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15. Conditional Asymptotic Stability of Integral Manifold
In this section, we establish the conditional asymptotic stability of the integral
manifold x = X(ψ, τ, ε) of system (12.1) with respect to a certain set
of initial data for slow variables. In the theorem presented below, we denote
by (xττ
0(y, ψ, ε); ϕττ
0(y, ψ, ε)) the solution of system (12.1) that takes the value
(y; ψ) for τ = τ0 and by n0 the integer number defined in Section 13.
Theorem 15.1. Suppose that the conditions of Theorem 14.1 are satisfied.
Then, for sufficiently small ε0 > 0 and any (ψ, τ0, ε) ∈ G1, in a certain neighborhood
of the point x(τ0) there exist an (n−n0)-dimensional manifold S+ and
an n0-dimensional manifold S− such that, for τ ∈ [τ0,∞) (τ ∈ (−∞, τ0]),
the solution (xττ
0(y, ψ, ε); ϕττ
0(y, ψ, ε)) of system (12.1) is defined for all y ∈ S+
(y ∈ S−), and the slow variables xττ
0(y, ψ, ε) tend exponentially to the integral
manifold x = X(ψ, τ, ε) as τ → +∞ (τ →−∞) for y ∈ S+ (y ∈ S−).
Proof. We construct a sequence {Zj(ψ, τ, ε, τ0, d)} using the recurrence
formula
Zj+1(ψ, τ, ε, τ0, d)
= Q(τ, τ0)d +
∞ _
τ0
Q(τ, t)[F(Zj, t) + _a(x(t) + Zj , ϕt
τ,j+1, t)
+ εA(x(t) + Zj , ϕt
τ,j+1, t, ε)]dt, Z0 ≡ 0, (15.1)
where
Zj = Zj(ϕt
τ,j+1, t, ε, τ0, d), Q(τ, τ0) = diag (0,Q−(τ, τ0)),
d is a constant n-dimensional vector whose first n0 coordinates are equal to zero,
ε ∈ (0, ε0], τ ≥ τ0, and ϕt
τ,j+1 = ϕt
τ,j+1(ψ, ε, d) is a solution of the Cauchy
problem
d
dt
ϕt
τ,j+1 = ω(t)
ε
+ b(x(t) + Zj , ϕt
τ,j+1, t, ε), ϕτ
τ,j+1 = ψ. (15.2)
Taking into account that Q(τ, τ0) = Q(τ, τ0) for τ > τ0, we deduce from (15.1)
that
166 Integral Manifolds Chapter 3
_Zj+1(ψ, τ, ε, τ0, d)_
≤ K_d_ + σ0 sup
ψ,τ
_Zj(ψ, τ, ε, τ0, d)_
+
2
γ
K[εσ1 + n2σ1 sup
ψ,τ
_Zj(ψ, τ, ε, τ0, d)_2]
+
_
k_=0
_ ∞_
s=−q
___
τ+_s+1
τ+s
Q(τ, t)ak(x(t), t) exp{i(k, ϕt
τ,j+1)}dt
___
+
___
_τ−q
τ0
Q(τ, t)ak(x(t), t) exp{i(k, ϕt
τ,j+1)}dt
___
_
. (15.3)
Here, q is the integer part of the number τ − τ0. Using conditions (12.2) and
(13.5) and relation (1.20), we estimate the last term on the right-hand side of
inequality (15.3) from above by the value σ4εα, where σ4 is the constant defined
in Section 13. Thus, inequality (15.3) yields
sup
ψ,τ
_Zj+1_
≤ K_d_ + σ0 sup
ψ,τ
_Zj_ +
2
γ
Kn2σ1 sup
ψ,τ
_Zj_2 +
_
σ4 +
2
γ
Kσ1
_
εα0
,
which, for ε0 ≤ (nd1)− 2
α and _d_ ≤
_
σ4K
−1 +
4
γ
σ1
_
εα0
, leads to the estimate
_Zj(ψ, τ, ε, τ0, d)_ ≤ 2
4Kσ1 + γσ4
γ(1 − σ0) εα0
= d1εα0
(15.4)
for all
j ≥ 0, (ψ, τ, ε, d) ∈ Rm × [τ0,∞) × (0, ε0] × L ≡ G2,
L =
_
d: d ∈ Rn, _d_ ≤
_
σ4K
−1 +
4
γ
σ1
_
εα0
_
,
where the first n0 coordinates of the vector d are equal to zero.
