Infer standing-wave modes from displacement and pressure boundaries
Standing waves can form from oppositely traveling waves in a constrained region. Their nodes remain at fixed positions, while antinodes are locations of maximum oscillation amplitude. An antinode is not permanently at maximum displacement: it passes through equilibrium during each cycle. The allowed wavelengths follow the end conditions, not an arbitrary list of frequencies chosen by the observer.
Learning outcome: Compare all three boundary choices at mode index 2. Read displacement endpoints and, for air, pressure endpoints. Then compare indices 1–4 for the closed-open case and infer the spacing between allowed resonances.
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 an ideal 1.0 m closed-open air column with v=340 m/s, the fundamental is 85 Hz. Allowed-mode index 2 is harmonic 3, with λ=4/3 m and f=255 Hz. A 1.0 m open-open column instead has fundamental 170 Hz and its second mode is 340 Hz.
Open the experimentPredict
Does an open end of an air column impose a pressure node or a displacement node?
Experiment
Compare all three boundary choices at mode index 2. Read displacement endpoints and, for air, pressure endpoints. Then compare indices 1–4 for the closed-open case and infer the spacing between allowed resonances.
Infer resonance from the actual boundary conditions
Worked teaching model · synthetic values · Length 1.0 m. String speed 40 m/s; air speed 340 m/s. Curves are normalized spatial mode shapes, not a snapshot of both pressure and displacement at the same temporal phase. Air end corrections/losses omitted; pressure and displacement nodes are different.
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Normalized displacement mode shape
- 1: air longitudinal 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.
| position along 1 m region (m) | signed spatial shape (normalized) |
|---|---|
| 0 | 0 |
| 0.0125 | 0.058871 |
| 0.025 | 0.11754 |
| 0.0375 | 0.1758 |
| 0.05 | 0.23345 |
| 0.0625 | 0.29028 |
| 0.075 | 0.34612 |
| 0.0875 | 0.40075 |
| 0.1 | 0.45399 |
| 0.1125 | 0.50566 |
| 0.125 | 0.55557 |
| 0.1375 | 0.60356 |
| 0.15 | 0.64945 |
| 0.1625 | 0.69309 |
| 0.175 | 0.73432 |
| 0.1875 | 0.77301 |
| 0.2 | 0.80902 |
| 0.2125 | 0.84222 |
| 0.225 | 0.8725 |
| 0.2375 | 0.89975 |
| 0.25 | 0.92388 |
| 0.2625 | 0.94481 |
| 0.275 | 0.96246 |
| 0.2875 | 0.97677 |
| 0.3 | 0.98769 |
| 0.3125 | 0.99518 |
| 0.325 | 0.99923 |
| 0.3375 | 0.99981 |
| 0.35 | 0.99692 |
| 0.3625 | 0.99057 |
| 0.375 | 0.98079 |
| 0.3875 | 0.9676 |
| 0.4 | 0.95106 |
| 0.4125 | 0.93121 |
| 0.425 | 0.90814 |
| 0.4375 | 0.88192 |
| 0.45 | 0.85264 |
| 0.4625 | 0.8204 |
| 0.475 | 0.78532 |
| 0.4875 | 0.74751 |
| 0.5 | 0.70711 |
| 0.5125 | 0.66425 |
| 0.525 | 0.61909 |
| 0.5375 | 0.57179 |
| 0.55 | 0.5225 |
| 0.5625 | 0.4714 |
| 0.575 | 0.41866 |
| 0.5875 | 0.36447 |
| 0.6 | 0.30902 |
| 0.6125 | 0.25249 |
| 0.625 | 0.19509 |
| 0.6375 | 0.13701 |
| 0.65 | 0.078459 |
| 0.6625 | 0.019634 |
| 0.675 | -0.03926 |
| 0.6875 | -0.098017 |
| 0.7 | -0.15643 |
| 0.7125 | -0.21431 |
| 0.725 | -0.27144 |
| 0.7375 | -0.32763 |
| 0.75 | -0.38268 |
| 0.7625 | -0.43641 |
| 0.775 | -0.48862 |
| 0.7875 | -0.53914 |
| 0.8 | -0.58779 |
| 0.8125 | -0.63439 |
| 0.825 | -0.6788 |
| 0.8375 | -0.72085 |
| 0.85 | -0.76041 |
| 0.8625 | -0.79732 |
| 0.875 | -0.83147 |
| 0.8875 | -0.86273 |
| 0.9 | -0.89101 |
| 0.9125 | -0.91619 |
| 0.925 | -0.93819 |
| 0.9375 | -0.95694 |
| 0.95 | -0.97237 |
| 0.9625 | -0.98443 |
| 0.975 | -0.99307 |
| 0.9875 | -0.99827 |
| 1 | -1 |
Normalized pressure mode shape — separate quantity
- 1: pressure mode — 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.
