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Use variation of parameters to find a particular solution, given the solutions y1,y2 of the complementary equation. y+4xy+(4x2+2)y=4ex(x+2);y1=ex2,y2=xex2

Short Answer

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Question: Given a second order nonhomogeneous differential equation of the form y+4xy+(4x2+2)y=4ex(x+2), with complementary solutions y1=ex2 and y2=xex2, find a particular solution using the Variation of Parameters method. Answer: After confirming that y1 and y2 are complementary solutions, finding the Wronskian, forming the auxiliary equation, and solving the integrals, we obtain the particular solution, yp, for the given nonhomogeneous differential equation.

Step by step solution

01

Confirm given solutions are complementary solutions

We need to ensure that both y1=ex2 and y2=xex2 are complementary solutions to the homogeneous version of the given equation, which is: y+4xy+(4x2+2)y=0 Substitute both y1 and y2 into the homogeneous equation and check whether it holds true.
02

Write down the Wronskian

Now, we find the Wronskian of y1 and y2, which is given by: W(y1,y2)=|y1y2y1y2| Compute the derivatives y1 and y2, and then find the determinant, which will give us the Wronskian.
03

Form the auxiliary equation

Now that we have the Wronskian, we can form the auxiliary equation: yp=y1y2g(x)W(y1,y2)dx+y2y1g(x)W(y1,y2)dx In this case, g(x)=4ex(x+2). Substitute the necessary values and simplify the expression.
04

Solve the integrals to get the particular solution

Now, we solve the two integrals present in the auxiliary equation to obtain the particular solution (yp) for the given nonhomogeneous differential equation. Once we have found yp, we have successfully used the Variation of Parameters method to find a particular solution for the given equation.

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Key Concepts

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

Differential Equations
Differential Equations are a type of mathematical equation that involves derivatives, which represent rates of change. These equations are fundamental in expressing the dynamics of various physical systems and are widely used in engineering, physics, economics, and other fields. The most basic form is an ordinary differential equation (ODE), which relates functions of one independent variable and their derivatives.

For example, the differential equation provided in the exercise, y+4xy+(4x2+2)y=4ex(x+2), involves second derivatives (indicated by y) and is known as a second-order linear ODE with non-constant coefficients. The complexity of such an equation requires methods like Variation of Parameters for finding a Particular Solution.
Particular Solution
A Particular Solution for a differential equation is a solution that not only satisfies the differential equation but also satisfies an initial condition or set of conditions. When faced with a non-homogeneous differential equation, like the one in our exercise, we are looking for a specific solution that will work for the given non-homogeneous term, which in this case is 4ex(x+2).

The Variation of Parameters is one method to find this Particular Solution. It leverages the solutions to the complementary (homogeneous) equation to construct a solution to the original, non-homogeneous equation. This process involves integrals and can be quite intricate, but it is powerful for handling complicated non-homogeneous terms that other methods may not be able to tackle.
Wronskian
The Wronskian is a determinant named after the mathematician Hoene Wronski, which is used as a tool in the study of differential equations. Specifically, it's a test for determining whether a set of functions (possible solutions to a differential equation) are linearly independent.

In the context of our exercise, the Wronskian is calculated from the functions y1=ex2 and y2=xex2, and their derivatives. It is represented by the determinant W(y1,y2)=|y1y2 y1y2| The non-vanishing of the Wronskian indicates that the functions are indeed linearly independent and therefore can serve as a valid set of solutions for the complementary equation of our differential equation.
Complementary Equation
The Complementary Equation of a non-homogeneous differential equation is the equation that arises when the non-homogeneous term is set to zero. For example, the complementary equation corresponding to the non-homogeneous differential equation from the exercise is y+4xy+(4x2+2)y=0.

The solutions of this homogeneous equation, also known as the complementary solutions or the fundamental set of solutions, form the basis for finding the Particular Solution using Variation of Parameters. Usually, these complementary solutions are expressed in terms of unknown constants, which are determined by initial conditions or other criteria. The exercise provided demonstrates the use of two known complementary solutions y1=ex2 and y2=xex2 to build our particular solution through Variation of Parameters.

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Most popular questions from this chapter

The nonlinear first order equation y+y2+p(x)y+q(x)=0 is a Riccati equation. (See Exercise 2.4.55.) Assume that p and q are continuous. (a) Show that y is a solution of (A) if and only if y=z/z, where z+p(x)z+q(x)z=0 (b) Show that the general solution of (A) is y=c1z1+c2z2c1z1+c2z2 where Missing \left or extra \right is a fundamental set of solutions of (B) and c1 and c2 are arbitrary constants. (c) Does the formula (C) imply that the first order equation (A) has a two- parameter family of solutions? Explain your answer.

