# Resistors in Series and Parallel Formula Derivation

## Formulas for Resistors in Series and Parallel

Resistors are ubiquitous components in electronic circuitry both in industrial and domestic consumer products. Often in circuit analysis, we need to work out the values when two or more resistors are combined. In this tutorial, we'll work out the formulas for resistors connected in series and parallel.

## Some Revision: A Circuit With One Resistor

In an earlier tutorial, you learned that when a single resistor was connected in a circuit with a voltage source V, the current I through the circuit was given by Ohm's Law:

I = V / R ........... Ohm's Law

## Ohms Law

I = V / R

## Two Resistors in Series

Now let's add a second resistor in series. Series means that the resistors are like links in a chain, one after another. We call the resistors R_{1} and R_{2}.

The same voltage source V causes a current I to flow.

We notice that the same current I flows through both resistors.

Let the voltage drop (also called the *potential difference*) measured across R_{1} be V_{1 }and let the voltage measured across R_{2} be V_{2} as shown in the diagram below.

From Ohm's Law, we know that for a circuit with a resistance R and voltage V:

I = V / R

Therefore

V = IR

So for resistor R_{1}

V

_{1}= IR_{1}

and for resistor R_{2}

V

_{2}= IR_{2}

From Kirchoff's Voltage Law, we know that the voltages around a loop in a circuit add up to zero. So in our example:

V = V

_{1 }+ V_{2}

Substitute for V_{1 }+ V_{2}

V = IR

_{1}+ IR_{2}= I(R_{1}+ R_{2})

Divide both sides by I

V / I = R

_{1}+ R_{2}

But from Ohm's Law, we know V / I = total resistance of the circuit. Let's call it R_{total}

Therefore

R_{total}= R_{1}+ R_{2}

In general if we have n resistors:

R_{total}= R_{1}+ R_{2}+ ...... R_{n}

So to get the total resistance of resistors connected in series, we just add all the values.

## Two Resistors in Parallel

Next we'll derive the expression for resistors in parallel. Parallel means all the ends of the resistors are connected together at one point and all the other ends of the resistors are connected at another point.

When resistors are connected in parallel, the current from the source is split between all the resistors instead of being the same as was the case with series connected resistors. However, the same voltage is now common to all resistors.

Let the current through resistor R_{1} be I_{1} and the current through R_{2} be I_{2}

The voltage drop across both R_{1} and R_{2 }is equal to the supply voltage V

Therefore from Ohm's Law

I

_{1}= V / R_{1}

and

I

_{2}= V / R_{2}

But from Kirchoff's Current Law, we know the current entering a node (connection point) is equal to the current leaving the node

Therefore

I = I

_{1}+ I_{2}

Substituting the values derived for I_{1} and I_{2 }gives us

I = V / R

_{1}+ V / R_{2 }= V(1 / R

_{1}+ 1 / R_{2})

The lowest common denominator (LCD) of 1 / R_{1} and 1 / R_{2 }is R_{1}R_{2} so we can replace the expression (1 / R_{1} + 1 / R_{2}) by

R

_{2}/ R_{1}R_{2}+ R_{1}/ R_{1}R_{2}

Switching around the two fractions

= R

_{1}/ R_{1}R_{2}+ R_{2}/ R_{1}R_{2 }

and since the denominator of both fractions is the same

= (R

_{1 }+ R_{2}) / R_{1}R_{2}

Therefore

I = V(1 / R

_{1}+ 1 / R_{2}) = V(R_{1 }+ R_{2}) / R_{1}R_{2}

Rearranging gives us

V / I = R

_{1}R_{2}/ (R_{1 }+ R_{2})

But from Ohm's Law, we know V / I = total resistance of the circuit. Let's call it R_{total}

Therefore

R_{total }= R_{1}R_{2}/ (R_{1 }+ R_{2})_{}

So for two resistors in parallel, the combined resistance is the product of the individual resistances divided by the sum of the resistances.

## Multiple Resistors in Parallel

If we have more than two resistors connected in parallel, the current I equals the sum of all the currents flowing through the resistors.

So for n resistors

I = I

_{1}+ I_{2}+ I_{3}. ........... + I_{n}= V / R

_{1}+ V / R_{2}+ V / R_{3}+ ............. V / R_{n}= V ( 1 / R

_{1}+ 1 / R_{2}+ V / R_{3 }........... 1 / R_{n})

Rearranging

I / V = ( 1 / R

_{1}+ 1 / R_{2}+ V / R_{3 }........... 1 / R_{n})

If V / I = R_{total} then

I / V = 1 / R

_{total}= ( 1 / R_{1}+ 1 / R_{2}+ V / R_{3 }........... 1 / R_{n})

So our final formula is

1 / R_{total}= ( 1 / R_{1}+ 1 / R_{2}+ V / R_{3 }........... 1 / R_{n})

We could invert the right side of the formula to give an expression for R_{total} , however it's easier to remember the equation for the reciprocal of resistance.

So to calculate the total resistance, we calculate the reciprocals of all the resistances first, sum them together giving us the reciprocal of the total resistance. The we take the reciprocal of this result giving us R_{total}

So

## Recommended Books

*Introductory Circuit Analysis* by Robert L Boylestad covers the basics of electricity and circuit theory and also more advanced topics such as AC theory, magnetic circuits and electrostatics. It's well illustrated and suitable for high school students and also first and second year electric or electronic engineering students. This hardcover 10th edition is available from Amazon with a "good - used" rating. Later editions are also available.

## References

Boylestad, Robert L, *Introductory Circuit Analysis* (1968) published by Pearson

ISBN-13: 9780133923605

**© 2020 Eugene Brennan**