Back to WAVES
JEE PHYSICS MCQ: WAVES
1
Medium
1 of 1
Understanding
+4 | -1
The reason for introducing Laplace correction in the expression for the velocity of sound in a gaseous medium is:
View answer and explanation
Correct option: B
No change in the heat of the medium during the propagation of the sound through it
Option B (No change in the heat of the medium during the propagation of the sound through it) is correct because Laplace's correction assumes adiabatic conditions where no heat exchange occurs during sound propagation.
More Questions from WAVES
Practice All Chapter MCQs →
The source of sound generating a frequency of reaches an observer with a speed of times, the velocity of sound in air. The frequency heard by the observer is
A source of sound emits waves with frequency and speed . Two observers move away from this source in opposite directions each with a speed relative to the source. The ratio of frequencies heard by the two observers will be
Assertion: The wave function of a pulse is given by it propagates in -direction.
Reason: The given wave function is of the form which represent a wave travelling in negative -direction. In the fundamental mode, time taken by the wave to reach the closed end of the air filled pipe is . the fundamental frequency is A rope long has a total mass of . It is stretched with a constant tension of wt. If it is fixed at one end and shaken by hand at the other end, what frequency of shaking will make it break up into three vibrating segments? Take . If is the reverberation time of an auditorium of volume then
Reason: The given wave function is of the form which represent a wave travelling in negative -direction. In the fundamental mode, time taken by the wave to reach the closed end of the air filled pipe is . the fundamental frequency is A rope long has a total mass of . It is stretched with a constant tension of wt. If it is fixed at one end and shaken by hand at the other end, what frequency of shaking will make it break up into three vibrating segments? Take . If is the reverberation time of an auditorium of volume then