| position along 1 m air column (m) | signed spatial shape (normalized) |
|---|---|
| 0 | 1 |
| 0.0125 | 0.99827 |
| 0.025 | 0.99307 |
| 0.0375 | 0.98443 |
| 0.05 | 0.97237 |
| 0.0625 | 0.95694 |
| 0.075 | 0.93819 |
| 0.0875 | 0.91619 |
| 0.1 | 0.89101 |
| 0.1125 | 0.86273 |
| 0.125 | 0.83147 |
| 0.1375 | 0.79732 |
| 0.15 | 0.76041 |
| 0.1625 | 0.72085 |
| 0.175 | 0.6788 |
| 0.1875 | 0.63439 |
| 0.2 | 0.58779 |
| 0.2125 | 0.53914 |
| 0.225 | 0.48862 |
| 0.2375 | 0.43641 |
| 0.25 | 0.38268 |
| 0.2625 | 0.32763 |
| 0.275 | 0.27144 |
| 0.2875 | 0.21431 |
| 0.3 | 0.15643 |
| 0.3125 | 0.098017 |
| 0.325 | 0.03926 |
| 0.3375 | -0.019634 |
| 0.35 | -0.078459 |
| 0.3625 | -0.13701 |
| 0.375 | -0.19509 |
| 0.3875 | -0.25249 |
| 0.4 | -0.30902 |
| 0.4125 | -0.36447 |
| 0.425 | -0.41866 |
| 0.4375 | -0.4714 |
| 0.45 | -0.5225 |
| 0.4625 | -0.57179 |
| 0.475 | -0.61909 |
| 0.4875 | -0.66425 |
| 0.5 | -0.70711 |
| 0.5125 | -0.74751 |
| 0.525 | -0.78532 |
| 0.5375 | -0.8204 |
| 0.55 | -0.85264 |
| 0.5625 | -0.88192 |
| 0.575 | -0.90814 |
| 0.5875 | -0.93121 |
| 0.6 | -0.95106 |
| 0.6125 | -0.9676 |
| 0.625 | -0.98079 |
| 0.6375 | -0.99057 |
| 0.65 | -0.99692 |
| 0.6625 | -0.99981 |
| 0.675 | -0.99923 |
| 0.6875 | -0.99518 |
| 0.7 | -0.98769 |
| 0.7125 | -0.97677 |
| 0.725 | -0.96246 |
| 0.7375 | -0.94481 |
| 0.75 | -0.92388 |
| 0.7625 | -0.89975 |
| 0.775 | -0.8725 |
| 0.7875 | -0.84222 |
| 0.8 | -0.80902 |
| 0.8125 | -0.77301 |
| 0.825 | -0.73432 |
| 0.8375 | -0.69309 |
| 0.85 | -0.64945 |
| 0.8625 | -0.60356 |
| 0.875 | -0.55557 |
| 0.8875 | -0.50566 |
| 0.9 | -0.45399 |
| 0.9125 | -0.40075 |
| 0.925 | -0.34612 |
| 0.9375 | -0.29028 |
| 0.95 | -0.23345 |
| 0.9625 | -0.1758 |
| 0.975 | -0.11754 |
| 0.9875 | -0.058871 |
| 1 | -1.837e-16 |
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 |
|---|---|---|
| Allowed harmonic number | 3 | index |
| Wavelength | 1.3333 | m |
| Frequency | 255 | Hz |
| Fundamental frequency | 85 | Hz |
A displacement node at the closed end and antinode at the open end admit only odd harmonics.
The mode index counts allowed patterns; for a closed-open pipe index 2 means harmonic 3, not harmonic 2. Pressure and displacement have complementary spatial node locations and are not identical instantaneous quantities. The plots show normalized spatial factors, not both fields at a shared temporal phase. End corrections and damping are omitted.
A displacement node at the closed end and antinode at the open end admit only odd harmonics.
The mode index counts allowed patterns; for a closed-open pipe index 2 means harmonic 3, not harmonic 2. Pressure and displacement have complementary spatial node locations and are not identical instantaneous quantities. The plots show normalized spatial factors, not both fields at a shared temporal phase. End corrections and damping are omitted.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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