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Delay differential equation

 
Wikipedia: Delay differential equation
 

In mathematics, delay differential equations (DDEs) are a type of differential equation in which the derivative of the unknown function at a certain time is given in terms of the values of the function at previous times.

A general form of the time-delay differential equation for x(t)\in R^n is

\frac{d}{dt}x(t)=f(t,x(t),x_t),

where x_t=\{x(\tau):\tau\leq t\} represents the trajectory of the solution in the past. In this equation, f is a functional operator from R\times R^n\times C^1 to R^n.\,

The following form is called — after the pantographs on trains — the pantograph equation:

\frac{d}{dt}x(t) = ax(t) + bx(\lambda t),

where a, b and λ are constants and 0 < λ < 1. Often some more general forms of this equation are used, also being called pantograph equation.

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Examples

  • Continuous delay
\frac{d}{dt}x(t)=f\left(t,x(t),\int_{-\infty}^0x(t+\tau)d\mu(\tau)\right)
  • Discrete delay
\frac{d}{dt}x(t)=f(t,x(t),x(t-\tau_1),\ldots,x(t-\tau_n)) for \tau_1>\ldots>\tau_n\geq 0.

Reduction to ODE

In some cases, delay differential equations are equivalent to a system of ordinary differential equations.

  • Example 1 Consider an equation

\frac{d}{dt}x(t)=f\left(t,x(t),\int_{-\infty}^0x(t+\tau)e^{\lambda\tau}d\tau\right).
Introduce y(t)=\int_{-\infty}^0x(t+\tau)e^{\lambda\tau}d\tau to get a system of ODEs

\frac{d}{dt}x(t)=f(t,x,y),\quad \frac{d}{dt}y(t)=x-\lambda y.
  • Example 2 An equation

\frac{d}{dt}x(t)=f\left(t,x(t),\int_{-\infty}^0x(t+\tau)\cos(\alpha\tau+\beta)d\tau\right)
is equivalent to

\frac{d}{dt}x(t)=f(t,x,y),\quad \frac{d}{dt}y(t)=\cos(\beta)x+\alpha z,\quad \frac{d}{dt}z(t)=\sin(\beta) x-\alpha y,
where

y=\int_{-\infty}^0x(t+\tau)\cos(\alpha\tau+\beta)d\tau,\quad z=\int_{-\infty}^0x(t+\tau)\sin(\alpha\tau+\beta)d\tau.

The characteristic equation

Solutions of linear DDEs can be studied by analyzing the characteristic equation, similarly to the ODEs. However, for DDEs, the characteristic equation has an (countably) infinite number of solutions, making the spectral analysis hard. Consider, for example, the following equation:

\frac{d}{dt}x(t)=-x(t-1).

As for ODEs, we seek a solution of the form x(t) = eλt. This results in the characteristic equation for λ:

\lambda=-e^{-\lambda}.\,

There are an infinite number of solutions to this equation for complex λ (they are given by the Lambert W function).

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