AL-5

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PH0101 UNIT 2 LECTURE 2 15 Important Vector notations in electromagnetism div grad S = S 2 ) S ( V ) V ( S ) V S ( curl grad = 0 0 ) ( 1. 2. 3. 4. E ) E ( ) E ( 2

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  • PH0101 UNIT 2 LECTURE 2 15

    Important Vector notations in electromagnetism

    div grad S = S2

    )S(V)V(S)VS(

    curl grad = 0 0)(

    1.

    2.

    3.

    4.

    E)E()E( 2

  • PH0101 UNIT 2 LECTURE 2 16

    Theorems in vector fields

    Gauss Divergence Theorem

    It relates the volume integral of the divergence of a vector V to the surface integral of the vector itself.

    According to this theorem, if a closed S bounds a volume , then

    div V) d = V ds

    Sd dsVV )(

    (or)

  • PH0101 UNIT 2 LECTURE 2 17

    Stokes Theorem

    It relates the surface integral of the curl of a

    vector to the line integral of the vector itself.

    According to this theorem, for a closed path C bounds a surface S,

    s (curl V) ds = V dlC

  • PH0101 UNIT 2 LECTURE 2 18

    Maxwells Equations

    Maxwells equations combine the fundamental laws of electricity and magnetism .

    The are profound importance in the analysis of most electromagnetic wave problems.

    These equations are the mathematical abstractions of certain experimentally observed facts and find their application to all sorts of problem in electromagnetism.

    Maxwells equations are derived from Amperes law, Faradays law and Gauss law.

  • PH0101 UNIT 2 LECTURE 2 19

    Maxwells Equations SummaryMaxwells

    Equations

    Differential form Integral form

    1. Equation from

    electrostatics

    2. Equation from

    magnetostatics

    3. Equation from

    Faradays law

    4. Equation from

    Ampere

    circuital law

    D. vs

    dvds.D

    0. B 0s

    ds.B

    t

    BE

    s

    ds.t

    Bdl.E

    t

    DEH

    sl

    ds).t

    DE(dl.H

  • PH0101 UNIT 2 LECTURE 2 20

    Maxwells equation: Derivation

    Maxwells First Equation

    If the charge is distributed over a volume V. Let be the volume density of the charge, then the charge q is given by,

    q = v

    dv