The inequality _Q(τ, t)_ ≤ Ke−γ|t−τ| and condition (12.2) guarantee that
the integral on the right-hand side of (15.1) converges uniformly for any ψ ∈ Rm,
Section 15 Conditional Asymptotic Stability of Integral Manifold 167
τ ∈ [τ0, T], ε ∈ (0, ε0], and d ∈ L (T > τ0
is arbitrary). Since Z0 ≡ 0 and
ϕt
τ,1 = ϕt
τ,1, using Lemmas 12.1–12.4 we establish the estimates
sup
G2
___
∂
∂ψ
Z1
___
≤ d2εα0
,
_m
ν=1
sup
G2
___
∂2
∂ψ∂ψν
Z1
___
≤ d3εα0
and the uniform
_
for all ψ ∈ Rm, τ ∈ [τ0, T], ε ∈ [ε0, ε0], and d ∈ L, where
T > τ0
and ε0
∈ (0, ε0) are arbitrary
_
convergence of the integrals obtained
from (15.1) for j = 0 by differentiation with respect to ψ and τ under the
integral sign. Moreover, by direct differentiation, one can verify that
∂Z1
∂τ
+ ∂Z1
∂ψ
_ω(τ )
ε
+ b(x(τ ), ψ, τ, ε)
_
= H(τ )Z1 + _a(x(τ ), ψ, τ) + εA(x(τ ), ψ, τ, ε),
Z1 = Z1(ψ, τ, ε, τ0, d),
and prove that Z1 is 2π-periodic in ψν, ν = 1,m, and twice continuously
differentiable with respect to ψ and τ for fixed ε, τ0, and d.
Using the method of mathematical induction, by analogy with Section 13 we
obtain the inequalities
___
∂
∂ψ
Zj
___
≤ d2εα0
,
_m
ν=1
___
∂2
∂ψ∂ψν
Zj
___≤
d3εα0
(15.5)
and the identity
∂Zj+1
∂τ
+ ∂Zj+1
∂τ
_ω(τ )
ε
+ b(x(τ) + Zj, ψ, τ, ε)
_
= H(τ )Zj+1 + F(Zj, τ) + _a(x(τ) + Zj, ψ, τ)
+ εA(x(τ) + Zj, ψ, τ, ε) (15.6)
for all (ψ, τ, ε, d) ∈ G2 and j ≥ 0. Furthermore, the functions Zj =
Zj(ψ, τ, ε, τ0, d) are periodic in ψν, ν = 1,m, with period 2π and twice
continuously differentiable with respect to ψ and τ for fixed ε, τ0, and d.
Moreover, according to Lemma 12.5, they satisfy estimates (14.9) and (14.10)
with Yj and G1 replaced by Zj and G2, respectively. This implies that the
168 Integral Manifolds Chapter 3
sequences {Zj} and
_ ∂
∂ψ
Zj
_
converge uniformly on the set G2, and equality
(15.6) yields the uniform convergence of the sequence
_ ∂
∂τ
Zj
_
on the set
ψ ∈ Rm, τ ∈ [τ0, T], ε∈ [ε0, ε0], d∈ L
for arbitrary T > τ0 and ε0 ∈ (0, ε0). Passing to the limit as j →∞ in (15.6),
for any (ψ, τ, ε, d) ∈ G2 we get
∂Z
∂τ
+ ∂Z
∂ψ
_ω(τ )
ε
+ b(x(τ) + Z, ψ, τ, ε)
_
= H(τ )Z + F(Z, τ) + _a(x(τ) + Z, ψ, τ) + εA(x(τ) + Z, ψ, τ, ε), (15.7)
where
Z = Z(ψ, τ, ε, τ0, d) = lim
j→∞
Zj(ψ, τ, ε, τ0, d).
Let ϕττ
0 = ϕττ
0(ψ, ε, d) denote a solution of the Cauchy problem
dϕττ
0
dτ
= ω(τ )
ε
+ b(x(τ) + Z(ϕττ
0, τ, ε, τ0, d), ϕττ
0, τ, ε),
ϕτ0
τ0 = ψ ∈ Rm.
