Conservation of Energy with springs

  • #1
heroslayer99
33
6
Homework Statement
A particle of mass m is suspended from a fixed point O by a light spring of natural length a and modulus of elasticity 4mg, the particle is pulled vertically down a distance d from its equilibrium position and released, find d if the particle just reaches O.
Relevant Equations
T = modulus of elasticity (extension) / natural length
EPE = modulus of elasticity (extension)^2 / 2 x natural length
Start by finding the equilibrium position, so we have {4mgx}/{a} = mg giving us x = a/4, therefore the spring's length is 5a/4. Now the loss in EPE (and therefore gain in energy of the particle) between the bottom and the equilibrium position is clearly 4mg((a/4 + d)^2 , and then from the equilibrium position up to O, the particle loses 4mg(a^2)/2a (as this is the gain in EPE), therefore in total the particle's energy has changed by 4mg((a/4 + d)^2 - 4mg(a^2)/2a, and this should equal the change in GPE (- the work done by gravity), which is clearly mg(5a/4 + d), this gives us d=5/4(a), whereas my textbook does something else, could someone let me know if either mine or the textbook's working is wrong? Thanks
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  • #2
The textbook answer is correct. Although, this is for an elastic string, which requires no force/energy to compress.

The total EPE stored in the string is ##\frac{4mg}{2a}(x - a)^2##, where ##x## is the total extension. In this case ##x = a + \frac a 4 + d##.

Alternatively, the total EPE in the string is ##\frac{4mg}{2a}(\Delta x)^2##, where ##\Delta x## is the extension beyond the natural length. In this case ##\Delta x = \frac a 4 + d##.

I'm struggling a little to understand what you have done.
 
  • #3
The textbook says that the energy gained from the spring's extension is enough to reach the top if the distance is 3/4a, I said that we need a little more energy to squish the spring down from its natural length to 0.
1706539404753.png
Textbook also says this, does that not imply that it costs energy to squish the spring?
 
  • #4
heroslayer99 said:
The textbook says that the energy gained from the spring's extension is enough to reach the top if the distance is 3/4a, I said that we need a little more energy to squish the spring down from its natural length to 0.
View attachment 339387Textbook also says this, does that not imply that it costs energy to squish the spring?
The textbook solution is for a string, not a spring. A spring makes little physical sense in this case - although that would be nothing new!

But, you still have a mistake in using the intermediate equilibrium point. I don't understand why you subtracted that term.
 
  • #5
As the particle moves a distance of d + a/4 up, it gains energy, we know it gains an equal amount to the EPE of the string. Then as the particle moves a distance of a up, it loses energy (As it costs energy to squish the spring down to a length of 0, from its natural length). Is my misunderstanding that the spring does not need any force to compress? I have edited my post aswell, check if that makes more sense now.
 
  • #6
heroslayer99 said:
Is my misunderstanding that the spring does not need any force to compress?
The textbook solution is for a sTring (with a T) not a sPring (with a P). A sTring requires no energy to compress from its natural length.
 
  • #7
PeroK said:
The textbook solution is for a sTring (with a T) not a sPring (with a P). A sTring requires no energy to compress from its natural length.
Ah I see. This is not mentioned explicitly in my book, is there a reason for this?
 
  • #8
I think I understand your approach. There is EPE stored in the initial extension from ##a## to ##\frac{5a}{4}## to reach the equilibrium position. The question is whether the mass is pulled far enough to utilise that energy. If you don't pull the mass at all, then that energy cannot be released. There is an assumption that the mass is pulled far enough to be accelerated up beyond the natural length and hence release all the EPE.

In this case, as ##d = \frac{3a}{4}##, that is much greater than ##\frac a 4##, so the string will definitely release all its EPE as the mass will go up and beyond the natural length.
 
  • #9
I am happy with all the EPE being released, the issue was that I thought the particle needed some energy to squish the string down from a length of a to 0, but apparently you don't need any extra energy for that.
 
  • #10
heroslayer99 said:
I am happy with all the EPE being released, the issue was that I thought the particle needed some energy to squish the string down from a length of a to 0, but apparently you don't need any extra energy for that.
In reality (think of a bungee jump), the string has some mass that needs to be accelerated upward. In this case, the assumption is that this is negligible.
 
  • #11
Alright, so we use the word light to mean little to no mass (effectively 0 mass), and this means that the string doesn't need any force to compress. However it still needs force to extend right? And if we use the word light to describe a spring, as my textbook does, do the same things still apply?
 
  • #12
heroslayer99 said:
Alright, so we use the word light to mean little to no mass (effectively 0 mass), and this means that the string doesn't need any force to compress. However it still needs force to extend right?
Yes. Think of a bungee rope as a good example.
heroslayer99 said:
And if we use the word light to describe a spring, as my textbook does, do the same things still apply?
A spring definitely needs force to compress. That would be a different problem - and EPE would again be stored in the spring as the mass moves upwards beyond the natural length.

My main complaint about even considering a spring is that it's unrealistic to assume that a spring (however light) is compressed to zero length.

A string simply gets out of the way and you can imagine the mass touching the ceiling at point O.

That was partly why I assumed that the question must be talking about a string in th first place!
 
  • #13
1706541521541.png

So here we would say that the epe at the start is equal to the epe at the end + the change in gpe.
 
  • #14
heroslayer99 said:
View attachment 339388
So here we would say that the epe at the start is equal to the epe at the end + the change in gpe.
Best to start a new thread. I'm offline now!
 

FAQ: Conservation of Energy with springs

What is the principle of conservation of energy in the context of springs?

The principle of conservation of energy states that the total energy in an isolated system remains constant. For springs, this means that the sum of the potential energy stored in the spring (elastic potential energy) and the kinetic energy of the mass attached to the spring remains constant, assuming no energy is lost to friction or other non-conservative forces.

How is the potential energy in a spring calculated?

The potential energy stored in a spring, also known as elastic potential energy, is calculated using Hooke's Law. The formula is \( PE = \frac{1}{2} k x^2 \), where \( k \) is the spring constant (a measure of the stiffness of the spring) and \( x \) is the displacement from the spring's equilibrium position.

What happens to the energy in a spring-mass system when the spring is compressed or stretched?

When a spring is compressed or stretched, the work done on the spring is stored as elastic potential energy. As the spring returns to its equilibrium position, this potential energy is converted into kinetic energy of the mass attached to the spring. If the system is ideal and frictionless, the total mechanical energy (sum of kinetic and potential energy) remains constant.

How does damping affect the conservation of energy in a spring system?

Damping introduces a non-conservative force, such as friction or air resistance, which causes the system to lose energy over time. In a damped spring system, the total mechanical energy decreases as some of the energy is dissipated as heat or other forms of energy, and the oscillations eventually cease.

Can the conservation of energy principle be applied to real-world spring systems?

Yes, the conservation of energy principle can be applied to real-world spring systems, but it must account for non-conservative forces such as friction, air resistance, and internal damping within the spring. In practical applications, these forces cause energy losses, meaning that the total mechanical energy of the system decreases over time. However, the principle still holds if we consider the total energy, including these losses.

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