For light, when the relative speed is much smaller than the speed of light, calculate the Doppler shift using . Multiply the emitted frequency by (v/c) to obtain the magnitude of the frequency change.
This is part of C.5 Doppler effect and applies to both SL and HL. Here, is the emitted frequency, is the change in observed frequency, is the radial relative speed, and .
The mechanism is that motion changes the rate at which successive wavefronts reach the observer. During approach, wavefronts arrive more frequently; during recession, they arrive less frequently. The speed of light remains in a vacuum: the Doppler effect changes the observed frequency and wavelength, not the propagation speed.
Rearranging gives:
Only the component of relative velocity along the line joining the source and observer is used.
If motion is not directly along the line of sight, use the radial component rather than the total speed. For transverse motion in this non-relativistic approximation, , so there is no first-order shift. This prevents overestimating the shift.
The fractional shift is dimensionless, so frequency units cancel before multiplication.
| Relative motion | Frequency and wavelength changes |
|---|---|
| Source and observer approach | , so ; wavelength decreases (blue shift) |
| Source and observer recede | , so ; wavelength increases () |
For example, a galaxy emitting light at recedes at . The magnitude of the shift is
Because the galaxy is receding, , giving
A common misconception is that frequency and wavelength shift in the same signed direction. Since , an increased frequency means a decreased wavelength; for small shifts, .
In an IB Calculate response, state the equation, substitute SI values, show the result, and interpret approach or recession. Do not use this approximation when is comparable to ; a relativistic expression is then required.
