How do I solve this integral using partial integration?

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In summary, the conversation discusses the use of integration to solve a function involving the Fermi integral and the Stefan-Boltzmann law. Various methods, such as partial integration and infinite series, are suggested. The conversation also touches on the difficulty of viewing LaTeX graphics, and the importance of changing integration limits when substituting variables. The final solution involves a product of the Riemann zeta function and the gamma function.
  • #1
P3X-018
"Simple" integral

Hey. I'm having problems with integrating the following function:

http://www.mainboard.dk/upload/files/Math.bmp

I used partial integration (if it's called that in english?), and end up with the same term. In equation (1.2) I just tried to integrate the middle term in (1.1), and as you can see it didn't work with parial integration. How do I then solve it?
By the way, I'm not on higher education, only in "senior high school". So it would best if you could show how you get to the solution.
 
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  • #2
well you alreaedy beat me by integrating 1/(e^x-1) but axxording to my basic philosophy of "make the rpoblem easier" you might try just doing x/[e^x-1].

or use infinite series as a last resort.
 
  • #3
No, I can't just do x/((e^x) -1)). I need the first value, in calculating stefan-boltzmanns law. But I don't know anything about integrating by use of the infinite series.
 
  • #4
The integral is called a Fermi integral. Look up the general form, the solution is a product of the Riemann zeta function and the gamma function.

[tex] \int^{\inf} _{0} \frac{x^{n-1}}{e^{x} - 1} dx = \Gamma (n) \zeta (n) [/tex]
 
  • #5
Why am I unable to see the latex graphic? It keeps saying: "LaTeX graphic is being generated. Reload this page in a moment."
And it's not helping by refreshing the page.
 
  • #6
My phyiscs professor in my first year at the university derived the Stefan-Boltzman law the same way you are trying to do from the Planck's BB radiation formula. He made the same substitution but on encountering the integral you mention he said "this is just the area undre a certain curve which can be shown to be [itex]\pi^4 / 15 [/itex]". I guess it's quite a tricky integral...
 
  • #7
Yea, I know it's 6,49 (pi^4/15). You can calculate the area, on the calculator, but I just wanted to know how you get to the solution. Well Dr Transport tells also how to solve it. But I can't see the latex graphic. Why? Is it because you've writin the command wrong?? Would you pls rewrite it again (not the last one, which is pi^4/15). I would appreciate that!
 
  • #8
Now we are talking about the substitution, I got the value -2pi(kT)^4. but shouldn't it be with af positive sign??
 
  • #9
I'm not sure what you mean, what value is that you got there?

The final answer is the intensity of the radiation is: [itex]I=\sigma T^4[/itex] (with [itex]\sigma[/itex] the stefan Boltzman constant. This constant turns out to be not fundamental if you work everything out:

[tex]\sigma = \frac{2 k^4 \pi^5}{15 h^3 c^2}[/tex]

The easiest way is to substitute [itex]x= hc/ \lambda kT[/itex] when integrating Plancks law over all wavelengths (now x) to get the total intensity (Stefan-Boltzmann law).

Note: You can see the latex code if you click on the (nongenerated) latex image
 
  • #10
Yes I know that da willem (check the link at #1). But I mean that after the substitution i get a negative value. (See the attached document). Can you tell why I get a negativ value (-kT)?
Or is it supposed to be negativ?
 

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  • #11
You get the minus sign from the differential d(lambda)=-(hc/kT)x^-2 dx. But you forgot to cancel it with the minus introduced by changing your integration limits.
 
  • #12
The LateX graphics have had some trouble since the server switch the other day. If you look at what was written, the general formula has been given. The problem is being fixed.

dt
 
  • #13
Phew I was wondering about what was going wrong with the TeX--- I thought it was just something I was experiencing, nice to know that that is indeed not the case.
 
  • #14
Ok. I thougt the same as Theelectricchild, that it was only me who was experiencing that!

By the way "da willem" what do you mean by "changing the integration limits"? Where do you change it? I mean you can't just change them.
 
  • #15
You have to integrate the wavelength from 0 to infinity. You made the substitution x= hc/ (wavelength)kT. So when the wavelength goes from 0 to infinity, x goes from infinity to 0 (because of the inverse relation between x and the wavelength). So you have to change your integration limits from (from 0 to infinity) to (from infinity to zero). You evaluated the integral from 0 to infinity where you should have evaluated from infinity to zero...

Thisis allowed; but you have to take into account another minus sign which you forgot. Because:

[tex] \int _a^b f(t) dt = - \int _b^a f(t) dt [/tex]

Got it?
 
  • #16
Yea I got ya. Well, thanks for help :)
 
  • #17
let's try this again

[tex] \int^{\infty} _{0} \frac{x^{n-1}}{e^{x} - 1} dx = \Gamma (n) \zeta (n) [/tex]
 

FAQ: How do I solve this integral using partial integration?

What is a simple integral?

A simple integral is a mathematical concept used in calculus to calculate the area under a curve. It is represented by the symbol ∫ and is commonly used to find the total value of a function within a given range.

How do you solve a simple integral?

To solve a simple integral, you first need to identify the function and the limits of integration. Then, you can use various techniques such as substitution, integration by parts, or trigonometric identities to simplify the integral and solve for the value.

What is the difference between a definite and indefinite simple integral?

A definite simple integral has specific limits of integration, while an indefinite simple integral does not. This means that a definite integral will give you a specific numerical value, while an indefinite integral will give you a function that represents the area under the curve.

What are some real-life applications of simple integrals?

Simple integrals have many real-life applications, such as calculating the distance traveled by an object with varying velocity, finding the area under a demand curve in economics, and determining the amount of medication in a patient's bloodstream over time.

What are some common techniques for evaluating simple integrals?

Some common techniques for evaluating simple integrals include substitution, integration by parts, trigonometric identities, and partial fractions. It is important to understand and practice these techniques in order to solve more complex integrals.

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