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Definition

A region D is a connected region    if, for any two points P 1 and P 2 , there is a path from P 1 to P 2 with a trace contained entirely inside D . A region D is a simply connected region    if D is connected for any simple closed curve C that lies inside D , and curve C can be shrunk continuously to a point while staying entirely inside D . In two dimensions, a region is simply connected if it is connected and has no holes.

All simply connected regions are connected, but not all connected regions are simply connected ( [link] ).

A diagram showing simply connected, connected, and not connected regions. The simply connected regions have no holes. The connected regions may have holes, but a path can still be found between any two points in the region. The not connected region has some points that cannot be connected by a path in the region. Here, this is illustrated by showing two circular shapes that are defined as part of region D1 but are separated by white space.
Not all connected regions are simply connected. (a) Simply connected regions have no holes. (b) Connected regions that are not simply connected may have holes but you can still find a path in the region between any two points. (c) A region that is not connected has some points that cannot be connected by a path in the region.

Is the region in the below image connected? Is the region simply connected?

A shaded circle with an open space in the shape of a circle inside it but very close to the boundary.

The region in the figure is connected. The region in the figure is not simply connected.

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Fundamental theorem for line integrals

Now that we understand some basic curves and regions, let’s generalize the Fundamental Theorem of Calculus to line integrals. Recall that the Fundamental Theorem of Calculus says that if a function f has an antiderivative F , then the integral of f from a to b depends only on the values of F at a and at b —that is,

a b f ( x ) d x = F ( b ) F ( a ) .

If we think of the gradient as a derivative, then the same theorem holds for vector line integrals. We show how this works using a motivational example.

Evaluating a line integral and the antiderivatives of the endpoints

Let F ( x , y ) = 2 x , 4 y . Calculate C F d r , where C is the line segment from (0,0) to (2,2)( [link] ).

We use [link] to calculate C F d r . Curve C can be parameterized by r ( t ) = 2 t , 2 t , 0 t 1 . Then, F ( r ( t ) ) = 4 t , 8 t and r ( t ) = 2 , 2 , which implies that

C F · d r = 0 1 4 t , 8 t · 2 , 2 d t = 0 1 ( 8 t + 16 t ) d t = 0 1 24 t d t = [ 12 t 2 ] 0 1 = 12.
A vector field in two dimensions. The arrows are longer the further away from the origin they are. They stretch out from the origin, forming a rectangular pattern. A line segment is drawn from P_0 at (0,0) to P_1 at (2,2).
The value of line integral C F d r depends only on the value of the potential function of F at the endpoints of the curve.

Notice that F = f , where f ( x , y ) = x 2 + 2 y 2 . If we think of the gradient as a derivative, then f is an “antiderivative” of F . In the case of single-variable integrals, the integral of derivative g ( x ) is g ( b ) g ( a ) , where a is the start point of the interval of integration and b is the endpoint. If vector line integrals work like single-variable integrals, then we would expect integral F to be f ( P 1 ) f ( P 0 ) , where P 1 is the endpoint of the curve of integration and P 0 is the start point. Notice that this is the case for this example:

C F d r = C f d r = 12

and

f ( 2 , 2 ) f ( 0 , 0 ) = 4 + 8 0 = 12 .

In other words, the integral of a “derivative” can be calculated by evaluating an “antiderivative” at the endpoints of the curve and subtracting, just as for single-variable integrals.

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The following theorem says that, under certain conditions, what happened in the previous example holds for any gradient field. The same theorem holds for vector line integrals, which we call the Fundamental Theorem for Line Integrals.

The fundamental theorem for line integrals

Let C be a piecewise smooth curve with parameterization r ( t ) , a t b . Let f be a function of two or three variables with first-order partial derivatives that exist and are continuous on C . Then,

C f d r = f ( r ( b ) ) f ( r ( a ) ) .
Practice Key Terms 6

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Source:  OpenStax, Calculus volume 3. OpenStax CNX. Feb 05, 2016 Download for free at http://legacy.cnx.org/content/col11966/1.2
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