To determine the length of an open tube, we equate the ninth harmonic frequency of a closed tube to the fourth harmonic frequency of an open tube.
For a closed organ pipe (closed at one end), the harmonic frequency formula is:
\( f_n = \frac{n v_1}{4L_1} \)
where \( n \) is an odd integer, \( v_1 \) is the speed of sound in the closed tube's gas, and \( L_1 \) is its length.
For an open organ pipe, the harmonic frequency formula is:
\( f_n = \frac{n v_2}{2L_2} \)
where \( n \) is any integer, \( v_2 \) is the speed of sound in the open tube's gas, and \( L_2 \) is its length.
Given that 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 the equation:
\( \frac{9 v_1}{40} = \frac{4 v_2}{2L_2} \)
\( \frac{9 v_1}{40} = \frac{2 v_2}{L_2} \)
Rearranging to solve for \( L_2 \):
\( L_2 = \frac{80 v_2}{9 v_1} \)
The speed of sound \( v \) in a medium is defined as:
\( v = \sqrt{\frac{B}{\rho}} \)
where \( B \) is the bulk modulus and \( \rho \) is the gas density. Assuming identical bulk moduli \( B \) for both gases, the speed ratio is:
\( \frac{v_1}{v_2} = \sqrt{\frac{\rho_2}{\rho_1}} \)
With the given density ratio \( \rho_1 : \rho_2 = 1 : 16 \):
\( \frac{v_1}{v_2} = \sqrt{\frac{16}{1}} = 4 \)
Substituting the speed ratio \( \frac{v_1}{v_2} = 4 \) into the equation for \( L_2 \):
\( L_2 = \frac{80 \times v_2}{9 \times 4 \times v_2} = \frac{80}{36} = \frac{20}{9} \, \text{cm} \)
Therefore, the length of the open tube is \( \frac{20}{9} \, \text{cm} \).