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Unit 1: Integration
If we let u = 1 – x , then du = – 2xdx, but we don't have –2xdx. Notes
2
Also, integration by parts will not function.
2 –3/2
2 –1/2
If we let u = (1 – x ) , then du = x(1 – x ) dx. dv = dx, and so v = x.
1 x x 2
Putting it together, we have: 2 dx 2 3/2 dx , which has only made the
1 x 1 x 1 x 2
integral worse.
But what happens if we let x = sin. Observe that the quantity inside of the square root turns out
t be 1 – sin = cos , by the Pythagorean Identity above.
2
2
Also, observe that dx = cosd. Unlike before, here we do not have to solve for dx; it is already
given to use.
So, now we just plug everything in and solve.
1 x cos cos
dx cos d d d d C
2
2
1 x 2 1 sin cos cos
The question remains, what is ? We need to solve for in terms of x.
If we gaze above, we observe such a relationship. Recall, we had let x = sin. That means that
–1
= sin (x) or arcsin(x).
1
So, we have that dx arcsin x . C
1 x 2
1
Example: Evaluate 2 dx .
x 4x 13
First we complete the square in the denominator by observing that 13 = 4 + 9 and then that
2
2
provides us x + 4x + 4 + 9 = (x + 2) .
1 1 1
2 dx dx dx .
2
2
x 4x 13 x 4x 4 9 x 2 3 2
Then we let x + 2 = 3tan. Observe that dx = 3sec d.
2
After substituting, we have
2
2
2
1 3sec d 3sec d 3sec d 1 1
dx
2 2 2 2 2 d . C
x 2 3 3tan 9 9tan 9 9sec 3 3
x 2
Solving for , we have arctan .
3
1 1 x 2
Thus, 2 dx arctan C .
x 4x 13 3 3
dx
Example: Evaluate 2
d 4 x 2
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