Ambulance 30 m/s toward you
f = 700 Hz, vs = 30, vo = 0 -> f′ ≈ 767 Hz.
Enter source frequency, source speed toward you, and observer speed toward the source. Blank c = 343 m/s (air).
Wavelength: λ = v/f. Wave speed: v = λ·f. Sound level: dB.
Enter values. The result shows up here.
An ambulance comes toward you and the siren sounds higher. The source packs waves ahead of itself. The usual high-school 1D formula: f′ = f · (c + vo) / (c − vs). This is not relativistic radar, and not ultrasound at an angle: a straight line, for sound or water.
Sign: positive vs means the source approaches you. Positive vo means you walk toward the source. Both positive raise f′. Negative vs (the ambulance has passed) drops the pitch. With vs = vo = 0 you get f′ = f: a check that nothing shifts when both are still.
Default c = 343 m/s (air, about 20°C). Water sonar: type 1480. For radar or light you may enter c of light, but this non-relativistic model breaks when v is close to c.
We reject vs ≥ c, because the denominator c − vs would hit zero or go negative. The old shortcut f·(1+v/c) was only a small-v approximation; here you get the full ratio. Δf = f′ − f sits beside it: positive means a higher pitch.
Speeds follow the header (m/s or ft/s). f stays in Hz. A blank c means 343 m/s; blank vs or vo means zero.
f′ = f · (c + vo) / (c − vs)
Positive vs, vo: approach. vs < c. Blank c = 343 m/s.
f = 700 Hz, vs = 30, vo = 0 -> f′ ≈ 767 Hz.
f = 700 Hz, vs = -30, vo = 0 -> f′ ≈ 644 Hz.
f = 440 Hz, vs = 0, vo = 2 -> f′ ≈ 443 Hz.
f = 500 Hz, vs = 20, vo = 5 -> f′ ≈ 536 Hz.
f = 440 Hz, vs = 40, vo = 0 -> f′ ≈ 498 Hz.
vs = vo = 0, f = 1000 Hz -> f′ = 1000 Hz.
sonar f = 40000, vs = 5, c = 1480 -> f′ ≈ 40136 Hz.
f = 523 Hz, vs = 8, vo = 0 -> f′ ≈ 535 Hz.
f′ = f·(c+vo)/(c−vs). Positive speeds mean approach. The usual 1D school formula, not one with a beam angle.
We use 343 m/s, a typical speed of sound in air at 20°C. In water type 1480.
The denominator c − vs would hit zero. In this model the source does not catch its own wave; vs must stay below c.
No. This is the classical version (sound, water). Light with v near c needs the relativistic formula, which is not here.
The source recedes from the observer. Waves stretch, pitch drops. Ambulance after it passes: vs negative.
No. c is wave speed relative to a still medium. Wind would change effective c and needs a different model.
f·(1+v/c) is an approximation when v is much smaller than c. Here you get the full school ratio, better at a 30 m/s siren.
It is f′ − f. Positive means higher pitch (approach). Negative means lower. At rest Δf = 0.
No. Source frequency must be positive. Blank vs and vo are allowed and mean zero.
Compute f′, then λ = c/f′ on the wavelength page, using the same c as here.