Potential energy and energy conservation problem

In summary: The right side is the total energy of the object just as it meets the spring when.....when the object has not met the spring yet and is travelling at a constant speed? Shouldn't it be 1/2mv^{2} instead of 1/2mv^{2} because the object's speed is constant?Yes, that is correct. The object is moving at a constant speed initially, so the kinetic energy is (1/2)mv2. After the object has compressed the spring, it has stopped moving and all of its initial kinetic energy has gone into the potential energy of the spring. The work done by friction is also added to this because it is a non-conservative force
  • #1
kyin01
47
0

Homework Statement


2-5.png



Homework Equations



K[tex]_{1}[/tex]+U[tex]_{1}[/tex] +W[tex]_{nc}[/tex] =K[tex]_{2}[/tex] + U [tex]_{2}[/tex] (The subscript coding is not working right, but they ARE suppose to be subscripts and nothing is squared)

Work on the spring = .5kx[tex]_{2}[/tex] - .2kx[tex]_{2}[/tex] (final minus initial)

The Attempt at a Solution


I didnt use the 1st equation because this problem doesn't involve any up and down movements (y direction / same potential all over).

So I tried the 2nd but because to net work is 0 both x (distance) become 0 also and I can't have any way of solving for k. They don't tell us how much it compressed so I can't make a new final / initial point.

What am I missing?
 
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  • #2
kyin01 said:

Homework Statement


2-5.png



Homework Equations



K[tex]_{1}[/tex]+U[tex]_{1}[/tex] +W[tex]_{nc}[/tex] =K[tex]_{2}[/tex] + U [tex]_{2}[/tex] (The subscript coding is not working right, but they ARE suppose to be subscripts and nothing is squared)
It is much better (and easier) to put an entire equation in LaTex, not parts of it. Here, you subscripts look like superscripts because the "bases" of the standard text and LaTex are different. Much better is
[tex]K_1+ U_1+ W_{nc}= K_2+ U_2[/tex]

Work on the spring = .5kx[tex]_{2}[/tex] - .2kx[tex]_{2}[/tex] (final minus initial)
What is x here?

The Attempt at a Solution


I didnt use the 1st equation because this problem doesn't involve any up and down movements (y direction / same potential all over).

So I tried the 2nd but because to net work is 0 both x (distance) become 0 also and I can't have any way of solving for k. They don't tell us how much it compressed so I can't make a new final / initial point.

What am I missing?
It's hard to tell because you haven't said what the "x" in your formula represents. Also the friction force is equal to the coefficient, [itex]\mu[/itex], times the speed isn't it? If x is the greatest compression of the spring, then the work done by friction, which is the integral of kv(t), plus the work done by the spring to stop the object must equal the kinetic energy of the object initially. Of course, you get the work from the spring back again during the "recoil". If the object stops at x= 0, then the loss of energy to friction must be equal to the initial kinetic energy of the object. That will depend upon the distance required for the greatest compression of the spring which, in turn, tells you k.
 
  • #3
HallsofIvy said:
It's hard to tell because you haven't said what the "x" in your formula represents. Also the friction force is equal to the coefficient, [itex]\mu[/itex], times the speed isn't it? If x is the greatest compression of the spring, then the work done by friction, which is the integral of kv(t), plus the work done by the spring to stop the object must equal the kinetic energy of the object initially. Of course, you get the work from the spring back again during the "recoil". If the object stops at x= 0, then the loss of energy to friction must be equal to the initial kinetic energy of the object. That will depend upon the distance required for the greatest compression of the spring which, in turn, tells you k.

Sorry, X is the distance compressed on the spring
and I thought the friction force is equal to the [itex]\mu[/itex] times the normal force?
 
  • #4
Okay, that's one kind of friction force. If that's what you were given, then that's what you should use.

Initially, the object has speed v and so kinetic energy (1/2)mv2. In compressing the spring a distance X, the object will have increased the potential energy of the spring (1/2)kX2 (integral of kx from 0 to X). The friction force is mg[itex]\mu[/itex] and so in distance X will have done work mg[itex]\mu[/itex]X on the object. If it comes to a halt in that distance, all of the object's kinetic energy must have gone into the potential energy of the spring or lost to friction: (1/2)kx2+ mg[itex]\mu[/itex]X= (1/2)mv2. That's a quadratic equation for X.

