Given Information: 9th harmonic of closed pipe: $\frac{9V_1}{4l_1}$ 4th harmonic of open pipe: $\frac{2V_2}{l_2}$ Step 1: Equate the frequencies The problem states that the 9th harmonic of the closed pipe is equal to the 4th harmonic of the open pipe. Therefore, we can write: \[ \frac{9V_1}{4l_1} = \frac{2V_2}{l_2} \]
Explanation: This equation sets the frequencies of the two harmonics equal to each other, which is a crucial step in relating the properties of the two pipes.
Step 2: Substitute the velocity expressions We know that the velocity of sound in a medium is given by $V = \sqrt{\frac{B}{\rho}}$, where $B$ is the bulk modulus and $\rho$ is the density. Substituting this into the previous equation, we get: \[ \frac{9}{4l_1} \sqrt{\frac{B}{\rho_1}} = \frac{2}{l_2} \sqrt{\frac{B}{\rho_2}} \]
Explanation: This step replaces the velocities $V_1$ and $V_2$ with their expressions in terms of bulk modulus and density, allowing us to relate the densities of the media in the pipes.
Step 3: Rearrange to find the ratio of lengths Rearranging the equation to find the ratio $\frac{l_2}{l_1}$, we get: \[ \frac{l_2}{l_1} = \frac{8}{9} \sqrt{\frac{\rho_1}{\rho_2}} \]
Explanation: This isolates the ratio of the lengths of the two pipes in terms of the ratio of the square roots of their densities.
Step 4: Substitute given values and solve for $l_2$ We are given that $l_2 = l_1 \times \frac{8}{9} \times \frac{1}{4}$. Substituting this into the equation, we get: \[ l_2 = l_1 \times \frac{8}{9} \times \frac{1}{4} = \frac{20}{9} \text{ cm} \]
Explanation: This step substitutes the given numerical values and simplifies the expression to find the value of $l_2$ in centimeters.
Final Result: The length of the open pipe $l_2$ is $\frac{20}{9}$ 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)
The steam volatile compounds among the following are: