Such a coordinate transformation to locally Minkowskian coordinates at each numerical interface assumes that the solution of the Riemann problem is the one in special relativity and planar symmetry. This last assumption is equivalent to the approach followed in classical fluid dynamics, when using the solution of Riemann problems in slab symmetry for problems in cylindrical or spherical coordinates, which breaks down near the singular points (e.g. the polar axis in cylindrical coordinates). In analogy to classical fluid dynamics, the numerical error depends on the magnitude of the Christoffel symbols, which might be large whenever huge gradients or large temporal variations of the gravitational field are present. Finer grids and improved time advancing methods will be required in those circumstances.
Following  we illustrate the procedure for computing the second flux integral in Eq. (54), which we call . We begin by expressing the integral on a basis , with and forming an orthonormal basis in the plane orthogonal to , with normal to the surface , and and tangent to that surface. The vectors of this basis verify with being the Minkowski metric (in the following, caret subscripts will refer to vector components in this basis).
Denoting by the coordinates at the center of the interface at time t, we introduce the following locally Minkowskian coordinate system , where the matrix is given by , calculated at . In this system of coordinates the equations of general relativistic hydrodynamics transform into the equations of special relativistic hydrodynamics in Cartesian coordinates, but with non-zero sources, and the flux integral reads
(the caret symbol representing the numerical flux in Eq. (54) is now removed to avoid confusion), with , where we have taken into account that, in the coordinates , is described by the equation (with ), where the metric elements and are calculated at . Therefore, this surface is not at rest but moves with speed .
At this point all the theoretical work on special relativistic Riemann solvers developed in recent years can be exploited. The quantity in parenthesis in Eq. (69) represents the numerical flux across , which can now be calculated by solving the special relativistic Riemann problem defined with the values at the two sides of of two independent thermodynamical variables (namely, the rest mass density and the specific internal energy ) and the components of the velocity in the orthonormal spatial basis ().
Once the Riemann problem has been solved, we can take advantage of the self-similar character of the solution of the Riemann problem, which makes it constant on the surface simplifying the calculation of the above integral enormously:
where the superscript (*) stands for the value on obtained from the solution of the Riemann problem. Notice that the numerical fluxes correspond to the vector fields , , , , and linearized Riemann solvers provide the numerical fluxes as defined in Eq. (69). Thus the additional relation has to be used for the momentum equations. The integral in the right hand side of Eq. (70) is the area of the surface and can be expressed in terms of the original coordinates as
which can be evaluated for a given metric. The interested reader is addressed to  for details on the testing and calibration of this procedure.
|Numerical Hydrodynamics in General Relativity
José A. Font
© Max-Planck-Gesellschaft. ISSN 1433-8351
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