GDC-15

4
37 The divergence of a vector field is defined as z F y F x F F F F z y x 3 2 1 3 2 1 ) ( div k j i k j i F F k j i F ) , , ( ) , , ( ) , , ( ) , , ( 3 2 1 z y x F z y x F z y x F z y x

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GDC

Transcript of GDC-15

  • 37

    The divergence of a vector field

    is defined as

    z

    F

    y

    F

    x

    F

    FFFzyx

    321

    321 )(

    div

    kjikji

    FF

    kjiF ),,(),,(),,(),,( 321 zyxFzyxFzyxFzyx

  • 38

    Divergence

    y ux zu

    vv vdiv = v

    x y z

    v v

    2 Physical meaning

    (x,y,z)v is a differentiable vector field

    div v is associated to local conservation laws: for example, we will show how that if the mass of fluid (or of charge) outcoming from a domain is equal to the mass entering, then

    is the fluid velocity (or the current) vectorfield

    div 0vv

    (x,y,z)V (x dx,y,z)V

    x x+dx

  • Geometrical Interpretation.

    The name divergence is well chosen, for . F is a

    measure of how much the vector F spreads out

    (diverges) from the point in question.

    The vector function has a large (positive) divergence

    at the point P; it is spreading out. (If the arrows

    pointed in, it would be a large negative divergence.)

    P

    39

    NOTE: P=electric field due to charge (+ ve or ve)

  • On the other hand, the function has zero divergence at

    P; it is not spreading out at all.

    40

    P

    So, for example, if the divergence is positive at a point, it

    means that, overall, that the tendency is for fluid to move away

    from that point (expansion); if the divergence is negative, then

    the fluid is tending to move towards that point (compression).