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{{Antennas|Characteristics}}
 
'''Radiation resistance''' is that part of an [[antenna (electronics)|antenna]]'s feedpoint resistance that is caused by the [[radiation]] of [[Electromagnetic radiation|electromagnetic]] waves from the antenna. The radiation resistance is determined by the geometry of the antenna, not by the materials of which it is made. It can be viewed as the equivalent resistance to a resistor in the same circuit.
 
Radiation resistance is caused by the [[radiation reaction]] of the conduction electrons in the [[antenna (electronics)|antenna]].
 
When electrons are accelerated, as occurs when an AC electrical field is impressed on an [[antenna (electronics)|antenna]], they will radiate electromagnetic waves. These waves carry energy that is taken from the electrons. The loss of energy of the electrons appears as an effective resistance to the movement of the electrons, analogous to the ohmic resistance caused by scattering of the electrons in the crystal lattice of the metallic conductor.
 
While the energy lost by ohmic resistance is converted to heat, the energy lost by radiation resistance is converted to electromagnetic radiation.  
 
[[Power (physics)|Power]] is calculated as
 
:<math>P = I^2R \,</math>
 
where <math>I</math> is the [[electric current]] flowing into the feeds of the [[antenna (electronics)|antenna]] and <math>P</math> is the power in the resulting electromagnetic field. The result is a virtual, effective [[Electrical resistance|resistance]]:
 
:<math>R = \frac{P}{I^2} \,</math>
 
This effective resistance is called the '''radiation''' resistance.
 
Thus the radiation resistance of an antenna is a good indicator of the strength of the electromagnetic field radiated by a transmitting antenna or being received by a receiving antenna, since its value is directly proportional.
 
==See also==
*[[Abraham-Lorentz force]]
*[[Impedance of free space]]
 
[[Category:Antennas (radio)]]

Revision as of 22:50, 20 June 2013



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Radiation resistance is that part of an antenna's feedpoint resistance that is caused by the radiation of electromagnetic waves from the antenna. The radiation resistance is determined by the geometry of the antenna, not by the materials of which it is made. It can be viewed as the equivalent resistance to a resistor in the same circuit.

Radiation resistance is caused by the radiation reaction of the conduction electrons in the antenna.

When electrons are accelerated, as occurs when an AC electrical field is impressed on an antenna, they will radiate electromagnetic waves. These waves carry energy that is taken from the electrons. The loss of energy of the electrons appears as an effective resistance to the movement of the electrons, analogous to the ohmic resistance caused by scattering of the electrons in the crystal lattice of the metallic conductor.

While the energy lost by ohmic resistance is converted to heat, the energy lost by radiation resistance is converted to electromagnetic radiation.

Power is calculated as

P=I2R

where I is the electric current flowing into the feeds of the antenna and P is the power in the resulting electromagnetic field. The result is a virtual, effective resistance:

R=PI2

This effective resistance is called the radiation resistance.

Thus the radiation resistance of an antenna is a good indicator of the strength of the electromagnetic field radiated by a transmitting antenna or being received by a receiving antenna, since its value is directly proportional.

See also