Question:

A signal is to be transmitted through a wave of wavelength \(\lambda\), using a linear antenna. The length l of the antenna and effective power radiated \(P_{eff}\) will be given respectively as :
(K is a constant of proportionality)

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An antenna radiates efficiently only if its length is comparable to the signal wavelength, and the radiated power varies as \((l/\lambda)^2\), i.e. as \(1/\lambda^2\) for a given length.
Updated On: Nov 11, 2026
  • \(\lambda,\ P_{eff} = K\left(\frac{1}{\lambda}\right)^{2}\)
  • \(\frac{\lambda}{8},\ P_{eff} = K\left(\frac{1}{\lambda}\right)\)
  • \(\frac{\lambda}{16},\ P_{eff} = K\left(\frac{1}{\lambda}\right)^{3}\)
  • \(\frac{\lambda}{5},\ P_{eff} = K\left(\frac{1}{\lambda}\right)^{\frac{1}{2}}\)
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The Correct Option is A

Solution and Explanation

For effective transmission the length of the antenna must be of the order of the wavelength, \(l \sim \lambda\) (a length much smaller than \(\lambda\), such as \(\lambda/16\), radiates very poorly).
The power radiated by an antenna of length l is proportional to \((l/\lambda)^2\); for \(l\) of the order of \(\lambda\) this gives \(P_{eff}\propto\left(\frac{1}{\lambda}\right)^2\), so \(P_{eff} = K\left(\frac{1}{\lambda}\right)^2\).
Only option (1) has both \(l = \lambda\) and the inverse-square dependence.
Answer: (1) \(\lambda,\ P_{eff} = K\left(\frac{1}{\lambda}\right)^{2}\)
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