Measuring Things — Question 9

Section 1-1 · Physics pages 28–29

Question 9 The volume that the water actually measures A fully submerged, nonabsorbing solid object is measured by water displacement. The initial reading is Vi = 40.0 ± 0.5 mL and the final reading is Vf = 57.0 ± 0.5 mL. Each ± is a hard reading-error bound. 40.0 mL Before 57.0 mL After immersion External air bubbles Schematic only. Object and attached external bubbles are fully below the water surface. External air bubbles cling to the submerged object. A separate check bounds their total volume as Vb = 3.0 ± 1.0 mL at the same immersion conditions. Assume no spill, evaporation, trapped water change, or other displacement contribution. The supplied physical model is Vf −Vi = Vobject + Vb. (a) Find the central estimate of the object’s volume. How would neglecting the bubbles bias the result? (b) Compute the smallest and largest object volumes allowed by all three bounds, without statis- tical cancellation assumptions. (c) After carefully removing the external bubbles, predict the central final water reading if the initial volume is unchanged. Explain why repeating the original bubble-contaminated mea- surement many times is not an adequate substitute for this control.
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Question 9 - Solution The volume that the water actually measures 40.0 mL Before 57.0 mL After immersion External air bubbles (a) Correct the quantity being measured. The central water rise is 57.0 −40.0 = 17.0 mL, but it includes the bubbles: Vobject = 57.0 −40.0 −3.0 = 14.0 mL . Neglecting the bubbles would give 17.0 mL, an overestimate of 3.0 mL for the central inputs. (b) Take the worst permitted combinations. δVo ≤δVf + δVi + δVb = 0.5 + 0.5 + 1.0 = 2.0 mL. The intervals are Vf ∈[56.5, 57.5], Vi ∈[39.5, 40.5], and Vb ∈[2.0, 4.0] mL. Hence Vmin = 56.5 −40.5 −4.0 = 12.0 mL, Vmax = 57.5 −39.5 −2.0 = 16.0 mL. Therefore Vobject ∈[12.0, 16.0] mL , equivalently a central estimate of 14.0 mL with a worst-case bound of 2.0 mL. The three absolute bounds add; no independence or probability model was supplied. (c) Remove the nuisance contribution. With no external bubbles, the predicted central final reading is 40.0 + 14.0 = 54.0 mL . This is a central prediction, not an uncertainty-free new measurement. Repeated readings with persistent bubbles can be highly consistent yet still measure object-plus-bubble volume. A control that removes bubbles addresses this mechanism; repetition alone does not.

Question 9

The volume that the water actually measures

A fully submerged, nonabsorbing solid object is measured by water displacement. The initial reading is Vi=40.0±0.5V_i=40.0\pm0.5 mL and the final reading is Vf=57.0±0.5V_f=57.0\pm0.5 mL. Each ±\pm is a hard reading-error bound.

Diagram shown in the original SVG worksheet.

External air bubbles cling to the submerged object. A separate check bounds their total volume as Vb=3.0±1.0V_b=3.0\pm1.0 mL at the same immersion conditions. Assume no spill, evaporation, trapped water change, or other displacement contribution. The supplied physical model is Vf−Vi=Vobject+Vb.V_f-V_i=V_{\mathrm{object}}+V_b.

  1. Find the central estimate of the object’s volume. How would neglecting the bubbles bias the result?

  2. Compute the smallest and largest object volumes allowed by all three bounds, without statistical cancellation assumptions.

  3. After carefully removing the external bubbles, predict the central final water reading if the initial volume is unchanged. Explain why repeating the original bubble-contaminated measurement many times is not an adequate substitute for this control.

Question 9 - Solution

The volume that the water actually measures

Diagram shown in the original SVG worksheet.

(a) Correct the quantity being measured.

The central water rise is 57.0−40.0=17.057.0-40.0=17.0 mL, but it includes the bubbles: Vobject=57.0−40.0−3.0=14.0mL.\boxed{V_{\mathrm{object}}=57.0-40.0-3.0=14.0\ \mathrm{mL}}. Neglecting the bubbles would give 17.017.0 mL, an overestimate of 3.03.0 mL for the central inputs.

(b) Take the worst permitted combinations.

δVo≤δVf+δVi+δVb=0.5+0.5+1.0=2.0mL.\delta V_o\le\delta V_f+\delta V_i+\delta V_b=0.5+0.5+1.0=2.0\ \mathrm{mL}.

The intervals are Vf∈[56.5,57.5]V_f\in[56.5,57.5], Vi∈[39.5,40.5]V_i\in[39.5,40.5], and Vb∈[2.0,4.0]V_b\in[2.0,4.0] mL. Hence Vmin=56.5−40.5−4.0=12.0mL,V_{\min}=56.5-40.5-4.0=12.0\ \mathrm{mL}, Vmax=57.5−39.5−2.0=16.0mL.V_{\max}=57.5-39.5-2.0=16.0\ \mathrm{mL}. Therefore Vobject∈[12.0,16.0]mL\boxed{V_{\mathrm{object}}\in[12.0,16.0]\ \mathrm{mL}}, equivalently a central estimate of 14.014.0 mL with a worst-case bound of 2.02.0 mL. The three absolute bounds add; no independence or probability model was supplied.

(c) Remove the nuisance contribution.

With no external bubbles, the predicted central final reading is 40.0+14.0=54.0mL40.0+14.0=\boxed{54.0\ \mathrm{mL}}. This is a central prediction, not an uncertainty-free new measurement. Repeated readings with persistent bubbles can be highly consistent yet still measure object-plus-bubble volume. A control that removes bubbles addresses this mechanism; repetition alone does not.