Latest revision as of 16:32, 9 February 2017

Let $\mathbb{T}$ be a time scale. Dynamic equations are a generalization and extension of differential equations and difference equations.

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-Dynamic equations are analogues of differential equations on a [[time scale]]. If we have $\mathbb{T}=\mathbb{R}$ then the resulting theory of dynamic equations is the thoery of differential equations. If $\mathbb{T}=h\mathbb{Z}$ then the resulting theory of dynamic equations is the theory of difference equations of stepsize $h$.
+Let $\mathbb{T}$ be a [[time scale]]. Dynamic equations are a generalization and extension of [[differential equation|differential equations]] and [[difference equation|difference equations]].
-Suppose that $f \colon \mathbb{T} \times \mathbb{R}^2 \rightarrow \mathbb{R}$. Then the equation
+=See Also=
-$$y^{\Delta} = f(t,y,y^{\sigma})$$
+[[Delta exponential dynamic equation]]<br />
-is called a first order dynamic equation.
+[[First order dynamic equations]]<br />
+[[Second order dynamic equations]]<br />
-Suppose there are [[continuity | rd-continuous]] functions $p_i \colon \mathbb{T} \rightarrow \mathbb{R}$. Define the operator
-$$Ly=y^{\Delta^n}+\displaystyle\sum_{k=1}^n p_i y^{\Delta^{n-i}}.$$
-We say that the equation $Ly=f$ is an $n$th order dynamic equation.

Difference between revisions of "Dynamic equation"