UNIT1 Vector Unit1 Review of Vector Analysis Cartesian

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UNIT-1 Vector

UNIT-1 Vector

Unit-1: Review of Vector Analysis �Cartesian, �Cylindrical and �Spherical Co-ordinate Systems, �Vector products, �Projection

Unit-1: Review of Vector Analysis �Cartesian, �Cylindrical and �Spherical Co-ordinate Systems, �Vector products, �Projection of Vectors, �Gradient, �Divergence �Curl, �Line, surface, volume integrals, �Divergence Theorem �Stokes theorem

Unit-2 Electrostatics: �Coulomb’s Law, �Electric field intensity, �Evaluation of Electric field intensity due to

Unit-2 Electrostatics: �Coulomb’s Law, �Electric field intensity, �Evaluation of Electric field intensity due to line charge, Surface charge and Volume charge distribution, �Electric flux density, �Gauss Law, �Electrostatic potential, �Potential gradient, �Electric dipole and Polarization

Unit-3 Magnetostatics : �Biot–Savart Law, �Ampere’s Circuital Law, � Magnetic field intensity, �Magnetic field

Unit-3 Magnetostatics : �Biot–Savart Law, �Ampere’s Circuital Law, � Magnetic field intensity, �Magnetic field intensity evaluation due to infinite, finite and circular current carrying conductors, �Magnetic flux �Flux density, �Magnetic dipole and Magnetization

Unit-4 Boundary Conditions & Maxwell’s Equations : �Boundary condition at Dielectric – Conductor interface,

Unit-4 Boundary Conditions & Maxwell’s Equations : �Boundary condition at Dielectric – Conductor interface, Dielectric – Dielectric interface, �Boundary conditions for magnetic materials interface, �Current continuity equation, � Maxwell’s equations.

Unit-5 Electromagnetic wave propagation : �Electromagnetic wave equation for free space, lossy dielectric material

Unit-5 Electromagnetic wave propagation : �Electromagnetic wave equation for free space, lossy dielectric material and perfect conductor, �Propagation constant, � Attenuation constant & Phase shift constant, �Skin depth, �Poynting Theorem, �Reflection of a plain wave in a normal incidence at Dielectric – Dielectric interface, Dielectric – Conductor interfaces

Unit-6 Radiation: : �Scalar and Vector magnetic potential, Retarded potential, Electric & Magnetic fields,

Unit-6 Radiation: : �Scalar and Vector magnetic potential, Retarded potential, Electric & Magnetic fields, �Power radiated and Radiation resistance due to oscillating dipole, Quarter wave monopole & Half wave dipole.

Unit-5 Electromagnetic wave propagation: Electromagnetic wave equation for free space, lossy dielectric material and

Unit-5 Electromagnetic wave propagation: Electromagnetic wave equation for free space, lossy dielectric material and perfect conductor, Propagation constant, Attenuation constant & Phase shift constant, Skin depth, Poynting Theorem, Reflection of a plain wave in a normal incidence at Dielectric – Dielectric interface, Dielectric – Conductor interfaces. 10 Unit-6 Radiation: Scalar and Vector magnetic potential, Retarded potential, Electric & Magnetic fields, Power radiated and Radiation resistance due to oscillating dipole, Quarter wave monopole & Half wave dipole.

Cartesian coordinate system 2 What is a vector? 1 Unit-1 Vector 6 Divergence, curl,

Cartesian coordinate system 2 What is a vector? 1 Unit-1 Vector 6 Divergence, curl, gradient, divergence theorem, stokes theorem Cylindrical coordinate system 3 4 5 Scalar product &vetor product Spherical Coordinate system

Vector analysis is a mathematical tool with which electromagnetic concepts are more conveniently expressed

Vector analysis is a mathematical tool with which electromagnetic concepts are more conveniently expressed and best comprehended. Since use of vector analysis in the study of electromagnetic field theory results in real economy of time and thought.

