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https://doi.org/10.5281/zenodo.3716321
28 March 2025, 16:19:17 UTC
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    • Climdyn-qgs-1598832
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    • qgs_rp.py
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    qgs_rp.py
    #!/usr/bin/env python
    # coding: utf-8
    
    # ## Reinhold and Pierrehumbert 1982 model version
    
    # This model version is a simple 2-layer channel QG atmosphere truncated at wavenumber 2 on a beta-plane with
    # a simple orography (a montain and a valley).
    # 
    # More detail can be found in the articles:
    # 
    # * Reinhold, B. B., & Pierrehumbert, R. T. (1982). Dynamics of weather regimes: Quasi-stationary waves and blocking.
    #   Monthly Weather Review, 110(9), 1105-1145.
    # * Cehelsky, P., & Tung, K. K. (1987). Theories of multiple equilibria and weather regimes—A critical reexamination.
    #   Part II: Baroclinic two-layer models. Journal of the atmospheric sciences, 44(21), 3282-3303.
    
    
    # ## Modules import
    import numpy as np
    import sys
    import time
    from multiprocessing import freeze_support, get_start_method
    
    # Importing the model's modules
    from qgs.params.params import QgParams
    from qgs.integrators.integrator import RungeKuttaIntegrator
    from qgs.functions.tendencies import create_tendencies
    
    # Initializing the random number generator (for reproducibility). -- Disable if needed.
    np.random.seed(21217)
    
    if __name__ == "__main__":
    
        if get_start_method() == "spawn":
            freeze_support()
    
        print_parameters = True
    
    
        def print_progress(p):
            sys.stdout.write('Progress {:.2%} \r'.format(p))
            sys.stdout.flush()
    
    
        class Bcolors:
            """to color the instructions in the console"""
            HEADER = '\033[95m'
            OKBLUE = '\033[94m'
            OKGREEN = '\033[92m'
            WARNING = '\033[93m'
            FAIL = '\033[91m'
            ENDC = '\033[0m'
            BOLD = '\033[1m'
            UNDERLINE = '\033[4m'
    
    
        print("\n" + Bcolors.HEADER + Bcolors.BOLD + "Model qgs v1.0.0 (Atmosphere + orography configuration)" + Bcolors.ENDC)
        print(Bcolors.HEADER + "=======================================================" + Bcolors.ENDC + "\n")
        print(Bcolors.OKBLUE + "Initialization ..." + Bcolors.ENDC)
        # ## Systems definition
    
        # General parameters
    
        # Time parameters
        dt = 0.1
        # Saving the model state n steps
        write_steps = 5
        # transient time to attractor
        transient_time = 1.e5
        # integration time on the attractor
        integration_time = 1.e4
        # file where to write the output
        filename = "evol_fields.dat"
        T = time.process_time()
    
        # Setting some model parameters
        # Model parameters instantiation with some non-default specs
        model_parameters = QgParams({'phi0_npi': np.deg2rad(50.)/np.pi, 'hd': 0.1})
        # Mode truncation at the wavenumber 2 in both x and y spatial coordinate
        model_parameters.set_atmospheric_channel_fourier_modes(2, 2)
    
        # Changing (increasing) the orography depth and the meridional temperature gradient
        model_parameters.ground_params.set_orography(0.2, 1)
        model_parameters.atemperature_params.set_thetas(0.2, 0)
    
        if print_parameters:
            print("")
            # Printing the model's parameters
            model_parameters.print_params()
    
        # Creating the tendencies functions
        f, Df = create_tendencies(model_parameters)
    
        # ## Time integration
        # Defining an integrator
        integrator = RungeKuttaIntegrator()
        integrator.set_func(f)
    
        # Start on a random initial condition
        ic = np.random.rand(model_parameters.ndim)*0.1
        # Integrate over a transient time to obtain an initial condition on the attractors
        print(Bcolors.OKBLUE + "Starting a transient time integration..." + Bcolors.ENDC)
        ws = 1000
        y = ic
        total_time = 0.
        t_up = ws * dt / integration_time * 100
        while total_time < transient_time:
            integrator.integrate(0., ws * dt, dt, ic=y, write_steps=0)
            t, y = integrator.get_trajectories()
            total_time += t
            if total_time/transient_time * 100 % 0.1 < t_up:
                print_progress(total_time/transient_time)
    
        # Now integrate to obtain a trajectory on the attractor
        total_time = 0.
        traj = np.insert(y, 0, total_time)
        traj = traj[np.newaxis, ...]
        t_up = write_steps * dt / integration_time * 100
    
        print(Bcolors.OKBLUE + "Starting the time evolution ..." + Bcolors.ENDC)
        while total_time < integration_time:
            integrator.integrate(0., write_steps * dt, dt, ic=y, write_steps=0)
            t, y = integrator.get_trajectories()
            total_time += t
            ty = np.insert(y, 0, total_time)
            traj = np.concatenate((traj, ty[np.newaxis, ...]))
            if total_time/integration_time*100 % 0.1 < t_up:
                print_progress(total_time/integration_time)
    
        print(Bcolors.OKGREEN + "Evolution finished, writing to file " + filename + Bcolors.ENDC)
    
        np.savetxt(filename, traj)
    
        print(Bcolors.OKGREEN + "Time clock :" + Bcolors.ENDC)
        print(str(time.process_time()-T)+' seconds')
    

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