Lorenz95 model¶
Introduction¶
The Lorenz95 model is an application of the Lorenz (1996) chaotic dynamics. This model is governed by \(I\) equations:
where \(i = 1, 2, \ldots, I\), with cyclic boundary conditions, and the constant \(F\) is independent of \(i\). The variables of this model may be thought of as values of some atmospheric quantity in \(I\) locations of a latitude circle. The so-called 40-variable version of this model assumes \(I=40\), with \(i = 1, 2, \ldots, 40\), which implies to the cyclic boundary conditions being defined as: \(x_{0} = x_{40}\); \(x_{-1} = x_{39}\); and, \(x_{41} = x_{1}\).
YAML parameters¶
The configurable Lorenz95 model parameters are as follows:
geometry
: define grid parametersresol
: define the number of variables \(I\)
model
: define model parametersf
: define the constant \(F\)name
: define the modeltstep
: define the time step
forecast length
: define the length of the forecastinitial condition
: define initial condition parametersdate
: define the initial date to issue a forecastfilename
: define the name of the file to be used as initial condition
output
: define output parametersdatadir
: define the directory to save filesdate
: define the output dateexp
: define an experiment identificationfrequency
: define the frequency to save output filestype
: define the type of output file
Note
Although the YAML parameters are defined using real time quantities for dates and time intervals (e.g., date
, tstep
, forecast length
, frequency
), the actual equivalence between real time and the time considered for this model is defined as a combination of the number of variables \(I\) and the constant \(F\). See details in Lorenz (1996) and Lorenz and Emanuel (1998).
References¶
Lorenz, E. N., 1996: Predictability: a problem partly solved. Seminar on Predictability, 4-8 September 1995, volume 1, pages 1–18, European Centre for Medium Range Weather Forecasts, Reading, England. ECMWF.
Lorenz, E. N. and Emanuel, K. A. (1998). Optimal sites for supplementary weather observations: Simulation with a small model. J. Atmos. Sci., 55(3):399–414.