2D

Suppose that  F  is a constant vector field (defined at every point) and  dX  is a fixed vector.

[Graphics:../HTMLFiles/Lect3_224.gif]

If we magnify a small increment of the parametric curve (and scale  F[X]  to the same magnitude) we see approximately a constant flow along a straight line segment.

[Graphics:../HTMLFiles/Lect3_225.gif]

A small increment  X[t+δt]-X[t]  is approximately  X'[t]δt  on a scale of  δt  (assuming   | X '[t] | ≠0).  The flow along this segment is thus approximately  F[X[t]]•X'[t]δt  and if we add all the segments along the curve we obtain the flow along the curve,

    Underoverscript[∑, Underscript[t = a, step δt], arg3] F[X[t ...  δt → ∫_a^bF[X[t]] •X '[t] dt ,   as  δt → 0

Rate of Flow Across a Straight Segment

Suppose that  F  is a constant vector field (defined at every point) and  dX  is a fixed vector.

[Graphics:../HTMLFiles/Lect3_229.gif]

In one second the fluid particles that have crossed the  dX  segment form a parallelogram,

[Graphics:../HTMLFiles/Lect3_230.gif]

Flow of  F  across dX to the right = Det[F, dX] = Det[(f dx)] = f dy - g dx                    g dy

Microscopic Rate of Flow Across:

[Graphics:../HTMLFiles/Lect3_232.gif]

    Underoverscript[∑, Underscript[t = a, step δt], arg3] Det[F ... ; δt → ∫_a^bDet[F[X[t]], X '[t]] dt ,   as  δt → 0


Created by Mathematica  (July 2, 2004)