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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Acta mathematicae applicatae sinica 9 (1993), S. 317-327 
    ISSN: 1618-3932
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract It is well known, that in the theory of stability in differential equations, Liapunov's second method may be the most important. The center problem of Liapunov's second method is construction of Liapunov function for concrete problems. Beyond any doubt, construction of Liapunov functions is an art. In the case of functional differential equations, there were also many attempts to establish various kinds of Liapunov type theorems. Recently Burton [2] presented an excellent theorem using the Liapunov functional to solve the asymptotic stability of functional differential equation with bounded delay. However, the construction of such a Liapunov functional is still very hard for concrete problems. In this paper, by utilizing this theorem due to Burton, we construct concrete Liapunov functional for certain and nonlinear delay differential equations and derive new sufficient conditions for asymptotic stability. Those criteria improve the result of literature [1] and they are with simple forms, easily checked and applicable.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Acta mathematicae applicatae sinica 10 (1994), S. 48-58 
    ISSN: 1618-3932
    Keywords: Unbounded delay ; exponential stability ; large scale system
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract In this paper, we first give a sufficient and necessary condition to guarantee the exponential stability of a special system with unbounded delay, then by using the delay-differential comparison theorem, obtain some simple criteria for the exponential stability of large scale systems with unbounded delay.
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Acta mathematicae applicatae sinica 4 (1988), S. 223-233 
    ISSN: 1618-3932
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract In recent ten years or more, many scholars have engaged in the investigation concerning the stability of large-scale systems, but up to the present, the problem on the existence of periodic solutions for large-scale systems has yet been seldomly touched upon in the literature. In this paper, by means of the method of constructing Lyapunov function. We study the problem on the existence of periodic solutions for linear and nonlinear large-scale systems, and obtain several sufficient conditions which guarantee the existence of periodic solutions.
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Acta mathematicae applicatae sinica 8 (1992), S. 82-96 
    ISSN: 1618-3932
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract In this paper, we discuss the problem of stability of Volterra integrodifferential equation (1) $$\dot x = A(t)x + \int_0^t {C(t,s)} x(s)ds$$ with the decomposition (2) $$\begin{gathered} \dot x_i = A_{ii} (t)x_i + \sum\limits_{\mathop {i = 1}\limits_{j \ne i} }^r {A_{ij} (t)x_j + \int_0^t {\left[ {C_{ii} (t,s)x_i (s) + \sum\limits_{\mathop {j = 1}\limits_{j \ne i} }^r {C_{ij} (t,s)x_j (s)} } \right]} ds,} \hfill \\ i = 1,2, \cdot \cdot \cdot ,r, \hfill \\ \end{gathered} $$ wherex ∈R n,x T=(x 1 T , ...,x r/T),x i ∈R ni and ∑ i=1 r n i=n;A(t)=(A ij(t)) in whichA ij(t) (i,j=1, ...,r) is ann i ×n j matrix of functions continuous for 0 ≤t〈∞;C(t,s)=(C ij (t,s,)) in whichC ij(t,s)(i,j=1, ...,r) is ann i ×n j matrix of functions continuous for 0≤s≤t〈∞. According to the decomposition theory of large scale system and with the help of Liapunov functional, we give a criterion for concluding that the zero solution of (2) (i.e. large scale system (1)) is uniformly asymptotically stable. We also discuss the large scale system (3) $$\dot x = A(t)x + \int_0^t {C(t,s)} x(s)ds + f(t)$$ with the decomposition (4) $$\begin{gathered} \dot x_i = A_{ii} (t)x_i + \sum\limits_{\mathop {i = 1}\limits_{j \ne i} }^r {A_{ij} (t)x_j + \int_0^t {\left[ {C_{ii} (t,s)x_i (s) + \sum\limits_{\mathop {j = 1}\limits_{j \ne i} }^r {C_{ij} (t,s)x_j (s)} } \right]} ds + f_i (t),} \hfill \\ i = 1,2, \cdot \cdot \cdot ,r, \hfill \\ \end{gathered} $$ and give a criterion for determining that the solutions of (4) (i.e. large scale system (3)) are uniformly bounded and uniformly ultimately bounded. Those criteria are of simple forms, easily checked and applied.
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