1 |
m_bates |
1.21 |
C $Header: /u/gcmpack/MITgcm/pkg/gmredi/gmredi_k3d.F,v 1.20 2015/01/20 20:52:12 jmc Exp $ |
2 |
m_bates |
1.1 |
C $Name: $ |
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jmc |
1.19 |
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4 |
m_bates |
1.1 |
#include "GMREDI_OPTIONS.h" |
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C !ROUTINE: GMREDI_K3D |
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C !INTERFACE: |
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SUBROUTINE GMREDI_K3D( |
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I iMin, iMax, jMin, jMax, |
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I sigmaX, sigmaY, sigmaR, |
11 |
m_bates |
1.4 |
I bi, bj, myTime, myThid ) |
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m_bates |
1.1 |
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C !DESCRIPTION: \bv |
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C *==========================================================* |
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C | SUBROUTINE GMREDI_K3D |
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C | o Calculates the 3D diffusivity as per Bates et al. (2013) |
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C *==========================================================* |
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C \ev |
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IMPLICIT NONE |
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C == Global variables == |
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#include "SIZE.h" |
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jmc |
1.19 |
#include "EEPARAMS.h" |
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#include "PARAMS.h" |
26 |
m_bates |
1.1 |
#include "GRID.h" |
27 |
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#include "DYNVARS.h" |
28 |
jmc |
1.20 |
#include "FFIELDS.h" |
29 |
m_bates |
1.1 |
#include "GMREDI.h" |
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31 |
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C !INPUT/OUTPUT PARAMETERS: |
32 |
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C == Routine arguments == |
33 |
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C bi, bj :: tile indices |
34 |
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C myThid :: My Thread Id. number |
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36 |
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INTEGER iMin,iMax,jMin,jMax |
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_RL sigmaX(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
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_RL sigmaY(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
39 |
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_RL sigmaR(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
40 |
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INTEGER bi, bj |
41 |
m_bates |
1.4 |
_RL myTime |
42 |
m_bates |
1.1 |
INTEGER myThid |
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44 |
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#ifdef GM_K3D |
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46 |
m_bates |
1.4 |
C === Functions ==== |
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LOGICAL DIFFERENT_MULTIPLE |
48 |
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EXTERNAL DIFFERENT_MULTIPLE |
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50 |
m_bates |
1.1 |
C !LOCAL VARIABLES: |
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C == Local variables == |
52 |
m_bates |
1.4 |
INTEGER i,j,k,kk,m |
53 |
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54 |
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C update_modes :: Whether to update the eigenmodes |
55 |
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LOGICAL update_modes |
56 |
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57 |
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C surfk :: index of the depth of the surface layer |
58 |
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C kLow_C :: Local version of the index of deepest wet grid cell on tracer grid |
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C kLow_U :: Local version of the index of deepest wet grid cell on U grid |
