Finding the Torque of Normal Force for a Sliding Block on an Inclined Plane

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SUMMARY

The discussion revolves around calculating the torque of the normal force acting on a cubical block sliding down a rough inclined plane at a uniform speed. The correct expression for the torque is established as \(\frac{1}{2}mga \sin(\alpha)\). Participants clarify that the normal force does not pass through the center of mass, which prevents the block from rolling. The balance of torques generated by the normal force and friction is crucial for understanding the dynamics of the sliding block.

PREREQUISITES
  • Understanding of torque and its calculation in physics
  • Familiarity with free body diagrams (FBD) and their construction
  • Knowledge of forces acting on inclined planes, including gravity and friction
  • Concept of uniform motion and its implications on forces
NEXT STEPS
  • Study the principles of torque in rigid body dynamics
  • Learn how to construct accurate free body diagrams for complex systems
  • Explore the effects of static and kinetic friction on motion
  • Investigate the conditions for rolling versus sliding motion in physics
USEFUL FOR

Students of physics, particularly those studying mechanics, educators teaching inclined plane problems, and anyone interested in the dynamics of rigid bodies in motion.

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Homework Statement



A cubical block of mass 'm' and edge length 'a' slides down a rough inclined plane of inclination alpha radian with a uniform speed. Find the torque of the normal[/color] force acting on the block about its center.

On the back of the book answer is \frac{1}{2}mga sin(alpha)
2. The attempt at a solution

I think the question is wrong. Am i correct?
The torque due to normal should zero since line of action of normal force makes zero angle with center.
this torque(as in answer) is of torque due to friction.

Is all the things i write here are correct
 
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The question is not wrong. Here is why.

I am sure you have drawn a free body diagram. Look at the (components of) forces along the incline: There is friction uphill and gsinθ downhill. They are equal and opposite because the speed is uniform and the acceleration is zero. This means that they form a couple. Couples exert the same torque regardless of reference point. So if the normal force exerts no counter-torque, how come the block is sliding and not rolling downhill like a die?
 
kuruman said:
The question is not wrong. Here is why.

I am sure you have drawn a free body diagram. Look at the (components of) forces along the incline: There is friction uphill and gsinθ downhill. They are equal and opposite because the speed is uniform and the acceleration is zero. This means that they form a couple. Couples exert the same torque regardless of reference point. So if the normal force exerts no counter-torque, how come the block is sliding and not rolling downhill like a die?
You are correct but the only force i can think of responsible for non rolling of this box is normal reaction. it is always perpendicular to plane so it must be in left with respect to center of mass of block(See attachemtn i draw a rough figure). am i correct?
 

Attachments

Correct. The normal force shifts off center just enough to make the net torque zero. If it didn't, the block would tumble which is not what's happening. So now you want to balance the torque generated by the couple with the counter-torque generated by the normal force.
 
kuruman said:
Correct. The normal force shifts off center just enough to make the net torque zero. If it didn't, the block would tumble which is not what's happening. So now you want to balance the torque generated by the couple with the counter-torque generated by the normal force.

Oh wow what a question. This is first time when i found that normal is not passing through center.
Is the free body diagram i draw(attachment in my last post) is correct?
In fbd ,backward force is friction ,normal to plane is normal reaction and forward one is due to gravity.
 
The FBD needs to be drawn a bit more carefully. The block needs to be a cube of side a, gsinθ must act at the center of mass and static friction must be drawn on the surface of the incline directed uphill. Call x the offset of the normal force from the center and find what x should be so that the torques are balanced.
 
kuruman said:
The FBD needs to be drawn a bit more carefully. The block needs to be a cube of side a, gsinθ must act at the center of mass and [size=+2]static friction[/color][/size] must be drawn on the surface of the incline directed uphill. Call x the offset of the normal force from the center and find what x should be so that the torques are balanced.
what static friction. I think it should be kinetic friction.
I have done question thanks yaar. I take lowest point on the cube as axis of rotation and did it.
 
Yes, kinetic friction of course. "Static" was a typo.
 

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