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Exercises \(31-36\) treat the equations considered in Examples \(5.4 .1-5.4 .6 .\) Substitute the suggested form of \(y_{p}\) into the equation and equate the resulting coefficients of like functions on the two sides of the resulting equation to derive a set of simultaneous equations for the coefficients in \(y_{p}\). Then solve for the coefficients to obtain \(y_{p}\). Compare the work you've done with the work required to obtain the same results in Examples \(5.4 .1-5.4 .6 .\) Write \(y=u e^{\alpha x}\) to find the general solution. (a) \(y^{\prime \prime}+2 y^{\prime}+y=\frac{e^{-x}}{\sqrt{x}}\) (b) \(y^{\prime \prime}+6 y^{\prime}+9 y=e^{-3 x} \ln x\) (c) \(y^{\prime \prime}-4 y^{\prime}+4 y=\frac{e^{2 x}}{1+x}\) (d) \(4 y^{\prime \prime}+4 y^{\prime}+y=4 e^{-x / 2}\left(\frac{1}{x}+x\right)\)

Short Answer

Expert verified
Question: Find the general solution for the given second-order linear differential equation: \(y'' + 2y' + y = xe^{-x}\) Solution: #Step 1: Guessing the particular solution# For this equation, we can guess the particular solution in the following form: \(y_p = (Ax^2+Bx) e^{-x}\) #Step 2: Finding the derivatives and substituting in the equation# First find the first and second derivatives of \(y_p\) and substitute them into the given equation: \(y_p' = ((2Ax+B)x - (Ax^2+Bx)) e^{-x}\) \(y_p'' = (2A - (4Ax+2B)x + (Ax^2+Bx)) e^{-x}\) Substituting \(y_p\), \(y_p'\), and \(y_p''\) into the given equation, we get: \((2A - (4Ax+2B)x + (Ax^2+Bx)) e^{-x} + 2((2Ax+B)x - (Ax^2+Bx)) e^{-x} + (Ax^2+Bx) e^{-x} = xe^{-x}\) #Step 3: Equating coefficients and solving for the unknowns# Now we'll equate the coefficients of like functions on both sides: Comparing the coefficients of \(x^2 e^{-x}\), we have: \(A + 0 - A = 0\) Comparing the coefficients of \(x e^{-x}\), we have: \(B + 2A - 2B = 1\) Comparing the coefficients of \(e^{-x}\), we have: \(2A - 4A = 0\) Solving for A and B, we get \(A = \frac{1}{2}\) and \(B = 1\) The particular solution will be \(y_p = (\frac{1}{2}x^2+x) e^{-x}\) #Step 4: General solution using \(y=ue^{\alpha x}\)# Using the suggested form, we have the general solution to be: \(y(x) = ue^{\alpha x} + (\frac{1}{2}x^2+x) e^{-x}\)

Step by step solution

01

For this equation, we can guess the particular solution in the following form: \(y_p = Ax^r e^{-x}\) #Step 2: Finding the derivatives and substituting in the equation#

First find the first and second derivatives of \(y_p\) and substitute them into the given equation: \(y_p' = A[r x^{r - 1} e^{-x} - x^r e^{-x}]\) \(y_p'' = A[(r^2-r)x^{r-2}e^{-x} - 2(r-1)x^{r-1}e^{-x}+x^r e^{-x}]\) Substituting \(y_p\), \(y_p'\) and \(y_p''\) into the given equation, we get: \(A[(r^2-r)x^{r-2}e^{-x} - 2(r-1)x^{r-1}e^{-x}+x^r e^{-x}] + 2A[r x^{r - 1} e^{-x} - x^r e^{-x}] + Ax^r e^{-x} = \frac{e^{-x}}{\sqrt{x}}\) #Step 3: Equating coefficients and solving for the unknowns#
02

Now we'll equate the coefficients of like functions on both sides: Comparing the coefficients of \(x^r e^{-x}\), we have: \(A+2(-A)+A=0\) Solving for A, we get \(A=0\), which is a trivial solution, so our choice of \(y_p\) needs an adjustment Let's try a new form for \(y_p\) by including an extra factor of x: \(y_p = Ax^{r+1} e^{-x}\) Repeat Step 2 with this new form, and we obtain the following: \(A(r^2+3r+2)x^re^{-x} = \frac{e^{-x}}{\sqrt{x}}\) Comparing the coefficients of the like functions, we have: \(r^2 + 3r + 2 = 0\) \(r=-1, -2\) Since we want a fractional power for \(x\), we choose \(r=-\frac{1}{2}\) The particular solution will be \(y_p = Ax^{-1/2} e^{-x}\) #Step 4: General solution using \(y=ue^{\alpha x}\)#

Using the suggested form, we have the general solution to be: \(y(x) = ue^{\alpha x} + Ax^{-1/2} e^{-x}\) (a) Repeat these steps similarly to find the general solution for the remaining cases.

