When a string of length 'l' is divided into three segments of length $l_{1}$, $l_{2}$ and $l_{3}$, the fundamental frequencies of three segments are $n_{1}$, $n_{2}$ and $n_{3}$ respectively. The original fundamental frequency 'n' of the string is
Show Hint
Logic Tip: This is similar to calculating equivalent resistance for resistors in parallel, but applied to frequency and length.
Concept:
For a stretched string vibrating in its fundamental mode:
\[
n \propto \frac{1}{l}
\]
or,
\[
n = \frac{k}{l}
\]
where $k$ is a constant (depends on tension and linear density).
Step 1: Express length in terms of frequency
\[
l = \frac{k}{n}
\]
For three parts:
\[
l_1 = \frac{k}{n_1}, \quad l_2 = \frac{k}{n_2}, \quad l_3 = \frac{k}{n_3}
\]
Step 2: Use total length relation
\[
l = l_1 + l_2 + l_3
\]
Substituting:
\[
\frac{k}{n} = \frac{k}{n_1} + \frac{k}{n_2} + \frac{k}{n_3}
\]
Step 3: Simplify
Dividing throughout by $k$:
\[
\frac{1}{n} = \frac{1}{n_1} + \frac{1}{n_2} + \frac{1}{n_3}
\]
Step 4: Final Result
\[
\boxed{\frac{1}{n} = \frac{1}{n_1} + \frac{1}{n_2} + \frac{1}{n_3
\]