CHAPTER 3. Higher-Order Differential Equations. (3.1~3.6). Chapter Contents. 3.1 Theory of Linear Equations 3.2 Reduction of Order 3.3 Homogeneous Linear Equations with Constants Coefficients 3.4 Undetermined Coefficients 3.5 Variation of Parameters 3.6 Cauchy-Euler Equations.
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Chapter Contents • 3.1 Theory of Linear Equations • 3.2 Reduction of Order • 3.3 Homogeneous Linear Equations with Constants Coefficients • 3.4 Undetermined Coefficients • 3.5 Variation of Parameters • 3.6 Cauchy-Euler Equations
Theorem 3.1.1 Existence of a Unique Solution Let an(x), an-1(x), …, a0(x),and g(x)be continuous on I, an(x) 0for all x on I. If x = x0 is any point in this interval, then a solution y(x)of (1) exists on the interval and is unique.
Example 1 Unique Solution of an IVP • The IVP possesses the trivial solution y = 0. Since this DE with constant coefficients, from Theorem 3.1.1, hence y = 0 is the only one solution on any interval containing x = 1.
Example 2 Unique Solution of an VP • Please verify y = 3e2x + e–2x– 3x,is a solution of This DE is linear and the coefficients and g(x)are all continuous, and a2(x) 0 on any I containing x = 0.This DE has an unique solution on I.
Boundary-Value Problem • Solve:Subject to: is called a boundary-value problem (BVP).See Fig 3.1.1.
Example 3 A BVP Can Have Money, Ine, or Not Solutions • In example 4 of Sec 1.1, we see the solution of is x = c1 cos 4t + c2 sin4t (2) (a) Suppose x(0) = 0,then c1 = 0, x(t) = c2 sin 4t Furthermore, x(/2) = 0,we obtain 0 = 0,hence(3)has infinite many solutions. See Fig 3.1.2. (b) If(4)we have c1 = 0, c2= 0, x = 0is the only solution.
Example 3 (2) (c) If (5)we have c1 = 0, and 1 = 0 (contradiction).Hence (5) has no solutions.
Homogeneous Equations • The following DE(6)is said to be homogeneous;(7)with g(x)not identically zero, is nonhomogeneous.
Differential Operators • Let dy/dx = Dy. This symbol D is called a differential operator. We define an nth-order differential operator as (8)In addition, we have(9)so the differential operator L is a linear operator. • Differential EquationsWe can simply write the DEs as L(y) = 0andL(y) = g(x)
Let y1, y2, …, ykbe a solutions of the homogeneous Nth-order differential equation (6) on an interval I. Then the linear combinationy = c1y1(x) + c2y2(x)+ …+ ckyk(x)where the ci, i = 1, 2, …, k are arbitrary constants, is also a solution on the interval. Theorem 3.1.2 Superposition Principles – Homogeneous Equations
Corollaries to Theorem 3.1.2 (a) y = cy1 is also a solution if y1is a solution. (b) A homogeneous linear DE always possesses the trivial solution y = 0.
A set of f1(x), f2(x), …, fn(x)is linearly dependent on an interval I, if there exists constants c1, c2, …, cn, not all zero, such thatc1f1(x) + c2f2(x) + … + cn fn(x) = 0If not linearly dependent, it is linearly independent. Definition 3.1.1 Linear Dependence / Independence Example 4 Superposition – Homogeneous DE • The function y1= x2, y2= x2 ln x are both solutions of Then y = x2+ x2 ln x is also a solution on (0, ).
In other words, if the set is linearly independent,when c1f1(x) + c2f2(x) + … + cn fn(x) = 0then c1 = c2 = … = cn= 0 • Referring to Fig 3.1.3, neither function is a constant multiple of the other, then these two functions are linearly independent. • If two functions are linearly dependent, then one is simply a constant multiple of the other. • Two functions are linearly independent when neither is a constant multiple of the other.
Let y1(x), y2(x), …, yn(x) be n solutions of the nth-order homogeneous DE (6) on an interval I. This set of solutions is linearly independent on I if and on if W(y1, y2, …, yn) 0 for every x in the interval. Theorem 3.1.3 Criterion for Linear Independence Solutions
Definition 3.1.3 Fundamental Set of Solutions Any set y1(x), y2(x),… , yn(x) of n linearly independent solutions is said to be a fundamentalset of solutions. There exists a fundamental set of solutions for (6) on an interval I. Theorem 3.1.4 Existence of a Fundamental Set
Let y1(x), y2(x), …, yn(x) be a fundamental set of solutions of homogeneous DE (6) on an interval I. Then the general solution isy = c1y1(x) + c2y2(x) + … + cnyn(x) where ci, i = 1, 2, …, n are arbitrary constants. Theorem 3.1.5 General Solution – Homogeneous Equations
Example 9 General Solution of a Homogeneous DE • The functions y1= ex,y2 = e2x , y3 = e3xare solutions of y’’’ –6y” + 11y’ –6y = 0on (-, ). Sincefor everyrealvalueof x. So y = c1ex + c2e2x + c3e3xis the general solution on (-, ).
Any ypfree of parameters satisfying (7) is called a particular solution. If y1(x), y2(x), …, yk(x) be a fundamental set of solutions of (6), then the general solution of (7) isy= c1y1 + c2y2 +… +ckyk + yp(10)where ci, i = 1, 2, …, n are arbitrary constants. Theorem 3.1.6 General Solution – Nonhomogeneous Equations Nonhomogeneous Equations • Complementary Functiony = c1y1 + c2y2 +… +ckyk +yp = yc + yp = complementary + particular
Given(12)where i = 1, 2, …, k. If ypi denotes a particular solution corresponding to the DE (12) with gi(x), then(13)is a particular solution of (14) Theorem 3.1.7 Superposition Principles – Nonhomogeneous Equations Any Superposition Principles
Example 11 Superposition – Nonmogeneous DE • We findis a particular solution ofis a particular solution ofis a particular solution of From Theorem 3.1.7, is a solution of
Note • If ypi is a particular solution of (12), then is also a particular solution of (12) when the right-hand member is
3.2 Reduction of Order • IntroductionWe know the general solution of (1)is y = c1y1 + c2y1. Suppose y1(x)denotes a known solution of (1). We assume the other solution y2has the form y2= uy1.Our goal is to find a u(x)and this method is called reduction of order.
Example 1 Finding s second Solution Given y1 = ex is a solution of y” – y = 0,find a second solution y2 by the method of reduction of order. Solution:If y = uex, then And Since ex 0, we let w = u’,then
Example 1 (2) Thus(2)Choosing c1= 0, c2= -2, we have y2= e-x. Because W(ex, e-x) 0for every x, they are independent on (-, ).
General Case • Rewrite (1) as the standard form(3)Let y1(x)denotes a known solution of (3) and y1(x) 0 for every x in the interval. • If we define y = uy1, thenwe have
Example 2 A second Solution by Formula (5) The function y1= x2is a solution of Find the general solution on (0, ). Solution:The standard form is From (5)The general solution is
Higher-Order Equations • Given (12)we have(13)as an auxiliary equation. • If the roots of (13) are real and distinct, then the general solution of (12) is