Dear Ding,
Thanks for your comment! Indeed, you are correct that the well rates have been specified as constant along the length of the well. While we appreciate that this is perhaps not a standard option in some simulators (and may be contrary to well physics), I will try to explain the reasoning below. The co-organizers may of course have other thoughts.
Firstly, it has been important for us to strive for a CSP description is precise enough that, at least in principle, there should exist a (unique) solution, so as to have a best possible basis to compare differences in the approximation and computational performance of the simulators. It turns out that in the presence of both mass and energy equations, containing both advective and diffusive processes (Darcy flux in addition to diffusion/dispersion for flow, and thermal conductivity for energy), rate based conditions are simpler to formulate precisely than potential-based conditions. This explains why both the well and boundary conditions are given in terms of rates.
Secondly, we do not expect it to be possible to provide physically realistic well conditions (again in the presence of both mass and energy equations) without being significantly more detailed in the description of the well itself. Well modeling is an important topic in itself, and similarly to other aspects of CO2 storage not included in the study (notably hysteresis, geomechanics, geochemistry, etc.), the influence of realistic models for these processes, relative to the CSP as a common baseline, will be interesting topic to understand, and we would be happy to see contributions to the SPE Journal special issue along these lines.
Finally, from a practical perspective, we believe that independently of what well models are implemented in various simulators, a constant flux along the well can be reasonably approximated by using a finite number of well segments of appropriate rates. In principle, this can be considered a numerical approximation, similar to the different representations of constitutive laws as either tables or expressions of elementary functions. Personally, I would expect that a reasonable approximation to a constant rate well can be achieved by a relatively low number of (independent) well segments (likely quite a bit coarser than the grid resolution in general), each injecting a prescribed rate proportional to their length.
I hope these thoughts were clarifying, and feel free to follow up with additional questions!
Best regards,
Jan