Volume-pressure equation for an expanding ideal gas

In summary, the problem is that the equation between pressure and volume does not hold when atmospheric pressure is not present.
  • #1
MatinSAR
597
182
Homework Statement
How do I find the volume-pressure equation for an expanding ideal gas for the figure below?
Relevant Equations
pV=nRT
There is no atmosphere pressure.
1674383660123.png


My work :
pA=k(x-x0) => pA=(k/A)(V-V0)

But this should be false beccause I want to use W=∫PdV to find work done by the gas but my final anwer is wrong ...
Please guide me where my mistake is if you have enough time. Thanks.
 
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  • #2
Please show more details of what you did. Is this expansion by adding heat at constant temperature? Please provide an exact word-for-word statement of the problem.
 
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  • #3
Chestermiller said:
Is this expansion by adding heat at constant temperature?
It just said that we heat the gas slowly.
Chestermiller said:
Please provide an exact word-for-word statement of the problem.
We heat the gas slowly so that it goes from (P1,V1) to (P2,V2). What is the work done on the gas?
We can use Hook's law for the spring. Piston is light(=forget mass of it).

Chestermiller said:
Please show more details of what you did.
I want to find the equation between pressure and volume.
And I don't know why this is wrong :
pA=k(x-x1) => pA=(k/A)(V-V1)
 
  • #4
MatinSAR said:
pA=(k/A)(V-V1)
I think I have founded the problem. It should be (p-p1)A=(k/A)(V-V1).
Is it true?
 
  • #5
MatinSAR said:
I think I have founded the problem. It should be (p-p1)A=(k/A)(V-V1).
Is it true?
yes
 
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  • #6
Chestermiller said:
yes
Thank you for your help and time.
 
  • #7
1674403349213.png


I'm having some doubts on this one?

Ignoring atmospheric pressure on the spring side seems like bit of blunder IMO. The spring would initially have to be compressed at ##x_o##.Bypassing that issue, I think it's understood to be in a state of "quasistatic equilibrium" this implies that the forces are balanced across the piston.

$$ - k ( x - x_o ) + F_g = 0 $$

$$ \implies P_x = \frac{k}{A}( x - x_o )$$

you can see that the absolute pressure in the gas must be 0 at ##x = x_o## in the absence of atmospheric pressure...is that really ok? Don't we have to be at absolute zero in temperature initially for this to be possible? can we have a gas at absolute 0 temp? Some of the question I have.

In terms of volume ## V\llap{-}##, just multiply through by ##A##:

$$ P_x A = \frac{k}{A}( V\llap{-}_x - V\llap{-}_o )$$

$$ \boxed{ P_x = \frac{k}{A^2}( V\llap{-}_x - V\llap{-}_o ) }$$

What am I missing?
 
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  • #8
erobz said:
View attachment 320900

I'm having some doubts on this one?

Ignoring atmospheric pressure on the spring side seems like bit of blunder IMO. The spring would initially have to be compressed at ##x_o##.Bypassing that issue, I think it's understood to be in a state of "quasistatic equilibrium" this implies that the forces are balanced across the piston.

$$ - k ( x - x_o ) + F_g = 0 $$

$$ \implies P_x = \frac{k}{A}( x - x_o )$$
In terms of volume ## V\llap{-}##, just multiply through by ##A##:

$$ P_x A = \frac{k}{A}( V\llap{-}_x - V\llap{-}_o )$$

$$ \boxed{ P_x = \frac{k}{A^2}( V\llap{-}_x - V\llap{-}_o ) }$$

What am I missing?
In my judgment, the confusion with this problem is yours.

The problem statement says that the atmospheric pressure is zero. This is the same as saying that the device is contained within a vacuum chamber. Who says that this is not allowed?

If the atmospheric pressure is zero, this means that the spring is under preload compression so that the forces on both sides of the piston are initially equal. Therefore, $$P_1A=A\frac{nRT_1}{V_1}=\frac{k}{A}(V_1-V_0)$$where ##V_0## would be the volume at which the sprig is unextended. At all other times, the forces on both sides of the piston also match: $$P=\frac{nRT}{V}=\frac{nRT_1}{V_1}+\frac{k}{A^2}(V-V_1)$$

So what's the problem?
 
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  • #9
Chestermiller said:
In my judgment, the confusion with this problem is yours.
Quite likely.
Chestermiller said:
So what's the problem?
One thing, if this is happening in the vacuum of space we have to have a gas at some initial volume ## V\llap{-}_o## ( zero pre-compressed spring state) with absolute zero temperature (with regards to the ideal gas law).
 
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  • #10
erobz said:
Quite likely.

One thing, if this is happening in the vacuum of space we have to have a gas at some initial volume ## V\llap{-}_o## ( zero pre-compressed spring state) with absolute zero temperature (with regards to the ideal gas law).
No. Vo is the chamber volume at which the spring is unextended. This is geometric, and independent of the gas.
 
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  • #11
Chestermiller said:
No. Vo is the chamber volume at which the spring is unextended. This is geometric, and independent of the gas.
Ahh, there is no gas in the chamber when ##V\llap{-} = V\llap{-}_o##. I guess that is the plausible alternative I was missing.

Thank You.
 
Last edited:

Related to Volume-pressure equation for an expanding ideal gas

What is the volume-pressure equation for an expanding ideal gas?

The volume-pressure equation for an expanding ideal gas is given by Boyle's Law, which states that for a given amount of gas at constant temperature, the product of the pressure and volume is constant. Mathematically, it is expressed as \( PV = k \), where \( P \) is the pressure, \( V \) is the volume, and \( k \) is a constant.

How does temperature affect the volume-pressure relationship in an ideal gas?

Temperature plays a critical role in the volume-pressure relationship of an ideal gas. According to the Ideal Gas Law, \( PV = nRT \), where \( n \) is the number of moles, \( R \) is the gas constant, and \( T \) is the temperature in Kelvin. If the temperature increases while the amount of gas remains constant, the product \( PV \) will also increase, meaning that either pressure or volume must increase to maintain the relationship.

What assumptions are made about the gas in the volume-pressure equation?

The volume-pressure equation for an ideal gas assumes that the gas behaves ideally, meaning that the gas molecules do not interact with each other and occupy no volume themselves. These assumptions hold true under low pressure and high temperature conditions, where the gas molecules are far apart and interactions are minimal.

Can the volume-pressure equation be applied to real gases?

While the volume-pressure equation provides a good approximation for many gases under a range of conditions, real gases deviate from ideal behavior at high pressures and low temperatures. For real gases, corrections can be made using the Van der Waals equation, which accounts for intermolecular forces and the finite volume of gas molecules.

How can the volume-pressure relationship be experimentally verified?

The volume-pressure relationship can be experimentally verified using a closed system where the amount of gas and temperature are kept constant. By measuring the pressure and volume of the gas at different states, one can plot \( P \) versus \( 1/V \). According to Boyle's Law, this plot should yield a straight line, confirming the inverse relationship between pressure and volume.

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