Basic Electrical Quantities Capacitance. Capacitance A capacitor is constructed of two parallel...
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Transcript of Basic Electrical Quantities Capacitance. Capacitance A capacitor is constructed of two parallel...
Basic Electrical QuantitiesBasic Electrical Quantities
CapacitanceCapacitance
Capacitance
A capacitor is constructed of two parallel conducting plates separated by an insulator called dielectric
The conducting surfaces can be rectangular or circular
The purpose of the capacitor is to store electrical energy by electrostatic stress in the dielectric
ELECTRICAL SCIENCE
Some Capacitors
insulatorconductor
ELECTRICAL SCIENCE
Capacitance : Definition
Take two chunks of conductor
Separated by insulator Apply a potential V between
them Charge will appear on the
conductors, with Q+ = +CV on the higher-potential and Q- = -CV on the lower potential conductor
C depends upon both the “geometry” and the nature of the material that is the insulator
0
V
Q+ = +CV+++++++++++
++++++++++++++++++++++
-----------
-----------
----------
Q- = -CV
V
Parallel Plate Capacitor
When it is connected to a voltage source, there is temporary flow of electrons from plate A to plate B A capacitor has a capacitance of 1
farad (F) if 1 coulomb (C) of charge is deposited on the plates by a potential difference of 1 volt across its plates
The farad is named after Michael Faraday, a nineteenth century English chemist and physicist
Capacitance Capacitance is a measure of a
capacitor’s ability to store charge on its plates A capacitor has a capacitance of one
farad (F) if one coulomb (C) of charge is deposited on the plates by a potential difference of one volt across its plates
The farad is named after Michael Faraday, a nineteenth century English chemist and physicist
Capacitance Suppose we give Q coulomb of
charge to one of the two plates and if a P.D. of V volts is established between the two plates, then the capacitance is
Difference PotentialCharge
VQC
Hence, Capacitance is the charge required per unit Potential Difference
Parallel Plate Capacitor
V E
+Q
-Q-
+
VEdV
V E+Q
-Q-
+
VdEV
The potential difference between the battery terminals and the plates will create a field and charges will flow from the battery to the plates until the potential difference is zeroed.Capacitance is inversely proportional to the
distance between the plates.
Capacitance The farad is generally too large a
measure of capacitance for most practical applications
So microfarad (106 ) or picofarad (1012 ) is more commonly used
Different capacitors for the same voltage across their plates will acquire greater or lesser amounts of charge on their plates
Hence, the capacitors have greater or lesser capacitance
Parallel Plate Capacitor
Charge Q(+) Charge Q(-)
+ _
IA B
Capacitance
Dielectric – Insulator of the capacitor The purpose of the dielectric is to
create an electric field to oppose the electric field setup by free charges on the parallel plates
Di for “opposing” and electric for “electric field”
Capacitance With different dielectric materials
between the same two parallel plates, different amounts of charge will deposit on the plates
Permittivity – The ratio of the flux density to the electric field intensity in the dielectric. A measure of how easily the dielectric will “permit” the establishment of flux lines within the dielectric
Parallel-Plate Capacitor
1. Calculate field strength E as a function of charge ±Q on the plates
2. Integrate field to calculate potential V between the plates
3. Q=CV, C = V/Q
Area A -Q
EDielectric constant
Separation d
Area A +Q
V
Parallel-Plate Capacitor
0 0 0
. . .
aE dl dl a dlz d z d z d
zz
z z z
Q QVA A
Area A -Q
dl E d
Area A+Q
ââzz
aE from Gauss's LawzQA
QdVA
Q ACV d
Basic Electrical QuantitiesBasic Electrical Quantities
Capacitance in Series Capacitance in Series & Parallel& Parallel
Series Combination
21
21
QQQVVV
22
22
11
11
CQ
CQV
CQ
CQV
1 2eq
Q Q QVC C C
21
111CCCeq
n
j jeq CC 1
11For series capacitors
Parallel Combination
VCVCQVCVCQ
2222
1111
21
21
VVVQQQ
1 1 2 2
1 2 eqQ C V C V C V
C V C V
21 CCCeq
For parallel capacitors
n
jjeq CC
1
Parallel Connections
All are parallel connections
This is not
Mixed Combination of Capacitors
Find the capacitance
Series and Parallel
Key ideas:1. For capacitors in series, the charges
are all the same.2. For capacitors in parallel, the
potential differences are all the same.
Mixed Combination of Capacitors
Find the capacitance
Inductance
Whenever a coil of wire is connected to a battery through a rheostat and effort is made to increase the current and hence flux through it, it is always opposed by the instantaneous production of counter emf. The energy required to oppose this is supplied by the battery
Similarly if the current is decreased then again is delayed due to production of counter emf
Inductance This property of the coil due to
which it opposes any increase or decrease of current or flux through it is known as inductance or Self inductanceNL=
I
N= turns in a coil = flux produced I= current produced in a coil
where
If NΦ=1 Wb-turn and I= 1 ampere, then L= 1 HenryHence a coil is said to have self-inductance of one Henry if a current of one ampere when flowing through it produces flux linkages of one Wb-turn in it
Coefficient of Inductance
It is defined as the Weber-turns per ampere in the coil
It is quantitatively measured in terms of coefficient of self induction
Symbol (L), Unit H (Henry) The property is analogous to inertia
in a material body
Electrical Energy Sources
Classification of Sources
Voltage Source Current Source
Further sub classified as
Ideal or Non-ideal Dependent or Independent
Voltage Source Current Source
Voltage Source An ideal voltage
source is a source of voltage with zero internal resistance (a perfect battery) Supply the same
voltage regardless of the amount of current drawn from it
Voltage Source An non-ideal or real
or practical voltage source has a small but finite resistance
The terminal voltage delivered is less by an amount equaling the voltage drop caused by the internal resistance
AB sE E ir
If r=0, then the source becomes Ideal Voltage Source
Independent Voltage Source
An ideal voltage source is shown to be connected to an arbitrary network
The defining equation is
( ) ( ) for any ( )t sv t v t i t The voltage source is
completely specified by its voltage for all t
It does not depend on the connected network in any manner
Such ideal voltage source is also called an Independent Voltage source
Arbitrary Network
i(t)
+
-
v(t)
+
-
vs(t)
Current Source An ideal current
source is capable of producing a specified current through it regardless of what is connected to it
The current supplied is independent of the voltage at the source terminals
Current Source
An non-ideal or real or practical current source has a large but finite resistance
ABsEi IR
If r=infinite, then the source becomes Ideal current Source
Independent Current Source
An ideal current source is shown to be connected to an arbitrary network
The defining equation is( ) ( ) for any ( )si t i t v t
The current source is completely specified by its current is(t) for all t
It does not depend on the connected network in any manner
Such ideal current source is also called an Independent current source
Arbitrary Network
i(t)
+
-
v(t)
+
-
is(t)