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Fix the spelling of "Siddhartha Mishra" (#2174)
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Arpit-Babbar authored Nov 22, 2024
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12 changes: 6 additions & 6 deletions src/equations/shallow_water_1d.jl
Original file line number Diff line number Diff line change
Expand Up @@ -201,7 +201,7 @@ end
Non-symmetric two-point volume flux discretizing the nonconservative (source) term
that contains the gradient of the bottom topography [`ShallowWaterEquations1D`](@ref).
Gives entropy conservation and well-balancedness on both the volume and surface when combined with
Gives entropy conservation and well-balancedness on both the volume and surface when combined with
[`flux_wintermeyer_etal`](@ref).
Further details are available in the papers:
Expand All @@ -210,7 +210,7 @@ Further details are available in the papers:
shallow water equations on unstructured curvilinear meshes with discontinuous bathymetry
[DOI: 10.1016/j.jcp.2017.03.036](https://doi.org/10.1016/j.jcp.2017.03.036)
- Patrick Ersing, Andrew R. Winters (2023)
An entropy stable discontinuous Galerkin method for the two-layer shallow water equations on
An entropy stable discontinuous Galerkin method for the two-layer shallow water equations on
curvilinear meshes
[DOI: 10.48550/arXiv.2306.12699](https://doi.org/10.48550/arXiv.2306.12699)
"""
Expand All @@ -237,7 +237,7 @@ This flux can be used together with [`flux_fjordholm_etal`](@ref) at interfaces
conservation and well-balancedness.
Further details for the original finite volume formulation are available in
- Ulrik S. Fjordholm, Siddhartha Mishr and Eitan Tadmor (2011)
- Ulrik S. Fjordholm, Siddhartha Mishra and Eitan Tadmor (2011)
Well-balanced and energy stable schemes for the shallow water equations with discontinuous topography
[DOI: 10.1016/j.jcp.2011.03.042](https://doi.org/10.1016/j.jcp.2011.03.042)
and for curvilinear 2D case in the paper:
Expand Down Expand Up @@ -310,7 +310,7 @@ is nonzero this should only be used as a surface flux otherwise the scheme will
For well-balancedness in the volume flux use [`flux_wintermeyer_etal`](@ref).
Details are available in Eq. (4.1) in the paper:
- Ulrik S. Fjordholm, Siddhartha Mishr and Eitan Tadmor (2011)
- Ulrik S. Fjordholm, Siddhartha Mishra and Eitan Tadmor (2011)
Well-balanced and energy stable schemes for the shallow water equations with discontinuous topography
[DOI: 10.1016/j.jcp.2011.03.042](https://doi.org/10.1016/j.jcp.2011.03.042)
"""
Expand Down Expand Up @@ -582,7 +582,7 @@ end
equations::ShallowWaterEquations1D)
Calculate Roe-averaged velocity `v_roe` and wavespeed `c_roe = sqrt{g * h_roe}`
See for instance equation (62) in
See for instance equation (62) in
- Paul A. Ullrich, Christiane Jablonowski, and Bram van Leer (2010)
High-order finite-volume methods for the shallow-water equations on the sphere
[DOI: 10.1016/j.jcp.2010.04.044](https://doi.org/10.1016/j.jcp.2010.04.044)
Expand Down Expand Up @@ -631,7 +631,7 @@ end
end

# Calculate the error for the "lake-at-rest" test case where H = h+b should
# be a constant value over time.
# be a constant value over time.
@inline function lake_at_rest_error(u, equations::ShallowWaterEquations1D)
h, _, b = u

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4 changes: 2 additions & 2 deletions src/equations/shallow_water_2d.jl
Original file line number Diff line number Diff line change
Expand Up @@ -329,7 +329,7 @@ This flux can be used together with [`flux_fjordholm_etal`](@ref) at interfaces
conservation and well-balancedness.
Further details for the original finite volume formulation are available in
- Ulrik S. Fjordholm, Siddhartha Mishr and Eitan Tadmor (2011)
- Ulrik S. Fjordholm, Siddhartha Mishra and Eitan Tadmor (2011)
Well-balanced and energy stable schemes for the shallow water equations with discontinuous topography
[DOI: 10.1016/j.jcp.2011.03.042](https://doi.org/10.1016/j.jcp.2011.03.042)
and for curvilinear 2D case in the paper:
Expand Down Expand Up @@ -491,7 +491,7 @@ is nonzero this should only be used as a surface flux otherwise the scheme will
For well-balancedness in the volume flux use [`flux_wintermeyer_etal`](@ref).
Details are available in Eq. (4.1) in the paper:
- Ulrik S. Fjordholm, Siddhartha Mishr and Eitan Tadmor (2011)
- Ulrik S. Fjordholm, Siddhartha Mishra and Eitan Tadmor (2011)
Well-balanced and energy stable schemes for the shallow water equations with discontinuous topography
[DOI: 10.1016/j.jcp.2011.03.042](https://doi.org/10.1016/j.jcp.2011.03.042)
"""
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