Measuring Pressure — Question 3

Section 14-4 · Physics pages 2116–2117

Question 3 Tap elevation must be included in a differential reading Two water-filled pressure lines connect taps A and B to a mercury U-manometer. Tap B is 0.50 m above A. The mercury interface on the B side is 0.10 m above the A-side interface. Use ρw = 1000, ρm = 13600 kg/m3 and g = 10 m/s2. All lines are static. A, zA B, zB zL zR Water lines connect the taps to mercury; both tap elevation and mercury-interface elevation enter the pressure path. (a) Derive and evaluate pA −pB using upward coordinate z. (b) If the two taps instead sample one connected static water reservoir, what interface-height difference should occur, despite their unequal tap pressures?
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Question 3 - Solution Tap elevation must be included in a differential reading A, zA B, zB zL zR (a) Derivation and calculation pL = pA + ρwg(zA −zL), pR = pB + ρwg(zB −zR). pL −pR = ρmg(zR −zL), h = zR −zL. pA −pB = ρwg(zB −zA) + (ρm −ρw)gh . (b) Result and interpretation pA −pB = 1000(10)(.50) + 12600(10)(.10) = 17600 Pa . For two taps in one static water reservoir, pA −pB = ρwg(zB −zA) ⇒(ρm −ρw)gh = 0 ⇒h = 0 . Physical check The manometer isolates the elevation-corrected pressure difference, which vanishes in a single static water body.

Question 3

Tap elevation must be included in a differential reading

Two water-filled pressure lines connect taps A and B to a mercury U-manometer. Tap B is 0.50m0.50\,\mathrm{m} above A. The mercury interface on the B side is 0.10m0.10\,\mathrm{m} above the A-side interface. Use ρw=1000\rho_w=1000, ρm=13600kg/m3\rho_m=13600\,\mathrm{kg/m^3} and g=10m/s2g=10\,\mathrm{m/s^2}. All lines are static.

Diagram shown in the original SVG worksheet.

  1. Derive and evaluate pA−pBp_A-p_B using upward coordinate zz.

  2. If the two taps instead sample one connected static water reservoir, what interface-height difference should occur, despite their unequal tap pressures?

Question 3 - Solution

Tap elevation must be included in a differential reading

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

pL=pA+ρwg(zA−zL),pR=pB+ρwg(zB−zR).p_L=p_A+\rho_wg(z_A-z_L),\quad p_R=p_B+\rho_wg(z_B-z_R).pL−pR=ρmg(zR−zL),h=zR−zL.p_L-p_R=\rho_mg(z_R-z_L),\quad h=z_R-z_L.pA−pB=ρwg(zB−zA)+(ρm−ρw)gh.\boxed{p_A-p_B=\rho_wg(z_B-z_A)+(\rho_m-\rho_w)gh}.

(b) Result and interpretation

pA−pB=1000(10)(.50)+12600(10)(.10)=17600Pa.\boxed{p_A-p_B=1000(10)(.50)+12600(10)(.10)=17600\,\mathrm{Pa}}.For two taps in one static water reservoir,pA−pB=ρwg(zB−zA)⇒(ρm−ρw)gh=0⇒h=0.p_A-p_B=\rho_wg(z_B-z_A)\Rightarrow(\rho_m-\rho_w)gh=0\Rightarrow\boxed{h=0}.

Physical check

The manometer isolates the elevation-corrected pressure difference, which vanishes in a single static water body.