Substitution with Definite Integrals
When you substitute in a definite integral, the limits are -values, so they have to become -values too. Once they do, you can finish entirely in and never switch back to .
What the symbols mean
- New lower limit
The u-value when x = a.
- New upper limit
The u-value when x = b.
Explanation
Substitution with definite integrals is simply the substitution rule plus one extra step: translating the endpoints into the new variable. All we're really saying is that if you rename as , you have to rename everything, including where the interval starts and stops. The formula has just that one new piece: and (the -values you get by plugging the old endpoints and into ). Everything else is the substitution you already know.
Think about why the limits have to change. The limits and say "from to ." Once the integral is written in , it's asking about , and doesn't run from to ; it runs from to . Leaving the old numbers on would answer a different question.
Two correct ways to finish:
- Change the limits to and , and evaluate in .
- Find the antiderivative in , substitute back to , and use the original limits.
A common mistake. It's tempting to mix the two: find the antiderivative in , then plug in the original -limits, because those are the numbers written on the integral. That gives the wrong answer. Either change the limits or switch back to , but not half of each.
Symmetry shortcuts on :
- odd (): .
- even (): .
See it
Worked examples
Evaluate .
- 1
Let , so . Convert the limits: when , , and when , .
Practice
Type your answer and check it. Solve them all to complete the lesson.
Evaluate .
Evaluate .
Evaluate .
Evaluate .
Evaluate .
Water flows into a tank at liters per minute. How much enters between and ?
The hardest one here. Get it, and you've got this lesson.
Evaluate .
Where it's used
Symmetry arguments like the odd-function rule save enormous effort in physics and signal processing: half of a Fourier calculation vanishes before you start.