Work done on a spring by an ideal gas

In summary: F=kΔx right?In summary, the question is asking for the work done by an ideal gas on a hooke's spring when heat is added until volume and pressure triple. The ideal gas law, heat equation, and work equation for a spring are given as reference. The process being described is a piston problem, where the spring is connected to the lid of the gas container and is initially at rest. The final volume is 3 times the initial volume, and the final pressure is 3 times the initial pressure. The work done by the gas is equal to the change in potential energy of the spring, but in order to determine this, the work done on other bodies must also be considered, such as the atmosphere and the
  • #1
physninj
37
0

Homework Statement



Find the work done by an ideal gas on a hooke's spring when heat is added until volume and pressure triple

Homework Equations


Pv=nrT
Q=ncΔt
W=(1/2)kx^2
F=kx=P*A

The Attempt at a Solution


I took the work equation for the spring and subbed in P*A to get w=(1/2)(PA)Δx and then i believe i can state that the work done on the spring is W=.5P2V2-.5P1V1 would you agree with this? I skipped some of the process so let me know if you need clarification.
 
Last edited:
Physics news on Phys.org
  • #2
physninj said:

Homework Statement



Find the work done by an ideal gas on a hooke's spring when heat is added until volume and pressure triple

Homework Equations


Pv=nrT
Q=ncΔt
W=(1/2)kx^2
F=kx=P*A

The Attempt at a Solution


I took the work equation for the spring and subbed in P*A to get w=(1/2)(PA)Δx and then i believe i can state that the work done on the spring is W=.5P2V2-.5P1V1 would you agree with this? I skipped some of the process so let me know if you need clarification.
I am not sure what the question is. Do we assume the spring is providing 0 pressure initially and during expansion the spring is compressed (or stretched). How does the spring length change with the volume? It depends on how the spring is connected to the gas container.

AM
 
  • #3
Its pretty much a piston problem, where the spring is above the container of the gas connected to the lid and is initially at rest, then heat is added to the gas until it expands, working against the spring. Its mostly conjecture, I'm trying to anticipate one of the problems that is likely to be on my exam.
 
  • #4
physninj said:
Its pretty much a piston problem, where the spring is above the container of the gas connected to the lid and is initially at rest, then heat is added to the gas until it expands, working against the spring. Its mostly conjecture, I'm trying to anticipate one of the problems that is likely to be on my exam.
The change in potential energy of the spring is equal to the work done on the spring by the gas. But in order to determine how much work is done by the gas on the spring, one has to know how much work is done on other bodies: eg the atmosphere; the piston.

Can you give us the exact question?

AM
 
Last edited:
  • #5
Yeah for sure I've attached one, thanks AM for being patient and responding to my incomplete posts. I think I can solve it I just need help with relating the mechanical work to the thermodynamic work.
 
Last edited:
  • #6
Originally the gas has Po pressure and Vo Volume. Assume slow heating, so the pressure of the gas is balanced by the atmospheric pressure and the pressure from the compressed spring. What is the pressure and the volume when the piston moves to the right by Δx, assuming k spring constant and A cross-section area of the cylinder?

How is work calculated? How much work does the gas do while its volume increases three times the original volume?

When the volume is 3 Vo the pressure is 3Po. What does it mean for the spring constant?



ehild
 

Attachments

  • springgas.JPG
    springgas.JPG
    4.1 KB · Views: 702
  • #7
Well I think I'm starting to get there. I can state the following

Wgas=PΔV=P*A*Δx=Wspring=-(1/2)k(Δx)^2

or PAΔx=(1/2)k(Δx)^2

I don't know where to go with this exactly, I know Δx is needed right? Work is calculated as pressure multiplied by the change in volume, but how do I use that when both pressure and volume are tripled?
 
  • #8
physninj said:
Well I think I'm starting to get there. I can state the following

Wgas=PΔV=P*A*Δx=Wspring=-(1/2)k(Δx)^2

or PAΔx=(1/2)k(Δx)^2

I don't know where to go with this exactly, I know Δx is needed right? Work is calculated as pressure multiplied by the change in volume, but how do I use that when both pressure and volume are tripled?

The gas does work against the surrounding atmosphere, too. The work ∫PdV from Vo to 3Vo. You need to express P in terms of V.

