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2.11.1 The finite volume method: finite volumes versus finite difference

The finite volume method is used to discretize the equations in space. The expression ``finite volume'' actually has two meanings; one is the method of embedded or intersecting boundaries (shaved or lopped cells in our terminology) and the other is non-linear interpolation methods that can deal with non-smooth solutions such as shocks (i.e. flux limiters for advection). Both make use of the integral form of the conservation laws to which the weak solution is a solution on each finite volume of (sub-domain). The weak solution can be constructed out of piece-wise constant elements or be differentiable. The differentiable equations can not be satisfied by piece-wise constant functions.

As an example, the 1-D constant coefficient advection-diffusion equation:

$\displaystyle \partial_t \theta + \partial_x ( u \theta - \kappa \partial_x \theta ) = 0 $

can be discretized by integrating over finite sub-domains, i.e. the lengths $ \Delta x_i$ :

$\displaystyle \Delta x \partial_t \theta + \delta_i ( F ) = 0 $

is exact if $ \theta(x)$ is piece-wise constant over the interval $ \Delta x_i$ or more generally if $ \theta_i$ is defined as the average over the interval $ \Delta x_i$ .

The flux, $ F_{i-1/2}$ , must be approximated:

$\displaystyle F = u \overline{\theta} - \frac{\kappa}{\Delta x_c} \partial_i \theta $

and this is where truncation errors can enter the solution. The method for obtaining $ \overline{\theta}$ is unspecified and a wide range of possibilities exist including centered and upwind interpolation, polynomial fits based on the the volume average definitions of quantities and non-linear interpolation such as flux-limiters.

Choosing simple centered second-order interpolation and differencing recovers the same ODE's resulting from finite differencing for the interior of a fluid. Differences arise at boundaries where a boundary is not positioned on a regular or smoothly varying grid. This method is used to represent the topography using lopped cell, see Adcroft et al. [1997]. Subtle difference also appear in more than one dimension away from boundaries. This happens because the each direction is discretized independently in the finite difference method while the integrating over finite volume implicitly treats all directions simultaneously. Illustration of this is given in Adcroft and Campin [2002].

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Next: 2.11.2 C grid staggering Up: 2.11 Spatial discretization of Previous: 2.11 Spatial discretization of   Contents
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