Air column in two identical tubes is vibrating. Tube A has one end closed and tube B has both ends open. Neglecting end correction, the ratio of the fundamental frequency of air column in tube A to that in tube B is
For a closed-end tube:
fA = \(\frac {v}{4L}\)
For an open-end tube:
fB = \(\frac {v}{2L}\)
Where fA and fB are the fundamental frequencies of Tube A and Tube B, v is the speed of sound in air, and L is the length of the tubes.
We are given that the tubes are identical, which means their lengths are the same (LA = LB = L).
Taking the ratio of fA to fB, we have:
\(\frac {f_A}{f_B}\) = \(\frac {v/4L}{v/2L}\)
\(\frac {f_A}{f_B}\) = \(\frac {v}{4L}\) x \(\frac {2L}{v}\)
\(\frac {f_A}{f_B}\) = \(\frac {1}{2}\)
Therefore, the ratio of the fundamental frequency of the air column in Tube A to that in Tube B is 1:2, or option (D) 1:2.
A sub-atomic particle of mass \( 10^{-30} \) kg is moving with a velocity of \( 2.21 \times 10^6 \) m/s. Under the matter wave consideration, the particle will behave closely like (h = \( 6.63 \times 10^{-34} \) J.s)