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Active Calculus - Multivariable

Activity 13.8.3.
Consider the vector field \(\vF = \displaystyle\frac{-y}{{x^2+y^2}}\vi + \frac{x}{{x^2+y^2}}\vj\text{.}\) Notice that \(\vF\) is smooth everywhere in the plane other than at the point \((0,0)\text{.}\) This vector field is plotted in Figure 13.8.6, but we have not plotted the vectors close to the origin as their magnitudes get so large that they make it hard to interpret the figure. Here Green’s Theorem applies to any simple closed curve \(C\) that neither passes through \((0,0)\) nor bounds a region containing \((0,0)\text{.}\)
A vector field with vectors tangent to circles oriented counterclockwise and centered at the origin as well as the unit circle centered at the origin and oriented counterclockwise. The vectors are longer close to the origin and shorter farther from the origin.
Figure 13.8.6. The vector field \(\vF\)
(a)
Find the circulation density of \(\vF\) (i.e., the integrand of the double integral in Green’s Theorem).
Hint.
Make sure to note any exceptional points at which your formula is not valid.
(b)
Suppose that \(C\) is the unit circle centered at the origin. Without doing any calculations, what can you say about \(\oint_C \vF\cdot d \vr\text{?}\) what does this tell you about if \(\vF\) is path-independent?
(c)
What would you get if you integrated the circulation density of \(\vF\) over the region bounded by \(C\text{?}\)
(e)
Is the vector field \(\vG = \displaystyle\frac{x}{x^2+y^2}\vi +\frac{y}{x^2+y^2}\vj\text{,}\) which is shown in Figure 13.8.7, path-independent? Why or why not?
A vector field with vectors radiating from the origin and orthogonal to circles centered at the origin. Vectors are longest near the origin and get shorter farther from the origin.
Figure 13.8.7. The vector field \(\vG\)
(f)
Suppose that \(C\) is the unit circle centered at the origin. Find \(\oint_C \vG\cdot d \vr\text{.}\) Can you do this using Green’s Theorem?