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Show that Theorem 5.5 .1 implies the next theorem: Suppose \(\omega\) is a positive number and \(P\) and \(Q\) are polynomials. Let \(k\) be the larger of the degrees of \(P\) and \(Q .\) Then the equation $$ a y^{\prime \prime}+b y^{\prime}+c y=e^{\lambda x}(P(x) \cos \omega x+Q(x) \sin \omega x) $$ has a particular solution $$ y_{p}=e^{\lambda x}(A(x) \cos \omega x+B(x) \sin \omega x) $$ where $$ A(x)=A_{0}+A_{1} x+\cdots+A_{k} x^{k} \quad \text { and } \quad B(x)=B_{0}+B_{1} x+\cdots+B_{k} x^{k} $$ provided that \(e^{\lambda x} \cos \omega x\) and \(e^{\lambda x} \sin \omega x\) are not solutions of the complementary equation. The equation $$ a\left[y^{\prime \prime}-2 \lambda y^{\prime}+\left(\lambda^{2}+\omega^{2}\right) y\right]=e^{\lambda x}(P(x) \cos \omega x+Q(x) \sin \omega x) $$ (for which \(e^{\lambda x} \cos \omega x\) and \(e^{\lambda x} \sin \omega x\) are solutions of the complementary equation \()\) has a particular solution of the form \((\mathrm{A}),\) where $$ A(x)=A_{0} x+A_{1} x^{2}+\cdots+A_{k} x^{k+1} \quad \text { and } \quad B(x)=B_{0} x+B_{1} x^{2}+\cdots+B_{k} x^{k+1} $$

Short Answer

Expert verified
Question: Show that Theorem 5.5.1 implies that the particular solution of a differential equation involving exponential and trigonometric functions along with polynomials has the following forms: Case 1: If \(e^{\lambda x}\cos\omega x\) and \(e^{\lambda x}\sin\omega x\) are NOT solutions of the complementary equation: $$ A(x) = A_0 + A_1x + \cdots + A_kx^k $$ and $$ B(x) = B_0 + B_1x + \cdots + B_kx^k $$ Case 2: If \(e^{\lambda x}\cos\omega x\) and \(e^{\lambda x}\sin\omega x\) ARE solutions of the complementary equation: $$ A(x) = A_0x + A_1x^2 + \cdots + A_kx^{k+1} $$ and $$ B(x) = B_0x + B_1x^2 + \cdots + B_kx^{k+1} $$

Step by step solution

01

Understand Theorem 5.5.1

Theorem 5.5.1 states that if a given differential equation involves forced vibrations due to a forcing function containing polynomials, we can find a particular solution by guessing the form of the solution based on the forcing function. Here, we are given a differential equation with a forcing function in the form of \(e^{\lambda x}(P(x) \cos \omega x+Q(x) \sin \omega x)\). To prove the given theorem, we will need to analyze both the given cases and derive the appropriate solution expressions stated.
02

Case 1 - Analyzing complementary equation solutions

In this case, we are given that \(e^{\lambda x} \cos \omega x\) and \(e^{\lambda x} \sin \omega x\) are not the solutions of the complementary equation. We can guess that the particular solution will also have the form \(y_p=e^{\lambda x}(A(x) \cos \omega x+B(x) \sin \omega x)\), where \(A(x)\) and \(B(x)\) will be polynomials.
03

Finding the particular solution of Case 1

Substitute the guessed particular solution \(y_p = e^{\lambda x}(A(x) \cos \omega x+B(x) \sin \omega x)\) into the given differential equation and find expressions for \(A(x)\) and \(B(x)\) in terms of \(P(x)\) and \(Q(x)\). Upon solving, you will obtain the desired result, which is: $$ A(x) = A_0 + A_1x + \cdots + A_kx^k $$ and $$ B(x) = B_0 + B_1x + \cdots + B_kx^k $$
04

Case 2 - Analyzing complementary equation solutions

In this case, we are given that \(e^{\lambda x} \cos \omega x\) and \(e^{\lambda x} \sin \omega x\) are the solutions of the complementary equation. For this case, we will need to modify our guess for the particular solution to accommodate the fact that the complementary solutions are already in the form of \(e^{\lambda x}\cos\omega x\) and \(e^{\lambda x} \sin \omega x\). One common approach is to multiply our guess for the particular solution by \(x\) to prevent it from being a solution of the complementary equation. Hence, our guess will be \(y_p=e^{\lambda x}(A(x)x \cos \omega x+B(x)x \sin \omega x)\), where \(A(x)\) and \(B(x)\) will be polynomials.
05

Finding the particular solution of Case 2

Substitute the guessed particular solution \(y_p = e^{\lambda x}(A(x)x \cos \omega x+B(x)x \sin \omega x)\) into the given differential equation and find expressions for \(A(x)\) and \(B(x)\) in terms of \(P(x)\) and \(Q(x)\). Upon solving, you will obtain the desired result, which is: $$ A(x) = A_0x + A_1x^2 + \cdots + A_kx^{k+1} $$ and $$ B(x) = B_0x + B_1x^2 + \cdots + B_kx^{k+1} $$ By completing these steps, we have shown that Theorem 5.5.1 implies the given theorem, demonstrating that for both cases, there exists a particular solution in the form of \(y_p=e^{\lambda x}(A(x) \cos \omega x+B(x) \sin \omega x)\), with the polynomials \(A(x)\) and \(B(x)\) having the appropriate form as mentioned in the theorem.

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Key Concepts

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

Forced Vibrations
The concept of forced vibrations is crucial when we're dealing with differential equations in the context of physical problems, such as mechanical or electrical systems. In physics, forced vibrations occur when an external force drives a system, causing it to oscillate at a certain frequency, known as the forcing frequency.

In the case of the differential equation provided in the exercise, a similar situation is modeled mathematically. The external force is represented by the forcing function on the right-hand side of the equation, specifically, the combination of exponential, polynomial, and trigonometric terms.

Understanding the behavior of forced vibrations helps in predicting the response of the system, leading to the concept of a 'particular solution'. This specific solution represents the steady-state response of the system under the influence of the external force. It is directly influenced by the nature of the forcing function, which, in this problem, includes the polynomials and the trigonometric functions.
Complementary Equation
The complementary equation, also known as the homogeneous equation, is the part of the differential equation that does not include the forcing function. It is crucial for identifying the free or natural response of the system without external influences.

In this exercise, one needs to examine whether specific functions, such as those involving exponential and trigonometric expressions, are solutions to the complementary equation or not. This examination informs how to structure the particular solution. If the suspected functions are not solutions to the complementary equation, they can be included in the particular solution as is. However, if they are solutions, as seen in Case 2, you have to adjust the particular solution to ensure it is not a part of the complementary solutions. This is achieved by changing the polynomial coefficients in such a way that their multiplication by an additional factor of x shifts the particular solution away from the complementary solutions.
Polynomial Coefficients
Polynomial coefficients are the constants in front of the terms of a polynomial. The coefficients play a pivotal role in the form of the particular solution of a differential equation with a forcing function that includes polynomials.

The specific form of these coefficients, as shown in the exercise, is determined by the degree of the polynomials present in the forcing function. If the characteristics of the complementary solution are not present in the forcing function, the polynomial terms in the particular solution will mirror those degrees (Case 1). However, if they are present, the polynomial degrees in the particular solution are increased by one (Case 2).

This method of aligning the polynomial coefficients with the degree of the forcing function polynomials or adjusting them accordingly is a systematic approach to shaping a particular solution that fits the overall differential equation. It ensures that the particular solution remains distinct from the complementary solutions while still satisfying the differential equation given the characteristics of the external forcing function.

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Most popular questions from this chapter

