.
 
  • #16
Ok so the the normal force is N*cos(alpha) and the horizontal force is N*sin(alpha). Is that right?
 
  • #17
postfan said:
Ok so the the normal force is N*cos(alpha) and the horizontal force is N*sin(alpha). Is that right?
Let me restate what I think you're trying to say:

The normal force is N. The vertical component of that force is N*cos(theta); the horizontal component is N*sin(theta).

Good. Keep going.
 
  • #18
Ok so from N2L the equations are N*sin(theta)=ma (x-axis) and N*cos(theta)-mg=0. Is that right?
 
  • #19
postfan said:
Ok so from N2L the equations are N*sin(theta)=ma (x-axis) and N*cos(theta)-mg=0. Is that right?
Yes, that's right.
 
  • #20
Ok so then the acceleration is (N*sin(theta))/m and the force is ((M+m)(N*sin(theta)))/m. Is that right?
 
  • #21
postfan said:
Ok so then the acceleration is (N*sin(theta))/m and the force is ((M+m)(N*sin(theta)))/m. Is that right?

Yes. Now use the vertical force equation to substitute for N.
 
  • #22
Ok, so N=mg/cos(theta) , hence a=mg/cos(theta)*sin(theta))/m which = g*tan(theta) and the force=(M+m)*g*tan(alpha). Is that right?
 
  • #23
When you solve for the acceleration, do not express it in terms of the unknown normal force.
 
  • #24
I did not express it in terms of the normal force.
 
  • #25
postfan said:
I did not express it in terms of the normal force.
Ah, OK.

postfan said:
Ok, so N=mg/cos(theta) , hence a=mg/cos(theta)*sin(theta))/m which = g*tan(theta) and the force=(M+m)*g*tan(alpha). Is that right?
Yes, that's correct now.
 
  • #26
Cool! Thanks for all your help!
 

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