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| The user has the option of specifying the full Keyword or the first two letters, regardless if using uppercase or lowercase. | The user has the option of specifying the full Keyword or the first two letters, regardless if using uppercase or lowercase. | ||
| If using either HSIMT (Wu and Zhu, 2010) or MPDATA (Margolin  | If using either HSIMT ([[Bibliography#WuH_2010a|Wu and Zhu, 2010]]) or MPDATA ([[Bibliography#SmolarkiewiczPK_1998a|Smolarkiewicz and Margolin, 1998]]) options, the user needs to set the same scheme for both horizontal and vertical advection to preserve monotonicity. | ||
| *Horizontal and vertical advection for each active (temperature and salinity) and inert tracer,  | *Horizontal and vertical advection for each active (temperature and salinity) and inert tracer, [1:[[Variables#NAT|NAT]]+[[Variables#NPT|NPT]],[[Variables#Ngrids|Ngrids]]] values are expected.<div class="box">   [[Variables#Hadvection|Hadvection]] == U3       \                     ! temperature<br />                 U3       \                     ! salinity<br />                 HSIMT    \                     ! dye_01, inert(1)<br />                 HSIMT                          ! dy2_02, inert(2)<br /><br />   [[Variables#Vadvection|Vadvection]] == C4       \                     ! temperature<br />                 C4       \                     ! salinity<br />                 HSIMT    \                     ! dye_01, inert(1)<br />                 HSIMT                          ! dy2_02, inert(2)</div> | ||
| *Horizontal and vertical advection for each active (temperature and salinity) and inert tracer for adjoint-based algorithms can have different horizontal schemes,  | *Horizontal and vertical advection for each active (temperature and salinity) and inert tracer for adjoint-based algorithms can have different horizontal schemes, [1:[[Variables#NAT|NAT]]+[[Variables#NPT|NPT]],[[Variables#Ngrids|Ngrids]]] values are expected.<div class="box">[[Variables#ad_Hadvection|ad_Hadvection]] == U3       \                     ! temperature<br />                 U3       \                     ! salinity<br />                 HSIMT    \                     ! dye_01, inert(1)<br />                 HSIMT                          ! dy2_02, inert(2)<br /><br />[[Variables#ad_Vadvection|ad_Vadvection]] == C4       \                     ! temperature<br />                 C4       \                     ! salinity<br />                 HSIMT    \                     ! dye_01, inert(1)<br />                 HSIMT                          ! dy2_02, inert(2)</div> | ||
Revision as of 15:06, 16 January 2020
 Notice: In SVN revision 933 (January 26, 2019), all "ocean_*.in" files were renamed to roms_*.in and all ocean* ROMS executables were renamed to roms* in order to facilitate and clarify model coupling efforts. More information can be found in the ROMS repository Trac ticket #794.
 Notice: In SVN revision 933 (January 26, 2019), all "ocean_*.in" files were renamed to roms_*.in and all ocean* ROMS executables were renamed to roms* in order to facilitate and clarify model coupling efforts. More information can be found in the ROMS repository Trac ticket #794.
File roms.in is the ROMS standard input file to any model run. This file sets the application spatial dimensions and many of the parameters that are not specified at compile time, including parallel tile decomposition, timestepping, physical coefficients and constants, vertical coordinate set-up, logical switches and flags to control the frequency of output, the names of input and output NetCDF files, and additional input scripts names for data assimilation, stations,  floats trajectories, ecosystem models, and sediment model.
This standard input ASCII file is organized in several sections as shown below, with links to more detailed explanation where required.
 Notice: A detailed information about ROMS input script file syntax can be found here.
 Notice: A detailed information about ROMS input script file syntax can be found here.
 Notice: A default roms.in input script is provided in the User/External subdirectory. Also there are several standard input scripts in the ROMS/External subdirectory which are used in the distributed test cases. They are usually named roms_app.in where app is the lowercase of the test case cpp option.
 Notice: A default roms.in input script is provided in the User/External subdirectory. Also there are several standard input scripts in the ROMS/External subdirectory which are used in the distributed test cases. They are usually named roms_app.in where app is the lowercase of the test case cpp option.
Configuration Parameters
- Application title. This string will be saved in the output NetCDF files. TITLE = Wind-Driven Upwelling/Downwelling over a Periodic Channel
- C-preprocessing Flag to define the specific configuration.MyAppCPP = UPWELLINGThough this is set by ROMS_APPLICATION in the makefile or build Script, ROMS is also compiled with -D$(ROMS_APPLICATION), which allows the use of#ifdef UPWELLINGfor instance. The net result of both-D$(ROMS_APPLICATION)=UPWELLING -DUPWELLINGis that ROMS_APPLICATION becomes 1 in the source code. ROMS therefore needs to be told the application name here as well in order to report it to the output file.
- Input variable information file name.  This file needs to be processed first so all information arrays can be initialized properly. Notice that we need an absolute or relative path for input metadata file varinfo.dat. There are many posts in the ROMS Forum of new users that fail to specify the correct location of this file.  Expert users usually have the own modified copy of this file for a particular application.VARNAME = ROMS/External/varinfo.dat
 NOTE: Starting with revision 460 file names can be up to 256 characters long. Previously only 80 characters were allowed. NOTE: Starting with revision 460 file names can be up to 256 characters long. Previously only 80 characters were allowed.
- Number of nested grids.Ngrids = 1
- Number of grid nesting layers.  This parameter is used to allow refinement and composite grid combinations.NestLayers = 1
- Number of grids in each nesting layer, [1:NestLayers] values are expected.GridsInLayer = 1
- Grid dimension parameters. These are used to dynamically allocate all model state variables upon execution.Lm == 41 ! Number of I-direction INTERIOR RHO-points
 Mm == 80 ! Number of J-direction INTERIOR RHO-points
 N == 16 ! Number of vertical levels
 Nbed = 0 ! Number of sediment bed layers
 NAT = 2 ! Number of active tracers (usually, 2)
 NPT = 0 ! Number of inactive passive tracers
 NCS = 0 ! Number of cohesive (mud) sediment tracers
 NNS = 0 ! Number of non-cohesive (sand) sediment tracers
- Domain decomposition parameters for serial, distributed-memory or shared-memory configurations used to determine tile horizontal range indices (Istr,Iend) and (Jstr,Jend), [1:Ngrids] values are expected.
Tracer Advection Schemes
Set horizontal and vertical advection schemes for active and inert tracers. A different advection scheme is allowed for each tracer. For example, a positive-definite (monotonic) algorithm can be activated for salinity and inert tracers, while a different one is set for temperature.
It is more advantageous to set the horizontal and vertical advection schemes for each tracer with switches instead of a single CPP flag for all of them. Positive-definite and monotonic algorithms (i.e., MPDATA and HSIMT) are appropriate and useful for positive fields like salinity, inert, biological, and sediment tracers. However, since the temperature has a dynamic range with negative and positive values in the ocean, other advection schemes are more appropriate.