Cartesian Coordinate system Rectangle(cartisian )

Cartesian Coordinate system Rectangle(cartisian )

Cartesian co-ordinates system i)Point ii) Differential length ii) Differential surfaces iii)Differential volume

Cartesian co-ordinates system i)Point ii) Differential length ii) Differential surfaces iii)Differential volume

Point representation

Point representation

p(x 0, y 0, Z 0)

p(x 0, y 0, Z 0)

Differential Length dz dx dy

Differential Length dz dx dy

Differential Surface

Differential Surface

Y

Y

Z az ay -ay ax X -ax -az Y

Z az ay -ay ax X -ax -az Y

z Ds 2=-dxdz ay dz dx Ds 2=+dxdz ay y dy Ds 1=dydz ax

z Ds 2=-dxdz ay dz dx Ds 2=+dxdz ay y dy Ds 1=dydz ax x Ds 1=+dydzax Ds 2=+dxdzay Ds 3=+dxdyaz

Differential Volume

Differential Volume

Differential volume z dz dx dy Dv=dxdydz x y

Differential volume z dz dx dy Dv=dxdydz x y

Position Vector

Position Vector

p(x 0, y 0, Z 0) r. P ap

p(x 0, y 0, Z 0) r. P ap

Displacement Vector Z Displacement vector A(x 1, y 1, z 1 ) B(x 2,

Displacement Vector Z Displacement vector A(x 1, y 1, z 1 ) B(x 2, y 2, z 2) r. A r. B Y X

Rectangular coordinate system Cylindrical coordinate system

Rectangular coordinate system Cylindrical coordinate system

Cylindrical Coordinate system Cylinder

Cylindrical Coordinate system Cylinder

CYLINDRICAL COORDINATE SYSTEM �Point �Differential length �Differential surfaces �Differential volume

CYLINDRICAL COORDINATE SYSTEM �Point �Differential length �Differential surfaces �Differential volume

Point representation

Point representation

�Why did we take as a differential length in rectangular coordinate system?

�Why did we take as a differential length in rectangular coordinate system?

p(x 0, y 0, Z 0)

p(x 0, y 0, Z 0)

Cylindrical Coordinate system z ρ=radius of cylinder Z =height of cylinder Φ=angle made by

Cylindrical Coordinate system z ρ=radius of cylinder Z =height of cylinder Φ=angle made by ρ with positive x-axis A(ρ, φ, z) Z ρ ρ φ x y

z ρ=radius of cylinder Z =height of cylinder Φ=angle made by ρ with positive

z ρ=radius of cylinder Z =height of cylinder Φ=angle made by ρ with positive x-axis Point A(ρ, φ, z) Z ρ ρ φ x y

Differential Length in cylindrical coordinate system �dl = dρaρ + ρd. Фa. Ф +

Differential Length in cylindrical coordinate system �dl = dρaρ + ρd. Фa. Ф + dz az

�Why did we take rectangular surfaces in rectangular coordinate system?

�Why did we take rectangular surfaces in rectangular coordinate system?

First Plane (varying ƍ) in aƍ direction dl = dρaρ + ρd. Фa. Ф

First Plane (varying ƍ) in aƍ direction dl = dρaρ + ρd. Фa. Ф + dz az dz

z dl = dρaρ + ρd. Фa. Ф + dz az Second plane(varying Ф

z dl = dρaρ + ρd. Фa. Ф + dz az Second plane(varying Ф ) in a. Ф direction dz y φ1 dƍ x

dl = dρaρ + ρd. Фa. Ф + dz az Third Plane (varying Z)

dl = dρaρ + ρd. Фa. Ф + dz az Third Plane (varying Z) in az direction z

Unit vectors in rectangular and cylindrical co ordinate system a z p(x, y, z)

Unit vectors in rectangular and cylindrical co ordinate system a z p(x, y, z) a y ax aØ aƍ

