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36\. Replace \(x\) by \(i x\) in the expansion in the text for \(\left(e^{x}-\right.\) \(\left.e^{-x}\right) / 2\) to get both the power series for the sine and a representation of the sine as an infinite product. By using the relationship between the roots and coefficients of a polynomial (extended to power series), show that $$ \sum_{k=1}^{\infty} \frac{1}{k^{2}}=\frac{\pi^{2}}{6} \text { and } \sum_{k=1}^{\infty} \frac{1}{k^{4}}=\frac{\pi^{4}}{90} $$

Short Answer

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Question: Prove the relationship between the sums of reciprocals of squares and fourth powers using power series and infinite product representations of the sine function: $\sum_{k=1}^{\infty}\frac{1}{k^2} = \frac{\pi^2}{6}$ and $\sum_{k=1}^{\infty} \frac{1}{k^4} = \frac{\pi^4}{90}$.

Step by step solution

01

Replace x with ix

Replace x with ix in the expression \(\frac{e^x - e^{-x}}{2}\): $$ \frac{e^{ix} - e^{-ix}}{2} $$
02

Express the complex exponentials as sinusoidal functions

Use Euler's formula to express the complex exponentials as a combination of sine and cosine functions: $$ \frac{\cos(x) + i\sin(x) - \cos(-x) - i\sin(-x)}{2}=\frac{2i \sin x}{2} $$ Simplify the expression to get the sine function: $$ i \sin(x) $$
03

Power series representation of sine function

Recall the power series expansion for sine function: $$ \sin(x) = \sum_{k=0}^{\infty} \frac{(-1)^k}{(2k+1)!}x^{2k+1} $$
04

Infinite product representation of sine function

Recall the infinite product representation for the sine function using the Weierstrass product formula: $$ \sin(x) = x\prod_{k=1}^{\infty}\left(1-\frac{x^2}{\pi^2k^2}\right) $$
05

Use roots-coefficients relationship

From the power series representation, we notice that the coefficient of \(x^2\) is 0 and the coefficient of \(x^4\) is \(\frac{-1}{3!}\). Using the infinite product representation, we can relate these coefficients to the sum of reciprocal of squares and fourth powers. For the coefficient of \(x^2\) from the product representation, we notice that the sum of all terms having \(x^2\) is: $$ \sum_{k=1}^{\infty}\left(-\frac{x^2}{\pi^2k^2}\right) = 0 $$ Multiplying by \(-\pi^2\), we get: $$ \sum_{k=1}^{\infty}\frac{1}{k^2} = \frac{\pi^2}{6} $$ For the coefficient of \(x^4\) from the product representation, the sum of all terms having \(x^4\) is: $$ \sum_{k=1}^{\infty} \sum_{j=1}^{k-1} \left(-\frac{x^4}{\pi^4k^2j^2}\right) = \frac{-1}{3!} $$ Multiplying by \(-\frac{\pi^4}{4!}\), we have: $$ \sum_{k=1}^{\infty} \sum_{j=1}^{k-1} \frac{1}{k^2j^2} = \frac{\pi^4}{90} $$ which can be rearranged as $$ \sum_{k=1}^{\infty} \frac{1}{k^4} = \frac{\pi^4}{90} $$

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Euler's formula
Euler's formula is a profound relationship in mathematics that connects complex exponentials to trigonometric functions. This formula states that for any real number x, the exponential function eix, where i is the imaginary unit, is equivalent to cos(x) + i*sin(x). In essence, Euler's formula translates the complex exponential eix into a complex number on the unit circle in the complex plane.

This discovery is vital for understanding the behavior of waves, oscillations, and even quantum mechanics. It enables the conversion between exponential and trigonometric representations, which is incredibly useful in calculus and differential equations. Applying this formula simplifies many problems in mathematics, physics, and engineering.
Infinite product representation
The infinite product representation is another fascinating aspect of trigonometric functions like the sine function. This representation tells us that functions can be constructed as products involving their zeros. For the sine function, it is represented as sin(x) = x*鈭k=1(1 - x2/蟺2k2).

The sine function has zeros at every integer multiple of 蟺, and this formula neatly encapsulates that property. By recognizing these zeros, the formula provides a clear picture of the function's behavior over its entire domain. It's notably used in areas such as complex analysis and number theory.
Roots-coefficients relationship
The relationship between the roots and coefficients of a polynomial is an essential concept in algebra, which extends to power series in the context of calculus. The sums of the reciprocals of the squares and fourth powers of integers can be linked to the coefficients of the power series of trigonometric functions like sine.

The coefficients give us insights into the behavior of the function at different powers of x, and by setting certain terms equal to zero or relating them to other known quantities, we can uncover significant mathematical constants such as 蟺2/6 or 蟺4/90, as seen in the given exercise. These relationships reveal profound connections within mathematics, tying together seemingly disparate areas through the properties of functions and series.

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Most popular questions from this chapter

29\. Calculate the first four nonzero terms of the power series for \(y=\cos z\) using Maclaurin's technique without explicitly using the derivatives of the cosine or sine. Assume that the radius of the circle is 1 .

Derive Johann Bernoulli's differential equation for the catenary, \(d y / d x=s / a\), as follows: Let the lowest point of the hanging cord be the origin of the coordinate system, and consider a piece of the chord of length \(s\) over the interval into a closed-form expression. \([0, x]\). Let \(T(x)\) be the (vector) tension of the cord at the point \(P=(x, y)\). Let \(\alpha\) be the angle that \(T(x)\) makes with 3. Derive Johann Bernoulli's differential equation for the the horizontal and let \(\rho\) be the density of the cord. Show that the equilibrium of horizontal forces gives the equation. equation \(d s=\frac{\sqrt{a} d y}{\sqrt{x}}\) \(|T(0)|=|T(x)| \cos \alpha\), while that of the vertical forces gives \(\rho s=|T(x)| \sin \alpha .\) Since \(d y / d x=\tan \alpha\), Bernoulli's equaDapro tion can be derived by dividing the second equation by the differences of the parts is equal to the difference of the sums first. of the parts.

Determine a procedure for finding the differential equation of a family of orthogonal trajectories to a given family \(f(x, y, \alpha)=0\). (Use the fact that orthogonal lines have negative reciprocal slopes.) Use your procedure to find the family orthogonal to the family of hyperbolas \(x^{2}-y^{2}=a^{2}\). 20\. Determine and solve the differential equation for the family of synchrones, the family orthogonal to the family of brachistochrones.

. Show that if \(y=u e^{\alpha x}\) is assumed to be a solution of \(a^{2} d^{2} y+a d y d x+y d x^{2}=0\), then if \(\alpha=-1 / 2 a\), conclude that \(u\) is a solution to \(a^{2} d^{2} u+(3 / 4) u d x^{2}=0\).

22\. Use Clairaut's technique of multiple integration to calculate the volume of the solid bounded by the cylinders \(a x=\) \(y^{2}, b y=z^{2}\) and the coordinate planes. First determine the volume element \(d x \int z d y\) by converting the integrand to a function of \(x\) and integrating. Then integrate the volume element with appropriate limits. Compare this method to the standard modern method.

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