Currently, the following tracer advection schemes are available and are activated using the associated Keyword:
- Keyword Advection Algorithm
 A4 4th-order Akima (horizontal/vertical)
 C2 2nd-order centered differences (horizontal/vertical)
 C4 4th-order centered differences (horizontal/vertical)
 HSIMT 3th-order HSIMT with TVD limiter (horizontal/vertical)
 MPDATA recursive flux corrected MPDATA (horizontal/vertical)
 SPLINES parabolic splines reconstruction (only vertical)
 SU3 split third-order upstream (horizontal/vertical)
 U3 3rd-order upstresm-bias (only horizontal)
The user has the option of specifying the full Keyword or the first two letters, regardless if using uppercase or lowercase.
If using either HSIMT (Wu and Zhu, 2010) or MPDATA (Smolarkiewicz and Margolin, 1998) options, the user needs to set the same scheme for both horizontal and vertical advection to preserve monotonicity.
- Horizontal and vertical advection for each active (temperature and salinity) and inert tracer, [1:NAT+NPT,Ngrids] values are expected.Hadvection == U3 \ ! temperature
 U3 \ ! salinity
 HSIMT \ ! dye_01, inert(1)
 HSIMT ! dy2_02, inert(2)
 Vadvection == C4 \ ! temperature
 C4 \ ! salinity
 HSIMT \ ! dye_01, inert(1)
 HSIMT ! dy2_02, inert(2)
- Horizontal and vertical advection for each active (temperature and salinity) and inert tracer for adjoint-based algorithms can have different horizontal schemes, [1:NAT+NPT,Ngrids] values are expected.ad_Hadvection == U3 \ ! temperature
 U3 \ ! salinity
 HSIMT \ ! dye_01, inert(1)
 HSIMT ! dy2_02, inert(2)
 ad_Vadvection == C4 \ ! temperature
 C4 \ ! salinity
 HSIMT \ ! dye_01, inert(1)
 HSIMT ! dy2_02, inert(2)
Lateral Open Boundary Conditions Parameters
- The lateral boundary conditions are now specified with logical switches instead of CPP flags to allow nested grid configurations. Their values are loaded into the structured array:where 1:4 are the numbered boundary edges, nLBCvar are the number LBC state variables, and Ngrids is the number of nested grids. For example, to apply gradient boundary conditions for free-surface we use:LBC(iwest, isFsur, ng) % gradientThe lateral boundary conditions are entered with a keyword. A value is expected for each boundary segment per nested grid for each state variable. Each tracer variable requires [1:4,1:NAT+NPT,Ngrids] values. [1:4,1:Ngrids] values are expected for other variables. The boundary order is: 1=west, 2=south, 3=east, and 4=north. That is, anticlockwise starting at the western boundary.
 LBC(ieast, ... , ng) % gradient
 LBC(isouth, ... , ng) % gradient
 LBC(inorth, ... , ng) % gradient
 The keyword is case insensitive and usually has three characters. However, it is possible to have compound keywords, if applicable. For example, the keyword RadNud implies radiation boundary condition with nudging. This combination is usually used in active/passive radiation conditions.! Keyword Lateral Boundary Condition Type
 !
 ! Cha Chapman
 ! Cla Clamped
 ! Clo Closed
 ! Fla Flather _____N_____ j=Mm
 ! Gra Gradient | 4 |
 ! Nes Nested | |
 ! Nud Nudging 1 W E 3
 ! Per Periodic | |
 ! Rad Radiation |_____S_____|
 ! Red Reduced Physics 2 j=1
 ! i=1 i=Lm
 ! W S E N
 ! e o a o
 ! s u s r
 ! t t t t
 ! h h
 !
 ! 1 2 3 4
 LBC(isFsur) == Per Clo Per Clo ! free-surface
 LBC(isUbar) == Per Clo Per Clo ! 2D U-momentum
 LBC(isVbar) == Per Clo Per Clo ! 2D V-momentum
 LBC(isUvel) == Per Clo Per Clo ! 3D U-momentum
 LBC(isVvel) == Per Clo Per Clo ! 3D V-momentum
 LBC(isMtke) == Per Clo Per Clo ! mixing TKE
 LBC(isTvar) == Per Clo Per Clo \ ! temperature
 Per Clo Per Clo ! salinity
- Adjoint-based algorithms can have different lateral boundary conditions keywords.ad_LBC(isFsur) == Per Clo Per Clo ! free-surface
 ad_LBC(isUbar) == Per Clo Per Clo ! 2D U-momentum
 ad_LBC(isVbar) == Per Clo Per Clo ! 2D U-momentum
 ad_LBC(isUvel) == Per Clo Per Clo ! 3D U-momentum
 ad_LBC(isVvel) == Per Clo Per Clo ! 3D V-momentum
 ad_LBC(isMtke) == Per Clo Per Clo ! mixing TKE
 ad_LBC(isTvar) == Per Clo Per Clo \ ! temperature
 Per Clo Per Clo ! salinity
- Lateral open boundary edge volume conservation switch for nonlinear model and adjoint-based algorithm. This is usually activated with radiation boundary conditions to enforce global mass conservation. Notice that these switches should not be activated if tidal forcing, [1:Ngrids] values are expected.VolCons(west) == F ! western boundary
 VolCons(east) == F ! eastern boundary
 VolCons(south) == F ! southern boundary
 VolCons(north) == F ! northern boundary
 ad_VolCons(west) == F ! western boundary
 ad_VolCons(east) == F ! eastern boundary
 ad_VolCons(south) == F ! southern boundary
 ad_VolCons(north) == F ! northern boundary
Timestepping and Iterations Parameters
- Timestepping parameters.
- Total number of timesteps for computing observations impacts interval during the analysis (NTIMES_ANA) or forecast (NTIMES_FCT) cycle.
