Measuring Pressure — Question 10

Section 14-4 · Physics pages 2130–2131

Question 10 A trapped gas makes a closed-end reading nonlinear A vertical U-tube of uniform area contains water. Initially its two surfaces are level; the left side is open to atmosphere at p0 = 100 kPa and the right side traps gas of length L0 = 0.20 m at p0. Gas of higher pressure is then applied on the left. The right water surface rises by x = 0.020 m while the left falls equally. The trapped gas obeys the supplied isothermal law pV = constant. Use ρ = 1000 kg/m3 and g = 10 m/s2. trapped gas Equal-area arms move by equal amounts; the closed-end gas is compressed as the right surface rises. (a) Find the final trapped-gas pressure and applied left pressure. (b) Explain why treating the closed end as a vacuum is invalid, and identify the singular limit of the ideal model.
Show solutionHide solution
Question 10 - Solution A trapped gas makes a closed-end reading nonlinear trapped gas (a) Derivation and calculation V0 = AL0, VR = A(L0 −x), pRVR = p0V0. pR = p0L0 L0 −x = 100(.200) .180 = 111.111 kPa . h = 2x = .0400 m, pL = pR + 2ρgx = 111.511 kPa . (b) Result and interpretation pL(x) = p0L0 L0 −x + 2ρgx, 0 ≤x < L0. x →L− 0 ⇒VR →0+, pR →∞. The gas is neither a vacuum nor a fixed-pressure reference. The ideal law has a zero-volume singularity and cannot be extended beyond it. Physical check At x = 0, both pressures return to p0, recovering the initial level-surface condition.

Question 10

A trapped gas makes a closed-end reading nonlinear

A vertical U-tube of uniform area contains water. Initially its two surfaces are level; the left side is open to atmosphere at p0=100kPap_0=100\,\mathrm{kPa} and the right side traps gas of length L0=0.20mL_0=0.20\,\mathrm{m} at p0p_0. Gas of higher pressure is then applied on the left. The right water surface rises by x=0.020mx=0.020\,\mathrm{m} while the left falls equally. The trapped gas obeys the supplied isothermal law pV=constantpV=\text{constant}. Use ρ=1000kg/m3\rho=1000\,\mathrm{kg/m^3} and g=10m/s2g=10\,\mathrm{m/s^2}.

Diagram shown in the original SVG worksheet.

  1. Find the final trapped-gas pressure and applied left pressure.

  2. Explain why treating the closed end as a vacuum is invalid, and identify the singular limit of the ideal model.

Question 10 - Solution

A trapped gas makes a closed-end reading nonlinear

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

V0=AL0,VR=A(L0−x),pRVR=p0V0.V_0=AL_0,\quad V_R=A(L_0-x),\quad p_RV_R=p_0V_0.pR=p0L0L0−x=100(.200).180=111.111kPa.\boxed{p_R=\frac{p_0L_0}{L_0-x}=\frac{100(.200)}{.180}=111.111\,\mathrm{kPa}}.h=2x=.0400m,pL=pR+2ρgx=111.511kPa.h=2x=.0400\,\mathrm m,\quad\boxed{p_L=p_R+2\rho gx=111.511\,\mathrm{kPa}}.

(b) Result and interpretation

pL(x)=p0L0L0−x+2ρgx,0≤x<L0.p_L(x)=\frac{p_0L_0}{L_0-x}+2\rho gx,\qquad0\le x<L_0.x→L0−⇒VR→0+,pR→∞.x\to L_0^-\Rightarrow V_R\to0^+,\quad p_R\to\infty.The gas is neither a vacuum nor a fixed-pressure reference. The ideal law has a zero-volume singularity and cannot be extended beyond it.

Physical check

At x=0x=0, both pressures return to p0p_0, recovering the initial level-surface condition.