(455) HL Doppler effect equations [IB Physics HL]
Overview of the Doppler Effect
The Doppler effect occurs when a source of sound moves relative to an observer.
When the source moves towards a stationary observer, wave fronts are compressed, resulting in a smaller wavelength and a higher frequency.
Conversely, when the source moves away, the wave fronts are stretched, leading to a larger wavelength and a lower frequency.
Key Equation
The fundamental equation is:[ V = F \Lambda ]
Where:
V = wave speed
F = frequency
( \Lambda ) = wavelength
Inverse relationship:
If wavelength decreases (source approaches), frequency increases.
If wavelength increases (source moves away), frequency decreases.
Observed Frequency Equation
For a moving source:[ F' = F \times \frac{V}{V \pm U_s} ]
Variables:
F' = observed frequency
F = emitted frequency
V = speed of sound (approx. 330 m/s)
U_s = speed of the source
Adding or subtracting depends on the source's direction:
Use the minus sign (V - U_s) when the source approaches (to increase frequency).
Moving Observer Equation
For a moving observer:[ F' = F \times \frac{V \pm U_o}{V} ]
Where:
U_o = speed of the observer
Again, the choice between plus or minus depends on desired frequency outcome.
Example Problem
A car approaches a stationary observer at 10 m/s; the observed frequency is 450 Hz.
Question: What is the emitted frequency F?
Given:
V = 330 m/s
U_s = 10 m/s
Substituting into the equation:[ F' = F \times \frac{330}{330 - 10} ]
Simplifying: ( F' = F \times \frac{330}{320} \approx 1.03125 F )
Solving for F: ( F = \frac{450}{1.03125} \approx 436.364 )
Rounded to significant figures: ( F \approx 440 Hz )
Conclusion
The Doppler effect equations allow for calculation of observed and emitted frequencies based on the movement of sources and observers.
Understanding when to add or subtract (in both equations) is essential for correctly determining the frequency shifts.