Any energy lost in compressing the spring is regained when it extends again. The energy lost to friction, however is the same moving in both directions so the total energy lost= total energy lost to friction= 2(mg[itex]\mu[/itex]X. If the object stops at the same position at which it initially met the spring, that must be equal to the initial kinetic energy: 2mg[itex]\mu[/itex]X= (1/2)mv2. Since X will depend upon k, you can solve that for k.
 
  • #5
What equation did you use to get (1/2)kx2+ mg[itex]\mu[/itex]X= (1/2)mv2

I understand how you got the (1/2)kx2 (because you took the sum of each force during the spring compression) and I also under the kinetic energy but what equation did you use to put them together like that
 
  • #6
"Conservation of Energy", of course. The right side is the total energy of the object just as it meets the spring (kinetic energy only since it has not yet started to compress the spring). The left side is the total energy of the object at maximum spring compression (potential energy only since now the velocity is 0) plus energy lost to friction.
 
  • #7
HallsofIvy said:
"Conservation of Energy", of course. The right side is the total energy of the object just as it meets the spring (kinetic energy only since it has not yet started to compress the spring). The left side is the total energy of the object at maximum spring compression (potential energy only since now the velocity is 0) plus energy lost to friction.

So just to clarify
You used the [tex]K_{1}[/tex]+[tex]U_{1}[/tex]+[tex]W_{nc}[/tex]=[tex]K_{2}[/tex]+[tex]U_{2}[/tex]

Except in this case because it is not gravatational potential it is elastic so the U (potential energy) in this case is 1/2k[tex]x^{2}[/tex] right?
And [tex]W_{nc}[/tex] is the total non conservative forces such as friction?


If that is the case, why did you say the right side is the total energy of the object just as it meets the spring when in the problem that was the initial starting point (in the equation the right side is the 2nd point)? Are we allowed to change the points freely?
 
  • #8
is that right?
 
  • #9
"Conservation of energy" means that the total energy- potential energy, kinetic energy and energy lost to friction, is the same at any two points.
 
  • #10
Ok so what you just said made sense. So next I tried to do the problem again by choosing my points at when it first touch the spring and just before it decompresses (like what you had set up), my following equation I had this

using [tex]K_{1}[/tex]+[tex]U_{1}[/tex]+[tex]W_{nc}[/tex]=[tex]K_{2}[/tex]+[tex]U_{2}[/tex]

1/2m[tex]v^{2}[/tex] + 0 + xmg[tex]\mu[/tex] = 0 + 1/2k[tex]x^{2}[/tex]

On the left side
When it hits the spring there is 0 potential because it has not yet compress the spring and it still remains on a horizonal surface. It has a kinetic energy and friction force
On the right side
I have 0 kinetic with potential energy.

So solving for K i get

[tex]\frac{mv^{2}+xmg\mu}{x^{2}}[/tex]

But according to the answer it does not depend on the variable X (distance compressed by spring)
 
Last edited:

1. What is potential energy?

Potential energy is the energy that an object possesses due to its position or configuration. It is stored energy that has the potential to be converted into other forms of energy, such as kinetic energy.

2. How is potential energy related to energy conservation?

Potential energy is a form of energy that is conserved in a closed system. This means that the total potential energy in a system remains constant, as long as there are no external forces acting on the system.

3. What are some examples of potential energy?

Some common examples of potential energy include a stretched rubber band, a compressed spring, an object at a height, and a charged battery. These objects have stored energy that can be released and converted into other forms of energy.

4. How is potential energy calculated?

The formula for calculating potential energy is PE = mgh, where m is the mass of the object, g is the acceleration due to gravity, and h is the height of the object. This formula is based on the gravitational potential energy of an object.

5. What is the relationship between potential energy and kinetic energy?

Potential energy and kinetic energy are two forms of energy that are interrelated. Potential energy can be converted into kinetic energy, and vice versa. For example, when an object falls from a height, its potential energy is converted into kinetic energy as it gains speed. Similarly, when a car brakes, its kinetic energy is converted into heat energy, reducing its speed and potential energy.

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