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In Exercises 27 solve the boundary value problem. yy=x,y(0)+y(0)=3,y(1)y(1)=2

Short Answer

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Question: Find the solution to the boundary value problem for the given second-order linear differential equation with boundary conditions: yy=x,y(0)+y(0)=3,y(1)y(1)=2 Answer: The particular solution that satisfies both the differential equation and the boundary conditions is given by: y(x)=2ex+21e2exx

Step by step solution

01

Solve the Homogeneous Differential Equation

First, we need to solve the homogeneous differential equation, which is obtained by setting the right-hand side of the given differential equation equal to zero: yy=0 The characteristic equation for this ODE is: r21=0 Factoring the expression, we get (r1)(r+1)=0. Thus, the roots are r1=1 and r2=1. Therefore, the general solution for the homogeneous differential equation is given by: yh(x)=C1ex+C2ex where C1 and C2 are constants that will need to be determined using the boundary conditions.
02

Find a Particular Solution to the Inhomogeneous Differential Equation

To find a particular solution to the inhomogeneous differential equation, we will use the method of undetermined coefficients. Since the right-hand side of the given differential equation is a polynomial of degree 1 (a linear function), we will assume a particular solution of the form: yp(x)=Ax+B where A and B are constants to be determined. Now, we differentiate yp(x) twice to get its second derivative: yp(x)=A yp(x)=0 Substitute yp(x), yp(x), and yp(x) into the given inhomogeneous differential equation: 0(Ax+B)=x Which simplifies to: AxB=x Comparing coefficients, we have: A=1 and B=0 Thus, the particular solution to the inhomogeneous differential equation is: yp(x)=x
03

Combine the Homogeneous and Particular Solutions

Now, we need to combine the homogeneous and particular solutions to obtain the general solution to the given inhomogeneous differential equation: y(x)=yh(x)+yp(x)=C1ex+C2exx
04

Apply the Boundary Conditions to Determine the Constants

Now, we will apply the given boundary conditions to determine the values of C1 and C2. First boundary condition is: y(0)+y(0)=3 Calculate y(x): y(x)=C1exC2ex1 Evaluate the first boundary condition: (C1+C2)+(C1C21)=3 Simplifying the equation gives: 2C11=3 From this, we can find the value of C1: C1=2 The second boundary condition is: y(1)y(1)=2 Plug in the values of x=1, and C1=2 into the general solution and its derivative, then apply the second boundary condition: (2e+C2e11)(2eC2e11)=2 Simplifying the equation gives: C2(1e2)=2 We can find the value of C2: C2=21e2
05

Write the Final Solution

Now, we have the values of C1 and C2. Plug them into the general solution to get the particular solution that satisfies both the differential equation and the boundary conditions: y(x)=2ex+21e2exx This is the final solution to the given boundary value problem.

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Key Concepts

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

Understanding Homogeneous Differential Equations
A homogeneous differential equation is a type of differential equation where all the terms are a function of the dependent variable and its derivatives only. In the given exercise, the homogeneous part is identified by setting the right-hand side of the original differential equation to zero.

The equation then simplifies to yy=0, which only involves the function y and its second derivative y. This equation is considered homogeneous because there are no terms involving only x or constants.

To solve this, we derive the characteristic equation, r21=0, from the coefficients of y and its derivatives. This equation helps in finding the roots which are critical in constructing the general solution to the homogeneous differential equation. Here, the roots are r1=1 and r2=1, leading us to the general solution yh(x)=C1ex+C2ex, where C1 and C2 are constants determined by the boundary conditions.
Finding a Particular Solution
When dealing with inhomogeneous differential equations like yy=x, we seek a particular solution that works for the non-homogeneous part, in this case x. The method of undetermined coefficients is a technique where we guess a form for the particular solution based on the type of the non-homogeneous term.

For our equation, since the non-homogeneous term is a polynomial of degree 1 (a linear term x), we assume a particular solution of the form yp(x)=Ax+B, where A and B are constants. By substituting yp and its derivatives back into the original equation and simplifying, we determine the values of the constants.

In this case, A=1 and B=0, leading to the particular solution yp(x)=x. This solution addresses the specific non-homogeneous part of our differential equation and is combined with the homogeneous solution to form the more complete general solution.
Characteristic Equation and Its Role
The characteristic equation is a foundational step in solving homogeneous linear differential equations with constant coefficients. It translates the differential equation into an algebraic form, which allows us to find the roots that represent the solutions to the differential equation.

This algebraic equation is obtained by assuming a solution of the form y=erx and substituting it into the homogeneous differential equation. For the exercise in question, this leads to the characteristic equation r21=0, which then factors into (r1)(r+1)=0 revealing the roots r1=1 and r2=1.

The roots of the characteristic equation tell us the form of the general solution to the homogeneous differential equation, which is a sum of solutions derived from each root, herein yh(x)=C1ex+C2ex. This process shows how the characteristic equation bridges the gap between differential and algebraic equations, making it easier to solve the former by using techniques from the latter.

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Most popular questions from this chapter

In Exercises 1619 find all values of ω such that boundary problem has a unique solution, and find the solution by the method used to prove Theorem 13.1.3. For other values of ω, find conditions on F such that the problem has a solution, and find all solutions by the method used to prove Theorem 13.1.4. y+ω2y=F(x),y(0)=0,y(π)=0

Consider the Sturm-Liouville problem y+λy=0,y(0)+αy(0)=0,y(1)+(α1)y(1)=0 where 0<α<1 (a) Show that λ=0 is an eigenvalue of (A), and find an associated eigenfunction. (b) Show that (A) has a negative eigenvalue, and find the form of an associated eigenfunction. (c) Give a graphical argument to show that (A) has infinitely many positive eigenvalues λ1<λ2< <λn<, and state the form of the associated eigenfunctions.

In Example 13.2 .4 we found that the eigenvalue problem x2y+xy+λy=0,y(1)=0,y(2)=0 is equivalent to the Sturm-Liouville problem (xy)+λxy=0,y(1)=0,y(2)=0 Multiply the differential equation in (B) by y and integrate to show that λ12y2(x)xdx=12x(y(x))2dx Conclude from this that the eigenvalues of (A) are all positive.

Take it as given that Missing \left or extra \right and xcoskx,xsinkx are fundamental sets of solutions of x2y2xy+2yk2x2y=0 and x2y2xy+2y+k2x2y=0 respectively. Find the first five eigenvalues of x2y2xy+2y+λx2y=0,y(1)=0,y(2)=0 with errors no greater than 5×108. State the form of the associated eienfunctions.

Deal with the Sturm-Liouville problem y+λy=0,αy(0)+βy(0),ρy(L)+δy(L)=0 where α2+β2>0 and ρ2+δ2>0 The point of this exercise is that (SL) can't have more than two negative eigenvalues. (a) Show that λ is a negative eigenvalue of (SL) if and only if λ=k2, where k is a positive solution of (αρβδk2)sinhkL+k(αδβρ)coshkL (b) Suppose αδβρ=0. Show that (SL) has a negative eigenvalue if and only if αρ and βδ are both nonzero. Find the negative eigenvalue and an associated eigenfunction. HINT: Show that in this case ρ=pα and s=qβ, where q0 (c) Suppose βραδ0. We know from Section 11.1 that (SL) has no negative eigenvalues if αρ=0 and βδ=0. Assume that either αρ0 or βδ0. Then we can rewrite (A) as tanhkL=k(βραδ)αρβδk2 By graphing both sides of this equation on the same axes (there are several possibilities for the right side), show that it has at most two positive solutions, so (SL) has at most two negative eigenvalues.

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