Concept:
According to Fourier series analysis, any non-sinusoidal periodic waveform can be broken down into a sum of pure sinusoidal components consisting of a fundamental frequency along with higher integer multiples called harmonics.
For an output voltage waveform from an inverter (such as a square wave):
• The frequency of the $n^{\text{th}}$ harmonic component is $n$ times the fundamental frequency:
\[ f_n = n \cdot f \]
• The peak amplitude voltage of the $n^{\text{th}}$ harmonic component is inversely proportional to its harmonic order:
\[ V_{n(\text{peak})} = \frac{V_m}{n} \]
• The corresponding Root-Mean-Square (RMS) voltage for any pure sine wave component is its peak amplitude divided by the square root of two:
\[ V_{n(\text{rms})} = \frac{V_{n(\text{peak})}}{\sqrt{2}} \]
Step 1: Calculating the frequency of the 5th harmonic.
We are looking for the properties of the $5^{\text{th}}$ harmonic component ($n = 5$).
Using the frequency relation:
\[
f_5 = 5 \times f = 5f
\]
Step 2: Finding the peak voltage of the 5th harmonic.
The peak voltage amplitude drops by a factor of 5 for the fifth harmonic:
\[
V_{5(\text{peak})} = \frac{V_m}{5}
\]
Step 3: Computing the RMS voltage of the 5th harmonic.
To find the RMS value, divide the peak voltage of this harmonic component by $\sqrt{2}$:
\[
V_{5(\text{rms})} = \frac{V_{5(\text{peak})}}{\sqrt{2}} = \frac{\left(\frac{V_m}{5}\right)}{\sqrt{2}} = \frac{V_m}{5\sqrt{2}}
\]
Step 4: Combining the answers.
The frequency is $5f$ and the RMS voltage is $\frac{V_m}{5\sqrt{2}}$, which matches option (4).
Hence, the correct choice is option (4).