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ENE 505 – Applied Computational Fluid Dynamics in Renewable Energy Technologies

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ENE 505 – Applied Computational Fluid Dynamics in Renewable

Energy Technologies

WEEK 6: NUMERICAL DISCRETIZATION CONTINUES

NUMERICAL DISCRETIZATION (Continues):

 FEM:

- Discretization of domain - Derive element equations

- Construct the variation formulation of the governing equations over an element

- Obtain approximation of the variation equation over an element

(using Ritz or a Weighted Residual method such as Galerkin, Least Squares etc)

- Assemble individual element equations for the whole problem - Impose the boundary conditions of the problem

- Solve the assembled equations - Post-processing of the results.

 FEM:

- Domain is divided into control volumes

- Integrate the differential equation over the control volume and apply the divergence theorem.

- To evaluate derivative terms, values at the control volume faces are needed: have to make an assumption about how the value varies.

- Result is a set of linear algebraic equations: one for each control volume. - Solve iteratively or simultaneously.

- Using finite volume method, the solution domain is subdivided into a finite number of small control volumes (cells) by a grid.

-The grid defines the boundaries of the control volumes while the computational node lies at the center of the control volume.

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 FVM Discretization example:

- The species transport equation (constant density, incompressible flow) is given by:

 

S

x

D

x

u

x

t

i i i i





Here

is the concentration of the chemical species and D is the diffusion coefficient. S is a source term.

- Discretize the above equation for a two-dimensional flow field, given in Figure 1. for a control volume containing the point P by using finite volume method (FVM) based central differencing scheme

and

- obtain a final simple algebraic form of this convection-diffusion equation. - determine each coefficient in this final discretization equation

Figure 1

- The differential equation above is converted into a solvable algebraic equations under steady state assumption

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- Convection term is balanced by the diffusion term

- The balance over the control volume is accomplished as:

- The values at the faces are determined by interpolation from the values at the the cell centers.

- The values at the faces are determined by using central differencing scheme.

References:

1. Versteeg H.K., and W. Malalasekera V., 1995, “Computational Fluid Dynamics: The Finite Volume Method", Longman Scientific & Technical, ISBN 0-582-21884-5.

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