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Green's Theorem: Circulation and Curl

Green's theorem ties how much a field circulates around a closed loop to how much it swirls inside: $\oint_C \mathbf{F}\cdot d\mathbf{r} = \iint_A (\nabla\times\mathbf{F})\,dA$ in the plane, where the scalar curl $\nabla\times\mathbf{F} = \partial F_y/\partial x - \partial F_x/\partial y$ measures the local rate of rotation. The left side adds up the tangential push of the field all the way around the boundary; the right side adds up the curl, the tiny paddlewheel spin, over the whole interior. Drag the circle through a vector field and the two numbers stay locked together: the circulation around any loop equals the curl enclosed. This is the planar version of Stokes's theorem and the mathematics behind Ampere's law, where the field is the magnetic field and the curl is the current density, so the circulation of $\mathbf{B}$ around a loop counts the current threading it. The point-vortex field makes that exact: its circulation is the same constant whenever the vortex is enclosed and zero when it is not.

Figure 1. Green's theorem in the plane. Top: the vector field (arrows), the curl shaded red for counterclockwise swirl and blue for clockwise, and a draggable, resizable circle whose boundary is coloured by the tangential flow F.t (red counterclockwise, blue clockwise). Bottom: the circulation and the area integral of curl F versus the circle radius, which coincide. Method: closed-form fields with boundary and area sampling. Source: Stewart, Calculus, 8th ed., Sec. 16.4.
radius R1.00

WHAT TO TRY

  • Drag the circle around the field: the circulation around it and the area integral of the curl stay equal wherever you put the loop and whatever its size.
  • On the rotation field the boundary is all red (the flow runs counterclockwise everywhere) and the circulation equals two times the area; on the irrotational source the boundary is half red and half blue and the circulation is zero (no curl inside).
  • Switch to the point vortex and move the circle so it does or does not enclose the vortex: the circulation jumps between a fixed value and zero, exactly as in Ampere's law.
  • On the varying-curl field, move the circle into the red (counterclockwise) and the blue (clockwise) regions and watch the circulation change sign.