Integrate: $\frac{dx}{(R^{2}+x^{2})^{3/2}}$

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The integral of the function $\frac{dx}{(R^{2}+x^{2})^{3/2}}$ is approached using the substitution $x = R \tan \theta$, leading to the transformation of the integral into terms of $\theta$. The discussion highlights the transition from an indefinite to a definite integral, with a focus on the limits of integration and the importance of changing them appropriately during variable substitution. Clarifications are made regarding the definitions of indefinite and definite integrals, emphasizing that they are not interchangeable. The conversation also touches on the concept of improper integrals, which may have contributed to the confusion. Understanding these distinctions is crucial for correctly evaluating integrals in calculus.
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Homework Statement



\int\frac{dx}{(R^{2}+x^{2})^{3/2}}

Homework Equations




The Attempt at a Solution



<br /> <br /> \mbox{Let }x = R\\tan\theta \Rightarrow dx = R\\sec^{2}d\theta\\<br /> x^{2} = R^{2}\\tan^{2}\theta\\<br /> \Rightarrow R^{2} + x^{2} = R^{2}\\( 1 + tan^{2}\theta)\\<br /> \Rightarrow R^{2} + x^{2} = R^{2}\\sec^{2}\\<br /> \Rightarrow (R^{2} + x^{2})^{3/2} = R^{3}\\sec^{3}\theta\\<br /> \\<br /> Therefore, \int\frac{dx}{(R^{2}+x^{2})^{3/2}}\\<br /> =\int\frac{R\\sec^{2}\theta}{R^{3}\\sec^{3}\theta}\\d\theta\\<br /> =\frac{1}{R^{2}}\\ \int^{\infty}_{-\infty}cos\theta\\ d\theta\\<br /> =\frac{1}{R^{2}}\stackrel{lim}{n\rightarrow\infty} \int^{N}_{-N}cos\theta\\ d\theta\\<br /> =\frac{1}{R^{2}}\stackrel{lim}{n\rightarrow\infty}(sin\theta)\mid^{N}_{-N}\\<br /> =\frac{1}{R^{2}}\stackrel{lim}{n\rightarrow\infty}(sin N + sin N)<br /> =\frac{2}{R}\stackrel{lim}{n\rightarrow\infty}sin N<br />

and then?
 
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Homework Statement



\int\frac{dx}{(R^{2}+x^{2})^{3/2}}

Homework Equations




The Attempt at a Solution



\mbox{Let }x = R\\tan\theta \Rightarrow dx = R\\sec^{2}d\theta

x^{2} = R^{2}\\tan^{2}\theta

\Rightarrow R^{2} + x^{2} = R^{2}\\( 1 + tan^{2}\theta)

\Rightarrow R^{2} + x^{2} = R^{2}\\sec^{2}\theta

\Rightarrow (R^{2} + x^{2})^{3/2} = R^{3}\\sec^{3}\theta

\mbox{Therefore, }\int\frac{dx}{(R^{2}+x^{2})^{3/2}}

=\int\frac{R\\sec^{2}\theta}{R^{3}\\sec^{3}\theta}\\d\theta

=\frac{1}{R^{2}}\\ \int^{\infty}_{-\infty}cos\theta\\ d\theta

=\frac{1}{R^{2}}\stackrel{lim}{n\rightarrow\infty} \int^{N}_{-N}cos\theta\\ d\theta

=\frac{1}{R^{2}}\stackrel{lim}{n\rightarrow\infty}(sin\theta)\mid^{N}_{-N}

=\frac{1}{R^{2}}\stackrel{lim}{n\rightarrow\infty}(sin N + sin N)

=\frac{2}{R^{2}}\stackrel{lim}{n\rightarrow\infty}sin N

and then?
 
Why did you suddenly switch from indefinite to definite (across the entire real axis, no less) integrals partway through? I would assume that you continue to use the indefinite integral.
 
Fixed your LaTex.
\begin{align*}<br /> \int \frac{dx}{(R^2+x^2)^{3/2}} &amp; = \int\frac{R\sec^2\theta}{R^3\sec^3\theta} d\theta \\<br /> &amp; = \frac{1}{R^2} \int^{\infty}_{-\infty}\cos\theta\,d\theta \\<br /> &amp; = \frac{1}{R^2} \lim_{N \to \infty} \int^N_{-N}\cos\theta\,d\theta \\<br /> &amp; = \frac{1}{R^2} \lim_{N \to \infty} (\sin\theta)\mid^N_{-N} \\<br /> &amp; = \frac{1}{R^2} \lim_{N \to \infty} (\sin N + \sin N) \\<br /> &amp; = \frac{2}{R^2} \lim_{N \to \infty} \sin N<br /> \end{align*}
You need to change the limits of the integral when you change variables.
 
I thought that an indefinite integral is just a definite integral with limits that are infinity.
Isn't that true?
 
hasan_researc said:
I thought that an indefinite integral is just a definite integral with limits that are infinity.
Isn't that true?
Nope, that is unfortunately not true at all.
 
But \theta from \infty to -\infty is the same as x from \infty to -\infty. Isn't it?
 
What is an indefinite integral, then?
 
\lim_{\theta\to\infty}{\tan(\theta)} doesn't exist. You have a better chance reversing the substitution before taking the limits.
 
  • #10
An indefinite integral simply produces the antiderivative of the function being integrated.
\int f(x) dx = F(x) + c
where differentiating F(x) yields the function f(x).

Meanwhile, a definite integral of a function over a specified interval is equal to the difference between the values of the antiderivative at the endpoints of the interval.
\int_{a}^{b}f(x) dx = F(b) - F(a)

One can view the antiderivative as the basis with which we employ the fundamental theorem of calculus to compute definite integrals.
 
  • #11
hasan_researc said:
I thought that an indefinite integral is just a definite integral with limits that are infinity.
Isn't that true?
As already noted, that's not true. You might be thinking of an improper integral.
 

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