Thursday 31 May 2018

SECOND-ORDER DIFFERENCE EQUATIONS - DIRECT METHOD


EDITOR: B. SOMANATHAN NAIR


Since difference equations are modifications of differential equations, we can expect similar solutions in the case of second-order difference equations, where we have to substitute the term an for the term et. Consider the second-order difference equation

                        y(n) + ay(n‒1) + by(n‒2) = 0  (1)
                                             

The characteristic equation of this difference equation can be written as

                                                            (C2 + aC + b)y = 0       (2)                                                  

where we have used C2 y = y(n), and so on. The roots of this equation, as in the case of differential equations, can be taken as α and β and depending on the values of these, we have four possible solutions to Eq. (2) as given below.

Solution I: Both a and b exist and are real and unequal

In this case, both the roots are real and unequal. That is the roots are α ± β. The solution can be written in a way similar to that given in Eq. (4) of solution to differential equation as


                                                y(n) = A(α + β)n + B(αβ)n  (3)
                                                                     

Solution II: Both the roots are real and equal

In this case, only α exists, β. = 0. The solution can be written similar to that given in Eq. (5) as


                                    y(n) = αn(A + Bn)  (4)                                                        

Solution III: Both the roots have real and imaginary parts

The roots are α ± , and the solution can be written similar to that given in Eq. (6) as                                       

                                                y(n) = A(α + )n u(n)+ B(α)n u(n)  (5)
           
Equation (5) may be manipulated mathematically to yield its trigonometric form                     

                        y(n) = rn‑(C cos nθ + D sin )   (6)                   

where we have used the new constants C = A+B and D = j(A−B). 
                                                                                                                                                                                                                     
Solution IV: Both the roots are imaginary and are equal to ± jb
The solution can be written in a form similar to that given in Eq. (6). Thus, we have

                        y(n) = C cos nb + D sin nb   (7)           
                                                          

In the forthcoming blogs, we illustrate the solutions of differential and difference equations using typical numerical examples.


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