ASSIGNMENT 1
CONDUCTOR AND INDUCTOR

TYPE OF INDUCTOR

TYPE OF CAPACITOR

FIXED

VARIABLE

IRON CORE

FERRITE CORE

AIR CORE

CORE LOSS

DEFINITION OF INDUCTOR

CALLED CHOKE IS ANOTHER PASSIVE TYPE ELECTRICALCOMPONENT DESIGNED TO TAKE ADVANTAGES OF THIS RELATIONSHIP BY PRODUCING A MUCH STRONGER MAGNETIC FIELD THAN ONE THAT WOULD BE PRODUCED BY A SIMPLE COIL

SYMBOL OF INDUCTANCE IS L
UNIT OF INDUCTANCE IS Henry
INDUCTANCE-the propety of an electric circuit by which an electromotive force is induced in it as the result of changing magnetic flux
ELECTROMAGNET-temporary magnet production due to flow of electric current
ELECTROMAGNETIC INDUCTION-production process electric form magnet

FIXED

VARIABLE

UNPOLARISED

POLARIZED

CERAMIC

FILM

MICA

AIR GAP

PAPER

ALUMINIUM

TANTALUM

TRIMMER

DEFINITION OF CAPACITOR

CAPACITOR IS AN ELECTRICAL DEVICE THAT IS USED TO STORED ELECTRICAL ENERGY

UNIT OF CAPACITANCE IS FARAD.THE SYMBOL IS C**

CAPACITANCE IS DEFINED TO BE THE AMOUNT OF CHARGE Q STORED IN BETWEEN THE TWO PLATES FOR A POTENTIAL DIFFERENCE OR VOLTAGE V EXISTING ACROSS THE PLATES

capacitance
q = charge
C = capacitance
V = voltage

CONSTRUCTION OF INDUCTOR

Inductor stores electrical energy in form of magnetic field.
Inductor is made of coil formed by conductive materials like copper,aluminium etc. The material around and within the coil affects its properties; common types are air-core (only a coil of wire), iron-core, and ferrite core. Iron and ferrite types are more efficient because they conduct the magnetic field much better than air; of the two, ferrite is more efficient because stray electricity cannot flow through it. Ferrite is more expensive but operates at much higher frequencies than iron cores.

CIRCUIT WITH INDUCTIVE LOAD

1. ELECTROMAGNETIC INDUCTION An e.m.f is induced in the conductor as a result of its movement across the
magnetic field͘ This effect is known as ͚electromagnetic induction͛͘ 2. FARADAY'S LAW
An induced e.m.f is setup whenever the magnetic field linking that circuit
changes.The magnitude of the induced e.m.f in any circuit is proportional to the rate of change of the magnetic flux linking the circuit.

THE FACTORS THAT INFLUENCE INDUCTANCE


i) The number of turns of wire (N) ʹ more turns the higher the inductance
ii) The cross-sectional area of the coil of wire (A) ʹ the greater the cross-sectional area
the higher the inductance
iii) The presence of magnetic core - when the coil is wound on an iron core, the same
current sets up a more concentrated magnetic field and the inductance is increased
iv) The way turns are arranged ʹ a short tick coil of wire has a higher inductance than
the along thin one.

CONSTRUCTION OF CONDUCTOR
By applying a voltage to a capacitor and measuring the charge on the plates, the ratio of
the charge Q to the voltage V will give the capacitance value of the capacitor and is therefore
given as: C = Q/V this equation can also be re-arranged to give the more familiar formula for the
quantity of charge on the plates as: Q = C x V.

CAPACITOR EQUIVALENT CIRCUITS

PARALLEL
Total charge,
QT = Q1 + Q2 + Q3
CTE = C1V1 + C2 V2 + C3 V3
Total voltage
ET = e1 = e2 = e3
Total equivalent circuit capacitance
CT = C1 + C2 + C3
It follows that for n parallel connected
capacitors:
CT = C1 + C2 + C3 н͙͙н Cn

SERIES-PARALLEL Total equivalent circuit capacitance Ct=C1/(C2+C3)

SERIES
Total voltage
VT = e1 + e2 + e3
Where CT is the total equivalent circuit
capacitance
1/CT=1/C1+1/C2+1/C3+....

ELEMENT RELATED TO CAPACITANCE
a.Electric field:
b. Line of electric force: .
c. Electric flux:
d. Electric flux density (D):
e. Electric field strength:
f. Dielectric: .
g. Absolute permittivity (ɸ):

FACTOR EFFECTING CAPACITANCE
a.Capacitance between two plates proportional to the surface area
b. Capacitance between two plates inversely proportional to the thickness of
dielectric
c. Increasing the dielectric constant of the material between the plates

CHARGING AND DISCHARGING AADADADA. rc-rc5

INDUCTANCE EQUIVALENTS CIRCUIT

PARALLEL
Total voltage,
ET = e1 = e2
Total current,
IT = I1 + I2
Total inductance
1/LT=1/L1+1/L2

SERIES-PARALLEL
Total current,
IT = I1 +I2
Total inductance,
LT=L1+(L2L3/(L2+L3))

SERIES
Total voltage,
ET = e1 + e2
Total inductance,
LT = L1 + L2
Current, I = IL1 = IL2

RISE AND DECAY CURRENT rise-of-current-in-inductive-circuit decay-of-current-in-inductive-circuit