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Series and Parallel Circuits (R. Bolton - 2012) Series and Parallel Circuits (R. Bolton - 2012) Preamble Series and Parallel Circuits Physics, 8th Edition Custom Edition Cutnell & Johnson Chapter 20.6-20.8, 20 6-20 8 20.10 20 10 Pages 610-618, 619-622 (R. Bolton - 2012) Series and Parallel Circuits (R. Bolton - 2012) 1 Physics 155.3: Introduction to Electricity and Magnetism 1 Series and Parallel Circuits (R. Bolton - 2012) Series Resistors Series and Parallel Circuits 2 Physics 155.3: Introduction to Electricity and Magnetism 2 Series and Parallel Circuits (R. Bolton - 2012) Kirchoff’ Voltage Law (KVL) The figure shows a series resistor circuit. Our first job is to determine how the two series resistors combine to form an equivalent i l t resistor. i t In this section of my lectures we will be developing the two common types of resistor arrangements; series and parallel. To do this we will introduce some very important laws and rules that you must become familiar with. Around any closed-circuit loop, the sum of the potential drops equals the sum of the potential rises. An alternative way of stating KVL is V l loop =0 Note: In this circuit the same current flows g each of the resistors. through (R. Bolton - 2012) Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 3 (R. Bolton - 2012) 3 Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 4 4 Series and Parallel Circuits (R. Bolton - 2012) Note that only voltage sources (i.e., a battery) are considered as a potential rise. Series and Parallel Circuits This is due to the convention off considering how positive charge is affected when going around a circuit. Since positive charge gains potential when going from a negative terminal on the voltage source to the positive terminal on the voltage source it experiences a potential rise. (R. Bolton - 2012) The figure is redrawn showing polarity information If this is the case, where are the potential drops in the loop shown above? (R. Bolton - 2012) Series and Parallel Circuits 5 Physics 155.3: Introduction to Electricity and Magnetism (R. Bolton - 2012) 5 Series and Parallel Circuits (R. Bolton - 2012) Series and Parallel Circuits 6 Physics 155.3: Introduction to Electricity and Magnetism 6 Series and Parallel Circuits (R. Bolton - 2012) Series Resistance Using Ohm’s Law VR1 = IR1 loop VR2 = IR2 Using Kirchoff’s Voltage Law (KVL) V Rseries = R1 + R2 + R3 + + Rn = V − IR1 − IR2 = 0 Rearranging (and using Ohm’s Law) V = IR1 + IR2 V = I (R1 + R2 ) V = IRseries where Rseries = R1 + R2 (R. Bolton - 2012) Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits Resistors in series (i.e., resistors with the same current flowing g through g them)) add. 7 Note: If the resistors do not have the same current flowing through them they are NOT in series! (R. Bolton - 2012) 7 Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 8 8 Series and Parallel Circuits (R. Bolton - 2012) Example 1 Series Resistor Voltages Series and Parallel Circuits (R. Bolton - 2012) Example 1 Solution: Consider the following circuit (4.00V, 8.00V) Using Ohm’s Law V = IRs + I + I= + V 12 V 12 V 12 V = = = = 0 .4 A Rs (R1 + R2 ) (10Ω + 20Ω ) 30Ω V1 = IR1 = 0.4 A ⋅ 10Ω = 4.0V V2 = IR2 = 0.4 A ⋅ 20Ω = 8.0V What is the voltage g across each resistor? (R. Bolton - 2012) Series and Parallel Circuits 9 Physics 155.3: Introduction to Electricity and Magnetism 9 Series and Parallel Circuits (R. Bolton - 2012) (R. Bolton - 2012) Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 10 Physics 155.3: Introduction to Electricity and Magnetism 10 Series and Parallel Circuits (R. Bolton - 2012) V2 = IR2 Note that it is possible to determine the voltage across each resistor in a series combination by recalling that the same current goes through each series resistor and th t th that the sum off th the resistor i t voltages lt mustt equal the battery voltage. Take for example the resistor R2 from the previous circuit: (R. Bolton - 