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where is any particular anti-derivative.
Our author does mention that a function is an anti-derivative of its rate-of-change: i.e.,
It looks different than the one above, but it says exactly the same thing, of course.
Important Example: We use this notion time and again in applications.
So, for example,
In free-fall, a particle's acceration near to the earth is approximately constant (the acceleration due to gravity is ).
Now, if the particle starts falling, with initial velocity (at ), then its velocity will be given by
or
or
(since the constant is known at ). (What are the units of velocity?)
Now we can calculate the position (initially at height ):
or
or
(What are the units of position?)
And that is what Newton was doing under the apple tree, when the apple fell on his head and he discovered the law of universal gravitation (and that the moon also could fall on his head, were he not lucky).
So, as mentioned in class, differentiation and integration are not quite inverse processes: the derivative of a function is unique, and an infinite number of functions have the same derivative; vice versa, a function has an infinite number of anti-derivatives.
represent?
More generally:
That's the general idea. So, in terms of a definite integral, the rule is that
We can always do the change of variables
and hope that the integral on the right is easier to solve (certainly less cluttered). Notice especially the change in the limits on the integral.
Writing it in this last way may be mysterious, because of the change of variable to u (and the change in the limits); but it's the disappearance of g'(x) that's really curious. It falls right out of the change of variables, however: