The fundamental frequency \(f\) of a stretched string is given by \( f = \frac{1}{2L}\sqrt{\frac{T}{\mu}} \), where \(L\) is the length of the string, \(T\) is the tension, and \( \mu \) is the linear mass density (mass per unit length).
Since tension \(T\) and linear mass density \( \mu \) are constant for the wire and its segments (assuming the wire is uniform), we can write \( f \propto \frac{1}{L} \), or \( L \propto \frac{1}{f} \).
Let \(L\) be the total length of the original wire, and \(L_1, L_2, L_3\) be the lengths of the three segments.
Then \( L = L_1 + L_2 + L_3 \).
Since \( L \propto 1/f \), let \( L = C/f \), \( L_1 = C/f_1 \), \( L_2 = C/f_2 \), \( L_3 = C/f_3 \), where C is a constant of proportionality \( (\frac{1}{2}\sqrt{T/\mu})^{-1} \).
Substituting these into the length equation:
\[ \frac{C}{f} = \frac{C}{f_1} + \frac{C}{f_2} + \frac{C}{f_3} \]
Assuming \( C \ne 0 \), we can divide by C:
\[ \frac{1}{f} = \frac{1}{f_1} + \frac{1}{f_2} + \frac{1}{f_3} \]
This matches option (3).