A loudspeaker producing sound of constant frequency is placed near the open end of a pipe, as shown in Fig. 4.1. [Figure 4.1] A movable piston is at distance x from the open end of the pipe. Distance x is increased from x = 0 by moving the piston to the left with a constant speed of 0.75cms⁻¹. The speed of the sound in the pipe is 340ms⁻¹.
- (a)(i)Define the wavelength of a progressive wave.[1]
- (a)(ii)State what is meant by an antinode of a stationary wave.[1]
- (b)(i)A much louder sound is first heard when x = 4.5cm. Assume that there is an antinode of a stationary wave at the open end of the pipe. Determine the frequency of the sound in the pipe.[3]
- (b)(ii)After a time interval, a second much louder sound is heard. Calculate the time interval between the first louder sound and the second louder sound being heard.[2]
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Mark scheme
Marking points from the official mark scheme (May/June 2018). The mark or mark type is shown in brackets.
- [B1] distance moved by wavefront/energy during one cycle/oscillation/period (of source) OR minimum distance between two wavefronts OR distance between two adjacent wavefronts
- [B1] (position where) maximum amplitude
- [C1] λ = 4 × 0.045 (= 0.18 (m) or 18 (cm))
- [C1] v = fλ
- [A1] f = 340/0.18 = 1900 Hz
- [C1] distance = λ/2 (= 0.09 (m) or 9 (cm))
- [A1] time = 0.09/0.0075 = 12 s
- OR
- (C1) t = 4.5/0.75 and t = 13.5/0.75
- (A1) time = 18 – 6 = 12 s
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