BELIEVE ME NOT! - - A SKEPTICs GUIDE
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Suppose we have a function g(x) which we know is the derivative
[with respect to x] of some other function f(x), but
we don't know which - i.e. we know g(x) explicitly
but we don't know [yet] what f(x) it is the derivative of.
We may then ask the question, ``What is the function f(x)
whose derivative [with respect to x] is g(x)?''
Another way of putting this would be to ask,
``What is the antiderivative of g(x)?''11.1
Another name for the antiderivative is the integral,
which is in fact the ``official'' version, but I like the former better
because the name suggests how we go about ``solving''
one.11.2
For a handy example consider
.
Then the antiderivative [integral] of g(x) with respect to x
is
[where f0 is some constant] because the derivative
[with respect to x] of x2 is 2x and the derivative of
any constant is zero. Since any combination of constants
is also a constant, it is equally valid to make the
arbitrary constant term of the same form as the part which
actually varies with x, viz.
.
Thus f0 is the same thing as
and it is a matter of taste which you want to use.
Naturally we have a shorthand way of writing this.
The differential equation
can be turned into the integral equation
|
(11.2) |
which reads,
``f(x) is the integral of g(x) with respect to x from x0 to x.''
We have used the rule that the integral of the differential
of f [or any other quantity] is just the quantity itself,11.3
in this case f:
|
(11.3) |
Our example then reads
where we have used the feature that any constant (like k)
can be brought ``outside the integral'' - i.e. to the left
of the integral sign
.
Now let's use these new tools to transform Newton's SECOND LAW
into something more comfortable.
Next: Impulse and Momentum
Up: Some Math Tricks
Previous: Differentials
Jess H. Brewer
1998-10-08