Calculating weights on a slope using virtual work.

In summary, the conversation discusses how to find the weight W of a cart on an inclined plane using the principle of virtual work. The given solution involves using the formula ∫Fdh = 0 for virtual displacement dh in statics, and F_p = W cos \theta for the part of the weight of the cart parallel to the slope. The conversation also includes attempts at solving the problem using forces and virtual work, and a discussion on finding the proportionality constant for the virtual work solution.
  • #1
albertrichardf
165
11

Homework Statement


A cart on an inclined plane is balanced by the weight w. All parts have negligible friction. Find the weight W of the cart using the principle of virtual work. Picture of set-up is attached.

Homework Equations


[tex] ∫Fdh = 0 [/tex] for virtual displacement dh in statics
[tex] F_p = W cos \theta [/tex] the part of the weight of the cart parallel to the slope
[tex] ∑F = 0 [/tex]
[tex] W = 4w/sin\theta [/tex]
This is the given solution, by the book.

The Attempt at a Solution


I tried two ways to get the solution: virtual work and forces but I got stuck in the virtual work solution, and I did not get the right answer with forces. So here is the force analysis first:

There are two pulleys in the diagram: one attached to the slope at the bottom, holding w, and the other attached at the top holding W. Let's call the one holding W P, and the other p. The tension in P must be such that it balances the parallel component of W, as given by the formula in Relevant equations. Let's call that tension T.
The perpendicular component of W can be ignored because it is balanced by the normal force. Because P supports p, the downwards force on p must be equal to T.

I assumed that both p and P are massless. Then the force on p is w, plus the pull of the slope on the other side. Since the strings in p are not moving, the pull of the slope must equal that of w. The downwards force on p is the sum of the two, namely 2w. This must equal T, and since T is the parallel component of W, by replacing I end up with:

[tex] 2w = W sin \theta [/tex]
Which is missing a factor of 2 to get the correct answer. Where did I miss that factor?

To apply the principle of virtual work, I let w fall a distance equal to the height of the slope, h. Then the point of the slope attached to p will rise by h, and the point attached to P rises by a h cos(theta). If P rises by h cos(theta), the string holding p will lengthen by h cos(theta), so the cart moves along the hypotenuse by this distance. The slope rotates around the point without any pulley by theta.
I drew two triangles to represent the slope. In the rotated one, I drew another triangle to figure out the height difference, and it was proportional to h. I then used the change in height of the pulley to calculate the change in height due to the pulley pulling the cart. Or rather I tried. I have absolutely no idea of how to do that because it does not form a triangle. Of course, I could calculate the height change again using proportionality, but then I end up with two proportionality constants and I have no idea of how to find them. Anyone can help me? Is my approach correct, and if so how do I calculate the change in height for W? If not what would be the correct approach, that is, what do I vary to apply the virtual work? Also why is my Force analysis missing a factor of 2? Thank you for answering the questions.
 

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  • #2
Albertrichardf said:
The tension in P must be such that it balances the parallel component of W
Draw a free body diagram for the pulley attached to the cart.
(Not sure what you mean by "tension in P". P is a pulley, with one string attached and one around it. Which string has the "tension in P"?
 
  • #3
the tension in the rope around the highest pulley must be 2w , so the pull on the cart must be 4w
 
  • #4
Is it 2w because there are two strings holding back the cart? If so, then I got it, thank you.
I still need to solve this with virtual work though.
Any ideas of how I could use virtual work to solve this?
 
  • #5
Albertrichardf said:
Any ideas of how I could use virtual work to solve this?
You have to work out the change in height of w for a small change in height of W (or vice versa).
 
  • #6
I tried dropping w and going through the calculations, (there are in the original post), but I'm getting stuck because I need the proportionality constant, which is dependant on the horizontal position of W and I can't find it. Any ideas on how I could find it? Thanks
 
  • #7
Albertrichardf said:
I tried dropping w and going through the calculations, (there are in the original post), but I'm getting stuck because I need the proportionality constant, which is dependant on the horizontal position of W and I can't find it. Any ideas on how I could find it? Thanks
If the cart moves a distance s up the slope, how much does it rise in the process?
 
