electronics and communication engineering : electromagnetiic theory, the gate academy
DESCRIPTION
THE GATE ACADEMY's GATE Correspondence Materials consist of complete GATE syllabus in the form of booklets with theory, solved examples, model tests, formulae and questions in various levels of difficulty in all the topics of the syllabus. The material is designed in such a way that it has proven to be an ideal material in-terms of an accurate and efficient preparation for GATE. Quick Refresher Guide : is especially developed for the students, for their quick revision of concepts preparing for GATE examination. Also get 1 All India Mock Tests with results including Rank,Percentile,detailed performance analysis and with video solutions GATE QUESTION BANK : is a topic-wise and subject wise collection of previous year GATE questions ( 2001 – 2013). Also get 1 All India Mock Tests with results including Rank,Percentile,detailed performance analysis and with video solutions Bangalore Head Office: THE GATE ACADEMY # 74, Keshava Krupa(Third floor), 30th Cross, 10th Main, Jayanagar 4th block, Bangalore- 560011 E-Mail: [email protected] Ph: 080-61766222TRANSCRIPT
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Syllabus Electromagnetic Theory
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Syllabus for Electromagnetic Theory
Elements of vector calculus: divergence and curl; Gauss and Stoke’s theorems, Maxwell’s
equations: differential and integral forms. Wave equation, Poynting vector. Plane waves:
propagation through various media; reflection and refraction; phase and group velocity; skin
depth. Transmission lines: characteristic impedance; impedance transformation; Smith chart;
impedance matching; S parameters, pulse excitation. Waveguides: modes in rectangular
waveguides; boundary conditions; cut-off frequencies; dispersion relations. Basics of
propagation in dielectric waveguide and optical fibers. Basics of Antennas: Dipole antennas;
radiation pattern; antenna gain.
Analysis of GATE Papers
(Electromagnetic Theory)
Year Percentage of marks Overall Percentage
2013 5.00
9.12%
2012 12.00
2011 9.00
2010 7.00
2009 8.00
2008 8.00
2007 10.67
2006 12.00
2005 8.71
2004 9.34
2003 10.67
Contents Electromagnetic Theory
THE GATE ACADEMY PVT.LTD. H.O.: #74, Keshava Krupa (third Floor), 30th Cross, 10th Main, Jayanagar 4th Block, Bangalore-11 : 080-65700750, [email protected] © Copyright reserved. Web: www.thegateacademy.com Page I
CC OO NN TT EE NN TT SS
Chapter Page No
#1. Electromagnetic Field 1 – 49 Introduction to Vector Calculus 1 – 7
Material and Physical Constants 7 – 8
Electromagnetic (EM Field) 8 – 18
Divergence of Current Density and Relaxation 18 – 22
The Magnetic Vector Potential 22 – 27
Faraday Law 27 – 29
Maxwell’s Equation’s 29 – 36
Assignment 1 37 – 39
Assignment 2 40 – 42
Answer keys 43
Exlanations 43 – 49
#2. EM Wave Propagation 50 – 86 Introduction 50
General wave equations 50 – 51
Plane wave in a Dielectric medium 51 – 53
Poynting Vector 53 – 54
Phase Velocity 55 – 64
Wave Polarization 64 -71
Assignment 1 72 – 74
Assignment 2 74 – 78
Answer keys 79
Exlanations 79 – 86
#3. Transmission Lines 87 – 127 Introduction 87 – 98
Transmission & Reflection of Waves on a Transmission Line 98 – 100
Impedance of a Transmission Line 100 – 106
The Smith Chart 107 – 108
Scattering Parameters 108 – 109
Strip Line 109 – 113
Assignment 1 114 – 116
Assignment 2 116 – 119
Answer keys 120
Exlanations 120 – 127
#4. Guided E.M Waves 128 – 161 Wave Guide 128 – 130
Transverse Magnetic Mode 130 – 133
Transverse Electric Mode 133 – 142
Circuter Wave Guide 142 – 152
Contents Electromagnetic Theory
THE GATE ACADEMY PVT.LTD. H.O.: #74, Keshava Krupa (third Floor), 30th Cross, 10th Main, Jayanagar 4th Block, Bangalore-11 : 080-65700750, [email protected] © Copyright reserved. Web: www.thegateacademy.com Page II
Assignment 1 153 – 155
Assignment 2 155 – 156
Answer keys 157
Exlanations 157 – 161
#5. Antennas 162 – 199 Inroduction 162
Hertzian Dipole 162 – 165
Field Regions 165
Radiation Pattern 165 – 166
Radiaton Intensity 166 – 168
Antenna Radiation Efficiency 168 – 170
Antenna Arrays 170 – 175
Solved Examples 176 – 188
Assignment 1 189 – 191
Assignment 2 191 – 193
Answer keys 194
Exlanations 194 – 199
Module Test 200 – 215 Test Questions 200 – 207
Answer Keys 208
Explanations 208 – 215
Reference Books 216
Chapter 1 Electromagnetic Theory
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CHAPTER 1
Electromagnetic Field
Introduction to vector calculus
Cartesian coordinates (x, y, z), x , y , z Cylindrical coordinates ( , , z), , , z Spherical coordinates (r, , ) , r , , Vector calculus formula
Table 1.1 S. No Cartesian coordinates Cylindrical
coordinates Spherical coordinates
(a) Differential displacement dl = dx + dy + dz
dl = d + d
+dz
dl = dr + rd + r sin d
(b) Differential area ds = dydz = dxdz
= dxdy
ds = d dz
= d dz = d d
ds = r sin d d = r sin dr d = r dr d
(c) Differential volume dv = dxdydz
dv = d d dz dv = r sin d d dr
Operators
1) V – gradient , of a Scalar V
2) .V – divergence , of a vector V
3) V – curl , of a vector V 4) V – laplacian , of a scalar V
DEL Operator
=
(Cartesian)
=
(Cylindrical)
=
(Spherical)
Gradient of a Scalar field V is a vector that represents both the magnitude and the direction of maximum space rate of increase of V.
