Solution to Problem 11.8-5© 2001 by Karl Hahn |
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5)The problem is to integrate
dx
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Step 1: Use the exponential substitution that you learned in this section. Remember that e2x is nothing more than the square of ex. When you've got this one substituted, click here to continue.
The substitution is
u = ex |
and | du |
So the substituted integral is
dx
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du
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Step 2: Apply trig substitution. Click here if you need a reminder on what trig substitution to make here. This problem is now very similar to worked example number 3. You can do it by trig substitution or by hyperbolic substitution. Here I will do it using the former, but if you are motivated you can work it through again using hyperbolic substitution on your own. Make the substitution and click here to continue.
The substitution is
tan(v) = u |
and | (tan2(v) + 1) dv = du |
The integral becomes
dx
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(tan2(v) + 1) dv |
___________ √tan2(v) + 1 |
Step 3: Use trig identities to simplify the whoopie out of this integrand. It is useful to get this one into terms of sines and cosines. Use identities from our recent table. Also remember that
tan2(v) = |
sin2(v) |
and | sec(v) = |
1
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Make the simplifications and then click here to continue.
The simplification steps are, first in the numerator:
___________
√tan2(v) + 1 = sec(v)
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Make that replacement, then convert the whole thing to sines and cosines. You find that
___________ √tan2(v) + 1 |
1
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cos(v) |
So now the integral is
dx
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cos(v) |
Step 4: Simple substitution. Do you see the one part of this integrand that is the derivative of the other? Make the substitution suggested by that and then click here to continue.
The substitution is
w = sin(v) |
and | dw = cos(v) dv |
When you make that substitution, the integral becomes trivial.
dx
|
cos(v) |
dw |
1
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Step 5: Substitute back. You have to go from w to v to u to x. You might have to use the identity table to do the back substitution of the trig functions. When you've done all of this, click here to see the final answer.
The progressive back substitutions are
dx
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1 1
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___________
√tan2(v) + 1
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______
√u2 + 1
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_______
√e2x + 1
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