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 experimentPredict
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
- 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.
| distance from each pulse center (m) | displacement / incident peak |
|---|---|
| -2 | 0 |
| -1.92 | 0 |
| -1.84 | 0 |
| -1.76 | 0 |
| -1.68 | 0 |
| -1.6 | 0 |
| -1.52 | 0 |
| -1.44 | 0 |
| -1.36 | 0 |
| -1.28 | 0 |
| -1.2 | 0 |
| -1.12 | 0 |
| -1.04 | 0 |
| -0.96 | 0.04 |
| -0.88 | 0.12 |
| -0.8 | 0.2 |
| -0.72 | 0.28 |
| -0.64 | 0.36 |
| -0.56 | 0.44 |
| -0.48 | 0.52 |
| -0.4 | 0.6 |
| -0.32 | 0.68 |
| -0.24 | 0.76 |
| -0.16 | 0.84 |
| -0.08 | 0.92 |
| 0 | 1 |
| 0.08 | 0.92 |
| 0.16 | 0.84 |
| 0.24 | 0.76 |
| 0.32 | 0.68 |
| 0.4 | 0.6 |
| 0.48 | 0.52 |
| 0.56 | 0.44 |
| 0.64 | 0.36 |
| 0.72 | 0.28 |
| 0.8 | 0.2 |
| 0.88 | 0.12 |
| 0.96 | 0.04 |
| 1.04 | 0 |
| 1.12 | 0 |
| 1.2 | 0 |
| 1.28 | 0 |
| 1.36 | 0 |
| 1.44 | 0 |
| 1.52 | 0 |
| 1.6 | 0 |
| 1.68 | 0 |
| 1.76 | 0 |
| 1.84 | 0 |
| 1.92 | 0 |
| 2 | 0 |
| distance from each pulse center (m) | displacement / incident peak |
|---|---|
| -2 | 0 |
| -1.92 | 0 |
| -1.84 | 0 |
| -1.76 | 0 |
| -1.68 | 0 |
| -1.6 | 0 |
| -1.52 | 0 |
| -1.44 | 0 |
| -1.36 | 0 |
| -1.28 | 0 |
| -1.2 | 0 |
| -1.12 | 0 |
| -1.04 | 0 |
| -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 |
| 1.04 | 0 |
| 1.12 | 0 |
| 1.2 | 0 |
| 1.28 | 0 |
| 1.36 | 0 |
| 1.44 | 0 |
| 1.52 | 0 |
| 1.6 | 0 |
| 1.68 | 0 |
| 1.76 | 0 |
| 1.84 | 0 |
| 1.92 | 0 |
| 2 | 0 |
| distance from each pulse center (m) | displacement / incident peak |
|---|---|
| -2 | 0 |
| -1.92 | 0 |
| -1.84 | 0 |
| -1.76 | 0 |
| -1.68 | 0 |
| -1.6 | 0 |
| -1.52 | 0 |
| -1.44 | 0 |
| -1.36 | 0 |
| -1.28 | 0 |
| -1.2 | 0 |
| -1.12 | 0 |
| -1.04 | 0 |
| -0.96 | 0 |
| -0.88 | 0 |
| -0.8 | 0 |
| -0.72 | 0 |
| -0.64 | 0.07862 |
| -0.56 | 0.17235 |
| -0.48 | 0.26607 |
| -0.4 | 0.3598 |
| -0.32 | 0.45352 |
| -0.24 | 0.54725 |
| -0.16 | 0.64098 |
| -0.08 | 0.7347 |
| 0 | 0.82843 |
| 0.08 | 0.7347 |
| 0.16 | 0.64098 |
| 0.24 | 0.54725 |
| 0.32 | 0.45352 |
| 0.4 | 0.3598 |
| 0.48 | 0.26607 |
| 0.56 | 0.17235 |
| 0.64 | 0.07862 |
| 0.72 | 0 |
| 0.8 | 0 |
| 0.88 | 0 |
| 0.96 | 0 |
| 1.04 | 0 |
| 1.12 | 0 |
| 1.2 | 0 |
| 1.28 | 0 |
| 1.36 | 0 |
| 1.44 | 0 |
| 1.52 | 0 |
| 1.6 | 0 |
| 1.68 | 0 |
| 1.76 | 0 |
| 1.84 | 0 |
| 1.92 | 0 |
| 2 | 0 |
Each plot rescales independently. Compare values and units rather than apparent screen angles. Different panels can represent different quantities and are not silently overlaid.
| Quantity | Value | Unit |
|---|---|---|
| Second/first mass-per-length ratio | 2 | ratio |
| Second-medium speed | 7.0711 | m/s |
| Reflected displacement coefficient | -0.17157 | ratio |
| Transmitted displacement coefficient | 0.82843 | ratio |
| Reflected power fraction | 0.029437 | ratio |
| Transmitted power fraction | 0.97056 | ratio |
| Incident wavelength | 2.5 | m |
| Transmitted wavelength | 1.7678 | m |
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.
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