2l, 2l/2, 2l/3
Reason — In fig. 1, we know l = . Hence, λ = 2l
In fig. 2, l = Hence, λ =
In fig. 3, l = . Hence, λ =
So, we get, the wavelength of different modes in Figure (1), (2) and (3) as 2l, ,
2l, 2l/2, 2l/3
Reason — In fig. 1, we know l = . Hence, λ = 2l
In fig. 2, l = Hence, λ =
In fig. 3, l = . Hence, λ =
So, we get, the wavelength of different modes in Figure (1), (2) and (3) as 2l, ,