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C kLow_V :: Local version of the index of deepest wet grid cell on V grid |
61 |
m_bates |
1.1 |
INTEGER surfk(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
62 |
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INTEGER kLow_C(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
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INTEGER kLow_U(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
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INTEGER kLow_V(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
65 |
m_bates |
1.4 |
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66 |
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C N2loc :: local N**2 |
67 |
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C slope :: local slope |
68 |
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C Req :: local equatorial deformation radius (m) |
69 |
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C deltaH :: local thickness of Eady integration (m) |
70 |
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C g_reciprho_sq :: (gravity*recip_rhoConst)**2 |
71 |
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C M4loc :: local M**4 |
72 |
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C maxDRhoDz :: maximum value of d(rho)/dz (derived from GM_K3D_minN2) |
73 |
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C sigx :: local d(rho)/dx |
74 |
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C sigy :: local d(rho)/dy |
75 |
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C sigz :: local d(rho)/dz |
76 |
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C hsurf :: local surface layer depth |
77 |
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C small :: a small number (to avoid floating point exceptions) |
78 |
m_bates |
1.10 |
_RL N2loc(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
79 |
m_bates |
1.1 |
_RL slope |
80 |
m_bates |
1.10 |
_RL slopeC(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
81 |
m_bates |
1.4 |
_RL Req |
82 |
m_bates |
1.10 |
_RL deltaH(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
83 |
m_bates |
1.1 |
_RL g_reciprho_sq |
84 |
m_bates |
1.10 |
_RL M4loc(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
85 |
m_bates |
1.13 |
_RL M4onN2(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
86 |
m_bates |
1.1 |
_RL maxDRhoDz |
87 |
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_RL sigx, sigy, sigz |
88 |
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_RL hsurf |
89 |
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_RL small |
90 |
m_bates |
1.4 |
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91 |
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C dfdy :: gradient of the Coriolis paramter, df/dy, 1/(m*s) |
92 |
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C dfdx :: gradient of the Coriolis paramter, df/dx, 1/(m*s) |
93 |
m_bates |
1.6 |
C gradf :: gradient of the Coriolis paramter at a cell centre, 1/(m*s) |
94 |
m_bates |
1.8 |
C Rurms :: a local mixing length used in calculation of urms (m) |
95 |
m_bates |
1.4 |
C RRhines :: The Rhines scale (m) |
96 |
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C Rmix :: Mixing length |
97 |
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C N2 :: Square of the buoyancy frequency (1/s**2) |
98 |
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C N2W :: Square of the buoyancy frequency (1/s**2) averaged to west of grid cell |
99 |
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C N2S :: Square of the buoyancy frequency (1/s**2) averaged to south of grid cell |
100 |
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C N :: Buoyancy frequency, SQRT(N2) |
101 |
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C BVint :: The vertical integral of N (m/s) |
102 |
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C ubar :: Zonal velocity on a tracer point (m/s) |
103 |
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C vbar :: Meridional velocity on a tracer point (m/s) |
104 |
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C Ubaro :: Barotropic velocity (m/s) |
105 |
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_RL dfdy( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
106 |
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_RL dfdx( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
