The frequencies of vibration for pipes depend on whether they are open or closed. For a closed organ pipe, the frequency for the \( n \)-th mode is given by:
\[
f_n = \frac{n v}{4 L}
\]
Where:
- \( n \) is the harmonic number (for the 3rd mode, \( n = 3 \)),
- \( v \) is the speed of sound in air,
- \( L \) is the length of the pipe.
For an open organ pipe, the frequency for the \( n \)-th mode is given by:
\[
f_n = \frac{n v}{2 L}
\]
Now, comparing the frequency for the 3rd mode in both cases:
- For the closed pipe, \( f_{\text{closed}} = \frac{3 v}{4 L} \),
- For the open pipe, \( f_{\text{open}} = \frac{3 v}{2 L} \).
The ratio of the frequencies is:
\[
\frac{f_{\text{closed}}}{f_{\text{open}}} = \frac{\frac{3 v}{4 L}}{\frac{3 v}{2 L}} = \frac{1}{2}
\]
Thus, the ratio of the frequencies is \( 1:2 \), meaning the open pipe's frequency is twice that of the closed pipe for the 3rd mode.