Circuit LawsOhm’s LawUnits for Resistance/ConductanceExamplesPower in a Resistive ElementOpen and Short CircuitsSlide 7Lumped-Parameter CircuitSlide 9Kirchhoff’s Current Law (KCL)KCL Statements and SignSlide 12Kirchhoff’s Voltage Law (KVL)KVL Statements and SignVoltage LabelingSlide 16Single Loop and Node CircuitsSingle Loop ExampleSingle Node-Pair ExampleVoltage DivisionCurrent DivisionKevin D. Donohue, University of Kentucky1Circuit LawsOhm’s Law, Kirchhoff’s Law, Single loop circuits, Single node-pair circuitsKevin D. Donohue, University of Kentucky2Ohm’s LawThe relationship between voltage and current through a material, characterized by resistance, is given by Ohm’s Law:)()( tiRtv Resistive elements will always absorb power (i.e. convert electric energy to heat): +v(t)-i(t)Kevin D. Donohue, University of Kentucky3Units for Resistance/ConductanceResistance can be characterized in units of ohms:A1V11R Conductance can be characterized in units of siemens: V1A1S1G Kevin D. Donohue, University of Kentucky4ExamplesFind the voltage across a 10 resistor when a current of 4 A is passing through it.Find the current in a .02S resistor when a voltage drop of 10 V occurs across it.Find the resistance of an element that exhibits a 14 V drop when 21 A pass through it.Kevin D. Donohue, University of Kentucky5Power in a Resistive ElementPower absorbed by a resistor is given by: +v(t)-i(t)G)(R)()(R)(G)(R)(R)()()()()()(2222titititip(t) tvtvtvtvtptitvtpR +v(t)-i(t)GKevin D. Donohue, University of Kentucky6Open and Short CircuitsIf a resistance value goes to infinity, no current flows through it. This is referred to as an open circuit.If a resistance value goes to zero, no voltage drops across it. This is referred to as a short circuit. +v(t)-i(t)RLimR+v(t)- i(t) +v(t)-i(t)RLimR0+v(t)- i(t)Kevin D. Donohue, University of Kentucky7ExamplesSolve for quantities (voltage, power, current, resistance) in resistive circuits with simple connections to independent and dependent sources.Kevin D. Donohue, University of Kentucky8Lumped-Parameter CircuitTo represent the flow of electrical charge through an actual circuit, a zero-resistance connector is used to connect symbols denoting electrical properties of circuit parts.Kevin D. Donohue, University of Kentucky9Lumped-Parameter CircuitDefine and Identify Nodes, Branches, Loops VR 1K R0 1K R1 1K R2 1K IR3 1K Node - connection between 2 or more circuit elementsBranch - circuit portion containing a single elementLoop - closed path containing no node more than onceKevin D. Donohue, University of Kentucky10Kirchhoff’s Current Law (KCL)The sum of all currents entering a node (or any closed surface) equals zeroLabel each branch current and write a set of equations based on KCLDraw an arbitrary surface containing several nodes and write an equation based on KCL VR 1K R0 1K R1 1K R2 1K IR3 1KKevin D. Donohue, University of Kentucky11KCL Statements and SignSum of all currents leaving a node equals zero.Denote leaving as positive and entering as negative.Sum of all currents entering a node equals zero.Denote entering as positive and leaving as negative.Sum of all currents leaving a node equals sum of all current entering the node.Place all currents entering a node on one side of equation and all currents leaving the node on the other side.Kevin D. Donohue, University of Kentucky12ExamplesFor circuits containing independent sources, dependent sources, and resistors, use KCL and Ohm’s Law to solve for unknown currents and voltages OR determine relations between quantities that cannot be resolved (i.e when more unknowns than independent equations exist).Kevin D. Donohue, University of Kentucky13Kirchhoff’s Voltage Law (KVL)The sum of all voltages around any loop equals zeroLabel each branch voltage and write a set of equations based on KVL VR 1K R0 1K R1 1K R2 1K IR3 1KKevin D. Donohue, University of Kentucky14KVL Statements and SignSum of all voltage drops around a loop equals zero.Denote drops as positive and rises as negative.Sum of all voltage rises around a loop equals zero.Denote rises as positive and drops as negative.Sum of all voltage rises equals the sum of all voltage drops around a loop.Place all voltage rises on one side of equation and all voltage drops on the other side.Kevin D. Donohue, University of Kentucky15Voltage LabelingR R0 a bcV+ VR0 -+VR-VocaacVVV cbbcRoVVVV baabRVVV 0Kevin D. Donohue, University of Kentucky16ExamplesFor circuits containing independent sources, dependent sources, and resistors, use KVL to solve for unknown voltages and currents or determine relation between quantities that cannot be resolved (i.e. when more unknowns than independent equations exist).Kevin D. Donohue, University of Kentucky17Single Loop and Node CircuitsSolving for circuit quantities will involve the following steps:Labeling the circuitDeriving a set of equation from circuitSolving the resulting equationsKevin D. Donohue, University of Kentucky18Single Loop ExampleFind reduced expressions for all unknown voltages and currents (V1 = 5v, V2=-2v, R1=3k, R2=2k, R3=5k): IR3V2R1V1R2Hint: Current in a single loop is the same through all elements, therefore use KVL.Kevin D. Donohue, University of Kentucky19Single Node-Pair ExampleFind reduced expressions all unknown voltages and currents (I1 = 1mA, R=4k): I1RA 1000abVbaHint: Voltage over a single node pair is the same over all elements, therefore use KCL.Kevin D. Donohue, University of Kentucky20Voltage DivisionFor single loops with resistive elements and a voltage source, the following formula can be used to compute the voltage drop across any resistor: VsR1R2RN+V1-+V2-+VN-NkskRRRRVV21Kevin D. Donohue, University of Kentucky21Current DivisionFor single node pairs with resistive elements and a current source, the following formula can be used to compute the current in any resistor: