MAT 412: Ordinary Differential Equation II: Introduction to Second Order ODE Imaga Ogbu Famous Department of Mathematics Covenant University Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 1 / 16 Objectives Learning Objectives 1 Identify linear and nonlinear differential equations 2 Identify homogeneous and nonhomogenous linear equation 3 Identify linearly dependent and independent functions Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 2 / 16 The general form of second order linear differential equation is Definition P(x)y′′ + Q(x)y′ + R(x)y = G(x) (1) where P(x), Q(x), R(x) and G(x) are real valued functions and P(x) ̸= 0. x is the independent variable while y is the dependent variable. Equation (1) is a homogeneous linear equation if G(x) = 0. If G(x) ̸= 0 then, it is a non homogeneous linear equation. Equation (1) is linear because y and its derivatives are raised to the first power and are not multiplied by one another. Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 3 / 16 Example Classify the following equations: y′′ + 5x3 y′ + xy3 = 3x (sin 2x)y′′ + (cos x)y′ + 6y = 0 4u2 x′′ + 3uxx′ + 4x = 0 xy′′ + xy = 4x6 (sin t)y′′ − sin y′ + (cos t)y − sin t = 0 (sin x2 )y′′ − (cos x)y′ + x3 y = y − 2 7xy′′ − 5x3 y′ + 3xy − 6x3 = 0 Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 4 / 16 Solution of a Differential Equation A solution of a differential equation is a relation between the dependent and independent variable when substituted into the differential equation reduces it to an identity. Show that y = x3 is a solution of x2 y − xy − 3y = 0 y = 2x2 is a solution of 12 x2 y′′ − xy′ + y = 0. Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 5 / 16 Superposition Principle The linear combination of two functions y1 (x) and y2 (x) is a function y(x) = c1 y1 (x) + c2 y2 (x) where c1 and c2 are two arbitrary constants. Theorem If y1 (x) and y2 (x) are solutions to a linear homogeneous differential equation, then the function y(x) = c1 y1 (x) + c2 y2 (x), where c1 and c2 are constants is also a solution. Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 6 / 16 Exercises Prove the Superposition Principle. If e−x and e5x are solutions to y′′ − 4y′ − 5y = 0, show that 3e−x + 2e5x is also a solution If e−2x and e−3x are solutions to y′′ + 5y′ + 6y = 0, show that 2e−2x + 3e−3x is also a solution. Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 7 / 16 Linearly Dependent and Independent Functions Definitions: Linearly Dependent functions A set of functions f1 (x), f2 (x), . . . , fn (x) is said to be linearly dependent if there are constants c1 , c2 , . . . , cn not all zero such that c1 f1 (x) + c2 f2 (x) + · · · + cn fn (x) = 0 for all x over the interval of interest. A set of functions that is not linearly dependent is said to be linearly independent i.e. c1 f1 (x) + c2 f2 (x) + · · · + cn fn (x) = 0 implies that c1 = c2 = · · · = cn = 0 Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 8 / 16 Proof: Linearly Dependent I Suppose f2 (x) ≡ 0, then choose c1 = 0 and c2 = 1 then the condition of linear dependence is met i.e. c1 f1 (x) + c2 f2 (x) = 0 + 0 = 0. Conversely, if f1 (x) ̸= 0 and f2 (x) ̸= 0 but f1 (x) = Cf2 (x) for some constant C, then choose c1 = C and c2 = −1, then the condition of linear dependence is also met i.e. c1 f1 (x) + c2 f2 (x) = 0 + 0 = 0. Next we show that if two functions are linearly dependent, then either one is identically zero or they are constant multiples of one another. Assume Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 9 / 16 Proof: Linearly Dependent II f1 (x) and f2 (x) are linearly dependent. Then, there are constants, c1 and c2 , not both zero, such that c1 f1 (x) + c2 f2 (x) = 0 for all x over the interval of interest. Then, c1 f1 (x) = −c2 f(x). Since, c1 , c2 can’t both be zero, assume c2 ̸= 0. Then, there are two cases: either c1 = 0 or c1 ̸= 0. If c1 = 0, then 0 = −c2 f2 (x) 0 = f2 (x), Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 10 / 16 Proof: Linearly Dependent III so one of the functions is identically zero. Now suppose c1 ̸= 0. Then, ( ) c2 f1 (x) = − f2 (x) c1 and we see that the function are constant multiples of one another. Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 11 / 16 Linear Dependence of Two Functions Theorem: Linearly Dependence of Two Functions Two functions, f1 (x) and f2 (x), are said to be linearly dependent if either one of them is identically zero or if f1 (x) = Cf2 (x) for some constant C and for all x over the interval of interest. Functions that are not linearly dependent are said to be linearly independent. Determine if the following pairs are linearly dependent or linearly independent f1 (x) = x2 and f2 (x) = 5x2 f1 (x) = sin x and f2 (x) = cos x f1 (x) = e3x and f2 (x) = e−3x f1 (x) = 3x and f2 (x) = 3x + 1 Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 12 / 16 General Solution to a Homogeneous Equation Theorem: Linearly Dependence of Two Functions If y1 (x) and y2 (x) are linearly independent solutions to a second-order, linear homogeneous differential equations, then the general solution is given by y(x) = c1 y1 (x) + c2 y2 (x), where c1 and c2 are constants. If y1 (t) = e3t and y2 (t) = e−3t are solutions to y′′ − 9y = 0, what is the general solution. Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 13 / 16 Second-Order Equations with Constant Coefficients General Form ay′′ + by′ + cy = 0, where a, b, c are constants. Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 14 / 16 Characteristic Equation Characteristic Equation The characteristic equation of the second-order differential equation ay′′ + by′ + cy = 0 is aλ2 + bλ + c = 0. Proof: Let y = eλx , then y′ = λeλx , y′′ = λ2 eλx . Substituting it into the second-order equation gives ay′′ + by′ + c = a(λ2 eλx ) + b(λeλx ) + ceλx = eλx (aλ2 + bλ + c). Since eλx ̸= 0, then Imaga O. F. (Dept. of Mathematics) (aλ2 + bλ + c) = 0. Ordinary Differential Equation II Second-Order ODE 15 / 16 The solution of the characteristic equation using the quadratic formula is √ −b ± b2 − 4ac λ= . 2a This gives three cases. The characteristic equation has distinct real roots; repeated real root; or complex conjugate. Imaga O. F. (Dept. of Mathematics) Ordinary Differential Equation II Second-Order ODE 16 / 16