A network that contains linear impedances and one or more voltage or current sources can be reduced to a Thevenin equivalent circuit.
A Thevenin equivalent circuit is shown in Figure1 with source internal impedance, "z=r+jx \\ \\Omega" and complex load "Z=R+jX \\ \\Omega"
The maximum power transferred from the source to the load depends on the following four conditions.
1. When the load is purely resistive ("X=0") and adjustable, maximum power transfer is achieved when
2. When both the load and the source impedance are purely resistive ("X=x=0"), maximum power transfer is achieved when
3. When the load resistance "R" and reactance "X" are both independently adjustable, maximum power transfer is achieved when
4. When the load resistance "R" is adjustable with reactance "X" fixed, maximum power transfer is achieved when
Given that "r=200\\ \\Omega, f=100\\ Hz, L=10\\ mH."
Then
"X=-j2\\pi(100\\ Hz)(0.01\\ H)=j(-2\\pi)\\ \\Omega"
"Z=(200-2\\pi j)\\ \\Omega"
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