Maximizing Energy Transfer in a Compressed Spring System

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In summary, when a box is pushed against a spring and compressed, the work done by the spring force is equal to the potential energy of the spring right after compression.
  • #1
GingerKhan
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Homework Statement



A spring with a force constant of 225 N/m is resting on a friction-less surface and mounted against a wall horizontally. A 1.5 kg box is pushed against the spring and compresses it 12 cm (0.12m) from equilibrium. When released the spring pushes the box across the surface.

Homework Equations



F = kx

W = FΔd

Ee = 1/2 k x^2

Ek = 1/2 m v^2

The Attempt at a Solution



a) How much force needs to be applied to the spring to compress it to 12 cm (0.12m)?

F = 225 x 0.12 = 27 Nb) How much work is done to compress the spring to 12 cm?

W = 27 x 0.12 = 3.24 Jc) How much elastic energy is stored in the spring when compressed?

Ee = 1/2 x 225 x 0.12^2 = 1.62 J

Question: Is it normal that Ee is less than the work energy applied to the system in b)?d) What maximum speed will the box attain once released?

1.62 = 1/2 x 1.5 x v^2

1.62/0.75 = v^2

v = 1.47 m/s

** not sure about this because I might be using a wrong Ek obtained in c) **Thanks in advance.
 
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  • #2
GingerKhan said:
... How much work is done to compress the spring to 12 cm?

W = 27 x 0.12 = 3.24 J


c) How much elastic energy is stored in the spring when compressed?

Ee = 1/2 x 225 x 0.12^2 = 1.62 J

Question: Is it normal that Ee is less than the work energy applied to the system in b)? ...

Note that the force doing the work is varying and so an AVERAGE value of the force must be taken.
 
  • #3
GingerKhan said:
b) How much work is done to compress the spring to 12 cm?

W = 27 x 0.12 = 3.24 J

This is not correct. You can only use "work equals force times distance" on the whole distance if both are constant. If they are not you must integrate the work up from the instantaneous force as a function of distance, e.g. W = ∫F(s)*ds, where s is distance.

In the context of this problem you may also solve b) by using conservation of energy. The original kinetic energy from the block must all be stored in the spring since there is no friction and nothing else moves, hence the block does the amount of work on the spring equal to its kinetic energy, which again is equal to the potential energy right after compression.
 
  • #4
Welcome to PF GingerKhan! :smile:

GingerKhan said:

Homework Statement



A spring with a force constant of 225 N/m is resting on a friction-less surface and mounted against a wall horizontally. A 1.5 kg box is pushed against the spring and compresses it 12 cm (0.12m) from equilibrium. When released the spring pushes the box across the surface.


Homework Equations



F = kx

W = FΔd

Ee = 1/2 k x^2

Ek = 1/2 m v^2

The Attempt at a Solution



a) How much force needs to be applied to the spring to compress it to 12 cm (0.12m)?

F = 225 x 0.12 = 27 N


b) How much work is done to compress the spring to 12 cm?

W = 27 x 0.12 = 3.24 J


c) How much elastic energy is stored in the spring when compressed?

Ee = 1/2 x 225 x 0.12^2 = 1.62 J

Question: Is it normal that Ee is less than the work energy applied to the system in b)?

Nope. :wink: These two numbers should be the same. The mistake is in assuming that W = FΔx. This is only true if the force is constant. The force is not constant here, but rather it varies with x. The more general formula is W = ∫F(x)dx where F(x) is the (position-varying) force function. But if you don't know integral calculus, don't worry. In this case, you've already (implicitly) been given the expression for the work done. Think about this: what is the work done by the spring force as the spring is compressed, (hint: how does this relate to the elastic potential energy stored)? Now, how does the work done by the applied force have to compare to the work done by the spring force?
 
  • #5
Since the force F is directly proportional to the compression the average value of the force will be (final value of F)/2.
 
  • #6
Oh, I forgot about the spring becoming harder to compress as it is being compressed.

So with a graph that illustrates the scenario, I would need to find the area of the right triangle and divide the whole thing by two, giving me 1.62 J

I could also use Ee = 1/2 k x^2 to calculate the work done because W = ΔE.

If c) is correct then d) is correct as well, right?

Thanks guys.
 
Last edited:

FAQ: Maximizing Energy Transfer in a Compressed Spring System

What is the problem with the box and string?

The problem with the box and string is that the string is not long enough to fully wrap around the box, making it difficult to securely tie the box closed.

How can the problem with the box and string be solved?

The problem with the box and string can be solved by using a longer string or by using a different method of securing the box, such as tape or a rubber band.

Why is the length of the string important in this problem?

The length of the string is important because it determines whether or not the box can be securely closed. If the string is too short, it will not be able to fully wrap around the box and may come loose.

Can this problem be avoided in the future?

Yes, this problem can be avoided by ensuring that the string is long enough to fully wrap around the box before attempting to tie it closed.

Are there any other solutions to this problem?

Aside from using a longer string or an alternative method of securing the box, another solution could be to use a box with a lid or flaps that can be folded and tucked in to keep the contents inside.

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