2012) Series and Parallel Circuits But the current is equal to I= V R1 + R2 Therefore V R2 V2 = R1 + R2 Rearranging R2 V2 = V R1 + R2 11 (R. Bolton - 2012) 11 Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 12 12 Series and Parallel Circuits (R. Bolton - 2012) Voltage Divider Rule (VDR) (for series resistors) Series and Parallel Circuits (R. Bolton - 2012) 14 Series and Parallel Circuits (R. Bolton - 2012) Consider the following circuit Physics 155.3: Introduction to Electricity and Magnetism 14 Example 3 Very Important Circuit (1)!!! (2.61V) Series and Parallel Circuits Series and Parallel Circuits Physics 155.3: Introduction to Electricity and Magnetism (R. Bolton - 2012) What is the voltage across the 4.7kΩ resistor? (R. Bolton - 2012) 13 Example 2 Solution: Consider the following circuit 13 Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits (R. Bolton - 2012) Example 2 Voltage Divider Circuit The voltage across any resistor in a series combination of resistances is equal to the voltage across the series combination multiplied by the value of the resistor in question over the total series resistance. (R. Bolton - 2012) Series and Parallel Circuits 15 What is the value of E for 20mA to flow in the circuit (in the direction shown)? What is VA? VB? VAB? (R. Bolton - 2012) 15 Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 16 16 Series and Parallel Circuits (R. Bolton - 2012) Is the circuit a series circuit? Is the circuit a parallel circuit? What is the direction of the current? What is the symbol on the bottom left? What does it do? What are the polarities of the voltage drops across the resistors? (R. Bolton - 2012) Series and Parallel Circuits 17 Physics 155.3: Introduction to Electricity and Magnetism (R. Bolton - 2012) 17 Series and Parallel Circuits (R. Bolton - 2012) Parallel Resistors (50V,-7V,57V) Before going too far consider (R. Bolton - 2012) Example 3 Solution: Procedure Series and Parallel Circuits Physics 155.3: Introduction to Electricity and Magnetism Physics 155.3: Introduction to Electricity and Magnetism (R. Bolton - 2012) At any circuit node, the sum of the currents into the node equals q the sum of the currents out of the node. Note: In this circuit the same voltage is across each of the resistors. Series and Parallel Circuits 18 Series and Parallel Circuits Our first job is to determine how the two parallel resistors combine to form an equivalent i l t resistor. i t (R. Bolton - 2012) 18 Kirchoff’s Current Law (KCL) The figure shows a parallel resistor circuit. Series and Parallel Circuits Note: Currents out of the node are considered positive and currents into the node are considered as negative negative. An alternative way of stating KCL is I 19 node =0 (R. Bolton - 2012) 19 Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 20 20 Series and Parallel Circuits (R. Bolton - 2012) The figure is redrawn showing current information Series and Parallel Circuits (R. Bolton - 2012) Using Ohm’s Law VR1 = I1 R1 VR2 = I 2 R2 But VR1 = VR2 = V Therefore I1 = (R. Bolton - 2012) Series and Parallel Circuits 21 Physics 155.3: Introduction to Electricity and Magnetism (R. Bolton - 2012) Using Kirchoff’s Current Law (KCL) I V V + R1 R2 Series and Parallel Circuits 22 22 Series and Parallel Circuits (R. Bolton - 2012) In order for this equation to be true (i.e., V V=V) V) 1 R parallel ll l 1 1 I = V + R1 R2 V R2 Physics 155.3: Introduction to Electricity and Magnetism V V = −I + + =0 R1 R2 Rearranging I= node d I2 = (R. Bolton - 2012) 21 Series and Parallel Circuits V R1 = 1 1 + R1 R2 Using Ohm’s Law (again) 1 1 V = V + R parallel R1 R2 (R. Bolton - 2012) Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 23 (R. Bolton - 2012) 23 Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 24 24 Series and Parallel Circuits (R. Bolton - 2012) Parallel Resistance R parallel = 1 1 1 1 + + ++ R1 R2 R3 Rn Note: If the resistors do not have the same voltage across them they are NOT in parallel! (R. Bolton - 