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SCIENCE · INVESTIGATE AND EXPLAIN

Explain inversion without confusing amplitude and transmitted energy

A pulse approaching a join can produce both reflected and transmitted disturbances. For two ideal strings under the same tension, the denser string has lower wave speed. Reflection from the slower side is inverted; reflection from a faster side is not. Equal strings have no reflected pulse in this idealization. Fixed-end and free-end reflection are useful limiting cases, not evidence that every boundary has the same sign.

Learning outcome: Compare density-ratio choices 0, 2 and 4 at 4 Hz. Retain sign, width and both power fractions. Then double frequency at one boundary and identify which coefficients stay fixed and which wavelengths change.

Starting recap

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

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Try

For density ratio μ2/μ1=4 and v1=10 m/s, v2=5 m/s. The optional coefficients are r=−1/3 and t=2/3; reflected power is 1/9 and transmitted power is 8/9. At 4 Hz, wavelengths are 2.5 m and 1.25 m, with unchanged frequency.

Open the experiment

Predict

Can a transmitted displacement amplitude exceed the incident amplitude while total power remains conserved?

Experiment

Compare density-ratio choices 0, 2 and 4 at 4 Hz. Retain sign, width and both power fractions. Then double frequency at one boundary and identify which coefficients stay fixed and which wavelengths change.

Audit a reflected and transmitted pulse

Worked teaching model · synthetic values · Joined ideal strings under equal tension; first wave speed 10 m/s. Required qualitative phase and frequency reasoning; supplied displacement reflection/transmission and power coefficients are optional enrichment. No physical tensioned-string activity.

Reset keeps your prediction, captures and practice history.

Separated pulse shapes, drawn around their own centers

-221-0.17157distance from each pulse center (m)displacement / incident peak
  • 1: incident reference — solid line
  • 2: reflected — long dashes
  • 3: transmitted, width scales with speed — short 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.

incident reference
distance from each pulse center (m)displacement / incident peak
-20
-1.920
-1.840
-1.760
-1.680
-1.60
-1.520
-1.440
-1.360
-1.280
-1.20
-1.120
-1.040
-0.960.04
-0.880.12
-0.80.2
-0.720.28
-0.640.36
-0.560.44
-0.480.52
-0.40.6
-0.320.68
-0.240.76
-0.160.84
-0.080.92
01
0.080.92
0.160.84
0.240.76
0.320.68
0.40.6
0.480.52
0.560.44
0.640.36
0.720.28
0.80.2
0.880.12
0.960.04
1.040
1.120
1.20
1.280
1.360
1.440
1.520
1.60
1.680
1.760
1.840
1.920
20
reflected
distance from each pulse center (m)displacement / incident peak
-20
-1.920
-1.840
-1.760
-1.680
-1.60
-1.520
-1.440
-1.360
-1.280
-1.20
-1.120
-1.040
-0.96-0.0068629
-0.88-0.020589
-0.8-0.034315
-0.72-0.04804
-0.64-0.061766
-0.56-0.075492
-0.48-0.089218
-0.4-0.10294
-0.32-0.11667
-0.24-0.1304
-0.16-0.14412
-0.08-0.15785
0-0.17157
0.08-0.15785
0.16-0.14412
0.24-0.1304
0.32-0.11667
0.4-0.10294
0.48-0.089218
0.56-0.075492
0.64-0.061766
0.72-0.04804
0.8-0.034315
0.88-0.020589
0.96-0.0068629
1.040
1.120
1.20
1.280
1.360
1.440
1.520
1.60
1.680
1.760
1.840
1.920
20
transmitted, width scales with speed
distance from each pulse center (m)displacement / incident peak
-20
-1.920
-1.840
-1.760
-1.680
-1.60
-1.520
-1.440
-1.360
-1.280
-1.20
-1.120
-1.040
-0.960
-0.880
-0.80
-0.720
-0.640.07862
-0.560.17235
-0.480.26607
-0.40.3598
-0.320.45352
-0.240.54725
-0.160.64098
-0.080.7347
00.82843
0.080.7347
0.160.64098
0.240.54725
0.320.45352
0.40.3598
0.480.26607
0.560.17235
0.640.07862
0.720
0.80
0.880
0.960
1.040
1.120
1.20
1.280
1.360
1.440
1.520
1.60
1.680
1.760
1.840
1.920
20

