Weak Form of the Poisson Problem

  • Context: Graduate 
  • Thread starter Thread starter Morberticus
  • Start date Start date
  • Tags Tags
    Form Poisson Weak
Click For Summary
SUMMARY

The weak form of the Poisson problem, represented by the equation \(\nabla^2 \phi = -f\), translates to the integral form \(\int \nabla \phi \cdot \nabla v = \int f v\) for all suitable test functions \(v\). For the more complex Poisson problem \(\nabla (\psi \nabla \phi) = -f\), the weak form is derived using the product rule, resulting in \(\int_V \psi (\nabla \phi) \cdot (\nabla v)\,dV = \int_V fv\,dV\). This formulation is essential for implementing finite element methods and variational principles in computational simulations.

PREREQUISITES
  • Understanding of weak formulations in partial differential equations
  • Familiarity with finite element methods (FEM)
  • Knowledge of vector calculus, particularly divergence and gradient operations
  • Experience with variational principles in mathematical physics
NEXT STEPS
  • Study the derivation of weak forms for various PDEs
  • Learn about finite element analysis (FEA) software such as ANSYS or COMSOL
  • Explore the application of variational methods in numerical simulations
  • Investigate advanced topics in vector calculus relevant to fluid dynamics
USEFUL FOR

Mathematicians, engineers, and computational scientists involved in numerical analysis, particularly those working with finite element methods and variational formulations in solving complex partial differential equations.

Morberticus
Messages
82
Reaction score
0
Hi,

I know the weak form of the Poisson problem

\nabla^2 \phi = -f

looks like

\int \nabla \phi \cdot \nabla v = \int f v

for all suitable v. Is there a similarly well-known form for the slightly more complicated poisson problem?

\nabla (\psi \nabla \phi ) = -f

I am writing some finite element code and variational/weak forms are very handy.

Thanks in advance
 
Last edited:
Physics news on Phys.org
Morberticus said:
Hi,

I know the weak form of the Poisson problem

\nabla^2 \phi = -f

looks like

\int \nabla \phi \cdot \nabla v = \int f v

for all suitable v. Is there a similarly well-known form for the slightly more complicated poisson problem?

\nabla (\psi \nabla \phi ) = -f

I am writing some finite element code and variational/weak forms are very handy.

Thanks in advance

By the product rule
<br /> \int_V v\nabla \cdot(\psi \nabla \phi)\,dV = \int_V\nabla\cdot(v\psi \nabla \phi) - \psi (\nabla \phi) \cdot (\nabla v)\,dV = \int_{\partial V} v\psi \nabla \phi \cdot dS - \int_V\psi (\nabla \phi) \cdot (\nabla v)\,dV
and hence the weak form of \nabla \cdot(\psi\nabla\phi) = - f is
<br /> \int_V \psi (\nabla \phi) \cdot (\nabla v)\,dV = \int_V fv\,dV<br />
 
  • Like
Likes   Reactions: 1 person

Similar threads

  • · Replies 6 ·
Replies
6
Views
4K
  • · Replies 0 ·
Replies
0
Views
3K
Replies
11
Views
3K
  • · Replies 1 ·
Replies
1
Views
974
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 8 ·
Replies
8
Views
5K
  • · Replies 13 ·
Replies
13
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
1
Views
2K