CIRCUITS by Ulaby & Maharbiz

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Presentation transcript:

CIRCUITS by Ulaby & Maharbiz 3. Analysis Techniques CIRCUITS by Ulaby & Maharbiz

Overview

Node-Voltage Method Node 1 Node 3 Node 2 Node 2 Node 3

Node-Voltage Method Three equations in 3 unknowns: Solve using Cramer’s rule, matrix inversion, or MATLAB

Supernode A supernode is formed when a voltage source connects two extraordinary nodes Current through voltage source is unknown Less nodes to worry about, less work! Write KVL equation for supernode Write KCL equation for closed surface around supernode

KCL at Supernode = Note that “internal” current in supernode cancels, simplifying KCL expressions Takes care of unknown current in a voltage source

Example 3-3: Supernode Solution: Supernode Determine: V1 and V2

Mesh-Current Method Two equations in 2 unknowns: Solve using Cramer’s rule, matrix inversion, or MATLAB

Example 3-5: Mesh Analysis But Mesh 1 Hence Mesh 2 Mesh 3

Supermesh A supermesh results when two meshes have a current source( with or w/o a series resistor) in common Voltage across current source is unknown Write KVL equation for closed loop that ignores branch with current source Write KCL equation for branch with current source (auxiliary equation)

Example 3-6: Supermesh Mesh 1 Solution gives: Mesh 2 SuperMesh 3/4 Supermesh Auxiliary Equation

Nodal versus Mesh When do you use one vs. the other? What are the strengths of nodal versus mesh? Nodal Analysis Node Voltages (voltage difference between each node and ground reference) are UNKNOWNS KCL Equations at Each UNKNOWN Node Constrain Solutions (N KCL equations for N Node Voltages) Mesh Analysis “Mesh Currents” Flowing in Each Mesh Loop are UNKNOWNS KVL Equations for Each Mesh Loop Constrain Solutions (M KVL equations for M Mesh Loops) Count nodes, meshes, look for supernode/supermesh

Nodal Analysis by Inspection Requirement: All sources are independent current sources

Example 3-7: Nodal by Inspection Off-diagonal elements Currents into nodes G11 G13 @ node 1 @ node 2 @ node 3 @ node 4

Mesh by Inspection Requirement: All sources are independent voltage sources

A circuit is linear if output is proportional to input Linearity A circuit is linear if output is proportional to input A function f(x) is linear if f(ax) = af(x) All circuit elements will be assumed to be linear or can be modeled by linear equivalent circuits Resistors V = IR Linearly Dependent Sources Capacitors Inductors We will examine theorems and principles that apply to linear circuits to simplify analysis

Superposition Superposition trades off the examination of several simpler circuits in place of one complex circuit

Example 3-9: Superposition Contribution from I0 alone Contribution from V0 alone I1 = 2 A I2 = ‒3 A I = I1 + I2 = 2 ‒ 3 = ‒1 A

Cell Phone Today’s systems are complex. We use a block diagram approach to represent circuit sections.

Equivalent Circuit Representation Fortunately, many circuits are linear Simple equivalent circuits may be used to represent complex circuits How many points do you need to define a line?

voltage across output with no load (open circuit) Thévenin’s Theorem Linear two-terminal circuit can be replaced by an equivalent circuit composed of a voltage source and a series resistor voltage across output with no load (open circuit) Resistance at terminals with all independent circuit sources set to zero

Norton’s Theorem Linear two-terminal circuit can be replaced by an equivalent circuit composed of a current source and parallel resistor Current through output with short circuit Resistance at terminals with all circuit sources set to zero

How Do We Find Thévenin/Norton Equivalent Circuits ? Method 1: Open circuit/Short circuit 1. Analyze circuit to find 2. Analyze circuit to find Note: This method is applicable to any circuit, whether or not it contains dependent sources.

Example 3-10: Thévenin Equivalent

How Do We Find Thévenin/Norton Equivalent Circuits? Method 2: Equivalent Resistance 1. Analyze circuit to find either or 2. Deactivate all independent sources by replacing voltage sources with short circuits and current sources with open circuits. 3. Simplify circuit to find equivalent resistance Note: This method does not apply to circuits that contain dependent sources.

Example 3-11: RTh (Circuit has no dependent sources) Replace with SC Replace with OC

How Do We Find Thévenin/Norton Equivalent Circuits? Method 3:

Example

To find

In many situations, we want to maximize power transfer to the load

Tech Brief 5: The LED

BJT: Our First 3 Terminal Device! Active device with dc sources Allows for input/output, gain/amplification, etc

BJT Equivalent Circuit Looks like a current amplifier with gain b

Digital Inverter With BJTs Out 1 BJT Rules: Vout cannot exceed Vcc=5V Vin cannot be negative Output high Input low In Out Output low Input high

Nodal Analysis with Multisim See examples on DVD

Multisim Example: SPDT Switch

Tech Brief 6: Display Technologies

Tech Brief 6: Display Technologies Digital Light Processing (DLP)

Summary