How to Prove the Integral Result Equals ln(2) - ζ(2)/4?

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In summary: Now, we can use the substitution $v = \ln u$ to rewrite the integral as:$$8\pi\int_{-\infty}^{0}{(1+e^v)\cdot v^4\over [\pi^2+v^2]^2}\mathrm dv$$Finally, using the identities $\zeta(2) = \pi^2/6$ and $\ln2 = \int_{0}^{1
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Tony1
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How to show that,

$$8\pi\int_{0}^{\pi/2}\cos^2x\cdot{\ln^2(\tan^2 x)\over [\pi^2+\ln^2(\tan^2 x)]^2}\mathrm dx=\ln 2-{1\over 4}\zeta(2)$$
 
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To show this, we can use the properties of logarithms and trigonometric identities to simplify the integrand.

First, we can rewrite the integrand as:

$$\cos^2x\cdot{\ln^2(\tan^2 x)\over [\pi^2+\ln^2(\tan^2 x)]^2} = {\cos^2x\cdot\ln^2(\sin^2x)\over [\pi^2+\ln^2(\sin^2x)]^2}$$

Next, we can use the identity $\ln(\sin^2x) = 2\ln(\sin x)$ to simplify the expression further:

$$ {\cos^2x\cdot\ln^2(\sin^2x)\over [\pi^2+\ln^2(\sin^2x)]^2} = {\cos^2x\cdot[2\ln(\sin x)]^2\over [\pi^2+[2\ln(\sin x)]^2]^2}$$

Now, we can use the double angle formula for cosine to rewrite $\cos^2x$ as $(1+\cos2x)/2$:

$${\cos^2x\cdot[2\ln(\sin x)]^2\over [\pi^2+[2\ln(\sin x)]^2]^2} = {(1+\cos2x)\cdot[2\ln(\sin x)]^2\over [\pi^2+[2\ln(\sin x)]^2]^2}$$

Using the identity $\ln(\sin x) = -\ln(\cos x)$, we can rewrite the expression as:

$$ {(1+\cos2x)\cdot[2\ln(\cos x)]^2\over [\pi^2+[2\ln(\cos x)]^2]^2}$$

Now, we can use the substitution $u = \cos x$ to change the limits of integration and rewrite the integral as:

$$8\pi\int_{0}^{1}{(1+u)\cdot[2\ln u]^2\over [\pi^2+[2\ln u]^2]^2}\mathrm du$$

Using the power rule for logarithms, we can simplify the expression further:

$$8\pi\int_{0}^{1}{(1+u)\cdot[2\ln u]^2\over
 

FAQ: How to Prove the Integral Result Equals ln(2) - ζ(2)/4?

1. What is the significance of the result integral ln2−ζ(2)/4?

The result integral ln2−ζ(2)/4, also known as the Euler-Mascheroni constant, is a mathematical constant that appears in various areas of mathematics and physics. It is closely related to the natural logarithm of 2 and the Riemann zeta function. It is also used in the study of prime numbers and the distribution of prime numbers.

2. How is the result integral ln2−ζ(2)/4 calculated?

The result integral ln2−ζ(2)/4 can be calculated using various methods such as the Euler-Maclaurin formula, the Cauchy integral formula, and the Fourier transform. These methods involve complex mathematical techniques and are beyond the scope of this answer, but they are based on the properties of the natural logarithm and the Riemann zeta function.

3. What is the relationship between the result integral ln2−ζ(2)/4 and the Riemann zeta function?

The result integral ln2−ζ(2)/4 is closely related to the Riemann zeta function, which is defined as ζ(s) = ∑(n=1 to ∞) 1/ns. In fact, the result integral can be expressed as a multiple of the Riemann zeta function, specifically ln2−ζ(2)/4 = ζ(2)/2 = π^2/12. This relationship is important in the study of the distribution of prime numbers.

4. How is the result integral ln2−ζ(2)/4 used in physics?

The result integral ln2−ζ(2)/4 has various applications in physics, particularly in quantum field theory and statistical mechanics. It appears in the calculation of the vacuum energy density, and it is also used in the study of phase transitions and critical phenomena. It has also been used in the calculation of the Casimir effect, which is a phenomenon in quantum physics.

5. Can the result integral ln2−ζ(2)/4 be generalized to other values?

Yes, the result integral ln2−ζ(2)/4 can be generalized to other values using the Riemann zeta function, which allows for the calculation of the result integral for any even integer. For example, the result integral for 4 can be expressed as ζ(4)/4 = π^4/90. However, the result integral for odd integers cannot be calculated using this method.

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