Help differentiating energy wrt time.

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Homework Help Overview

The discussion revolves around differentiating an energy equation related to a mass-spring system to demonstrate equivalence with Newton's second law. The problem involves a mass suspended by springs, with the energy equation incorporating kinetic and potential energy terms.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss substituting velocity with the time derivative of position and express uncertainty about handling the spring energy terms. There are questions about the correct expressions for spring extensions and whether the springs have the same stiffness constant. Some participants suggest corrections to the energy equation and emphasize the importance of differentiating correctly.

Discussion Status

Some participants have provided suggestions and clarifications regarding the setup of the springs and the energy equation. There appears to be a productive exchange of ideas, with one participant indicating they have gained clarity after considering the feedback. However, there is no explicit consensus on all aspects of the problem.

Contextual Notes

Participants note potential typos in the energy equation and question the assumptions regarding the arrangement of the springs. There is also mention of the known distance between fixtures, which influences the deformation expressions.

caius
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Homework Statement



I have a problem where I have a mass suspended in a system of springs. I need to differentiate the equation wrt time so I can can show equivalence with Newton's second law.

The mass and springs are vertically aligned so the motion is in one dimension. The actual problem has several springs, but for simplicity I am describing a system with just two. The equation below I think shows the total energy of the system.

Homework Equations



E = 1/2 mv^2 + k(x-l)^2 + 2k(l-x)^2 -mgx

where m=mass, v= velocity, k= stiffness, x=current position and l=spring's natural length.

The Attempt at a Solution



I think the way to approach it is to substitute dx/dt in place of the velocity, however I can't see what to do with the spring parts.

I seem to have some kind of mental block on this, and it's very frustrating. Any assistance on how to approach it would be gratefully received!
 
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E = 1/2 mv^2 + k(x-l)^2 + 2k(l-x)^2 -mgx - don't think this is quite right

I am guessing that we have one spring above the mass and one below?

The terms for elastic spring energy are based on 1/2ke^2. Where e is spring extension.

Isn't the extension of the springs l+x and l-x?

Are both springs of the same stiffness constant k? Perhaps there is a typo here?

Make these corrections and multiply out brackets before differentiating.

Remember
[tex]\frac{d}{dt}v^2=2v\frac{dv}{dt}=2\frac{dx}{dt}a[/tex]
Where a is acceleration. So the kinetic energy term after differentiating will have ma in it, which is starting to look like N2L. It will also have dx/dt in it. All other terms of your equation will either go to zero because they are independent of t or be a multiple of dx/dt. So dx/dt will cancel throughout. This will leave terms that are all forces.
 
apelling said:
Isn't the extension of the springs l+x and l-x?
I don't see how it could be l+x. l-x and x-l make sense if the springs are in series with the endpoints fixed 2l apart, and x being the position of the join. But then, the expression simplifies to 3k(l-x)2.
 
Thanks for your suggestions. I think I have it now.

The lengths were the correct way round, but I didn't make it quite clear in the question I asked. The distance between the two fixtures is known, so the deformation can be expressed in relation to that.

The answer I got did end up as m.a equated with the spring forces according to Hooke's law and gravity which is what I needed.

It's amazing the difference a nights sleep makes.
 
haruspex said:
I don't see how it could be l+x. l-x and x-l make sense if the springs are in series with the endpoints fixed 2l apart, and x being the position of the join. But then, the expression simplifies to 3k(l-x)2.

I was thinking L was the extension of the springs when at equilibrium and x was the displacement from equilibrium. Anyhow it does not matter much since the constants drop out during differentiation.
 

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