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Given that \(y=\sum_{n=0}^{\infty} n x^{n},\) compute \(y^{\prime}\) and \(y^{\prime \prime}\) and write out the first four terms of each series as well as the coefficient of \(x^{n}\) in the general term.

Short Answer

Expert verified
Question: Write down the first four terms and the general term for the first and second derivatives of the power series \(y=\sum_{n=0}^{\infty} nx^n\). Answer: For the first derivative \(y'\): The first four terms are \(0 + 0 + 2x + 6x^2\) and the general term is given by \(y'= \sum_{n=0}^{\infty} n(n-1)x^{n-1}\). For the second derivative \(y''\): The first four terms are \(0 + 0 + 0 + 6x\) and the general term is given by \(y''= \sum_{n=0}^{\infty} n(n-1)(n-2)x^{n-2}\).

Step by step solution

01

Find the general formula for the first derivative \(y'\)

To find the derivative of a power series, we can take the derivative of each term in the series and sum them up. The derivative of the general term \(n x^n\) is obtained using the power rule for differentiation: \((n x^n)' = n(n-1)x^{n-1}\). The series \(y'\) will be given by: $$ y'=\sum_{n=0}^{\infty}n(n-1)x^{n-1} $$
02

Find the first four terms of the first derivative \(y'\)

Now, let's calculate the first four terms of the series \(y'\). When \(n=0\): $$ 0(0-1)x^{-1} = 0 $$ When \(n=1\): $$ 1(1-1)x^{1-1} = 0 $$ When \(n=2\): $$ 2(2-1)x^{2-1} = 2x $$ When \(n=3\): $$ 3(3-1)x^{3-1} = 6x^2 $$ So, the first four terms of the series are: $$ y' = 0 + 0 + 2x + 6x^2 + \cdots $$ The general term for the first derivative is: $$ y'= \sum_{n=0}^{\infty} n(n-1)x^{n-1} $$
03

Find the general formula for the second derivative \(y''\)

We will apply the same method we used in step 1 to the first derivative: take the derivative of each term in the series and sum them up. The derivative of the general term \(n(n-1)x^{n-1}\) is \((n(n-1)x^{n-1})' = n(n-1)(n-2)x^{n-2}\). The series \(y''\) will be given by: $$ y''=\sum_{n=0}^{\infty}n(n-1)(n-2)x^{n-2} $$
04

Find the first four terms of the second derivative \(y''\)

Now let's calculate the first four terms of the series \(y''\). When \(n=0\): $$ 0(0-1)(0-2)x^{-2} = 0 $$ When \(n=1\): $$ 1(1-1)(1-2)x^{1-2} = 0 $$ When \(n=2\): $$ 2(2-1)(2-2)x^{2-2} = 0 $$ When \(n=3\): $$ 3(3-1)(3-2)x^{3-2} = 6x $$ So, the first four terms of the series are: $$ y'' = 0 + 0 + 0 + 6x + \cdots $$ The general term for the second derivative is: $$ y''= \sum_{n=0}^{\infty} n(n-1)(n-2)x^{n-2} $$ In conclusion, the first derivative \(y'\) is given by: $$ y' = 0 + 0 + 2x + 6x^2 + \cdots = \sum_{n=0}^{\infty} n(n-1)x^{n-1} $$ And the second derivative \(y''\) is given by: $$ y'' = 0 + 0 + 0 + 6x + \cdots = \sum_{n=0}^{\infty} n(n-1)(n-2)x^{n-2} $$

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Most popular questions from this chapter

The Legendre Equation. Problems 22 through 29 deal with the Legendre equation $$ \left(1-x^{2}\right) y^{\prime \prime}-2 x y^{\prime}+\alpha(\alpha+1) y=0 $$ As indicated in Example \(3,\) the point \(x=0\) is an ordinaty point of this equation, and the distance from the origin to the nearest zero of \(P(x)=1-x^{2}\) is 1 . Hence the radius of convergence of series solutions about \(x=0\) is at least 1 . Also notice that it is necessary to consider only \(\alpha>-1\) because if \(\alpha \leq-1\), then the substitution \(\alpha=-(1+\gamma)\) where \(\gamma \geq 0\) leads to the Legendre equation \(\left(1-x^{2}\right) y^{\prime \prime}-2 x y^{\prime}+\gamma(\gamma+1) y=0\) It can be shown that the general formula for \(P_{n}(x)\) is $$ P_{n}(x)=\frac{1}{2^{n}} \sum_{k=0}^{\ln / 2-} \frac{(-1)^{k}(2 n-2 k) !}{k !(n-k) !(n-2 k) !} x^{n-2 k} $$ where \([n / 2]\) denotes the greatest integer less than or equal to \(n / 2 .\) By observing the form of \(P_{n}(x)\) for \(n\) even and \(n\) odd, show that \(P_{n}(-1)=(-1)^{n} .\)

