GSO001 Problem 15
Problem Statement
Oscillation of a Liquid Column in a U-Tube with Adiabatic Change
Problem Statement
A U-tube with uniform cross-sectional area S is fixed horizontally. The left tube is closed at the top and the right tube is open at the top. A liquid of density ρ is poured into the U-tube, trapping an ideal gas (monatomic) in the closed left tube. Let the atmospheric pressure be P0 and the magnitude of gravitational acceleration be g.
[State 0] In the initial state, the trapped gas has temperature T0 and the liquid levels in both tubes are at the same height. At this time, the length of the trapped gas column is l0.
[State 1] The gas on the left is slowly heated, causing it to expand and push the liquid to the right. When the gas column length reaches l1 (l1>l0), heating stops and thermal equilibrium is reached. Let the gas pressure at this point be P1.
[State 2 (Small Oscillations)] Starting from state 1, the liquid column is displaced slightly along the tube and then released, causing the liquid column to oscillate. The period of this oscillation is sufficiently short that the state change of the trapped gas can be treated as an adiabatic process.
Let the total length of the liquid column be L. All energy dissipation other than the kinetic energy of the liquid column motion (viscosity, friction with the tube, etc.) is negligible. The mass of the gas is negligible compared to the liquid.
Find the square of the angular frequency ω2 of this small oscillation of the liquid column.
Constraints
- Atmospheric pressure: P0=1.013×105 Pa
- Gravitational acceleration: g=9.80 m/s2
- Liquid density: ρ=1.00×103 kg/m3
- Total length of liquid column: L=2.00 m
- Length of gas column in state 0: l0=0.400 m
- Length of gas column in state 1: l1=0.500 m
- Heat capacity ratio of monatomic ideal gas: γ=35
Input Format
Compute ω2 in units of rad2/s2 and give the answer as a positive integer equal to the value multiplied by 10.
Solution
1. Gas Pressure P1 in State 1
When the gas expands from length l0 to l1, the left liquid level drops by (l1−l0) and the right level rises by (l1−l0). The height difference between liquid levels:
Δh=2(l1−l0)Force balance at the left liquid surface:
P1=P0+ρgΔh=P0+2ρg(l1−l0)2. Adiabatic Pressure Change in State 2
Let the displacement of the liquid column from equilibrium position be y (positive = liquid rises on left side). The gas column length becomes l1−y and volume V=S(l1−y).
By Poisson's law PVγ=const for adiabatic processes:
P=P1(l1−yl1)γ=P1(1−l1y)−γApplying the first-order Taylor expansion (1+x)n≈1+nx for small y/l1:
P≈P1+l1γP1y3. Equation of Motion of the Liquid Column
When displaced by y, the left level rises by y and the right level drops by y, so the height difference becomes 2(l1−l0)−2y.
The net force on the liquid column (total mass M=ρLS):
F=[P0+ρg(2(l1−l0)−2y)]S−PSSubstituting P1=P0+2ρg(l1−l0) and P≈P1+l1γP1y:
F=−(l1γP1+2ρg)SyThe equation of motion My¨=F with M=ρLS:
y¨=−ρLl1γP1+2ρgyComparing with y¨=−ω2y:
ω2=ρLl1γP1+2ρg4. Numerical Calculation
l1−l0=0.500−0.400=0.100 m
P1=1.013×105+2×(1.00×103)×9.80×0.100=101300+1960=103260 PaNumerator (with γ=5/3):
Numerator=35×0.500103260+2×(1.00×103)×9.80 =35×206520+19600=344200+19600=363800Denominator: ρL=1.00×103×2.00=2000
ω2=2000363800=181.9 rad2/s2The required answer is 181.9×10=1819.
Final Answer: 1819