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Ideal Gas Law with spring, no numbers, closed container

  1. Apr 27, 2012 #1
    1. The problem statement, all variables and given/known data
    The closed cylinder of the figure has a tight-fitting but frictionless piston of mass M. the piston is in equilibrium when the left chamber has pressure p0 and length L0 while the spring on the right is compressed by ΔL.

    a. What is ΔL in terms of p0, L0, A, M, and k?

    b. Suppose the piston is moved a small distance x to the right. Find an expression for the net force on the piston. Assume all motions are slow enough for the gas to remain at the same temperature as its surroundings

    c. If released, the piston will oscillate around the equilibrium position. Assuming x << L0 find an expression for the oscillation period T.

    qdtHj.jpg


    2. Relevant equations
    for a.
    Not quite sure, All this chapter in the book really taught me was the Ideal Gas Law pV = nRT

    Given that the question is concerned that I include M I suppose they want me to use kinematics? I don't know how M (mass of the piston) affects the gasses, or ΔL.

    I know pressure = Force/Area, and Force = Mass X Acceleration -k X Δx since it's a spring

    for b.
    force of spring = -kΔx
    p1 = nRT/V1
    V=A*L0
    p1*v1 = p2*v2

    for c.
    not sure
    3. The attempt at a solution

    Note: spring is being compressed, p=0 on other side of piston

    first off, V1 = A*L0

    then p1 = (-kΔL)/A (I'm lead to believe p = 0 when ΔL = 0

    I need to fit in M somewhere to fulfill a.

    p1*A = Fsp = -kΔL or, since it's a Force, M*acceleration.

    need k, cross out F=Ma approach

    what does M effect?
    • not volume
    • not temperature
    • movement
    • pressure?
    • Fsp?

    I wonder... Potential spring energy is Usp = 1/2k * Δx^2...

    Kinetic energy is 1/2m * v^2

    could I turn the isothermal (p1v1 = p2v2) into kinematics? energy?

    forces to the right are sourced from p1 and forces to the left are sourced from the spring

    p1 = 1/V1

    V1 = A*L0.... but plus ΔL if it ever gets larger or smaller

    p1 = 1/(A*(L0+ΔL))

    equilibrium lets p1 also equal Fsp/A

    -k*ΔL/A = 1/(A*(L0+ΔL))

    I think I am stuck here

    I need some clues, or hints as to how I should approach this. I feel that once I find out how M effects ΔL the rest wont be so hard!
     
  2. jcsd
  3. Apr 27, 2012 #2
    For part A, I don't think you need all the properties. For example the mass will probably be a component of part C but for part A just do a free body diagram on the mass. The mass isn't moving so the force from the gas = the force from the spring
     
  4. Apr 27, 2012 #3
    That's what's so confusing to me that there's really not too much to say about the system when it's in that state! Yet a. is asking for.... an equation by the sound of it. That seems to be impossible so I will assume you are right about that.

    I might as well move on to b.
     
  5. Apr 28, 2012 #4
    There is an equation. If you do a free body diagram on he mass M the force pushing to the right is P0*A. The force pushing on the mass by the spring is k*ΔL. Set them equal to each other because the forces are equal and solve for ΔL.

    Part b the mass is moved to the right a very small distance x. This is where you use the ideal gas law but to=tf so Po*Vo=Pf*Vf

    You know Po, V0 is lo*A, the new Vf is (Lo+x) * A solve for Pf. Force f is Pf*A

    Part c. Since x is small this is simple harmonic motion for a spring
     
  6. Apr 28, 2012 #5
    ok so I did up part a.

    decided I should find the force of pressure Fp

    p=F/A
    so Fp = p*A
    p=nRT/V
    v=A*(L0+ΔL)

    combine them both into

    nRT/A*(L0+ΔL) * A = Fp
    simplified
    Fp = nRT/(L0+ΔL)

    <-----------*----------->
    Fsp(-kΔL) Fp(nRT/(L0+ΔL)

    and that's all I could do for a.



    For b. I made a Fnet equation:

    Fnet = Fsp + Fp

    Left is negative and Right is positive

    Fnet = -kΔL + nRT/(L0+ΔL)

    T stays the same so obviously the Fnet is going to go left, and real quick unless there is a substantial gain in T (which there isn't)

    Attempting c. need to find out how to do oscillations.... and what "x << L0" even means!
     
  7. Apr 28, 2012 #6
    note, on a. when it said to show ΔL in terms of p0, L0, A, M, and k, I interpreted that as something like "find an equation to solve ΔL using these variables" I must have been mistaken
     
  8. Apr 28, 2012 #7
    What's the definition for the period of a spring/mass system in simple harmonic motion?
     
  9. Apr 28, 2012 #8
    i slightly remember doing stuff like that two quarters ago. Going to have to look through some notes I guess!
     
  10. Apr 28, 2012 #9
    So close to answering c.

    5 hours of straight physics, and I can't refresh myself with kinematics. Gonna try this again tomorrow morning and see if I can answer it.
     
  11. Apr 28, 2012 #10
    c.


    ω = √k/M

    so 2pi/T = √k/M

    2pi = T*√k/M

    2pi/√k/M = T

    I guess that's all they ask for!
     
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