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Compensation theorem for antennas
Short answer
If branch impedance Z carrying current I changes by ΔZ, the resulting current changes equal those produced by a series voltage source −IΔZ, with other sources replaced by internal impedances. New current is I'=I+ΔI. It is used for nearby objects, parasitic elements, or load changes in antenna systems.
State the compensation theorem for an antenna system.
Compensation theorem: If the impedance Z of a branch carrying current I is changed by ΔZ, the changes in currents everywhere in the network are the same as those produced by a voltage source of value −I·ΔZ (opposing the original current) placed in series with the changed branch, with all other sources replaced by their internal impedances.
Original Changed Compensation network
--[ Z ]-- I --[Z+ΔZ]-- I' --[Z+ΔZ]--(−I·ΔZ)--
gives ΔI = I' − I
So the new current is I' = I + ΔI, where ΔI is found from the compensation source alone.
Use in antenna systems:
- To find the change in antenna current and input impedance when a nearby object, parasitic element or ground changes the impedance of a branch.
- To find the effect of changing a load or tuning impedance at the antenna terminals without solving the whole system again.
- In arrays, to study how changing one element's impedance alters currents in the other (mutually coupled) elements.
The theorem holds for linear, bilateral networks, so it applies to antennas in a linear medium.
✓ Answer checked by Claude Opus 5.5 (high effort)
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