107 |
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_RL gradf( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
108 |
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_RL dummy( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
109 |
m_bates |
1.8 |
_RL Rurms( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
110 |
m_bates |
1.4 |
_RL RRhines(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
111 |
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_RL Rmix( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
112 |
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_RL N2( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
113 |
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_RL N2W( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
114 |
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_RL N2S( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
115 |
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_RL N( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
116 |
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_RL BVint( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
117 |
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_RL Ubaro( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
118 |
m_bates |
1.21 |
_RL ubar( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
119 |
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120 |
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_RL tmpU( 1-Olx:sNx+Olx,1-Oly:sNy+Oly ) |
121 |
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_RL tmpV( 1-Olx:sNx+Olx,1-Oly:sNy+Oly ) |
122 |
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_RL uFldX( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr ) |
123 |
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_RL vFldY( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr ) |
124 |
m_bates |
1.4 |
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125 |
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C Rmid :: Rossby radius (m) |
126 |
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C KPV :: Diffusivity (m**2/s) |
127 |
m_bates |
1.13 |
C Kdqdx :: diffusivity multiplied by zonal PV gradient |
128 |
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C Kdqdy :: diffusivity multiplied by meridional PV gradient |
129 |
m_bates |
1.4 |
C SlopeX :: isopycnal slope in x direction |
130 |
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C SlopeY :: isopycnal slope in y direction |
131 |
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C dSigmaDx :: sigmaX averaged onto tracer grid |
132 |
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C dSigmaDy :: sigmaY averaged onto tracer grid |
133 |
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C tfluxX :: thickness flux in x direction |
134 |
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C tfluxY :: thickness flux in y direction |
135 |
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C fCoriU :: Coriolis parameter averaged to U points |
136 |
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C fCoriV :: Coriolis parameter averaged to V points |
137 |
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C cori :: Coriolis parameter forced to be finite near the equator |
138 |
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C coriU :: As for cori, but, at U point |
139 |
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C coriV :: As for cori, but, at V point |
140 |
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C surfkz :: Depth of surface layer (in r units) |
141 |
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_RL Rmid(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
142 |
m_bates |
1.3 |
_RL KPV(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
143 |
m_bates |
1.13 |
_RL Kdqdy(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
144 |
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_RL Kdqdx(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
145 |
m_bates |
1.1 |
_RL SlopeX(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
146 |
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_RL SlopeY(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
147 |
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_RL dSigmaDx(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
148 |
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_RL dSigmaDy(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
149 |
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_RL tfluxX(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
150 |
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_RL tfluxY(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
151 |
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_RL cori(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
152 |
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_RL coriU(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
153 |
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_RL coriV(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
154 |
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_RL fCoriU(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
155 |
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_RL fCoriV(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
156 |
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_RL surfkz(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
157 |
m_bates |
1.4 |
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158 |
m_bates |
1.16 |
C centreX,centreY :: used for calculating averages at centre of cell |
159 |
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C numerator,denominator :: of the renormalisation factor |
160 |
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C uInt :: column integral of u velocity (sum u*dz) |
161 |
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C vInt :: column integral of v velocity (sum v*dz) |
162 |
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C KdqdxInt :: column integral of K*dqdx (sum K*dqdx*dz) |
163 |
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C KdqdyInt :: column integral of K*dqdy (sum K*dqdy*dz) |
164 |
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C uKdqdyInt :: column integral of u*K*dqdy (sum u*K*dqdy*dz) |
165 |
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C vKdqdxInt :: column integral of v*K*dqdx (sum v*K*dqdx*dz) |
166 |
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C uXiyInt :: column integral of u*Xiy (sum u*Xiy*dz) |
167 |
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C vXixInt :: column integral of v*Xix (sum v*Xix*dz) |
168 |
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C Renorm :: renormalisation factor at the centre of a cell |
169 |
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C RenormU :: renormalisation factor at the western face of a cell |
170 |
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C RenormV :: renormalisation factor at the southern face of a cell |
171 |
m_bates |
1.15 |
_RL centreX, centreY |
172 |
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_RL numerator, denominator |
173 |
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_RL uInt(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
174 |
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_RL vInt(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
175 |
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_RL KdqdxInt(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
176 |
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_RL KdqdyInt(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
177 |
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_RL uKdqdyInt(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
178 |
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_RL vKdqdxInt(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
179 |
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_RL uXiyInt(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
180 |
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_RL vXixInt(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
181 |
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_RL Renorm(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
182 |
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_RL RenormU(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
183 |
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_RL RenormV(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
184 |
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185 |
m_bates |
1.4 |
C gradqx :: Potential vorticity gradient in x direction |
