Series and Parallel Circuits



" It would be better for the true physics if there were no mathematicians on earth."
Daniel Bernoulli


fig1The same current flows in each resistor, the voltages across them are typically different, where V = V1 + V2 + V3 which leads to the equivalent resistance formula

Req = R1 + R2 + R3
The potential difference across each resistor is the same, but the currents through them are typically different, where I = I1 + I2 + I3.  This lead to the equivalent resistance formula,
eqn1

Note that both of the diagrams below represent resistors in parallel.
fig2                              fig3

Some circuits can be analysed as combinations of series and parallel circuits. In the circuit below R2 and R3 are in parallel, their equivalent resistance is then in series with R1.
fig4
exclamation Note that it is not possible to represent all circuits as combinations of series and parallel elements, this is most obvious in many cases where there is more than one battery in the circuit, see example below.  To analyse this type of circuit we must use Kirchhoff's Laws.

fig5

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Dr. C. L. Davis
Physics Department
University of Louisville
email: c.l.davis@louisville.edu