The Legendre Equation. Problems 22 through 29 deal with the Legendre equation $$ \left(1-x^{2}\right) y^{\prime \prime}-2 x y^{\prime}+\alpha(\alpha+1) y=0 $$ As indicated in Example \(3,\) the point \(x=0\) is an ordinaty point of this equation, and the distance from the origin to the nearest zero of \(P(x)=1-x^{2}\) is 1 . Hence the radius of convergence of series solutions about \(x=0\) is at least 1 . Also notice that it is necessary to consider only \(\alpha>-1\) because if \(\alpha \leq-1\), then the substitution \(\alpha=-(1+\gamma)\) where \(\gamma \geq 0\) leads to the Legendre equation \(\left(1-x^{2}\right) y^{\prime \prime}-2 x y^{\prime}+\gamma(\gamma+1) y=0\) Show that two linearly independent solutions of the Legendre equation for \(|x|<1\) are $$ \begin{aligned} y_{1}(x)=& 1+\sum_{m=1}^{\infty}(-1)^{m} \\ & \times \frac{\alpha(\alpha-2)(\alpha-4) \cdots(\alpha-2 m+2)(\alpha+1)(\alpha+3) \cdots(\alpha+2 m-1)}{(2 m) !} x^{2 m} \\ y_{2}(x)=& x+\sum_{m=1}^{\infty}(-1)^{m} \\ & \times \frac{(\alpha-1)(\alpha-3) \cdots(\alpha-2 m+1)(\alpha+2)(\alpha+4) \cdots(\alpha+2 m)}{(2 m+1) !} x^{2 m+1} \end{aligned} $$

Use the results of Problem 21 to determine whether the point at infinity is an ordinary point, a regular singular point, or an irregular singular point of the given differential equation. \(y^{\prime \prime}-2 x y^{\prime}+\lambda y=0, \quad\) Hermite equation

First Order Equations. The series methods discussed in this section are directly applicable to the first order linear differential equation \(P(x) y^{\prime}+Q(x) y=0\) at a point \(x_{0}\), if the function \(p=Q / P\) has a Taylor series expansion about that point. Such a point is called an ordinary point, and further, the radius of convergence of the series \(y=\sum_{n=0}^{\infty} a_{n}\left(x-x_{0}\right)^{n}\) is at least as large as the radius of convergence of the series for \(Q / P .\) In each of Problems 16 through 21 solve the given differential equation by a series in powers of \(x\) and verify that \(a_{0}\) is arbitrary in each case. Problems 20 and 21 involve nonhomogeneous differential equations to which series methods can be easily extended. Where possible, compare the series solution with the solution obtained by using the methods of Chapter 2 . $$ y^{\prime}=e^{x^{2}} y, \quad \text { three terms only } $$

First Order Equations. The series methods discussed in this section are directly applicable to the first order linear differential equation \(P(x) y^{\prime}+Q(x) y=0\) at a point \(x_{0}\), if the function \(p=Q / P\) has a Taylor series expansion about that point. Such a point is called an ordinary point, and further, the radius of convergence of the series \(y=\sum_{n=0}^{\infty} a_{n}\left(x-x_{0}\right)^{n}\) is at least as large as the radius of convergence of the series for \(Q / P .\) In each of Problems 16 through 21 solve the given differential equation by a series in powers of \(x\) and verify that \(a_{0}\) is arbitrary in each case. Problems 20 and 21 involve nonhomogeneous differential equations to which series methods can be easily extended. Where possible, compare the series solution with the solution obtained by using the methods of Chapter 2 . $$ y^{\prime}-y=x^{2} $$

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