Help differentiating energy wrt time.

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SUMMARY

The discussion centers on differentiating the total energy equation of a mass-spring system with respect to time to demonstrate equivalence with Newton's second law. The total energy equation is given as E = 1/2 mv^2 + k(x-l)^2 + 2k(l-x)^2 - mgx, where m is mass, v is velocity, k is spring stiffness, x is the current position, and l is the spring's natural length. Participants clarified the correct expressions for spring extensions and emphasized the importance of correctly substituting dx/dt for velocity during differentiation. Ultimately, the solution confirmed that the mass's acceleration equates to the spring forces according to Hooke's law and gravity.

PREREQUISITES
  • Understanding of Newton's second law of motion
  • Familiarity with Hooke's law and spring mechanics
  • Knowledge of differentiation in calculus
  • Basic principles of energy conservation in mechanical systems
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  • Study the principles of energy conservation in mass-spring systems
  • Learn about differentiating complex equations in physics
  • Explore the applications of Hooke's law in real-world scenarios
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Students studying physics, particularly those focusing on mechanics, as well as educators and tutors looking to enhance their understanding of energy differentiation in mass-spring systems.

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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
\frac{d}{dt}v^2=2v\frac{dv}{dt}=2\frac{dx}{dt}a
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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