Resistors are said to be connected together in parallel when both of their terminals are respectively connected to each terminal of the other resistor or resistors.

In a parallel resistor network the circuit current can take more than one path as there are multiple paths for the current. Then parallel circuits are classed as current dividers.

Since there are multiple paths for the supply current to flow through, the current may not be the same through all the branches in the parallel network. However, the voltage drop across all of the resistors in a parallel resistive network IS the same. Then, **Resistors in Parallel** have a **Common Voltage** across them and this is true for all parallel connected elements.

So we can define a parallel resistive circuit as one where the resistors are connected to the same two points (or nodes) and is identified by the fact that it has more than one current path connected to a common voltage source. Then in our parallel resistor example below the voltage across resistor R_{1} equals the voltage across resistor R_{2} which equals the voltage across R_{3} and which equals the supply voltage. Therefore, for a parallel resistor network this is given as:

In the following resistors in parallel circuit the resistors R_{1}, R_{2} and R_{3} are all connected together in parallel between the two points A and B as shown.

**Parallel Resistor Circuit**

In the previous series resistor network we saw that the total resistance, R_{T} of the circuit was equal to the sum of all the individual resistors added together. For resistors in parallel the equivalent circuit resistance R_{T} is calculated differently.

Here, the reciprocal ( 1/R ) value of the individual resistances are all added together instead of the resistances themselves with the inverse of the algebraic sum giving the equivalent resistance as shown.

**Parallel Resistor Equation**

Then the inverse of the equivalent resistance of two or more resistors connected in parallel is the algebraic sum of the inverses of the individual resistances.

If the two resistances or impedances in parallel are equal and of the same value, then the total or equivalent resistance, R_{T} is equal to half the value of one resistor. That is equal to R/2 and for three equal resistors in parallel, R/3, etc.

Note that the equivalent resistance is always less than the smallest resistor in the parallel network so the total resistance, R_{T} will always decrease as additional parallel resistors are added.

Parallel resistance gives us a value known as **Conductance**, symbol **G** with the units of conductance being the **Siemens**, symbol **S**. Conductance is the reciprocal or the inverse of resistance, ( G = 1/R ). To convert conductance back into a resistance value we need to take the reciprocal of the conductance giving us then the total resistance, R_{T} of the resistors in parallel.

We now know that resistors that are connected between the same two points are said to be in parallel. But a parallel resistive circuit can take many forms other than the obvious one given above and here are a few examples of how resistors can be connected together in parallel.

**Various Parallel Resistor Networks**

The five resistive networks above may look different to each other, but they are all arranged as **Resistors in Parallel** and as such the same conditions and equations apply.

**Resistors in Parallel Example 1**

Find the total resistance, R_{T} of the following resistors connected in a parallel network.

This method of reciprocal calculation can be used for calculating any number of individual resistances connected together within a single parallel network.

If however, there are only two individual resistors in parallel then we can use a much simpler and quicker formula to find the total or equivalent resistance value, R_{T} and help reduce the reciprocal maths a little.

This much quicker product-over-sum method of calculating two resistor in parallel, either having equal or unequal values is given as:

**Currents in a Parallel Resistor Circuit**

The total current, I_{T} entering a parallel resistive circuit is the sum of all the individual currents flowing in all the parallel branches. But the amount of current flowing through each parallel branch may not necessarily be the same, as the resistive value of each branch determines the amount of current flowing within that branch.

For example, although the parallel combination has the same voltage across it, the resistances could be different therefore the current flowing through each resistor would definitely be different as determined by Ohms Law.

Consider the two resistors in parallel above. The current that flows through each of the resistors ( I_{R1} and I_{R2} ) connected together in parallel is not necessarily the same value as it depends upon the resistive value of the resistor. However, we do know that the current that enters the circuit at point A must also exit the circuit at point B.

Kirchhoff’s Current Laws states that: “the total current leaving a circuit is equal to that entering the circuit – no current is lost“. Thus, the total current flowing in the circuit is given as:

I_{T} = I_{R1} + I_{R2}

Then by using *Ohm’s Law*, the current flowing through each resistor of Example No2 above can be calculated as:

Current flowing in R_{1} = V_{S} ÷ R_{1} = 12V ÷ 22kΩ = 0.545mA or 545μA

Current flowing in R_{2} = V_{S} ÷ R_{2} = 12V ÷ 47kΩ = 0.255mA or 255μA

thus giving us a total current I_{T} flowing around the circuit as:

I_{T} = 0.545mA + 0.255mA = 0.8mA or 800μA

and this can also be verified directly using Ohm’s Law as:

I_{T} = V_{S} ÷ R_{T} = 12 ÷ 15kΩ = 0.8mA or 800μA (the same)

The equation given for calculating the total current flowing in a parallel resistor circuit which is the sum of all the individual currents added together is given as:

Then parallel resistor networks can also be thought of as “current dividers” because the supply current splits or divides between the various parallel branches. So a parallel resistor circuit having *N* resistive networks will have N-different current paths while maintaining a common voltage across itself. Parallel resistors can also be interchanged with each other without changing the total resistance or the total circuit current.

**Resistors in Parallel Example 2**

Calculate the individual branch currents and total current drawn from the power supply for the following set of resistors connected together in a parallel combination.

This total circuit current value of 5 amperes can also be found and verified by finding the equivalent circuit resistance, R_{T} of the parallel branch and dividing it into the supply voltage, V_{S} as follows.

So to summarise. When two or more resistors are connected so that both of their terminals are respectively connected to each terminal of the other resistor or resistors, they are said to be connected together in parallel. The voltage across each resistor within a parallel combination is exactly the same but the currents flowing through them are not the same as this is determined by their resistance value and Ohms Law. Then parallel circuits are current dividers.

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