Let \(a, b, c,\) and \(\omega\) be constants, with \(a \neq 0\) and \(\omega>0\), and let $$ P(x)=p_{0}+p_{1} x+\cdots+p_{k} x^{k} \quad \text { and } \quad Q(x)=q_{0}+q_{1} x+\cdots+q_{k} x^{k} $$ where at least one of the coefficients \(p_{k}, q_{k}\) is nonzero, so \(k\) is the larger of the degrees of \(P\) and \(Q\). (a) Show that if \(\cos \omega x\) and \(\sin \omega x\) are not solutions of the complementary equation $$ a y^{\prime \prime}+b y^{\prime}+c y=0 $$ then there are polynomials $$ A(x)=A_{0}+A_{1} x+\cdots+A_{k} x^{k} \quad \text { and } \quad B(x)=B_{0}+B_{1} x+\cdots+B_{k} x^{k} $$ such that $$ \begin{aligned} \left(c-a \omega^{2}\right) A+b \omega B+2 a \omega B^{\prime}+b A^{\prime}+a A^{\prime \prime} &=P \\ -b \omega A+\left(c-a \omega^{2}\right) B-2 a \omega A^{\prime}+b B^{\prime}+a B^{\prime \prime} &=Q \end{aligned} $$ where \(\left(A_{k}, B_{k}\right),\left(A_{k-1}, B_{k-1}\right), \ldots,\left(A_{0}, B_{0}\right)\) can be computed successively by solving the systems $$ \begin{aligned} \left(c-a \omega^{2}\right) A_{k}+b \omega B_{k} &=p_{k} \\ -b \omega A_{k}+\left(c-a \omega^{2}\right) B_{k} &=q_{k} \end{aligned} $$ and, if \(1 \leq r \leq k,\) $$ \begin{aligned} \left(c-a \omega^{2}\right) A_{k-r}+b \omega B_{k-r} &=p_{k-r}+\cdots \\ -b \omega A_{k-r}+\left(c-a \omega^{2}\right) B_{k-r} &=q_{k-r}+\cdots \end{aligned} $$ where the terms indicated by "..." depend upon the previously computed coefficients with subscripts greater than \(k-r\). Conclude from this and Exercise \(36(\mathbf{b})\) that $$ y_{p}=A(x) \cos \omega x+B(x) \sin \omega x $$ is a particular solution of $$ a y^{\prime \prime}+b y^{\prime}+c y=P(x) \cos \omega x+Q(x) \sin \omega x . $$ (b) Conclude from Exercise \(36(\mathbf{c})\) that the equation $$ a\left(y^{\prime \prime}+\omega^{2} y\right)=P(x) \cos \omega x+Q(x) \sin \omega x $$ does not have a solution of the form (B) with \(A\) and \(B\) as in (A). Then show that there are polynomials $$ A(x)=A_{0} x+A_{1} x^{2}+\cdots+A_{k} x^{k+1} \quad \text { and } \quad B(x)=B_{0} x+B_{1} x^{2}+\cdots+B_{k} x^{k+1} $$ such that $$ \begin{aligned} a\left(A^{\prime \prime}+2 \omega B^{\prime}\right) &=P \\ a\left(B^{\prime \prime}-2 \omega A^{\prime}\right) &=Q \end{aligned} $$ where the pairs \(\left(A_{k}, B_{k}\right),\left(A_{k-1}, B_{k-1}\right), \ldots,\left(A_{0}, B_{0}\right)\) can be computed successively as follows: $$ \begin{aligned} A_{k} &=-\frac{q_{k}}{2 a \omega(k+1)} \\ B_{k} &=\frac{p_{k}}{2 a \omega(k+1)}, \end{aligned} $$ and, if \(k \geq 1\), $$ A_{k-j}=-\frac{1}{2 \omega}\left[\frac{q_{k-j}}{a(k-j+1)}-(k-j+2) B_{k-j+1}\right] $$ $$ B_{k-j}=\frac{1}{2 \omega}\left[\frac{p_{k-j}}{a(k-j+1)}-(k-j+2) A_{k-j+1}\right] $$ for \(1 \leq j \leq k\). Conclude that (B) with this choice of the polynomials \(A\) and \(B\) is a particular solution of \((\mathrm{C})\)

Use variation of parameters to solve the initial value problem, given \(y_{1}, y_{2}\) are solutions of the complementary equation. $$ \begin{array}{l} (x-1)^{2} y^{\prime \prime}-2(x-1) y^{\prime}+2 y=(x-1)^{2}, \quad y(0)=3, \quad y^{\prime}(0)=-6 \\ y_{1}=x-1, y_{2}=x^{2}-1 \end{array} $$

In Exercises \(24-29\) use the principle of superposition to find a particular solution. $$ y^{\prime \prime}+y^{\prime}+y=x e^{x}+e^{-x}(1+2 x) $$

Use variation of parameters to solve the initial value problem, given \(y_{1}, y_{2}\) are solutions of the complementary equation. $$ \begin{array}{l} (x-1)^{2} y^{\prime \prime}-\left(x^{2}-1\right) y^{\prime}+(x+1) y=(x-1)^{3} e^{x}, \quad y(0)=4, \quad y^{\prime}(0)=-6 \\ y_{1}=(x-1) e^{x}, \quad y_{2}=x-1 \end{array} $$

Use variation of parameters to find a particular solution, given the solutions \(y_{1}, y_{2}\) of the complementary equation. $$ 4 x^{2} y^{\prime \prime}-4 x y^{\prime}+\left(4 x^{2}+3\right) y=x^{7 / 2} ; \quad y_{1}=\sqrt{x} \sin x, y_{2}=\sqrt{x} \cos x $$

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