V =
=
=
Chapter 1 Electromagnetic Theory
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The following are the fundamental properties of the gradient of a scalar field V:
1. The m gnitude of V equ ls the m ximum r te of ch nge in V per unit dist nce. 2. V points in the direction of the maximum rate of change in V. 3. V t ny point is perpendicular to the constant V surface that passes through that point. 4. If A = V, V is s id to be the sc l r potenti l of A. 5. The projection of V in the direction of unit vector |a| is V. |a| and is called the directional
derivative of V along |a|. This is the rate of change of V in direction of |a|.
Example: Find the gradient of the following scalar fields:
(a) V = e sin 2x cosh y (b) U = z cos (c) W = r sin cos
Solution
(a) V =
= e cos x cosh y e sin x sinh y e sin x cosh y
(b) U =
= z cos z sin cos
(c) W =
= sin cos sin cos sin
Divergence of vector
A at a given point P is the outward flux per unit volume as the volume shrinks about P.
Hence,
divA = . A = lim ∮ .
(1)
Where, V is the volume enclosed by the closed surf ce S in which P is loc ted. Physic lly, we
may regard the divergence of the vector field A⃗⃗ at a given point as a measure of how much the field diverges or emanates from that point.
.A =
=
( A )
=
(r A )
(A sin )
From equation (1), ∮ A ds
= ∫ . A dv
Chapter 1 Electromagnetic Theory
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This is called divergence theorem which states that the total outward flux of the vector field A through a closed surface S is same as the volume integral of the divergence of A. Example
Determine the divergence of these vector field:
(a) P = x yz xz (b) Q = sin z z cos
(c) T =
cos r sin cos cos
Solution
(a) P =
P
P
P
=
x(x yz)
y( )
z(xz)
= xyz x
(b) Q =
( Q )
Q
Q
=
( sin )
( z)
z (z cos )
= sin cos
(c) T =
(r T )
(T sin )
(T )
=
r
r(cos )
r sin
(r sin cos )
r sin
(cos )
=
r sin r sin cos cos
= cos cos
Curl of a vector field provides the maximum value of the circulation of the field per unit area and indicates the direction along which this maximum value occurs.
That is,
curl A = A = lim (∮ .
)
------------- (2)
A = |
A A A
|
=
|
A A A
|
Chapter 1 Electromagnetic Theory
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=
|
r r sin
A rA r sin A
|
From equation (2) we may expect that ∮ . = ∫ (
).
This is called stoke’s theorem, which states that the circulation of a vector field A around a (closed) path L is equal to the surface integral of the curl of A over the open surface S bounded by L. Example Determine the curl of each of the vector fields of previous Example. Solution
(a) = (
) (
) (
)
= ( ) ( ) ( )
= ( )
(b) = *
+ *
+
*
( )
+
= (
) ( )
( )
=
( ) ( )
(c) =
*
( )
+
*
( )+
*
( )
+
=
[
( )
( )]
[
( )
( )]
[
( )
( )
]
=
( )
( )
(
)
= (
)
(
)
(a) Laplacian of a scalar field V, is the divergence of the gradient of V and is written as .
=
=
(
)
=
(
)
(
)
If = 0, V is said to be harmonic in the region. A vector field is solenoid if .A = ; it is irrot tion l or conserv tive if A =
. ( ) = ( ) =
Chapter 1 Electromagnetic Theory
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(b) Laplacian of vector A̅
A⃗⃗ = is lw ys vector qu ntity
A⃗⃗ = ( A ) ̂x ( A ) ̂y ( A ) ̂z
A Sc l r qu ntity A Sc l r qu ntity
A Sc l r qu ntity
V =
........Poission’s Eqn
V = ........Laplace Eqn
E = ⃗⃗
E
....... wave Eqn
Example
The potential (scalar) distribution is given as
V = y x if E0 : permittivity of free space what is the change density p at the point (2,0)?
Solution
Poission’s Eqn V =
(
) ( y x ) =
x x x x x y =
At pt( , ) x x x =
=
Example
Find the Laplacian of the following scalar fields,
(a) V = e sin 2x cosh y (b) U = z cos (c) W = r sin cos
Solution
The Laplacian in the Cartesian system can be found by taking the first derivative and later the second derivative.
(a) V =
=
x( e cos x coshy)
y(e sin x sinh y)
z( e sin x cosh y)
= e sin x cosh y e sin x coshy e sin x cosh y = e sin x cosh y
(b) U =
(
)
Chapter 1 Electromagnetic Theory
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=
( z cos )
z cos
= z cos z cos =
(c) W =
(r
)
(sin
)
=
r
r( r sin cos )
r sin
( r sin sin cos )
r sin cos
r sin
= sin cos
r
r cos sin cos
r sin
r sin cos cos
r sin
cos
r
= cos
r ( sin cos cos )
= cos
r( cos )
Stoke’s theorem
Statement:- closed line integral of any vector A⃗⃗ integrated over any closed curve C is always
equal to the surface integral of curl of vector A⃗⃗ integr ted over the surf ce re ‘s’ which is enclosed by the closed curve ‘c’
∮ A⃗⃗ . d ⃗ = ∫ ∫( x A⃗⃗ ) dS⃗
The theorem is valid irrespective of
(i) Shape of closed curve ‘C’ (ii) Type of vector ‘A’ (iii) Type of co-ordinate system. Divergence theorem
∯ A⃗⃗
dS⃗ = ∭ V⃗⃗ . A⃗⃗ dv
S
V
S
C