Showing posts with label circuit analysis. Show all posts
Showing posts with label circuit analysis. Show all posts

Saturday, September 1, 2012

Using Circuit Magic to calculate Norton Thévenin's & Norton's equivalents

Sample circuit shown below

Step 1 Remove branch connecting
node 1 and node 2.



Step 2: Solve circuit using Node
Voltage method.
Result shown below.
V1=-10
V2=0
V3=-5
V4=-5
V5=0



Step 3.: Resistance calculation. Remove
All DC Voltage sources and branches
with current sources. And connect
node 1 and node 2 using the branch
with current source (current =1 A). (as
shown below)



Step 4: Solve circuit using node voltage
method.
V1=-7,2727
V2=4,5455
V3=-3,6364
V4=-0,90909
V5=0


Step 5. Calculate resistance using
Ohms law.



ohms


Thévenin's equivalent



Monday, August 27, 2012

Resistors in Series & Resistors in Parallel

Series Connection
A series circuit is one with all the loads
in a row. Like links in a chain. There is
only one path for the electricity to
flow.


Parallel Connection
A parallel circuit is one that has two or
more paths for the electricity to flow.
In other words, the loads are parallel
to each other.


Sunday, August 26, 2012

Norton & Thevenin theorem

Thé venin's Theorem

Any voltage network which may be
viewed from two terminals can be
replaced by a voltage-source
equivalent circuit comprising a single
voltage source E and a single series
resistance R.. The voltage V is the
open-circuit voltage between the two
terminals and the resistance Z is the
resistance of the network viewed from
the terminals with all voltage sources
removed from circuit.


Sample




All circuits are equivalent. Resistors
R1,R2, R3 and voltage source are
transformed into Required Eq,


see parallel,
series simplifications.


To determine Eequ we shall break off
branch connecting node 1 and node
2




Norton's Theorem


Any current network which may be
viewed from two terminals can be
replaced by a current-source
equivalent circuit comprising a single
current source I and a single shunt
conductance G. The current I is the
short-circuit current between the two
terminals and the conductance G is
the conductance of the network
viewed from the terminals with all
branches containing current sources
are broken off.