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
Second/first mass-per-length ratio2ratio
Second-medium speed7.0711m/s
Reflected displacement coefficient-0.17157ratio
Transmitted displacement coefficient0.82843ratio
Reflected power fraction0.029437ratio
Transmitted power fraction0.97056ratio
Incident wavelength2.5m
Transmitted wavelength1.7678m

Reflection is inverted on entering the slower string.

The plotted centered pulses are separated events, not three pulses simultaneously superposed at one location. The transmitted amplitude may exceed the incident amplitude without power gain: speed/impedance changes the power conversion. Coefficient calculations are supplied enrichment; phase inversion, continuous frequency and changed wavelength are the core comparisons.

Reflection is inverted on entering the slower string.

The plotted centered pulses are separated events, not three pulses simultaneously superposed at one location. The transmitted amplitude may exceed the incident amplitude without power gain: speed/impedance changes the power conversion. Coefficient calculations are supplied enrichment; phase inversion, continuous frequency and changed wavelength are the core comparisons.

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

Understand

Establish the model and evidence

A pulse approaching a join can produce both reflected and transmitted disturbances. For two ideal strings under the same tension, the denser string has lower wave speed. Reflection from the slower side is inverted; reflection from a faster side is not. Equal strings have no reflected pulse in this idealization. Fixed-end and free-end reflection are useful limiting cases, not evidence that every boundary has the same sign.

The source frequency remains continuous across a stationary boundary. Because speeds differ, wavelengths differ in the same ratio as speed. A pulse of a given duration is spatially narrower in the slower string. In the plot, pulses are centered separately to compare shape and sign: they are not three contributions occupying one place at the same time, so adding those displayed profiles would misinterpret the diagram.

The supplied quantitative coefficients are optional enrichment beyond the core qualitative boundary reasoning. With speeds v1 and v2 and equal tension, reflected displacement coefficient r=(v2−v1)/(v2+v1), while transmitted coefficient t=1+r. These follow displacement continuity and the string boundary constraints. The signs refer to displacement relative to the incident pulse, not to negative energy.

Power fractions are r² and (v1/v2)t² in this equal-tension model. They add to one, even when the transmitted displacement amplitude exceeds the incoming amplitude. A different medium converts displacement amplitude to energy flux differently. Therefore a tall transmitted pulse alone is not an energy-creation claim, and squaring both displacement coefficients without the speed factor would give a wrong ledger. No physical string tension or apparatus is requested.

Work a reference case

For density ratio μ2/μ1=4 and v1=10 m/s, v2=5 m/s. The optional coefficients are r=−1/3 and t=2/3; reflected power is 1/9 and transmitted power is 8/9. At 4 Hz, wavelengths are 2.5 m and 1.25 m, with unchanged frequency.

Predict before investigating

Can a transmitted displacement amplitude exceed the incident amplitude while total power remains conserved?

Compare density-ratio choices 0, 2 and 4 at 4 Hz. Retain sign, width and both power fractions. Then double frequency at one boundary and identify which coefficients stay fixed and which wavelengths change.

Transfer to changed conditions

A stationary equal-tension join has wave speeds 12 and 6 m/s with source frequency 3 Hz. Predict reflection sign and both wavelengths before using any coefficient formula.

Compare your reasoning

The reflected pulse is inverted. Incident wavelength is 4 m and transmitted wavelength is 2 m; frequency remains 3 Hz. The optional coefficients would again be −1/3 and 2/3.

Reflect and qualify the evidence

Why must an energy ledger use the boundary’s conversion factors rather than just add squared plotted heights?

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.

Apply

When a string pulse reaches a slower string at equal tension, the reflected displacement is:

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

Why must an energy ledger use the boundary’s conversion factors rather than just add squared plotted heights?

Continue

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