186 |
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C gradqy :: Potential vorticity gradient in y direction |
187 |
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C XimX :: Vertical integral of phi_m*K*gradqx |
188 |
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C XimY :: Vertical integral of phi_m*K*gradqy |
189 |
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C cDopp :: Quasi-Doppler shifted long Rossby wave speed (m/s) |
190 |
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C umc :: ubar-c (m/s) |
191 |
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C eady :: Eady growth rate (1/s) |
192 |
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C urms :: the rms eddy velocity (m/s) |
193 |
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C supp :: The suppression factor |
194 |
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C ustar :: The eddy induced velocity in the x direction |
195 |
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C vstar :: The eddy induced velocity in the y direction |
196 |
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C Xix :: Xi in the x direction (m/s**2) |
197 |
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C Xiy :: Xi in the y direction (m/s**2) |
198 |
m_bates |
1.1 |
_RL gradqx(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
199 |
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_RL gradqy(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
200 |
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_RL XimX(GM_K3D_NModes,1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
201 |
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_RL XimY(GM_K3D_NModes,1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
202 |
m_bates |
1.4 |
_RL cDopp(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
203 |
m_bates |
1.1 |
_RL umc( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
204 |
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_RL eady( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
205 |
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_RL urms( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
206 |
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_RL supp( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
207 |
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_RL ustar(1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
208 |
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_RL vstar(1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
209 |
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_RL Xix( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
210 |
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_RL Xiy( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
211 |
m_bates |
1.4 |
#ifdef GM_K3D_PASSIVE |
212 |
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C psistar :: eddy induced streamfunction in the y direction |
213 |
m_bates |
1.1 |
_RL psistar(1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
214 |
m_bates |
1.4 |
#endif |
215 |
m_bates |
1.1 |
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216 |
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C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
217 |
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218 |
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C ====================================== |
219 |
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C Initialise some variables |
220 |
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C ====================================== |
221 |
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small = TINY(zeroRL) |
222 |
m_bates |
1.4 |
update_modes=.FALSE. |
223 |
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IF ( DIFFERENT_MULTIPLE(GM_K3D_vecFreq,myTime,deltaTClock) ) |
224 |
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& update_modes=.TRUE. |
225 |
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226 |
m_bates |
1.1 |
DO j=1-Oly,sNy+Oly |
227 |
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DO i=1-Olx,sNx+Olx |
228 |
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kLow_C(i,j) = kLowC(i,j,bi,bj) |
229 |
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ENDDO |
230 |
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ENDDO |