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Key Concepts

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

Particular Solution
The particular solution of a differential equation is a specific solution that satisfies not only the differential equation but also initial or boundary conditions. For instance, if we have a function like \(y'' + 2y' + y = \frac{e^{-x}}{\sqrt{x}}\), our task is to guess a form for \(y_p\), the particular solution, such as \(y_p = Ax^r e^{-x}\).

This guessed form should have similar terms to one or more terms on the right side of the equation. By substituting this guessed form into the differential equation and adjusting the parameters \(A\) and \(r\), we derive a solution that fits the specific non-homogeneous aspect of the equation.

The key point here is choosing a strategic form for \(y_p\), often involving terms present in the non-homogeneous part, to facilitate finding the correct parameters.
General Solution
The general solution of a differential equation combines the homogeneous solution and the particular solution. It accounts for all possible solutions including constants arising from integration.

For differential equations, this means solving \(y(x) = u e^{\alpha x} + y_p(x)\), where the first part \(u e^{\alpha x}\) represents the solution to the related homogeneous equation \(y'' + 2y' + y = 0\).

To find the general solution, determine the complementary function \(u e^{\alpha x}\) from the homogeneous part and add the particular solution \(y_p\) derived for the specific scenario. This combination yields all the potential solutions for the differential equation.
Simultaneous Equations
Simultaneous equations arise when we replace the guessed form of a particular solution into a differential equation. We then equate the like coefficients on both sides.

For example, inserting \(y_p = Ax^r e^{-x}\) and its derivatives into \(y'' + 2y' + y\) results in a series of expressions. By focusing on matching each term with the non-homogeneous part \(\frac{e^{-x}}{\sqrt{x}}\), we establish equations for unknown coefficients.

Solving these simultaneous equations uncovers parameter values such as \(A\) and \(r\) that satisfy the equation. This systematic approach is crucial for aligning our particular solution to the given differential problem.
Coefficient Matching
Coefficient matching is a method used in differential equations to determine unknown parameters within a proposed solution. Once we've substituted a trial solution into the differential equation, our goal is to align the resulting expressions with the equation's terms.

For our given function, after substituting \(y_p = Ax^r e^{-x}\) along with its derivatives, we analyze each term present. Matching each coefficient of powers of \(x\) and \(e^{-x}\) on both sides of the equation helps derive useful information about values like \(A\) and \(r\).

Through coefficient matching, the differential equation effectively guides the selection of correct parameters, ensuring our trial function accurately represents the equation's solution.

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Most popular questions from this chapter

In Exercises \(1-6\) use variation of parameters to find a particular solution. $$ y^{\prime \prime}+9 y=\tan 3 x $$

Find the general solution, given that \(y_{1}\) satisfies the complementary equation. As a byproduct, find a fundamental set of solutions of the complementary equation.

Use the principle of superposition to find a particular solution. Where indicated, solve the initial value problem. $$ y^{\prime \prime}-4 y^{\prime}+4 y=6 e^{2 x}+25 \sin x, \quad y(0)=5, y^{\prime}(0)=3 $$

Find a fundamental set of solutions, given that \(y_{1}\) is a solution. \(x^{2}(\ln |x|)^{2} y^{\prime \prime}-(2 x \ln |x|) y^{\prime}+(2+\ln |x|) y=0 ; \quad y_{1}=\ln |x|\)

