Nodal Analysis

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 NODAL ANALYSIS:

 

Nodal analysis involves looking at a circuit and determining all the node voltages in the circuit. The voltage at any given node of a circuit is the voltage drop between that node and a reference node (usually ground). Once the node voltages are known any of the currents flowing in the circuit can be determined. The node method offers an organized way of achieving this.


Approach:

 

Firstly all the nodes in the circuited are counted and identified. Secondly nodes at which the voltage is already known are listed. A set of equations based on the node voltages are formed and these equations are solved for unknown quantities. The set of equations are formed using KCL at each node. The set of simultaneous equations that is produced is then solved. Branch currents can then be found once the node voltages are known. This can be reduced to a series of steps:

Step 1: Identify the nodes

Step 2: Choose a reference node

 

Step 3: Identify which node voltages are known if any Step 4: Identify the BRANCH currents

 

Step 5: Use KCL to write an equation for each unknown node voltage Step 6: Solve the equations

 

This is best illustrated with an example. Find all currents and voltages in the following circuit using the node method. (In this particular case it can be solved in other ways as well)


Step 1:

There are four nodes in the circuit. A, B, C and D

 

Step 2:

Ground, node D is the reference node.

 

Step 3:

Node voltage B and C are unknown. Voltage at A is V and at D is 0

 

Step 4:

The currents are as shown. There are 3 different currents


Step 5:

I need to create two equations so I apply KCL at node B and node C

 

The statement of KCL for node B is as follows:


The statement of KCL for node C is as follows:


Step 6:

 

We now have two equations to solve for the two unknowns VB and VC. Solving the above two equations we get:


Further Calculations

 

The node voltages are know all known. From these we can get the branch currents by a simple application of Ohm's Law:



Problem 1: Find the current through each resistor of the circuit shown in fig, using nodal analysis


Solution:

 

At node1,

 

-I1-I2-I3 = 0 -[V1-15/1]-[V1/1][V1-V2/0.5] = 0

-V1+15-V1-2V1+2V2 = 0

4V1-2V2 = 15 --------------------- (1)

At node2,

I3-I4-I5 = 0

V1-V2/0.5 –V2/2 –V2-20/1 = 0

2V1-2V2-0.5V2-V2 + 20 = 0

2V1-3.5V2 = -20 ------------------ (2)

Multiplying (2) by 2 & subtracting from (1)

5V2 = 55 V2 = 11V V = 9.25V

 

I1 = V1-5/1 = 9.25-15 = -5.75A = 5.75 I2 = V1/1 = 9.25A

 

I3 = V1-V2/0.5 = -3.5A = 3.5A ÃŸ I4 = V2/2 = 5.5A

I5 = V2-20/I = 11-20/1 = -9A=9A.

 

Problem 2: For the bridge network shown in Figure determine the currents in each of the resistors.


 

Let the current in the 2 resistor be I1, and thens currentby law,Kirchhoff’thecurrentinthe14 resistor is (I -I1). Let the current in the 32 resistor be I2 as shown in Figure Then the current in the 1resistor is (I1 - I2) and that in the 3 resistor is (I - I1 + I2). Applying Kirchhoff’s and moving in a clockwise direction as shown in Figure gives:

 


54 = 2I1 +11(I1 _-I2)

 i.e. 13I1 - 11I2 = 54

 

Applying Kirchhoff’s voltage law to loop 2 and direction as shown in Figure gives:

 

0 = 2I1 + 32I2 -14(I - I1

However I = 8 A

Hence 0 = 2I1 + 32I2 –14(8 -_I1) i.e. 16I1 + 32I2 = 112

Equations (1) and (2) are simultaneous equations with two unknowns, I1 and I2.

16 * (1) gives: 208I1 _-176I= 864

16 * (1) gives: 208I1 _-176I2    = 864

13 * (2) gives: 208I1 + 416I2    = 1456

(4) - (3) gives:       592I2 = 592, I2 = 1 A

Substituting for I2 in (1) gives:

13I1 - 11 = 54                           

I1 = 65/13 = 5 A                      

Hence,                            

the current flowing in the 2     resistor  = I1 = 5 A

the current flowing in the 14             resistor = I -I1 = 8 -5 = 3 A

the current flowing in the 32             resistor = I2 = 1 A

the current flowing in the 11             resistor = I1 - I2 = 5 -1 = 4 A and

the current flowing in the 3     resistor = I - I1 + I2 = 8 - 5 + 1 = 4 A

Problem 3: Determine the values of currents I, I1 and I2 shown in the network of Figure


Total circuit impedance,

ZT = 5 + (8)(j6)/8 + j6

= 5 + (j48)(8 - j6)/82 + 62

= 5 + (j384 + 288)/100 

 

=  (7.88 + j3.84) or 8.776 25.98° A Current I = V/ZT

 

=           50∟   0°/8.77∟   25.98° 

= 5.7066 25.98° A 

Current I1 = I (j6/8 + j6)

=           (5.702∟5.98°)   (6∟   90°)/10∟   36.87° 

= 3.426∟27.15° A 

Current I2 = I (8/ (8 + j6)

=           (5-.2570∟.98°)*8∟   0°/10∟   36.87° 

= 4.5666 62.85° A 

[Note:            I   =   I1   +   I2-62.=85°  3.42   ∟27.15°   +   4.56∟

= 3.043 + j1.561 + 2.081 - j4.058 

= 5.124 - j2.497 A = 5.706 -25.98° A 

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