To solve this problem, we need to find the length of an open tube when the ninth harmonic of a closed tube matches the fourth harmonic of the open tube.
For a closed organ pipe (closed at one end), the formula for the frequency of the nth harmonic is:
\( f_n = \frac{n v_1}{4L_1} \)
where \( n \) is an odd integer, \( v_1 \) is the speed of sound in the gas inside the closed tube, and \( L_1 \) is the length of the closed tube.
For an open organ pipe, the formula for the frequency of the nth harmonic is:
\( f_n = \frac{n v_2}{2L_2} \)
where \( n \) is any integer, \( v_2 \) is the speed of sound in the gas inside the open tube, and \( L_2 \) is the length of the open tube.
Given: The ninth harmonic of the closed tube (\( n=9 \)) matches the fourth harmonic of the open tube (\( n=4 \)):
\( \frac{9 v_1}{4 \times 10} = \frac{4 v_2}{2L_2} \)
Simplifying that:
\( \frac{9 v_1}{40} = \frac{4 v_2}{2L_2} \)
\( \frac{9 v_1}{40} = \frac{2 v_2}{L_2} \)
\( L_2 = \frac{80 v_2}{9 v_1} \)
The speed of sound \( v \) in a medium is given by:
\( v = \sqrt{\frac{B}{\rho}} \)
where \( B \) is the bulk modulus, and \( \rho \) is the density of the gas. Given that the bulk modulus \( B \) is the same for both gases, the speed ratio is:
\( \frac{v_1}{v_2} = \sqrt{\frac{\rho_2}{\rho_1}} \)
Given the density ratio \( \rho_1 : \rho_2 = 1 : 16 \):
\( \frac{v_1}{v_2} = \sqrt{\frac{16}{1}} = 4 \)
Substituting \( \frac{v_1}{v_2} = 4 \) into the equation for \( L_2 \):
\( L_2 = \frac{80 \times v_2}{9 \times 4 \times v_2} = \frac{80}{36} = \frac{20}{9} \, \text{cm} \)
Thus, the length of the open tube is \( \frac{20}{9} \, \text{cm} \).
Speed of sound in a gas: \(v=\sqrt{B/\rho}\). With the same bulk modulus \(B\), the ratio of speeds is \[ \frac{v_1}{v_2}=\sqrt{\frac{\rho_2}{\rho_1}}=\sqrt{16}=4 \] so \(v_1=4v_2\).
For a closed tube (one end closed) the fundamental frequency is \(f_{c1}=\dfrac{v_1}{4L_c}\). If we interpret the “9th harmonic” as the 9th multiple of the fundamental (9th partial, which is allowed because 9 is odd), its frequency is \[ f_{c9}=\frac{9\,v_1}{4L_c}. \]
For an open tube the \(n\)-th harmonic is \[ f_{o n}=\frac{n\,v_2}{2L_o}. \] For the 4th harmonic \[ f_{o4}=\frac{4\,v_2}{2L_o}=\frac{2v_2}{L_o}. \]
Equate the two frequencies: \[ \frac{9v_1}{4L_c}=\frac{2v_2}{L_o}. \] Solve for \(L_o\): \[ L_o=\frac{8L_c\,v_2}{9v_1}. \] Substitute \(v_2/v_1=\tfrac{1}{4}\) and \(L_c=10\ \text{cm}\): \[ L_o=\frac{8\times10\ \text{cm}\times\frac{1}{4}}{9}=\frac{2\times10}{9}\ \text{cm}=\frac{20}{9}\ \text{cm}. \]
\(\displaystyle L_o=\frac{20}{9}\ \text{cm}.\) (Option 3)
Two loudspeakers (\(L_1\) and \(L_2\)) are placed with a separation of \(10 \, \text{m}\), as shown in the figure. Both speakers are fed with an audio input signal of the same frequency with constant volume. A voice recorder, initially at point \(A\), at equidistance to both loudspeakers, is moved by \(25 \, \text{m}\) along the line \(AB\) while monitoring the audio signal. The measured signal was found to undergo \(10\) cycles of minima and maxima during the movement. The frequency of the input signal is _____________ Hz.
(Speed of sound in air is \(324 \, \text{m/s}\) and \( \sqrt{5} = 2.23 \)) 
The equivalent resistance between the points \(A\) and \(B\) in the given circuit is \[ \frac{x}{5}\,\Omega. \] Find the value of \(x\). 
Method used for separation of mixture of products (B and C) obtained in the following reaction is: 
In the following \(p\text{–}V\) diagram, the equation of state along the curved path is given by \[ (V-2)^2 = 4ap, \] where \(a\) is a constant. The total work done in the closed path is: 
Let \( ABC \) be a triangle. Consider four points \( p_1, p_2, p_3, p_4 \) on the side \( AB \), five points \( p_5, p_6, p_7, p_8, p_9 \) on the side \( BC \), and four points \( p_{10}, p_{11}, p_{12}, p_{13} \) on the side \( AC \). None of these points is a vertex of the triangle \( ABC \). Then the total number of pentagons that can be formed by taking all the vertices from the points \( p_1, p_2, \ldots, p_{13} \) is ___________.