Skip to main content
Course and syllabus guidance

University Physics II · unit UPII-PREFLIGHT-W

Unnumbered preflight · Waves for E&M and Optics

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.

Extra challenging questions

A selection from this pathway. Open a topic below for its complete practice and challenge set.

Extra challenging · 01

Wave quantities and representations: infer an input with uncertainty

A periodic travelling wave is a disturbance whose pattern repeats over a distance λ in space and a time T at any fixed point, and which carries that pattern forward at speed v = λ/T. Use the supplied topic model Y_out = 2*pi/lam, where Y_out is WAVE NUMBER k (rad m⁻¹). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793. lam is Wavelength λ, measured in m. Keep amp (Amplitude A) = 6 mm; per (Period T) = 0.05 s fixed. For this exercise use only 0.435937 m ≤ lam ≤ 1.81406 m 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 = 4.9218362 rad m⁻¹, with a bounded reading uncertainty ±0.21874 rad m⁻¹. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown lam by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.000137812 m, 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

WAVE NUMBER k against lam

Predictions from the supplied Wave quantities and representations 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): WAVE NUMBER k / rad m⁻¹

WAVE NUMBER k against lamPredictions from the supplied Wave quantities and representations 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: lam: Wavelength λ / m. Vertical axis: WAVE NUMBER k / rad m⁻¹. Exact values are available in the data table below.3.0265.9828.93811.8914.850.38080.75291.1251.4971.869xy

Horizontal axis (x): lam: Wavelength λ / m

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

Reading 1lam: Wavelength λ / m: 0.4359WAVE NUMBER k / rad m⁻¹: 14.41
Read the exact data as a table
WAVE NUMBER k against lam — supplied values
lam: Wavelength λ / mWAVE NUMBER k / rad m⁻¹
0.435937514.4130415648564
0.78046874999999998.050527720910782
1.1255.585053606381854
1.46953124999999974.275639124502856
1.81406253.4635991357406852

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(lam) = 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(0.435937) = 14.413 rad m⁻¹ and Y_out(1.81406) = 3.4636 rad m⁻¹. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives lam_line = 0.435937 + (4.92184 − 14.413)(1.81406 − 0.435937)/(3.4636 − 14.413) = 1.63053 m. 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 lam = 1.27659 m; substituting back gives Y_out = 4.9218362 rad m⁻¹.
  4. The interpolation error in the input is |lam_line − lam| = 0.353931 m. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 4.7030962 rad m⁻¹ and 5.1405762 rad m⁻¹. Sort the roots even if the response decreases: 1.22227 m ≤ lam ≤ 1.33597 m.
  6. The lower and upper input deviations are 0.0543212 m and 0.0593741 m. 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 lam ≈ 1.27659 m; compatible interval [1.22227, 1.33597] m. Endpoint interpolation gives 1.63053 m.

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

Extra challenging · 02

Phase, Superposition & Coherence: infer an input with uncertainty

Superposition is the rule that two waves crossing at a point add their displacements, and the phase difference — how far out of step they are, in radians — decides whether that sum is larger or smaller than either wave alone. Use the supplied topic model Y_out = sqrt(1+a2*a2+2*a2*cosd(360*d+phi0)), where Y_out is RESULTANT A_R (× A₁). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; sqrt(x) means √x; sind/cosd/tand use degrees. phi0 is Source phase offset Δφ₀, measured in °. Keep d (Path difference Δr) = 0.25 λ; a2 (Amplitude ratio A₂/A₁) = 1 × A₁ fixed. For this exercise use only 94.95 ° ≤ phi0 ≤ 265.05 ° 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 = 1.6252968 × A₁, with a bounded reading uncertainty ±0.055926 × A₁. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown phi0 by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.01701 °, 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

RESULTANT A_R against phi0

Predictions from the supplied Phase, Superposition & Coherence 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): RESULTANT A_R / × A₁

RESULTANT A_R against phi0Predictions from the supplied Phase, Superposition & Coherence 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: phi0: Source phase offset Δφ₀ / °. Vertical axis: RESULTANT A_R / × A₁. Exact values are available in the data table below.0.0098960.52611.0421.5582.07588.15134.1180225.9271.9xy

Horizontal axis (x): phi0: Source phase offset Δφ₀ / °

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

Reading 1phi0: Source phase offset Δφ₀ / °: 94.95RESULTANT A_R / × A₁: 0.08637
Read the exact data as a table
RESULTANT A_R against phi0 — supplied values
phi0: Source phase offset Δφ₀ / °RESULTANT A_R / × A₁
94.949999999999990.08636693241118089
137.4750.8050939805765227
1801.414213562373095
222.5251.8307986460666417
265.051.99813431805419

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(phi0) = 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(94.95) = 0.0863669 × A₁ and Y_out(265.05) = 1.99813 × A₁. The target lies between them. On the selected branch the response is strictly increasing.
  2. Endpoint interpolation gives phi0_line = 94.95 + (1.6253 − 0.0863669)(265.05 − 94.95)/(1.99813 − 0.0863669) = 231.877 °. 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 phi0 = 198.711 °; substituting back gives Y_out = 1.6252968 × A₁.
  4. The interpolation error in the input is |phi0_line − phi0| = 33.1657 °. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 1.5693708 × A₁ and 1.6812228 × A₁. Sort the roots even if the response decreases: 193.383 ° ≤ phi0 ≤ 204.409 °.
  6. The lower and upper input deviations are 5.32782 ° and 5.69848 °. 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 phi0 ≈ 198.711 °; compatible interval [193.383, 204.409] °. Endpoint interpolation gives 231.877 °.

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

Extra challenging · 03

Wave functions, speed & dispersion: infer an input with uncertainty

A wave function is a rule y(x, t) giving the displacement of every point of the medium at every instant, and it describes a travelling wave when x and t enter only through the combination x − vt, so the whole shape slides at speed v. Use the supplied topic model Y_out = vg/max(vp,0.01), where Y_out is SPEED RATIO v_g / v_p (dimensionless). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; max(a,b) selects the larger value. vp is Phase speed v_p, measured in m s⁻¹. Keep vg (Group speed v_g) = 1.5 m s⁻¹; t (Time t) = 1.5 s fixed. For this exercise use only 0.871875 m s⁻¹ ≤ vp ≤ 3.62812 m s⁻¹ 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 = 0.58750092, with a bounded reading uncertainty ±0.02611. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown vp by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.000275625 m s⁻¹, 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

SPEED RATIO v_g / v_p against vp

Predictions from the supplied Wave functions, speed & dispersion 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): SPEED RATIO v_g / v_p

SPEED RATIO v_g / v_p against vpPredictions from the supplied Wave functions, speed & dispersion 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: vp: Phase speed v_p / m s⁻¹. Vertical axis: SPEED RATIO v_g / v_p. Exact values are available in the data table below.0.36120.7141.0671.421.7730.76161.5062.252.9943.738xy

Horizontal axis (x): vp: Phase speed v_p / m s⁻¹

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

Reading 1vp: Phase speed v_p / m s⁻¹: 0.8719SPEED RATIO v_g / v_p: 1.72
Read the exact data as a table
SPEED RATIO v_g / v_p against vp — supplied values
vp: Phase speed v_p / m s⁻¹SPEED RATIO v_g / v_p
0.8718751.7204301075268817
1.56093749999999990.9609609609609611
2.250.6666666666666666
2.93906249999999950.5103668261562999
3.6281250.41343669250646

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(vp) = 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(0.871875) = 1.72043 and Y_out(3.62812) = 0.413437. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives vp_line = 0.871875 + (0.587501 − 1.72043)(3.62812 − 0.871875)/(0.413437 − 1.72043) = 3.26105 m s⁻¹. 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 vp = 2.55319 m s⁻¹; substituting back gives Y_out = 0.58750092.
  4. The interpolation error in the input is |vp_line − vp| = 0.707863 m s⁻¹. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 0.56139092 and 0.61361092. Sort the roots even if the response decreases: 2.44455 m s⁻¹ ≤ vp ≤ 2.67193 m s⁻¹.
  6. The lower and upper input deviations are 0.108642 m s⁻¹ and 0.118747 m s⁻¹. 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 vp ≈ 2.55319 m s⁻¹; compatible interval [2.44455, 2.67193] m s⁻¹. Endpoint interpolation gives 3.26105 m s⁻¹.

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

Extra challenging · 04

Wave Energy, Power and Intensity: infer an input with uncertainty

A wave carries energy at the wave speed. Average power is the energy crossing a point per second, ½μvω²A² on a string; intensity spreads that power over the wavefront area, I = P(av)/A(⊥), and both scale as amplitude squared. Use the supplied topic model Y_out = 1/10^((10*n*log(r)+0.0043429*a*(r-1))/20), where Y_out is AMPLITUDE A(r)/A(1 m) (dimensionless). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; log(x) means log₁₀x. r is Microphone distance r, measured in m. Keep n (Spreading exponent n (I ∝ r⁻ⁿ)) = 2; a (Absorption α) = 10 ×10⁻³ m⁻¹ fixed. For this exercise use only 107.144 m ≤ r ≤ 893.856 m 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 = 0.000090945346, with a bounded reading uncertainty ±0.00001171. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown r by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.0786712 m, 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

AMPLITUDE A(r)/A(1 m) against r

Predictions from the supplied Wave Energy, Power and Intensity 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): AMPLITUDE A(r)/A(1 m)

AMPLITUDE A(r)/A(1 m) against rPredictions from the supplied Wave Energy, Power and Intensity 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: r: Microphone distance r / m. Vertical axis: AMPLITUDE A(r)/A(1 m). Exact values are available in the data table below.-2.06e-40.0012730.0027510.004230.00570975.68288.1500.5712.9925.3xy

Horizontal axis (x): r: Microphone distance r / m

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

Reading 1r: Microphone distance r / m: 107.1AMPLITUDE A(r)/A(1 m): 0.00549
Read the exact data as a table
AMPLITUDE A(r)/A(1 m) against r — supplied values
r: Microphone distance r / mAMPLITUDE A(r)/A(1 m)
107.143750.005489683563791768
303.8218750.0007241331007762083
500.50.0001644207569246912
697.17812499999990.0000441509709101146
893.85624999999990.000012880704432217978

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(r) = 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(107.144) = 0.00548968 and Y_out(893.856) = 0.0000128807. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives r_line = 107.144 + (0.0000909453 − 0.00548968)(893.856 − 107.144)/(0.0000128807 − 0.00548968) = 882.643 m. 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 r = 587.038 m; substituting back gives Y_out = 0.000090945346.
  4. The interpolation error in the input is |r_line − r| = 295.604 m. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 0.000079235346 and 0.00010265535. Sort the roots even if the response decreases: 569.042 m ≤ r ≤ 607.691 m.
  6. The lower and upper input deviations are 17.9966 m and 20.6523 m. 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 r ≈ 587.038 m; compatible interval [569.042, 607.691] m. Endpoint interpolation gives 882.643 m.

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

Choose a topic