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;