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Calculus- Early Transcendentals, 2021a

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274 Techniques of Integration<br />

Exercise 7.3.11<br />

∫ √<br />

x 2 + 1 dx<br />

Exercise 7.3.17<br />

∫ √<br />

4x 2 + 1 dx<br />

Exercise 7.3.12<br />

∫ √<br />

x 2 + 4 dx<br />

Exercise 7.3.18<br />

∫ √<br />

1 − 9x 2 dx<br />

Exercise 7.3.13<br />

∫ √<br />

1 − x 2 dx<br />

Exercise 7.3.19<br />

∫ √<br />

16x 2 − 1 dx<br />

Exercise 7.3.14<br />

∫ √<br />

9 − x 2 dx<br />

Exercise 7.3.20<br />

∫<br />

8<br />

√<br />

x 2 + 2 dx<br />

Exercise 7.3.15<br />

∫ √<br />

x 2 − 1 dx<br />

Exercise 7.3.21<br />

∫<br />

3<br />

√<br />

7 − x 2 dx<br />

Exercise 7.3.16<br />

∫ √<br />

x 2 − 16 dx<br />

∫<br />

Exercise 7.3.22<br />

5<br />

√<br />

x 2 − 8 dx<br />

Exercises 7.3.11 to 7.3.22 were adapted by Lyryx from APEX <strong>Calculus</strong>, Version 3.0, written by G. Hartman. This material<br />

is released under Creative Commons license CC BY-NC (https://creativecommons.org/licenses/by-nc/4.0/ ). See<br />

the Copyright and Revision History pages in the front of this text for more information.<br />

7.4 Integration by Parts<br />

To explore the technique known as integration by parts, we start with the product rule:<br />

We can rewrite this as<br />

d<br />

dx f (x)g(x)= f ′ (x)g(x)+ f (x)g ′ (x).<br />

∫<br />

f (x)g(x)=<br />

∫<br />

f ′ (x)g(x)dx+<br />

f (x)g ′ (x)dx,<br />

and then<br />

∫<br />

∫<br />

f (x)g ′ (x)dx = f (x)g(x) −<br />

f ′ (x)g(x)dx.<br />

This may not seem particularly useful at first glance, but it turns out that in many cases we have an integral<br />

of the form<br />

∫<br />

f (x)g ′ (x)dx<br />

but that<br />

∫<br />

f ′ (x)g(x)dx<br />

is easier. This technique for turning one integral into another is called integration by parts, and is usually<br />

written in more compact form. If we let u = f (x) and v = g(x) then du = f ′ (x)dx and dv = g ′ (x)dx and<br />

∫<br />

∫<br />

udv= uv − vdu.<br />

To use this technique we need to identify likely candidates for u = f (x) and dv = g ′ (x)dx.

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