Potential energy for the harmonic oscillator

In summary, the second derivative of (1/2)kx^2 at the equilibrium point is kb, which makes sense because as you move away from equilibrium the restoring force increases.
  • #1
CanIExplore
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0
Hey all,

In the classical harmonic oscillator the force is given by Hooke's Law,
F = -kx which gives us the potential energy function V(x)=(1/2)kx^2. Now I understand that the first derivative at the point of equilibrium must be zero since the slope at the point of equilibrium is zero. But what is the meaning of the second derivative at that point? Is it how fast the slope is changing? My professor says that it has to be positive or equal to zero but that for simple harmonic motion it is always positive. I don't see how you can have the first derivative of a function evaluated at some point be zero but the second derivative at the same point be nonzero.
 
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  • #2
CanIExplore said:
Now I understand that the first derivative at the point of equilibrium must be zero since the slope at the point of equilibrium is zero.
The slope of the potential energy function tells you the force, which you know must equal zero at equilibrium.
But what is the meaning of the second derivative at that point? Is it how fast the slope is changing?
Sure. Since slope relates to force, it's the rate of change of the force as you move past x = 0.
My professor says that it has to be positive or equal to zero but that for simple harmonic motion it is always positive.
That's true.
I don't see how you can have the first derivative of a function evaluated at some point be zero but the second derivative at the same point be nonzero.
Why do you think that? Plot the potential energy function and you get a parabola. The slope of the tangent to that curve happens to be zero at x = 0 (the first derivative is zero) but the slope certainly changes as you go from x < 0 to x > 0. The rate of change of the slope--the second derivative--is non-zero.
 
  • #3
Read the first couple of paragraphs of this page: http://www-users.math.umd.edu/~tjp/220%2002.2%20lecture%20notes.pdf
 
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  • #4
The slope of the potential energy function tells you the force, which you know must equal zero at equilibrium.

I forgot that the potential energy can be written as the gradient of the force, this helps in understanding what is going on physically. Thanks!

Why do you think that? Plot the potential energy function and you get a parabola. The slope of the tangent to that curve happens to be zero at x = 0 (the first derivative is zero) but the slope certainly changes as you go from x < 0 to x > 0. The rate of change of the slope--the second derivative--is non-zero.

Ahhh... I think I understand now. Before I was thinking that if I took the derivative at the equilibrium point that it would be zero and that the derivative of zero is zero. But I have to compute the second derivative of the function first and then evaluate it at the point of equilibrium correct?

Actually now that I think about it, if I take the second derivative of (1/2)kx^2 then you get kx, and plugging in a value of x taken to be the equilibrium point say x=b, you don't get zero, just some constant: kb. This would mean that the slope is zero since it's just a straight line which makes sense. But isn't it supposed to be zero? I'm confusing myself now, I'm forgetting my basic calculus.

Thanks for your quick reply by the way.
 
  • #5
CanIExplore said:
Actually now that I think about it, if I take the second derivative of (1/2)kx^2 then you get kx, and plugging in a value of x taken to be the equilibrium point say x=b, you don't get zero, just some constant: kb. This would mean that the slope is zero since it's just a straight line which makes s.ense. But isn't it supposed to be zero? I'm confusing myself now, I'm forgetting my basic calculus.
Careful. kx is the first derivative of (1/2)kx^2. And that equals zero at x = 0, the equilibrium point. For x = b ≠ 0, you'll get kb. Which should make sense, since as you move away from equilibrium, the restoring force increases. (The second derivative is just k, a constant.)
 
  • #6
Careful. kx is the first derivative of (1/2)kx^2. And that equals zero at x = 0, the equilibrium point. For x = b ≠ 0, you'll get kb. Which should make sense, since as you move away from equilibrium, the restoring force increases. (The second derivative is just k, a constant.)

OHH Ok now I really do get it. I was imagining a potential energy function that was symmetric about a point other than zero, for example the point x=b. But in that case the function would be different from (1/2)kx^2. My mistake.

Thanks!

Also thanks for the link it is a good review.

||SOLVED||
 

1. What is potential energy for the harmonic oscillator?

The potential energy for the harmonic oscillator is the energy that is stored in the system when the oscillator is displaced from its equilibrium position. It is a result of the restoring force that brings the oscillator back to its equilibrium position.

2. How is potential energy related to the harmonic oscillator's displacement?

Potential energy for the harmonic oscillator is directly proportional to the square of the displacement from the equilibrium position. This means that as the displacement increases, the potential energy also increases.

3. Can potential energy be negative for a harmonic oscillator?

Yes, potential energy for a harmonic oscillator can be negative. This occurs when the oscillator's displacement is greater than the equilibrium position, causing the restoring force to act in the opposite direction, resulting in a negative potential energy.

4. What is the relationship between potential energy and kinetic energy in a harmonic oscillator?

In a harmonic oscillator, the total energy is the sum of potential energy and kinetic energy. As the potential energy decreases, the kinetic energy increases, and vice versa. This relationship is known as the conservation of energy.

5. How does the potential energy for a harmonic oscillator change with changes in the spring constant or mass?

The potential energy for a harmonic oscillator is directly proportional to the square of the spring constant and the mass. This means that an increase in either the spring constant or the mass will result in an increase in potential energy.

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