Thermal Expansion — Question 8

Section 18-5 · Physics pages 2906–2907

Question 8 A warming pendulum clock loses time A small-angle pendulum clock is calibrated at temperature T0. Its rod expands as L = L0(1 + α∆T) with α = 20.0 × 10−6 K−1. Use P = 2π √ L/g, with constant g. The clock counts oscillations and assigns each its original calibrated duration. The operating temperature is 40.0 K above T0. L(T) Rod expansion is exaggerated; small-angle motion is assumed. (a) Find the period ratio and the indicated time after a true 86400 s. (b) Find the first-order daily time loss and compare it with the exact modeled result. State the sign of the error.
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Question 8 - Solution A warming pendulum clock loses time L(T) (a) Method and calculation P P0 = √ 1 + .000020(40) = √ 1.0008. tindicated = tP0 P = 86400 √ 1.0008 s ≈86365.461 s. The clock loses approximately 34.539 s. (b) Interpretation and further calculation (1 + ϵ)−1/2 ≃1 −ϵ/2, ϵ = α∆T. t −tindicated ≃tα∆T 2 = 34.560 s. The first-order loss exceeds the exact loss by about .021 s; the clock runs slow because each real oscillation takes longer. Physical check Clock time scales inversely with the actual period, not proportionally to it.

Question 8

A warming pendulum clock loses time

A small-angle pendulum clock is calibrated at temperature T0T_0. Its rod expands as L=L0(1+αΔT)L=L_0(1+\alpha\Delta T) with α=20.0×10−6K−1\alpha=20.0\times10^{-6}\,\mathrm{K^{-1}}. Use P=2πL/gP=2\pi\sqrt{L/g}, with constant gg. The clock counts oscillations and assigns each its original calibrated duration. The operating temperature is 40.0K40.0\,\mathrm K above T0T_0.

Diagram shown in the original SVG worksheet.

  1. Find the period ratio and the indicated time after a true 86400s86400\,\mathrm s.

  2. Find the first-order daily time loss and compare it with the exact modeled result. State the sign of the error.

Question 8 - Solution

A warming pendulum clock loses time

Diagram shown in the original SVG worksheet.

(a) Method and calculation

PP0=1+.000020(40)=1.0008.\frac P{P_0}=\sqrt{1+.000020(40)}=\sqrt{1.0008}.tindicated=tP0P=864001.0008s≈86365.461s.t_{\mathrm{indicated}}=t\frac{P_0}{P}=\frac{86400}{\sqrt{1.0008}}\,\mathrm s\approx86365.461\,\mathrm s.The clock loses approximately 34.53934.539 s.

(b) Interpretation and further calculation

(1+ϵ)−1/2≃1−ϵ/2,ϵ=αΔT.(1+\epsilon)^{-1/2}\simeq1-\epsilon/2,\quad\epsilon=\alpha\Delta T.t−tindicated≃tαΔT2=34.560s.t-t_{\mathrm{indicated}}\simeq\frac{t\alpha\Delta T}{2}=34.560\,\mathrm s.The first-order loss exceeds the exact loss by about .021.021 s; the clock runs slow because each real oscillation takes longer.

Physical check

Clock time scales inversely with the actual period, not proportionally to it.