Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Linear differential equation
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
==Types of solution== {{anchor|solving by quadrature}} A linear differential equation or a system of linear equations such that the associated homogeneous equations have constant coefficients may be '''solved by quadrature''', which means that the solutions may be expressed in terms of [[antiderivative|integrals]]. This is also true for a linear equation of order one, with non-constant coefficients. An equation of order two or higher with non-constant coefficients cannot, in general, be solved by quadrature. For order two, [[Kovacic's algorithm]] allows deciding whether there are solutions in terms of integrals, and computing them if any. The solutions of homogeneous linear differential equations with [[polynomial]] coefficients are called [[holonomic function]]s. This class of functions is stable under sums, products, [[derivative|differentiation]], [[antiderivative|integration]], and contains many usual functions and [[special function]]s such as [[exponential function]], [[logarithm]], [[sine]], [[cosine]], [[inverse trigonometric functions]], [[error function]], [[Bessel function]]s and [[hypergeometric function]]s. Their representation by the defining differential equation and initial conditions allows making algorithmic (on these functions) most operations of [[calculus]], such as computation of [[antiderivative]]s, [[limit (mathematics)|limits]], [[asymptotic expansion]], and numerical evaluation to any precision, with a certified error bound.
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)