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SCIENCE · INVESTIGATE AND EXPLAIN

Read a wave snapshot without mistaking it for particle travel

A wave transports a disturbance and energy through space. In the small-amplitude string model, a marked piece of string moves transversely about its equilibrium position while the pattern travels horizontally. It does not ride along with a crest. Longitudinal sound instead involves local motion parallel to propagation and alternating pressure compressions and rarefactions; the pressure profile is not a picture of the air itself moving across the entire room.

Learning outcome: Capture F=10 and 40 N at 4 Hz, then 40 N at 8 Hz. Predict speed, spatial spacing and temporal period before checking. Compare corresponding crests between the two snapshots while tracking the separate x=0 element.

Starting recap

Distinguish spatial and temporal axes, signed disturbances, material boundaries and exact versus approximate wave geometry. Identify supplied numerical enrichment before applying it.

All lessons are open directly. Your saved experiments remain when you leave and return.

Try

At F=40 N and μ=0.10 kg/m, v=20 m/s. With f=4 Hz, λ=5 m and T=0.25 s. Doubling frequency to 8 Hz leaves v unchanged but halves λ to 2.5 m and T to 0.125 s. A 0.05 s snapshot shift moves the pattern 1 m, not each string element 1 m.

Open the experiment

Predict

If frequency doubles at fixed tension, will a crest move twice as fast?

Experiment

Capture F=10 and 40 N at 4 Hz, then 40 N at 8 Hz. Predict speed, spatial spacing and temporal period before checking. Compare corresponding crests between the two snapshots while tracking the separate x=0 element.

Separate spatial snapshots from time traces

Worked teaching model · synthetic values · Ideal string mass per length 0.10 kg/m, small transverse displacement amplitude 0.02 m; v=√(F/μ), wavelength v/f. Spatial and temporal plots have independent horizontal units. A marked element oscillates without traveling with the disturbance.

Reset keeps your prediction, captures and practice history.

Two spatial snapshots

0120.019999-0.02position (m)transverse displacement (m)
  • 1: t=0 s — solid line
  • 2: t=0.05 s — long dashes
Accessible coordinates for this panel

These tables sample up to 82 displayed coordinates per series, including both endpoints. Fine curves may contain additional calculated points between table entries; use the ledger for exact analytic minima, frequencies or other named evidence. Values are synthetic, not instrument readings.

t=0 s
position (m)transverse displacement (m)
00
0.150.0052685
0.30.010165
0.450.014343
0.60.017508
0.750.019437
0.90.019992
1.050.019135
1.20.016926
1.350.013522
1.50.0091621
1.650.0041553
1.8-0.001145
1.95-0.0063645
2.1-0.011134
2.25-0.015118
2.4-0.018033
2.55-0.019675
2.7-0.019926
2.85-0.01877
3-0.016288
3.15-0.012656
3.3-0.0081293
3.45-0.0030284
3.60.0022863
3.750.0074396
3.90.012067
4.050.015843
4.20.018499
4.350.019848
4.50.019795
4.650.018344
4.80.015597
4.950.011748
5.10.0070698
5.250.0018916
5.4-0.0034201
5.55-0.0084902
5.7-0.012961
5.85-0.016515
6-0.018904
6.15-0.019956
6.3-0.019599
6.45-0.017858
6.6-0.014855
6.75-0.010803
6.9-0.005987
7.05-0.00074864
7.20.0045427
7.350.009513
7.50.013811
7.650.017134
7.80.019246
7.950.019999
8.10.019339
8.250.017313
8.40.014064
8.550.0098212
8.70.0048847
8.85-0.00039682
9-0.0056503
9.15-0.010505
9.3-0.014617
9.45-0.017697
9.6-0.019526
9.75-0.019976
9.9-0.019016
10.05-0.016711
10.2-0.013227
10.35-0.0088076
10.5-0.0037663
10.650.001541
10.80.0067394
10.950.011462
11.10.015374
11.250.018201
11.40.019742
11.550.019888
11.70.01863
11.850.016055
120.012346
t=0.05 s
position (m)transverse displacement (m)
0-0.019021
0.15-0.016721
0.3-0.01324
0.45-0.0088237
0.6-0.003784
0.750.0015231
0.90.0067225
1.050.011447
1.20.015363
1.350.018194
1.50.019739
1.650.01989
1.80.018636
1.950.016066
2.10.01236
2.250.0077816
2.40.0026534
2.55-0.0026623
2.7-0.0077899
2.85-0.012367
3-0.016071
3.15-0.018639
3.3-0.019891
3.45-0.019738
3.6-0.01819
3.75-0.015357
3.9-0.01144
4.05-0.0067141
4.2-0.0015141
4.350.0037928
4.50.0088317
4.650.013247
4.80.016726
4.950.019024
5.10.019978
5.250.01952
5.40.017684
5.550.014599
5.70.010482
5.850.0056245
60.0003699
6.15-0.0049108
6.3-0.0098446
6.45-0.014083
6.6-0.017326
6.75-0.019346
6.9-0.019999
7.05-0.019239
7.2-0.01712
7.35-0.013792
7.5-0.0094893
7.65-0.0045164
7.80.00077555
7.950.0060127
8.10.010825
8.250.014873
8.40.01787
8.550.019605
8.70.019955
8.850.018895
90.0165
9.150.01294
9.30.0084658
9.450.0033936
9.6-0.0019184
9.75-0.0070949
9.9-0.01177
10.05-0.015614
10.2-0.018355
10.35-0.019799
10.5-0.019845
10.65-0.018488
10.8-0.015826
10.95-0.012046
11.1-0.0074146
11.25-0.0022596
11.40.0030551
11.550.0081539
11.70.012677
11.850.016304
120.01878

One marked element at x=0

010.02-0.02time (s)transverse displacement (m)
  • 1: element displacement — solid line
Accessible coordinates for this panel

These tables sample up to 82 displayed coordinates per series, including both endpoints. Fine curves may contain additional calculated points between table entries; use the ledger for exact analytic minima, frequencies or other named evidence. Values are synthetic, not instrument readings.

element displacement
time (s)transverse displacement (m)
00
0.0125-0.0061803
0.025-0.011756
0.0375-0.01618
0.05-0.019021
0.0625-0.02
0.075-0.019021
0.0875-0.01618
0.1-0.011756
0.1125-0.0061803
0.125-2.4493e-18
0.13750.0061803
0.150.011756
0.16250.01618
0.1750.019021
0.18750.02
0.20.019021
0.21250.01618
0.2250.011756
0.23750.0061803
0.254.8986e-18
0.2625-0.0061803
0.275-0.011756
0.2875-0.01618
0.3-0.019021
0.3125-0.02
0.325-0.019021
0.3375-0.01618
0.35-0.011756
0.3625-0.0061803
0.375-7.3479e-18
0.38750.0061803
0.40.011756
0.41250.01618
0.4250.019021
0.43750.02
0.450.019021
0.46250.01618
0.4750.011756
0.48750.0061803
0.59.7972e-18
0.5125-0.0061803
0.525-0.011756
0.5375-0.01618
0.55-0.019021
0.5625-0.02
0.575-0.019021
0.5875-0.01618
0.6-0.011756
0.6125-0.0061803
0.625-1.2246e-17
0.63750.0061803
0.650.011756
0.66250.01618
0.6750.019021
0.68750.02
0.70.019021
0.71250.01618
0.7250.011756
0.73750.0061803
0.751.4696e-17
0.7625-0.0061803
0.775-0.011756
0.7875-0.01618
0.8-0.019021
0.8125-0.02
0.825-0.019021
0.8375-0.01618
0.85-0.011756
0.8625-0.0061803
0.875-1.7145e-17
0.88750.0061803
0.90.011756
0.91250.01618
0.9250.019021
0.93750.02
0.950.019021
0.96250.01618
0.9750.011756
0.98750.0061803
11.9594e-17

Each plot rescales independently. Compare values and units rather than apparent screen angles. Different panels can represent different quantities and are not silently overlaid.

Calculated evidence ledger — original synthetic model
QuantityValueUnit
Propagation speed14.142m/s
Wavelength3.5355m
Period0.25s
Displacement amplitude0.02m

A spatial crest spacing gives wavelength; one element’s repeat time gives period. Neither is the path of matter carried with a crest.

The disturbance travels +x. Tension sets speed independently of the selected source frequency. Higher frequency shortens wavelength at fixed tension. The fixed amplitude does not determine frequency; energy comparisons require specifying the medium, amplitude and frequency, not just counting visible crests.

A spatial crest spacing gives wavelength; one element’s repeat time gives period. Neither is the path of matter carried with a crest.

The disturbance travels +x. Tension sets speed independently of the selected source frequency. Higher frequency shortens wavelength at fixed tension. The fixed amplitude does not determine frequency; energy comparisons require specifying the medium, amplitude and frequency, not just counting visible crests.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

Establish the model and evidence

A wave transports a disturbance and energy through space. In the small-amplitude string model, a marked piece of string moves transversely about its equilibrium position while the pattern travels horizontally. It does not ride along with a crest. Longitudinal sound instead involves local motion parallel to propagation and alternating pressure compressions and rarefactions; the pressure profile is not a picture of the air itself moving across the entire room.

A position graph at one instant measures wavelength between corresponding crests. A time graph at one fixed position measures period between corresponding repetitions. Their horizontal axes have different physical units, so a slope or spacing cannot be transferred from one graph without interpretation. Frequency is reciprocal period and propagation speed satisfies v=fλ. Displacement amplitude is independent of those repeat intervals.

For an ideal stretched string, speed is √(F/μ), where F is tension and μ is mass per length. Changing the source frequency while preserving tension and density changes wavelength, not the medium speed. Changing tension while keeping frequency fixed changes speed and wavelength together. The model stipulates small oscillations and fixed μ=0.10 kg/m; its computed values are not measurements of a real string.

Energy depends on more than the visual height of one trace. At fixed string properties and frequency, larger oscillation amplitude carries more energy; at fixed displacement amplitude, increasing frequency also increases the motion and energy transfer. Do not apply that comparison while silently changing all other quantities, or confuse pressure amplitude in sound with displacement amplitude on a string. The model plots two spatial snapshots and a separate marked-element time trace so the distinction remains visible.

Work a reference case

At F=40 N and μ=0.10 kg/m, v=20 m/s. With f=4 Hz, λ=5 m and T=0.25 s. Doubling frequency to 8 Hz leaves v unchanged but halves λ to 2.5 m and T to 0.125 s. A 0.05 s snapshot shift moves the pattern 1 m, not each string element 1 m.

Predict before investigating

If frequency doubles at fixed tension, will a crest move twice as fast?

Capture F=10 and 40 N at 4 Hz, then 40 N at 8 Hz. Predict speed, spatial spacing and temporal period before checking. Compare corresponding crests between the two snapshots while tracking the separate x=0 element.

Transfer to changed conditions

A different ideal string has tension 9 N, mass per length 0.010 kg/m and source frequency 6 Hz. Find speed and wavelength; explain what changes if frequency doubles.

Compare your reasoning

Speed is √900=30 m/s and wavelength is 5 m. At 12 Hz, speed remains 30 m/s and wavelength becomes 2.5 m under unchanged medium assumptions.

Reflect and qualify the evidence

Which observation distinguishes propagation speed from a marked element’s oscillation?

Separate sound speed, pitch and pressure amplitude

For the same ordinary gas under comparable conditions, higher temperature increases sound speed. The source frequency determines perceived pitch, while larger pressure-variation amplitude generally produces louder sound; neither is the distance that the whole gas moves across the room. The energy comparisons above hold other relevant wave and medium parameters fixed.

Predict and check: an ideal sound packet has equilibrium pressure 100 kPa and pressure variation ±0.20 kPa. Its pressure amplitude is 0.20 kPa, not 100.20 kPa. Doubling that variation raises amplitude while leaving a stipulated 500 Hz pitch unchanged. A separate supplied medium change raises sound speed from 330 to 360 m/s at the same frequency; wavelength changes from 0.660 to 0.720 m. Sketch compressions and rarefactions with particle displacement parallel to propagation, contrasting the transverse string drawing. No loud audio or physical exposure is requested. (Current clauses 14.1.A and 14.2.A.)

Sources and boundaries

Original text, calculations and diagrams; checked 30 October 2026 against the current AP Physics 2 course framework and primary textbook verification. Controls generate virtual evidence, not actual measurements or independent practical competence. No lasers, sunlight focusing, loud audio, traffic observations or chemical-film preparation are requested. Public feedback is practice; retain your derivation and critique in the course evidence workspace.

Clause-level source/action reconciliation checked 31 October 2026 against the linked current framework and Fall 2026 clarification. Added packets are original virtual comparisons; no new practical or learner-completion claim.

Apply

For μ=0.10 kg/m, F=40 N and f=4 Hz, the wavelength is:

Public practice checks a specific claim. It does not establish independent mastery.

Which observation distinguishes propagation speed from a marked element’s oscillation?

Continue

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