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As you mentioned, Thevenin does apply, and your effective area formula
is correct (gain w.r.t. isotropic radiator). So a thin halve wave dipole antenna has an internal resistance of about 70 Ohms, and half the power is lost, but not as heat in the antenna. If I may add just a simple observation to the exhaustive Wim's explanation, I would say that we generally tend to consider resistors as things that necessarily dissipate power, turning it into heat. That is not always the case. As a matter of fact, having current in phase with voltage (what we usually call resistance) signify the transformation of electrical power into any form of power, not just heat. For instance: - an ideal electrical engine (no ohmic loss, no friction) fully transforming the applied electrical power into mechanical power. It looks like a resistor, but no heat is generated anywhere - an ideal antenna (no ohmic loss) fully transforming the applied electrical power into electromagnetic power. Again it looks like a resistor, but no heat is generated anywhere .. 73 Tony I0JX |
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