Maximizing Energy Transfer in a Compressed Spring System

  • Thread starter Thread starter GingerKhan
  • Start date Start date
  • Tags Tags
    Box String
AI Thread Summary
A spring with a force constant of 225 N/m compresses 12 cm when a 1.5 kg box is pushed against it. The force required to compress the spring is calculated to be 27 N, resulting in 3.24 J of work done. However, the elastic energy stored in the spring is only 1.62 J, raising questions about the relationship between work and energy in this context. The discrepancy arises because the force exerted on the spring is not constant, necessitating the use of integration to accurately calculate work. Ultimately, the elastic potential energy should equal the work done on the spring, highlighting the importance of understanding variable forces in energy transfer systems.
GingerKhan
Messages
13
Reaction score
0

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.
 
Physics news on Phys.org
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.
 
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.
 
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?
 
Since the force F is directly proportional to the compression the average value of the force will be (final value of F)/2.
 
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:
Thread 'Variable mass system : water sprayed into a moving container'
Starting with the mass considerations #m(t)# is mass of water #M_{c}# mass of container and #M(t)# mass of total system $$M(t) = M_{C} + m(t)$$ $$\Rightarrow \frac{dM(t)}{dt} = \frac{dm(t)}{dt}$$ $$P_i = Mv + u \, dm$$ $$P_f = (M + dm)(v + dv)$$ $$\Delta P = M \, dv + (v - u) \, dm$$ $$F = \frac{dP}{dt} = M \frac{dv}{dt} + (v - u) \frac{dm}{dt}$$ $$F = u \frac{dm}{dt} = \rho A u^2$$ from conservation of momentum , the cannon recoils with the same force which it applies. $$\quad \frac{dm}{dt}...
TL;DR Summary: I came across this question from a Sri Lankan A-level textbook. Question - An ice cube with a length of 10 cm is immersed in water at 0 °C. An observer observes the ice cube from the water, and it seems to be 7.75 cm long. If the refractive index of water is 4/3, find the height of the ice cube immersed in the water. I could not understand how the apparent height of the ice cube in the water depends on the height of the ice cube immersed in the water. Does anyone have an...
Back
Top