- Model iteration loops parameters.ERstr = 1 ! Starting perturbation or iteration
 ERend = 1 ! Ending perturbation or iteration
 Nouter = 1 ! Maximum number of 4DVar outer loop iterations
 Ninner = 1 ! Maximum number of 4DVar inner loop iterations
 Nintervals = 1 ! Number of stochastic optimals interval divisions
- Number of eigenvalues (NEV) and eigenvectors (NCV) to compute for the Lanczos/Arnoldi problem in the Generalized Stability Theory (GST) analysis. NCV must be greater than NEV. Notice: At present, there is no apriori analysis to guide the selection of NCV relative to NEV.  The only formal requirement is that NCV > NEV. However in optimal perturbations, it is recommended to have NCV ≥ 2*NEV. In Finite Time Eigenmodes (FTE) and Adjoint Finite Time Eigenmodes (AFTE) the requirement is to have NCV ≥ 2*NEV+1. The efficiency of calculations depends critically on the combination of NEV and NCV.  If NEV is large (greater than 10 say), you can use NCV=2*NEV+1 but for NEV small (less than 6) it will be inefficient to use NCV=2*NEV+1. In complicated applications, you can start with NEV=2 and NCV=10. Otherwise, it will iterate for very long time. Notice: At present, there is no apriori analysis to guide the selection of NCV relative to NEV.  The only formal requirement is that NCV > NEV. However in optimal perturbations, it is recommended to have NCV ≥ 2*NEV. In Finite Time Eigenmodes (FTE) and Adjoint Finite Time Eigenmodes (AFTE) the requirement is to have NCV ≥ 2*NEV+1. The efficiency of calculations depends critically on the combination of NEV and NCV.  If NEV is large (greater than 10 say), you can use NCV=2*NEV+1 but for NEV small (less than 6) it will be inefficient to use NCV=2*NEV+1. In complicated applications, you can start with NEV=2 and NCV=10. Otherwise, it will iterate for very long time.
Output Frequency Parameters
- Flags controlling the frequency of output.NRREC = 0 ! Model restart flag
 LcycleRST == T ! Switch to recycle restart time records
 NRST == 288 ! Number of timesteps between writing restart records
 NSTA == 1 ! Number of timesteps between stations records
 NFLT == 1 ! Number of timesteps between floats records
 NINFO == 1 ! Number of timesteps between printing information diagnostics
- Output history, average, diagnostic files parameters.LDEFOUT == T ! File creation/append switch
 NHIS == 72 ! Number of timesteps between writing history records
 NDEFHIS == 0 ! Number of timesteps between creation of new history file
 NQCK == 0 ! Number of timesteps between writing quicksave records
 NDEFQCK == 0 ! Number of timesteps between creation of new quicksave file
 NTSAVG == 1 ! Starting averages timestep
 NAVG == 72 ! Number of timesteps between writing averages records
 NDEFAVG == 0 ! Number of timesteps between creation of new averages file
 NTSDIA == 1 ! Starting diagnostics timestep
 NDIA == 72 ! Number of timesteps between writing diagnostics records
 NDEFDIA == 0 ! Number of timesteps between creation of new diagnostics file
- Output tangent linear and adjoint models parameters.LcycleTLM == F ! Switch to recycle TLM time records
 NTLM == 72 ! Number of timesteps writing between TLM records
 NDEFTLM == 0 ! Number of timesteps between creation of new TLM file
 LcycleADJ == F ! Switch to recycle ADM time records
 NADJ == 72 ! Number of timesteps between writing ADM records
 NDEFADJ == 0 ! Number of timesteps between creation of new ADM file
 NSFF == 72 ! Number of timesteps between 4DVAR adjustment of
 ! surface forcing fluxes
 NOBC == 72 ! Number of timesteps between 4DVAR adjustment of
 ! open boundary fields
- Output check pointing GST restart parameters.LmultiGST = F ! one eigenvector per history file
 LrstGST = F ! GST restart switch
 MaxIterGST = 500 ! maximum number of iterations
 NGST = 10 ! check pointing interval
Physical and Numerical Parameters
- Relative accuracy of the Ritz values computed in the GST analysis.Ritz_tol = 1.0d-15
- Harmonic/biharmonic horizontal diffusion of all active and passive (dye) tracers for the nonlinear model and adjoint-based algorithms: [1:NAT+NPT,Ngrids] values are expected. Diffusion coefficients for biology and sediment tracers are set in their respective input scripts.
- Harmonic/biharmonic, horizontal viscosity coefficient for the nonlinear model and adjoint-based algorithms: [1:Ngrids values are expected. Only used if the appropriate CPP options are defined.
- Logical switches (TRUE/FALSE) to increase/decrease horizontal viscosity and/or diffusivity in specific areas of the application domain (like sponge areas) for the desired application grid.
- Background vertical mixing coefficients for active (NAT) and inert (NPT) tracers for the nonlinear model and basic state scale factor in adjoint-based algorithms: [1:NAT+NPT,Ngrids] values are expected.
- Background vertical mixing coefficient for momentum for the nonlinear model and basic state scale factor in the adjoint-based algorithms: [1:Ngrids] values are expected.
- Upper threshold values to limit vertical mixing coefficients computed from vertical mixing parameterizations. Although this is an engineering fix, the vertical mixing values inferred from ocean observations are rarely higher than this upper limit value.
- Turbulent closures parameters.
- Generic length-scale turbulence closure parameters. These parameters are used when GLS_MIXING is activated.GLS_P == 3.0d0 ! K-epsilon
 GLS_M == 1.5d0 ! Turbulent kinetic energy exponent
 GLS_N == -1.0d0 ! Turbulent length scale exponent
 GLS_Kmin == 7.6d-6 ! Minimum value of specific turbulent energy
 GLS_Pmin == 1.0d-12 ! Minimum Value of dissipation
 ! Closure independent constraint parameters:
 GLS_CMU0 == 0.5477d0 ! Stability coefficient
 GLS_C1 == 1.44d0 ! Shear production coefficient
 GLS_C2 == 1.92d0 ! Dissipation coefficient
 GLS_C3M == -0.4d0 ! Buoyancy production coefficient (minus)
 GLS_C3P == 1.0d0 ! Buoyancy production coefficient (plus)
 GLS_SIGK == 1.0d0 ! Constant Schmidt number for turbulent
 ! kinetic energy diffusivity
 GLS_SIGP == 1.30d0 ! Constant Schmidt number for turbulent
 ! generic statistical field, "psi"
- Constants used in surface turbulent kinetic energy flux computation.CHARNOK_ALPHA == 1400.0d0 ! Charnok surface roughness
 ZOS_HSIG_ALPHA == 0.5d0 ! Roughness from wave amplitude
 SZ_ALPHA == 0.25d0 ! roughness from wave dissipation
 CRGBAN_CW == 100.0d0 ! Craig and Banner wave breaking
- Constants used in momentum stress computation.
- Height (m) of atmospheric measurements for Bulk fluxes parameterization.
- Minimum depth for wetting and drying.DCRIT == 0.10d0 ! m
- Jerlov water type used to set vertical depth scale for shortwave radiation absorption.WTYPE == 1
- Deepest and shallowest levels to apply surface momentum stress as a body-force.
- Mean Density and Brunt-Vaisala frequency.
- Timestamp assigned for model initialization, reference time origin for tidal forcing, and model reference time for output NetCDF units attribute.
- Nudging/relaxation time scales, inverse scales will be computed internally, [1:Ngrids] values are expected. These values are used for two purposes.
