vector cal. please show step where is a Cl function. Let it be defined in the wh
ID: 3197144 • Letter: V
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vector cal. please show step
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In plane : A point in a region in the plane is an interior point of if it is the center of a disk that lies entirely in . A point is a boundary point of if every disk centered at contains points that lie outside as well as points that lie in (The boundary point itself need not belong to ) . The interior of the region is the set of interior points of The boundary of the region is the set of boundary points of A region is open if it consists entirely of interior points. A region is closed if it contains all of its boundary points.
By a parametrized curve, or simply a curve, in R n , we mean the image C of a continuous function : [r, s] R n , where [r, s] is a closed interval in R. C is called a plane curve, resp. a space curve, if n = 2, resp. n = 3. An example of the former, resp.the latter, is the cycloid, resp. the right circular helix, parametrized by : [0, 2] R 2 with (t) = (t sin t, 1 cost), resp. : [3, 6] R 3 with (t) = (cost,sin t, t). Note that a parametrized curve C has an orientation, i.e., a direction; it starts at P = (r), moves along as t increases from r, and ends at Q = (s). We call the direction from P to Q positive and the one from Q to P negative. It is customary to say that C is a closed curve if P = Q. We say that C is differentiable iff is a differentiable function. Definition. Let C be a differentiable curve in R n parametrized by an as above. Let a = (t0), with t0 (r, s). Then 0 (t0) is called the tangent vector to C at a (in the positive direction). For example, consider the unit circle C in the plane given by : [0, 2] R 2 , t (cost,sin t). Clearly is differentiable, and we have 0 (t) = ( sin t, cost) for all t (0, 2). Consider the point a = (1/2, 3/2) on the circle; clearly, a = (/3). By the above definition, the tangent vector to C at a is given by 0 (/3) = ( 3/2, 1/2). Let us now check that this agrees with our notion of a tangent from one variable Calculus. To this end we want to think of C as the graph of a one variable function, but this is not possible for all of C. However, we can express the upper and the lower semi-circles as graphs of such functions. And since the point of interest a lies on the upper semi-circle C +, we look at the function y = f(x) with f(x) = 1 x 2 , whose graph is C +. Note that (by the chain rule) f 0 (x) = x(1 x 2 ) 1/2 . The slope of the tangent to C + at a is then given by f 0 (1/2) = 1/ 3. Hence the tangent line to C at a is the line L passing through (1/2, 3/2) of slope 1/ 3. This is the unique line passing through a in the direction of the tangent vector ( 3/2, 1/2). (In other words L is the unique line passing through a and parallel to the line joining the origin to ( 3/2, 1/2).) The situation is similar for any plane curve which is the graph of a one-variable function f, i.e. of the form (t) = (t, f(t)). So the definition of a tangent vector above is very reasonable.
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