118 Ordinary Differential Equations
FUNDAMENTAL THEOREM OF INTEGRAL CALCULUS
If f ( x) is continuous on the interval [a , b] and if F' ( x) = f ( x) for all
x E [a , b], then
1 b f(x) dx = F(x) lb a= F(b) - F(a)
Problems which appear in calculus texts are chosen very carefully so that
required integrations can be performed- that is , so that the antiderivative
of the integrand can be written as an elementary function. In this respect,
problems which appear in calculus texts are somewhat artificial, because in
practice the required integration usually cannot be performed explicitly. Look
at the section on computing arc length in any calculus text and you will see
that very few examples and exercises are given. This is because it is difficult
to choose many functions y(x) such that the integral of Jl + [y'(x)]2 can be
written as an elementary function.
Unfortunately, most functions f(x) which arise in practice do not
have antiderivatives that can be written as elementary functions.
So we need to answer the following questions:
"How can we rewrite any definite integral J: f(x) dx as an initial value
problem?"
"How can we numerically solve the resulting initial value problem and
thereby compute a value for the definite integral?"
If f(x) is integrable on [a, b], we can symboli cally write the antiderivative
of f(x) on [a, b] as
(1) F(x) = 1x f(t) dt for x E [a, b].
Suppose F(x) is differentiable on [a, b]. Differentiating (1) with respect to
x, we find F'(x) = f(x ) for all x E [a, b]. So F(x) satisfies the differential
equation y' = f(x) on [a , b]. Evaluating F(x) at x = a, we get F(a) = 0.
Thus, the antiderivative F(x) of f(x) satisfies the initial value problem
(2) y' = f(x); y(a) = 0
on the interval [a , b] and the value of the definite integral of f(x) on [a , b] is
lb f(t) dt = y(b) = F(b).