@@ -63,30 +63,29 @@ to science codes.
6363
6464The current pyro solvers are:
6565
66- * linear advection (including a second-order unsplit CTU scheme, a
67- method-of-lines piecewise linear solver$^\star$, a 4th-order
68- finite-volume scheme$^\star$, and a WENO method$^\star$)
66+ - linear advection (including a second-order unsplit CTU scheme, a
67+ method-of-lines piecewise linear solver$^\\ star$, a 4th-order
68+ finite-volume scheme$^\\ star$, a WENO method$^\\ star$, and
69+ advection with a non-uniform velocity field$^\\ star$)
6970
70- * compressible hydrodynamics (including a second-order unsplit CTU
71- scheme, a method-of-lines piecewise linear solver$^\star$, and two
71+ - compressible hydrodynamics (including a second-order unsplit CTU
72+ scheme, a method-of-lines piecewise linear solver$^\\ star$, and two
7273 4th-order finite-volume schemes, one with Runge-Kutta integration
7374 and the other using a spectral deferred corrections
74- method$^\star$)
75+ method$^\\ star$)
7576
76- * diffusion using a second-order implicit discretization
77+ - diffusion using a second-order implicit discretization
7778
78- * incompressible hydrodynamics using a second-order approximate
79+ - incompressible hydrodynamics using a second-order approximate
7980 projection method.
8081
81- * low Mach number atmospheric solver$^\star$, using an approximate
82+ - low Mach number atmospheric solver$^\ \ star$, using an approximate
8283 projection method.
8384
84- * shallow water equations solver$^\star$
85+ - shallow water equations solver$^\ \ star$
8586
86- (solvers since the first pyro paper are marked with a $^\star$). Also
87+ (solvers since the first pyro paper are marked with a $^\\ star$). Also
8788new is support for Lagrangian tracer particles, which can be added to
8889any solver that has a velocity field.
8990
90-
91-
9291# References
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