I've been reading up on the background for SCM implementations and through 
the source code for Chrono's own implementation.

I am curious why Chrono's current implementation has elected not to include 
Coulumb friction in the calculations. For calculating shear stress (and 
thus, shear forces) at each node, Chrono's SCM uses only the 
Janosi-Hanamoto model for these calculations. The limitation of the J-H 
model is that

Meanwhile, this often-cited SCM implementation by Krenn and Herizinger 
<https://elib.dlr.de/60535/1/elib_ISTVS2009_KrennHirzinger.pdf> uses a 
different approach, with Coulumb friction being explicitly included at each 
node in combination with the max possible Mohr-Coulomb shear stress. This 
doesn't necessary capture all of the dynamics that J-H does, but it does 
always return a shear stress when a normal stress is applied (even when 
shear stress is negligible).

I'm curious as to why Janosi-Hanamoto is used here and what the limits to 
J-H are in Chrono's context? I can see it being more accurate for moving 
through very soft soils, but yielding ver little (or zero) shear stress on 
more rigid soils SCM terrains or when the slip is negligible (say, when a 
wheel has stopped moving) seems like a limitation. Does the current Chrono 
limitation account for the fact that J-H returns zero shear stress while a 
wheel is static?

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