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 \( \frac{20}{9} \, \text{cm} \).