231 |
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DO j=1-Oly,sNy+Oly |
232 |
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DO i=1-Olx+1,sNx+Olx |
233 |
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kLow_U(i,j) = MIN( kLow_C(i,j), kLow_C(i-1,j) ) |
234 |
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ENDDO |
235 |
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ENDDO |
236 |
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DO j=1-Oly+1,sNy+Oly |
237 |
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DO i=1-Olx,sNx+Olx |
238 |
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kLow_V(i,j) = MIN( kLow_C(i,j), kLow_C(i,j-1) ) |
239 |
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ENDDO |
240 |
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ENDDO |
241 |
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242 |
m_bates |
1.18 |
C Dummy values for the edges. This does not affect the results |
243 |
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C but avoids problems when solving for the eigenvalues. |
244 |
m_bates |
1.1 |
i=1-Olx |
245 |
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DO j=1-Oly,sNy+Oly |
246 |
m_bates |
1.18 |
kLow_U(i,j) = 0 |
247 |
m_bates |
1.1 |
ENDDO |
248 |
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j=1-Oly |
249 |
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DO i=1-Olx,sNx+Olx |
250 |
m_bates |
1.18 |
kLow_V(i,j) = 0 |
251 |
m_bates |
1.1 |
ENDDO |
252 |
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253 |
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g_reciprho_sq = (gravity*recip_rhoConst)**2 |
254 |
|
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C Gradient of Coriolis |
255 |
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DO j=1-Oly+1,sNy+Oly |
256 |
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DO i=1-Olx+1,sNx+Olx |
257 |
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dfdx(i,j) = ( fCori(i,j,bi,bj)-fCori(i-1,j,bi,bj) ) |
258 |
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& *recip_dxC(i,j,bi,bj) |
259 |
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dfdy(i,j) = ( fCori(i,j,bi,bj)-fCori(i,j-1,bi,bj) ) |
260 |
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& *recip_dyC(i,j,bi,bj) |
261 |
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ENDDO |
262 |
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ENDDO |
263 |
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264 |
jmc |
1.20 |
C Coriolis at C points enforcing a minimum value so |
265 |
m_bates |
1.1 |
C that it is defined at the equator |
266 |
|
|
DO j=1-Oly,sNy+Oly |
267 |
|
|
DO i=1-Olx,sNx+Olx |
268 |
|
|
cori(i,j) = SIGN( MAX( ABS(fCori(i,j,bi,bj)),GM_K3D_minCori ), |
269 |
|
|
& fCori(i,j,bi,bj) ) |
270 |
|
|
ENDDO |
271 |
|
|
ENDDO |
272 |
|
|
C Coriolis at U and V points |
273 |
m_bates |
1.17 |
DO j=1-Oly,sNy+Oly |
274 |
m_bates |
1.1 |
DO i=1-Olx+1,sNx+Olx |
275 |
|
|
C Limited so that the inverse is defined at the equator |
276 |
|
|
coriU(i,j) = op5*( cori(i,j)+cori(i-1,j) ) |
277 |
jmc |
1.20 |
coriU(i,j) = SIGN( MAX( ABS(coriU(i,j)),GM_K3D_minCori ), |
278 |
m_bates |
1.1 |
& coriU(i,j) ) |
279 |
|
|
|
280 |
m_bates |
1.17 |
C Not limited |
281 |
|
|
fCoriU(i,j) = op5*( fCori(i,j,bi,bj)+fCori(i-1,j,bi,bj) ) |
282 |
|
|
ENDDO |
283 |
|
|
ENDDO |
284 |
|
|
DO j=1-Oly+1,sNy+Oly |
285 |
|
|
DO i=1-Olx,sNx+Olx |
286 |
|
|
C Limited so that the inverse is defined at the equator |
287 |
m_bates |
1.1 |
coriV(i,j) = op5*( cori(i,j)+cori(i,j-1) ) |
288 |
jmc |
1.20 |
coriV(i,j) = SIGN( MAX( ABS(coriV(i,j)),GM_K3D_minCori ), |
289 |
m_bates |
1.1 |
& coriV(i,j) ) |
290 |
|
|
|
291 |
|
|
C Not limited |
292 |
|
|
fCoriV(i,j) = op5*( fCori(i,j,bi,bj)+fCori(i,j-1,bi,bj) ) |
293 |
|
|
ENDDO |
294 |
|
|
ENDDO |
295 |
|
|
DO j=1-Oly,sNy+Oly |
296 |
|
|
DO i=1-Olx,sNx+Olx |
297 |
m_bates |
1.6 |
gradf(i,j) = recip_rSphere*fCoriCos(i,j,bi,bj) |
298 |
m_bates |
1.1 |
ENDDO |
299 |
|
|
ENDDO |
300 |
m_bates |
1.17 |
C Some dummy values at the edges |
301 |
|
|
i=1-Olx |
302 |
|
|
DO j=1-Oly,sNy+Oly |
303 |
|
|
coriU(i,j)=cori(i,j) |
304 |
|
|
fCoriU(i,j)=fCori(i,j,bi,bj) |
305 |
|
|
ENDDO |
306 |
|
|
j=1-Oly |
307 |
|
|
DO i=1-Olx,sNx+Olx |
308 |
|
|
coriV(i,j)=cori(i,j) |
309 |
|
|
fCoriV(i,j)=fCori(i,j,bi,bj) |
310 |
|
|
ENDDO |
311 |
m_bates |
1.1 |
