Any collection of batteries and resistances with two terminals is electrically equivalent to an ideal
current source i in parallel with a single resistor
r. The value of
r is the same as that in the
Thevenin equivalent and the current
i can be found by dividing the open circuit voltage by
r.
Any collection of batteries and resistances with two terminals is electrically equivalent to an ideal current source i in parallel with a single resistor r.
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