Conversion between Cartesian and Cylindrical coordinate system

Conversion between Cartesian and Cylindrical coordinate system

Differential Length in cylindrical coordinate system �dl = dρaρ + ρd. Фa. Ф +

Differential Length in cylindrical coordinate system �dl = dρaρ + ρd. Фa. Ф + dz az

Differential surfaces in cylindrical coordinate system �dl = dρaρ + ρd. Фa. Ф +

Differential surfaces in cylindrical coordinate system �dl = dρaρ + ρd. Фa. Ф + dz az

Differential volume dv = dρρd. Фdz dv = ρdρd. Фdz

Differential volume dv = dρρd. Фdz dv = ρdρd. Фdz

Spherical Coordinate system Sphere

Spherical Coordinate system Sphere

Spherical Co-ordinates system i)Differential length ii)Differential surfaces iii)Differential volume

Spherical Co-ordinates system i)Differential length ii)Differential surfaces iii)Differential volume

Point representation in spherical coordinate system

Point representation in spherical coordinate system

r = radius of sphere Ɵ = angle made by r to the positive

r = radius of sphere Ɵ = angle made by r to the positive z-axis Ø = angle made by rsinƟ with positive x-axix r

Z

Z

Differential length

Differential length

Unit vectors in Spherical coordinate system

Unit vectors in Spherical coordinate system

Z

Z

Conversion between spherical and Cartesian coordinates

Conversion between spherical and Cartesian coordinates

Transformation of vector from Cylindrical to Cartesian

Transformation of vector from Cylindrical to Cartesian

Transformation of vector from Cartesian to cylindrical or vice versa

Transformation of vector from Cartesian to cylindrical or vice versa

Transformation of vector from Spherical to Cartesian coordinate system

Transformation of vector from Spherical to Cartesian coordinate system

Transformation of vector from Cartesian to Spherical coordinate system

Transformation of vector from Cartesian to Spherical coordinate system

Scalar Product(Dot Product) B Ɵ A

Scalar Product(Dot Product) B Ɵ A

Vector product(Cross product)

Vector product(Cross product)

Divergence of vector in different coordinate system Cartesian Coordinate system Cylindrical Co-ordinates system Spherical

Divergence of vector in different coordinate system Cartesian Coordinate system Cylindrical Co-ordinates system Spherical Co-ordinates system

Divergence Theorem The volume integral of the divergence of vector field D taken over

Divergence Theorem The volume integral of the divergence of vector field D taken over any volume V is equal to the surface integral of D taken over the closed surface enclosing the volume V

Curl

Curl

Gradient �V –Scalar field

Gradient �V –Scalar field

Stoke’s theorem �It stats that integration of tangential component of vector field along the

Stoke’s theorem �It stats that integration of tangential component of vector field along the closed path is equal to integral of normal component of curl of the vector field over the surface enclosed by the closed path.

Line

Line

Z Line X=2, Z=4 Means || to Y axis 2 4 Y X

Z Line X=2, Z=4 Means || to Y axis 2 4 Y X

Line Y=4, Z=2 Mean || to X axis Z 4 2 Y X

Line Y=4, Z=2 Mean || to X axis Z 4 2 Y X

Z Line X=1, Y=2 Mean || to Z axis 1 2 Y X

Z Line X=1, Y=2 Mean || to Z axis 1 2 Y X

Line is at x=3 , y=5 Means parellel to z axis (3, 5) XY

Line is at x=3 , y=5 Means parellel to z axis (3, 5) XY plane

Plane

Plane

z Y=4 plane or xz plane ay Y=4 x y

z Y=4 plane or xz plane ay Y=4 x y

az Z=4 plane or YZplane z Z=4 y x

az Z=4 plane or YZplane z Z=4 y x

X=4 plane or yz plane z y x=4 a x x

X=4 plane or yz plane z y x=4 a x x

z Y=4 plane or xz plane Y=4 x y

z Y=4 plane or xz plane Y=4 x y