- When climatology nudging is active throughout the domain because the logical flags LtracerCLM, Lm3CLM, Lm2CLM etc. are TRUE, these values are the default nudging time scales set in Functionals/ana_nudgcoef.h. Since the user can choose to customize ana_nudgcoef.h, or provide 3-D climatology nudging time scales in an external file, these parameters might not be used
- When nudging is applied in the lateral open boundary conditions because the LBC logical flags are set to "RadNud" the values here set the nudging time scale when the Orlanski radiation scheme detects outflow conditions. When the Orlanski scheme detects inflow conditions, the nudging time scale is TNUDG/OBCFAC (see OBCFAC below).
- Factor between passive (outflow) and active (inflow) (in the Orlanksi radiation sense) open boundary condition nudging time scales, [1:Ngrids]. If OBCFAC > 1, nudging on inflow is stronger than on outflow (recommended) because the inflow time scale TNUDG/OBCFAC is less than the outflow timescale TNUDG (see above). The passive/active radiation conditions in ROMS follow the method proposed by  Marchesiello et al. (2001): withwhere represents the external boundary data and is the nudging time scale with for outflow, for inflow, and . At outflow, a weak nudging is used to prevent a numerical drift in the solution while avoiding over-specification of the boundary data. During inflow, a strong nudging is applied to avoid data-shock in the solution. The nudging time scales provided above are for the outflow (passive) conditions, , in days. The inflow nudging factor in the above equation is .OBCFAC == 10.0d0 ! nondimensional
- Linear equation of State parameters, [1:Ngrids] values are expected.
- Slipperiness parameter: 1.0 (free slip) or -1.0 (no slip).GAMMA2 = 1.0d0
- Logical switches (TRUE/FALSE) to activate horizontal momentum transport point Sources/Sinks (like river runoff) and mass point Sources/Sinks (like volume vertical influx): [1:Ngrids] values are expected. These switches replace obsolete CPP options UV_PSOURCE and Q_PSOURCE, respectively. In nesting, a particular grid may or may not have Sources/Sinks forcing.
- Logical switches (TRUE/FALSE) to activate tracers point Sources/Sinks (like river runoff) and to specify which tracer variables to consider: [1:NAT+NPT,Ngrids] values are expected.  Other biological and sediment tracer switches are activated in their respective input scripts. This switch replaces obsolete CPP option TS_PSOURCE. In nesting, a particular grid may or may not have tracers Sources/Sinks forcing.LtracerSrc == F F ! temperature, salinity, inert
- Logical switches (TRUE/FALSE) to read and process climatology fields.LsshCLM == F ! sea-surface height
 Lm2CLM == F ! 2D momentum
 Lm3CLM == F ! 3D momentum
 LtracerCLM == F F ! temperature, salinity, inert
- Logical switches (TRUE/FALSE) to nudge the desired climatology field(s). If not analytical climatology fields, users need to turn ON the logical switches above to process the fields from the climatology NetCDF file that are needed for nudging.LnudgeM2CLM == F ! 2D momentum
 LnudgeM3CLM == F ! 3D momentum
 LnudgeTCLM == F F ! temperature, salinity, inert
Vertical Coordinates Parameters
- Set vertical, terrain-following coordinates transformation equation and stretching function (see Vertical S-coordinate for more details).
- S-coordinate surface control parameter, [1:Ngrids] values are expected. The range of optimal values depends on the vertical stretching function.THETA_S == 3.0d0 ! surface stretching parameter
- S-coordinate bottom control parameter, [1:Ngrids] values are expected. The range of optimal values depends on the vertical stretching function.THETA_B == 0.0d0 ! bottom stretching parameter
- Critical depth (hc) in meters (positive) controlling the stretching. It can be interpreted as the width of surface or bottom boundary layer in which higher vertical resolution (levels) is required during stretching.TCLINE == 25.0d0 ! critical depth (m)
Adjoint Sensitivity Parameters
- Starting (DstrS) and ending (DendS) day for adjoint sensitivity forcing. DstrS must be less or equal to DendS. If both values are zero, their values are reset internally to the full range of the adjoint integration.
- Starting and ending vertical levels of the 3D adjoint state variables whose sensitivity is required.
- Logical switches (TRUE/FALSE) to specify the adjoint state variables whose sensitivity is required.Lstate(isFsur) == F ! free-surface
 Lstate(isUbar) == F ! 2D U-momentum
 Lstate(isVbar) == F ! 2D V-momentum
 Lstate(isUvel) == F ! 3D U-momentum
 Lstate(isVvel) == F ! 3D V-momentum
 Lstate(isWvel) == F ! 3D W-momentum
- Logical switches (TRUE/FALSE) to specify the adjoint state tracer variables whose sensitivity is required, [1:NT,1:Ngrids] values are expected.Lstate(isTvar) == F F ! NT tracers
Stochastic Optimals Parameters
- Logical switches (TRUE/FALSE) to specify the state variables required by Forcing Singular Vectors or Stochastic Optimals.Fstate(isFsur) == F ! free-surface
 Fstate(isUbar) == F ! 2D U-momentum
 Fstate(isVbar) == F ! 2D V-momentum
 Fstate(isUvel) == F ! 3D U-momentum
 Fstate(isVvel) == F ! 3D V-momentum
 Fstate(isTvar) == F F ! NT tracers
 Fstate(isUstr) == F ! surface U-stress
 Fstate(isVstr) == F ! surface V-stress
 Fstate(isTsur) == F F ! NT surface tracers flux
- Stochastic optimals time decorrelation scale (days) assumed for red noise processes.SO_decay == 2.0d0 ! days
- Stochastic Optimals surface forcing standard deviation for dimensionalization.SO_sdev(isFsur) == 1.0d0 ! free-surface
 SO_sdev(isUbar) == 1.0d0 ! 2D U-momentum
 SO_sdev(isVbar) == 1.0d0 ! 2D V-momentum
