Understanding Normal Force on an Inclined Plane: Pushing vs. Carrying a Mass

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Discussion Overview

The discussion revolves around the differences in forces required when pushing versus carrying a mass up an inclined plane at constant velocity. Participants explore the implications of normal force in both scenarios, considering factors such as friction and mechanical advantage.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions whether there is a difference in the force needed when pushing versus carrying a mass up an incline.
  • Another participant states that pushing a mass up a frictionless incline requires a force of mgsinθ, while carrying it requires supporting the full weight, mg.
  • It is noted that the normal force exerted by the incline acts perpendicular to the surface, and when pushing, this force is referred to as the reaction force.
  • A participant proposes that when pushing, the reaction force is mgcosθ, while carrying the mass requires a total force of mgcosθ + Mgsinθ, suggesting a paradox.
  • Some participants clarify that the work done against gravity is the same regardless of the method, but the distance and force exerted differ.
  • There is a discussion about the reaction force when carrying the mass, with some participants asserting that it is provided by the person rather than the incline.
  • Concerns are raised about the conditions of friction and acceleration, with participants seeking clarification on how these factors influence the forces involved.
  • A participant emphasizes that the force required varies depending on whether one is pushing or carrying the mass, with pushing being more efficient in terms of force exerted.
  • There is mention of the mechanical advantage provided by the incline, allowing less force to be applied when pushing compared to lifting directly.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the forces involved in pushing versus carrying a mass on an inclined plane. The discussion remains unresolved, with differing interpretations of the normal force and the implications of friction.

Contextual Notes

Participants highlight the importance of assumptions regarding friction and acceleration in their arguments, indicating that the discussion's conclusions depend on these conditions.

Donald K
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Is there any difference in the force I need to apply between pushing and carrying a mass upward along an inclined plane with a constant velocity ?

I'm puzzled with the normal force of the mass at the inclined plane. When I push up a mas, the normal force of it is exerted by the inclined plane. If I carry it, the normal force is exerted by me.

Thanks!
 
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Not sure I quite understand the question. If you're pushing a mass up a frictionless incline, then you only need to push a fraction of the weight (mgsinθ). If you are carrying it up an incline (with friction, otherwise you won't be able to walk), then you must support the full weight. OK. What's the issue?
 
The push of the plane on the mass is sometimes called the reaction of the plane on the mass. If there is no friction, this reaction will be normal to the plane. Hence it is usually called the 'normal force'. This is the force with which the plane pushes on the mass.
 
Assume there is no friction.

When I push up a mass up the inclined plane ,the reaction force (mgcosθ) is offered by the plane. The force I need to apply is Mgsinθ, <mg.

If I carry the mass, (e.g. I put it above my head) the reaction force is provided by me.

The total force I need to provide is mgcosθ + Mgsinθ which is > mg.

Is it a paradox?
 
Donald K said:
The total force I need to provide is mgcosθ + Mgsinθ which is > mg.
Those components are perpendicular; they must be added as vectors. They add to mg.
Is it a paradox?
No paradox. The work you need to do against gravity to raise the object a certain height is the same. With the incline, since you exert less force, the distance you have to push is greater. (Allowing you to exert less force is the benefit of using an incline.)
 
Thanks!

I know the work done is path independent.

But how about the mgcosθ ( the reaction force) if I carry it (in my hands / put it on my head)

If I carry the mass in my hands, the reaction force exerted by the incline is ( my mass +m)cosθ.

The reaction force I need to keep the mass from falling down my hand is mgcosθ, is it right?

So the total force I need to spend (mgcosθ + mgsinθ) is greater at the incline if I carry the mass in my hands?
 
Donald K said:
Thanks!

I know the work done is path independent.

But how about the mgcosθ ( the reaction force) if I carry it (in my hands / put it on my head)

If I carry the mass in my hands, the reaction force exerted by the incline is ( my mass +m)cosθ.
So both you and the object are on the frictionless incline now? (What's preventing you from sliding down?) If so, the normal force exerted by the incline will be (M + m)cosθ. So?

The reaction force I need to keep the mass from falling down my hand is mgcosθ, is it right?
If you are holding the mass in your hand, and it's not accelerating, then you must be exerting a force of mg on it to support it. If you are sliding down the incline as you hold the mass, then you only exert a force of mgcosθ on it.

So the total force I need to spend (mgcosθ + mgsinθ) is greater at the incline if I carry the mass in my hands?
I'm still not understanding your point. If you are holding the mass as you both slide down a frictionless incline, then the force you exert on the mass is as outlined above.
 
Assume constant velocity. There is no acceleration and friction on the ramp.

The force needed to push up the incline is mgsinθ which is smaller than directly raising up , i.e., mg. This is mechanical advantage of the incline.



But how about the reaction force component mgcosθ if I hold the mass? If I hold it, it is offered by me rather than the incline surface.

It means the total force I need to spend is more. i.e. mgcosθ + mgsinθ

Hence, the ramp can save your force only if you pushing up the mass (the mgcosθ is done by the incline), not carrying it.

The force needed to handle a mass up a ramp varies on your lifting method. If you hold it
by your arms, you spend more. If you just push it up, it's saving your force.
 
Donald K said:
Assume constant velocity. There is no acceleration and friction on the ramp.
Still confusing. Friction? Yes or no?

If the object is being slid up a frictionless incline at constant velocity, then something is pushing it along.

The force needed to push up the incline is mgsinθ which is smaller than directly raising up , i.e., mg. This is mechanical advantage of the incline.
OK.

But how about the reaction force component mgcosθ if I hold the mass? If I hold it, it is offered by me rather than the incline surface.
Describe this situation. You are now on the frictionless incline holding the mass? What's pushing you up the incline?

It means the total force I need to spend is more. i.e. mgcosθ + mgsinθ

Hence, the ramp can save your force only if you pushing up the mass (the mgcosθ is done by the incline), not carrying it.

The force needed to handle a mass up a ramp varies on your lifting method. If you hold it
by your arms, you spend more. If you just push it up, it's saving your force.
Are you comparing:
- the force needed to push an object up a frictionless incline (= mgsinθ)
to
- the force needed to carry an object as you walk up an incline (with friction) (= mg)

If so, then sure, carrying an object up a ramp requires more force.

(There's no conservation law for force.)
 
  • #10
of course: as log as the inclined plane is not vertical...
that's one reason the wheel (as "wagon wheel") is so useful.

push,carry,roll will each, in general, require a different force from you.
 

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