Ideal gas in a cylinder with a piston

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SUMMARY

The discussion focuses on the dynamics of an ideal gas in a vertical cylinder with a piston. The equilibrium pressure of the gas is determined to be p1 = p0 + mg/πr². When the piston is displaced by a small distance y, the net force acting on the piston is calculated as ∑F = (h/(h + y) - 1)(mg + p0πr²). The correct simplification leads to the textbook answer of ∑F = -(y/h)(mg + p0πr²), highlighting the importance of understanding the relationship between y and h in this context.

PREREQUISITES
  • Understanding of ideal gas laws, specifically pV = nRT.
  • Familiarity with basic mechanics, particularly force calculations (F = ma).
  • Knowledge of pressure calculations in fluid dynamics.
  • Ability to manipulate algebraic expressions and simplifications.
NEXT STEPS
  • Study the implications of the ideal gas law in varying conditions.
  • Learn about the concept of equilibrium in thermodynamic systems.
  • Explore the significance of the approximation y << h in physical calculations.
  • Investigate the effects of varying piston mass on gas pressure and force dynamics.
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Students studying thermodynamics, physics enthusiasts, and educators looking to deepen their understanding of gas behavior in confined systems.

Elias Waranoi
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Homework Statement


A vertical cylinder of radius r contains an ideal gas and is fitted with a piston of mass m that is free to move. The piston and the walls of the cylinder are frictionless, and the entire cylinder is placed in a constant-temperature bath. The outside air pressure is p0. In equilibrium, the piston sits at a height h above the bottom of the cylinder. (a) Find the absolute pressure of the gas trapped below the piston when in equilibrium. (b) The piston is pulled up by a small distance and released. Find the net force acting on the piston when its base is a distance h + y above the bottom of the cylinder, where y << h.

Homework Equations


F = pA = ma
pV = nRT (pressure p, volume V, moles in gas n, gas constant R, temperature T)
V = πr2h

The Attempt at a Solution


I managed to solve a) by myself and get p1 = p0 + mg/πr2

Trying to solve b)
Positive force is upwards so ∑F = F - F0 - Fp where F is the force upwards on the piston by the pressure of the gas underneath, F0 is the downward force on the piston by the air pressure p0 above and Fp is the downward force by the weight of the piston.

F0 = p0A = p0πr2
Fp = mg

moles in ideal gas n = p1V1/RT1 (1)
pressure p2 = nRT2/V2 (2)
Because of heat conduction and the constant temperature outside the cylinder, T2 = T1. Inserting (1) in (2) yields:
p2 = p1V1/V2
V1 = πr2h
V2 = πr2(h + y)
p2 = p1h/(h + y)

∑F = p2A - p0A - mg. A = πr2.
Simplifying yields my answer: ∑F = (h/(h + y) - 1)(mg + p0πr2)
Textbook answer: ∑F = -(y/h)(mg + p0πr2)

I tried replacing the variables with values to see the result of both answers. My answer is not correct apparently, what did I do wrong?
 
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Elias Waranoi said:

Homework Statement


A vertical cylinder of radius r contains an ideal gas and is fitted with a piston of mass m that is free to move. The piston and the walls of the cylinder are frictionless, and the entire cylinder is placed in a constant-temperature bath. The outside air pressure is p0. In equilibrium, the piston sits at a height h above the bottom of the cylinder. (a) Find the absolute pressure of the gas trapped below the piston when in equilibrium. (b) The piston is pulled up by a small distance and released. Find the net force acting on the piston when its base is a distance h + y above the bottom of the cylinder, where y << h.

Homework Equations


F = pA = ma
pV = nRT (pressure p, volume V, moles in gas n, gas constant R, temperature T)
V = πr2h

The Attempt at a Solution


I managed to solve a) by myself and get p1 = p0 + mg/πr2

Trying to solve b)
Positive force is upwards so ∑F = F - F0 - Fp where F is the force upwards on the piston by the pressure of the gas underneath, F0 is the downward force on the piston by the air pressure p0 above and Fp is the downward force by the weight of the piston.

F0 = p0A = p0πr2
Fp = mg

moles in ideal gas n = p1V1/RT1 (1)
pressure p2 = nRT2/V2 (2)
Because of heat conduction and the constant temperature outside the cylinder, T2 = T1. Inserting (1) in (2) yields:
p2 = p1V1/V2
V1 = πr2h
V2 = πr2(h + y)
p2 = p1h/(h + y)

∑F = p2A - p0A - mg. A = πr2.
Simplifying yields my answer: ∑F = (h/(h + y) - 1)(mg + p0πr2)
Textbook answer: ∑F = -(y/h)(mg + p0πr2)

I tried replacing the variables with values to see the result of both answers. My answer is not correct apparently, what did I do wrong?
Your answer is correct, but simplify the factor h/(h+y)-1, and use that y<<h.
 
I don't even know what y<<h is. And simplifying h/(h+y)-1 gives me (h-y)/(h+y)
 
Elias Waranoi said:
I don't even know what y<<h is. And simplifying h/(h+y)-1 gives me (h-y)/(h+y)
Check your math. This is wrong.
 
h/(h+y) - 1 = h/(h+y) - (h+y)/(h+y) = (h - (h+y))/(h+y) = (h - h - y)/(h+y) = -y/(h+y)
oops, you're right. But what am I supposed to do now?
 
Elias Waranoi said:
h/(h+y) - 1 = h/(h+y) - (h+y)/(h+y) = (h - (h+y))/(h+y) = (h - h - y)/(h+y) = -y/(h+y)
oops, you're right. But what am I supposed to do now?
Dividing numerator and denominator by h yields:
$$\frac{y}{h+y}=\frac{y}{h}\frac{1}{(1+\frac{y}{h})}$$For y much smaller than h, y/h is much smaller than 1. Therefore, $$\frac{1}{(1+\frac{y}{h})}\rightarrow 1$$and $$\frac{y}{h+y}\rightarrow \frac{y}{h}$$
 
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