Wavelength and Frequency — Question 10

Section 16-3 · Physics pages 2450–2451

Question 10 Wavelength bounds propagate through a reciprocal relation A nondispersive wave speed is known exactly as v = 12 m/s. Its frequency is bounded by 19 ≤f ≤21 Hz; these are hard bounds, not standard deviations. f λ The reciprocal frequency-wavelength relation decreases and is curved; axes are schematic. (a) Find exact wavelength bounds. (b) Compare them with the symmetric first-order estimate about f = 20 Hz. Why are the exact bounds asymmetric?
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Question 10 - Solution Wavelength bounds propagate through a reciprocal relation f λ Method and mathematical working Use monotonicity to map the endpoints of the frequency interval. Keep exact hard bounds distinct from a differential estimate of the deviations. dλ df = −v f2 < 0, d2λ df2 = 2v f3 > 0. 12 21 ≤λ ≤12 19 ⇒0.57143 ≤λ ≤0.63158 (m), λ0 = 0.600 m, |δλ| ≃12 202 (1) = 0.030 m. (a) Calculation and conclusion λ = v/f decreases with frequency, so 12/21 ≤λ ≤12/19, or .57143 ≤λ ≤.63158 m. The larger frequency yields the smaller wavelength. (b) Interpretation and limits The central value is .600 m and |dλ| ≈(v/f2)|df| = .030 m. The estimate is .600 ± .030 m. The reciprocal function is curved, making exact upper and lower deviations unequal; hard bounds should use the endpoint calculation. Physical check The positive curvature explains the asymmetric exact interval about the central value. Combining the lowest frequency with the largest wavelength is a necessary ordering check.

Question 10

Wavelength bounds propagate through a reciprocal relation

A nondispersive wave speed is known exactly as v=12m/sv=12\,\mathrm{m/s}. Its frequency is bounded by 19≤f≤21Hz19\le f\le21\,\mathrm{Hz}; these are hard bounds, not standard deviations.

Diagram shown in the original SVG worksheet.

  1. Find exact wavelength bounds.

  2. Compare them with the symmetric first-order estimate about f=20Hzf=20\,\mathrm{Hz}. Why are the exact bounds asymmetric?

Question 10 - Solution

Wavelength bounds propagate through a reciprocal relation

Diagram shown in the original SVG worksheet.

Method and mathematical working

Use monotonicity to map the endpoints of the frequency interval. Keep exact hard bounds distinct from a differential estimate of the deviations.dλdf=−vf2<0,d2λdf2=2vf3>0.1221≤λ≤1219⇒0.57143≤λ≤0.63158(m),λ0=0.600m,|δλ|≃12202(1)=0.030m.\begin{aligned}\frac{d\lambda}{df}&=-\frac v{f^2}<0,\qquad \frac{d^2\lambda}{df^2}=\frac{2v}{f^3}>0.\\[4pt]\frac{12}{21}\le\lambda\le\frac{12}{19}&\Rightarrow0.57143\le\lambda\le0.63158\quad(\mathrm m),\\\lambda_0&=0.600\,\mathrm m,\qquad |\delta\lambda|\simeq\frac{12}{20^2}(1)=0.030\,\mathrm m.\end{aligned}

(a) Calculation and conclusion

λ=v/f\lambda=v/f decreases with frequency, so 12/21≤λ≤12/1912/21\le\lambda\le12/19, or .57143≤λ≤.63158m.57143\le\lambda\le.63158\,\mathrm{m}. The larger frequency yields the smaller wavelength.

(b) Interpretation and limits

The central value is .600m.600\,\mathrm{m} and |dλ|≈(v/f2)|df|=.030m|d\lambda|\approx(v/f^2)|df|=.030\,\mathrm{m}. The estimate is .600±.030m.600\pm.030\,\mathrm{m}. The reciprocal function is curved, making exact upper and lower deviations unequal; hard bounds should use the endpoint calculation.

Physical check

The positive curvature explains the asymmetric exact interval about the central value. Combining the lowest frequency with the largest wavelength is a necessary ordering check.