From f58b0f44d8f56601fc1aa42f4967ff661d8c450e Mon Sep 17 00:00:00 2001 From: apcraig Date: Mon, 13 May 2024 19:50:05 -0600 Subject: [PATCH] update documentation --- doc/source/science_guide/sg_dynamics.rst | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/doc/source/science_guide/sg_dynamics.rst b/doc/source/science_guide/sg_dynamics.rst index eaf07db3a..a8999ddc2 100644 --- a/doc/source/science_guide/sg_dynamics.rst +++ b/doc/source/science_guide/sg_dynamics.rst @@ -223,7 +223,7 @@ With :math:`\beta=\beta^* \Delta t \left( m \Delta t_e \right)^{-1}` :cite:`Bou + \underbrace{\left((\beta+1){m\over\Delta t}+{\tt vrel} \cos\theta + C_b \right)}_{\tt cca} & v^{k+1} = \underbrace{{\partial\sigma_{2j}^{k+1}\over\partial x_j}}_{\tt strinty} + \underbrace{\tau_{ay} - mg{\partial H_\circ\over\partial y} }_{\tt forcey} \\ - & + {\tt vrel}\underbrace{\pm \left(U_w\sin\theta+V_w\cos\theta\right)}_{\tt watery} + {m\over\Delta t}(\beta v^k + v^n), + & + {\tt vrel}\underbrace{\left( \pm U_w\sin\theta+V_w\cos\theta\right)}_{\tt watery} + {m\over\Delta t}(\beta v^k + v^n), :label: vmomr2 At this point, the solutions :math:`u^{k+1}` and :math:`v^{k+1}` for the B or the C grids are obtained in the same manner as for the standard EVP approach (see Section :ref:`evp-momentum` for details).