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bib: fix fieldstone #6193

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2 changes: 1 addition & 1 deletion benchmarks/viscosity_grooves/doc/viscosity_grooves.md
Original file line number Diff line number Diff line change
Expand Up @@ -22,7 +22,7 @@ where $\epsilon$ controls the viscosity contrast. It is easy to verify that
the flow is incompressible as the velocity field satisfies
$\nabla\cdot \mathbf u = 0$. The right hand side term of the Stokes equation
is obtained by inserting the expressions for velocity, pressure and viscosity
in the momentum conservation equation, see {cite:t}`thieulot:2019` for details. The
in the momentum conservation equation, see {cite:t}`fieldstone` for details. The
velocity, pressure and right hand side magnitude are shown in {numref}`fig:benchmark-grooves-3x3`
for $L=3$ and $\epsilon=0.1$.

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10 changes: 5 additions & 5 deletions doc/sphinx/references.bib
Original file line number Diff line number Diff line change
Expand Up @@ -11855,11 +11855,11 @@ @article{garzanti:etal:2018
doi = {10.1016/j.earscirev.2017.11.012},
}

@Misc{thieulot:2019,
author = {C. Thieulot},
title = {The Finite Element Method in Geodynamics},
url = {https://github.com/cedrict/fieldstone/blob/master/manual.pdf},
year = {2019}
@article{fieldstone,
author = "Cedric Thieulot",
title = "{Fieldstone: a computational geodynamics (self-)teaching tool}",
year = "2023",
doi = "10.5194/egusphere-egu23-14212"
}

@incollection{john:knobloch:2006,
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