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University Physics I · topic UPI-EXT-WS.07

Sound waves and the speed of sound

Connect the ideas, make your working visible, and test the result. Use the hints when you need a starting point; open the full solution after your attempt.

Further practice

Work through a fresh case before tackling the extension.

Further practice · 01

Sound Waves & the Speed of Sound: predict a finite change

A sound wave is a longitudinal disturbance in which fluid elements oscillate along the direction of propagation; the compressions and rarefactions that result travel at v = √(B/ρ), set by the medium's stiffness and density alone. Use the supplied topic model Y_out = (331+0.6*th)/f, where Y_out is WAVELENGTH λ (m). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793. f is Frequency f, measured in Hz. Keep th (Air temperature θ) = 20 °C; s (Displacement s(max)) = 10 μm fixed. For this exercise use only 347.813 Hz ≤ f ≤ 702.188 Hz on this continuous branch. A grid of test settings is an input restriction for this exercise, not by itself a claim of physical quantisation. This calculation retains the topic model's stated assumptions; it does not extend them to a different physical setup. Calculate Y_out at f = 425.775 Hz and 475.387 Hz. Find the signed output change ΔY_out and the average sensitivity ΔY_out/Δf across this interval. State whether the response increases or decreases; distinguish this interval average from a derivative at one point.

Explore the question data

WAVELENGTH λ against f

Predictions from the supplied Sound Waves & the Speed of Sound model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law.

Vertical axis (y): WAVELENGTH λ / m

WAVELENGTH λ against fPredictions from the supplied Sound Waves & the Speed of Sound model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law. Horizontal axis: f: Frequency f / Hz. Vertical axis: WAVELENGTH λ / m. Exact values are available in the data table below.0.46860.60290.73730.87171.006333.6429.3525620.7716.4xy

Horizontal axis (x): f: Frequency f / Hz

Axes show the supplied calibration interval; the origin may lie outside the plot.

Reading 1f: Frequency f / Hz: 347.8WAVELENGTH λ / m: 0.9862
Read the exact data as a table
WAVELENGTH λ against f — supplied values
f: Frequency f / HzWAVELENGTH λ / m
347.81250.9861635220125786
436.406250.7859649122807018
5250.6533333333333333
613.593750.5590017825311943
702.18750.4884735202492212

These are the supplied values, not a worked answer. No fitted trend is drawn.

Show a hint

Substitute each value of f separately while keeping every other input fixed, then subtract in the same order.

Reveal the worked solution
  1. At f = 425.775 Hz, substitute into Y_out = (331+0.6*th)/f: Y₀ = 0.80559 m.
  2. At f = 475.387 Hz, the same fixed-parameter model gives Y₁ = 0.721517 m.
  3. Signed change: ΔY_out = Y₁ − Y₀ = -0.0840731 m; the input change is Δf = 49.6125 Hz.
  4. Average sensitivity is ΔY_out/Δf = -0.0016946 m per Hz. Its negative sign means that this response decreases over the specified interval.
  5. This is a secant slope between two settings. It equals a point derivative only for a locally linear relation or in a justified small-interval limit.

Answer Y₀ = 0.80559 m, Y₁ = 0.721517 m; ΔY_out = -0.0840731 m; average sensitivity = -0.0016946 m per Hz.

Compare the assumptions, method and units with your attempt. Explain any correction before trying another question.

Extra challenging questions

Work through the linked stages and explain what each result means.

Extra challenging · 01

Sound Waves & the Speed of Sound: infer an input with uncertainty

A sound wave is a longitudinal disturbance in which fluid elements oscillate along the direction of propagation; the compressions and rarefactions that result travel at v = √(B/ρ), set by the medium's stiffness and density alone. Use the supplied topic model Y_out = (331+0.6*th)/f, where Y_out is WAVELENGTH λ (m). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793. f is Frequency f, measured in Hz. Keep th (Air temperature θ) = 20 °C; s (Displacement s(max)) = 10 μm fixed. For this exercise use only 347.813 Hz ≤ f ≤ 702.188 Hz on this continuous branch. A grid of test settings is an input restriction for this exercise, not by itself a claim of physical quantisation. This calculation retains the topic model's stated assumptions; it does not extend them to a different physical setup. A reading gives Y_out = 0.60817625 m, with a bounded reading uncertainty ±0.017955 m. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown f by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.0354375 Hz, using a numerical bracket if required. Find the full input interval consistent with the bounded reading uncertainty and compare it with a symmetric input-error assumption. Do not assume that the supplied calibration points prove monotonicity outside this branch.

Explore the question data

WAVELENGTH λ against f

Predictions from the supplied Sound Waves & the Speed of Sound model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law.

Vertical axis (y): WAVELENGTH λ / m

WAVELENGTH λ against fPredictions from the supplied Sound Waves & the Speed of Sound model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law. Horizontal axis: f: Frequency f / Hz. Vertical axis: WAVELENGTH λ / m. Exact values are available in the data table below.0.46860.60290.73730.87171.006333.6429.3525620.7716.4xy

Horizontal axis (x): f: Frequency f / Hz

Axes show the supplied calibration interval; the origin may lie outside the plot.

Reading 1f: Frequency f / Hz: 347.8WAVELENGTH λ / m: 0.9862
Read the exact data as a table
WAVELENGTH λ against f — supplied values
f: Frequency f / HzWAVELENGTH λ / m
347.81250.9861635220125786
436.406250.7859649122807018
5250.6533333333333333
613.593750.5590017825311943
702.18750.4884735202492212

These are the supplied values, not a worked answer. No fitted trend is drawn.

Show a hint

The model's endpoint predictions bracket the reading. Solve Y_out(f) = Y_measured and then solve again at Y_measured − u and Y_measured + u; a nonlinear inverse can give unequal input deviations.

Reveal the worked solution
  1. Endpoint predictions are Y_out(347.813) = 0.986164 m and Y_out(702.188) = 0.488474 m. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives f_line = 347.813 + (0.608176 − 0.986164)(702.188 − 347.813)/(0.488474 − 0.986164) = 616.954 Hz. This estimates the inverse of the endpoint chord, rather than assuming that chord is the physical model.
  3. Use the actual equation, not the chord, and bracket its root. Evaluating the midpoint and retaining the sign-changing half-interval gives f = 563.981 Hz; substituting back gives Y_out = 0.60817625 m.
  4. The interpolation error in the input is |f_line − f| = 52.9732 Hz. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 0.59022125 m and 0.62613125 m. Sort the roots even if the response decreases: 547.808 Hz ≤ f ≤ 581.138 Hz.
  6. The lower and upper input deviations are 16.1728 Hz and 17.1568 Hz. They differ because the inverse response is nonlinear; a symmetric error bar would only be a local approximation. This interval includes reading uncertainty only, not model error or uncertainty in fixed inputs.

Answer f ≈ 563.981 Hz; compatible interval [547.808, 581.138] Hz. Endpoint interpolation gives 616.954 Hz.

Compare the assumptions, method and units with your attempt. Explain any correction before trying another question.