![]() ![]() If the source moves toward the observer, equation 16.14 16.14 16.14 predicts a higher observed frequency, f t ′ f_ Δ + < Δ − ĭ) It depends on the original frequency, f f f.Į) It depends on the source velocity, v v v. ![]() Consider the case of a stationary observer and a source moving with constant velocity (less than the speed of sound) and emitting a sound of frequency f f f. ![]()
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