Elliptic operator (nonfiction): Difference between revisions

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In the theory of [[Partial differential equation (nonfiction)|partial differential equations]], '''elliptic operators''' are differential operators that generalize the Laplace operator. They are defined by the condition that the coefficients of the highest-order derivatives be positive, which implies the key property that the principal symbol is invertible, or equivalently that there are no real characteristic directions.
[[File:Laplace's equation on an annulus.jpg|thumb|A solution to Laplace's equation defined on an annulus. The Laplace operator is the most famous example of an elliptic operator.]]In the theory of [[Partial differential equation (nonfiction)|partial differential equations]], '''elliptic operators''' are [[Differential operator (nonfiction)|differential operators]] that generalize the [[Laplace operator (nonfiction)|Laplace operator]]. They are defined by the condition that the coefficients of the highest-order derivatives be positive, which implies the key property that the [[Symbol of a differential operator (nonfiction)|principal symbol]] is invertible, or equivalently that there are no real [[Method of characteristics (nonfiction)|characteristic directions]].


Elliptic operators are typical of potential theory, and they appear frequently in electrostatics and continuum mechanics. Elliptic regularity implies that their solutions tend to be smooth functions (if the coefficients in the operator are smooth). Steady-state solutions to hyperbolic and parabolic equations generally solve elliptic equations.
Elliptic operators are typical of [[Potential theory (nonfiction)|potential theory]], and they appear frequently in electrostatics and continuum mechanics. Elliptic regularity implies that their solutions tend to be [[Smoothness (nonfiction)|smooth functions]] (if the coefficients in the operator are smooth). Steady-state solutions to hyperbolic and parabolic equations generally solve elliptic equations.


== In the News ==
== In the News ==
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== Nonfiction cross-reference ==
== Nonfiction cross-reference ==


* [[Differential equation (nonfiction)]] - a mathematical equation that relates some function with its derivatives. The functions usually represent physical quantities, the derivatives represent their rates of change, and the equation defines a relationship between the two.
* [[Differential operator (nonfiction)]]
* [[Dirac operator (nonfiction)]]
* [[Elliptic complex (nonfiction)]]
* [[Hopf maximum principle (nonfiction)]]
* [[Hyperbolic partial differential equation (nonfiction)]]
* [[Laplace operator (nonfiction)]]
* [[Mathematics (nonfiction)]]
* [[Mathematics (nonfiction)]]
* [[Physics (nonfiction)]]
* [[Method of characteristics (nonfiction)]]
* [[Parabolic partial differential equation (nonfiction)]]
* [[Partial differential equation (nonfiction)]]
* [[Potential theory (nonfiction)]]
* [[Semi-elliptic operator (nonfiction)]]
* [[Smoothness (nonfiction)]]
* [[Symbol of a differential operator (nonfiction)]]
* [[Ultrahyperbolic wave equation (nonfiction)]]
* [[Weyl's lemma (nonfiction)]]


External links:
External links:


* [https://en.wikipedia.org/wiki/Differential_equation Differential equation] @ Wikipedia
* [https://en.wikipedia.org/wiki/Elliptic_operator Elliptic operator] @ Wikipedia
* [http://www.eoht.info/page/History+of+differential+equations History of differential equations]
 
Attribution: By Nicoguaro - Own work, CC BY 4.0, https://commons.wikimedia.org/w/index.php?curid=59094163


[[Category:Nonfiction (nonfiction)]]
[[Category:Nonfiction (nonfiction)]]
[[Category:Elliptical operators (nonfiction)]]
[[Category:Mathematics (nonfiction)]]
[[Category:Mathematics (nonfiction)]]
[[Category:Differential equations (nonfiction)]]
[[Category:Partial differential equations (nonfiction)]]

Latest revision as of 16:32, 22 May 2019

A solution to Laplace's equation defined on an annulus. The Laplace operator is the most famous example of an elliptic operator.

In the theory of partial differential equations, elliptic operators are differential operators that generalize the Laplace operator. They are defined by the condition that the coefficients of the highest-order derivatives be positive, which implies the key property that the principal symbol is invertible, or equivalently that there are no real characteristic directions.

Elliptic operators are typical of potential theory, and they appear frequently in electrostatics and continuum mechanics. Elliptic regularity implies that their solutions tend to be smooth functions (if the coefficients in the operator are smooth). Steady-state solutions to hyperbolic and parabolic equations generally solve elliptic equations.

In the News

Fiction cross-reference

Nonfiction cross-reference

External links: