Add signed disturbances and distinguish beats from cancellation
In a linear wave model, disturbances at the same position and time add algebraically. Two pulses pass through one another rather than collide like rigid objects. For example, an upward displacement of 3 mm overlapping a downward displacement of 2 mm gives +1 mm at that instant. After separation, the original pulses continue under the assumed linear, nondissipative model; the overlap is not evidence they bounced.
Learning outcome: Capture frequency differences 0, 2 and 4 Hz at zero phase, then compare 0 and 180° at equal frequency. Check several same-time coordinate rows by adding components yourself. Explain which changes alter beat spacing and which alter phase timing.
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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For 20 Hz and 24 Hz components, beat rate is 4 Hz and the beat period is 0.25 s. At equal 20 Hz with a 180° relative phase, the signed sum at the modeled point is zero throughout, not a sequence of 20 beats per second.
Open the experimentPredict
If two equal-frequency contributions are opposite in phase, will their relative phase gradually drift?
Experiment
Capture frequency differences 0, 2 and 4 Hz at zero phase, then compare 0 and 180° at equal frequency. Check several same-time coordinate rows by adding components yourself. Explain which changes alter beat spacing and which alter phase timing.
Resolve component waves and their signed sum
Worked teaching model · synthetic values · Two equal 1 Pa pressure-amplitude contributions at 20 Hz and 20+Δf Hz at one point. Linear small-amplitude superposition; the sum is not particle travel. Beat rate |Δf|; same-frequency cancellation depends on phase. Silent plotted evidence only.
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Components and their sum at one position
- 1: first component — solid line
- 2: second component — long dashes
- 3: signed sum — 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.
| time (s) | pressure disturbance (Pa) |
|---|---|
| 0 | 0 |
| 0.0125 | 1 |
| 0.025 | 1.2246e-16 |
| 0.0375 | -1 |
| 0.05 | -2.4493e-16 |
| 0.0625 | 1 |
| 0.075 | 3.6739e-16 |
| 0.0875 | -1 |
| 0.1 | -4.8986e-16 |
| 0.1125 | 1 |
| 0.125 | 6.1232e-16 |
| 0.1375 | -1 |
| 0.15 | -7.3479e-16 |
| 0.1625 | 1 |
| 0.175 | 8.5725e-16 |
| 0.1875 | -1 |
| 0.2 | -9.7972e-16 |
| 0.2125 | 1 |
| 0.225 | 1.1022e-15 |
| 0.2375 | -1 |
| 0.25 | -1.2246e-15 |
| 0.2625 | 1 |
| 0.275 | -2.2056e-15 |
| 0.2875 | -1 |
| 0.3 | -1.4696e-15 |
| 0.3125 | 1 |
| 0.325 | -1.9607e-15 |
| 0.3375 | -1 |
| 0.35 | -1.7145e-15 |
| 0.3625 | 1 |
| 0.375 | 5.3897e-15 |
| 0.3875 | -1 |
| 0.4 | -1.9594e-15 |
| 0.4125 | 1 |
| 0.425 | 5.6346e-15 |
| 0.4375 | -1 |
| 0.45 | -2.2044e-15 |
| 0.4625 | 1 |
| 0.475 | 5.8795e-15 |
| 0.4875 | -1 |
| 0.5 | -2.4493e-15 |
| 0.5125 | 1 |
| 0.525 | -9.8096e-16 |
| 0.5375 | -1 |
| 0.55 | 4.4112e-15 |
| 0.5625 | 1 |
| 0.575 | 6.3694e-15 |
| 0.5875 | -1 |
| 0.6 | -2.9392e-15 |
| 0.6125 | 1 |
| 0.625 | -4.911e-16 |
| 0.6375 | -1 |
| 0.65 | 3.9213e-15 |
| 0.6625 | 1 |
| 0.675 | -7.3516e-15 |
| 0.6875 | -1 |
| 0.7 | -3.429e-15 |
| 0.7125 | 1 |
| 0.725 | -1.238e-18 |
| 0.7375 | -1 |
| 0.75 | -1.0779e-14 |
| 0.7625 | 1 |
| 0.775 | 7.3491e-15 |
| 0.7875 | -1 |
| 0.8 | -3.9189e-15 |
| 0.8125 | 1 |
| 0.825 | 1.4699e-14 |
| 0.8375 | -1 |
| 0.85 | -1.1269e-14 |
| 0.8625 | 1 |
| 0.875 | 7.839e-15 |
| 0.8875 | -1 |
| 0.9 | -4.4087e-15 |
| 0.9125 | 1 |
| 0.925 | 9.7848e-16 |
| 0.9375 | -1 |
| 0.95 | -1.1759e-14 |
| 0.9625 | 1 |
| 0.975 | 8.3288e-15 |
| 0.9875 | -1 |
| 1 | -4.8986e-15 |
| time (s) | pressure disturbance (Pa) |
|---|---|
| 0 | 0 |
| 0.0125 | 0.95106 |
| 0.025 | -0.58779 |
| 0.0375 | -0.58779 |
| 0.05 | 0.95106 |
| 0.0625 | 3.6739e-16 |
| 0.075 | -0.95106 |
| 0.0875 | 0.58779 |
| 0.1 | 0.58779 |
| 0.1125 | -0.95106 |
| 0.125 | -7.3479e-16 |
| 0.1375 | 0.95106 |
| 0.15 | -0.58779 |
| 0.1625 | -0.58779 |
| 0.175 | 0.95106 |
| 0.1875 | 1.1022e-15 |
| 0.2 | -0.95106 |
| 0.2125 | 0.58779 |
| 0.225 | 0.58779 |
| 0.2375 | -0.95106 |
| 0.25 | -1.4696e-15 |
| 0.2625 | 0.95106 |
| 0.275 | -0.58779 |
| 0.2875 | -0.58779 |
| 0.3 | 0.95106 |
| 0.3125 | 5.3897e-15 |
| 0.325 | -0.95106 |
| 0.3375 | 0.58779 |
| 0.35 | 0.58779 |
| 0.3625 | -0.95106 |
| 0.375 | -2.2044e-15 |
| 0.3875 | 0.95106 |
| 0.4 | -0.58779 |
| 0.4125 | -0.58779 |
| 0.425 | 0.95106 |
| 0.4375 | -9.8096e-16 |
| 0.45 | -0.95106 |
| 0.4625 | 0.58779 |
| 0.475 | 0.58779 |
| 0.4875 | -0.95106 |
| 0.5 | -2.9392e-15 |
| 0.5125 | 0.95106 |
| 0.525 | -0.58779 |
| 0.5375 | -0.58779 |
| 0.55 | 0.95106 |
| 0.5625 | 6.8593e-15 |
| 0.575 | -0.95106 |
| 0.5875 | 0.58779 |
| 0.6 | 0.58779 |
| 0.6125 | -0.95106 |
| 0.625 | -1.0779e-14 |
| 0.6375 | 0.95106 |
| 0.65 | -0.58779 |
| 0.6625 | -0.58779 |
| 0.675 | 0.95106 |
| 0.6875 | 4.8862e-16 |
| 0.7 | -0.95106 |
| 0.7125 | 0.58779 |
| 0.725 | 0.58779 |
| 0.7375 | -0.95106 |
| 0.75 | -4.4087e-15 |
| 0.7625 | 0.95106 |
| 0.775 | -0.58779 |
| 0.7875 | -0.58779 |
| 0.8 | 0.95106 |
| 0.8125 | 8.3288e-15 |
| 0.825 | -0.95106 |
| 0.8375 | 0.58779 |
| 0.85 | 0.58779 |
| 0.8625 | -0.95106 |
| 0.875 | 1.9619e-15 |
| 0.8875 | 0.95106 |
| 0.9 | -0.58779 |
| 0.9125 | -0.58779 |
| 0.925 | 0.95106 |
| 0.9375 | 1.9582e-15 |
| 0.95 | -0.95106 |
| 0.9625 | 0.58779 |
| 0.975 | 0.58779 |
| 0.9875 | -0.95106 |
| 1 | -5.8783e-15 |
| time (s) | pressure disturbance (Pa) |
|---|---|
| 0 | 0 |
| 0.0125 | 1.9511 |
| 0.025 | -0.58779 |
| 0.0375 | -1.5878 |
| 0.05 | 0.95106 |
| 0.0625 | 1 |
| 0.075 | -0.95106 |
| 0.0875 | -0.41221 |
| 0.1 | 0.58779 |
