Divergence and curl example

For F : R3$ \to$R3, the formulas for the divergence and curl are

div F = $\displaystyle {\frac{{\partial F_1}}{{\partial x}}}$ + $\displaystyle {\frac{{\partial F_2}}{{\partial y}}}$ + $\displaystyle {\frac{{\partial F_3}}{{\partial z}}}$    
curl F = $\displaystyle \left(\vphantom{\frac{\partial F_3}{\partial y}-\frac{\partial F_...
... x}, \frac{\partial F_2}{\partial x} - \frac{\partial F_1}{\partial y} }\right.$$\displaystyle {\frac{{\partial F_3}}{{\partial y}}}$ - $\displaystyle {\frac{{\partial F_2}}{{\partial z}}}$,$\displaystyle {\frac{{\partial F_1}}{{\partial z}}}$ - $\displaystyle {\frac{{\partial F_3}}{{\partial x}}}$,$\displaystyle {\frac{{\partial F_2}}{{\partial x}}}$ - $\displaystyle {\frac{{\partial F_1}}{{\partial y}}}$$\displaystyle \left.\vphantom{\frac{\partial F_3}{\partial y}-\frac{\partial F_...
... x}, \frac{\partial F_2}{\partial x} - \frac{\partial F_1}{\partial y} }\right)$.    

(The formula for curl was somewhat motivated in an earlier reading.)

Given these formulas, there isn't a whole lot to computing the divergence and curl. Just "plug and chug," as they say.

Example

Calculate the divergence and curl of F = (- y, xy, z).

Solution: Since

$\displaystyle {\frac{{\partial F_1}}{{\partial x}}}$ = 0,        $\displaystyle {\frac{{\partial F_2}}{{\partial y}}}$ = x,        $\displaystyle {\frac{{\partial F_3}}{{\partial z}}}$ = 1    

we calculate that

div(F) = 0 + x + 1 = x + 1.    

Since

$\displaystyle {\frac{{\partial F_1}}{{\partial y}}}$ = - 1,$\displaystyle {\frac{{\partial F_2}}{{\partial x}}}$ = y,    
$\displaystyle {\frac{{\partial F_1}}{{\partial z}}}$ = $\displaystyle {\frac{{\partial F_2}}{{\partial z}}}$ = $\displaystyle {\frac{{\partial F_3}}{{\partial x}}}$ = $\displaystyle {\frac{{\partial F_3}}{{\partial y}}}$ = 0,    

we calculate that

curl(F) = (0 - 0, 0 - 0, y + 1) = (0, 0, y + 1).    

Good things we can do this with math. If you can figure out the divergence or curl from the picture of the vector field (below), you doing better than I can.

Back to list of readings.



Duane Nykamp
nykamp@math.umn.edu
2007-03-15
04522 hits since
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