3. CCPP Configuration and Build Options¶
While the CCPP-Framework code can be compiled independently, the CCPP-Physics code can only be used within a host modeling system that provides the variables and the kind, type, and DDT definitions. As such, it is advisable to integrate the CCPP configuration and build process with the host model’s. Part of the build process, known as the prebuild step since it precedes compilation, involves running a Python script that performs multiple functions. These functions include configuring the CCPP-Physics for use with the host model and autogenerating FORTRAN code to communicate variables between the physics and the dynamical core. The prebuild step will be discussed in detail in Chapter 8.
There are some differences between building and running the SCM and the UFS Atmosphere. In the case of the UFS Atmosphere as the host model, there are several build options (Figure 3.1). The choice can be specified through command-line options supplied to the compile.sh
script for manual compilation or through a regression test (RT) configuration file. Detailed instructions for building the code are discussed in Chapter 9.
The relevant options for building CCPP with the UFS Atmosphere can be described as follows:
- Without CCPP (CCPP=N): The code is compiled without CCPP and runs using the original UFS Atmosphere physics drivers, such as
GFS_physics_driver.F90
. This option entirely bypasses all CCPP functionality and is only used for RT against the unmodified UFS Atmosphere codebase.
With CCPP (CCPP=Y): The code is compiled with CCPP enabled and restricted to CCPP-compliant physics. That is, any parameterization to be called as part of a suite must be available in CCPP. Physics scheme selection and order is determined at runtime by an external suite definition file (SDF; see Chapter 4 for further details on the SDF). The existing physics-calling code
GFS_physics_driver.F90
andGFS_radiation_driver.F90
are bypassed altogether in this mode and any additional code needed to connect parameterizations within a suite previously contained therein is executed from the so-called CCPP-compliant “interstitial schemes”. One further option determines how the CCPP-compliant physics are called within the host model:- Dynamic CCPP (STATIC=N): This option is recommended for research and development users, since it allows choosing any physics schemes within the CCPP library at runtime by making adjustments to the CCPP SDF and the model namelist. This option carries computational overhead associated with the higher level of flexibility. Note that the CCPP-Framework and CCPP-physics are dynamically linked to the executable.
- Static CCPP (STATIC=Y): The code is compiled with CCPP enabled but restricted to CCPP-compliant physics defined by one or more SDFs used at compile time. This option is recommended for users interested in production-mode and operational applications, since it limits flexibility in favor of runtime performance and memory footprint. Note that the CCPP-Framework and CCPP-physics are statically linked to the executable.
Conversely, for the SCM, only the dynamic CCPP build is supported.
For all options that activate the CCPP, the ccpp_prebuild.py
Python script must be run. This may be done manually or as part of a host model build-time script. In the case of the SCM, ccpp_prebuild.py
must be run manually, as it is not incorporated in that model’s build system. In the case of the UFS Atmosphere, ccpp_prebuild.py
is run automatically as a step in the build system, although it can be run manually for debugging purposes.
The path to a host-model specific configuration file is the only required argument to ccpp_prebuild.py
. Such files are included with the SCM and NEMSfv3gfs repositories, and must be included with the code of any host model to use the CCPP. Figure 3.2 depicts the main functions of the ccpp_prebuild.py
script for the dynamic build. Using information included in the configuration file, the script reads metadata associated with all physics variables provided by the host model and metadata associated with all physics variables requested by all physics schemes in the CCPP (at least those whose entry/exit point source files are listed in the configuration file). The script matches the variables and autogenerates software caps for each physics scheme entry point so that they are available to be called by the host model, depending on the contents of a SDF provided at runtime.
In case of a static build, the basic function of the script is the same, but the output (namely, autogenerated software caps) take a different, more computationally-efficient approach. For a general idea of how the static option is different, compare Figure 3.3 for the static case with Figure 3.2 for the dynamic case. As mentioned, during the build step, one or more SDFs are used as an additional input. The script parses the SDF(s) and only matches provided/requested variables that are used within the particular physics suite(s). Rather than autogenerate software caps for each physics scheme (regardless of request), in static mode, the script autogenerates software caps for the physics suite(s) as a whole and for each physics group as defined in the SDF(s). At runtime, a single SDF is used to select the suite that will be executed in the run. This arrangement allows for more efficient variable recall (which is done once for all physics schemes within each group of a suite), leads to a reduced memory footprint of the CCPP compared to the dynamic option and speeds up execution to be on par with physics called using the existing physics-calling code.