It now follows from (15.7) that (xττ
0(ψ, ε, d); ϕττ
0(ψ, ε, d)), where xττ
0(ψ, ε, d) =
x(τ)+Z(ϕττ
0(ψ, ε, d), τ, ε, τ0, d), is a solution of system (12.1) for τ ≥ τ0, and
_xττ
0(ψ, ε, d) − x(τ )_ ≤ d1εα0
∀(ψ, τ, ε, d) ∈ G2. (15.8)
Thus, x(τ0) + Z(ψ, τ0, ε, τ0, d) ≡ S+ (for fixed ψ, τ0, and ε) is an (n −
n0)-dimensional manifold that possesses the following property: every solution
of system (12.1) with initial data from the set S+×Rm is defined for all τ ≥ τ0,
and, according to (15.8), its slow variables are uniformly bounded.
To construct the manifold S−, it is necessary to consider the following sequence
instead of the sequence {Zj} defined by (15.1) and (15.2):
_ Zj+1(ψ,τ, ε, τ0, d)
= _Q(τ, τ0)d +
_τ
−∞
Q(τ, t)[F( _ Zj, t) + _a(x(t) + _ Zj , _ϕt
τ,j+1, t)
+ εA(x(t) + _ Zj , _ϕt
τ,j+1, t, ε)]dt, _ Z0 ≡ 0,
Section 15 Conditional Asymptotic Stability of Integral Manifold 169
where τ ≤ τ0,
_ Zj = _ Zj(_ϕt
τ,j+1, t, ε, τ0, d), _Q(τ, τ0) = diag (−Q+(τ, τ0), 0),
d is a constant n-dimensional vector the last n − n0 coordinates of which are
equal to zero, and _ϕt
τ,j+1 = _ϕt
τ,j+1(ψ, ε, d) is a solution of the Cauchy problem
d_ϕt
τ,j+1
dt
= ω(t)
ε
+ b(x(t) + _ Zj , _ϕt
τ,j+1, t, ε), _ϕτ
τ,j+1 = ψ.
Then
S− = x(τ0) + lim
j→∞
_ Zj(ψ, τ0, ε, τ0, d).
We now prove the second part of the theorem. Taking into account relations
(13.7) and the equality
Q−(τ, τ0)Q−(τ0, t) = Q−(τ, t), t≤ τ0 ≤ τ,
one can represent the function Yj+1(ψ, τ, ε) for τ ≥ τ0 in the form
Yj+1(ψ, τ, ε) = Q(τ, τ0)yj+1 +
∞ _
τ0
Q(τ, t)[F(Yj, t) + _a(x(t) + Yj, ϕt
τ,j+1, t)
+ εA(x(t) + Yj, ϕt
τ,j+1, t, ε)]dt, (15.9)
where Yj = Yj(ϕt
τ,j+1, t, ε), yj+1 = yj+1(ψ, τ, ε) is the n-dimensional vector
the first n0 coordinates of which are equal to zero and the other coordinates
coincide with the vector
_τ0
−∞
Q−(τ0, t)[F−(Yj, t) + _a−(x(t) + Yj, ϕt
τ,j+1, t)
+ εA−(x(t) + Yj, ϕt
τ,j+1, t, ε)]dt.
Here, we preserve the notation of Section 13. According to inequalities (1.20),
(12.2), and (13.3), for any (ψ, τ, ε) ∈ G1 we have
_yj+1(ψ, τ, ε)_ ≤
_ 1
γ
(n2d21
σ1εα0
+ σ1)K +
1
2σ0d1 + σ4
_
εα < d1εα.
170 Integral Manifolds Chapter 3
Now consider the inequality
_Zj+1(ψ, τ, ε, τ0, d) − Yj(ψ, τ, ε)_
≤ Ke
−γ(τ−τ0)_d − yj+1(ψ, τ, ε)_
+
____
_−∞
τ0
Q(τ, t){[Fj − Fj] + [_aj − _aj] + ε[Aj − Aj ]}dt
____
, (15.10)
which follows from (15.1) and (15.9). In this inequality, Fj , _aj , and Aj have
the same meaning as in (14.1), and
Fj = F(Zj, t), _aj = _a(x(t) + Zj , ϕt
τ,j+1, t),
Aj = A(x(t) + Zj , ϕt
τ,j+1, t, ε), Zj = Zj(ϕt
τ,j+1, t, ε, τ0, d).
