The radio frequency source can be modeled as a constant voltage source with a series characteristic impedance of say 50 Ohms. That means it can drive a 50 Ohm load.
Q1.Does that mean the E/H ratio is 50 as in vacuum E/H is 120π.
Secondly, when source is perfectly matched to a reactive load say 1+j45 ohms by a matching network, by maximum power transfer theorem, half of the power is transferred. Q2.Then where the other half power is dissipated?
I have used an L section matching at frequency of 13.56 MHz.
My detector says 100% forward power and 0% reflected power for an input RF power of 1 kilowatt.
Q1.Does that mean the E/H ratio is 50 as in vacuum E/H is 120π.
Secondly, when source is perfectly matched to a reactive load say 1+j45 ohms by a matching network, by maximum power transfer theorem, half of the power is transferred. Q2.Then where the other half power is dissipated?
I have used an L section matching at frequency of 13.56 MHz.
My detector says 100% forward power and 0% reflected power for an input RF power of 1 kilowatt.