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Load affects the performance of circuits that output AC , with the household's appliances collectively making up the load. When a power-hungry appliance switches on, it dramatically reduces the load Impedance , causing the output voltage to drop. This drop is easily observed; for instance, turning on a Vacuum Cleaner dims the lights.


A MORE TECHNICAL APPROACH

(Two sidenotes on generality, for advanced readers. This discussion will disregard Nonlinearity . It will also use simple Resistance s, but they can be readily generalized to impedances for AC analysis.)

When discussing the effect of load on a circuit, it is helpful to disregard the circuit's actual design and consider only the Thévenin Equivalent . (The Norton Equivalent works just as well, but this discussion will use the Thévenin form.) The Thévenin equivalent of a circuit looks like this:

''Rs''.]]

With no load (open-circuited terminals), all of V_S falls across the output; the output voltage is V_S. However, the circuit will behave differently if a load is added. We would like to ignore the details of the load circuit, as we did for the power supply, and represent it as simply as possible. If we use an Input Resistance to represent the load, the complete circuit looks like this:

Whereas the voltage source by itself was an Open Circuit , adding the load makes a Closed Circuit and allows current to flow. This current places a voltage drop across R_S, so the voltage at the output terminal is no longer V_S. The output voltage can be determined by the Voltage Division rule:

:V_{OUT} = V_S \cdot rac{R_{L}}{R_{L} + R_S}


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