{"shas":[["e3bd8f5acfb5420e12b99e27b88e8e3052f5e438","82dc7c3318a035b287f7e2e167a73ca7a97740a3@auckland.ac.nz","LAPACK solver fixes.","Chris Bradley"],["18352f88ffbe0218403e14b79df3364838965f54","82dc7c3318a035b287f7e2e167a73ca7a97740a3@auckland.ac.nz","Merge pull request #34 from chrispbradley/master\n\nFixes for LAPACK solver","Chris Bradley"],["8b3bd66e854f46afcb6c35cae04364fdc730bfd6","194249e5b726d0a63f3d41276566266d8e6ed936@aucklanduni.ac.nz","Add a quadratic poroelastic constitutive relation\n\nAlso renamed the Static relation to StaticINRIA to differentiate it.\nTracker item 3039","Adam Reeve"],["4076fc43924a5dcf99b79a8b5ea9a1d154ce7aaf","194249e5b726d0a63f3d41276566266d8e6ed936@aucklanduni.ac.nz","Share materials field between Darcy pressure and Solid\n\nWe want to be able to access the fluid density so that it can be\naccounted for in the gravity loading part of the finite elasticity\nresidual evaluation. Tracker item 3039.","Adam Reeve"],["cdfae12637f13dc91d2989a67abcc32c0cc27dcd","194249e5b726d0a63f3d41276566266d8e6ed936@aucklanduni.ac.nz","Include the effect of fluid influx on gravity loading\n\nWhen the fluid volume fraction changes the total\nLagrangian density also changes.\nTracker item 3039.","Adam Reeve"]],"ref":"refs/heads/elasticityfluidpressure","size":5,"head":"cdfae12637f13dc91d2989a67abcc32c0cc27dcd","push_id":42924844}