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Titlebook: Difference Equations and Their Applications; A. N. Sharkovsky,Yu. L. Maistrenko,E. Yu. Romanenk Book 1993 Springer Science+Business Media

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https://doi.org/10.1007/978-3-7091-6441-9 mathematical models of a number of real phenomena (Heiden and Mackey (1982)). The outward simplicity of (3.1) conceals a complicated dynamics, which has not been clarified completely till now. However, the results concerning local stability (instability) of a stationary solution are well-known (Pes
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Some Current Issues in Gauge Theories,which is based on the reduction of the original problem to a difference (differential-difference) equation or to an equation of another type (with one independent variable). This method can be also applied to many-dimensional hyperbolic systems, the investigation of which is of particular importance
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Wadi Ad Dawasir and Its Hinterland current .(., τ) and a voltage .(., τ) (0 ≤.≤ . is a coordinate of a point on a line; τ ≥ 0 is the time) in a circuit consisting of a long line with a tunnel diode are governed by the system of telegraph equations which has (for a lossless line) the form.with . and . being, respectively, the specific inductance and capacitance of the line.
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Nonlinear Difference Equationsction, .(.): ℝ. → . is an unknown function, and . ∈ ℝ. is some closed bounded interval. We are interested in the investigation of the behavior of solutions to eqn. (1.1) as . →+ ∞ depending on the function . and the initial data
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Reduction of Boundary Value Problems to Difference and Differential-Difference Equations current .(., τ) and a voltage .(., τ) (0 ≤.≤ . is a coordinate of a point on a line; τ ≥ 0 is the time) in a circuit consisting of a long line with a tunnel diode are governed by the system of telegraph equations which has (for a lossless line) the form.with . and . being, respectively, the specific inductance and capacitance of the line.
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