2012) Series and Parallel Circuits 25 (R. Bolton - 2012) Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 26 Physics 155.3: Introduction to Electricity and Magnetism 26 Series and Parallel Circuits (R. Bolton - 2012) (1.2A, 0.6A) Using Ohm’s Law V = IR parallel R + R2 V V I= = = V 1 R R R parallel 1 2 R1R2 R1 + R2 30Ω I = 12V = 1 .8 A 10Ω ⋅ 20Ω What is the total current and the current through each of the resistors? (R. Bolton - 2012) Series and Parallel Circuits Example 4 Solution: Consider the following circuit R1 R2 R1 + R2 (R. Bolton - 2012) Example 4 Parallel Resistor Currents It turns out that we have two resistors in parallel a lot of the time in the circuits we use. The previous formula can be simplified to R parallel = 25 Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits (R. Bolton - 2012) Two resistors in parallel Resistors in parallel (i.e., resistors with the same voltage g across them)) do NOT add. 1 Series and Parallel Circuits and I1 = 27 V 12V = = 1 .2 A R1 10Ω (R. Bolton - 2012) 27 Physics 155.3: Introduction to Electricity and Magnetism I2 = V 12V = = 0 .6 A R2 20Ω Series and Parallel Circuits 28 28 Series and Parallel Circuits (R. Bolton - 2012) Note that it is possible to determine the current through each resistor in a parallel combination by recalling that the same voltage is across each parallel resistor and that the sum of the resistor currents must equal the total current. Take for example the resistor R2 from the previous example: (R. Bolton - 2012) Series and Parallel Circuits Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 30 Physics 155.3: Introduction to Electricity and Magnetism 30 Series and Parallel Circuits (R. Bolton - 2012) Two Resistors in Parallel The current through any resistor in a parallel combination of resistances is equal to the total current through the parallel combination multiplied by the value of the equivalent resistance of the parallel resistors over the value of the resistor in question. Series and Parallel Circuits Rearranging and substituting for V (R. Bolton - 2012) (R. Bolton - 2012) (R. Bolton - 2012) V V = R1 R2 (R parallel ) R1 + R2 RR I 1 2 R + R2 I (R parallel ) I2 = 1 = R2 R2 Current Divider rule (CDR) (for parallel resistors) But the total current is equal q to I= 29 Series and Parallel Circuits (R. Bolton - 2012) V = I 2 R2 29 Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits It turns out that we have two resistors in parallel a lot of the time in the circuits we use. The previous formula can be simplified R1 I 2 = I R1 + R2 31 Does this make sense? (R. Bolton - 2012) 31 Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 32 32 Series and Parallel Circuits (R. Bolton - 2012) Example 5 Parallel Resistor Current (R. Bolton - 2012) Example p 5 Solution: (2.13mA) Consider the following circuit What is the current through the 4.7kΩ resistor? Before going too far, think about it… (R. Bolton - 2012) Series and Parallel Circuits 33 Physics 155.3: Introduction to Electricity and Magnetism (R. Bolton - 2012) 33 Series and Parallel Circuits (R. Bolton - 2012) Example 6 Very Important Circuit (2)!!! Series and Parallel Circuits Physics 155.3: Introduction to Electricity and Magnetism (R. Bolton - 2012) Before going too far consider What is Vab? Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 34 Series and Parallel Circuits (R. Bolton - 2012) 34 Procedure Consider the following circuit Series and Parallel Circuits 35 Is the circuit a series circuit? Is the circuit a parallel circuit? What is the value of Is? What is the symbol on the bottom left? What does it do? Can there be more than one in a circuit? What is the polarity of the voltage, voltage Vab? (R. Bolton - 2012) 35 Physics 155.3: Introduction to Electricity and Magnetism Series and Parallel Circuits 36 36 Series and Parallel Circuits (R. Bolton - 2012) Example 6 Solution: (R. Bolton - 2012) Physics 155.3: Introduction to Electricity and Magnetism (0V) Series and Parallel Circuits 37 37