# Elementary differential equations 7th edition - Boyce W.E

ISBN 0-471-31999-6

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/ + p(t) y'+ q (t )y = g(t), (1)

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542

Chapter 10. Partial Differential Equations and Fourier Series

with the initial conditions

y(to) = yo, y' (tf = y0 ? (2)

Physical applications often lead to another type of problem, one in which the value of the dependent variable y or its derivative is specified at two different points. Such conditions are called boundary conditions to distinguish them from initial conditions that specify the value of y and y' at the same point. A differential equation together with suitable boundary conditions form a two-point boundary value problem. A typical example is the differential equation

y" + P(x ) y'+ q (x ) y = g(x ) (3)

with the boundary conditions

y(a) = yo’ y(fi) = yv (4)

The natural occurrence of boundary value problems usually involves a space coordinate as the independent variable so we have used x rather than t in Eqs. (3) and (4). To

solve the boundary value problem (3), (4) we need to find a function y = $(x) that

satisfies the differential equation (3) in the interval a < x < 3 and that takes on the specified values y0 and y1 at the endpoints of the interval. Usually, we seek first the general solution of the differential equation and then use the boundary conditions to determine the values of the arbitrary constants.

Boundary value problems can also be posed for nonlinear differential equations but we will restrict ourselves to a consideration of linear equations only. An important classification of linear boundary value problems is whether they are homogeneous or nonhomogeneous. If the function g has the value zero for each x, and if the boundary values y0 and y1 are also zero, then the problem (3), (4) is called homogeneous. Otherwise, the problem is nonhomogeneous.

Although the initial value problem (1), (2) and the boundary value problem (3), (4) may superficially appear to be quite similar, their solutions differ in some very important ways. Under mild conditions on the coefficients initial value problems are certain to have a unique solution. On the other hand, boundary value problems under similar conditions may have a unique solution, but may also have no solution or, in some cases, infinitely many solutions. In this respect, linear boundary value problems resemble systems of linear algebraic equations.

Let us recall some facts (see Section 7.3) about the system

Ax = b, (5)

where A is a given n x n matrix, b is a given n x 1 vector, and x is an n x 1 vector to be determined. If A is nonsingular, then the system (5) has a unique solution for any b. However, if A is singular, then the system (5) has no solution unless b satisfies a certain additional condition, in which case the system has infinitely many solutions. Now consider the corresponding homogeneous system

Ax = 0, (6)

obtained from the system (5) when b = 0. The homogeneous system (6) always has the solution x = 0. If A is nonsingular, then this is the only solution, but if A is singular, then there are infinitely many (nonzero) solutions. Note that it is impossible for the homogeneous system to have no solution. These results can also be stated in the following way: The nonhomogeneous system (5) has a unique solution if and only

10.1 Two-Point Boundary Value Problems

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if the homogeneous system (6) has only the solution x = 0, and the nonhomogeneous system (5) has either no solution or infinitely many if and only if the homogeneous system (6) has nonzero solutions.

We now turn to some examples of linear boundary value problems that illustrate very similar behavior. A more general discussion of linear boundary value problems appears in Chapter 11.

EXAMPLE

1

Solve the boundary value problem

y" + 2y = 0, y (0) = 1, y (n) = 0. (7)

The general solution of the differential equation (7) is

y = c1 cos V2x + c2 sin V2x. (8)

The first boundary condition requires that c1 = 1. The second boundary condition

implies that c1 cos + c2 sin -/in = 0, so c2 = — cot -/in = -0.2762. Thus the

solution of the boundary value problem (7) is

y = cos V2x — cot V2n sin V2x. (9)

This example illustrates the case of a nonhomogeneous boundary value problem with a unique solution.

EXAMPLE

2

Solve the boundary value problem

y" + y = 0, y (0) = 1, y (n) = a, (10)

where a is a given number.

The general solution of this differential equation is

y = c1 cos X + c2sin X (11)

and from the first boundary condition we find that c1 = 1. The second boundary condition now requires that —c1 = a. These two conditions on c1 are incompatible if a = — 1 so the problem has no solution in that case. However, if a = — 1, then both boundary conditions are satisfied provided that c1 = 1, regardless of the value of c2. In this case there are infinitely many solutions of the form

y = cos x + c2sin x , (12)

where c2 remains arbitrary. This example illustrates that a nonhomogeneous boundary value problem may have no solution, and also that under special circumstances it may have infinitely many solutions.

Corresponding to the nonhomogeneous boundary value problem (3), (4) is the homogeneous problem consisting of the differential equation

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