Initial value problem
An initial value problem[a] is an ordinary differential equation together with an initial condition which specifies the value of the unknown function at a given point in the domain. Modeling a system in physics or other sciences frequently amounts to solving an initial value problem. In that context, the differential initial value is an equation which specifies how the system evolves with time given the initial conditions.
Definition
An initial value problem is a differential equation
- with where is an open set of ,
together with a point in the domain of
- ,
called the initial condition.
A solution to an initial value problem is a function that is a solution to the differential equation and satisfies
- .
In higher dimensions, the differential equation is replaced with a family of equations , and is viewed as the vector , most commonly associated with the position in space. More generally, the unknown function can take values on infinite dimensional spaces, such as Banach spaces or spaces of distributions.
Initial value problems are extended to higher orders by treating the derivatives in the same way as an independent function, e.g. .
Existence and uniqueness of solutions
For a large class of initial asdwproblems, the existence and uniqueness dsa The Picard–Lindelöf theorem guarantees a unique solution on some interval containing t0 if ƒ is continuous on a region containing t0 and y0 and satisfies the Lipschitsdwsz candidas] on the variable y.w an equivalent [as[integral equation. The integral can be considered an operator which maps one function into another, such that the solution is a [[Fixed point (mathematics)|fixsdes poasd An older proof of the Picard–Lindelöf theorem constructs a sequence of funcdtions which converge to the solution of the integral equation, and thus, the solution of the initial value problem. Such a construction is sometimes called "Picard's method" d Hiroshi Okamura obtaianed a [[necessary and sa
Examples
A simple example is to solve and . We are trying to find a formula for that satisfies these two equations.
Start by noting that , so
Now rearrange the equation so that is on the left and on the right
Now integrate both sides (this introduces an unknown constant ).
Eliminate the
Let be a new unknown constant, , so
Now we need to find a value for . Use as given at the start and substitute 0 for and 19 for
this gives the final solution of .
- Second example
The solution of
can be found to be
Indeed,
Notes
- [a] Also called a Cauchy problem by some authors[citation needed]
See also
References
- Coddington, Earl A.; Levinson, Norman (1955). Theory of ordinary differential equations. New York-Toronto-London: McGraw-Hill Book Company, Inc.
- Hirsch, Morris W. and Smale, Stephen (1974). Differential equations, dynamical systems, and linear algebra. New York-London: Academic Press.
{{cite book}}
: CS1 maint: multiple names: authors list (link) - Okamura, Hirosi (1942). "Condition nécessaire et suffisante remplie par les équations différentielles ordinaires sans points de Peano". Mem. Coll. Sci. Univ. Kyoto Ser. A. (in French). 24: 21–28. MR 0031614.
- Agarwal, Ravi P.; Lakshmikantham, V. (1993). Uniqueness and Nonuniqueness Criteria for Ordinary Differential Equations. Series in real analysis. Vol. 6. World Scientific. ISBN 978-981-02-1357-2.
- Polyanin, Andrei D.; Zaitsev, Valentin F. (2003). Handbook of exact solutions for ordinary differential equations (2nd ed.). Boca Raton, Florida: Chapman & Hall/CRC. ISBN 1-58488-297-2.
- Robinson, James C. (2001). Infinite-dimensional dynamical systems: An introduction to dissipative parabolic PDEs and the theory of global attractors. Cambridge: Cambridge University Press. ISBN 0-521-63204-8.