earthkit.meteo.vertical.fieldlist.pressure_on_hybrid_levels¶
- earthkit.meteo.vertical.fieldlist.pressure_on_hybrid_levels(sp, A=None, B=None, levels=None, alpha_top='ifs', output='full')¶
Compute pressure and related parameters on hybrid (IFS model) levels.
- Parameters:
sp (
FieldList|Field) – Surface pressure (Pa). Can be a single Field or a FieldList. If a FieldList is provided, it must contain exactly one Field.A (
ArrayLike | None, optional) – A-coefficients defining the hybrid levels. Must contain all the half-levels in ascending order with respect to the model level number (from the top of the atmosphere toward the surface). When None (default), the A and B coefficients will be inferred from the metadata of the input fieldsp.B (
ArrayLike | None, optional) – B-coefficients defining the hybrid levels. Must contain all the half-levels in ascending order with respect to the model level number. (from the top of the atmosphere toward the surface). Must have the same size asA. When None (default), the A and B coefficients will be inferred from the metadata of the input fieldsp.levels (
ArrayLike | None, optional) – Hybrid full-levels to return. Level numbering starts at 1 at the top of the atmosphere and increases towards the surface. If None (default), all the levels are returned in the order defined by the A and B coefficients (i.e. ascending order with respect to the model level number). If only half-levels are requested inoutputthelevelsare interpreted as half-level numbers (so 0 is a valid half-level number corresponding to the top of the atmosphere).alpha_top (
{"ifs", "arpege"}, default"ifs") – Option to initialise the alpha parameter on the top of the model atmosphere. Seeearthkit.meteo.vertical.array.pressure_on_hybrid_levels()for details.output (
{"full", "half", "delta", "alpha"}| list | tuple, default"full") –Specify which outputs to return. Possible values are “full”, “half”, “delta” and “alpha”. Can be a single string or a list/tuple of strings. Default is “full”. The outputs are:
”full”: pressure (Pa) on full-levels
”half”: pressure (Pa) on half-levels. When
levelsis None, returns all the half-levels. Whenlevelsis not None, only returns the half-levels below the requested full-levels.”delta”: logarithm of pressure difference between two adjacent half-levels. Uses the same indexing as the full-levels.
”alpha”: alpha parameter defined for layers (i.e. for full-levels). Uses the same indexing as the full-levels. Used for the calculation of the relative geopotential thickness on full-levels. See
relative_geopotential_thickness_on_hybrid_levels()for details..
- Returns:
Pressure and/or related parameters on hybrid levels. When a single output type is requested, a single FieldList is returned. When multiple output types are requested, a tuple of FieldLists is returned, one for each requested output type, in the same order as specified in the input.
- Return type:
FieldList|tuple[FieldList,]
Notes
The hybrid model levels divide the atmosphere into \(NLEV\) layers. These layers are defined by the pressures at the interfaces between them for \(0 \leq k \leq NLEV\), which are the half-levels \(p_{k+1/2}\) (indices increase from the top of the atmosphere towards the surface). The half-levels are defined by the
AandBcoefficients in such a way that at the top of the atmosphere the first half-level pressure \(p_{0+1/2}\) is a constant, while at the surface \(p_{NLEV+1/2}\) is the surface pressure.The full-level pressure \(p_{k}\) associated with each model level is defined as the middle of the layer for \(1 \leq k \leq NLEV\).
The level definitions can be written as:
\[ \begin{align}\begin{aligned}p_{k+1/2} = A_{k+1/2} + p_{s} B_{k+1/2} \quad k=0, 1, ..., NLEV\\p_{k} = \frac{1}{2} (p_{k-1/2} + p_{k+1/2}) \quad k=1, 2, ..., NLEV\end{aligned}\end{align} \]where
\(p_{s}\) is the surface pressure
\(p_{k+1/2}\) is the pressure at the half-levelss
\(p_{k}\) is the pressure at the full-levels
\(A_{k+1/2}\) and \(B_{k+1/2}\) are the A- and B-coefficients defining the model levels.
For more details see [IFS-CY49R1-Dynamics] Chapter 2, Section 2.2.1.