Step 1: Recall the frequency of a closed organ pipe.
The fundamental frequency of a closed organ pipe is given by: \[ f_{\text{closed}} = \frac{v}{4L_{\text{closed}}}, \] where: \( v \) is the speed of sound in air, \( L_{\text{closed}} \) is the length of the closed organ pipe. Substitute \( L_{\text{closed}} = 20 \, \mathrm{cm} = 0.2 \, \mathrm{m} \): \[ f_{\text{closed}} = \frac{v}{4 \cdot 0.2} = \frac{v}{0.8}. \]
Step 2: Recall the frequency of the second overtone of an open pipe.
For an organ pipe open at both ends, the frequency of the second overtone (third harmonic) is: \[ f_{\text{open, overtone}} = \frac{3v}{2L_{\text{open}}}, \] where \( L_{\text{open}} \) is the length of the open pipe.
Step 3: Equate the frequencies.
Given that the fundamental frequency of the closed pipe is equal to the second overtone of the open pipe: \[ \frac{v}{0.8} = \frac{3v}{2L_{\text{open}}}. \] Simplify by canceling \( v \) from both sides: \[ \frac{1}{0.8} = \frac{3}{2L_{\text{open}}}. \] Rearrange to find \( L_{\text{open}} \): \[ L_{\text{open}} = \frac{3 \cdot 0.8}{2} = 1.2 \, \mathrm{m}. \] Thus, the length of the open organ pipe is \( \mathbf{1.2 \, \mathrm{m}} \).
Given, the function \( f(x) = \frac{a^x + a^{-x}}{2} \) (\( a > 2 \)), then \( f(x+y) + f(x-y) \) is equal to