What is the volume of the gas if the piston moves to the right by Δx?

What is the pressure balanced by the spring and the atmospheric pressure if the spring is compressed by Δx?

ehild
 
  • #9
Hmm. I used the ideal gas equation to get the integral into one variable and get the work done on the surroundings as W=nRTln(V2/V1), so that must be the total work done by the gas in expanding.

The Volume of the gas moved by the piston is V+(A*Δx) or V2/3V1

I don't understand where any of this is getting me I'm sorry. I don't mean to be high maintenance.


is it just

nrTln(V2/V1)=(1/2)kΔx^2

or what. That's the work done in the expansion of the gas, but it doesn't take into effect the extra work the gas had to do to push the spring.
 
  • #10
The formula you use for work is for an isothermal process. Why should it be isothermal expansion when both volume and pressure increases three times? Think of the Ideal Gas Law.

You need the work done on the spring but for that you need both k and Δx.

You know that V= Vo+AΔx.

How is the pressure related to Δx? What force is exerted on the piston from the spring?

ehild
 
  • #11
I do not know what kind of process it is, that is the problem, its not given. Its not isobaric because the pressure triples. Its not isochoric because the volume triples. Its not adiabatic because heat is added. I know this stuff, but nowhere in any of my thermo chapters is there a problem like this. So how am I supposed to calculate work?? Unfortunately this cryptic stuff is just leading me down nonsense paths...


anyways, why would I need to deal with k if its constant and given in the problem? and yeah I need Δx. Not sure how to get it though. I keep trying to set things equal different ways but not really seeing any progress.

Pressure is related to work which is related to Δx, I think I established that, although I don't know if I did so correctly. and the force exerted by the spring is going to be F=kΔx
 
Last edited:
  • #12
You wrote already that the work done on the spring is 0.5 kΔx2.
But neither k nor Δx are given.

You can assume a quasi-static process when the total force of the gas exerted on the piston is equal to the external force. Yes, the spring exerts kΔx force on the piston, nut also the outside atmosphere exerts some force.


Initially the pressure of the gas was equal to the atmospheric pressure.


ehild
 
  • #13
oh wow you're right It is not provided. Goodness I think its time I went to sleep, its 1:30 a.m. here. Thank you for your help this evening, I'll be back to trying to figure this out tomorrow.
 
  • #14
Ok, let me go ahead and try to do a force summation of the internal and external And see if I can get down to two equations two unknowns. If anybody is willing to tell me what the bigger picture is it would really help me out. I haven't had a clue what I've been working towards this whole time.

Let me just show you the process I tried to use before, this guessing game is getting me lost I think. I suck at being led to water I guess.

so

W=(1/2)kx^2 and kx=F
W=(1/2)(F)*x=(1/2)(P*A)x and since Δx is the change in height of the chamber I can state the following, letting x represent the height of the container
W=(1/2)P*A*(x+Δx)-(1/2)P*A*(x)
W=(1/2)P2V2-(1/2)P1V1

And If it has to do work against the outside pressure as well I'm not sure how to account for it. this could very well be wrong. Heres the force summation I was talking about, I found it in this thread https://www.physicsforums.com/showthread.php?t=256682


Ftot=k*v+Fatm which forms a linear equation going through both my known points. Can I then solve for k using the slope formula? I don't understand why the spring force would be k*V.
 
Last edited:
  • #15
The spring force is not equal to PA.
Initially, the gas was in equilibrium and the spring was unstretched. The initial pressure was equal to the atmospheric pressure, Po.
The piston moves to the right by Δx, the spring gets shorter by Δx during the process.
The piston exerts kΔx force on the spring, the spring exerts also kΔx force on the piston. The atmospheric pressure means APo force on the piston. So the external force on the piston is PoA +kΔx. The gas also exerts force on the piston: It is PA. The piston is stationary at the end: The inward and outward forces balance.

PoA +kΔx=P(final)A and P(final)=3Po.

You know that the final volume is Vf=Vi+AΔx, and Vf=3Vi.

