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In [[mathematics]], the '''biharmonic equation''' is a fourth-order [[partial differential equation]] which arises in areas of [[continuum mechanics]], including [[linear elasticity]] theory and the solution of [[Stokes flow]]s. It is written as
 
:<math>\nabla^4\varphi=0</math>
 
or
 
:<math>\nabla^2\nabla^2\varphi=0</math>
 
or
 
:<math>\Delta^2\varphi=0</math>
 
where <math>\nabla^4</math> is the fourth power of the [[del]] operator and the square of the [[laplacian]] operator <math>\nabla^2</math> (or <math>\Delta</math>), and it is known as the '''biharmonic operator''' or the '''bilaplacian operator'''.
 
For example, in three dimensional [[cartesian coordinates]] the biharmonic equation has the form
: <math>
{\partial^4 \varphi\over \partial x^4 } +
{\partial^4 \varphi\over \partial y^4 } +
{\partial^4 \varphi\over \partial z^4 }+
2{\partial^4 \varphi\over \partial x^2\partial y^2}+
2{\partial^4 \varphi\over \partial y^2\partial z^2}+
2{\partial^4 \varphi\over \partial x^2\partial z^2} = 0.
</math>
 
As another example, in ''n''-dimensional [[Euclidean space]],
 
:<math>\nabla^4 \left({1\over r}\right)= {3(15-8n+n^2)\over r^5}</math>
 
where
 
:<math>r=\sqrt{x_1^2+x_2^2+\cdots+x_n^2}.</math>
 
which, for ''n=3 and n=5'' only, becomes the biharmonic equation.
 
A solution to the biharmonic equation is called a '''biharmonic function'''. Any [[harmonic function]] is biharmonic, but the converse is not always true.
 
In two-dimensional [[polar coordinates]], the biharmonic equation is
 
:<math>
\frac{1}{r} \frac{\partial}{\partial r} \left(r \frac{\partial}{\partial r} \left(\frac{1}{r} \frac{\partial}{\partial r} \left(r \frac{\partial \varphi}{\partial r}\right)\right)\right)
+ \frac{2}{r^2} \frac{\partial^4 \varphi}{\partial \theta^2 \partial r^2}
+ \frac{1}{r^4} \frac{\partial^4 \varphi}{\partial \theta^4}
- \frac{2}{r^3} \frac{\partial^3 \varphi}{\partial \theta^2 \partial r}
+ \frac{4}{r^4} \frac{\partial^2 \varphi}{\partial \theta^2} = 0
</math>
 
which can be solved by separation of variables. The result is the [[Michell solution]].
 
==2 dimensional space==
The general solution to the 2 dimensional case is
:<math>
x v(x,y) - y u(x,y) + w(x,y)
</math>
where <math>u(x,y)</math>, <math>v(x,y)</math> and <math>w(x,y)</math> are [[harmonic functions]] and <math>v(x,y)</math> is a [[harmonic conjugate]] of <math>u(x,y)</math>.
 
Just as [[harmonic functions]] in 2 variables are closely related to complex [[analytic functions]], so are biharmonic functions in 2 variables. The general form of a biharmonic function in 2 variables can also be written as
:<math>
\operatorname{Im}(\bar{z}f(z) + g(z))
</math>
where <math>f(z)</math> and <math>g(z)</math> are [[analytic functions]].
 
==See also==
 
* [[Harmonic function]]
 
== References ==
 
* Eric W Weisstein, ''CRC Concise Encyclopedia of Mathematics'', CRC Press, 2002. ISBN 1-58488-347-2.
* S I Hayek, ''Advanced Mathematical Methods in Science and Engineering'', Marcel Dekker, 2000. ISBN 0-8247-0466-5.
* {{cite book | author=J P Den Hartog |  title=Advanced Strength of Materials | publisher=Courier Dover Publications | year=Jul 1, 1987 | isbn= 0-486-65407-9}}
 
==External links==
* {{MathWorld | urlname=BiharmonicEquation | title=Biharmonic Equation}}
* {{MathWorld | urlname=BiharmonicOperator | title=Biharmonic Operator}}
 
[[Category:Elliptic partial differential equations]]

Revision as of 20:56, 21 December 2013

In mathematics, the biharmonic equation is a fourth-order partial differential equation which arises in areas of continuum mechanics, including linear elasticity theory and the solution of Stokes flows. It is written as

or

or

where is the fourth power of the del operator and the square of the laplacian operator (or ), and it is known as the biharmonic operator or the bilaplacian operator.

For example, in three dimensional cartesian coordinates the biharmonic equation has the form

As another example, in n-dimensional Euclidean space,

where

which, for n=3 and n=5 only, becomes the biharmonic equation.

A solution to the biharmonic equation is called a biharmonic function. Any harmonic function is biharmonic, but the converse is not always true.

In two-dimensional polar coordinates, the biharmonic equation is

which can be solved by separation of variables. The result is the Michell solution.

2 dimensional space

The general solution to the 2 dimensional case is

where , and are harmonic functions and is a harmonic conjugate of .

Just as harmonic functions in 2 variables are closely related to complex analytic functions, so are biharmonic functions in 2 variables. The general form of a biharmonic function in 2 variables can also be written as

where and are analytic functions.

See also

References

  • Eric W Weisstein, CRC Concise Encyclopedia of Mathematics, CRC Press, 2002. ISBN 1-58488-347-2.
  • S I Hayek, Advanced Mathematical Methods in Science and Engineering, Marcel Dekker, 2000. ISBN 0-8247-0466-5.
  • 20 year-old Real Estate Agent Rusty from Saint-Paul, has hobbies and interests which includes monopoly, property developers in singapore and poker. Will soon undertake a contiki trip that may include going to the Lower Valley of the Omo.

    My blog: http://www.primaboinca.com/view_profile.php?userid=5889534

External links



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