How do you integrate #int 1/sqrt(9x^2-18x+13) # using trigonometric substitution?
I can give you a solution but it uses a hyperbolic substitution as oppose to a standard trig substitution but it is still very similar.
We begin by re writing the quadratic under the square root in completed square / vertex form.
We can re write the integral as:
At this point we may like to consider the substitution:
It also follows from this substitution that:
Notice it is not a standard trig function but a hyperbolic function
Now putting this into the integral we get:
Which simplifies to:
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To integrate (\int \frac{1}{\sqrt{9x^2 - 18x + 13}}) using trigonometric substitution, we can use the substitution (x = \frac{1}{3} + \frac{2}{3} \sin(\theta)). This substitution helps simplify the expression into a form that can be integrated more easily. Here's how it works:
Given the integral (\int \frac{1}{\sqrt{9x^2 - 18x + 13}} dx),
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Substitute (x = \frac{1}{3} + \frac{2}{3} \sin(\theta)) into the integral.
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Calculate (dx) and substitute into the integral.
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Simplify the integrand using trigonometric identities.
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Integrate with respect to (\theta).
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Substitute back for (x) to find the final answer.
Here are the steps in detail:
Given: [ x = \frac{1}{3} + \frac{2}{3} \sin(\theta) ] Differentiate both sides with respect to (\theta) to find (dx): [ dx = \frac{2}{3} \cos(\theta) d\theta ] Substitute (dx) and (x) into the integral: [ \begin{aligned} \int \frac{1}{\sqrt{9x^2 - 18x + 13}} dx &= \int \frac{1}{\sqrt{9\left(\frac{1}{3} + \frac{2}{3}\sin(\theta)\right)^2 - 18\left(\frac{1}{3} + \frac{2}{3}\sin(\theta)\right) + 13}} \frac{2}{3}\cos(\theta) d\theta \ &= \int \frac{1}{\sqrt{9\left(\frac{1}{3} + \frac{4}{9}\sin^2(\theta)\right) - 6\left(\frac{1}{3} + \frac{2}{3}\sin(\theta)\right) + 13}} \frac{2}{3}\cos(\theta) d\theta \ &= \int \frac{1}{\sqrt{1 + \frac{4}{9}\sin^2(\theta)}} \frac{2}{3}\cos(\theta) d\theta \ &= \int \frac{1}{\sqrt{1 + \frac{4}{9}(1 - \cos^2(\theta))}} \frac{2}{3}\cos(\theta) d\theta \ &= \int \frac{1}{\sqrt{1 + \frac{4}{9} - \frac{4}{9}\cos^2(\theta)}} \frac{2}{3}\cos(\theta) d\theta \ &= \int \frac{1}{\sqrt{\frac{13}{9} - \frac{4}{9}\cos^2(\theta)}} \frac{2}{3}\cos(\theta) d\theta \ &= \int \frac{1}{\sqrt{\frac{13}{9}\left(1 - \frac{4}{13}\cos^2(\theta)\right)}} \frac{2}{3}\cos(\theta) d\theta \ &= \int \frac{1}{\sqrt{\frac{13}{9}}\sqrt{1 - \frac{4}{13}\cos^2(\theta)}} \frac{2}{3}\cos(\theta) d\theta \ &= \int \frac{1}{\sqrt{\frac{13}{9}}\sqrt{1 - \left(\frac{2}{\sqrt{13}}\right)^2\cos^2(\theta)}} \frac{2}{3}\cos(\theta) d\theta \ \end{aligned} ]
At this point, we can see that the integral can be simplified further using a trigonometric identity. We can use the substitution (u = \frac{2}{\sqrt{13}}\cos(\theta)) to simplify the integral.
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To integrate ( \int \frac{1}{\sqrt{9x^2 - 18x + 13}} ) using trigonometric substitution, we first complete the square in the denominator:
[ 9x^2 - 18x + 13 = 9(x^2 - 2x) + 13 ]
[ = 9(x^2 - 2x + 1) + 13 - 9 ]
[ = 9(x - 1)^2 + 4 ]
Now, let ( x - 1 = \frac{2}{3} \sec(\theta) ). Then, ( dx = \frac{2}{3} \sec(\theta) \tan(\theta) d\theta ).
Substituting into the integral:
[ \int \frac{1}{\sqrt{9x^2 - 18x + 13}} , dx ]
[ = \int \frac{1}{\sqrt{9\left(\frac{2}{3}\sec(\theta)\right)^2 + 4}} \cdot \frac{2}{3} \sec(\theta) \tan(\theta) , d\theta ]
[ = \int \frac{1}{\sqrt{4\sec^2(\theta) + 4}} \cdot \frac{2}{3} \sec(\theta) \tan(\theta) , d\theta ]
[ = \int \frac{1}{\sqrt{4(\sec^2(\theta) + 1)}} \cdot \frac{2}{3} \sec(\theta) \tan(\theta) , d\theta ]
[ = \int \frac{1}{\sqrt{4\tan^2(\theta) + 4}} \cdot \frac{2}{3} \sec(\theta) \tan(\theta) , d\theta ]
[ = \int \frac{1}{\sqrt{4(\tan^2(\theta) + 1)}} \cdot \frac{2}{3} \sec(\theta) \tan(\theta) , d\theta ]
[ = \int \frac{1}{\sqrt{4\tan^2(\theta) + 4}} \cdot \frac{2}{3} \sec(\theta) \tan(\theta) , d\theta ]
[ = \int \frac{1}{\sqrt{4\tan^2(\theta) + 4}} \cdot \frac{2}{3} \sec(\theta) \tan(\theta) , d\theta ]
[ = \int \frac{1}{2\sqrt{\tan^2(\theta) + 1}} \cdot \frac{4}{3} \tan(\theta) , d\theta ]
[ = \frac{2}{3} \int \frac{\tan(\theta)}{\sqrt{\tan^2(\theta) + 1}} , d\theta ]
Now, using the substitution ( u = \tan(\theta) ), ( du = \sec^2(\theta) , d\theta ):
[ = \frac{2}{3} \int \frac{du}{\sqrt{u^2 + 1}} ]
[ = \frac{2}{3} \sinh^{-1}(u) + C ]
[ = \frac{2}{3} \sinh^{-1}(\tan(\theta)) + C ]
Finally, substitute back ( \theta = \sec^{-1}\left(\frac{3}{2}(x - 1)\right) ) to get the final answer in terms of ( x ).
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When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
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