How do you integrate #int 1/(x^4sqrt(x^2+3))# by trigonometric substitution?

Answer 1

#sqrt(x^2+3)/(9x)-(x^2+3)^(3/2)/(27x^3)+C#

#int dx/(x^4*sqrt(x^2+3))#
After using #x=sqrt3*tany# and #dx=sqrt3*(secy)^2*dy# transforms, I found
#int (sqrt3*(secy)^2*dy)/((sqrt3*tany)^4*sqrt((sqrt3*tany)^2+3))#
=#int (sqrt3*(secy)^2*dy)/((9(tany)^4*sqrt((sqrt3*secy)^2))#
=#int (sqrt3*(secy)^2*dy)/((9(tany)^4*sqrt3*secy)#
=#1/9int (secy*dy)/(tany)^4#
=#1/9int (coty)^4*secy*dy#
=#1/9int (cosy/siny)^4*(dy/cosy)#
=#1/9int ((cosy)^3*dy)/(siny)^4#
=#1/9int ((cosy)^2*cosy*dy)/(siny)^4#
=#1/9int ((1-(siny)^2)*cosy*dy)/(siny)^4#
After using #z=siny# and #dz=cosy*dy# transforms, it became
#1/9int ((1-z^2)*dz)/z^4#
=#1/9int z^(-4)*dz-1/9int z^(-2)*dz#
=#1/9z^(-1)-1/27z^(-3)+C#
=#1/9(siny)^(-1)-1/27(siny)^(-3)+C#
=#1/9cscy-1/27(cscy)^3+C#
After using #x=sqrt3*tany#, #tany=x/sqrt3#, #secy=sqrt(x^2+3)/sqrt3# and #cscy=secy/tany=sqrt(x^2+3)/x# inverse transforms, I found
#sqrt(x^2+3)/(9x)-(x^2+3)^(3/2)/(27x^3)+C#
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Answer 2

To integrate ( \int \frac{1}{{x^4\sqrt{x^2+3}}} ) by trigonometric substitution, follow these steps:

  1. Substitute ( x = \sqrt{3}\tan{\theta} ).
  2. Calculate ( dx ) using ( x = \sqrt{3}\tan{\theta} ).
  3. Express ( x^2 + 3 ) in terms of ( \theta ).
  4. Substitute ( dx ) and the expression for ( x^2 + 3 ) into the integral.
  5. Simplify the integral using trigonometric identities.
  6. Integrate the simplified expression.
  7. Substitute ( \theta ) back in terms of ( x ) to find the final result.
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Answer 3

To integrate ( \int \frac{1}{x^4\sqrt{x^2+3}} ) by trigonometric substitution, we can use the substitution ( x = \sqrt{3}\tan(\theta) ). After substituting and simplifying, we can then use trigonometric identities to express the integral in terms of trigonometric functions. Finally, we evaluate the integral in terms of theta. The detailed steps are as follows:

  1. Let ( x = \sqrt{3}\tan(\theta) ). Then, ( dx = \sqrt{3}\sec^2(\theta) , d\theta ).

  2. Substitute ( x ) and ( dx ) into the integral: [ \int \frac{1}{(\sqrt{3}\tan(\theta))^4\sqrt{(\sqrt{3}\tan(\theta))^2+3}} \cdot \sqrt{3}\sec^2(\theta) , d\theta ]

  3. Simplify the expression inside the integral: [ = \int \frac{\sqrt{3}\sec^2(\theta)}{3\tan^4(\theta)\sqrt{3\tan^2(\theta)+3}} , d\theta ]

  4. Simplify further: [ = \int \frac{\sec^2(\theta)}{3\tan^4(\theta)} , d\theta ]

  5. Rewrite in terms of sine and cosine using the identity ( \tan^2(\theta) + 1 = \sec^2(\theta) ): [ = \int \frac{1}{3(\tan^2(\theta)+1)\tan^4(\theta)} , d\theta ]

  6. Rewrite ( \tan^2(\theta) ) as ( \sec^2(\theta) - 1 ): [ = \int \frac{1}{3((\sec^2(\theta) - 1)+1)\tan^4(\theta)} , d\theta ]

  7. Simplify inside the integral: [ = \int \frac{1}{3(\sec^2(\theta)\tan^4(\theta))} , d\theta ]

  8. Rewrite ( \sec^2(\theta)\tan^4(\theta) ) as ( (\sec^2(\theta))^2 - \sec^2(\theta) ): [ = \int \frac{1}{3(\sec^4(\theta) - \sec^2(\theta))} , d\theta ]

  9. Let ( u = \sec(\theta) ) and ( du = \sec(\theta)\tan(\theta) , d\theta ): [ = \frac{1}{3} \int \frac{1}{u^4 - u^2} , du ]

  10. Factor the denominator: [ = \frac{1}{3} \int \frac{1}{u^2(u^2 - 1)} , du ]

  11. Perform partial fraction decomposition: [ = \frac{1}{3} \int \left(\frac{1}{u^2} - \frac{1}{u^2 - 1}\right) , du ]

  12. Integrate each term separately: [ = \frac{1}{3} \left(-\frac{1}{u} - \ln|u - 1| + \ln|u|\right) + C ]

  13. Substitute back ( u = \sec(\theta) ) and simplify: [ = -\frac{1}{3\sec(\theta)} - \frac{1}{3}\ln|\sec(\theta) - 1| + \frac{1}{3}\ln|\sec(\theta)| + C ]

  14. Finally, substitute back ( \theta ) using the original substitution ( x = \sqrt{3}\tan(\theta) ) to obtain the integral in terms of ( x ).

This process provides the integral of ( \frac{1}{x^4\sqrt{x^2+3}} ) by trigonometric substitution.

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Answer from HIX Tutor

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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