 SO_sdev(isUvel) == 1.0d0 ! 3D U-momentum
 SO_sdev(isVvel) == 1.0d0 ! 3D V-momentum
 SO_sdev(isTvar) == 1.0d0 1.0d0 ! NT tracers
 SOstate(isUstr) == 1.0d0 ! surface u-stress
 SOstate(isVstr) == 1.0d0 ! surface v-stress
 SO_sdev(isTsur) == 1.0d0 1.0d0 ! NT surface tracer flux
History Output Variables Switches
- Logical switches (TRUE/FALSE) to activate writing of fields into history output file.Hout(idUvel) == T ! u 3D U-velocity
 Hout(idVvel) == T ! v 3D V-velocity
 Hout(idu3dE) == F ! u_eastward 3D U-eastward at RHO-points
 Hout(idv3dN) == F ! v_northward 3D V-northward at RHO-points
 Hout(idWvel) == T ! w 3D W-velocity
 Hout(idOvel) == T ! omega omega vertical velocity
 Hout(idUbar) == T ! ubar 2D U-velocity
 Hout(idVbar) == T ! vbar 2D V-velocity
 Hout(idu2dE) == F ! ubar_eastward 2D U-eastward at RHO-points
 Hout(idv2dN) == F ! vbar_northward 2D V-northward at RHO-points
 Hout(idFsur) == T ! zeta free-surface
 Hout(idBath) == T ! bath time-dependent bathymetry
 Hout(idTvar) == T T ! temp, salt temperature and salinity
 Hout(idpthR) == F ! z_rho time-varying depths of RHO-points
 Hout(idpthU) == F ! z_u time-varying depths of U-points
 Hout(idpthV) == F ! z_v time-varying depths of V-points
 Hout(idpthW) == F ! z_w time-varying depths of W-points
 Hout(idUsms) == F ! sustr surface U-stress
 Hout(idVsms) == F ! svstr surface V-stress
 Hout(idUbms) == F ! bustr bottom U-stress
 Hout(idVbms) == F ! bvstr bottom V-stress
 Hout(idUbrs) == F ! bustrc bottom U-current stress
 Hout(idVbrs) == F ! bvstrc bottom V-current stress
 Hout(idUbws) == F ! bustrw bottom U-wave stress
 Hout(idVbws) == F ! bvstrw bottom V-wave stress
 Hout(idUbcs) == F ! bustrcwmax bottom max wave-current U-stress
 Hout(idVbcs) == F ! bvstrcwmax bottom max wave-current V-stress
 Hout(idUbot) == F ! Ubot bed wave orbital U-velocity
 Hout(idVbot) == F ! Vbot bed wave orbital V-velocity
 Hout(idUbur) == F ! Ur bottom U-velocity above bed
 Hout(idVbvr) == F ! Vr bottom V-velocity above bed
 Hout(idW2xx) == F ! Sxx_bar 2D radiation stress, Sxx component
 Hout(idW2xy) == F ! Sxy_bar 2D radiation stress, Sxy component
 Hout(idW2yy) == F ! Syy_bar 2D radiation stress, Syy component
 Hout(idU2rs) == F ! Ubar_Rstress 2D radiation U-stress
 Hout(idV2rs) == F ! Vbar_Rstress 2D radiation V-stress
 Hout(idU2Sd) == F ! ubar_stokes 2D U-Stokes velocity
 Hout(idV2Sd) == F ! vbar_stokes 2D V-Stokes velocity
 Hout(idW3xx) == F ! Sxx 3D radiation stress, Sxx component
 Hout(idW3xy) == F ! Sxy 3D radiation stress, Sxy component
 Hout(idW3yy) == F ! Syy 3D radiation stress, Syy component
 Hout(idW3zx) == F ! Szx 3D radiation stress, Szx component
 Hout(idW3zy) == F ! Szy 3D radiation stress, Szy component
 Hout(idU3rs) == F ! u_Rstress 3D U-radiation stress
 Hout(idV3rs) == F ! v_Rstress 3D V-radiation stress
 Hout(idU3Sd) == F ! u_stokes 3D U-Stokes velocity
 Hout(idV3Sd) == F ! v_stokes 3D V-Stokes velocity
 Hout(idWamp) == F ! Hwave wave height
 Hout(idWlen) == F ! Lwave wave length
 Hout(idWdir) == F ! Dwave wave direction
 Hout(idWptp) == F ! Pwave_top wave surface period
 Hout(idWpbt) == F ! Pwave_bot wave bottom period
 Hout(idWorb) == F ! Ub_swan wave bottom orbital velocity
 Hout(idWdis) == F ! Wave_dissip wave dissipation
 Hout(idPair) == F ! Pair surface air pressure
 Hout(idUair) == F ! Uair surface U-wind component
 Hout(idVair) == F ! Vair surface V-wind component
 Hout(idTsur) == F F ! shflux, ssflux surface net heat and salt flux
 Hout(idLhea) == F ! latent latent heat flux
 Hout(idShea) == F ! sensible sensible heat flux
 Hout(idLrad) == F ! lwrad longwave radiation flux
 Hout(idSrad) == F ! swrad shortwave radiation flux
 Hout(idEmPf) == F ! EminusP E-P flux
 Hout(idevap) == F ! evaporation evaporation rate
 Hout(idrain) == F ! rain precipitation rate
 Hout(idDano) == F ! rho density anomaly
 Hout(idVvis) == F ! AKv vertical viscosity
 Hout(idTdif) == F ! AKt vertical T-diffusion
 Hout(idSdif) == F ! AKs vertical Salinity diffusion
 Hout(idHsbl) == F ! Hsbl depth of surface boundary layer
 Hout(idHbbl) == F ! Hbbl depth of bottom boundary layer
 Hout(idMtke) == F ! tke turbulent kinetic energy
 Hout(idMtls) == F ! gls turbulent length scale
- Logical switches (TRUE/FALSE) to activate writing of extra inert passive tracers other than biological and sediment tracers. An inert passive tracer is one that it is only advected and diffused. Other processes are ignored. These tracers include, for example, dyes, pollutants, oil spills, etc. [1:NPT] values are expected. However, these switches can be activated using compact parameter specification.Hout(inert) == T ! dye_01, ... inert passive tracers
Quicksave Output Variables Switches
- Logical switches (TRUE/FALSE) to activate writing of fields into quicksave output file.Qout(idUvel) == F ! u 3D U-velocity
 Qout(idVvel) == F ! v 3D V-velocity
 Qout(idu3dE) == F ! u_eastward 3D U-eastward at RHO-points
 Qout(idv3dN) == F ! v_northward 3D V-northward at RHO-points
 Qout(idWvel) == F ! w 3D W-velocity
 Qout(idOvel) == F ! omega omega vertical velocity
 Qout(idUbar) == T ! ubar 2D U-velocity
 Qout(idVbar) == T ! vbar 2D V-velocity
 Qout(idu2dE) == T ! ubar_eastward 2D U-eastward at RHO-points
 Qout(idv2dN) == T ! vbar_northward 2D V-northward at RHO-points
 Qout(idFsur) == T ! zeta free-surface
 Qout(idBath) == T ! bath time-dependent bathymetry
 Qout(idTvar) == F F ! temp, salt temperature and salinity
 Qout(idUsur) == T ! u_sur surface U-velocity
 Qout(idVsur) == T ! v_sur surface V-velocity
 Qout(idUsuE) == T ! u_sur_eastward surface U-eastward velocity
 Qout(idVsuN) == T ! v_sur_northward surface V-northward velocity
