An electric circuit is a path in which electrons from a voltage or current source flow. The point where those electrons enter an electrical circuit is called the "source" of electrons.
2. Electrical Circuits
• Electric circuit consists of any number of elements joined at
terminal points, providing at least one closed path through
which charge can flow
• + terminal of battery attracts the electrons through the wire at
the same rate at which electrons are supplied by the –
terminal
• Two types: (1) Series circuit (2) Parallel circuit
3. Series Circuit and Parallel Circuit
Two elements are in series if one is
connected end on end and have
only one terminal in common and
the common point is not connected
to another current carrying element
Characteristics of series circuit
• current is same through all the resistors
• voltage drop across each is different depending on its
resistance and
• sum of the three voltage drops is equal to the voltage
applied across the resistors.
4. Series Circuit
• Voltage drop across each resistor (using Ohm’s) is
V1 = I. R1, V2 = I. R2, V3 = I. R3
• Voltage applied = Sum of the voltage drops
E = V1 + V2 + V3 = I. R1 + I. R2 + I. R3
E = I (R1 + R2 + R3)
But E = I R, R = Equivalent resistance of the series combination
So I R = = I (R1 + R2 + R3)
• R = R1 + R2 + R3
5. Series Circuit
• Power delivered to each resistor
P1 = V1I = I2
R1 = V1
2
/R1, P2 = V2I = I2
R2 = V2
2
/R2,
and P3 = V3I = I2
R3 = V3
2
/R3
• The power delivered by the source, P = E I
• The total power delivered to a resistive network is equal to the
total power dissipated by the resistive elements.
• That is, Pdel = P1 + P2 + P3 + ……
6. Series Circuit
• Ex: (a) Find the total resistance for the series circuit of Fig. 2.3.
(b) Calculate the source current IS.
(c) Determine the voltages V1, V2 and V3 .
(d) Calculate the power dissipated by R1, R2, and R3.
(e) Determine the power delivered by the source, and compare it to the sum of
the powers dissipated in the resistor R1, R2, and R3.
7. Parallel Circuit
Two elements, branches, or networks are in parallel if they have
two points in common as shown in Fig.
All the elements have terminals a and b in common
Characteristics of parallel circuit
– potential difference across all resistance is the same,
– current in each resistor is different and is given by
Ohm’s law and
– total current is the sum of the three separate currents
8. Terminals of battery are connected directly across resistors R1 and R2(Fig.2.5)
I1 = E/R1, I2 = E/R2,
And I = I1 + I2 = E/R1 + E/R2 = E( 1/R1 + 1/R2)
And I = E/R, where R is equivalent resistance of the parallel combination
So, E/R = E( 1/R1 + 1/R2) so 1/R = 1/R1 + 1/R2
If n number of resistors are connected in parallel as in Fig.2.6
Total resistance
Parallel Circuits
10. A
Parallel Circuits
For the parallel network of Fig. 2.7,
a) Calculate RT
, (b) Determine IS
,
(c) Calculate I1
and I2
and demonstrate that IS
= I1
+ I2
.
(d) Determine the power to each resistor
(e) Determine the power delivered by the source, and compare it to the
total power dissipated by the resistors.
12. Kirchhoff’s voltage law
Kirchhoff’s voltage law (KVL) states that the algebraic sum of
the potential rises and drops around a closed loop (or path) is
zero.
To apply Kirchhoff’s voltage law, the summation of potential
rises and drops must by made in one direction around the
closed loop. A plus sign is assigned to a potential rise – to +)
and a minus sign to a potential drop (+ to -).
According to Kirchhoff’s voltage law from Fig.
Applied voltage = sum of voltage drops in series elements
t is, the applied voltage of a series circuit equals the sum of the voltage drops across the series elements. Kirchhoff’s can also be stated
13. Ex: Determine the unknown voltages for Fig. 2.10.
Ex: For the circuit of Fig. 2.11:
(a)Determine V2 using Kirchhoff’s Voltage law.
(b)Determine I.
(c) Find R1 and R2.
Kirchhoff’s voltage law
14. Voltage divider rule
•In series circuits, the voltage across the resistive elements will
divide as the magnitude of the resistive levels
•Voltage divider rule (VDR) permits determining the
voltage levels without first finding the current
•VDR can be derived by analyzing the network
• Applying Ohm’s law
•In general, VDR
• VDR states that the voltage across a resistor in a series
circuit is equal to the value of that resistor times the total
impressed voltage across the series elements divided by the
15. Voltage divider rule
Example: Using voltage divider rule, determine V1 and V3 for the series circuit
of Fig. 2.13.
• EX : Design the voltage divider of Fig. 5.30 such that VR1 4VR2
• Total resistance
•
16. Kirchhoff’s current law
•Kirchhoff’s current law states that the algebraic sum of the
currents entering and leaving an area, system, or junction is zero.
•In other words, the sum of the currents entering an area, system, or junction
must equal the sum of the currents leaving the area, system, or junction.
•In equation form:
18. Current divider rule (CDR)
Current divider rule determines the current entering a set of
parallel branches will split between the elements.
•For two parallel elements of equal value, the current will divide equally.
•For parallel elements with different values, the smaller the resistance, the
greater the share of input current.
•For parallel elements of different values, the current will split with a ratio
equal to the inverse of their resistor values.
Input current
and
Current I1 Current I2
19. Current divider rule (CDR)
The current through any parallel branch is equal to the product of
the total resistance of the parallel branches and the input current
divided by the resistance of the branch through which the current
is to be determined.
For the particular case of two parallel resistors, as shown
and
20. Current divider rule (CDR)
Ex: Determine the current I2 for network of Fig. 2.20 using current divider rule
Ex: Determine the magnitudes of currents I1, I2 and I3 for network of Fig. 2.21
Using CDR
Applying KCL
Using CDR again
Total current entering the parallel branches
must equal that leaving
21. Open circuit (OC) and short circuits (SC)
Open Circuit
• simply two isolated terminals not connected by an element of any kind, as
shown in Fig.
• OC current must be always be zero
• Voltage across OC can be determined by the system it is connected to
• OC can have a p.d (voltage) across its terminals, but the current is always
zero amperes
Short circuit
• a very low resistance, direct connection between the terminals of a
network, as shown in Fig.
• Current through the short circuit can be any value, as determined by the
system is connected to
• Voltage across SC will always by zero volts (V = IR = I (0) = 0 V)
• SC can carry a current of a level determined by the external circuit, but p.d
(voltage) across its terminals is always zero volts