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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 19:56, 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

4φ=0

or

22φ=0

or

Δ2φ=0

where 4 is the fourth power of the del operator and the square of the laplacian operator 2 (or Δ), 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

4φx4+4φy4+4φz4+24φx2y2+24φy2z2+24φx2z2=0.

As another example, in n-dimensional Euclidean space,

4(1r)=3(158n+n2)r5

where

r=x12+x22++xn2.

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

1rr(rr(1rr(rφr)))+2r24φθ2r2+1r44φθ42r33φθ2r+4r42φθ2=0

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

xv(x,y)yu(x,y)+w(x,y)

where u(x,y), v(x,y) and w(x,y) are harmonic functions and v(x,y) is a harmonic conjugate of u(x,y).

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

(z¯f(z)+g(z))

where f(z) and g(z) 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

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