23
BASICS OF CIRCUIT THEORY Compiled By Shruti Bhatnagar Dasgupta

Circuit theory basics

Embed Size (px)

DESCRIPTION

Circuit Theory Basics, Resistors, Capacitors, Inductors, Current Sources and Voltage Sources. Also visit for http://shrutizpresentations.blogspot.com/ more ppts.

Citation preview

Page 1: Circuit theory basics

BASICS OF CIRCUIT THEORY

Compiled By

Shruti Bhatnagar Dasgupta

Page 2: Circuit theory basics

CIRCUIT ELEMENTSIn circuits, we think about basic circuit elements

that are the “building blocks” of our circuits. This is

similar to what we do in Chemistry with chemical

elements like oxygen or nitrogen.

A circuit element cannot be broken down or

subdivided into other circuit elements.

A circuit element can be defined in terms of the

behavior of the voltage and current at its terminals.

Page 3: Circuit theory basics

THE 5 BASIC CIRCUIT ELEMENTS

There are 5 basic circuit elements:

1. Voltage sources

2. Current sources

3. Resistors

4. Inductors

5. Capacitors

Page 4: Circuit theory basics

VOLTAGE SOURCES

A voltage source is a two-terminal circuit element that maintains a voltage across its terminals.The value of the voltage is the defining characteristic of a voltage source. Any value of the current can go through the voltage source, in any direction. The current can also be zero. The voltage source is not concerned about the current. It focuses only about voltage.

Page 5: Circuit theory basics

VOLTAGE SOURCES – 2 KINDS

There are 2 kinds of voltage sources:

1. Independent voltage sources

2. Dependent voltage sources, of which there are 2

forms:i. Voltage-dependent voltage sourcesii. Current-dependent voltage sources

Page 6: Circuit theory basics

VOLTAGE SOURCES – SCHEMATIC SYMBOL FOR INDEPENDENT SOURCES

The schematic symbol

that we use for

independent voltage

sources is shown here.

Independentvoltagesource

+

-

vS=#[V]

This is intended to indicate that the schematic symbol can be labeled either with a variable, like vS, or a value, with some number, and units. An example might be 1.5[V]. It could also be labeled with both.

Page 7: Circuit theory basics

VOLTAGE SOURCES – SCHEMATIC

SYMBOLS FOR DEPENDENT VOLTAGESOURCES

The schematic symbols that we use for dependent

voltage sources are shown here, of which

there are 2 forms:i. Voltage-dependent voltage sourcesii. Current-dependent voltage sources

Voltage-dependentvoltagesource

+vS=m vX

-

Current-dependentvoltagesource

+vS=r iX

-

Page 8: Circuit theory basics

Voltage-dependentvoltagesource

+vS=m vX

-

SCHEMATIC SYMBOLS FOR DEPENDENT VOLTAGE

SOURCESThe schematic symbols that we use for dependent

voltage sources are shown here, of which there are 2 forms:

i. Voltage-dependent voltage sourcesii. Current-dependent voltage sourcesThe symbol m is the coefficient of the

voltage vX. It is dimensionless. For example, it might be 4.3 vX. The vX is a voltage somewhere in the circuit.

Current-dependentvoltagesource

+vS=r iX

-

The symbol r is the coefficient of the current iX. It has dimensions of [voltage/current]. For example, it might be 4.3[V/A] iX. The iX is a current somewhere in the circuit.

Page 9: Circuit theory basics

CURRENT SOURCES

A current source is a two-terminal circuit element that

maintains a current through its terminals.

The value of the current is the defining characteristic of

the current source.

Any voltage can be across the current source, in either

polarity. It can also be zero. The current source does not

“care about” voltage. It “cares” only about current.

Page 10: Circuit theory basics

CURRENT SOURCES - IDEAL

A current source maintains a current through its

terminals no matter what you connect to those terminals.

While there will be devices that reasonably model

current sources, these devices are not as familiar as

batteries.

Page 11: Circuit theory basics

CURRENT SOURCES – 2 KINDS

There are 2 kinds of current sources:

1. Independent current sources

2. Dependent current sources, of which there

are 2 forms:i. Voltage-dependent current sourcesii. Current-dependent current sources

Page 12: Circuit theory basics

Independentcurrentsource

iS=#[A]

CURRENT SOURCES – SCHEMATIC SYMBOL FOR INDEPENDENT SOURCES

The schematic symbols that we use for current sources are shown here.

