commit 16ea3677eab3418adb201a5c2e88cac7761eded5
parent 507e1e81596ab25729f4c822ff9a7c7d183c61a6
Author: Anders Damsgaard <anders@adamsgaard.dk>
Date: Fri, 5 Apr 2019 14:54:50 +0200
Remove old comments from simulation setup
Diffstat:
1 file changed, 3 insertions(+), 9 deletions(-)
diff --git a/1d_fd_simple_shear_damsgaard2013.h b/1d_fd_simple_shear_damsgaard2013.h
@@ -15,38 +15,32 @@ struct simulation init_sim(void)
sim.G = 9.81;
- sim.P_wall = 10e3; /* larger normal stress deepens the deformational depth */
+ sim.P_wall = 10e3; /* larger normal stress deepens the shear depth */
sim.mu_wall = 0.40;
sim.nz = 100;
/* lower values of A mean that the velocity curve can have sharper curves,
* e.g. at the transition from μ ≈ μ_s */
- //sim.A = 0.48; /* Henann and Kamrin 2016 */
sim.A = 0.40; /* Loose fit to Damsgaard et al 2013 */
- /* lower values of b mean larger shear velocity for a given stress ratio above */
- /* yield */
+ /* lower values of b mean larger shear velocity for a given stress ratio
+ * above yield */
sim.b = 0.9377; /* Henann and Kamrin 2016 */
- /*sim.mu_s = 0.3819; // Henann and Kamrin 2016 */
sim.mu_s = atan(DEG2RAD(22.0)); /* Damsgaard et al 2013 */
- /*sim.phi = 0.38; // Henann and Kamrin 2016 */
sim.phi = 0.25; /* Damsgaard et al 2013 */
/* lower values of d mean that the shear velocity curve can have sharper
* curves, e.g. at the transition from μ ≈ μ_s */
- /*sim.d = 1e-3; // Henann and Kamrin 2016 */
sim.d = 0.04; /* Damsgaard et al 2013 */
/* grain material density [kg/m^3] */
- /*sim.rho_s = 2.485e3; // Henann and Kamrin 2016 */
sim.rho_s = 2.6e3; /* Damsgaard et al 2013 */
/* Spatial settings */
sim.origo_z = 0.0;
- /*sim.L_z = 20.0*d; // Henann and Kamrin 2016 */
sim.L_z = 0.7; /* Damsgaard et al 2013 */
return sim;