Hence, the characteristic equation of (28) is P(A) = X® – nz X³ – na X* – n3 X³ – n2 X² – nd – no, (29) - nA where, (2ε+6μ-2εμ+ &-3) (2 µ (1 – e)) (2ε+4μ-6εμ+2 έμ-+15) (2μ (ε- 1)) (2ε+3μ +2 εμ- μ+2@-12 (2 µ (e – 1)) n5 n4 = (E+2μ-2εμ+3) n2 = n3 (µ (1 – e)) n1 no = -1. Now, let T(A) = 1® and V(A) = -ng 15 – n4 X4 – ng 13 – n2 X² – n1 A – no. Consider |A|=1, then one has (2ε+6μ-2εμ + ε23) (2μ (1 - 0) ) (2e+4μ-6εμ+2ε μ-+15) (2μ (ε - 1) (2ε+3μ +2εμ- μ+2 22-12) (2μ (ε -1) ) (ε+2μ-2εμ+3) (µ (1 – €)) %3D (1– +1, 2 + (2ε46μ-2εμ + 2-3) (4ε+7μ-4εμ+ θμ + +3) (2 µ (1 – €)) (e + 2µ – 2 e µ +3) (1– e) (и (1 — е)) (2 e + µ – 2 €u + e² µ+ 6) , (e +2µ – 2 €µ+3) , (1– e) (2μ (ε - 1) ) (-3μ+2εμ + μ) μ(ε-1) (1-) (2 µ (e – 1)) –3 µ +2 € µ+ e² µ –µ(e – 1)² 2 и (е — 1) (2 µ (e – 1)) +1, + 1, (H (1 – €)) +1, %3D µ(E – 1) -4μ+4με + 1, +1 = 2µ (e – 1) = 3 > 1. Then, from Rouché's Theorem 1.2, V(A) and Y(A) + ¥(A) = P(^) have the same number of zeros in an open unit disk |A| < 1, that means there are only five roots lie inside unit disk. Thus, from Theorem 1.1 the equilibrium point Eo is not asymptotically stable. By solving (29), we find that 1, implies Eo is nonhyperbolic point.

Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
Problem 1RQ
icon
Related questions
Question

