We have,the circulation of
around a square of side 3, centered at the origin, lying in the yz-plane, and oriented counterclockwise when viewed from the positive x-axis is

From the Question we have the equation to be

Therefore

Where
For i

For j


For z


Therefore

Generally considering
as the origin
We apply Stoke's Theorem





Therefore
The circulation of
around a square of side 3, centered at the origin, lying in the yz-plane, and oriented counterclockwise when viewed from the positive x-axis is
