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 \(3P\).