Example 1
Tuning fork 440 Hz, v = 343 m/s -> λ ≈ 0.78 m.
Enter wave speed and frequency. The calculator divides v by f and you get the distance between crests. A 440 Hz tuning fork at 343 m/s has λ ≈ 0.78 m, about an arm’s length. When you know λ and f and want v, open v = λ·f.
The inverse of this sum: v = λ·f. Photon energy from f: E = h·f. Doppler: f′ from source motion.
Speed v (m/s) and Frequency f (Hz). The result shows up here.
You stand next to a speaker or an antenna and hear or measure one frequency. The wave also has a speed v in the medium. Wavelength is v divided by f: λ = v/f. That is the distance between successive crests, compressions, or field maxima. In one period T = 1/f the wave advances by one λ, so v = λ/T is the same formula from the other side.
Take a tuning fork from the cupboard. f = 440 Hz, classroom air about 343 m/s. λ = 343/440 ≈ 0.780 m, rounded on the page to 0.78 m. A 1000 Hz tone at the same v drops to 0.343 m. A 50 Hz bass note stretches to 6.86 m: a 20 cm speaker is likely to radiate that poorly, because the cone is much shorter than λ.
The same ratio works for radio and light. FM at 100 MHz with v = 3e8 m/s gives λ = 3 m, hence a dipole around 1.5 m. Wi-Fi at 2.4 GHz is 12.5 cm. Yellow light at f = 5e14 Hz drops to 600 nm. Sound in water is faster, about 1480 m/s, so 1000 Hz already has λ = 1.48 m, not 34 cm.
Frequency and speed have to be positive. At f = 0 you would divide by zero. Period T = 1/f sits beside the result, because it is the same information in seconds: at 440 Hz, T ≈ 0.00227 s. Speed and length follow the metric/US switch. Hertz stays in hertz. When λ falls into the visible range, the result also writes nanometers.
On the form, type v, then f. Air 343 and 440 give 0.78 m. You can type 3e8 and 1e8: you get exactly 3 m. A comma and a period both parse. The chart of λ versus f at fixed v falls as 1/f: higher pitch, shorter wave.
When you know λ and f and want the medium speed, open v = λ·f. When the source is moving, Doppler gives the frequency you hear, then you come back here with f′. A photon from that f is E = h·f, not a length.
λ = v / f
T = 1 / f. f > 0, v > 0.
Crest spacing is λ = v/f. A 440 Hz tuning fork in 343 m/s air has λ ≈ 0.78 m, about an arm length.
Tuning fork 440 Hz, v = 343 m/s -> λ ≈ 0.78 m.
v = 343 m/s, f = 1000 Hz -> λ ≈ 0.34 m.
v = 331 m/s, f = 262 Hz -> λ ≈ 1.26 m.
v = 3e8 m/s, f = 1e8 Hz -> λ = 3 m (dipole).
v = 3e8 m/s, f = 2.4e9 Hz -> λ = 12.5 cm.
v = 3e8 m/s, f = 5e14 Hz -> λ ≈ 600 nm.
v = 1480 m/s, f = 1000 Hz -> λ = 1.48 m.
v = 343 m/s, f = 40000 Hz -> λ ≈ 8.6 mm.
v = 3e8 m/s, f = 8.8e7 Hz -> λ ≈ 3.4 m.
v = 343 m/s, f = 20 Hz -> λ ≈ 17 m.
λ = 343/440 ≈ 0.780 m, about 0.78 m on the page. At 1000 Hz that is 0.343 m.
In air, about 343 m/s at 20 °C. In water, about 1480 m/s. For light in vacuum, 3e8 m/s.
In time T = 1/f the wave advances by one λ, so v = λ/T. Substitute T and you get λ = v/f.
You would divide by zero. Frequency must be positive, or there is no period and no wavelength.
Yes. In vacuum v = c, so λ = c/f. 5e14 Hz gives 600 nm. In glass v is smaller, so λ is shorter at the same f.
When you know λ and f and want the medium speed. That is the v = λ·f page. Here the unknown is λ.
T = 1/f. At 440 Hz that is about 0.00227 s. In that time the wave takes one step of length λ.
2.4e9 Hz. λ = 3e8 / 2.4e9 = 0.125 m, or 12.5 cm, typical Wi-Fi.
When λ falls to about 1e-7 m, as with visible light. Radio stays in meters or centimeters.
No. λ, v and f describe the travel of the wave. Phase is a snapshot shift; amplitude is loudness, not length.
The formula is the school one. Units follow SI; NIST SP 330 and BIPM define the measures, not your result.
Page updated in 2026.