From these two equations you get expressions for k and Δx in terms of A and the pressure Po and volume Vi. Use them to determine the spring energy.

ehild
 
Last edited:
  • #16
I've got it! science be praised. Here's what I did

Forces:

PA=Patm+kx

Divide both sides by A to get a linear function for pressure in terms of volume

P=Patm+(k/A)x

Then I can take the equation for volume and solve for x to eliminate it in the above equation

V=V0+Ax
x=(V-V0)/A

So I have

P=Patm+(k/A2)(V-V0)Now this is a linear function and the slope is defined by the term (k/A2)
SO I can use the given initial and final pressures and volumes to calculate the slope m=ΔP/ΔV (getting a numerical value) thereby eliminating the not given values for k and A. Then the above equation can be integrated with respect to volume to give the work.

∫PdV=∫(Patm+(m)(V-V0))dV
W=Patm(V-V0)+(1/2)m(V-V0)2

man it seems so simple now that I see it all worked out like this. Oh well, as my instructor says, you got to embrace the struggle. Thanks for your help ehild.
 
  • #17
physninj said:
I've got it! science be praised. Here's what I did

Forces:

PA=Patm+kx

Divide both sides by A to get a linear function for pressure in terms of volume

P=Patm+(k/A)x

Then I can take the equation for volume and solve for x to eliminate it in the above equation

V=V0+Ax
x=(V-V0)/A

So I have

P=Patm+(k/A2)(V-V0)


Now this is a linear function and the slope is defined by the term (k/A2)
SO I can use the given initial and final pressures and volumes to calculate the slope m=ΔP/ΔV (getting a numerical value) thereby eliminating the not given values for k and A. Then the above equation can be integrated with respect to volume to give the work.

∫PdV=∫(Patm+(m)(V-V0))dV
W=Patm(V-V0)+(1/2)m(V-V0)2

man it seems so simple now that I see it all worked out like this. Oh well, as my instructor says, you got to embrace the struggle. Thanks for your help ehild.

It is even simpler than that :biggrin: You do not need to integrate to get the work on the spring,. It is 1/2 kx2.

As you wrote correctly, P=Patm+(k/A)x, and x=(V-Vo)/A .

P-Patm=kx/A = k(V-Vo)/A2, that is k=(P-Patm) A2/(V-Vo)

Substitute for x and k in W=1/2 kx2 . A cancels.

ehild
 

Related to Work done on a spring by an ideal gas

1. What is the equation for calculating work done on a spring by an ideal gas?

The equation for calculating work done on a spring by an ideal gas is W = ½kΔx², where W is the work done, k is the spring constant, and Δx is the change in length of the spring.

2. How does the work done on a spring by an ideal gas differ from other types of work?

The work done on a spring by an ideal gas is different from other types of work because it involves a change in the potential energy of the gas, rather than a change in its kinetic energy. This is due to the fact that the spring is compressed or stretched by the gas, rather than directly pushing or pulling on it.

3. What factors affect the work done on a spring by an ideal gas?

The work done on a spring by an ideal gas is affected by the spring constant, the change in length of the spring, and the amount of gas present. It is also influenced by the pressure and temperature of the gas, as well as the volume of the container it is in.

4. How does the work done on a spring by an ideal gas relate to the concept of work in physics?

The work done on a spring by an ideal gas follows the same principles as work in physics, which is defined as the product of force and displacement. In this case, the force is exerted by the gas on the spring, and the displacement is the change in length of the spring.

5. What is the significance of understanding work done on a spring by an ideal gas?

Understanding work done on a spring by an ideal gas is significant in various fields of science and engineering, such as thermodynamics, fluid dynamics, and material science. It can also have practical applications in areas such as gas-powered engines and machinery that use springs as a source of energy.

Similar threads

  • Introductory Physics Homework Help
Replies
12
Views
855
  • Introductory Physics Homework Help
Replies
1
Views
537
  • Introductory Physics Homework Help
Replies
17
Views
2K
  • Introductory Physics Homework Help
Replies
2
Views
577
  • Introductory Physics Homework Help
Replies
10
Views
975
  • Introductory Physics Homework Help
Replies
2
Views
1K
  • Introductory Physics Homework Help
Replies
4
Views
1K
  • Introductory Physics Homework Help
Replies
4
Views
2K
  • Introductory Physics Homework Help
Replies
9
Views
1K
  • Introductory Physics Homework Help
Replies
3
Views
243
Back
Top