Explain Doppler observations before using a numerical extension
Doppler reasoning concerns the rate at which an observer encounters repeated wavefronts. In the required qualitative treatment, approaching motion raises observed pitch and receding motion lowers it for the stipulated sound geometry. A source and observer moving together with the same velocity have no relative approach and receive the original repetition rate. Source frequency and observed frequency are distinct quantities.
Learning outcome: Compare (source, observer) velocities (40,0), (0,40), (40,40) and (−40,0). Predict higher/lower/same pitch first. Use the optional spacing ledger to explain rather than memorize the signs.
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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At source velocity +40 m/s and stationary observer, forward spacing is (340−40)/500=0.60 m and the optional received frequency is 340/0.60≈566.67 Hz, higher than 500 Hz. If both instead move at +40 m/s, encounter speed is 300 m/s and received frequency returns to 500 Hz.
Open the experimentPredict
If source and observer move right at the same velocity, is the source approaching the observer?
Experiment
Compare (source, observer) velocities (40,0), (0,40), (40,40) and (−40,0). Predict higher/lower/same pitch first. Use the optional spacing ledger to explain rather than memorize the signs.
Explain pitch changes using wavefront spacing
Worked teaching model · synthetic values · Source remains left of observer in stationary air; sound speed 340 m/s, source frequency 500 Hz. Qualitative Doppler reasoning is required; supplied numerical fobs=f(v−vo)/(v−vs) is optional enrichment. Subsonic constant velocities, not relativistic light. No audio playback or traffic experiment.
Reset keeps your prediction, captures and practice history.
Observer held at selected velocity
- 1: supplied numerical illustration — 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.
| source velocity (m/s) | received frequency (Hz) |
|---|---|
| -60 | 425 |
| -58 | 427.14 |
| -56 | 429.29 |
| -54 | 431.47 |
| -52 | 433.67 |
| -50 | 435.9 |
| -48 | 438.14 |
| -46 | 440.41 |
| -44 | 442.71 |
| -42 | 445.03 |
| -40 | 447.37 |
| -38 | 449.74 |
| -36 | 452.13 |
| -34 | 454.55 |
| -32 | 456.99 |
| -30 | 459.46 |
| -28 | 461.96 |
| -26 | 464.48 |
| -24 | 467.03 |
| -22 | 469.61 |
| -20 | 472.22 |
| -18 | 474.86 |
| -16 | 477.53 |
| -14 | 480.23 |
| -12 | 482.95 |
| -10 | 485.71 |
| -8 | 488.51 |
| -6 | 491.33 |
| -4 | 494.19 |
| -2 | 497.08 |
| 0 | 500 |
| 2 | 502.96 |
| 4 | 505.95 |
| 6 | 508.98 |
| 8 | 512.05 |
| 10 | 515.15 |
| 12 | 518.29 |
| 14 | 521.47 |
| 16 | 524.69 |
| 18 | 527.95 |
| 20 | 531.25 |
| 22 | 534.59 |
| 24 | 537.97 |
| 26 | 541.4 |
| 28 | 544.87 |
| 30 | 548.39 |
| 32 | 551.95 |
| 34 | 555.56 |
| 36 | 559.21 |
| 38 | 562.91 |
| 40 | 566.67 |
| 42 | 570.47 |
| 44 | 574.32 |
| 46 | 578.23 |
| 48 | 582.19 |
| 50 | 586.21 |
| 52 | 590.28 |
| 54 | 594.41 |
| 56 | 598.59 |
| 58 | 602.84 |
| 60 | 607.14 |
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 |
|---|---|---|
| Forward wavefront separation | 0.6 | m |
| Source frequency | 500 | Hz |
| Observer encounter frequency — enrichment | 566.67 | Hz |
| Observer minus source velocity | -40 | m/s |
The source-observer separation decreases: the received pitch is higher.
The denominator changes front spacing because emission positions move through the air; observer motion changes the encounter rate. Numerical values and this formula are optional enrichment beyond required qualitative AP2 Doppler reasoning. This is a one-dimensional sound model in stationary air, not a formula for light or supersonic motion.
The source-observer separation decreases: the received pitch is higher.
The denominator changes front spacing because emission positions move through the air; observer motion changes the encounter rate. Numerical values and this formula are optional enrichment beyond required qualitative AP2 Doppler reasoning. This is a one-dimensional sound model in stationary air, not a formula for light or supersonic motion.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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Public practice checks a specific claim. It does not establish independent mastery.
Why can identical received frequency occur both for stationary objects and for co-moving objects?
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