 Qout(idsurT) == T T ! temp_sur, salt_sur surface temperature and salinity
 Qout(idpthR) == F ! z_rho time-varying depths of RHO-points
 Qout(idpthU) == F ! z_u time-varying depths of U-points
 Qout(idpthV) == F ! z_v time-varying depths of V-points
 Qout(idpthW) == F ! z_w time-varying depths of W-points
 Qout(idUsms) == F ! sustr surface U-stress
 Qout(idVsms) == F ! svstr surface V-stress
 Qout(idUbms) == F ! bustr bottom U-stress
 Qout(idVbms) == F ! bvstr bottom V-stress
 Qout(idUbrs) == F ! bustrc bottom U-current stress
 Qout(idVbrs) == F ! bvstrc bottom V-current stress
 Qout(idUbws) == F ! bustrw bottom U-wave stress
 Qout(idVbws) == F ! bvstrw bottom V-wave stress
 Qout(idUbcs) == F ! bustrcwmax bottom max wave-current U-stress
 Qout(idVbcs) == F ! bvstrcwmax bottom max wave-current V-stress
 Qout(idUbot) == F ! Ubot bed wave orbital U-velocity
 Qout(idVbot) == F ! Vbot bed wave orbital V-velocity
 Qout(idUbur) == F ! Ur bottom U-velocity above bed
 Qout(idVbvr) == F ! Vr bottom V-velocity above bed
 Qout(idW2xx) == F ! Sxx_bar 2D radiation stress, Sxx component
 Qout(idW2xy) == F ! Sxy_bar 2D radiation stress, Sxy component
 Qout(idW2yy) == F ! Syy_bar 2D radiation stress, Syy component
 Qout(idU2rs) == F ! Ubar_Rstress 2D radiation U-stress
 Qout(idV2rs) == F ! Vbar_Rstress 2D radiation V-stress
 Qout(idU2Sd) == F ! ubar_stokes 2D U-Stokes velocity
 Qout(idV2Sd) == F ! vbar_stokes 2D V-Stokes velocity
 Qout(idW3xx) == F ! Sxx 3D radiation stress, Sxx component
 Qout(idW3xy) == F ! Sxy 3D radiation stress, Sxy component
 Qout(idW3yy) == F ! Syy 3D radiation stress, Syy component
 Qout(idW3zx) == F ! Szx 3D radiation stress, Szx component
 Qout(idW3zy) == F ! Szy 3D radiation stress, Szy component
 Qout(idU3rs) == F ! u_Rstress 3D U-radiation stress
 Qout(idV3rs) == F ! v_Rstress 3D V-radiation stress
 Qout(idU3Sd) == F ! u_stokes 3D U-Stokes velocity
 Qout(idV3Sd) == F ! v_stokes 3D V-Stokes velocity
 Qout(idWamp) == F ! Hwave wave height
 Qout(idWlen) == F ! Lwave wave length
 Qout(idWdir) == F ! Dwave wave direction
 Qout(idWptp) == F ! Pwave_top wave surface period
 Qout(idWpbt) == F ! Pwave_bot wave bottom period
 Qout(idWorb) == F ! Ub_swan wave bottom orbital velocity
 Qout(idWdis) == F ! Wave_dissip wave dissipation
 Qout(idPair) == F ! Pair surface air pressure
 Qout(idUair) == F ! Uair surface U-wind component
 Qout(idVair) == F ! Vair surface V-wind component
 Qout(idTsur) == F F ! shflux, ssflux surface net heat and salt flux
 Qout(idLhea) == F ! latent latent heat flux
 Qout(idShea) == F ! sensible sensible heat flux
 Qout(idLrad) == F ! lwrad longwave radiation flux
 Qout(idSrad) == F ! swrad shortwave radiation flux
 Qout(idEmPf) == F ! EminusP E-P flux
 Qout(idevap) == F ! evaporation evaporation rate
 Qout(idrain) == F ! rain precipitation rate
 Qout(idDano) == F ! rho density anomaly
 Qout(idVvis) == F ! AKv vertical viscosity
 Qout(idTdif) == F ! AKt vertical T-diffusion
 Qout(idSdif) == F ! AKs vertical Salinity diffusion
 Qout(idHsbl) == F ! Hsbl depth of surface boundary layer
 Qout(idHbbl) == F ! Hbbl depth of bottom boundary layer
 Qout(idMtke) == F ! tke turbulent kinetic energy
 Qout(idMtls) == F ! gls turbulent length scale
- Logical switches (TRUE/FALSE) to activate writing of extra inert passive tracers other than biological and sediment tracers into the quicksave output file. An inert passive tracer is one that it is only advected and diffused. Other processes are ignored. These tracers include, for example, dyes, pollutants, oil spills, etc. [1:NPT] values are expected. However, these switches can be activated using compact parameter specification.Qout(inert) == F ! dye_01, ... inert passive tracers
 Qout(Snert) == F ! dye_01, ... surface inert passive tracers
Time-averaged Output Variables Switches
- Logical switches (TRUE/FALSE) to activate writing of fields into time-averaged output file.Aout(idUvel) == T ! u 3D U-velocityy
 Aout(idVvel) == T ! v 3D V-velocity
 Aout(idu3dE) == F ! u_eastward 3D U-eastward at RHO-points
 Aout(idv3dN) == F ! v_northward 3D V-northward at RHO-points
 Aout(idWvel) == T ! w 3D W-velocity
 Aout(idOvel) == T ! omega omega vertical velocity
 Aout(idUbar) == T ! ubar 2D U-velocity
 Aout(idVbar) == T ! vbar 2D V-velocity
 Aout(idu2dE) == F ! ubar_eastward 2D U-eastward at RHO-points
 Aout(idv2dN) == F ! vbar_northward 2D V-northward at RHO-points
 Aout(idFsur) == T ! zeta free-surface
 Aout(idTvar) == T T ! temp, salt temperature and salinity
 Aout(idUsms) == F ! sustr surface U-stress
 Aout(idVsms) == F ! svstr surface V-stress
 Aout(idUbms) == F ! bustr bottom U-stress
 Aout(idVbms) == F ! bvstr bottom V-stress
 Aout(idW2xx) == F ! Sxx_bar 2D radiation stress, Sxx component
 Aout(idW2xy) == F ! Sxy_bar 2D radiation stress, Sxy component
 Aout(idW2yy) == F ! Syy_bar 2D radiation stress, Syy component
 Aout(idU2rs) == F ! Ubar_Rstress 2D radiation U-stress
 Aout(idV2rs) == F ! Vbar_Rstress 2D radiation V-stress
 Aout(idU2Sd) == F ! ubar_stokes 2D U-Stokes velocity
 Aout(idV2Sd) == F ! vbar_stokes 2D V-Stokes velocity
 Aout(idW3xx) == F ! Sxx 3D radiation stress, Sxx component
 Aout(idW3xy) == F ! Sxy 3D radiation stress, Sxy component
 Aout(idW3yy) == F ! Syy 3D radiation stress, Syy component
 Aout(idW3zx) == F ! Szx 3D radiation stress, Szx component
 Aout(idW3zy) == F ! Szy 3D radiation stress, Szy component
 Aout(idU3rs) == F ! u_Rstress 3D U-radiation stress
 Aout(idV3rs) == F ! v_Rstress 3D V-radiation stress
 Aout(idU3Sd) == F ! u_stokes 3D U-Stokes velocity
 Aout(idV3Sd) == F ! v_stokes 3D V-Stokes velocity
 Aout(idPair) == F ! Pair surface air pressure
 Aout(idUair) == F ! Uair surface U-wind component
 Aout(idVair) == F ! Vair surface V-wind component
 Aout(idTsur) == F F ! shflux, ssflux surface net heat and salt flux
 Aout(idLhea) == F ! latent latent heat flux
 Aout(idShea) == F ! sensible sensible heat flux
 Aout(idLrad) == F ! lwrad longwave radiation flux
 Aout(idSrad) == F ! swrad shortwave radiation flux
 Aout(idevap) == F ! evaporation evaporation rate
 Aout(idrain) == F ! rain precipitation rate
 Aout(idDano) == F ! rho density anomaly
 Aout(idVvis) == F ! AKv vertical viscosity
 Aout(idTdif) == F ! AKt vertical T-diffusion
 Aout(idSdif) == F ! AKs vertical Salinity diffusion
 Aout(idHsbl) == F ! Hsbl depth of surface boundary layer
 Aout(idHbbl) == F ! Hbbl depth of bottom boundary layer
 Aout(id2dRV) == F ! pvorticity_bar 2D relative vorticity
 Aout(id3dRV) == F ! pvorticity 3D relative vorticity
 Aout(id2dPV) == F ! rvorticity_bar 2D potential vorticity
 Aout(id3dPV) == F ! rvorticity 3D potential vorticity
 Aout(idu3dD) == F ! u_detided detided 3D U-velocity
 Aout(idv3dD) == F ! v_detided detided 3D V-velocity
 Aout(idu2dD) == F ! ubar_detided detided 2D U-velocity
 Aout(idu3dD) == F ! vbar_detided detided 2D V-velocity
 Aout(idFsuD) == F ! zeta_detided detided free-surface
 Aout(idTrcD) == F F ! temp_detided, ... detided temperature and salinity
 Aout(idHUav) == F ! Huon u-volume flux, Huon
 Aout(idHVav) == F ! Hvom v-volume flux, Hvom
 Aout(idUUav) == F ! uu quadratic <u*u> term
 Aout(idUVav) == F ! uv quadratic <u*v> term
 Aout(idVVav) == F ! vv quadratic <v*v> term
 Aout(idU2av) == F ! ubar2 quadratic <ubar*ubar> term
 Aout(idV2av) == F ! vbar2 quadratic <vbar*vbar> term
 Aout(idZZav) == F ! zeta2 quadratic <zeta*zeta> term
 Aout(idTTav) == F F ! temp2, ... quadratic <t*t> tracer terms
 Aout(idUTav) == F F ! utemp, ... quadratic <u*t> tracer terms
 Aout(idVTav) == F F ! vtemp, ... quadratic <v*t> tracer terms
 Aout(iHUTav) == F F ! Huontemp, ... tracer volume flux, <Huon*t>
 Aout(iHVTav) == F F ! Hvomtemp, ... tracer volume flux, <Hvom*t>
- Logical switches (TRUE/FALSE) to activate writing of extra inert passive tracers other than biological and sediment tracers into the time-averaged output file. An inert passive tracer is one that it is only advected and diffused. Other processes are ignored. These tracers include, for example, dyes, pollutants, oil spills, etc. [1:NPT,1:Ngrids] values are expected. However, these switches can be activated using compact parameter specification.Aout(inert) == T ! dye_01, ... inert passive tracers
Time-averaged Diagnostic Output Variables Switches
- Logical switches (TRUE/FALSE) to activate writing time-averaged. 2D momentum (ubar, vbar) diagnostic terms into the diagnostics output file.Dout(M2rate) == T ! ubar_accel, ... acceleration
 Dout(M2pgrd) == T ! ubar_prsgrd, ... pressure gradient
 Dout(M2fcor) == T ! ubar_cor, ... Coriolis force
 Dout(M2hadv) == T ! ubar_hadv, ... horizontal total advection
 Dout(M2xadv) == T ! ubar_xadv, ... horizontal XI-advection
 Dout(M2yadv) == T ! ubar_yadv, ... horizontal ETA-advection
 Dout(M2hrad) == T ! ubar_hrad, ... horizontal total radiation stress
 Dout(M2hvis) == T ! ubar_hvisc, ... horizontal total viscosity
 Dout(M2xvis) == T ! ubar_xvisc, ... horizontal XI-viscosity
 Dout(M2yvis) == T ! ubar_yvisc, ... horizontal ETA-viscosity
 Dout(M2sstr) == T ! ubar_sstr, ... surface stress
 Dout(M2bstr) == T ! ubar_bstr, ... bottom stress
- Logical switches (TRUE/FALSE) to activate writing of time-averaged, 3D momentum (u,v) diagnostic terms into the diagnostics output file.                               Dout(M3rate) == T ! u_accel, ... acceleration
 Dout(M3pgrd) == T ! u_prsgrd, ... pressure gradient
 Dout(M3fcor) == T ! u_cor, ... Coriolis force
 Dout(M3hadv) == T ! u_hadv, ... horizontal total advection
 Dout(M3xadv) == T ! u_xadv, ... horizontal XI-advection
 Dout(M3yadv) == T ! u_yadv, ... horizontal ETA-advection
 Dout(M3vadv) == T ! u_vadv, ... vertical advection
 Dout(M3hrad) == T ! u_hrad, ... horizontal total radiation stress
 Dout(M3vrad) == T ! u_vrad, ... vertical radiation stress
 Dout(M3hvis) == T ! u_hvisc, ... horizontal total viscosity
 Dout(M3xvis) == T ! u_xvisc, ... horizontal XI-viscosity
 Dout(M3yvis) == T ! u_yvisc, ... horizontal ETA-viscosity
 Dout(M3vvis) == T ! u_vvisc, ... vertical viscosity
- Logical switches (TRUE/FALSE) to activate writing of time-averaged, active (temperature and salinity) and passive (inert) tracer diagnostic terms into the diagnostics output file. [1:NAT+NPT,1:Ngrids] values are expected.Dout(iTrate) == T T ! temp_rate, ... time rate of change
 Dout(iThadv) == T T ! temp_hadv, ... horizontal total advection
 Dout(iTxadv) == T T ! temp_xadv, ... horizontal XI-advection
 Dout(iTyadv) == T T ! temp_yadv, ... horizontal ETA-advection
 Dout(iTvadv) == T T ! temp_vadv, ... vertical advection
 Dout(iThdif) == T T ! temp_hdiff, ... horizontal total diffusion
 Dout(iTxdif) == T T ! temp_xdiff, ... horizontal XI-diffusion
 Dout(iTydif) == T T ! temp_ydiff, ... horizontal ETA-diffusion
 Dout(iTsdif) == T T ! temp_sdiff, ... horizontal S-diffusion
 Dout(iTvdif) == T T ! temp_vdiff, ... vertical diffusion
Generic User Parameters
- NUSER is the number (integer) of user parameters to consider. USER is a vector containing NUSER user parameters (real array).This array is primarily used with the SANITY_CHECK to test the correctness of the tangent linear adjoint models. It contains the model variable and grid point to perturb:! INT(user(1)): tangent state variable to perturbSet tangent and adjoint parameters to the same values if perturbing and reporting the same variable.
