Theorem IV.4. [The Fundamental Theorem Of Calculus For Differential
Equations]
Suppose
that P is a positive continuous function on [A,B].
Then there is a function F so that F'(t) = P(t) for all t where A < t < B. In fact, F can be defined at x = t to be the area of the region enclosed by the Xaxis, the graph of the function P (i.e., Y = P(X) ), the line X = A, and the line X = t. See Figure IV.HA.i. Proof: For t > A let F(t) denote the area of the region enclosed by the X axis, X = A, X = t, and Y = P(x). Notice that F(A) = 0 because the "region" in this case is a line and its area is 0. We must show that F'(a) = P(a) for a > A, so that F is a solution for the differential equation for the interval [A,B] We interpret the expression F(a+h)  F(a) when
h > 0
Examining this region more carefully in Figure IV.HA.iii, we notice that since P is continuous on [a, a + h], P will have extreme values. We let c_{*} and c^{*} denote the points
in [a, a + h] where P has its minimum and maximum
values.
E.O.P.


Notes: 1. Another proof of this result in a slightly more general
setting is given in the next chapter.
2. Geometric Interpretation of F'(a) = P(a): This result has the same informational content as Barrow's Theorem discussed in Chapter 0. At this stage you might review the statement of Barrow's Theorem in terms of how to draw the tangent line at a point on the area curve determined by a given curve and the Xaxis. Under an appropriate interpretation of the derivative as the slope of the tangent line, the proof of Barrow's Theorem given in the appendix to Chapter 0 gives a geometric argument that can be modified to justify Theorem IV.4 as well. 3. Velocity Interpretations of F'(a) = P(a): Consider P as a velocity function for some moving object, X, and F as a position function for another moving object,Y, with its position at time t being equal to the area of the region described in the theorem. Under this interpretation, the inequality Under the same interpretation, the inequality 