A counterintuitive Laws of Motion problem

In summary: But if you push the box at an angle relative to the floor, your push will be greater at the corners than in the middle. The reason is that the line of action of the force is not the same at the corners as it is in the middle.
  • #1
Differentiate it
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Homework Statement
No friction, massless string, massless pulley and wedge M is not fixed, pulley is attached to M.
Apply Newton's 2nd law on (Mass M + pulley) in Horizontal and Vertical directions.
My question: When I was watching this on YouTube, the teacher summed the forces as usual(I've added a picture). But there is a force of tension acting on the top right of wedge, so wouldn't that create a torque... Or something? What force counters that torque? And why can we just sum the forces as usual rather than thinking about the torques?
Also, I've added an image(blue ink) of how the forces kinda look like on the (Mass M + pulley) system
Relevant Equations
F = ma
Screenshot_20220828-172557~2.jpg
Screenshot_20220828-173636~2.jpg
n.jpg
 
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  • #2
Differentiate it said:
... But there is a force of tension acting on the top right of wedge, so wouldn't that create a torque... Or something? What force counters that torque? And why can we just sum the forces as usual rather than thinking about the torques?
There are two opposing torques about the bottom right edge of the wedge: one from the weights of the block and the wedge and another from the resultant of the tension at the axis of the pulley.
Simplification of the problem, I guess, assuming the wedge is long enough not to tip over.
 
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  • #3
Lnewqban said:
There are two opposing torques about the bottom right edge of the wedge: one from the weights of the block and the wedge and another from the resultant of the tension at the axis of the pulley.
Simplification of the problem, I guess, assuming the wedge is long enough not to tip over.
Even then, is it ok to just sum the forces as is? Also, I don't know if this is a stupid question.. but if a force(like friction) doesn't like, point through the center of mass of an object, why do we sum it as a regular force? And tension here, why are we summing it as a regular force rather than... you know, torque, or something?
 
  • #4
Differentiate it said:
Even then, is it ok to just sum the forces as is? Also, I don't know if this is a stupid question.. but if a force(like friction) doesn't like, point through the center of mass of an object, why do we sum it as a regular force? And tension here, why are we summing it as a regular force rather than... you know, torque, or something?
Ok so, is it just for simplicity that they didn't consider any torques?
 
  • #5
Differentiate it said:
Even then, is it ok to just sum the forces as is? Also, I don't know if this is a stupid question.. but if a force(like friction) doesn't like, point through the center of mass of an object, why do we sum it as a regular force? And tension here, why are we summing it as a regular force rather than... you know, torque, or something?
Forces sum the same regardless of their application point. Then you generally have torque balance to consider but that is a separate issue. You consider all for es in the force balance and the torques of all forces in the torque balance. You do not add torques with forces.
 
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  • #6
Differentiate it said:
Ok so, is it just for simplicity that they didn't consider any torques?
Probably. What was the original question,?
 
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  • #7
Orodruin said:
Forces sum the same regardless of their application point. Then you generally have torque balance to consider but that is a separate issue. You consider all for es in the force balance and the torques of all forces in the torque balance. You do not add torques with forces.
I know that we don't add torques with forces, but could you please elaborate on your first sentence? And being realistic, friction also generates a torque which is countered by the normal force. In such a case, we sum the forces as usual. But these forces are causing torques, so how do sum them as regular forces?
 
  • #8
Differentiate it said:
Even then, is it ok to just sum the forces as is? Also, I don't know if this is a stupid question.. but if a force(like friction) doesn't like, point through the center of mass of an object, why do we sum it as a regular force? And tension here, why are we summing it as a regular force rather than... you know, torque, or something?
The problem stated no friction.
Forces alone induce linear movement of the center of mass; therefore, you can assume all are applied to the center of mass.
Forces combined with their respective levers induce rotation; therefore, the location of the tail of the vector that represents each force respect to the fulcrum or pivot is important.
 
  • #9
Lnewqban said:
There are two opposing torques about the bottom right edge of the wedge: one from the weights of the block and the wedge and another from the resultant of the tension at the axis of the pulley.
You left out the normal force from the ground.
Differentiate it said:
could you please elaborate on your first sentence?
Vectors have magnitude and direction. Forces are vectors, but a force also has "line of action". For purposes of linear acceleration of the mass centre of a body, the line of action is irrelevant. You just sum the forces as vectors in the usual way.
But for rotational acceleration about the mass centre you need to add the torques those forces exert about the mass centre. These will depend on by how much the force's line of action misses the mass centre.

Here's a common source of confusion. Consider pushing a box along a smooth floor. If you push square on in the middle of one face you get a certain acceleration. If instead you push in the same direction but near one corner of the box it will spin but have a much smaller linear acceleration. How come you pushed just as hard but got less linear acceleration?
Answer is that you may feel you pushed as hard but the force you applied was less. It feels as hard because you are having to accelerate your arm/ body more to keep up.
 

FAQ: A counterintuitive Laws of Motion problem

1. What is a counterintuitive Laws of Motion problem?

A counterintuitive Laws of Motion problem is a scenario that challenges our common understanding of Newton's laws of motion. It may involve objects moving in unexpected ways or defying the laws of physics.

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