Functional differential equation explained

A functional differential equation is a differential equation with deviating argument. That is, a functional differential equation is an equation that contains a function and some of its derivatives evaluated at different argument values.[1]

Functional differential equations find use in mathematical models that assume a specified behavior or phenomenon depends on the present as well as the past state of a system.[2] In other words, past events explicitly influence future results. For this reason, functional differential equations are more applicable than ordinary differential equations (ODE), in which future behavior only implicitly depends on the past.

Definition

Unlike ordinary differential equations, which contain a function of one variable and its derivatives evaluated with the same input, functional differential equations contain a function and its derivatives evaluated with different input values.

f'(x)=2f(x)+1

f'(x)=2f(x+3)-[f(x-1)]2

The simplest type of functional differential equation called the retarded functional differential equation or retarded differential difference equation, is of the form[3]

x'(t)=fl(t,x(t),x(t-r)r)

Examples

The simplest, fundamental functional differential equation is the linear first-order delay differential equation[4] which is given by

x'(t)=\alpha1x(t)+\alpha2x(t-\tau)+f(t),t\geq0

where

\alpha1,\alpha2,\tau

are constants,

f(t)

is some continuous function, and

x

is a scalar. Below is a table with a comparison of several ordinary and functional differential equations.
Ordinary differential equationFunctional differential equation
Examples

f'(x)=x2-3

f'(x)=3x-f(x-4)

f'(x)=f(x)-8

x'(t)=3x(2t)-l[x(t-1)r]2

Fl(t,x(t),x'(t),x''(t)r)=0

2x(3t+1)-5x(4t)=1

f'(x)=4f(x)-3x

Types of functional differential equations

"Functional differential equation" is the general name for a number of more specific types of differential equations that are used in numerous applications. There are delay differential equations, integro-differential equations, and so on.

Differential difference equation

Differential difference equations are functional differential equations in which the argument values are discrete. The general form for functional differential equations of finitely many discrete deviating arguments is

x(n)(t)=fl(t,

(n1)
x

l(t-\tau1(t)r),

(n2)
x
(nk)
l(t-\tau
2(t)r),\ldots,x

l(t-\tauk(t)r)r)

where

x(t)\in\Rm,n1,n2,\ldots,ni\geq0,

and

\tau1(t),\tau2(t),\ldots,\taui(t)\geq0

Differential difference equations are also referred to as retarded, neutral, advanced, and mixed functional differential equations. This classification depends on whether the rate of change of the current state of the system depends on past values, future values, or both.[5]

Classifications of differential difference equations[6]
Retarded

x'(t)=fl(t,x(t),x(t-\tau)r)

Neutral

x'(t)=fl(t,x(t),x(t-\tau),x'(t-\tau)r)

Advanced

x'(t-\tau)=fl(t,x(t),x(t-\tau)r)

Delay differential equation

See main article: Delay differential equation. Functional differential equations of retarded type occur when

max\{n1,n2,\ldots,nk\}<n

for the equation given above. In other words, this class of functional differential equations depends on the past and present values of the function with delays.

A simple example of a retarded functional differential equation is

x'(t)=-x(t-\tau)

whereas a more general form for discrete deviating arguments can be written as

x'(t)=fl(t,xl(t-\tau1(t)r),xl(t-\tau2(t)r),\ldots,xl(t-\tauk(t)r)r).

Neutral differential equations

Functional differential equations of neutral type, or neutral differential equations occur when

max\{n1,n2,\ldots,nk\}=n.

Neutral differential equations depend on past and present values of the function, similarly to retarded differential equations, except it also depends on derivatives with delays. In other words, retarded differential equations do not involve the given function's derivative with delays while neutral differential equations do.

Integro-differential equation

See main article: Integro-differential equation. Integro-differential equations of Volterra type are functional differential equations with continuous argument values. Integro-differential equations involve both the integrals and derivatives of some function with respect to its argument.

The continuous integro-differential equation for retarded functional differential equations,

x'(t)=fl(t,x(t-\tau1(t)),x(t-\tau2(t)),\ldots,x(t-\tauk(t))r)

, can be written as
t
x'(t)=fl(t,\int
t-\tau(t)

K(t,\theta,x(\theta))d\thetar),\tau(t)\geq0

Application

Functional differential equations have been used in models that determine future behavior of a certain phenomenon determined by the present and the past. Future behavior of phenomena, described by the solutions of ODEs, assumes that behavior is independent of the past. However, there can be many situations that depend on past behavior.

FDEs are applicable for models in multiple fields, such as medicine, mechanics, biology, and economics. FDEs have been used in research for heat-transfer, signal processing, evolution of a species, traffic flow and study of epidemics.

Population growth with time lag

A logistic equation for population growth is given by = \rho\,x(t)\left(1- \frac k \right),where ρ is the reproduction rate and k is the carrying capacity.

x(t)

represents the population size at time t, and \rho \left(1- \frac \right) is the density-dependent reproduction rate.[7]

If we were to now apply this to an earlier time

t-\tau

, we get = \rho\,x(t) \left(1- \frac k \right)

Mixing model

Upon exposure to applications of ordinary differential equations, many come across the mixing model of some chemical solution.

Suppose there is a container holding liters of salt water. Salt water is flowing in, and out of the container at the same rate

r

of liters per second. In other words, the rate of water flowing in is equal to the rate of the salt water solution flowing out. Let

V

be the amount in liters of salt water in the container and

x(t)

be the uniform concentration in grams per liter of salt water at time

t

. Then, we have the differential equation[8] x'(t)=-\frac r V x(t), \frac r V > 0

The problem with this equation is that it makes the assumption that every drop of water that enters the contain is instantaneously mixed into the solution. This can be eliminated by using a FDE instead of an ODE.

Let

x(t)

be the average concentration at time

t

, rather than uniform. Then, let's assume the solution leaving the container at time

t

is equal to

x(t-\tau),\tau>0

, the average concentration at some earlier time. Then, the equation is a delay-differential equation of the formx'(t)=- \frac x(t-\tau)

Volterra's predator-prey model

The Lotka–Volterra predator-prey model was originally developed to observe the population of sharks and fish in the Adriatic Sea; however, this model has been used in many other fields for different uses, such as describing chemical reactions. Modelling predatory-prey population has always been widely researched, and as a result, there have been many different forms of the original equation.

One example, as shown by Xu, Wu (2013),[9] of the Lotka–Volterra model with time-delay is given below:p'(t)=p(t)\Biggl[r_1(t)-a_{11}(t)p\biggl(t-\tau_{11}(t)\biggr)-a_{12}(t)P_1\biggl(t-\tau_{12}(t)\biggr)-a_{13}(t)P_2\biggl(t-\tau_{13}(t)\biggr)\Biggr]P_1'(t)=P_1(t)\Biggl[-r_2(t)+a_{21}(t)p\biggl(t-\tau_{21}(t)\biggr)-a_{22}(t)P_1\biggl(t-\tau_{22}(t)\biggr)-a_{23}(t)P_2\biggl(t-\tau_{23}(t)\biggr)\Biggr]P_2'(t)=P_2(t)\Biggl[-r_2(t)+a_{31}(t)p\biggl(t-\tau_{31}(t)\biggr)-a_{32}(t)P_1\biggl(t-\tau_{32}(t)\biggr)-a_{33}(t)P_2\biggl(t-\tau_{33}(t)\biggr)\Biggr]where

p(t)

denotes the prey population density at time t,

P1(t)

and

P2(t)

denote the density of the predator population at time

t,ri,aij\inC(\R,[0,infty))

and

\tauij\inC(\R,\R)

Other models using FDEs

Examples of other models that have used FDEs, namely RFDEs, are given below:

See also

Further reading

Notes and References

  1. Book: Applied Theory of Functional Differential Equations. Kolmanovskii. V.. Myshkis. A.. Kluwer Academic Publishers. 1992. 0-7923-2013-1. The Netherlands. Myshkis, Anatoliĭ Dmitrievich.
  2. Book: Hale, Jack K.. Functional Differential Equations. Springer-Verlag. 1971. 0-387-90023-3. United States.
  3. Book: Introduction to Functional Differential Equations. Hale. Jack K.. Verduyn Lunel. Sjoerd M.. Springer-Verlag. 1993. 0-387-94076-6. United States.
  4. Web site: Falbo. Clement E.. Some Elementary Methods for Solving Functional Differential Equations. https://web.archive.org/web/20161220114251/http://www.mathfile.net/hicstat_FDE.pdf . 2016-12-20 .
  5. Book: Bifurcation Theory of Functional Differential Equations. Guo. S.. Wu. J.. Springer. 2013. 978-1-4614-6991-9. New York. 41–60.
  6. Book: Differential-Difference Equations. limited. Bellman. Richard. Cooke. Kenneth L.. Academic Press. 1963. 978-0124109735. New York, NY. 42–49.
  7. Book: Mathematical Modelling with Case Studies. Barnes. B.. Fulford. G. R.. Taylor & Francis Group LLC. 2015. 978-1-4822-4772-5. 75–77.
  8. Book: Delay and Functional Differential Equations and Their Applications . Academic Press . 1972 . Schmitt . Klaus . Klaus Schmitt . United States.
  9. Xu. Changjin. Wu. Yusen. 2013. Dynamics in a Lotka–Volterra Predator–Prey Model with Time-varying Delays. Abstract and Applied Analysis. 2013. 1–9. 10.1155/2013/956703. free.
  10. García López . Álvaro . On an electrodynamic origin of quantum fluctuations . Nonlinear Dynamics . 1 September 2020 . 102 . 1 . 621–634 . 10.1007/s11071-020-05928-5 . 2001.07392 . 210838940 .