What Is the Potential Energy at Point B?

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Homework Help Overview

The problem involves a 0.40-kg particle moving under a conservative force, with given potential energy at point A and work done as it moves to point B. The original poster notes the absence of a diagram, which they believe would clarify the situation.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the relationship between work, kinetic energy, and potential energy, with some suggesting that energy conservation principles apply. Questions arise about how to calculate kinetic energy at point B and the implications of conservative forces on potential energy changes.

Discussion Status

There is an ongoing exploration of the problem, with some participants providing insights into energy conservation and mechanical energy. Multiple interpretations of the work-energy relationship are being discussed, but no consensus has been reached on the best approach to solve the problem.

Contextual Notes

Participants express uncertainty about the necessity of a diagram and the implications of the conservative force on energy calculations. There is also a discussion about the assumptions regarding the nature of forces involved and their impact on potential and kinetic energy.

Yuravian
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Homework Statement


A 0.40-kg particle moves under the influence of a single conservative force. At point A where the particle has a speed of 10 m/s, the potential energy associated with the conservative force is +40 J. As the particle moves from A to B, the force does +25 J of work on the particle. What is the value of the potential energy at point B?

The problem, for me is that there is no diagram included on the homework sent out in the email from the professor and I think the proper problem would have had a diagram of the path. I may be wrong though.

Homework Equations


Well, this is clearly a work and kinetic energy problem, so:
[tex]W=\Delta U+\Delta K[/tex]
[tex]W=Fdcos\theta[/tex] (not sure if it applies here)
[tex]\Delta K=1/2mv^{2}_{o}-1/2mv^{2}_{f}[/tex]
[tex]\Delta U=mgh_{o}-mgh_{f}[/tex] (again, I don't think this applies)

The Attempt at a Solution


straighten out my variables:
[tex]v_o=10 m/s[/tex]
[tex]K_o=1/2mv^2_o=20 J[/tex]
[tex]U_o=40 J[/tex]
[tex]W=25 J=U_f-U_o+K_f-K_o[/tex]

So at this point, I do not have the acceleration of the particle (cannot find F or v final), and no information on the final state of the particle other than the amount of work done on it. Where should I go from here?
 
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Actually I don't think you need a diagram to solve this. Think about: if we assume that the energy is conserved in the system then the total energy is equal to the kinetic + potential energy. We know the potential energy at point a and can calculate the kinetic energy at point a as well...

It might be helpful to know that

[tex]W = \Delta K[/tex]
 
Last edited:
Sorry, I just cut that out. I mis-read the question. I still do not think it can be solved though.
 
qspeechc said:
Sorry, I just cut that out. I mis-read the question. I still do not think it can be solved though.

No, I really think it can be solved. You can find the total mechanical energy, and then find the kinetic energy at point b and from that find the potential at point b.
 
How would you find the kinetic energy at B?
 
At point A: [tex]KE = \frac{1}{2}mv^2 = \frac{1}{2}(0.40kg)(10\frac{m}{s})^2 = 20J[/tex]

[tex]E_{mec} = KE + U = 20J + 40J = 60J[/tex]

We know the work done from point A to B and
[tex]W = \Delta K = \frac{1}{2}m(v_f^2-v_o^2)[/tex]

We need to solve for the velocity of the particle at point B... we get:

[tex]v_{f}^2 = \sqrt{\frac{2W}{m}+v_o^2} = \sqrt{\frac{2(25J)}{0.40kg}+10\frac{m}{s}^2} = 15\frac{m}{s}[/tex]

So KE at B: [tex]\frac{1}{2}mv^2 = \frac{1}{2}(0.40kg)(15\frac{m}{s})^2 = 45J[/tex]

Then find the potential energy

[tex]U = E_{mec} - KE = 60J - 45J = 15J[/tex]
 
As Yuravian states, work is change in mechanical energy, that is
W = ∆KE + ∆U

Not:
W = ∆KE
as you have stated.
 
qspeechc said:
As Yuravian states, work is change in mechanical energy, that is
W = ∆KE + ∆U

Not:
W = ∆KE
as you have stated.

We're talking about a single conservative force acting on the particle. Conservative forces won't change the total amount of mechanical energy we have.

∆KE + ∆U = ∆E = W (by non conservative forces)
 
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So? Can a single conservative force not change the potential energy? What if I lift a bag of sand vertically in a vacuum?
 
  • #10
qspeechc said:
So? Can a single conservative force not change the potential energy? What if I lift a bag of sand vertically in a vacuum?

It will change the potential energy, but it will not change the total amount of energy in the system.
 
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  • #11
If I do work in lifting the bag of sand, initially at rest on the floor, can I not lift it vertically some distance AND give it some speed, so that now it has BOTH potential AND kinetic energy, where originally it had none?
 
  • #12
qspeechc said:
If I do work in lifting the bag of sand, initially at rest on the floor, can I not lift it vertically some distance AND give it some speed, so that now it has BOTH potential AND kinetic energy, where originally it had none?

Sure, but ∆KE = -∆U = W, U is going to be changing negatively since the work is in the opposite direction of the force of gravity. The total energy will still be 0.
 
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  • #13
Feldoh said:
At point A: [tex]KE = \frac{1}{2}mv^2 = \frac{1}{2}(0.40kg)(10\frac{m}{s})^2 = 20J[/tex]

[tex]E_{mec} = KE + U = 20J + 40J = 60J[/tex]

We know the work done from point A to B and
[tex]W = \Delta K = \frac{1}{2}m(v_f^2-v_o^2)[/tex]

We need to solve for the velocity of the particle at point B... we get:

[tex]v_{f}^2 = \sqrt{\frac{2W}{m}+v_o^2} = \sqrt{\frac{2(25J)}{0.40kg}+10\frac{m}{s}^2} = 15\frac{m}{s}[/tex]

So KE at B: [tex]\frac{1}{2}mv^2 = \frac{1}{2}(0.40kg)(15\frac{m}{s})^2 = 45J[/tex]

Then find the potential energy

[tex]U = E_{mec} - KE = 60J - 45J = 15J[/tex]

Ah, I see... I missed the part about the force being conservative. If a force is conservative, then W = ∆KE = -∆U, since E=KE+U and E doesn't change at all, right? so would it not be easier to simply say [tex]U_f = U_o+\Delta U = 40J - 25J = 15 J[/tex]?
 
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  • #14
Feldoh said:
Sure, but ∆KE = -∆U = W, U is going to be changing negatively since the work is in the opposite direction of the force of gravity. The total energy will still be 0.

Wait a minute. If your v is high and stays constant, wouldn't your U increase while K stayed constant? Correct me if I'm wrong, but if you lift a bag of sand, the force you put on it isn't conservative in the first place.
 
  • #15
Yuravian said:
Wait a minute. If your v is high and stays constant, wouldn't your U increase while K stayed constant? Correct me if I'm wrong, but if you lift a bag of sand, the force you put on it isn't conservative in the first place.

Oh I think he meant like throwing it upwards. I think you're right though the force of the push is not conservative...

Yuravian said:
Ah, I see... I missed the part about the force being conservative. If a force is conservative, then W = ∆KE = -∆U, since E=KE+U and E doesn't change at all, right? so would it not be easier to simply say [tex]U_f = U_o+\Delta U = 40J - 25J = 15 J[/tex]?

Haha, yeah your way sure beats mine :P
 

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