PISM, A Parallel Ice Sheet Model
stable v2.1.1 committed by Constantine Khrulev on 2024-12-04 13:36:58 -0900
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◆ D2()
This function computes \(D^2\) defined by \[ 2D^2 = D_{ij} D_{ij}\] or \[ D^2 = \frac{1}{2}\,\left(\frac{1}{2}\,(v_{z})^2 + (v_{y} + u_{x})^2 + (v_{y})^2 + \frac{1}{2}\,(v_{x} + u_{y})^2 + \frac{1}{2}\,(u_{z})^2 + (u_{x})^2\right) \] (note the use of the summation convention). Here \(D_{ij}\) is the strain rate tensor. See StressBalance::compute_volumetric_strain_heating() for details.
Definition at line 440 of file StressBalance.cc. Referenced by pism::Time::calendar_year_start(), pism::stressbalance::StressBalance::compute_volumetric_strain_heating(), and pism::Time::year_fraction(). |