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Vectors 445<br />
= (0 – 0) iˆ – (2 z – 0) ˆj (3 y – 1) kˆ – 2 zj ˆ (3 y – 1) kˆ<br />
<br />
ˆ ˆ ˆ 2 2 2<br />
<br />
i j k ( x y z 16)<br />
ˆn = | = x y z<br />
|<br />
| |<br />
2xiˆ<br />
2yj ˆ 2zkˆ<br />
xiˆ<br />
yj ˆ zkˆ<br />
xiˆ<br />
yj ˆ zkˆ<br />
=<br />
=<br />
=<br />
2 2 2 2 2 2<br />
4x 4y 4z<br />
x y z 4<br />
<br />
ˆ ˆ ˆ<br />
( F)<br />
nˆ<br />
= [– 2 ˆ (3 – 1) ˆ xi yj zk<br />
zj y k]<br />
<br />
2 yz (3y 1) z<br />
=<br />
4<br />
4<br />
ˆk n<br />
xiˆ<br />
yj ˆ zkˆ<br />
z<br />
ds = dx dy <br />
. k ds = dx dy ds = dx dy<br />
4<br />
4<br />
<br />
ds = 4 dx dy<br />
z<br />
2 (3 1) 4<br />
( F)<br />
nˆ<br />
ds yz y z dx dy<br />
<br />
<br />
4 z <br />
= [ 2 y (3 y 1)] dx dy = ( y 1) dxdy<br />
On putting x = r cos , y = r sin , dx dy = r d dr, we get<br />
=<br />
=<br />
= ( r sin 1) r d dr<br />
2<br />
3 2<br />
4<br />
<br />
<br />
2<br />
d ( r sin r)<br />
dr<br />
= r<br />
r <br />
d <br />
<br />
sin <br />
3 2 = 64 <br />
d <br />
sin 8 <br />
0 <br />
<br />
3<br />
0 0<br />
<br />
2<br />
64 64 64<br />
= cos 8 <br />
= 16<br />
= – 16 <br />
3 3 3<br />
0<br />
The line integral is equal to the surface integral, hence Stoke’s Theorem is verified. Proved.<br />
<br />
2 2<br />
Example 98. Verify Stoke’s theorem for a <strong>vector</strong> field defined by F ( x – y ) iˆ 2xy ˆj<br />
in<br />
the rectangular in xy-plane bounded by lines x = 0, x = a, y = 0, y = b.<br />
(Nagpur University, Summer 2000)<br />
Solution. Here we have to verify Stoke’s theorem F <br />
. dr<br />
<br />
= ( ). ˆ<br />
C F<br />
nds<br />
S<br />
Where ‘C’ be the boundary of rectangle (ABCD) and S be the surface enclosed by curve C.<br />
2<br />
F 2 2<br />
= ( x – y ) iˆ (2 xy)<br />
ˆj<br />
<br />
F . dr =<br />
2 2<br />
[( x – y ) iˆ 2 xyj ˆ].[ idx ˆ ˆj dy]<br />
<br />
F . dr = (x<br />
2<br />
+ y 2 ) dx + 2xy dy ...(1)<br />
Now, F <br />
. dr<br />
<br />
<br />
= F . dr F . dr F . dr F . dr<br />
C<br />
...(2)<br />
OA AB BC CO<br />
<br />
Along OA, put y = 0 so that k dy = 0 in (1) and F . dr = x 2 dx,<br />
Where x is from 0 to a.<br />
3<br />
a<br />
a<br />
2<br />
F <br />
. dr<br />
<br />
3<br />
x dx<br />
x a<br />
OA = <br />
0 3 3<br />
<br />
Along AB, put x = a so that dx = 0 in (1), we get F .<br />
Where y is from 0 to b.<br />
<br />
b<br />
0<br />
0<br />
<br />
d r<br />
= 2ay dy<br />
...(3)<br />
2 2<br />
F . dr 2aydy<br />
= [ ay ] b<br />
0<br />
ab<br />
...(4)<br />
AB