91Ó°ÊÓ

The integral derivativeof a function $\mathit{f}\mathbf{(}\mathbf{x}\mathbf{,}\mathbf{y}\mathbf{,}\mathbf{z}\mathbf{)}$over an open surface area is equal to the volume integral of the function, $\mathbf{∫}\mathbf{(}\mathbf{∇}\mathbf{·}\mathbf{v}\mathbf{)}\mathbf{·}\mathbf{ }\mathit{d}\mathit{l}\mathbf{=}\underset{\mathbf{s}}{\mathbf{âˆ\circledR }}\mathit{v}\mathbf{·}\mathbf{ }\mathit{d}\mathit{s}$.The right side of the gauss divergence theorem is the surface integral, that is, $\underset{s}{âˆ\circledR }v·da$

The diagram of the triangular path is shown below:

Let the vector be defined as $\mathbf{v}=xy i+2yz j+3zx k$and the $∇$operator be defined as $∇=\frac{∂}{∂x}i+\frac{∂}{∂y}j+\frac{∂}{∂z}k$. The divergence of vector v is computed as follows:

$\begin{array}{rcl}∇·v& =& \left(\frac{∂}{∂x}i+\frac{∂}{∂y}j+\frac{∂}{∂z}k\right)·\left(xy i+2yz j+3zx k\right)\\ & =& y+2z+3x\\ & & \end{array}$

Now, compute the left part of gauss divergence theorem as:

$\begin{array}{rcl}∫\left(∇·v\right)dv& =& \underset{0}{\overset{2}{∫}}\underset{0}{\overset{2}{∫}}\underset{0}{\overset{2}{∫}}\left(3x+2z+y\right)dxdydz\\ & =& \underset{0}{\overset{2}{∫}}\underset{0}{\overset{2}{∫}}\left(\frac{3}{2}×4+2z×2+y×2\right)dydz\\ & =& \underset{0}{\overset{2}{∫}}\underset{0}{\overset{2}{∫}}\left(6+4z+2y\right)dydz\\ & =& \underset{0}{\overset{2}{∫}}\left(12+8z+4\right)dz\\ & & \end{array}$

Solve further as:

$\begin{array}{rcl}∫\left(∇·v\right)dv& =& {\left(12z+4z^2+4z\right)}_0^2\\ & =& \left(24+4×4+4z\right)-\left(0\right)\\ & =& 48\\ & & \end{array}$

Step 2: Compute the left side of strokes theorem

The area vector is given by $\stackrel{→}{da}= dydz i$as the open surface area lies in y-z plane. The left part of the strokes theorem is calculated as:

$\begin{array}{rcl}\underset{S}{\overset{}{∫}}\left(∇×\mathbf{v}\right)·\stackrel{→}{da}& =& \underset{S}{∫}\left(-2yi -3zj -xk\right)·\left(dy dz i\right)\\ & =& \underset{S}{∫}-2y dydz\\ & & \end{array}$

The equation of line (i) is $y+z=2$. Along this line,z varies 0 to 2 and y varies from 0 to $ 2-z$. Thus the integral $\underset{S}{\overset{}{∫}}\left(∇×\mathbf{v}\right)·\stackrel{→}{da}=\underset{S}{∫}-2y dydz$ can be written as:

$\begin{array}{rcl}\underset{S}{\overset{}{∫}}\left(∇×\mathbf{v}\right)·\stackrel{→}{da}& =& \underset{0}{\overset{2}{∫}}dz\underset{0}{\overset{2-z}{∫}}-2y dy\\ & =& \underset{0}{\overset{2}{∫}}dz{\left(\frac{-2y^2}{2}\right)}_0^{2-z}\\ & =& \underset{0}{\overset{2}{∫}}dz{\left(-y^2\right)}_0^{2-z}\\ & =& \underset{0}{\overset{2}{∫}}dz\left(-{\left(2-z\right)}^2-\left(0\right)\right)\\ & & \end{array}$

Solve further as,

$\begin{array}{rcl}\underset{S}{\overset{}{∫}}\left(∇×\mathbf{v}\right)·\stackrel{→}{da}& =& \underset{0}{\overset{2}{∫}}-\left(4+z^2-4z\right)dz\\ & =& -{\left(4z+\frac{z^3}{3}-2z^2\right)}_0^2\\ & =& -\left(\left(8+\frac{8}{3}-8\right)-\left(0\right)\right)\\ & =& -\frac{8}{3}\\ & & \end{array}$

The surface integral of vector $\stackrel{→}{v}$, in the xy plane is computed as:

$\begin{array}{rcl}\underset{}{\overset{}{∫}}v· da& =& \underset{}{\overset{}{∫}}\underset{}{\overset{}{∫}}\left(2xzi+\left(x+2\right)j+y\left(z^3-3\right)k\right)\left(dx dy k\right)\\ & =& \underset{0}{\overset{2}{∫}}\underset{0}{\overset{2}{∫}}y\left(z^2-3\right) dx dy\\ & =& \underset{0}{\overset{2}{∫}}\underset{0}{\overset{2}{∫}}y\left(0-3\right) dx dy\\ & =& \underset{0}{\overset{2}{∫}}\underset{0}{\overset{2}{∫}}-3y dx dy\\ & & \end{array}$

The differential length vector is given by $\stackrel{→}{dl}= dx i+dy j+dz k$. The right part of the strokes theorem is calculated as:

$\begin{array}{rcl}\underset{}{\overset{}{∫}}v· dl& =& \underset{}{\overset{}{∫}}\left(2xzi+\left(x+2\right)j+y\left(z^3-3\right)k\right)\left(dx i+dy j+dz k\right)\\ & =& \underset{}{\overset{}{∫}}\left(xy\right) dx+\left(2yz\right) dy +\left(3zx\right) dz\\ & & \end{array}$

Along the path (i),$z=x=0 $, thus $dx= dz=0$and $y=0$. Hence the above integral becomes, $\underset{}{\overset{}{∫}}v· dl=\underset{}{\overset{}{∫}}\left(2yz\right) dy $.

Along the path (ii), $x=0 $, $z=2-y$ thus $dx=0$and $dz=-dy$. Hence the above integral becomes,

$\begin{array}{rcl}\underset{}{\overset{}{∫}}v· dl& =& \underset{2}{\overset{0}{∫}}2y\left(2-y\right) dy \\ & =& -\underset{0}{\overset{2}{∫}}4y-2y^2 dy \\ & =& {\left(-2y^2-\frac{2}{3}{y}^3\right)}_0^2\\ & =& -\left(8-\frac{16}{3}\right)\\ & =& -\frac{8}{3}\\ & & \end{array}$

Along the path (ii)i, $x=y=0 $, thus $dx=dy=0$ and z varies deom 2 to 0.. Hence the integral $\underset{}{\overset{}{∫}}v· dl$becomes 0 along path (iii).

The integral of all the three parts are added to give:

$\begin{array}{rcl}\underset{}{\overset{}{∫}}v· dl& =& 0-\frac{8}{3}+0\\ & =& \frac{8}{3}\\ & & \end{array}$

Thus the left and right side gives same result. Hence strokes theorem is verified.