 ! INT(user(2)): adjoint state variable to perturb
 ! [ isFsur = 1 ] free-surface
 ! [ isUbar = 2 ] 2D U-momentum
 ! [ isVbar = 3 ] 2D V-momentum
 ! [ isUvel = 4 ] 3D U-momentum
 ! [ isVvel = 5 ] 3D V-momentum
 ! [ isTvar = 6 ] First tracer (temperature)
 ! [ ... ] ...
 ! [ isTvar = ? ] Last tracer
 !
 ! INT(user(3)): I-index of tangent variable to perturb
 ! INT(user(4)): I-index of adjoint variable to perturb
 ! INT(user(5)): J-index of tangent variable to perturb
 ! INT(user(6)): J-index of adjoint variable to perturb
 ! INT(user(7)): K-index of tangent variable to perturb, if 3D
 ! INT(user(8)): K-index of adjoint variable to perturb, if 3D
- This parameter could also be used to adjust constants in analytical functions at run time.
NetCDF-4/HDF5 Compression Parameters
- NetCDF-4/HDF5 compression parameters for output files. This capability is used when both HDF5 and DEFLATE C-preprocessing options are activated. The user needs to compile with the NetCDF-4/HDF5 and MPI libraries. File deflation cannot be used in parallel I/O for writing libraries. File deflation cannot be used in parallel I/O for writing to exactly map the data to the disk location.  For more information, check NetCDF official website.NC_SHUFFLE = 1 ! if non-zero, turn on shuffle filter
 NC_DEFLATE = 1 ! if non-zero, turn on deflate filter
 NC_DLEVEL = 1 ! deflate level [0-9]
Input NetCDF Files
 NOTE: Starting with revision 460 file names can be up to 256 characters long. Previously only 80 characters were allowed.
NOTE: Starting with revision 460 file names can be up to 256 characters long. Previously only 80 characters were allowed.
- Input NetCDF file names, [1:Ngrids] values are expected.GRDNAME == roms_grd.nc ! Grid
 ININAME == roms_ini.nc ! NLM initial conditions
 ITLNAME == roms_itl.nc ! TLM initial conditions
 IRPNAME == roms_irp.nc ! RPM initial conditions
 IADNAME == roms_iad.nc ! ADM initial conditions
 FWDNAME == roms_fwd.nc ! Forward trajectory
 ADSNAME == roms_ads.nc ! Adjoint sensitivity functionals
- Input adjoint forcing NetCDF filenames for computing observations impacts during the analysis-forecast cycle. If the forecast error metric is defined in state-space, then FOInameA and FOInameB should be regular adjoint forcing files just like ADSNAME. If the forecast error metric is defined in observation space (OBS_SPACE is activated) then the forecast is initialized OIFnameA and OIFnameB (specified in s4dvar.in input script) will have the structure of a 4D-Var observation file.
- Input NetCDF filenames for the forecasts initialized from the analysis of the current 4D-Var cycle (FCTnameA) and initialized from the analysis of the previous 4D-Var cycle (FCTnameB).
- Nesting grids connectivity data: contact points information. This NetCDF file is special and complex. It is currently generated using the script matlab/grid/contact.m from the Matlab repository.NGCNAME = roms_ngc.nc
- Input lateral boundary conditions and climatology file names. The user has the option to split input data time records into several NetCDF files (see the File Syntax Notes). If so, use a single line per entry with a vertical bar (|) symbol after each entry, except the last one.
- Input climatology nudging coefficients file name.NUDNAME == roms_nud.nc
- Input Sources/Sinks forcing (like river runoff) file name. This file is separated from the regular forcing files to allow manipulations over nested grids. A particular nesting grid may or may not have Sources/Sinks forcing.SSFNAME == roms_rivers.nc
- Input tidal forcing file name.TIDENAME == roms_tides.nc
- Input forcing NetCDF file name(s). The user has the option to enter several files names for each nested grid. For example, the user may have a different files for wind products, heat fluxes, tides, etc. The model will scan the file list and will read the needed data from the first file in the list containing the forcing field. Therefore, the order of the file names is very important. If multiple forcing files per grid, enter first all the file names for grid 1, then grid 2, and so on. It is also possible to split input data time records into several NetCDF files (see the File Syntax Notes). Use a single line per entry with a continuation ( \ ) or vertical bar ( | ) symbol after each entry, except the last one.
Output NetCDF Files
 NOTE: Starting with revision 460 file names can be up to 256 characters long. Previously only 80 characters were allowed.
NOTE: Starting with revision 460 file names can be up to 256 characters long. Previously only 80 characters were allowed.
- Output NetCDF file names, [1:Ngrids] files are expected.DAINAME == roms_dai.nc ! Data assimilation next cycle initial conditions or restart file
 GSTNAME == roms_gst.nc ! GST analysis restart
 RSTNAME == roms_rst.nc ! Restart
 HISNAME == roms_his.nc ! History
 QCKNAME == roms_qck.nc ! Quicksave
 TLMNAME == roms_tlm.nc ! TLM history
 TLFNAME == roms_tlf.nc ! Impulse TLM forcing
 ADJNAME == roms_adj.nc ! ADM history
 AVGNAME == roms_avg.nc ! Averages
 HARNAME == roms_har.nc ! least-squares detiding harmonics
 DIANAME == roms_dia.nc ! Diagnostics
 STANAME == roms_sta.nc ! Stations
 FLTNAME == roms_flt.nc ! Floats
Additional Input Scripts
 NOTE: Starting with revision 460 file names can be up to 256 characters long. Previously only 80 characters were allowed.
NOTE: Starting with revision 460 file names can be up to 256 characters long. Previously only 80 characters were allowed.
- Input ASCII parameter filenames.APARNAM = ROMS/External/s4dvar.in
 SPOSNAM = ROMS/External/stations.in
 FPOSNAM = ROMS/External/floats.in
 BPARNAM = ROMS/External/biology.in
 SPARNAM = ROMS/External/sediment.in
 USRNAME = ROMS/External/MyFile.dat
