Find a closed form interpretation for the integral :

Click For Summary
SUMMARY

The integral $\displaystyle \int^{\infty}_0 \, \frac{\log (1+e^{ax})}{1+e^{bx}}\, dx$ can be transformed using the substitution $u=bx$, leading to $\frac{1}{b} \int_{0}^{\infty} \frac{\ln(1+e^{au/b})}{1+e^{u}}\,du$. Further manipulation introduces symmetry and factors out $e^{au/(2b)}$, resulting in a more complex expression involving hyperbolic functions. The discussion suggests that while some parts of the integral are tractable, others remain challenging, and numerical integration may be a viable approach if the values of $a$ and $b$ are known.

PREREQUISITES
  • Understanding of integral calculus, particularly improper integrals.
  • Familiarity with logarithmic and hyperbolic functions.
  • Knowledge of substitution techniques in integration.
  • Experience with numerical integration methods.
NEXT STEPS
  • Explore advanced techniques in integral calculus, focusing on improper integrals.
  • Study the properties and applications of hyperbolic functions in integrals.
  • Learn about numerical integration methods, such as Simpson's rule and the trapezoidal rule.
  • Investigate power series expansions and their use in evaluating integrals.
USEFUL FOR

Mathematicians, physicists, and students engaged in advanced calculus or mathematical analysis, particularly those interested in evaluating complex integrals and numerical methods.

alyafey22
Gold Member
MHB
Messages
1,556
Reaction score
2
$\displaystyle \int^{\infty}_0 \, \frac{\log (1+e^{ax})}{1+e^{bx}}\, dx $​

I am not sure whether it can be solved :confused:
 
Physics news on Phys.org
I don't know if there are any constraints on $b$ and $a$, but here's an idea or two:

1. Let $u=bx$. Let's assume $b>0$. Then you have $du=b\,dx$, and the integral becomes
$$ \frac{1}{b} \int_{0}^{ \infty} \frac{ \ln(1+e^{au/b})}{1+e^{u}}\,du.$$

Next, you can introduce symmetry where there isn't by factoring out, up top, a $e^{au/(2b)}$, which gets you
$$ \int= \frac{1}{b} \int_{0}^{ \infty} \frac{ \ln(e^{au/(2b)}(e^{-au/(2b)}+e^{au/(2b)}))}{e^{u/2}(e^{-u/2}+e^{u/2})}\,du
= \frac{1}{b} \int_{0}^{ \infty} \frac{ (au/(2b))+\ln(e^{-au/(2b)}+e^{au/(2b)})}{e^{u/2}(e^{-u/2}+e^{u/2})}\,du$$
$$=\frac{1}{2b} \int_{0}^{ \infty} \frac{ (au/(2b))+ \ln(2 \cosh(au/(2b)))}{e^{u/2} \cosh(u/2)}\,du=\frac{1}{2b} \int_{0}^{ \infty} \frac{ (au/(2b))+ \ln(2)+ \ln( \cosh(au/(2b)))}{e^{u/2} \cosh(u/2)}\,du.$$
You could break that up into three integrals. The middle one is tractable, actually. The outer two are still problematic.

That's about as far as I can go. Perhaps someone else has other ideas? Or could run with these?

Naturally, if you know what $a$ and $b$ are, you could integrate numerically. I think the integrals will likely converge, as the original denominator will dominate the numerator significantly.
 
Today I tried and got a reduced more promising to solve integral :

$\displaystyle \int^1_0 \, \frac{\log \left(t^{\frac{a}{b}}+1 \right)}{t+1}\, dt$

A power-series expansion looked for the first glance the first way to go ... :rolleyes:
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 29 ·
Replies
29
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
Replies
2
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 6 ·
Replies
6
Views
3K