Mesh-Current Method - Lecture Slides | ES A309, Study notes of Engineering

Material Type: Notes; Professor: Miller; Class: Elements of Electrical Engineering; Subject: Engineering Science ; University: University of Alaska - Anchorage; Term: Fall 2008;

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ES309
Elements of Electrical Engineering
Lecture #6
Jeffrey Miller, Ph.D.
Outline
Chapter 4.5-4.8
Mesh-Current Method
Mesh
A loop with no other loops inside of it
Mesh Current
Current that exists only in the perimeter of a
mesh
NOTE: Mesh-Current Method is applicable
only to planar circuits
Mesh-Current Method
Identify all of the meshes in the circuit by drawing
a curved arrow to identify the direction the current
is flowing in the mesh
Assign a variable name to the current in each
mesh
Use Kirchhoff’s Voltage Law to write an equation
around each of the meshes in the direction of the
current arrow
Solve the equations
Calculate the desired output value
pf3
pf4
pf5

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ES

Elements of Electrical Engineering

Lecture

Jeffrey Miller, Ph.D.

Outline

• Chapter 4.5-4.

Mesh-Current Method

• Mesh

  • A loop with no other loops inside of it

• Mesh Current

  • Current that exists only in the perimeter of a mesh

NOTE: Mesh-Current Method is applicable

only to planar circuits

Mesh-Current Method

  • Identify all of the meshes in the circuit by drawing a curved arrow to identify the direction the current is flowing in the mesh
  • Assign a variable name to the current in each mesh
  • Use Kirchhoff’s Voltage Law to write an equation around each of the meshes in the direction of the current arrow
  • Solve the equations
  • Calculate the desired output value

Mesh-Current/Kirchhoff Example

Assume v 1 , v 2 , R 1 , R 2 , R 3 are given Find i 1 , i 2 , i 3 First do this problem using Kirchhoff’s Laws, then using the Mesh-Current method

Mesh-Current Example –

Kirchhoff’s Approach

  • Using Kirchhoff’s Current Law, we get: i 1 = i 2 + i 3
  • Using Kirchhoff’s Voltage Law, we get: v 1 = i 1 R 1 + i 3 R 3 -v 2 = i 2 R 2 – i 3 R 3

Mesh-Current Example –

Kirchhoff’s Approach

Using i 3 = i 1 – i 2

v 1 = i 1 R 1 + i 3 R 3 v 1 = i 1 R 1 + (i 1 – i 2 )R 3 v 1 = i 1 (R 1 + R 3 ) – i 2 R 3

-v 2 = i 2 R 2 – i 3 R 3 -v 2 = i 2 R 2 – (i 1 – i 2 ) R 3 -v 2 = -i 1 R 3 + i 2 (R 2 + R 3 )

Mesh-Current Example –

Mesh-Current Approach

  • Apply Kirchhoff’s voltage law around the two meshes v 1 = iaR 1 + (ia – ib) R 3 -v 2 = (ib – ia) R 3 + ibR 2

Mesh-Current Sample Problem

40V = 2Ω ia + 8Ω (ia – ib)

0 = 8Ω (ib – ia) + 6Ω ib + 6Ω (ib – ic)

-20V = 6Ω (ic – ib) + 4Ω ic

Mesh-Current Sample Problem

ia = 5.6A ib = 2.0A ic = -0.80A p40V = -40V ia = -40V * 5.6A = -224W p20V = 20V ic = 20V * -0.80A = -16W So both voltage sources are delivering power to the circuit

Mesh-Current Sample Problem

The current across the 8Ω resistor is ia – ib So the voltage drop across the resistor is v 0 = 8Ω (ia – ib) = 8Ω (5.6A – 2.0A) = 8Ω (3.6A) = 28.8V

Node-Voltage vs Mesh-Current

• What is the advantage to using the Node-

Voltage or the Mesh-Current method over

Kirchhoff’s and Ohm’s Laws?

  • It reduces the number of simultaneous equations that need to be manipulated

• When does one use the Node-Voltage

method over the Mesh-Current method?

  • There is no answer, but one method may result in fewer simultaneous equations

Mesh-Current Example

  • Find i 0 in the following diagram using the mesh- current method.

Mesh-Current Example

-50V + 2Ω (ia – ib) + 6Ω (ia – ic) = 0 10Ω ib + 8Ω (ib – ic) + 2Ω (ib – ia) = 0 -10V + 6Ω (ic – ia) + 8Ω (ic – ib) = 0 ia = 16A ib = 6A ic = 11A i 0 = ia – ic = 5A

Homework

No Chapter 4 Homework Yet!