Density and Pressure — Question 9

Section 14-2 · Physics pages 2088–2089

Question 9 Bounds on a quotient are asymmetric A mass is bounded by 98 ≤m ≤102 g and its volume by 49 ≤V ≤51 cm3. These are hard independent bounds, not standard deviations. The nominal values are 100 g and 50 cm3. V m 49 51 98 102 Independent bounds define an allowed rectangle. Opposite corners give the extreme quotients; units are cm3 and g. (a) Find the tight density interval and compare it with the nominal density. (b) Can a material of density 2.10 g/cm3 satisfy both bounds? Explain why simply adding or averaging the measurement endpoints would fail.
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Question 9 - Solution Bounds on a quotient are asymmetric V m 49 51 98 102 (a) Derivation and calculation ρ = m/V, ∂ρ ∂m = 1/V > 0, ∂ρ ∂V = −m/V 2 < 0. ρmin = 98/51 = 1.92157 , ρmax = 102/49 = 2.08163 g/cm3. ρnominal = 2.00000, ∆ρ−= −.07843, ∆ρ+ = +.08163. (b) Result and interpretation 2.10 > 2.08163 ⇒2.10 g/cm3 is incompatible . The tight extrema pair small mass with large volume, and large mass with small volume. Averaging endpoints supplies a central value, not a guaranteed bound. Physical check The asymmetric interval arises from the reciprocal dependence on volume, even though the input intervals are symmetric.

Question 9

Bounds on a quotient are asymmetric

A mass is bounded by 98≤m≤102g98\le m\le102\,\mathrm{g} and its volume by 49≤V≤51cm349\le V\le51\,\mathrm{cm^3}. These are hard independent bounds, not standard deviations. The nominal values are 100g100\,\mathrm{g} and 50cm350\,\mathrm{cm^3}.

Diagram shown in the original SVG worksheet.

  1. Find the tight density interval and compare it with the nominal density.

  2. Can a material of density 2.10g/cm32.10\,\mathrm{g/cm^3} satisfy both bounds? Explain why simply adding or averaging the measurement endpoints would fail.

Question 9 - Solution

Bounds on a quotient are asymmetric

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

ρ=m/V,∂ρ∂m=1/V>0,∂ρ∂V=−m/V2<0.\rho=m/V,\qquad\frac{\partial\rho}{\partial m}=1/V>0,\quad\frac{\partial\rho}{\partial V}=-m/V^2<0.ρmin=98/51=1.92157,ρmax=102/49=2.08163g/cm3.\boxed{\rho_{\min}=98/51=1.92157},\quad\boxed{\rho_{\max}=102/49=2.08163}\quad\mathrm{g/cm^3}.ρnominal=2.00000,Δρ−=−.07843,Δρ+=+.08163.\rho_{\mathrm{nominal}}=2.00000,\quad\Delta\rho_-=-.07843,\quad\Delta\rho_+=+.08163.

(b) Result and interpretation

2.10>2.08163⇒2.10g/cm3is incompatible.2.10>2.08163\Rightarrow\boxed{2.10\,\mathrm{g/cm^3}\ \text{is incompatible}}.The tight extrema pair small mass with large volume, and large mass with small volume. Averaging endpoints supplies a central value, not a guaranteed bound.

Physical check

The asymmetric interval arises from the reciprocal dependence on volume, even though the input intervals are symmetric.