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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