Inclined plane with spring underneath.

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Homework Help Overview

The problem involves a mass on a frictionless inclined plane with a spring underneath. The mass is given as 2.5 kg, the incline angle is 40°, and the height is 1.6 m. The spring has an initial extension of 30 cm and is compressed by a maximum of 12 cm. The goal is to determine the spring constant "k".

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the conservation of energy principle, questioning how to apply it given the inclined plane's geometry. There is uncertainty about the correct value for "x" in the energy equations, with some suggesting it should be the compression of the spring while others consider the initial and final lengths of the spring.

Discussion Status

Participants are exploring different interpretations of the problem, particularly regarding the height measurement and the relationship between gravitational potential energy and the spring's compression. Some guidance has been offered about the height difference and the need to consider the geometry of the situation.

Contextual Notes

There is a discussion about the orientation of the spring and whether the height should be measured relative to the incline or from the ground. Participants are also clarifying the definitions of potential energy in this context.

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Homework Statement



A body of mass m = 2.5kg is on a frictionless inclined plane (by 40°). At an height of h = 1.6m.
On the bottom of the plane there's a spring, which at rest has an extension of 30cm.
If the spring is compressed maximum of 12cm, what's the "k" of the spring?

Homework Equations





The Attempt at a Solution



Alright, there is conservation of energy because there is no friction.
mgh = 1/2kx^2

But there is an inclined plane so ...
mg(h/sen40) = 1/2kx^2

Now, the only step I don't fully get, what is X?
I thought x would be:
30cm - 12cm = 18cm.
So I could solve for k.

Is this right? Thanks.
 
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Assuming that the spring is lying on the ground and not sitting up against the slope then the angle of inclination doesn't matter, all you need is
mgh = \frac{1}{2}kx^2
Where x is the distance it is compressed (given as 12cm in the problem)

As a side note I reread your problem and you may be correct in saying that the x is 18cm, I'm not exactly sure what your wording means.
 
It means that when it is not compressed, the spring has a length of 30cm's.
Then when the block pushes it, it's compressed of a maximum of 12 cm's.
Now I would like to know what I must plug into x.
 
A spring is comprensed or stretched along only one axis. That said, it seems that the confusion here is what must we use as x. If 12 cm (0.12 m) is the compressed lenght, then x = 0.12 m. But if 0.12 m is the final length of the spring, x would be instead 18 cm.
One question: is the spring lying along the inclined plane or is parallel to the floor at the bottom?
Note: you didn't have to use E = mg(h/sen 40°), since h must be and it is already parallel to g.
 
the spring would be perpendicular to the inclined plane, something like this (check attachment).

So, a question, when we have an inclined plane, and we want to find the potential energy.

mgh

h is always the height from the ground or it should be relative to the inclination of the plane?
 

Attachments

  • scar.png
    scar.png
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The height h doesn't depends of inclination; it is measured from the ground.
From the drawing you made, it is clear that not all gravitational potential energy goes into compressing the spring, if you take ground as a point of 0 gravitational potential energy. Try to find the difference in height between the upper point and the lower point (when the spring is compressed): that will give the amount of gravitational energy that goes in the spring.
Hint: draw a triangle whose hypotenuse is 18 cm at the position of the spring, in order to find the height of the lower point.
 
Last edited:
I don't think I follow.
 
To find the difference in height, try 1.6 m - (0.18 m) sen 40°. Calculate gravitational energy and equate it to elastic potential energy.
 

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