Resistors in Parallel

by Rajesh Kakkad
07.23.2022

As we mentioned earlier, there were 2 types of circuits, SERIES and PARALLEL. We have already gone thru Series. Now we are going to discuss the difference between a Series and a PARALLEL circuit. In the series circuit, all the electricity followed the same path. In our waterflow representation, this meant that all the water flowed through 1 pipe. In PARALLEL circuit, however, there are multiple paths that current can flow through.

Notice that in the picture to the left, that there are 3 different paths which the water can take. All 3 paths have the same incoming pressure, but the flow of some paths can be more restricted than in others.

Parallel circuits in electronics work on the same principle. While there may be multiple paths for the electricity to flow through, the electrical pressure (Voltage) remains the same through all paths.

 

 

As you can see from the diagram on the left, there are 4 meters placed in this circuit to measure the current.

The first 3, (A1, A2, and A3) measure only the current flowing through that individual leg of the circuit. The 4th, AT measures the Total current of the circuit. If you take the three individual currents, and add them all together, they will equal the total current, measured on the 4th meter. From this we can see that the current in a parallel circuit is additive. I1 + I2 + IX… = ITotal

Resistance in a parallel circuit can be quite a bit trickier than in a series circuit. It is found by “Reciprocating the Sum of the Reciprocals”. Simple. Taking the reciprocal of a number means dividing “1” by that number. The reciprocal of 2 would be 1 divided by 2 or ½. Most modern calculators have a [1/X] button just for this purpose.

So if you take the reciprocals of the values of all of the resistors, which would, of course, give you a bunch of fractions, and add them all up, then reciprocate their sum, you would have the answer.

The formula would look something like this:

                        1

     ———————————–

      1        1        1        1        1

    —- + —- + —- + —- + —- +

     R1      R2       R3       R4      RX…

Direct Current Theory

Let’s begin with a very simple circuit: 2 resistors and 1 battery. You are given the following information about the circuit:

R1 = 50 W
R2 = 200 W
A1 reads .2 Amps in current ( I=.2 )

Find:
Total Voltage
Total Circuit Resistance
Total Current
And Finally, the Current through A2

We know according to Ohm’s law, that if we know the resistance and current, we can find the voltage.
ER1= IR1 x R1.
E = .2 x 50 = 10
E = 10 Volts.

Now that we know that the voltage for the entire circuit is 10 volts, let’s find the total Resistance.
First, we find the reciprocals of the individual resistances:
R1= 50 ohms. 1/50 = .02
R2= 200 ohms. 1/200 = .005
Now we add the two reciprocals together:
.02 + .005 = .025

Finally we take the reciprocal of the sum:
1 / .025 = 40 W

If the Total Voltage of the circuit is 10 Volts, and the Total Resistance = 40 W then by using Ohms Law again we can find the total current.
ITotal = ETotal / RTotal
I = 10/40 = ¼ Ampere.

So far we know:
R1 = 50 W
R2 = 200 W
A1 reads .2 Amps in current ( I=.2 )
VTotal= 10
RTotal= 40
and
ITotal = ¼

Now we have at least 2 methods by which we can find the current through A2.
We know that the Total current is the sum of all the individual leg currents, so if we subtract the current of A1 from the Total current we get this:
ITotal – I1 = I2 .25 – .2 = I2 = .05 Amperes.

The other method would be by using Ohms Law. We know the resistance of R2 = 200 W. We also know that the voltage across R2 = 10 Volts. Hence:
10 Volts / 200 W = .05 Amperes.

Either way, our final result is A2 = .05 Amps

 

Articles in this category

Special




FoxDelta kits for Ham Radio

The Author

Rajesh Kakkad

Related Posts

Maxwell’s Equations

Maxwell’s Equations

Quantities and units. Electricity is a difficult substance to appreciate with the human senses. About the only way you get a feeling for it is to moisten the tongue and apply it between the terminals of a 9 volt battery. Of course, you get more idea if you are...

read more
Semiconductors: Diodes and Transistors

Semiconductors: Diodes and Transistors

Semiconductors: Diodes & Transistors In the early days of electricity there were only two groups of material: insulators and conductors. Insulators are matters, which do not allow the flow of electric current through them. Glass, porcelain, dry air and dry wood...

read more
FM Detector

FM Detector

FM stands for Frequency Modulation. It means that the RF-frequency will change according to the input audio signal. Example: A FM radio signal at 105.1MHz will not be exactly stable at 105.1MHz, The audio signal in the RF will modulate (change) the frequency for about...

read more