CIRCUIT ANALYSIS METHODS Topic 3 CIRCUIT ANALYSIS METHODS

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CIRCUIT ANALYSIS METHODS Topic 3

CIRCUIT ANALYSIS METHODS Topic 3

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit Norton equivalent circuit Maximum power transfer Superposition principle

INTRODUCTION OF NODEVOLTAGE METHOD • Use KCL. • Important step: select one of the

INTRODUCTION OF NODEVOLTAGE METHOD • Use KCL. • Important step: select one of the node as reference node • Then define the node voltage in the circuit diagram.

Node-voltage example

Node-voltage example

 • In the diagram, node 3 is define as reference node and node

• In the diagram, node 3 is define as reference node and node 1 and 2 as node voltage V 1 and V 2. • The node-voltage equation for node 1 is,

 • Node-voltage equation of node 2,

• Node-voltage equation of node 2,

 • Solving for V 1 and V 2 yields

• Solving for V 1 and V 2 yields

THE NODE-VOLTAGE METHOD AND DEPENDENT SOURCES • If the circuit contains dependent sources, the

THE NODE-VOLTAGE METHOD AND DEPENDENT SOURCES • If the circuit contains dependent sources, the node-voltage equations must be supplemented with the constraint equation imposed by the presence of the dependent sources.

example… Use the node-voltage method to find the power dissipated in the 5Ω resistor.

example… Use the node-voltage method to find the power dissipated in the 5Ω resistor.

 • The circuit has 3 node. • Thus there must be 2 node-voltage

• The circuit has 3 node. • Thus there must be 2 node-voltage equation. • Summing the currents away from node 1 generates the equation,

 • Summing the current away from node 2 yields,

• Summing the current away from node 2 yields,

 • As written, these two equations contain three unknowns namely V 1, V

• As written, these two equations contain three unknowns namely V 1, V 2 and iØ. • To eliminate iØ, express the current in terms of node-voltage,

 • Substituting this relationship into the node 2 equation,

• Substituting this relationship into the node 2 equation,

 • Solving for V 1 and V 2 gives,

• Solving for V 1 and V 2 gives,

 • Then,

• Then,

SPECIAL CASE • When a voltage source is the only element between two essential

SPECIAL CASE • When a voltage source is the only element between two essential nodes, the nodevoltage method is simplified.

Example…

Example…

 • There is three essential nodes, so two simultaneous equation are needed. •

• There is three essential nodes, so two simultaneous equation are needed. • Only one unknown node voltage, V 2 where as V 1=100 V. • Therefore, only a single nodevoltage equation is needed which is at node 2.

Using V 1 =100 V, thus V 2=125 V.

Using V 1 =100 V, thus V 2=125 V.

SUPERNODE • When a voltage source is between two essential nodes, those nodes can

SUPERNODE • When a voltage source is between two essential nodes, those nodes can be combine to form a supernode (voltage sourse is assume as open circuit).

Supernode example…

Supernode example…

 • Nodes chosen,

• Nodes chosen,

 • Node-voltage equation for node 2 and 3,

• Node-voltage equation for node 2 and 3,

 • Summing both equation, Above equation can be generates directly using supernode approach

• Summing both equation, Above equation can be generates directly using supernode approach

Supernode

Supernode

 • Starting with resistor 5Ω branch and moving counterclockwise around the supernode,

• Starting with resistor 5Ω branch and moving counterclockwise around the supernode,

 • Using V 1 =50 V and V 3 as a function of

• Using V 1 =50 V and V 3 as a function of V 2,

 • Substitute into the node-voltage equation,

• Substitute into the node-voltage equation,

 • Using V 2 value, gives

• Using V 2 value, gives

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit Norton equivalent circuit Maximum power transfer Superposition principle

INTRODUCTION OF MESHCURRENT METHOD • A mesh is a loop with no loop inside

INTRODUCTION OF MESHCURRENT METHOD • A mesh is a loop with no loop inside it. • A mesh current is the current that exist only in the perimeter of a mesh. • Mesh-current method use KVL to generates equation for each mesh.

Mesh-current example…

Mesh-current example…

 • Mesh-current circuit with mesh current ia and ib.

• Mesh-current circuit with mesh current ia and ib.

 • Use KVL on both mesh,

• Use KVL on both mesh,

 • Solving for ia and ib, and you can compute any voltages or

• Solving for ia and ib, and you can compute any voltages or powers of interest.

THE MESH-CURRENT METHOD AND DEPENDENT SOURCES • If the circuit contains dependent sources, the

THE MESH-CURRENT METHOD AND DEPENDENT SOURCES • If the circuit contains dependent sources, the mesh-current equations must be supplemented by the appropriate constraint equations.

Example…

Example…

 • Use the mesh-current method to determine the power dissipated in the 4Ω

• Use the mesh-current method to determine the power dissipated in the 4Ω resistor.

 • Using KVL,

• Using KVL,

 • But • Substituting into the mesh-current equation,

• But • Substituting into the mesh-current equation,

 • Using Cramer rule, the values of i 2 and i 3 can

• Using Cramer rule, the values of i 2 and i 3 can be determine,

 • Power dissipated by 4Ω resistor is

• Power dissipated by 4Ω resistor is

SPECIAL CASE (SUPERMESH) • When a branch includes a current source, the mesh-current method

SPECIAL CASE (SUPERMESH) • When a branch includes a current source, the mesh-current method can be simplified. • To create a supermesh, remove the current source from the circuit by simply avoiding the branch when writing the mesh-current equations.

 • Supermesh equation,

• Supermesh equation,

 • Mesh 2 equation,

• Mesh 2 equation,

 • From the circuit, ic –ia= 5 A • Using Cramer rule, the

• From the circuit, ic –ia= 5 A • Using Cramer rule, the three mesh current can be obtain.

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit Norton equivalent circuit Maximum power transfer Superposition principle

SOURCE TRANSFORMATION • Source transformation allows a voltage source in series with a resistor

SOURCE TRANSFORMATION • Source transformation allows a voltage source in series with a resistor to be replaced by a current source in parallel with the same resistor or vice versa.

Source transformation

Source transformation

Example…

Example…

 • Source transformation procedure From To method Use,

• Source transformation procedure From To method Use,

From To method Use,

From To method Use,

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit Norton equivalent circuit Maximum power transfer Superposition principle

THEVENIN EQUIVALENT CIRCUIT • Thevenin equivalent circuit consist of an independent voltage source, VTh

THEVENIN EQUIVALENT CIRCUIT • Thevenin equivalent circuit consist of an independent voltage source, VTh in series with a resistor RTh.

Thevenin equivalent circuit

Thevenin equivalent circuit

 • Thevenin voltage, VTh = open circuit voltage in the original circuit. •

• Thevenin voltage, VTh = open circuit voltage in the original circuit. • Thevenin resistance, RTh is the ratio of open-circuit voltage to the short-circuit current.

Example…

Example…

 • Step 1: node-voltage equation for open-circuit:

• Step 1: node-voltage equation for open-circuit:

 • Step 2: short-circuit condition at terminal a -b

• Step 2: short-circuit condition at terminal a -b

 • Node-voltage equation for shortcircuit:

• Node-voltage equation for shortcircuit:

Short-circuit current: Thevenin resistance:

Short-circuit current: Thevenin resistance:

Thevenin equivalent circuit

Thevenin equivalent circuit

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit Norton equivalent circuit Maximum power transfer Superposition principle

NORTON EQUIVALENT CIRCUIT • A Norton equivalent circuit consists of an independent current source

NORTON EQUIVALENT CIRCUIT • A Norton equivalent circuit consists of an independent current source in parallel with the Norton equivalent resistance. • Can be derive from a Thevenin equivalent circuit simply by making a source transformation. • Norton current, IN = the short-circuit current at the terminal of interest. • Norton resistance, RN = Thevenin resistance, RTh

Example

Example

Step 1: Source transformation

Step 1: Source transformation

Step 2: Parallel sources and parallel resistors combined

Step 2: Parallel sources and parallel resistors combined

Step 3: Source transformation, series resistors combined, producing the Thevenin equivalent circuit THEVENIN EQUIVALENT

Step 3: Source transformation, series resistors combined, producing the Thevenin equivalent circuit THEVENIN EQUIVALENT CIRCUIT

Step 4: Source transformation, producing the Norton equivalent circuit NORTON EQUIVALENT CIRCUIT

Step 4: Source transformation, producing the Norton equivalent circuit NORTON EQUIVALENT CIRCUIT

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit Norton equivalent circuit Maximum power transfer Superposition principle

MAXIMUM POWER TRANSFER • Two basic types of system: – Emphasizes the efficiency of

MAXIMUM POWER TRANSFER • Two basic types of system: – Emphasizes the efficiency of the power transfer – Emphasizes the amount of power transferred.

 • Maximum power transfer is a technique for calculating the maximum value of

• Maximum power transfer is a technique for calculating the maximum value of p that can be delivered to a load, RL. • Maximum power transfer occurs when RL=RTh.

Example…

Example…

 • Power dissipated by resistor RL

• Power dissipated by resistor RL

 • Derivative of p with repect to RL

• Derivative of p with repect to RL

 • Derivative is zero and p is maximum when

• Derivative is zero and p is maximum when

 • The maximum power transfer occurs when the load resistance, RL = RTh

• The maximum power transfer occurs when the load resistance, RL = RTh • Maximum pwer transfer delivered to RL:

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit

CIRCUIT ANALYSIS METHODS • • Node-Voltage method Mesh-current method Source transformation Thevenin equivalent circuit Norton equivalent circuit Maximum power transfer Superposition principle

SUPERPOSITION PRINCIPLE • In a circuit with multiple independent sources, superposition allows us to

SUPERPOSITION PRINCIPLE • In a circuit with multiple independent sources, superposition allows us to activate one source at a time and sum the resulting voltages and currents to determine the voltages and currents that exist when all independent sources are activate.

Step of Superposition principle 1. Deactivated all the sources and only remain one source

Step of Superposition principle 1. Deactivated all the sources and only remain one source at one time. Do circuit analysis to find voltages or currents. 2. Repeat step 1 for each independent sources. 3. Sum the resulting voltages or currents.

REMEMBER!!! 1. Independent voltage source will become short-circuit with 0Ω resistance. 2. Independent current

REMEMBER!!! 1. Independent voltage source will become short-circuit with 0Ω resistance. 2. Independent current source will become open-circuit. 3. Dependent sources are never deactivated when applying superposition.

Example…

Example…

 • Step 1: deactivated all sources except voltage source

• Step 1: deactivated all sources except voltage source

 • V 0 is calculated using voltage divider:

• V 0 is calculated using voltage divider:

 • Step 2: Deactivated all sources except current source

• Step 2: Deactivated all sources except current source

 • V 0 is calculated by using current divider:

• V 0 is calculated by using current divider:

 • Step 3: Sum all the resulting voltages: V 0 =2+5=7 V.

• Step 3: Sum all the resulting voltages: V 0 =2+5=7 V.

Question 1 (nodevoltage) • Calculate the value of Io

Question 1 (nodevoltage) • Calculate the value of Io

Solution • Node 1:

Solution • Node 1:

 • Node 2:

• Node 2:

Question 2 (mesh-current) • Determine the value of currents, I 1, I 2 and

Question 2 (mesh-current) • Determine the value of currents, I 1, I 2 and I 3.

 • Supermesh: • Mesh 3:

• Supermesh: • Mesh 3:

 • Dependent current source • Vo

• Dependent current source • Vo

 • Substitute V 0

• Substitute V 0

 • Use Cramer rule

• Use Cramer rule

 • Current I 2:

• Current I 2:

 • Current I 3:

• Current I 3:

Question 3 (thevenin)

Question 3 (thevenin)

 • Open-circuit voltage, Voc:

• Open-circuit voltage, Voc:

 • Node-voltage equation for Voc

• Node-voltage equation for Voc

 • Thevenin resistance, RTh:

• Thevenin resistance, RTh:

 • Thevenin equivalent circuit:

• Thevenin equivalent circuit:

Question 4 (norton)

Question 4 (norton)

 • Open-circuit current, Isc:

• Open-circuit current, Isc:

 • Norton resistance, RN: RN = 4Ω

• Norton resistance, RN: RN = 4Ω

 • Norton equivalent circuit:

• Norton equivalent circuit:

Question 5 (superposition) • Use superposition principle to determine the voltage Vo. +

Question 5 (superposition) • Use superposition principle to determine the voltage Vo. +

 • Deactivated current source +

• Deactivated current source +

 • Deactivated voltage source

• Deactivated voltage source

 • Summing the voltage V 0

• Summing the voltage V 0

Question 6 (node-voltage) • Determine the value of Vo.

Question 6 (node-voltage) • Determine the value of Vo.

node-voltage equation: Current iΔ:

node-voltage equation: Current iΔ:

 • Thus: V 0 =50 V

• Thus: V 0 =50 V