Electrical Circuits

Electrical Circuits
A simple Electric Circuit is a closed
connection
of Batteries
,
Resistors
,
Wires.
An
Electric circuit consist of voltage
loops
and current
nodes
.

The following physical quantities  are  measured  in
an electrical circuit;

Current,:
Denoted by  I measured in Amperes (A).

Resistance
,:

Denoted by  R  measured in  Ohms ( W
) .

Electrical
Potential Difference ,:
Denoted by  V 
measured
in  volts. (v)

 

Three basic laws govern the flow of current in an electrical circuit
:

1. Ohm’s
Law

2. Kirchhoff’s
Voltage Law
Conservation of Energy.

3. Kirchhoff’s
Current Law
Conservation of Charge .

 

 

 

 

Simple circuits are categorized  in  two type :

1. Series
Circuits

2. Parallel
Circuits

 

 For circuits with series and parallel sections, break the
circuit
up into portions of series and

parallel, then calculate values for these portions, and use these

values to calculate the resistance of the entire circuit. That is,

first,  for each individual series path, calculate the total
resistance
for that path.

Second, using these values, by assuming that each path as a single
resistor, calculate the total resistance of

the circuit.

Useful
Rules

 

 We can apply  the methods for solving linear systems to
solve
problems  involving  electrical circuits. In a given circuit
if  enough values of currents, resistance, and potential
difference 
is known, we should be able to find the other unknown values of these
quantities.
We mainly use the Ohm’s Law , Kirchhoff’s
Voltage
Law  and Kirchhoff’s current Law.

 

Example: 
Find the currents in the circuit for the following network.

Solution :
Lets
assign currents to each part of the  circuit between the node
points. 
We have two node points  Which will give us three different
currents. 
Lets assume that the currents are in clockwise direction.

 

 

 So the current on the segment EFAB is I1,
on
the segment BCDE is I3 and on the segment EB is I2

Using the  Kirchhoff’s current Law for
the
node  B   yields the equation

I1 + I2 = I3.

For the node E we will get the same
equation.Then
we use Kirchhoff’s  voltage law

-4 I1+ (-30) -5 I1 
– 10I1  -60  +10I2 =0

When  through the  battery from (-)
to (+),   on the segment EF,  potential difference 
is  -30, and on segment FA  moving through the resistor
of 
5W

 will result in the potential difference
of -5 I1  and  in a similar way we can find the
potential
differences on the other segment of the loop EFAB.

 

 In the  loop  BCDE, Kirchhoff’s 
voltage
law will yield the following equation:

-30 I3+ 120-10I2+60 =0

 Now we have three equations with three unknowns:

 I1         
+     I2   
–   
I3           =0


-19 I1  +10 I2                    
=
90


           
-10
I2      -30 I3         
= -180

 

 This linear system can be solved  by methods of linear
Algebra. 
Linear Algebra is more useful when the network is very complicated
and 
the number of the unknowns is large.

The system above has the following solution:

I1   = -1.698
I2 = 5.7736
I3  =
4.0755

 

Exercises,