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edison (4593)

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Olaaa!! Perrrfect answer. 807  [1086 rates]

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Proof for purely resistive circuits
 
 
In the diagram opposite, power is being transferred from the source, with voltage V and fixed source resistance RS, to a load with resistance RL, resulting in a current I. By Ohm's law, I is simply the source voltage divided by the total circuit resistance:
I = {V over R_mathrm{S} + R_mathrm{L}}.
The power PL dissipated in the load is the square of the current multiplied by the resistance:
P_mathrm{L} = I^2 R_mathrm{L} = {{ left( {V over {R_mathrm{S} + R_mathrm{L}}} 
ight) }^2} R_mathrm{L} = {{V^2} over {R_mathrm{S}^2 / R_mathrm{L} + 2R_mathrm{S} + R_mathrm{L}}}.
We could calculate the value of RL for which this expression is a maximum, but it is easier to calculate the value of RL for which the denominator
R_mathrm{S}^2 / R_mathrm{L} + 2R_mathrm{S} + R_mathrm{L}
is a minimum. The result will be the same in either case. Differentiating with respect to RL:
{dover{dR_mathrm{L}}} left( {R_mathrm{S}^2 / R_mathrm{L} + 2R_mathrm{S} + R_mathrm{L}} 
ight) = -R_mathrm{S}^2 / R_mathrm{L}^2+1.
For a maximum or minimum, the first derivative is zero, so
{R_mathrm{S}^2 / R_mathrm{L}^2} = 1
or
R_mathrm{L} = pm R_mathrm{S}.
In practical resistive circuits, RS and RL are both positive. To find out whether this solution is a minimum or a maximum, we must differentiate again:
{{d^2} over {dR_mathrm{L}^2}} left( {R_mathrm{S}^2 / R_mathrm{L} + 2 R_mathrm{S} + R_mathrm{L}} 
ight) = {2 R_mathrm{S}^2} / {R_mathrm{L}^3}
This is positive for positive values of RS and RL, showing that the denominator is a minimum, and the power is therefore a maximum, when
RS = RL.

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