DC Circuits Lab ECE 002 Professor Ahmadi George Washington University Outline Basic Components of a Circuit Series Circuit Parallel Circuit Ohm’s Law Lab Overview George Washington University Basic Circuit Components We represent real electrical components with symbols 1.5V 1.5 V A Battery… …can be represented with this symbol …called a “DC voltage source” A DC Voltage Source • Provides Power for our circuit • Battery or Lab ‘power supply’ is an example • DC voltage is supplied across the two terminals • Its voltage is VOLTS (V) George Washington University Basic Circuit Components We represent real electrical components with symbols RΩ A Light Bulb…or any ‘device’… …can be represented with this symbol …called a “resistor” A Resistor • Represents any device that requires power to operate • Could be a light bulb, your computer, a toaster, etc. • Each device has a certain amount of ‘resistance’, R, in the unit called: OHMS (Ω) George Washington University Basic Circuit Components We represent real electrical components with symbols The Earth… …can be represented with this symbol …called the “ground” symbol The Ground • Represents 0 volts • We use it as a ‘reference’ voltage…to measure other voltages against it • The ‘Earth’ is at 0 volts, so we call this ground George Washington University Building a Circuit… We wish to ‘power’ our flashlight’s light bulb… We need a battery… 1.5 V We need to attach the light bulb to the battery… We use wires to connect the light bulb to the battery… Instead…let's represent the real components with their symbols George Washington University Building a Circuit…creating a schematic .5 Ω 1.5V 1.5 V Since this “node” is at GND (OV) this node must be 1.5Volts higher Replace the battery with a ‘DC Voltage Source’ symbol Replace the light bulb with a ‘Resistor’ symbol Mark the symbol’s values (V=, R=, etc.) Add the Ground reference 0V Instead…let's represent the real components with their symbols George Washington University Analyzing the Circuit…using Ohm’s Law .5 Ω 1.5V When we attach the resistor to the DC voltage source, current begins to flow How much current will flow? Ohm’s Law (V=IR) ->Describes the relationship between the voltage (V), current (I), and resistance (R) in a circuit Using Ohm’s Law, we can determin how much current is flowing through George Washington Universityour circuit 0V Analyzing the Circuit…using Ohm’s Law How much current will flow? I = 3 Amps .5 Ω 1.5V Use Ohm’s Law: V =I x R 1.5V =I x .5 Ω Solve for I: 0V I = 1.5V / .5 Ω = 3 Amps So, 3 Amps will flow through the .5 Ohm resistor, when 1.5 Volts are across it George Washington University Resistors in Series R1 = .5 Ω 1.5V Req R2 = .5 1 ΩΩ Resistors connected by only 1 terminal, back-to-back, are considered to be in ‘series’ We can replace the two series resistors with 1 single resistor, we call Req The value of Req is the SUM of R1 & R2: Req=R1+R2=.5 Ω + .5 Ω = 1Ω 0V George Washington University Resistors in Series I = 1.5 Amps Now we can find the current through the circuit using Ohm’s Law Use Ohm’s Law: 1.5V Req = 1 Ω V =I x Req 1.5V =I x 1 Solve for Ω I: I = 1.5V / 1 Ω = 1.5 Amps 0V The bigger the resistance in the circuit, the harder it is for current to flow George Washington University I = 1.5 Amps Resistors in Series The current is the SAME through each resistor R1 = .5 Ω 1.5V Back to our original series circuit, with R1 and R2 R2 = .5 Ω 0V Current flows like water through the circuit, notice how the 1.5 Amp ‘stream of current’ flows through both resistors equally Ohm’s Law shows us voltage across each resistor: V(R1) = 1.5Amps x .5 Ω = .75V V(R2) = 1.5Amps x .5 Ω = .75V George Washington University Resistors in Parallel 1.5V R1 = .5 Ω Resistors connected at 2 terminals, sharing the same node on each side, are considered to be in ‘parallel’ Unlike before, we cannot just add them. We must add their inverses to find 1 1 1 R2 = .5 Ω Req: 0V George Washington University Re q R1 R 2 1 1 1 Re q .5 .5 Req = .25 Ω Resistors in Parallel I = 6 Amps This is the equivalent circuit Use Ohm’s Law, we find the current through Req: 1.5V Req = .25 Ω V =I x Req 1.5V =I x .25 Solve for Ω I: I = 1.5V / .25 Ω = 6 Amps 0V The small the resistance in the circuit, the easier it is for current to flow George Washington University Resistors in Parallel Back to our original series circuit, with R1 and R2 The current is NOT the SAME through all parts of the circuit Current flows like water 1.5V through the circuit, notice how the 6 Amp ‘stream of current’ splits to flow into the two resistors R1 = .5 Ω R2 = .5 Ω The Voltage across each resistor is equal when they are in parallel 0V George Washington University Resistors in Parallel I = 6 Amps I=3A I=3A 1.5V The voltage is 1.5 V across each resistor Ohm’s Law tells us the current through each: I(R1)= V / R = 1.5V / .5 Ω = 3A I(R2)= V / R = 1.5V / .5 Ω = 3A R1 = .5 Ω 0V The 6Amps of current has split down the two legs of R2 = .5 Ω our circuit It split equally between the two legs, because the resistors have the same value George Washington The current will split differently if the University resistors are not equal… In Summary… Ohm’s Law: V=IR Describes the relationship between the voltage (V), current (I), and resistance (R) in a circuit Current is equal through two resistors in series Voltage drops across each resistor Req = R1 + R2 + . . . Voltage is equal across two resistors in parallel Current splits through branches of parallel circuits 1/Req = 1/R1 + 1/R2 George Washington University In Lab Today You will build series circuits Build parallel circuits Work with a breadboard Verify Ohm’s Law by measuring voltage using a multimeter And yes, there is HW! George Washington University