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

  • Thread starter hasan_researc
  • Start date
  • Tags
    Integration
In summary, the symbol "R" in the given integral represents the radius of the circle in the denominator and does not change as x varies. To solve the integral, you can use the substitution or trigonometric substitution methods. The domain of the integral is all real numbers except for x = ±R where it is undefined. It can be simplified using trigonometric functions or as a rational function with an arctangent term. The integral has physical significance in physics and engineering, specifically in calculating gravitational potential energy between two point masses at a distance R from the point.
  • #1
hasan_researc
170
0

Homework Statement



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

Homework Equations




The Attempt at a Solution



[tex]

\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}\\
\Rightarrow (R^{2} + x^{2})^{3/2} = R^{3}\\sec^{3}\theta\\
\\
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}\stackrel{lim}{n\rightarrow\infty}sin N
[/tex]

and then?
 
Last edited:
Physics news on Phys.org
  • #2

Homework Statement



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

Homework Equations




The Attempt at a Solution



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

[tex]x^{2} = R^{2}\\tan^{2}\theta[/tex]

[tex]\Rightarrow R^{2} + x^{2} = R^{2}\\( 1 + tan^{2}\theta)[/tex]

[tex]\Rightarrow R^{2} + x^{2} = R^{2}\\sec^{2}\theta[/tex]

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

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

[tex]=\int\frac{R\\sec^{2}\theta}{R^{3}\\sec^{3}\theta}\\d\theta[/tex]

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

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

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

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

[tex]=\frac{2}{R^{2}}\stackrel{lim}{n\rightarrow\infty}sin N[/tex]

and then?
 
  • #3
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.
 
  • #4
Fixed your LaTex.
[tex]\begin{align*}
\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} \lim_{N \to \infty} \int^N_{-N}\cos\theta\,d\theta \\
& = \frac{1}{R^2} \lim_{N \to \infty} (\sin\theta)\mid^N_{-N} \\
& = \frac{1}{R^2} \lim_{N \to \infty} (\sin N + \sin N) \\
& = \frac{2}{R^2} \lim_{N \to \infty} \sin N
\end{align*}[/tex]
You need to change the limits of the integral when you change variables.
 
  • #5
I thought that an indefinite integral is just a definite integral with limits that are infinity.
Isn't that true?
 
  • #6
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.
 
  • #7
But [tex]\theta[/tex] from [tex]\infty[/tex] to [tex]-\infty[/tex] is the same as [tex]x[/tex] from [tex]\infty[/tex] to [tex]-\infty[/tex]. Isn't it?
 
  • #8
What is an indefinite integral, then?
 
  • #9
[tex]\lim_{\theta\to\infty}{\tan(\theta)}[/tex] 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.
[tex]\int f(x) dx = F(x) + c[/tex]
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.
[tex]\int_{a}^{b}f(x) dx = F(b) - F(a)[/tex]

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.
 

1. What does the symbol "R" represent in the given integral?

The symbol "R" represents the radius of the circle in the denominator of the integral. It is a constant value and does not change as x varies.

2. How do you solve this integral?

To solve this integral, you can use the substitution method by letting u = R^2 + x^2 and then using the substitution formula for integrals. Alternatively, you can use the trigonometric substitution method by letting x = Rtanθ and using the appropriate trigonometric identities.

3. What is the domain of this integral?

The domain of this integral is all real numbers except for x = ±R, where the integral is undefined due to division by zero.

4. Can this integral be simplified?

Yes, this integral can be simplified by using the trigonometric substitution method to rewrite it in terms of trigonometric functions. It can also be rewritten as a rational function with an arctangent term.

5. What is the physical significance of this integral?

This integral has physical significance in physics and engineering, specifically in calculating the gravitational potential energy between two point masses. The integral represents the gravitational potential at a point due to a point mass at a distance R from the point.

Similar threads

  • Calculus and Beyond Homework Help
Replies
5
Views
1K
  • Calculus and Beyond Homework Help
Replies
3
Views
538
Replies
14
Views
986
  • Calculus and Beyond Homework Help
Replies
3
Views
778
  • Calculus and Beyond Homework Help
Replies
8
Views
861
  • Calculus and Beyond Homework Help
Replies
17
Views
582
  • Calculus and Beyond Homework Help
Replies
6
Views
347
  • Calculus and Beyond Homework Help
Replies
2
Views
859
  • Calculus and Beyond Homework Help
Replies
1
Views
216
  • Calculus and Beyond Homework Help
Replies
3
Views
224
Back
Top