From 4dc4356fe4dd543b2ecc3abf293f73641297ec89 Mon Sep 17 00:00:00 2001 From: Michael Zingale Date: Thu, 5 Dec 2024 11:26:48 -0500 Subject: [PATCH] some fixes --- sphinx_docs/source/nse.rst | 20 ++++++++++---------- 1 file changed, 10 insertions(+), 10 deletions(-) diff --git a/sphinx_docs/source/nse.rst b/sphinx_docs/source/nse.rst index 031847fac..bf77f5569 100644 --- a/sphinx_docs/source/nse.rst +++ b/sphinx_docs/source/nse.rst @@ -118,7 +118,7 @@ Therefore each of these auxiliary equations obeys an advection equation in the hydro part of the advancement. The table also provides $dY_e/dt$, $(d\langle -B/A\rangle/dt)_\mathrm{weak}$, and $\epsilon_{\nu,\mathrm{react}$, the +B/A\rangle/dt)_\mathrm{weak}$, and $\epsilon_{\nu,\mathrm{react}}$, the weak rate neutrino losses. These quantities are used to update the thermodynamic state as we integrate. @@ -229,13 +229,13 @@ The composition check considers the following nuclei groups: and we then say that a composition supports NSE if: -* :math:`X(C_\mathrm{group})` < ``network.C_nse`` +* :math:`X(\mathrm{C}_\mathrm{group})` < ``network.C_nse`` -* :math:`X(O_\mathrm{group})` < ``network.O_nse`` +* :math:`X(\mathrm{O}_\mathrm{group})` < ``network.O_nse`` -* :math:`X(Si_\mathrm{group})` < ``network.Si_nse`` +* :math:`X(\mathrm{Si}_\mathrm{group})` < ``network.Si_nse`` -* :math:`X(Fe_\mathrm{group}) + X(He_\mathrm{group})` > ``network.He_Fe_nse`` +* :math:`X(\mathrm{Fe}_\mathrm{group}) + X(\mathrm{He}_\mathrm{group})` > ``network.He_Fe_nse`` @@ -289,8 +289,8 @@ different syntax. The overall framework is constructed following :cite:`Kushnir_2020` with slight variations. The overview of the steps we take are the following: -* Minimum Temperature Check: require ``T > T_min_nse``, where ``T_min_nse`` is - a runtime parameter with a default value ``T_min_nse = 4.0e9``. +* Minimum Temperature Check: require ``T > nse.T_min_nse``, where ``nse.T_min_nse`` is + a runtime parameter with a default value ``nse.T_min_nse = 4.0e9``. * Mass Abundance Check: compare the current mass abundances of the nuclei to the NSE mass fractions. A detailed criteria are the following: @@ -319,13 +319,13 @@ variations. The overview of the steps we take are the following: .. math:: - \epsilon_{abs} = Y^i - Y^i_{NSE} < \mbox{nse_abs_tol} + \epsilon_{abs} = Y^i - Y^i_{NSE} < \mbox{nse.nse_abs_tol} .. math:: - \epsilon_{rel} = \frac{\epsilon_{abs}}{Y^i} < \mbox{nse_rel_tol} + \epsilon_{rel} = \frac{\epsilon_{abs}}{Y^i} < \mbox{nse.nse_rel_tol} - where ``nse_rel_tol = 0.2`` and ``nse_abs_tol = 0.005`` by default. + where ``nse.nse_rel_tol = 0.2`` and ``nse.nse_abs_tol = 0.005`` by default. * **Removed** :cite:`Kushnir_2020` also requires a fast reaction cycle that