This is intended to indicate that the schematic symbol can be labeled either with a variable, like iS, or a value, with some number, and units. An example might be 0.2[A]. It could also be labeled with both.

Page 13: Circuit theory basics

SCHEMATIC SYMBOLS FOR DEPENDENT CURRENT SOURCES

The schematic symbols that we use for dependent current

sources are shown here, of which there are 2 forms:i. Voltage-dependent current sourcesii. Current-dependent current sources

Voltage-dependentcurrentsource

iS=g vX

Current-dependentcurrentsource

iS=b iX

Page 14: Circuit theory basics

Current-dependentcurrentsource

iS=b iX

Voltage-dependentcurrentsource

iS=g vX

SCHEMATIC SYMBOLS FOR DEPENDENT CURRENT SOURCES

The schematic symbols that we use for dependent current sources are shown here, of which there are 2 forms:

i. Voltage-dependent current sourcesii. Current-dependent current sourcesThe symbol g is the coefficient of the

voltage vX. It has dimensions of [current/voltage]. For example, it might be 16[A/V] vX. The vX is a voltage somewhere in the circuit.

The symbol b is the coefficient of the current iX. It is dimensionless. For example, it might be 53.7 iX. The iX is a current somewhere in the circuit.

Page 15: Circuit theory basics

Voltage and Current Sources• Real Voltage Source and Real Current

Source• In “real” sources there is always some energy loss.

+Vs

-

i

V

R+I s

-

i

V

R

Page 16: Circuit theory basics

LINEAR COMPONENTS

Resistor, Capacitor, Inductor, and Transformer

VR

+ V= I.RI

vC

+

i

i = C. dv dt

v

+i

L

v = L. di dt

-

-

-

Page 17: Circuit theory basics

)f(xβ)f(xα)xβxf(α 2121

LINEARITY’S PRINCIPLE

)()()(:ionSuperposit

)()(:Scaling

2121 xfxfxxf

xfkxkf

Linearity = Scaling + Superposition

Page 18: Circuit theory basics

RESISTORSA resistor is a two terminal circuit element that has a constant ratio of the voltage across its terminals to the current through its terminals.The value of the ratio of voltage to current is the defining characteristic of the resistor.

where R is the resistance.

+

R

viR -

Page 19: Circuit theory basics

OHM’S LAW

The voltage across a conductor is proportional to

the current flowing through it:-

The Proportionality constant is called Resistance

(R).

V= I.R

Page 20: Circuit theory basics

CAPACITORA capacitor or a condenser is a passive two-terminal electrical

component used to store energy electrostatically in an electric field.

The forms of practical capacitors contain at least two electrical

conductors (plates) separated by a dielectric (insulator). The conductors

can be thin films of metal, aluminum foil or disks, etc. The 'non-

conducting' dielectric acts to increase the capacitor's charge capacity. A

dielectric can be glass, ceramic, plastic film, air, paper, mica, etc.

Unlike a resistor, a capacitor does not dissipate energy. Instead, a

capacitor stores energy in the form of an electrostatic field between its

plates.

Page 21: Circuit theory basics

Its symbols are:

+

A capacitor A Polarised A Variable

Capacitor Capacitor

An ideal capacitor is wholly characterized by a constant capacitance C,

defined as the ratio of charge ±Q on each conductor to the voltage V

between them:

C= Q/V

Page 22: Circuit theory basics

INDUCTORSAn inductor or coil or reactor, is a passive two-terminal electrical

component which resists changes in electric current passing

through it.

It consists of a conductor such as a wire, usually wound into a coil.

When a current flows through it, energy is stored temporarily in a

magnetic field in the coil. When the current flowing through an

inductor changes, the time-varying magnetic field induces a voltage

in the conductor, according to Faraday’s law of electromagnetic

induction, which opposes the change in current that created it.

Page 23: Circuit theory basics

Its symbol is:

inductance is determined by how much magnetic

flux Φ through the circuit is created by a given

current (i)

L = Φ/i