Work by a Spring Force - Understanding Uinitial and Ufinal

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Discussion Overview

The discussion revolves around the relationship between work done by a spring force and changes in potential energy, exploring concepts of energy conservation, mathematical formulations, and interpretations of work and energy in mechanical systems.

Discussion Character

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

Main Points Raised

  • Some participants propose that the work done by the spring is equal to the negative change in potential energy, suggesting a relationship between initial and final potential energy states.
  • Others argue that work done can be understood in terms of energy transformations within a system, emphasizing the importance of considering the spring as part of the system.
  • A participant introduces the idea of using equations of motion to derive relationships involving work and energy, although some express difficulty with the complexity of these equations.
  • There is a discussion about the limitations of general statements regarding work and energy, with some preferring concrete examples to illustrate concepts.
  • Concerns are raised about the validity of certain definitions of work and energy, particularly in the presence of other forces or potential energies that may affect the system.
  • A later reply emphasizes the importance of idealized conditions, such as the absence of friction, when applying these concepts.
  • One participant notes that energy conservation should be considered, particularly in the context of how energy is transferred from the spring to the device it drives.

Areas of Agreement / Disagreement

Participants express varying viewpoints on the relationship between work and potential energy, with no consensus reached. Some agree on the negative change in potential energy being related to work done, while others highlight the complexity of the situation depending on additional forces and conditions.

Contextual Notes

Limitations include the dependence on idealized conditions, such as the absence of friction and the assumption of a simple spring model. The discussion also reflects varying levels of comfort with mathematical formulations and the complexity of the underlying physics.

hquang001
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Here it writes Wby spring= Uinitial - Ufinal. So is it equal to opposite of the change in potential energy ?
 
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You can ask yourself, The work of the spring, on who is done? Well the increase or decrease in energy of that system depending on whether the potential of the decrease or increases, why? because when you include the spring as part of the system and you assume that the energy only transforms and does not escape from the system.

##E_f = W_r + E_i##

That is, ##\Delta E = W_r##

But the one that delivers energy from the spring does so as a function of decreasing its potential and vice versa

##W = -\Delta U_r##

Then the conservation of mechanical energy holds

##\Delta E + \Delta U_r = 0##
 
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hquang001 said:
Here it writes Wby spring= Uinitial - Ufinal. So is it equal to opposite of the change in potential energy ?
Think of potential energy as "money in the bank"; and, work done as money you spend.

Money spent = initial balance - final balance
 
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You can also simply use the equation of motion,
$$m \ddot{x}=-k x=-\frac{k}{2} \frac{\mathrm{d}}{\mathrm{d} x} (x^2).$$
Now multiply this equation with ##\dot{x}## and integrate the result from ##t_1## to ##t_2##. What do you get?
 
vanhees71 said:
You can also simply use the equation of motion,
$$m \ddot{x}=-k x=-\frac{k}{2} \frac{\mathrm{d}}{\mathrm{d} x} (x^2).$$
Now multiply this equation with ##\dot{x}## and integrate the result from ##t_1## to ##t_2##. What do you get?
Sorry but this is quite complicated for me, I've never seen this
 
PeroK said:
Think of potential energy as "money in the bank"; and, work done as money you spend.

Money spent = initial balance - final balance
So work done equal negative change of potential energy
and in case of kinetic energy, work done is equal to the change of kinetic energy
am i correct ?
 
hquang001 said:
So work done equal negative change of potential energy
and in case of kinetic energy, work done is equal to the change of kinetic energy
am i correct ?
I never liked these general soundbites about work and energy. I prefer to think in terms of concrete examples:

A block sliding down a frictionless ramp; a block sliding down a ramp with friction.

I see the rules as reflecting the phenomena, not the other way round.
 
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hquang001 said:
So work done equal negative change of potential energy
and in case of kinetic energy, work done is equal to the change of kinetic energy
am i correct ?
It would only be true if there are no other possible potentials of other forces or interactions that could be altered in the system, that is why I understand that @PeroK does not like the idea of defining it that way very much and I share his concern.
So if no other potential is altered and you also maintain idealized statement conditions such as no friction, then ##\Delta K + \Delta W_r = 0##
 
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Richard R Richard said:
It would only be true if there are no other possible potentials of other forces or interactions that could be altered in the system, that is why I understand that @PeroK does not like the idea of defining it that way very much and I share his concern.
So if no other potential is altered and you also maintain idealized statement conditions such as no friction, then ##\Delta K + \Delta W_r = 0##
Oh ok
Thank you
 
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hquang001 said:
So is it equal to opposite of the change in potential energy ?
It's probably a good idea to think in terms of Energy being conserved (ignore any friction within the spring, which can change things anyway). Energy that's transferred from the extended spring (change in potential Energy) must all turn up in the device it's driving. If you do the process slowly enough (quasi-statically) then all the Energy from ('work done by ') the spring has to be 'done on' the driven device and you can ignore any Kinetic Energy.

hquang001 said:
Sorry but this is quite complicated for me, I've never seen this
The equations that have been written here will only apply to a simple, ideal spring (Hooke's Law) and the appropriate equations would actually be a lot more complicated, But there is no real need ( at least for starters) to understand the Maths in order to get the basic idea. People can get very bothered when Integral Signs turn up and can lose the message. Having said that, it's not possible to get much further without getting into the Maths so I am not offering you a free pass to avoid Maths for long.
 
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