| 0.1125 | 0.048943 |
| 0.125 | -1.2246e-16 |
| 0.1375 | -0.048943 |
| 0.15 | -0.58779 |
| 0.1625 | 0.41221 |
| 0.175 | 0.95106 |
| 0.1875 | -1 |
| 0.2 | -0.95106 |
| 0.2125 | 1.5878 |
| 0.225 | 0.58779 |
| 0.2375 | -1.9511 |
| 0.25 | -2.6942e-15 |
| 0.2625 | 1.9511 |
| 0.275 | -0.58779 |
| 0.2875 | -1.5878 |
| 0.3 | 0.95106 |
| 0.3125 | 1 |
| 0.325 | -0.95106 |
| 0.3375 | -0.41221 |
| 0.35 | 0.58779 |
| 0.3625 | 0.048943 |
| 0.375 | 3.1853e-15 |
| 0.3875 | -0.048943 |
| 0.4 | -0.58779 |
| 0.4125 | 0.41221 |
| 0.425 | 0.95106 |
| 0.4375 | -1 |
| 0.45 | -0.95106 |
| 0.4625 | 1.5878 |
| 0.475 | 0.58779 |
| 0.4875 | -1.9511 |
| 0.5 | -5.3884e-15 |
| 0.5125 | 1.9511 |
| 0.525 | -0.58779 |
| 0.5375 | -1.5878 |
| 0.55 | 0.95106 |
| 0.5625 | 1 |
| 0.575 | -0.95106 |
| 0.5875 | -0.41221 |
| 0.6 | 0.58779 |
| 0.6125 | 0.048943 |
| 0.625 | -1.127e-14 |
| 0.6375 | -0.048943 |
| 0.65 | -0.58779 |
| 0.6625 | 0.41221 |
| 0.675 | 0.95106 |
| 0.6875 | -1 |
| 0.7 | -0.95106 |
| 0.7125 | 1.5878 |
| 0.725 | 0.58779 |
| 0.7375 | -1.9511 |
| 0.75 | -1.5188e-14 |
| 0.7625 | 1.9511 |
| 0.775 | -0.58779 |
| 0.7875 | -1.5878 |
| 0.8 | 0.95106 |
| 0.8125 | 1 |
| 0.825 | -0.95106 |
| 0.8375 | -0.41221 |
| 0.85 | 0.58779 |
| 0.8625 | 0.048943 |
| 0.875 | 9.8009e-15 |
| 0.8875 | -0.048943 |
| 0.9 | -0.58779 |
| 0.9125 | 0.41221 |
| 0.925 | 0.95106 |
| 0.9375 | -1 |
| 0.95 | -0.95106 |
| 0.9625 | 1.5878 |
| 0.975 | 0.58779 |
| 0.9875 | -1.9511 |
| 1 | -1.0777e-14 |
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 |
|---|---|---|
| First frequency | 20 | Hz |
| Second frequency | 24 | Hz |
| Beat frequency | 4 | Hz |
| Beat period | 0.25 | s |
Different frequencies drift in and out of phase; the beat count follows their frequency difference.
Instantaneous pressure disturbances add with signs. The envelope is not a new carrier traveling at the difference frequency. At equal frequency and 180° phase difference this point’s disturbances cancel, but cancellation at a location does not establish destruction of energy everywhere in the complete source/field system. No audible tone is generated.
Different frequencies drift in and out of phase; the beat count follows their frequency difference.
Instantaneous pressure disturbances add with signs. The envelope is not a new carrier traveling at the difference frequency. At equal frequency and 180° phase difference this point’s disturbances cancel, but cancellation at a location does not establish destruction of energy everywhere in the complete source/field system. No audible tone is generated.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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Why is a small or zero local sum not sufficient to claim the waves destroyed energy everywhere?
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