The stationary wave y = 2a sinkx cos`omega`t in a stretched string is the result of superposition of `y_(1)=a sin(kx-omegat)` and

The stationary wave y = 2a sin kx cos omega t in a closed organ pipe is the result of the superposition of y = a sin( omega t — kx) and

The stationary wave y = 2a sin kx cos omega t in a closed organ pipe is the result of the superposition of y = a sin (omega t - kx)

The stationary wave y = 2a sin kx cos omega t in a closed organ pipe is the result of the superposition of y = a sin (omega t - kx)

The resultant ampiltude of a vibrating particle by the superposition of the two waves y_(1) = a sin ( omega t + (pi)/(3)) and y_(2) = a sin omega t is :

A travelling wave in a stretched string is described by the equation y = A sin (kx - omegat) the maximum particle velocity is

A travelling wave in a stretched string is described by the equation y = A sin (kx - omegat) the maximum particle velocity is

The resultant amplitude of a vibrating particle by the superposition of the two waves y_(1)=asin[omegat+(pi)/(3)] and y_(2)=asinomegat is