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準周期的Duffing方程式の解の存在と一意性および近似解の精度保証について (精度保証付き数値計算法とその周辺)

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(1)

準周期的

Duffing 方程式の解の存在と

意性および近似解の

精度保証について

By

篠原能州 (Yosんitane $SHINoHARA*$),今井仁司 (Hitoshi $IMAI^{**}$),

竹内敏己 (Toshiki $TAKEUCHI**$), 蔭西義輝 (Yoshiteru $KAGENIsHI^{*}$)

( $\mathrm{i}\mathrm{k}_{0}\mathrm{k}\mathrm{u}$ University; **The University ofTokushima)

The present paper is concerned with the existence and uniqueness of the quasiperiodic

solutions to the Duffing’s General Type equation

(1) $\frac{d^{2}x}{dt^{2}}+2\mu\frac{dx}{dt}+\nu\epsilon X^{3}+2_{X=}\sum_{k=1}m(ak\cos\nu_{k}t+b_{k}\sin\nu_{k}t)$ ,

where $\mu,$$\nu,$$\nu_{k}=2\pi/w_{k}$ and, $w_{k}(k=1,2, \ldots,m)$ are all positive, and $1/w_{k}$ are rationally

linearly independent. Putting $y=dx/dt$,

$z=$

,

$A=$

,

$\phi(t)=$

,

$\eta(z)=$

,

the equation (1) can be written in the vector form as follows:

(2) $\frac{dz}{dt}=Az+\phi(t)+\epsilon\eta(z)$

.

The lineardifferential equation

(3) $Lz=\phi(t)$, $L= \frac{d}{dt}-A$

satisfies the generalized exponential dichotomy for $\mu\neq 0$

.

Let $\Phi(t)$ be the fundamental

matrix of the equation $Lz=0$ such that $\Phi(0)=E$ (unit matrix)

,

we have

(4) $||\Phi(t)||\leq K_{0}e^{-\sigma_{\circ}t}$

.

In the paper we use the $p_{\infty}$

-norm

$||\cdot||$ in Euclidean space and denote that $||f||= \sup_{t\in R}||$

$f(t)||$ for any bounded function $f=f(t)$

.

数理解析研究所講究録

(2)

Then there exist a projection matrix $P$ (Duffing: $P=E$) , positive numbers

$\sigma_{1},$$\sigma_{2}$ and

non-negative functions $C_{1}(t, s),c2(t, S)$ such that

(5) $\{$

(i) $P^{2}=P$

(ii) $||\Phi(t)P\Phi^{-}1(s)||\leq C_{1}(t, \mathit{8})e^{-}\sigma_{1}(\iota-s)$

for

$t\geq s$, (iii) $||\Phi(t)(E-P)\Phi^{-1}(s)||\leq C_{2}(t, s)e^{-\sigma \mathrm{t}}2s-t)$

for

$t<s$,

(iv) $\int_{-\infty}^{\ell}c_{1}(t, S)e-\sigma 1(t-\mathit{8})ds+\int_{t}^{+\infty}c_{2}(t, s)e-\sigma_{2}1^{s}-\ell)ds$ $\leq M$,

where $M=$ . $\frac{K_{0}}{\mu-\sqrt{\mu^{2}-\nu^{2}}}$ if$\mu>\nu>0$, $\int_{-\infty}^{t}IC_{0}(t-s)e-\mu \mathrm{t}t-s\rangle ds$ if $\mu=\nu$, $\tau$ $\frac{K_{0}}{\mu}$ if$0<\mu<\nu$

.

Theorem 1 Consider a nonlinear

differential

equation

(6) $\frac{dz}{dt}=X(t, z)$,

where $z$ and$X(t, z)$ are vectors and$X(t, z)$ is quasiperiodic in$t$ withperiods

$w_{1},w_{2},$$\ldots,$$w_{m}$

and is continuously

differentiable

with respect to $z$ belonging to a region $D$

of

z-8pace.

Suppose that there is a continuously

differentiable

quasiperiodic

function

$z_{0}(t)$ with

periods $w_{1},w_{2},$$\ldots,$$w_{m}$ such that

$\{$

$z_{0}(t)\in D$,

$|| \frac{dz_{0}(t)}{dt}-X[t, z0(t)]||\leq r$,

for

all $t\in R$

.

Further suppose that there are a positive number $\delta$, a non-negative number $\kappa<1$ and a

quasiperiodic matrix$A(t)$ with periods $w_{1},$ $w_{2},$$\ldots,$$w_{m}$ such that

(i) the equation (3)

satisfies

a generalized exponential dichotomy,

(ii) $D_{\delta}=$

{

$z;||z-z_{0}(t)|\iota\leq\delta$

for

some $t\in R$

}

$\subset D$,

(iii) $||\Psi(t, z)-A(t)||\leq\overline{M}$ whenever $||z-z\mathrm{o}(t)||\leq\delta$,

and

(iv) $\frac{Mr}{1-\kappa}\leq\delta$,

(3)

where $\Psi(t, z)i_{\mathit{8}}$ the Jacobian matrix

of

$X(t, z)$ with respect to $z$

.

Then the equation (6) $pos\mathit{8}eSses$ a solution $z=\hat{z}$ quasiperiodic in $t$ with periods

$w_{1},w_{2},$$\ldots,$$w_{m}$ such that

(7) $||z_{\mathrm{o}(t)-\hat{Z}()||\leq}t \frac{Mr}{1-\kappa}$

.

for

all $t\in R.$ Furthermore, to the equation (6) there is no other quasiperiodic $\mathit{8}oluti_{\mathit{0}}n$

belonging to $D_{\delta}$ besides $z=\hat{z}(t)$

.

Let $z_{0}(t)$ be the quasiperiodic solution to the linear equation (3) and bounded by $K$ as

$||z_{0}(t)||\leq K$

.

Theorem 2

If

$the1$ parameter

$\epsilon sa\iota isfieS$ the inequality

(8) $|\epsilon|\leq\overline{13K^{2}M}$

the equation (1) possesses a $quasipe\dot{n}odi_{C}$ solution$z=\hat{z}(t)$ with period8$w_{1},$ $w_{2},$$\ldots,$$w_{m}$ such

that

(9) $||z_{0}(t)-\hat{Z}(t)||\leq K$

for

all $t\in R$

.

If the inequality (8) does not hold, or the error estimation (9) is too crude, we should

compute a

more

accurate approximation than $z_{0}(t)$

.

For this purpose the Galerkin method

is usefull.

Starting from the solution $z=z_{0}(t)$ of the equation (3), we can compute the following

Galerkin approximation of n-th order to the solution $x(t)$ of the equation (1) :

(10) $x_{n}(t)= \alpha(\mathrm{o},\mathrm{o})+\sum_{r=1}n\mathrm{I}\mathrm{P}\sum_{|=t}\{\alpha_{\mathrm{P}}cos(p, \nu)t+\beta_{p}sin(p, \nu)t\}$,

$(p, \nu)=\sum_{k=1}pk\nu mk,$ $|p|=k=1 \sum|mp_{k}|$

.

Theorem 1 in the paper makes us to veryfy the existence and uniqueness of an exact

quasiperiodic solution and know the error bound of the approximation (10) to the

quasiperi-odic solution of Duffing’s general type equation (1) which is a fundamental equation in

nonlinear oscillations.

(4)

参考文献

[1] Y.Shinohara,Investigationof the quasiperiodic solutions to Duffing’s general

type equations, Bulletin ofthe Faculty of Engineering,The University

ofTokushima,Vol.44(1999),1-13.

参照

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