If a linear antenna radiates a power \(P\) at a wavelength \(\lambda\), then the power radiated by the same antenna at a wavelength of \(\frac{\lambda}{\sqrt{3}}\) is:
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For antennas, power radiated varies inversely with the square of the wavelength. Reducing the wavelength increases the power radiated accordingly.
Power radiated by a linear antenna is inversely proportional to the square of the wavelength, i.e.,
\[
P \propto \frac{1}{\lambda^2}
\]
Given the original power is \(P\) at wavelength \(\lambda\).
At wavelength \(\frac{\lambda}{\sqrt{3}}\), the power radiated \(P'\) is:
\[
P' = P \times \left(\frac{\lambda}{\frac{\lambda}{\sqrt{3}}}\right)^2 = P \times (\sqrt{3})^2 = 3P
\]
Thus, the power radiated at \(\frac{\lambda}{\sqrt{3}}\) is \(3P\).