For the difference _aj−_aj , we use a representation of the form (14.2) with Zj
instead of Yj−1. Then, taking into account conditions (12.2), (13.13), and (15.5),
we deduce from (15.10) the following inequality:
_Zj+1(ψ, τ, ε, τ0, d) − Yj(ψ, τ, ε)_
≤ 2d1εα0
Ke
−γ(τ−τ0) + K
∞ _
τ0
e
−γ|τ−t|
__
(md1 + 3nd1 + 1)nσ1εα0
+ sup
ψ,τ
___
∂_a(x(τ ), ψ, τ)
∂x
___
_
_Zj − Yj_
+ εα0
(m + n(m + n)d1)σ1_ϕt
τ,j+1
− ϕt
τ,j+1
_
_
dt
+
_
k_=0
____
_τ−q
τ0
Q(τ, t)ak(x(t), t)(exp{i(k, θ
t
τ,j+1)}
− exp{i(k, θt
τ,j+1)}) exp
_ i
ε
(k,
_t
τ
ω(r)dr)
_
dt
___
Section 15 Conditional Asymptotic Stability of Integral Manifold 171
+
∞_
s=−q
___
τ+_s+1
τ+s
Q(τ, t)ak(x(t), t)(exp{i(k, θ
t
τ,j+1)}
− exp{i(k, θt
τ,j+1)}) exp
_ i
ε
_
k,
_t
τ
ω(r)dr
__
dt
___
_
, (15.11)
where q is the integer part of the number τ − τ0 and
θ
t
τ,j+1 = ϕt
τ,j+1
− 1
ε
_t
τ
ω(r)dr.
Denote
Mj = sup
τ∈[τ0,∞)
[e
γ
l (τ−τ0)pj(τ, ε)], l=
⎧⎪⎨
⎪⎩
2, σ0 = 0,
_
1 +
2σ0
1 − σ0
_1
2, σ0 > 0,
pj(τ, ε) = sup
ψ∈Rm
_Zj(ψ, τ, ε, τ0, d) − Yj(ψ, τ, ε)_.
It is clear that
pj(τ, ε) ≤ Mje
γ
l (τ−τ0) ∀τ ≥ τ0,
∞ _
τ0
e
−γ_τ−t_
pj(t, ε)dt ≤ 2l2
γ(l2 − 1)Mje
−γ
l (τ−τ0). (15.12)
To estimate _ϕt
τ,j+1
− ϕt
τ,j+1
_ ≡ Δϕj+1, we use Lemma 12.5. As a result, we
get
Δϕj+1 ≤ σ8e
γ
2
l−1
l
|t−τ| max
ξ∈N(τ,t)
pj(ξ, ε)
for c19εα0
≤ γ(l − 1)
4l
and σ8 = c18 max
_
1;
4l
γ(l − 1)
_
. If t < τ, then
max
ξ∈[t,τ ]
pj(ξ, ε) ≤ e
−γ
l (t−τ0) max
ξ∈[t,τ ]
[e
−γ
l (ξ−τ0)pj(ξ, ε)] ≤ Mje
−γ
l (t−τ0);
if t ≥ τ, then
max
ξ∈[τ,t]
pj(ξ, ε) ≤ Mje
−γ
l (τ−τ0).
172 Integral Manifolds Chapter 3
Taking this arguments into account, we obtain
_ϕt
τ,j+1
− ϕt
τ,j+1
_ ≤ σ8e
γ
2
l−1
l
|t−τ|− γ
l (min{τ;t}−τ0),
∞ _
τ0
e
−γ|τ−t|_ϕt
τ,j+1
− ϕt
τ,j+1
_dt ≤ σ8
4l2
γ(l2 − 1)Mje
−γ
l (τ−τ0). (15.13)
Then it follows from (15.12) and (15.13) that
∞ _
τ0
e
−γ|τ−t|_Zj(ϕt
τ,j+1, t, ε, τ0, d) − Yj(ϕt
τ,j+1, t, ε)_dt
≤ 2l2
γ(l2 − 1)
(1 + 2σ8d2εα0
)Mje
−γ
l (τ−τ0). (15.14)
According to (1.20) and (14.8), each of the integrals over the segments [τ +s, τ +
s + 1] and [τ0, τ − q] on the right-hand side of (15.11) can be estimated from
above by the value
σ3K(1 + nσ1 + σ1 + mσ1)εα0
max
t
e
−γ|t−τ|
×
_
_k_ sup
G
_ak_ + sup
G
___
∂ak
∂τ
___
+ sup
G
___
∂ak
∂x
___
_
×
_
max
t
_ϕt
τ,j+1
− ϕt
τ,j+1
_(1 + d2εα0
) + max
t
p(t, ε)
_
, (15.15)
where ak = ak(x, τ ) and the maximum with respect to t is taken over all t ∈
[τ + s, τ + s + 1] or t ∈ [τ0, τ − q], depending on which integral is considered.
Therefore, taking into account conditions (12.2) for the Fourier coefficients of the
function _a(x, ϕ, τ ) and inequalities (15.12), (15.13) and (15.15), we can estimate
the last of the three terms on the right-hand side of (15.11) by the value
σ13εα0Mje
−γ
l (τ−τ0),
where
σ_____________13 = 4eγ
_
1 − e
γ(l−1)
2l
_−1
Kσ3(2 + d2εα0
)(1 + σ8)(1 + σ1(1 + n + m))σ1.
Thus, with regard for inequalities (15.13) and (15.14), inequality (15.11) takes the
form
Mj+1 ≤ 2Kd1εα0
+
_
σ14εα0
+ σ0
l2
l2 − 1
_
Mj, j≥ 0. (15.16)
Section 15 Conditional Asymptotic Stability of Integral Manifold 173
Here,
σ14 = σ13 +
2l2
γ(l2 − 1)K[2(m + (n + m)n)σ1σ8
+ nσ1(1 + md1 + 3nd1)(1 + 2σ8d2)] + γK
−1σ8d2σ0.
Since σ0
l2
l2 − 1
≤ 1 + σ0
2
and M0 = 0, for σ14εα0
≤ 1 − σ0
4
relation
(15.16) yields
Mj ≤ 8
1 − σ0
Kd1εα0
∀j ≥ 0,
or
_Zj(ψ, τ, ε, τ0, d) − Yj(ψ, τ, ε)_ ≤ 8
1 − σ0
Kd1εα0
e
−γ
l (τ−τ0) (15.17)
for all (ψ, τ, ε, d) ∈ G2 and j ≥ 0. Passing to the limit as j → ∞ in (15.17),
we get
_Z(ψ, τ, ε, τ0, d) − Y (ψ, τ, ε)_ ≤ 8
1 − σ0
Kd1εα0
e
−γ
l (τ−τ0)
for ψ ∈ Rm, τ ≥ τ0, ε ∈ (0, ε0], and d ∈ L. Hence, as τ → ∞, the
slow variables xττ
0(ψ, ε, d) = x(τ) + Z(ϕττ
0(ψ, ε, d), τ, ε, τ0, d) of the solution
(xττ
0(ψ, ε, d); ϕττ
0(ψ, ε, d)) of system (12.1) tend exponentially to the curve x =
x(τ)+Y (ϕττ
0(ψ, ε, d), τ, ε), which lies on the integral manifold x = X(ψ, τ, ε).
By analogy, one can establish that, as τ → −∞,
the slow variables of every
solution of system (12.1) with initial data from the set S− × Rm tend exponentially
to the integral manifold. Theorem 15.1 is proved.
Remark 2. Inequality (15.8) can be regarded as an error estimate of the averaging
method on the semiaxis [τ0,∞) under the condition xτ0
τ0(ψ, ε, d) ∈ S+.
Remark 3. Theorem 15.1 remains true for n0 = 0. In this case, the integral
manifold x = X(ψ, τ, ε) of system (12.1) is asymptotically stable for all initial
values of the slow variable x from a certain small neighborhood of the point
X(ψ, τ0, ε).
174 Integral Manifolds Chapter 3
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