Measuring Pressure — Question 9

Section 14-4 · Physics pages 2128–2129

Question 9 A density calibration error survives perfect height readings A liquid-column gauge is labeled using density ρc = 1000 kg/m3. Its actual liquid density at use is ρa = 960 kg/m3. The measured vertical separation is 0.250 m and g = 10 m/s2. Height and gravity are exact. An exact height reading still requires the correct working-liquid density. (a) Find the indicated and actual pressure differences and the indicated error relative to the true value. (b) If the true pressure difference is held fixed while the liquid density decreases further, does the observed height increase or decrease? Derive the fractional relation for small density changes.
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Question 9 - Solution A density calibration error survives perfect height readings (a) Derivation and calculation ∆pindicated = ρcgh = (1000)(10)(.250) = 2500 Pa . ∆pactual = ρagh = (960)(10)(.250) = 2400 Pa . ∆pindicated −∆pactual ∆pactual = 100 2400 = 4.1667% . (b) Result and interpretation At fixed true pressure difference and gravity, h = ∆p ρg , ρh = constant. ρ dh + h dρ = 0 ⇒dh h = −dρ ρ . A density decrease increases the observed height; exact geometric measurements cannot correct a wrong density calibration. Physical check The small-change relation follows from a differential; for finite changes use h2/h1 = ρ1/ρ2.

Question 9

A density calibration error survives perfect height readings

A liquid-column gauge is labeled using density ρc=1000kg/m3\rho_c=1000\,\mathrm{kg/m^3}. Its actual liquid density at use is ρa=960kg/m3\rho_a=960\,\mathrm{kg/m^3}. The measured vertical separation is 0.250m0.250\,\mathrm{m} and g=10m/s2g=10\,\mathrm{m/s^2}. Height and gravity are exact.

Diagram shown in the original SVG worksheet.

  1. Find the indicated and actual pressure differences and the indicated error relative to the true value.

  2. If the true pressure difference is held fixed while the liquid density decreases further, does the observed height increase or decrease? Derive the fractional relation for small density changes.

Question 9 - Solution

A density calibration error survives perfect height readings

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Δpindicated=ρcgh=(1000)(10)(.250)=2500Pa.\boxed{\Delta p_{\mathrm{indicated}}=\rho_cgh=(1000)(10)(.250)=2500\,\mathrm{Pa}}.Δpactual=ρagh=(960)(10)(.250)=2400Pa.\boxed{\Delta p_{\mathrm{actual}}=\rho_agh=(960)(10)(.250)=2400\,\mathrm{Pa}}.Δpindicated−ΔpactualΔpactual=1002400=4.1667%.\boxed{\frac{\Delta p_{\mathrm{indicated}}-\Delta p_{\mathrm{actual}}}{\Delta p_{\mathrm{actual}}}=\frac{100}{2400}=4.1667\%}.

(b) Result and interpretation

At fixed true pressure difference and gravity,h=Δpρg,ρh=constant.h=\frac{\Delta p}{\rho g},\quad\rho h=\text{constant}.ρdh+hdρ=0⇒dhh=−dρρ.\rho\,dh+h\,d\rho=0\Rightarrow\boxed{\frac{dh}{h}=-\frac{d\rho}{\rho}}.A density decrease increases the observed height; exact geometric measurements cannot correct a wrong density calibration.

Physical check

The small-change relation follows from a differential; for finite changes use h2/h1=ρ1/ρ2h_2/h_1=\rho_1/\rho_2.