|
312 |
|
|
C Zeroing some cumulative fields |
313 |
|
|
DO j=1-Oly,sNy+Oly |
314 |
|
|
DO i=1-Olx,sNx+Olx |
315 |
m_bates |
1.10 |
eady(i,j) = zeroRL |
316 |
|
|
BVint(i,j) = zeroRL |
317 |
|
|
Ubaro(i,j) = zeroRL |
318 |
|
|
deltaH(i,j) = zeroRL |
319 |
|
|
ENDDO |
320 |
|
|
ENDDO |
321 |
|
|
DO k=1,Nr |
322 |
|
|
DO j=1-Oly,sNy+Oly |
323 |
|
|
DO i=1-Olx,sNx+Olx |
324 |
|
|
slopeC(i,j,k)=zeroRL |
325 |
|
|
ENDDO |
326 |
m_bates |
1.1 |
ENDDO |
327 |
|
|
ENDDO |
328 |
|
|
|
329 |
m_bates |
1.17 |
C initialise remaining 2d variables |
330 |
|
|
DO j=1-Oly,sNy+Oly |
331 |
|
|
DO i=1-Olx,sNx+Olx |
332 |
|
|
dfdy(i,j)=zeroRL |
333 |
|
|
dfdy(i,j)=zeroRL |
334 |
|
|
Rurms(i,j)=zeroRL |
335 |
|
|
RRhines(i,j)=zeroRL |
336 |
|
|
Rmix(i,j)=zeroRL |
337 |
|
|
ENDDO |
338 |
|
|
ENDDO |
339 |
|
|
C initialise remaining 3d variables |
340 |
|
|
DO k=1,Nr |
341 |
|
|
DO j=1-Oly,sNy+Oly |
342 |
|
|
DO i=1-Olx,sNx+Olx |
343 |
|
|
N2loc(i,j,k)=GM_K3D_minN2 |
344 |
|
|
N2W(i,j,k) = GM_K3D_minN2 |
345 |
|
|
N2S(i,j,k) = GM_K3D_minN2 |
346 |
|
|
M4loc(i,j,k)=zeroRL |
347 |
|
|
M4onN2(i,j,k)=zeroRL |
348 |
|
|
urms(i,j,k)=zeroRL |
349 |
|
|
SlopeX(i,j,k)=zeroRL |
350 |
|
|
SlopeY(i,j,k)=zeroRL |
351 |
|
|
dSigmaDx(i,j,k)=zeroRL |
352 |
|
|
dSigmaDy(i,j,k)=zeroRL |
353 |
|
|
gradqx(i,j,k)=zeroRL |
354 |
|
|
gradqy(i,j,k)=zeroRL |
355 |
|
|
ENDDO |
356 |
|
|
ENDDO |
357 |
|
|
ENDDO |
358 |
|
|
|
359 |
m_bates |
1.1 |
C Find the zonal velocity at the cell centre |
360 |
jmc |
1.20 |
#ifdef ALLOW_EDDYPSI |
361 |
m_bates |
1.9 |
IF (GM_InMomAsStress) THEN |
362 |
m_bates |
1.21 |
DO k=1,Nr |
363 |
|
|
DO i = 1-olx,snx+olx |
364 |
|
|
DO j = 1-oly,sny+oly |
365 |
|
|
uFldX(i,j,k) = uEulerMean(i,j,k,bi,bj) |
366 |
|
|
vFldY(i,j,k) = vEulerMean(i,j,k,bi,bj) |
367 |
|
|
ENDDO |
368 |
|
|
ENDDO |
369 |
|
|
ENDDO |
370 |
m_bates |
1.9 |
ELSE |
371 |
|
|
#endif |
372 |
m_bates |
1.21 |
DO k=1,Nr |
373 |
|
|
DO i = 1-olx,snx+olx |
374 |
|
|
DO j = 1-oly,sny+oly |
375 |
|
|
uFldX(i,j,k) = uVel(i,j,k,bi,bj) |
376 |
|
|
vFldY(i,j,k) = vVel(i,j,k,bi,bj) |
377 |
|
|
ENDDO |
378 |
|
|
ENDDO |
379 |
|
|
ENDDO |
380 |
jmc |
1.20 |
#ifdef ALLOW_EDDYPSI |
381 |
m_bates |
1.9 |
ENDIF |
382 |
|
|
#endif |
383 |
m_bates |
1.1 |
|
384 |
m_bates |
1.21 |
C The following comes from rotate_uv2en_rl |
385 |
|
|
C This code does two things: |
386 |
|
|
C 1) go from C grid velocity points to A grid velocity points |
387 |
|
|
C 2) go from model grid directions to east/west directions |
388 |
|
|
DO k = 1,Nr |
389 |
|
|
|
390 |
|
|
DO i = 1-Olx,sNx+Olx |
391 |
|
|
j=sNy+Oly |
392 |
|
|
tmpU(i,j)=zeroRL |
393 |
|
|
tmpV(i,j)=zeroRL |
394 |
|
|
ENDDO |
395 |
|
|
DO j = 1-Oly,sNy+Oly-1 |
396 |
|
|
i=sNx+Olx |
397 |
|
|
tmpU(i,j)=zeroRL |
398 |
|
|
tmpV(i,j)=zeroRL |
399 |
|
|
DO i = 1-Olx,sNx+Olx-1 |
400 |
|
|
tmpU(i,j) = 0.5 _d 0 |
401 |
|
|
& *( uFldX(i+1,j,k) + uFldX(i,j,k) ) |
402 |
|
|
tmpV(i,j) = 0.5 _d 0 |
403 |
|
|
& *( vFldY(i,j+1,k) + vFldY(i,j,k) ) |
404 |
|
|
|
405 |
|
|
tmpU(i,j) = tmpU(i,j) * maskC(i,j,k,bi,bj) |
406 |
|
|
tmpV(i,j) = tmpV(i,j) * maskC(i,j,k,bi,bj) |
407 |
|
|
ENDDO |
408 |
|
|
ENDDO |
409 |
|
|
|
410 |
|
|
DO j = 1-oly,sny+oly |
411 |
|
|
DO i = 1-olx,snx+olx |
412 |
|
|
ENDDO |
413 |
|
|
ENDDO |
414 |
|
|
|
415 |
|
|
C rotation |
416 |
|
|
DO j = 1-oly,sny+oly |
417 |
|
|
DO i = 1-olx,snx+olx |
418 |
|
|
ubar(i,j,k) = |
419 |
|
|
& angleCosC(i,j,bi,bj)*tmpU(i,j) |
420 |
|
|
& -angleSinC(i,j,bi,bj)*tmpV(i,j) |
421 |
|
|
ENDDO |
422 |
|
|
ENDDO |
423 |
|
|
ENDDO |
424 |
|
|
|
425 |
m_bates |
1.1 |
C Square of the buoyancy frequency at the top of a grid cell |
426 |
|
|
DO k=2,Nr |
427 |
|
|
DO j=1-Oly,sNy+Oly |
428 |
|
|
DO i=1-Olx,sNx+Olx |
429 |
|
|
N2(i,j,k) = -gravity*recip_rhoConst*sigmaR(i,j,k) |
430 |
|
|
ENDDO |
431 |
|
|
ENDDO |
432 |
|
|
ENDDO |
433 |
|
|
C N2(k=1) is always zero |
434 |
|
|
k=1 |
435 |
|
|
DO j=1-Oly,sNy+Oly |
436 |
|
|
DO i=1-Olx,sNx+Olx |
437 |
m_bates |
1.17 |
N2(i,j,k) = zeroRL |
438 |
|
|
N(i,j,k) = zeroRL |
439 |
m_bates |
1.1 |
ENDDO |
440 |
|
|
ENDDO |
441 |
jmc |
1.20 |
C Enforce a minimum N2 |
442 |
m_bates |
1.1 |
DO k=2,Nr |
443 |
|
|
DO j=1-Oly,sNy+Oly |
444 |
|
|
DO i=1-Olx,sNx+Olx |
445 |
|
|
IF (N2(i,j,k).LT.GM_K3D_minN2) N2(i,j,k)=GM_K3D_minN2 |
446 |
|
|
N(i,j,k) = SQRT(N2(i,j,k)) |
447 |
|
|
ENDDO |
448 |
|
|
ENDDO |
449 |
|
|
ENDDO |
450 |
|
|