In calculus you learned that \(e^{u}, \cos u,\) and \(\sin u\) can be represented by the infinite series $$ \begin{array}{c} e^{u}=\sum_{n=0}^{\infty} \frac{u^{n}}{n !}=1+\frac{u}{1 !}+\frac{u^{2}}{2 !}+\frac{u^{3}}{3 !}+\cdots+\frac{u^{n}}{n !}+\cdots \\ \cos u=\sum_{n=0}^{\infty}(-1)^{n} \frac{u^{2 n}}{(2 n) !}=1-\frac{u^{2}}{2 !}+\frac{u^{4}}{4 !}+\cdots+(-1)^{n} \frac{u^{2 n}}{(2 n) !}+\cdots, \end{array} $$ and $$ \sin u=\sum_{n=0}^{\infty}(-1)^{n} \frac{u^{2 n+1}}{(2 n+1) !}=u-\frac{u^{3}}{3 !}+\frac{u^{5}}{5 !}+\cdots+(-1)^{n} \frac{u^{2 n+1}}{(2 n+1) !}+\cdots $$ for all real values of \(u\). Even though you have previously considered (A) only for real values of \(u\), we can set \(u=i \theta,\) where \(\theta\) is real, to obtain $$ e^{i \theta}=\sum_{n=0}^{\infty} \frac{(i \theta)^{n}}{n !} $$ Given the proper background in the theory of infinite series with complex terms, it can be shown that the series in (D) converges for all real \(\theta\). (a) Recalling that \(i^{2}=-1,\) write enough terms of the sequence \(\left\\{i^{n}\right\\}\) to convince yourself that the sequence is repetitive: $$ 1, i,-1,-i, 1, i,-1,-i, 1, i,-1,-i, 1, i,-1,-i, \cdots $$ Use this to group the terms in (D) as $$ \begin{aligned} e^{i \theta} &=\left(1-\frac{\theta^{2}}{2}+\frac{\theta^{4}}{4}+\cdots\right)+i\left(\theta-\frac{\theta^{3}}{3 !}+\frac{\theta^{5}}{5 !}+\cdots\right) \\ &=\sum_{n=0}^{\infty}(-1)^{n} \frac{\theta^{2 n}}{(2 n) !}+i \sum_{n=0}^{\infty}(-1)^{n} \frac{\theta^{2 n+1}}{(2 n+1) !} \end{aligned} $$ In calculus you learned that \(e^{u}, \cos u,\) and \(\sin u\) can be represented by the infinite series $$ \begin{array}{c} e^{u}=\sum_{n=0}^{\infty} \frac{u^{n}}{n !}=1+\frac{u}{1 !}+\frac{u^{2}}{2 !}+\frac{u^{3}}{3 !}+\cdots+\frac{u^{n}}{n !}+\cdots \\ \cos u=\sum_{n=0}^{\infty}(-1)^{n} \frac{u^{2 n}}{(2 n) !}=1-\frac{u^{2}}{2 !}+\frac{u^{4}}{4 !}+\cdots+(-1)^{n} \frac{u^{2 n}}{(2 n) !}+\cdots, \end{array} $$ and $$ \sin u=\sum_{n=0}^{\infty}(-1)^{n} \frac{u^{2 n+1}}{(2 n+1) !}=u-\frac{u^{3}}{3 !}+\frac{u^{5}}{5 !}+\cdots+(-1)^{n} \frac{u^{2 n+1}}{(2 n+1) !}+\cdots $$ for all real values of \(u\). Even though you have previously considered (A) only for real values of \(u\), we can set \(u=i \theta,\) where \(\theta\) is real, to obtain $$ e^{i \theta}=\sum_{n=0}^{\infty} \frac{(i \theta)^{n}}{n !} $$ Given the proper background in the theory of infinite series with complex terms, it can be shown that the series in (D) converges for all real \(\theta\). (a) Recalling that \(i^{2}=-1,\) write enough terms of the sequence \(\left\\{i^{n}\right\\}\) to convince yourself that the sequence is repetitive: $$ 1, i,-1,-i, 1, i,-1,-i, 1, i,-1,-i, 1, i,-1,-i, \cdots $$ Use this to group the terms in (D) as $$ \begin{aligned} e^{i \theta} &=\left(1-\frac{\theta^{2}}{2}+\frac{\theta^{4}}{4}+\cdots\right)+i\left(\theta-\frac{\theta^{3}}{3 !}+\frac{\theta^{5}}{5 !}+\cdots\right) \\ &=\sum_{n=0}^{\infty}(-1)^{n} \frac{\theta^{2 n}}{(2 n) !}+i \sum_{n=0}^{\infty}(-1)^{n} \frac{\theta^{2 n+1}}{(2 n+1) !} \end{aligned} $$ (c) If \(\alpha\) and \(\beta\) are real numbers, define $$ e^{\alpha+i \beta}=e^{\alpha} e^{i \beta}=e^{\alpha}(\cos \beta+i \sin \beta) $$ Show that if \(z_{1}=\alpha_{1}+i \beta_{1}\) and \(z_{2}=\alpha_{2}+i \beta_{2}\) then $$ e^{z_{1}+z_{2}}=e^{z_{1}} e^{z_{2}} $$ (d) Let \(a, b,\) and \(c\) be real numbers, with \(a \neq 0 .\) Let \(z=u+i v\) where \(u\) and \(v\) are real-valued functions of \(x .\) Then we say that \(z\) is a solution of $$ a y^{\prime \prime}+b y^{\prime}+c y=0 $$ if \(u\) and \(v\) are both solutions of (G). Use Theorem \(5.2 .1(\mathbf{c})\) to verify that if the characteristic equation of (G) has complex conjugate roots \(\lambda \pm i \omega\) then \(z_{1}=e^{(\lambda+i \omega) x}\) and \(z_{2}=e^{(\lambda-i \omega) x}\) are both solutions of (G).

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