The relationship for the fundamental frequency of a closed organ pipe (length \( L_1 \)) and the first overtone of an open organ pipe (length \( L_2 \)) is given by:
\[ \frac{\lambda}{4} = L_1 \quad \text{and} \quad 2 \left( \frac{\lambda}{2} \right) = \lambda \]
The velocity of sound is \( v \), thus:
\[ v = f \lambda \]
For the closed pipe:
\[ v = f_1 (4L_1) \]
For the open pipe:
\[ f_2 = \frac{v}{2L_2} \]
Equating the fundamental frequency of the closed pipe to the first overtone of the open pipe:
\[ f_1 = f_2 \] \[ \frac{v}{4L_1} = \frac{v}{2L_2} \] \[ L_2 = 4L_1 \]
Given \( L_2 = 60 \, \text{cm} \):
\[ 60 = 4 \times L_1 \] \[ L_1 = 15 \, \text{cm} \]
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)