Work Done by Friction & Gravity on Incline: Explained

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SUMMARY

The discussion focuses on the work done by friction and gravity on an incline, specifically addressing the use of vertical displacement in the work done by gravity, represented by the formula ##W = -mgh##. Participants clarify that using the displacement in the direction of the force and the full force magnitude is equivalent to using the force component in the displacement direction. The inclined plane is identified as a simple machine that reduces the force needed to lift an object while increasing the distance moved. Key formulas discussed include ##W = F d \cos\theta## and ##W_{gravity} = -mg \cdot s \cos\alpha##.

PREREQUISITES
  • Understanding of basic physics concepts, particularly work and energy.
  • Familiarity with vector components and trigonometric functions.
  • Knowledge of inclined planes and mechanical advantage.
  • Proficiency in using formulas related to work, such as ##W = F d \cos\theta##.
NEXT STEPS
  • Study the principles of work and energy in physics, focusing on conservative forces.
  • Learn about the mechanics of inclined planes and their applications in real-world scenarios.
  • Explore the concept of mechanical advantage and how it applies to simple machines.
  • Investigate the differences between conservative and non-conservative forces in terms of work done.
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Students of physics, educators teaching mechanics, and engineers interested in the applications of inclined planes and work-energy principles.

simphys
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Homework Statement
You are a member of an Alpine Rescue Team. You must project
a box of supplies up an incline of constant slope angle a so that it reaches a
stranded skier who is a vertical distance h above the bottom of the incline.
The incline is slippery, but there is some friction present, with kinetic friction coefficient mk. Use the work–energy theorem to calculate the minimum speed you must give the box at the bottom of the incline so that it
will reach the skier. Express your answer in terms of g, h, mk, and a
Relevant Equations
##W = Fscos(alpha)##
where ##s=h/sin(alpha)##
So for the work done by the kinetic friction, the displacement along the incline is ##s## as given.
What I canNOT understand is why the displacement in the y-direction is used for the work done by gravity i.e. ##W = -mgh## where ##h## is the displacement in het y-direction. This instead of the displacement along the incline
This is complete bullshit, the work done on a force was supposed to be the component along the displacement wasn't it ?

Can someone explain that to me please? Thanks in advance
Edit: this was the answer from the book

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Last edited:
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Using the displacement in the force direction and the full force magnitude is completely equivalent to using the force component in the displacement direction and the full displacement.
 
Orodruin said:
Using the displacement in the force direction and the full force magnitude is completely equivalent to using the force component in the displacement direction and the full displacement.
What a disaster... of course, thanks a lot! it comes down to the same thing but a little bit of a different formula.
 
The formula is the same, ##W = F d \cos\theta##, the difference is in the interpretation of that formula in words.
 
Last edited:
simphys said:
What a disaster... of course, thanks a lot! it comes down to the same thing but a little bit of a different formula.
Our incline of constant slope angle works as a simple machine: the inclined plane.
##W{gravity}~=~-mgh~=~-mgscos\alpha##

Copied from
https://en.wikipedia.org/wiki/Inclined_plane#Inclined_plane_with_friction

"Moving an object up an inclined plane requires less force than lifting it straight up, at a cost of an increase in the distance moved. The mechanical advantage of an inclined plane, the factor by which the force is reduced, is equal to the ratio of the length of the sloped surface to the height it spans. Owing to conservation of energy, the same amount of mechanical energy (work) is required to lift a given object by a given vertical distance, disregarding losses from friction, but the inclined plane allows the same work to be done with a smaller force exerted over a greater distance.
...
The mechanical advantage MA of a simple machine is defined as the ratio of the output force exerted on the load to the input force applied. For the inclined plane the output load force is just the gravitational force of the load object on the plane, its weight Fw. The input force is the force Fi exerted on the object, parallel to the plane, to move it up the plane."
 
I take it ##\alpha## is supposed to be the angle between the incline and the horizontal direction.

When you write ##W=Fs\cos\alpha##, what does ##\alpha## represent? Is it the same angle as above? If so, are you sure it's the right angle to be using when calculating the work?
 
Orodruin said:
The formula is the same, ##W = F d \cos\theta##, the difference is in the interpretation of that formula in words.
I prefer the interpretation that treats the vectors on an equal footing, "The work done by a constant force is the product of three quantities: (a) the magnitude of the force vector; (b) the magnitude of the displacement vector; (c) the cosine of the angle between the two."
 
simphys said:
What a disaster... of course, thanks a lot! it comes down to the same thing but a little bit of a different formula.
In fact for a conservative force (which includes gravity and other forces but not friction) the work done is path independent. The gravitational work calculated along any path from 1 to 2 will produce the same number.
So you can just choose a horizontal segment (Wgrav=0) plus a vertical segment (Wgrav=-mgh) Have you not seen this in your text?
 

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