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Circuit Elements Voltage and current sources Electrical resistance

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Presentation on theme: "Circuit Elements Voltage and current sources Electrical resistance"— Presentation transcript:

1 Circuit Elements Voltage and current sources Electrical resistance
Kirchhoff’s Laws Resistive Circuits

2 Voltage and current sources
An electrical source is a device that is capable of converting nonelectric energy to electric energy (and vice versa) An ideal voltage source is a circuit element that maintains a prescribed voltage across its terminals regardless of current flowing in these terminals An ideal current source is a circuit element that maintains a prescribed current across its terminals regardless of voltage across the terminals

3 Ideal voltage source Current-voltage characteristic Circuit symbol

4 Ideal current source Current-voltage characteristic Circuit symbol

5 Connections of ideal sources
Valid connections

6 Connections of ideal sources
Invalid connections

7 Connections of ideal sources
Valid or invalid?

8 Electrical resistance
Resistance is the capacity of materials to impede the flow of current A resistor is a circuit element that displays this behavior Current-voltage characteristic Circuit symbol

9 Electrical resistance, cont.
Resistor’s obey Ohm’s Law: V = I R The voltage “drop” across a resistor is linearly proportional to the current passing through the resistor

10 Electrical resistance, cont.
Example #1 I = V/R = 5V/1E3W = 5mA

11 Electrical resistance, cont.
Example #2 What is voltage drop across R1 What is voltage polarity?

12 Kirchhoff’s Laws A node is a point in a circuit where two or more elements meet

13 Kirchhoff’s current law
The algebraic sum of all the currents at any node in a curcuit equals zero I1 + I2 + I3 = 0

14 Kirchhoff’s voltage law
The algebraic sum of all the voltages around any closed path in a circuit equals zero VR3 + VR1 + VR2 + VC0 + VC4 = 0

15 Resistors in series Using KVL and KCL, we have: -V1 + I*R1 + I*R2 = 0
I*( ) = I = 30V/30W = 1A

16 Resistors in series Resistors in series add together
This is equivalent to: Rs = R1 + R2 Resistors in series add together

17 Resistors in parallel Using KVL and KCL, we have:
V1 = I1R1 = I2R2 = 10V I1 = 0.100A I2 = 0.033A It = = 0.133A

18 Resistors in parallel Resistors in parallel are
This is equivalent to: Resistors in parallel are combined by adding their reciprocals 1/Rp = 1/R1 + 1/R2

19 Classwork Find (a) the current through R3, (b) the current
through R2, and (c) voltage across R1


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