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First Order Differential Equations Systems

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Dynamical Systems
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Abstract

A typical system of n first order differential equations is of the form

$$\dot{x}(t) = A(t)x(t) + b(t); x(0) = {{x}_{0}}$$
((5.1))

when A(t) is in general an n × n time variant coefficient matrix and b(t) a time variant n-vector. The constant coefficient case emerges as a particular one in which A and b are constant. The system (5.1) is homogeneous if b = 0 and non-homogeneous if b ≠ 0. The solution of the homogeneous part, = Ax is called the general solution of the complementary function, x c (t) and the solution that fits (5.1) is called the particular integral (x p ) or equilibrium solution (x e ). The combination of the two, x(t) = x c (t) + x e , gives the complete solution of (5.1). In general, if vectors x1, x2,…, xn are each a solution of (5.1), so is their linear combination

$$x\left( t \right) = {c_1}{x^1}\left( t \right) + {c_2}{x^2}\left( t \right) + \cdots + {c_n}{x^n}\left( t \right).$$
((5.2))

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© 1994 Springer-Verlag Berlin · Heidelberg

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Tu, P.N.V. (1994). First Order Differential Equations Systems. In: Dynamical Systems. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-78793-5_5

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  • DOI: https://doi.org/10.1007/978-3-642-78793-5_5

  • Publisher Name: Springer, Berlin, Heidelberg

  • Print ISBN: 978-3-540-57661-7

  • Online ISBN: 978-3-642-78793-5

  • eBook Packages: Springer Book Archive

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