Energy to compress a spring 3 units

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Discussion Overview

The discussion revolves around determining the energy required to compress a spring by moving a block on a frictionless surface, where the forces acting on the block are given by \(F = e^x\) and \(F = kx\). Participants explore different approaches to calculate the work done and the energy involved in this process, considering concepts from classical mechanics such as Newton's laws and the work-energy principle.

Discussion Character

  • Exploratory, Technical explanation, Conceptual clarification, Debate/contested, Mathematical reasoning

Main Points Raised

  • One participant sets up Newton's second law and conservation of energy but expresses uncertainty about the initial conditions of the block's motion.
  • Another participant suggests calculating the work done on the block using the integral of the net force, \(W = \int_0^3 (e^x - kx) \, dx\), and emphasizes the importance of considering the direction of forces.
  • There is a discussion about the conditions under which the net force changes sign, depending on the relationship between \(k\) and \(e\), with one participant noting that if \(k < e\), there would be no switching, while \(k > e\) would result in two switches.
  • Some participants clarify that the work integral does not need to be split into regions based on intersections of the force functions, as work can be negative.
  • A later reply asserts that the work calculated in this manner is equivalent to the energy, as both have the same units.

Areas of Agreement / Disagreement

Participants generally agree on the approach of calculating work to find energy but express differing views on how to handle the sign of the forces and the conditions under which the net force changes direction. The discussion remains unresolved regarding the implications of the spring constant \(k\) on the behavior of the forces.

Contextual Notes

There are limitations regarding the initial conditions of the block's motion, which are not explicitly stated, and the dependence on the value of the spring constant \(k\) is crucial for determining the behavior of the forces involved.

Dustinsfl
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Consider a block on a frictionless surface. The force applied the block in the positive x direction is \(F = e^x\) and the force in the negative x is \(kx\) where k is the spring constant.

How is the energy required determined to move the block 3 units?

I set up Newton's 2nd but I don't think that is going to help:
\[
\ddot{x} + \frac{k}{m}x = \frac{1}{m}e^x
\]
Then I set up CoE assuming at 3 units, we only have \(PE = \frac{1}{2}kx^2\) and the block at rest only has \(KE = e^x\).
\[
e^x = \frac{1}{2}kx^2
\]
but this will only tell me the spring constant.
 
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dwsmith said:
Consider a block on a frictionless surface. The force applied the block in the positive x direction is \(F = e^x\) and the force in the negative x is \(kx\) where k is the spring constant.

How is the energy required determined to move the block 3 units?

I set up Newton's 2nd but I don't think that is going to help:
\[
\ddot{x} + \frac{k}{m}x = \frac{1}{m}e^x
\]
Then I set up CoE assuming at 3 units, we only have \(PE = \frac{1}{2}kx^2\) and the block at rest only has \(KE = e^x\).
\[
e^x = \frac{1}{2}kx^2
\]
but this will only tell me the spring constant.
For starters we have no given information to tell us that the block is not moving initially, or at least you didn't post it, so your analysis of the balancing point x may be in error. Anyway unless you need an equation of motion we can do this more directly by considering the work done on the box:
[math]W = \int _0 ^3 F \cdot dx[/math]

where [math]F = e^x - kx[/math]. Be careful of the direction of F...it will be positive on some interval and negative on another. I leave that one to you.

-Dan
 
topsquark said:
For starters we have no given information to tell us that the block is not moving initially, or at least you didn't post it, so your analysis of the balancing point x may be in error. Anyway unless you need an equation of motion we can do this more directly by considering the work done on the box:
[math]W = \int _0 ^3 F \cdot dx[/math]

where [math]F = e^x - kx[/math]. Be careful of the direction of F...it will be positive on some interval and negative on another. I leave that one to you.

-Dan

Can you explain this more?
 
topsquark's approach is probably the simplest. We know that
$$W=\int \mathbf{F} \cdot d\mathbf{r},$$
technically. So if the net force is in the direction of travel, we'll get positive work done by that force, otherwise negative. In this case, the spring force is always to the left, and the exponential force is always to the right. The effect of the spring force is simply going to be to increase the amount of work required. So you must compute
$$W=\int_0^3 (e^{x}-kx) \, dx.$$
Does that answer your question?
 
Ackbach said:
topsquark's approach is probably the simplest. We know that
$$W=\int \mathbf{F} \cdot d\mathbf{r},$$
technically. So if the net force is in the direction of travel, we'll get positive work done by that force, otherwise negative. In this case, the spring force is always to the left, and the exponential force is always to the right. The effect of the spring force is simply going to be to increase the amount of work required. So you must compute
$$W=\int_0^3 (e^{x}-kx) \, dx.$$
Does that answer your question?

I was mainly asking about the positive negative switch. That is determined by k though which we don't know.
 
Right. If $k<e$, you get no switching, if $k=e$ you get one intersection, and if $k>e$ you get two switches. However, I don't think the force in the work integral is a magnitude. That is, I don't think you have to split the integral up into regions, and use different expressions depending on where the two graphs intersect. Work can definitely be negative. In other words, you can compute
$$W=\int_0^3 \left( e^{x}-kx \right) \, dx,\quad \text{not} \quad \int_0^3 \left| e^x - kx \right| \, dx.$$
 
Ackbach said:
Right. If $k<e$, you get no switching, if $k=e$ you get one intersection, and if $k>e$ you get two switches. However, I don't think the force in the work integral is a magnitude. That is, I don't think you have to split the integral up into regions, and use different expressions depending on where the two graphs intersect. Work can definitely be negative. In other words, you can compute
$$W=\int_0^3 \left( e^{x}-kx \right) \, dx,\quad \text{not} \quad \int_0^3 \left| e^x - kx \right| \, dx.$$

Also, how would I go from work to energy afterwards?
 
dwsmith said:
Also, how would I go from work to energy afterwards?

The work computed in this way would BE the energy: work has units of joules, the same as energy.
 

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