Theorem 3.1. The system (4) has a prime period-two solutions if and only if ? +€ -1 + 0, (22) 7 is true. Proof. First, assume that the system (4) has a distinct prime period-two solution in the follow- ing form ., (a1, B1), (a2, B2), (a1, 31), (a2, B2), ... where a + a2 and B1 + B2. Then, from (11) and (12), we obtain (@1 + a2) (B1 + B2) B2 – € (a1 + a2) (B1 + B2) B1 - € (@1 + a2) (B1 + B2) + Hy (23) a2 = + Hy (24) + €, (25) a2 – µ (a1 + a2) (B1 + B2) B2 = + €. (26) By some calculations from equations (23)-(26), we get 2 µ e (e – 1) e2 + € – 1 µ² (e? – (e + 1)) (e² +e – 1) (e² + € – 1)² - a1 + a2 = and a1 ¤2 = B1 + B2 = 1 and B1 B2 = 0, hence, we see that (a1 + a2)² – 4 a1 a2 # 0 and (ß1 + B2)² – 4 B1 32 # 0, which implies that a1 # a2 and ß1 # B2. Thus, µ (e? – (e + 1)) H (e² – e + 1) e2 + € – 1 , d2 = B1 = 0 and 6B2 = 1. (27) e2 + € – 1 Clearly a; exist if and only if e2 +e-1#0 and they are positive if e > 1 for i = 1, 2. Secondly, suppose that e² + € – 1 7 0 is satisfied. Then, the system (4) has a prime period two solution (e1, 5) = (" - (-+ 1),) and (a2, 52) = ("-+D). e2 + € – e2 + € – 1 Now, we show that (w1, z1) (a1, B1). From (4), we have (wo+ w_1) (z–1 + z-2) Wi %3D 20 – € (a1 + a2) (B1 + B2) + H, B2 - € (2εμ(ε-1) 1- € 1 + µ, e? + € – 1 2 e µ(e – 1) + µ (1 – e) (e² + e – 1) (1 – e) (e² + e – 1) 8

Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
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show me steps of the determine green and all information is here explain to me step by step i need every details

Theorem 3.1. The system (4) has a prime period-two solutions if and only if
? +€-1+ 0,
(22)
7
is true.
Proof. First, assume that the system (4) has a distinct prime period-two solution in the follow-
ing form
..., (a1, B1), (a2, B2), (a1, B1), (a2, B2), ...
where a1 + a2 and B1 + B2. Then, from (11) and (12), we obtain
(a1 + a2) (B1 + B2)
B2 – €
(a1 + a2) (B1 + B2)
B1 – €
(a1 + a2) (B1 + B2)
(23)
a2 =
(24)
+ €,
(25)
a2 - H
(a1 + a2) (B1 + B2)
B2
+ E.
(26)
By some calculations from equations (23)-(26), we get
2με (ε-1)
e2 + € – 1
µ? (e? - (e+1)) (e² +e – 1)
(e? + € – 1)2
ai + a2 =
and a1 a2 =
B1 + B2 = 1
and B1 B2 = 0,
hence, we see that (a1 + a2)² – 4a1 a2 # 0 and (B1 + B2)2 – 4 B1 B2 # 0, which implies that
a1 7 a2 and B1 # B2. Thus,
µ (e² – (e + 1))
e2 + € – 1
µ (e? – e+ 1)
e2 + € – 1
, &2 =
B1 = 0 and B2 = 1.
(27)
Clearly a; exist if and only if e²+e-1 7 0 and they are positive if e > 1 for i = 1, 2. Secondly,
suppose that e²+ € – 1 7 0 is satisfied. Then, the system (4) has a prime period two solution
(az, 61) = (4
H(2² – (e + 1))
e2 + € – 1
H (e? – e + 1) ,1)
and (a2, B2)
e2 + € – 1
Now, we show that (w1, z1) = (a1, B1). From (4), we have
(wo + w-1) (z-1+2-2)
Wi
20 – €
(a1 + a2) (B1 + B2)
B2 - €
(2εμ(ε -
+ µH,
1
+ l,
e2 + € – 1
2εμ(ε-1)+μ (1-) (2+-1)
(1 – e) (e² + e – 1)
8
Transcribed Image Text:Theorem 3.1. The system (4) has a prime period-two solutions if and only if ? +€-1+ 0, (22) 7 is true. Proof. First, assume that the system (4) has a distinct prime period-two solution in the follow- ing form ..., (a1, B1), (a2, B2), (a1, B1), (a2, B2), ... where a1 + a2 and B1 + B2. Then, from (11) and (12), we obtain (a1 + a2) (B1 + B2) B2 – € (a1 + a2) (B1 + B2) B1 – € (a1 + a2) (B1 + B2) (23) a2 = (24) + €, (25) a2 - H (a1 + a2) (B1 + B2) B2 + E. (26) By some calculations from equations (23)-(26), we get 2με (ε-1) e2 + € – 1 µ? (e? - (e+1)) (e² +e – 1) (e? + € – 1)2 ai + a2 = and a1 a2 = B1 + B2 = 1 and B1 B2 = 0, hence, we see that (a1 + a2)² – 4a1 a2 # 0 and (B1 + B2)2 – 4 B1 B2 # 0, which implies that a1 7 a2 and B1 # B2. Thus, µ (e² – (e + 1)) e2 + € – 1 µ (e? – e+ 1) e2 + € – 1 , &2 = B1 = 0 and B2 = 1. (27) Clearly a; exist if and only if e²+e-1 7 0 and they are positive if e > 1 for i = 1, 2. Secondly, suppose that e²+ € – 1 7 0 is satisfied. Then, the system (4) has a prime period two solution (az, 61) = (4 H(2² – (e + 1)) e2 + € – 1 H (e? – e + 1) ,1) and (a2, B2) e2 + € – 1 Now, we show that (w1, z1) = (a1, B1). From (4), we have (wo + w-1) (z-1+2-2) Wi 20 – € (a1 + a2) (B1 + B2) B2 - € (2εμ(ε - + µH, 1 + l, e2 + € – 1 2εμ(ε-1)+μ (1-) (2+-1) (1 – e) (e² + e – 1) 8
In this paper, we solve and study the properties of the following system
Wn-p
Zn-h
Wn-p
Zn-h
p=0
h=1
p=1
h=0
Wn+1
+
and
Zn+1
+ €,
(4)
%3D
Zn - €
Wn - L
where u ande are arbitrary positive real numbers with initial conditions w; and z; for i =
-2, –1,0.
