2 The local stability of the solutions The equilibrium point x of Eq. (1) is the positive solution of the equation Ỹ=(A+B+C+D)x+ x= where d = e. If [(A+B+C+D) − 1] (e – d) > 0, then the only positive equilibrium point Ỹ of Eq. (1) is given by b [(A+B+C+D) − 1] (e – d) * Let us now introduce a continuous F: (0,∞)4 → (0,∞) which is defined by F(uo, u1, U2, U3) = Auo + Bu₁ + Cu₂+ Du3+ provided du₁eu₂. Consequently, we get ƏF(x,x,x,x) = дио JF(x,x,x,x) ди JF(x,x,x,x) 242 bx (d- e)x = C+ = B_ e [(A+B+C+D) −1] (e - d) = A = Po, JF(x,x,x,x) = Ju3 e[(A+B+C+D) −1] (ed) 2 D = P3, function (7) bu₁ (du₁ - eu₂) (8) = P1, P2, (9) where e ‡ d. Thus, the linearized equation of Eq. (1) about x takes the form Cat1 Zn+1-Pozn-P1Zn-k-P2²n-1-P3²n-σ = 0, where po, P1, P2 and p3 are given by (9). (10) (6)
2 The local stability of the solutions The equilibrium point x of Eq. (1) is the positive solution of the equation Ỹ=(A+B+C+D)x+ x= where d = e. If [(A+B+C+D) − 1] (e – d) > 0, then the only positive equilibrium point Ỹ of Eq. (1) is given by b [(A+B+C+D) − 1] (e – d) * Let us now introduce a continuous F: (0,∞)4 → (0,∞) which is defined by F(uo, u1, U2, U3) = Auo + Bu₁ + Cu₂+ Du3+ provided du₁eu₂. Consequently, we get ƏF(x,x,x,x) = дио JF(x,x,x,x) ди JF(x,x,x,x) 242 bx (d- e)x = C+ = B_ e [(A+B+C+D) −1] (e - d) = A = Po, JF(x,x,x,x) = Ju3 e[(A+B+C+D) −1] (ed) 2 D = P3, function (7) bu₁ (du₁ - eu₂) (8) = P1, P2, (9) where e ‡ d. Thus, the linearized equation of Eq. (1) about x takes the form Cat1 Zn+1-Pozn-P1Zn-k-P2²n-1-P3²n-σ = 0, where po, P1, P2 and p3 are given by (9). (10) (6)
Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
Problem 1RQ
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