  • #8
It should rise a distance s sin ø from trig.
However, in doing so, the string attached to the cart must shorten by s, and conversely, the string holding the other pulley should lengthen by s. The pulley holding the weight w is lowered by s as well. Because of this the slope will rotate anticlockwise by a certain amount, and the weight W will fall a little because of this. I'm having difficulty computing by how much the weight will fall. I set up similar triangles to calculate the drop in height, but I can't calculate the proportionality constant. How could I proceed with this?
 
  • #9
Albertrichardf said:
the string attached to the cart must shorten by s
You mean the string that goes around the pulley attached to the cart?
There are two portions to that string parallel to the slope, one above the pulley and one below. Which portion will shorten by s?
 
  • #10
Both I would think, because they would have to cover less distance to the cart, and since there must be tension in them, they must be taut, but I am not sure. Does it matter though? Because the one below the pulley won't do any work right? The length on top will have to decrease anyway because otherwise there is no tension
 
  • #11
Albertrichardf said:
Both I would think
Right. So if the cart moves distance s, how much rope that was parallel to the slope no longer is?
Albertrichardf said:
the one below the pulley won't do any work
At the moment we're just trying to figure out how far things move. We'll deal with work later.
 
  • #12
2s I would think, since it would be s for each string, one above the pulley, and the one below. I'm not sure if I understood your question well though. I'm supposing you mean the amount of string in all that moves out of the way. But since only the upper half of the string is attached to the pulley holding w, w would drop by only s as well.
 
  • #13
Albertrichardf said:
2s I would think, since it would be s for each string, one above the pulley, and the one below
Right, the total length of string parallel to the slope has reduced by 2s. Where has it all gone?
 
  • #14
I think the string holding the pulley holding w increases by 2s. It's hard to tell what would happen to the string below the pulley, but I believe it should run across the pulley attached to the cart, then the one holding the string attached to the cart, so that the string holding the pulley holding w increases by s, and since I'm shortening the string above the pulley as well by s, the overall increase in length would be 2s.
 
  • #15
Albertrichardf said:
the string holding the pulley holding w increases by 2s
The string as a whole does not change length, but yes, the vertical portion, from the top pulley to the lower pulley, would increase by 2s.
Not sure about the rest of what you wrote in that post, but I think you have the idea.

We have established that the lower pulley descends by 2s, yes? There is a string running over that pulley, with two vertical portions. One portion is fixed to the ground. If the pulley descends 2s, what happens to the length of that portion of string? Where does it go?
 
  • #16
Never mind what I wrote. Just my ramblings about how I calculated that 2s.
As to the string attached to the ground, I think it decreases by 2s. If the pulley is lowered, the string attached to the ground goes slack since it cannot move. If it goes slack there can't be any tension, and if there is no tension, w falls. It will fall until the string is taut again.

The string is taut again if w falls by 2s. So w falls by 4s in all, and that's the solution.

Thanks a lot for taking the time to help me. I know it was long, several days in fact, and I am not easy to deal with. Thank you for bearing with me and guiding me through the solution.
 

FAQ: Calculating weights on a slope using virtual work.

How do you calculate weights on a slope using virtual work?

To calculate weights on a slope using virtual work, you first need to find the forces acting on the object. Then, you can use the formula W = Fd, where W is the weight, F is the force, and d is the displacement. Make sure to take into account the angle of the slope in your calculations.

What is virtual work in the context of calculating weights on a slope?

Virtual work is a method used in physics and engineering to calculate the work done by forces on a system. It involves using the principle of conservation of energy to calculate the work done by a virtual displacement, which is an imaginary displacement that does not actually occur.

Why is virtual work useful for calculating weights on a slope?

Virtual work allows for the calculation of work done by forces on a slope without physically moving the object. This is especially useful in situations where the object is too heavy or difficult to move, or when the slope is too steep to measure with traditional methods.

What are some common applications of calculating weights on a slope using virtual work?

Calculating weights on a slope using virtual work is commonly used in engineering and construction to determine the load capacity of structures on a slope. It is also used in physics experiments to analyze the effects of forces on objects on an inclined plane.

Are there any limitations to using virtual work for calculating weights on a slope?

Virtual work is based on the assumption that the slope is frictionless and that the forces acting on the object are conservative. This may not always be the case in real-world scenarios, so it is important to consider potential limitations when using virtual work to calculate weights on a slope.

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