Lecture 1-Coulomb_s Law

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  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Engineering Electromagnetics

    LECTURE 1: Coulombs Law

    Instructor: Sir Tim

    Summer Term

  • Coulombs Law

    ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    POINT CHARGES

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    ATOMIC MODEL

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    VALENCE

    The NUMBER OF ELECTRONS in THEOUTERMOST SHELL determines thevalence of the atom

    The outermost shell is called theVALENCE SHELL

    The electrons residing in the outermostshell is called VALENCE ELECTRONS

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Electrostatics

    Deals with the phenomena due to theATTRACTIONS OR REPULSIONS OFELECTRIC CHARGES that are NOTMOVING.

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Static Electricity

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Coulombs Law

    Coulombs First Law of Electrostatics The size of the force of attraction or repulsion

    between two charges is DIRECTLYproportional to the value of the charge

    Coulombs Second Law of Electrostatics The size of the force varies INVERSELY asthe square of the distance between the twocharges

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Mathematical Form

    k = 1/(4pi),(for air o = shift constant 32)

    F force in newtons

    Q1 and Q2 charge in coulombs

    r distance bet. two charges in meters

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    NATURE OF CHARGES

    LIKE charges REPEL

    UNLIKE charges ATTRACT

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    ELECTRIC FIELD

    Defined as the force per unit positivecharge that would be experienced by astationary point charge in a given locationin a field

    The space between and around thecharged bodies where their influence is felt

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    ELECTRIC FIELD

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    ELECTRIC FIELD

    k = 1/(4pi),(for air o = shift constant 32)

    E electric field intensity in V/m orN/C

    Q charge in coulombs r distance in meters

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Problem 1

    Point charges 1 mC and -2 mC are locatedat (3, 2, -1) and (-1, -1, 4) respectively.Calculate the electric force on a 10-nCcharge located at (0, 3, 1) and the electricfield intensity at that point.

    Ans: F = -6.507ax 3.817ay + 7.506az mN

    E = -650.7ax 381.7ay 750.6az kV/m

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Problem 2

    Two point charges of equal mass m, chargeQ are suspended at a common point by twothreads of negligible mass and length l.Show that at equilibrium, the inclinationangle of each thread to the vertical isgiven by

    2 = 162 sin2 tan

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Problem 3

    A practical application of electrostaticsseparation of solids. Assuming zero initialvelocity and displacement, determine theseparation between the particles after falling80 cm. Take E = 500 kV/m and Q/m = 9C/kg for both positively and negativelycharged particles.

    Ans: 73.4 cm

  • Coulombs Law

    ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    CHARGE DISTRIBUTION

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    VOLUME CHARGE DISTRIBUTION

    =

    where:

    V is the volume charge density; and

    Q is the total charge within some finite volume

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    FIELD OF A LINE CHARGE

    =2

    where:

    L is the line chargedensity

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    FIELD OF A SHEET OF CHARGE

    =2

    where:

    S is the surface chargedensity

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Problem 1

    Find the force on a point charge 50 C at (0,0, 5) m due to a circular disk with surfacecharge density of s = 20 C/m

    2 and 5m, z = 0 m.

    Ans: F = 16.5az N

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Problem 2

    The finite sheet 0 1, 0 1 on the z= 0 plane has a charge density =

    (2 + 2 + 25)3

    2 nC/m2. Find:(a) the total charge on the sheet(b) the electric field at (0, 0, 5)(c) the force experienced by a -1 mC charge

    located at (0, 0, 5)

    Ans: (a) Q = 33.15 nC(b) E = -1.5ax, -1.5ay, 11.25az V/m(c) F = 1.5ax, 1.5ay, -11.25az mN

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Problem 3

    Determine E at (2, 0, 2) m due to threestandard charge distributions as follows: auniform sheet at x = 0 m with s1 = (1/3)nC/m2, a uniform sheet at x = 4 m with s2= (-1/3) nC/m2, and a uniform line at x =6 m, y = 0 m with l = -2 nC/m.

    Ans: E = 21ax V/m

  • ECE Department, TUP Manila Engineering Electromagnetics Timothy M. Amado, ECE Summer

    Thank you.

    Lecture 1: Coulomb's Law

    Engineering Electromagnetics

    Timothy M. AmadoFaculty, Electronics Engineering Department

    Technological University of the Philippines Manila

    [email protected]