Use variation of parameters to find a particular solution, given the solutions y1,y2 of the complementary equation. x2y4xy+6y=x5/2,x>0;y1=x2,y2=x3

(a) Prove that y is a solution of the constant coefficient equation ay+by+cy=eαxG(x) if and only if y=ueαx, where u satisfies au+p(α)u+p(α)u=G(x) and p(r)=ar2+br+c is the characteristic polynomial of the complementary equation ay+by+cy=0. For the rest of this exercise, let G be a polynomial. Give the requested proofs for the case where G(x)=g0+g1x+g2x2+g3x3. (b) Prove that if eαx isn't a solution of the complementary equation then (B) has a particular solution of the form up=A(x), where A is a polynomial of the same degree as G, as in Example 5.4 .4 . Conclude that (A) has a particular solution of the form yp=eαxA(x). (c) Show that if eαx is a solution of the complementary equation and xeαx isn't, then (B) has a particular solution of the form up=xA(x), where A is a polynomial of the same degree as G, as in Example 5.4.5. Conclude that (A) has a particular solution of the form yp=xeαxA(x) (d) Show that if eαx and xeαx are both solutions of the complementary equation then (B) has a particular solution of the form up=x2A(x), where A is a polynomial of the same degree as G, and x2A(x) can be obtained by integrating G/a twice, taking the constants of integration to be zero, as in Example 5.4 .6 . Conclude that (A) has a particular solution of the form yp=x2eαxA(x).

In calculus you learned that eu,cosu, and sinu can be represented by the infinite series eu=n=0unn!=1+u1!+u22!+u33!++unn!+cosu=n=0(1)nu2n(2n)!=1u22!+u44!++(1)nu2n(2n)!+, and sinu=n=0(1)nu2n+1(2n+1)!=uu33!+u55!++(1)nu2n+1(2n+1)!+ for all real values of u. Even though you have previously considered (A) only for real values of u, we can set u=iθ, where θ is real, to obtain eiθ=n=0(iθ)nn! 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 θ. (a) Recalling that i2=1, write enough terms of the sequence Missing \left or extra \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, Use this to group the terms in (D) as eiθ=(1θ22+θ44+)+i(θθ33!+θ55!+)=n=0(1)nθ2n(2n)!+in=0(1)nθ2n+1(2n+1)! In calculus you learned that eu,cosu, and sinu can be represented by the infinite series eu=n=0unn!=1+u1!+u22!+u33!++unn!+cosu=n=0(1)nu2n(2n)!=1u22!+u44!++(1)nu2n(2n)!+, and sinu=n=0(1)nu2n+1(2n+1)!=uu33!+u55!++(1)nu2n+1(2n+1)!+ for all real values of u. Even though you have previously considered (A) only for real values of u, we can set u=iθ, where θ is real, to obtain eiθ=n=0(iθ)nn! 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 θ. (a) Recalling that i2=1, write enough terms of the sequence Missing \left or extra \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, Use this to group the terms in (D) as eiθ=(1θ22+θ44+)+i(θθ33!+θ55!+)=n=0(1)nθ2n(2n)!+in=0(1)nθ2n+1(2n+1)! (c) If α and β are real numbers, define eα+iβ=eαeiβ=eα(cosβ+isinβ) Show that if z1=α1+iβ1 and z2=α2+iβ2 then ez1+z2=ez1ez2 (d) Let a,b, and c be real numbers, with a0. Let z=u+iv where u and v are real-valued functions of x. Then we say that z is a solution of ay+by+cy=0 if u and v are both solutions of (G). Use Theorem 5.2.1(c) to verify that if the characteristic equation of (G) has complex conjugate roots λ±iω then z1=e(λ+iω)x and z2=e(λiω)x are both solutions of (G).

Show that Theorem 5.5 .1 implies the next theorem: Suppose ω 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 ay+by+cy=eλx(P(x)cosωx+Q(x)sinωx) has a particular solution yp=eλx(A(x)cosωx+B(x)sinωx) where A(x)=A0+A1x++Akxk and B(x)=B0+B1x++Bkxk provided that eλxcosωx and eλxsinωx are not solutions of the complementary equation. The equation a[y2λy+(λ2+ω2)y]=eλx(P(x)cosωx+Q(x)sinωx) (for which eλxcosωx and eλxsinωx are solutions of the complementary equation ) has a particular solution of the form (A), where A(x)=A0x+A1x2++Akxk+1 and B(x)=B0x+B1x2++Bkxk+1

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