Let w2n-1 = Un, w2n-2 = Vn, 22n-1=
Хn and z2m-2—
Yn, implies that
Vn+1 – ko Un – ko Vn = µ,
(11)
Un+1 – ki Vn+1 – kį Un = H,
and
Yn+1 - Vo Xn – v Yn = e,
(12)
Xn+1 – Vị Yn+1 - Vị Xn = €.
It is observe that, the equations (11) and (12) are system of linear non-homogeneous difference
equations with constants coefficients. First, we solve the system in (11). Thus, consider (11) is
(E - ko) Vn – ko Un
(E – ki ) Un – ki E V,
(13)
l,
(14)
where E = A + 1, is the shift operator. Multiplying (13) and (14) by (E – k1) and ko,
respectively,
(E – ki) (E – ko) Vn – (E – ki) ko Un
(E – k1) µ,
(15)
ko (E – ki) Un – ko ki E V,
ko H.
(16)
Thus, the combination of (15) and (16) is
(E – (ko + ki + ko k1) E + ko ki) Va = (1– kı + ko) µ,
(E² – Ø E + ko ki) V = (1– kị + ko) H,
(17)
where ø = ko + kı + ko k1. Clearly, (17) is linear difference equations from order two and it is
easy to obtain the solution,
0 + Vo? – 4 ko kı
(1– k + ko
- k1
4 ko ki
Vn = A
+ B
(18)
2
- ko -
since A and B are constants. By Substituting (18) in (13), we give
1
= A
ko
$² – 4 ko k1
- 1
$+ V62 - 4 ko ki
Un
2
2 – 4 ko ki
1
6² – 4 ko ki
(19)
+ B
2
• ((-) ( .
- ki + ko
- ko – ki
ko
ko
6
Transcribed Image Text:In this paper, we solve and study the properties of the following system Wn-p Zn-h Wn-p Zn-h p=0 h=1 p=1 h=0 Wn+1 + and Zn+1 + €, (4) %3D Zn - € Wn - L where u ande are arbitrary positive real numbers with initial conditions w; and z; for i = -2, –1,0. Let w2n-1 = Un, w2n-2 = Vn, 22n-1= Хn and z2m-2— Yn, implies that Vn+1 – ko Un – ko Vn = µ, (11) Un+1 – ki Vn+1 – kį Un = H, and Yn+1 - Vo Xn – v Yn = e, (12) Xn+1 – Vị Yn+1 - Vị Xn = €. It is observe that, the equations (11) and (12) are system of linear non-homogeneous difference equations with constants coefficients. First, we solve the system in (11). Thus, consider (11) is (E - ko) Vn – ko Un (E – ki ) Un – ki E V, (13) l, (14) where E = A + 1, is the shift operator. Multiplying (13) and (14) by (E – k1) and ko, respectively, (E – ki) (E – ko) Vn – (E – ki) ko Un (E – k1) µ, (15) ko (E – ki) Un – ko ki E V, ko H. (16) Thus, the combination of (15) and (16) is (E – (ko + ki + ko k1) E + ko ki) Va = (1– kı + ko) µ, (E² – Ø E + ko ki) V = (1– kị + ko) H, (17) where ø = ko + kı + ko k1. Clearly, (17) is linear difference equations from order two and it is easy to obtain the solution, 0 + Vo? – 4 ko kı (1– k + ko - k1 4 ko ki Vn = A + B (18) 2 - ko - since A and B are constants. By Substituting (18) in (13), we give 1 = A ko $² – 4 ko k1 - 1 $+ V62 - 4 ko ki Un 2 2 – 4 ko ki 1 6² – 4 ko ki (19) + B 2 • ((-) ( . - ki + ko - ko – ki ko ko 6
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