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BASIC ELECTRICAL Parallel Resistance OBJECTIVES Define Parallel Connection Define Parallel Circuit Calculate Parallel Resistive Circuit INTRODUCTION We have worked with Series Connections as one way to connect loads together to make a circuit, in this lesson we will discuss another way to connect loads together called Parallel Connections. This lesson will cover parallel resistive connections, parallel resistive circuits, and calculating total resistance for a parallel resistive circuit. Parallel Connection A parallel connection is defined as anytime two electrical components are connected so that there is more than one path for current through the two components. (See Figure 1 for examples of parallel connections.) Look at the Schematic Diagram View, if Current enters at 1 and travels to the right through the two resistors it will have to leave at 2 . There are multiple paths (two in this case) through the two resistors, this is what is called a Parallel connection. ������������� 1 2 ���������������� � � � � �� �� �� �� �� �� �� �� �� Figure 1 Schematic Diagram Physical Layout Breadboard Layout Parallel connections can be made be adding more than just two electrical components together. There can be many paths that divide up the initial current and share the same voltage. A good example would be the electrical system of an automobile in which the 12 V battery’s Voltage is made common throughout the vehicle, to the starter, to the radio, to the lights, and anything else that needs the electrical pressure to do work. Though there is one Voltage source (the battery) there are multiple paths; a different path through each of the components mentioned. (See Figure 2 for an example of multiple resistors in a parallel connection.) ������������� R1 R1 R2 R2 R3 R3 ���������������� � � � � �� �� �� �� �� �� �� �� �� �� �� �� Figure 2 Schematic Diagram Physical Layout Breadboard Layout All contents copyrighted © 2010 Seven Wanders LLC. All rights reserved 1 �������� �������� �������� �������� �������� �������� �������� �������� �������� �������� �������� �������� Alternate Circuits with 2 Parallel Resistive Paths All contents copyrighted © 2010 Seven Wanders LLC. All rights reserved 2 Parallel Circuit As stated in the “Series Resistance Lesson” , resistive connections are typically the “LOAD” of an electrical circuit. To make a complete electrical circuit we need to add the rest of the components of a circuit. Remember an electrical circuit had four main parts, the source, the circuit path, the load, and the control. The parallel connection we have discussed so far represents the Load and what type of path the circuit is. Figure 3 shows the rest of the components that make up a Parallel Circuit. These examples have three components in the “LOAD”. SW1 R1 R2 ����������������� ���� ���� R1 R2 R3 R3 ������� Schematic Diagram of Series Circuit B1 ������� B1 SW1 Physical Diagram of Series Circuit SW1 in the Physical Diagrams is a SPDT but is being used as a SPST as in the schematic diagram, this is OK to do. ������� Figure 3 � �� �� �� �� � �� �� �� �� �� � ������� ������������� ���������������� � R1 R2 R3 Physical Diagram of Parallel Circuit built on Breadboard All contents copyrighted © 2010 Seven Wanders LLC. All rights reserved 3 Calculate Parallel Resistive Circuit The resistive value of a parallel circuit can look at as if it was just one total resistance. This means the parallel circuit may have R1, R2, and R3, but these resistances can be looked at as one “Total Resistance”. There are several ways the total resistance can be calculated for a parallel circuit. Figure 4 shows the formula for a circuit that has just two parallel resistances. Figure 4 R1 x R2 = Rt R1 + R2 Formula for resolving two resistances into Rt Example 1 200 Ω 200 Ω 200 x 200 40000 = 200 + 200 400 = 100 Ω Two 200Ω Resistors would look like a single 100Ω Resistor to the rest of the circuit. 100 Ω Notice that the color for the first strip on the resistor has changed. In the electronic component lesson these color bands or strips will be explained, it should be noted know that the resistance is as labeled. (100 Ω) The formula in figure 4 can only be used to solve for two resistances at a time. This does not mean that the formula cannot be used to solve for circuits that have more than two parallel resistances. However, it does mean that to solve for more than two resistances in parallel you would need to solve for two resistances at a time using the formula and then use the formula again for the next two resistances, and so on until the circuit is down to just one resistance (Rt). This is shown in Figure 5. 4 All contents copyrighted © 2010 Seven Wanders LLC. All rights reserved Solve for these two reisitors as in Figure 4. Then redraw the circuit to see what is left to solve for. 200 Ω 200 Ω 200 Ω R1 R2 R3 200 Ω R4 200 x 200 40000 = 200 + 200 400 = 100 Ω Two 200Ω Resistors would look like a single 100Ω Resistor to the rest of the circuit. In the second step you can solve for any two of the remaining three resistors. 200 Ω 200 Ω R1 R2 The 100 Ω Resistor shown is not really there, R3 and R4 are still in the circuit. The 100 Ω resistor shown is just the mathematical equivalant of the the two. We have NOT changed he original circuit. 100 Ω 200 x 200 40000 = 200 + 200 400 = 100 Ω Two 200Ω Resistors would look like a single 100Ω Resistor to the rest of the circuit. In the final step in this example select the two remaining resistance values. 100 Ω 100 Ω 5 All contents copyrighted © 2010 Seven Wanders LLC. All rights reserved 100 x 100 10000 = 100 + 100 200 = 50 Ω Two 100Ω Resistors would look like a single 50Ω Resistor to the rest of the circuit. Since there is just one resistance left this is Rt. The above steps can be a long process for a circuit that has many parallel paths, also inaccuracies because of rounding can build up. So, is there a different way to calculate parallel resistances that can deal with these issues? Yes there is, but at first glance this formula may look harder than the previous way shown, believe me it is not. See figure 5. 1 1 1 1 1 + + + = R1 R2 R3 ••• Rn Rt Figure 5 Using a calculator, this one formula can solve for any number of resistances in parallel. (Notice the ... Rn) This formula can be changed to another useful formula by taking the reciprocal of (that is inverting) both sides of the formula. See figure 6. 1 Rt = 1 1 1 1 + + + R1 R2 R3 ••• Rn Figure 6 6 All contents copyrighted © 2010 Seven Wanders LLC. All rights reserved The way to perform the calculations in figure 6 uses the X-1 or 1/X button on your calculator. Follow the steps in figure 7 for the circuit shown. R1 R2 ��X 200 Ω 200 Ω 200 Ω 200 Ω R1 R2 R3 R4 R3 ��X ��X R4 ��X ��X 200 ��X ��X For this example 200 200 ��X 200 ��X ��X The calculator should show 50 Ω Figure 7 The Example below shows a schematic diagram version of the simplification process. SW1 SW1 B1 200 Ω 400 Ω 400 Ω R1 R2 R3 B1 Circuit 1 200 ��X 100 Ω Rt Circuit 2 400 ��X 400 ��X ��X The calculator should show 100 Ω The battery and the switch would not see a difference between circuit 1 and circuit 2, it is said that R1, R2, and R3 are equivalent (equal) to Rt. In the following lessons being able to simplify a circuit to its total resistance will be very important. All contents copyrighted © 2010 Seven Wanders LLC. All rights reserved 7