Block at rest on an inclined surface

Click For Summary

Homework Help Overview

The discussion revolves around a block at rest on an inclined surface, focusing on the forces acting on the block, including friction, weight components, and applied forces. Participants are exploring the conditions under which the block remains stationary and how to relate various forces to determine the range of angles for the incline.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants are attempting to clarify the direction of the friction force and its relationship to other forces acting on the block. Questions about the calculation of the normal force and the components of the applied force are raised. There is also a focus on understanding how to set up inequalities involving the forces to find the range of angles.

Discussion Status

The discussion is ongoing, with participants providing insights and corrections regarding the components of forces. Some have suggested drawing free-body diagrams to clarify the situation, while others are questioning the assumptions made about the forces involved. There is no explicit consensus yet, but several productive lines of inquiry are being explored.

Contextual Notes

Participants note the complexity of the problem due to the presence of multiple forces acting in different directions, including the weight of the block and the applied force. There is an emphasis on understanding the normal force and its role in the context of the inclined plane.

  • #31
Yes, that is all correct, except I do not understand this line:
Akash47 said:
there is still a case when Fcosθ=Wsinθ
In what sense is this a special case? Isn't it just encompassed by the range of values for which the system is static?
 
Physics news on Phys.org
  • #32
Oh! It's not a special case.When ##Fcosθ=Wsinθ##,then there is no friction force working.How will you explain it?
 
  • #33
Akash47 said:
Oh! It's not a special case.When ##Fcosθ=Wsinθ##,then there is no friction force working.How will you explain it?
What's to explain? If the net of the other forces tending to make the surfaces slide against each other is zero then there is no frictional force.
 
  • Like
Likes   Reactions: jbriggs444
  • #34
I was saying that there is a case ##θ=45^°## when also the block will not move and there will be no friction.And the range of the values of θ is##:tan^{-1}\frac{1-μ}{1+μ} ≤θ≤ tan^{-1}\frac{1+μ}{1-μ}##.And to get the value θ=45,you have to put μ=0 in either the lower bound or the upper bound.But can a static friction co-efficient of a surface ever
be zero(at least not in this problem where μ is clearly mentioned)?Then what is your answer to this?
Though the question asks for the range of values in terms of μ (which don't really need the value θ=45),I think the full solution also need the value ##θ=45^°##.
 
Last edited:
  • #35
Akash47 said:
I was saying that there is a case θ=45 when also the block will not move and there will be no friction.And the range of the values of θ is##: \frac{1-μ}{1+μ} ≤θ≤ \frac{1+μ}{1-μ}##.And to get the value θ=45,you have to put μ=0 in either the lower bound or the upper bound.But can a static friction co-efficient of a surface ever
be zero(at least not in this problem where μ is clearly mentioned)?Then what is your answer to this?
Though the question asks for the range of values in terms of μ (which don't really need the value θ=45),I think the full solution also need the value θ=45.
It is clear that ##\theta## = 45 degrees falls within the solution set regardless of the value of ##\mu##

You are going to need to write down some equations so that we can see where you are going wrong. It is pretty clear that those formulas for ##\theta## are not correct. For one thing, they give a result that is unitless, but you are using degrees, so ##\theta## should not be unitless.
 
  • #36
Sorry for that,I have edited my post.Now see it and clearly answer the questions.
 
  • #37
Akash47 said:
Sorry for that,I have edited my post.Now see it and clearly answer the questions.
Without having worked the problem your way, those formulas look plausible. But they go singular when ##\mu## = 1.

Hint: With ##\mu## = 1, the inclined plane could be vertical, the tangent would be infinite and the object would not fall. [Think of pressing a book against a wall to prevent its fall].

With ##\mu## > 1, is there still a limiting angle?

There is a different approach to the problem that removes the singularity. What if you started by combining W+F into one combined force and rotated your coordinate system by 45 degrees? [Don't forget that 45 degree offset when reporting your computed result]
 

Similar threads

  • · Replies 6 ·
Replies
6
Views
2K
Replies
43
Views
2K
  • · Replies 11 ·
Replies
11
Views
3K
Replies
11
Views
1K
  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 19 ·
Replies
19
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
24
Views
3K