Does the Normal Force Do Work on an Inclined Plane?

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Homework Help Overview

The discussion revolves around the work done by the normal force on a mass moving down an inclined plane. The original poster questions the assertion in their textbook that the work done is zero, suggesting that the normal force should do work due to the mass's diagonal movement along the incline.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between the normal force and the displacement of the mass, questioning the conditions under which work is done. There are discussions about breaking down the normal force into components and considering the work done by each component.

Discussion Status

Some participants have provided clarifications regarding the nature of work as a scalar quantity, emphasizing that work does not have directional components in the way the original poster suggested. There is an acknowledgment of the need to consider the total work done by the normal force, but no consensus has been reached regarding the original question.

Contextual Notes

Participants are navigating misconceptions about the vector nature of work and its calculation, as well as the implications of the normal force being perpendicular to the displacement along the incline.

endaman95
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Homework Statement


Consider the mass m1 on a simple incline plane. It passes from point A downwards with the velocity v0 and stops at point B (still on the plane).

What is the work done by the normal force on mass m during the complete motion?

Homework Equations





The Attempt at a Solution


In my book it says zero but I don't think it is because the mass moves diagonally down which shows movement in x and y axis. Since the normal force acting on the mass isn't perpendicular to the y-axis movement. It should do work in the opposite direction. What do you think?
 
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endaman95 said:
In my book it says zero but I don't think it is because the mass moves diagonally down which shows movement in x and y axis. Since the normal force acting on the mass isn't perpendicular to the y-axis movement. It should do work in the opposite direction. What do you think?
Work it out. What are the vertical and horizontal components of the normal force and the displacement? Figure out the work done by each component and add together to get the total.

Your book is correct. Note that the normal force is perpendicular to the displacement down the incline. But you'll get the same answer when you break it into vertical and horizontal components.
 
You seem to be under the impression that there is a "work in the y-direction" and "work in the x-direction". There isn't. Work is a scalar quantity, not a vector.
 
Thank you. My misconception was thinking of it as a vectoral quantity. Now I get it.
 
HallsofIvy said:
You seem to be under the impression that there is a "work in the y-direction" and "work in the x-direction". There isn't. Work is a scalar quantity, not a vector.
You can certainly choose to look at the components of a force separately and consider the work done by each to get the total. (Of course you must add them up!)
 
HallsofIvy said:
Work is a scalar quantity, not a vector.
While it may not be a vector there can still be a direction associated with work in the same way that kinetic energy is also a scalar quantity but the velocity still has a direction associated with it. Direction in this sense then doesn't necessarily mean a vector but rather that it is a function of the x and y variables.
 
Last edited:
paisiello2 said:
While it may not be a vector there can still be a direction associated with work in the same way that kinetic energy is also a scalar quantity but the velocity still has a direction associated with it. Direction in this sense then doesn't necessarily mean a vector but rather that it is a function of the x and y variables.
To put some algebra around that notion, let the (normal) force vector be expressed as ##\vec F = F_x\vec i + F_y \vec j## and the displacement vector by ##\vec r = r_x\vec i + r_y \vec j##. Then the work done is ##\int \vec F.d\vec r = \int F_x.dx + \int F_y.dy##.
In the present problem, ##\int F_x.dx ## and ## \int F_y.dy## are equal and opposite, so cancel.
 

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