Box Slipping and Tipping: Finding the Critical Force P

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Homework Help Overview

The problem involves a homogeneous box on a surface with static friction, where a force is applied at an angle to determine the conditions for slipping and tipping. Participants are analyzing the forces and torques acting on the box, particularly focusing on the role of the normal force and the moments about specific points.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the calculation of torque and the effects of the applied force on the box's stability. There are attempts to clarify the role of the normal force at different points and how it changes during tipping. Questions arise regarding the accuracy of the free-body diagram and the correct application of distances in torque calculations.

Discussion Status

The discussion is ongoing, with participants providing hints and corrections regarding the torque equation and the normal force. There is a recognition of differing interpretations of the normal force's behavior during tipping, and some participants suggest that the normal force at one point may become zero, while others challenge this notion. No consensus has been reached, but various perspectives are being explored.

Contextual Notes

Participants are navigating the complexities of the problem, including the implications of static friction and the geometry of the box. There is an emphasis on ensuring that all forces and moments are accurately represented in the analysis.

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Homework Statement



We have a homogenous box on a surface with static friction μ=0.5. We apply a force on the top of the box at an angle 30 degrees to the horizontal (see picture) and we want to know for what values of P does the box slip and tip. I have drawn a free-body diagram here of the situation:

http://i.imgur.com/jRh1zqa.png

The Attempt at a Solution



I have found that for slipping, P=0.448mg but I need help to determine P for the box to tip. If we take the moment(torque) around point C we get;

(Pcosθ)d+(Psinθ)2d+(N_B)2d-mgd=0 and hence P = (mg-2N_B)/(cosθ+2sinθ). How can I get rid of N_B in this case?
 
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Hint: you missed a torque in the torque equation. Just have a look at the FBD again.
 
darkxponent said:
Hint: you missed a torque in the torque equation. Just have a look at the FBD again.

Do you mean the friction force F_B? Because its line of action is parallel and pass through C and therefore no moment.
 
oh sorry i didn't see the mgd in equation. So you have taken all the Forces that give torque but still the equation is incorrect. Just see whether the perpendicular distances you have taken are correct?

Correcting it still won't give you the answer. Now focus on N_B. Hows is tipping going to effect it.
 
darkxponent said:
oh sorry i didn't see the mgd in equation. So you have taken all the Forces that give torque but still the equation is incorrect. Just see whether the perpendicular distances you have taken are correct?

Correcting it still won't give you the answer. Now focus on N_B. Hows is tipping going to effect it.

N_B=0 if it is tipping right? So P = (mg)/(cosθ+2sinθ)) which is correct.
 
No N_B is not zero when it is tipping. Normal becomes zero only when object leaves the surface. But the answer you got is still correct!. Now try too think what happens to N_B at tipping?
 
darkxponent said:
No N_B is not zero when it is tipping. Normal becomes zero only when object leaves the surface. But the answer you got is still correct!. Now try too think what happens to N_B at tipping?
I think Zeralda is defining NB as the normal force acting at B (and presumably has NC for a normal force at C, but that has no moment about C). With that definition, NB does go to zero.
 
haruspex said:
I think Zeralda is defining NB as the normal force acting at B (and presumably has NC for a normal force at C, but that has no moment about C). With that definition, NB does go to zero.

I don't know how to define normal at B and C separately. I thought N_B is the net normal at Base. And that what Zeralda has shown in the FBD( Normal is in the middle of the objects Base). I was trying to say that N_B shifts at point C at tipping and hence its moment is zero.

I also said Zeralda has done some mistake in taking the perpendicular distances. I was talking about N_B, it should be (N_B*d) not (N_B*2d). As we always take normal at the middle of the surface.

Correct me if i am wrong somewhere. I am just a student.
 
darkxponent said:
I don't know how to define normal at B and C separately. I thought N_B is the net normal at Base. And that what Zeralda has shown in the FBD( Normal is in the middle of the objects Base). I was trying to say that N_B shifts at point C at tipping and hence its moment is zero.

I also said Zeralda has done some mistake in taking the perpendicular distances. I was talking about N_B, it should be (N_B*d) not (N_B*2d). As we always take normal at the middle of the surface.

Correct me if i am wrong somewhere. I am just a student.
I based that on the diagram, which shows separate frictional forces at B and C. It also explains the use of 2d as the multiplier.
In practice, the normal force is distributed over the base. There are two ways to represent this (for the purposes of this question). We can do it as one force which acts in different positions according to the force P, or as two forces, a normal at each of B and C, that vary in relative magnitude. Either way, we agree that on point of tipping the normal force will be entirely at C.
 

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