Show me the determine red and all information is here

Hence, the characteristic equation of (28) is
P(A) = X° – ng X* – na X* – n3 X³ – n2 1² – n1 1 – no,
(29)
-
where,
(2ε+6μ-2εμ + -3)
(2μ (1 - e)
(2ε+4μ =6εμ# 2 μ- 2+ 15 )
(2μ (ε-1) )
(2ε+3μ+2 εμ- έμ+ 222-12)
n5
n4 =
(2μ (ε - 1) )
(ε+2μ-2εμ + 3)
n2 =
n3
(µ (1 – )
(1 – e)
n1
no = -1.
Now, let T(A) = 16 and V(A) = -nz 15 – n4 X4 – n3 13 – n2 X? – nị 1 – no. Consider |A|=1,
then one has
(2ε+6μ-2 εμ # ε- 3)
(2 μ (1-)
(2ε+ 3μ + 2 εμ - ε?μ + 22-12 )
(2μ (ε - 1)
( E+2μ-2εμ# 3)
(µ (1 – e))
(4ε+7μ-4εμ + ε'μ + 243)
(2μ (ε-1))
(2ε+4μ = 6εμ+ 2 μ - ?+ 15)
+
(1 – €)
+
+ 1,
(2 μ (ε - 1) )
(2ε + 6μ = 2εμ + ε? - 3)
(2μ (1 - ε) )
( ε+2μ-2 εμ+3)
(и (1 — е))
(2ε+μ-2εμ+ μ+6)
(2μ (ε -1) )
2
(1 €)
+ 1,
(e + 2 µ – 2 € µ + 3)
(1
(и (1 — е))
+1,
2
(-3μ +2εμ+' μ) μ (ε-1) (1-e)
+ 1,
(2 μ (ε- 1) )
н (€ — 1)
-3 u +2 € u + e? µ - µ (e – 1)2
-4μ+4με
+ 1,
2 µ (e – 1)
+1=
2μ (ε- 1)
= 3 > 1.
Then, from Rouché's Theorem 1.2, V(A) and Y(A) + ¥(A) = P(X) have the same number of
zeros in an open unit disk |A| < 1, that means there are only five roots lie inside unit disk.
Thus, from Theorem 1.1 the equilibrium point Eo is not asymptotically stable. By solving (29),
we find that A1 = 1, implies Eo is nonhyperbolic point.
Transcribed Image Text:Hence, the characteristic equation of (28) is P(A) = X° – ng X* – na X* – n3 X³ – n2 1² – n1 1 – no, (29) - where, (2ε+6μ-2εμ + -3) (2μ (1 - e) (2ε+4μ =6εμ# 2 μ- 2+ 15 ) (2μ (ε-1) ) (2ε+3μ+2 εμ- έμ+ 222-12) n5 n4 = (2μ (ε - 1) ) (ε+2μ-2εμ + 3) n2 = n3 (µ (1 – ) (1 – e) n1 no = -1. Now, let T(A) = 16 and V(A) = -nz 15 – n4 X4 – n3 13 – n2 X? – nị 1 – no. Consider |A|=1, then one has (2ε+6μ-2 εμ # ε- 3) (2 μ (1-) (2ε+ 3μ + 2 εμ - ε?μ + 22-12 ) (2μ (ε - 1) ( E+2μ-2εμ# 3) (µ (1 – e)) (4ε+7μ-4εμ + ε'μ + 243) (2μ (ε-1)) (2ε+4μ = 6εμ+ 2 μ - ?+ 15) + (1 – €) + + 1, (2 μ (ε - 1) ) (2ε + 6μ = 2εμ + ε? - 3) (2μ (1 - ε) ) ( ε+2μ-2 εμ+3) (и (1 — е)) (2ε+μ-2εμ+ μ+6) (2μ (ε -1) ) 2 (1 €) + 1, (e + 2 µ – 2 € µ + 3) (1 (и (1 — е)) +1, 2 (-3μ +2εμ+' μ) μ (ε-1) (1-e) + 1, (2 μ (ε- 1) ) н (€ — 1) -3 u +2 € u + e? µ - µ (e – 1)2 -4μ+4με + 1, 2 µ (e – 1) +1= 2μ (ε- 1) = 3 > 1. Then, from Rouché's Theorem 1.2, V(A) and Y(A) + ¥(A) = P(X) have the same number of zeros in an open unit disk |A| < 1, that means there are only five roots lie inside unit disk. Thus, from Theorem 1.1 the equilibrium point Eo is not asymptotically stable. By solving (29), we find that A1 = 1, implies Eo is nonhyperbolic point.
Σ
1
E zn-h
Wn-p
h=0
Wn-p
Zn-h
h=1
p=0
p=1
Wn+1
+µ and zn+1
+ €,
(4)
Zn - €
Wn - H
where u and e are arbitrary positive real numbers with initial conditions w; and z; for i =
-2, -1,0.
The nontrivial positive equilibrium point of (4) is Eo = (w, z) = ( ,1) such that e > 1.
µ(e-1)
e+3
T
(Wn + Wn-1) (zn-1 + Zn-2)
(Wn-1 + Wn-2) (žn + žn-1)
Ln+1 =
+ l, Wn, Wn-1,
+ €, Zn, Zn-1
Zn - €
Wn - µ
Theorem 4.1. The positive equilibrium point E, of system (4) is not asymptotically stable
and nonhyperbolic point .
Proof. The linearized system of (4) evaluated at Eo is written in the matrix form as
Ln+1
Q Ln,
where Ln
(Wn, 2n, Wn-1, žn-1, Wn-2, zn-2) and the Jacobian matrix determined at Eo is equal
금
-(44)
(e+2e-3)
e+3
e+3
-(e2+2e-3)
4 µ
-(e+3)
2 u
-(c+3)
1-e
2
(28)
1
1
1
9.
O O
Transcribed Image Text:Σ 1 E zn-h Wn-p h=0 Wn-p Zn-h h=1 p=0 p=1 Wn+1 +µ and zn+1 + €, (4) Zn - € Wn - H where u and e are arbitrary positive real numbers with initial conditions w; and z; for i = -2, -1,0. The nontrivial positive equilibrium point of (4) is Eo = (w, z) = ( ,1) such that e > 1. µ(e-1) e+3 T (Wn + Wn-1) (zn-1 + Zn-2) (Wn-1 + Wn-2) (žn + žn-1) Ln+1 = + l, Wn, Wn-1, + €, Zn, Zn-1 Zn - € Wn - µ Theorem 4.1. The positive equilibrium point E, of system (4) is not asymptotically stable and nonhyperbolic point . Proof. The linearized system of (4) evaluated at Eo is written in the matrix form as Ln+1 Q Ln, where Ln (Wn, 2n, Wn-1, žn-1, Wn-2, zn-2) and the Jacobian matrix determined at Eo is equal 금 -(44) (e+2e-3) e+3 e+3 -(e2+2e-3) 4 µ -(e+3) 2 u -(c+3) 1-e 2 (28) 1 1 1 9. O O
Expert Solution
steps

Step by step

Solved in 6 steps

Blurred answer
Recommended textbooks for you
Advanced Engineering Mathematics
Advanced Engineering Mathematics
Advanced Math
ISBN:
9780470458365
Author:
Erwin Kreyszig
Publisher:
Wiley, John & Sons, Incorporated
Numerical Methods for Engineers
Numerical Methods for Engineers
Advanced Math
ISBN:
9780073397924
Author:
Steven C. Chapra Dr., Raymond P. Canale
Publisher:
McGraw-Hill Education
Introductory Mathematics for Engineering Applicat…
Introductory Mathematics for Engineering Applicat…
Advanced Math
ISBN:
9781118141809
Author:
Nathan Klingbeil
Publisher:
WILEY
Mathematics For Machine Technology
Mathematics For Machine Technology
Advanced Math
ISBN:
9781337798310
Author:
Peterson, John.
Publisher:
Cengage Learning,
Basic Technical Mathematics
Basic Technical Mathematics
Advanced Math
ISBN:
9780134437705
Author:
Washington
Publisher:
PEARSON
Topology
Topology
Advanced Math
ISBN:
9780134689517
Author:
Munkres, James R.
Publisher:
Pearson,