C Calculate the minimum drho/dz |
451 |
|
|
maxDRhoDz = -rhoConst*GM_K3D_minN2/gravity |
452 |
|
|
|
453 |
jmc |
1.20 |
C Calculate the barotropic velocity by vertically integrating |
454 |
m_bates |
1.1 |
C and the dividing by the depth of the water column |
455 |
|
|
C Note that Ubaro is on the U grid. |
456 |
|
|
DO k=1,Nr |
457 |
|
|
DO j=1-Oly,sNy+Oly |
458 |
|
|
DO i=1-Olx,sNx+Olx |
459 |
jmc |
1.20 |
Ubaro(i,j) = Ubaro(i,j) + |
460 |
m_bates |
1.21 |
& drF(k)*hfacC(i,j,k,bi,bj)*ubar(i,j,k) |
461 |
m_bates |
1.1 |
ENDDO |
462 |
|
|
ENDDO |
463 |
|
|
ENDDO |
464 |
|
|
DO j=1-Oly,sNy+Oly |
465 |
|
|
DO i=1-Olx,sNx+Olx |
466 |
|
|
IF (kLow_C(i,j).GT.0) THEN |
467 |
|
|
C The minus sign is because r_Low<0 |
468 |
|
|
Ubaro(i,j) = -Ubaro(i,j)/r_Low(i,j,bi,bj) |
469 |
|
|
ENDIF |
470 |
|
|
ENDDO |
471 |
|
|
ENDDO |
472 |
|
|
|
473 |
|
|
C Integrate the buoyancy frequency vertically using the trapezoidal method. |
474 |
|
|
DO k=1,Nr |
475 |
|
|
DO j=1-Oly,sNy+Oly |
476 |
|
|
DO i=1-Olx,sNx+Olx |
477 |
|
|
IF (k.LT.kLow_C(i,j)) THEN |
478 |
|
|
BVint(i,j) = BVint(i,j) + hFacC(i,j,k,bi,bj)*drF(k) |
479 |
|
|
& *(N(i,j,k)+N(i,j,k+1)) |
480 |
|
|
ELSEIF (k.EQ.kLow_C(i,j)) THEN |
481 |
|
|
C Assume that N(z=-H)=0 |
482 |
|
|
BVint(i,j) = BVint(i,j) + hFacC(i,j,k,bi,bj)*drF(k)*N(i,j,k) |
483 |
|
|
ENDIF |
484 |
|
|
ENDDO |
485 |
|
|
ENDDO |
486 |
|
|
ENDDO |
487 |
|
|
DO j=1-Oly,sNy+Oly |
488 |
|
|
DO i=1-Olx,sNx+Olx |
489 |
|
|
BVint(i,j) = op5*BVint(i,j) |
490 |
|
|
ENDDO |
491 |
|
|
ENDDO |
492 |
|
|
|
493 |
|
|
C Calculate the eigenvalues and eigenvectors |
494 |
m_bates |
1.4 |
IF (update_modes) THEN |
495 |
|
|
CALL GMREDI_CALC_EIGS( |
496 |
|
|
I iMin,iMax,jMin,jMax,bi,bj,N2,myThid, |
497 |
|
|
I kLow_C, maskC(:,:,:,bi,bj), |
498 |
|
|
I hfacC(:,:,:,bi,bj), recip_hfacC(:,:,:,bi,bj), |
499 |
|
|
I R_Low(:,:,bi,bj), 1, .TRUE., |
500 |
|
|
O Rmid, modesC(:,:,:,:,bi,bj)) |
501 |
|
|
|
502 |
|
|
C Calculate the Rossby Radius |
503 |
|
|
DO j=1-Oly+1,sNy+Oly |
504 |
|
|
DO i=1-Olx+1,sNx+Olx |
505 |
|
|
Req = SQRT(BVint(i,j)/(2*pi*gradf(i,j))) |
506 |
|
|
Rdef(i,j,bi,bj) = MIN(Rmid(i,j),Req) |
507 |
|
|
ENDDO |
508 |
|
|
ENDDO |
509 |
|
|
ENDIF |
510 |
m_bates |
1.1 |
|
511 |
|
|
C Average dsigma/dx and dsigma/dy onto the centre points |
512 |
jmc |
1.20 |
|
513 |
m_bates |
1.1 |
DO k=1,Nr |
514 |
|
|
DO j=1-Oly,sNy+Oly-1 |
515 |
|
|
DO i=1-Olx,sNx+Olx-1 |
516 |
|
|
dSigmaDx(i,j,k) = op5*(sigmaX(i,j,k)+sigmaX(i+1,j,k)) |
517 |
|
|
dSigmaDy(i,j,k) = op5*(sigmaY(i,j,k)+sigmaY(i,j+1,k)) |
518 |
|
|
ENDDO |
519 |
|
|
ENDDO |
520 |
|
|
ENDDO |
521 |
|
|
|
522 |
|
|
C =============================== |
523 |
|
|
C Calculate the Eady growth rate |
524 |
|
|
C =============================== |
525 |
|
|
DO k=1,Nr |
526 |
|
|
|
527 |
m_bates |
1.10 |
DO j=1-Oly,sNy+Oly-1 |
528 |
|
|
DO i=1-Olx,sNx+Olx-1 |
529 |
jmc |
1.20 |
M4loc(i,j,k) = g_reciprho_sq*( dSigmaDx(i,j,k)**2 |
530 |
m_bates |
1.10 |
& +dSigmaDy(i,j,k)**2 ) |
531 |
|
|
IF (k.NE.kLow_C(i,j)) THEN |
532 |
|
|
N2loc(i,j,k) = op5*(N2(i,j,k)+N2(i,j,k+1)) |
533 |
|
|
ELSE |
534 |
|
|
N2loc(i,j,k) = op5*N2(i,j,k) |
535 |
|
|
ENDIF |
536 |
|
|
ENDDO |
537 |
|
|
ENDDO |
538 |
m_bates |
1.1 |
C The bottom of the grid cell is shallower than the top |
539 |
|
|
C integration level, so, advance the depth. |
540 |
m_bates |
1.10 |
IF (-rF(k+1) .LE. GM_K3D_EadyMinDepth) CYCLE |
541 |
m_bates |
1.1 |
|
542 |
jmc |
1.7 |
C Do not bother going any deeper since the top of the |
543 |
m_bates |
1.1 |
C cell is deeper than the bottom integration level |
544 |
|
|
IF (-rF(k).GE.GM_K3D_EadyMaxDepth) EXIT |
545 |
|
|
|
546 |
|
|
C We are in the integration depth range |
547 |
|
|
DO j=1-Oly,sNy+Oly-1 |
548 |
|
|
DO i=1-Olx,sNx+Olx-1 |
549 |
jmc |
1.20 |
IF ( (kLow_C(i,j).GE.k) .AND. |
550 |
m_bates |
1.10 |
& (-hMixLayer(i,j,bi,bj).LE.-rC(k)) ) THEN |
551 |
m_bates |
1.1 |
|
552 |
m_bates |
1.12 |
slopeC(i,j,k) = SQRT(M4loc(i,j,k))/N2loc(i,j,k) |
553 |
m_bates |
1.1 |
C Limit the slope. Note, this is not all the Eady calculations. |
554 |
m_bates |
1.13 |
IF (slopeC(i,j,k).LE.GM_maxSlope) THEN |
555 |
|
|
M4onN2(i,j,k) = M4loc(i,j,k)/N2loc(i,j,k) |
556 |
m_bates |
1.1 |
ELSE |
557 |
m_bates |
1.13 |
slopeC(i,j,k) = GM_maxslope |
558 |
|
|
M4onN2(i,j,k) = SQRT(M4loc(i,j,k))*GM_maxslope |
559 |
m_bates |
1.1 |
ENDIF |
560 |
jmc |
1.20 |
eady(i,j) = eady(i,j) |
561 |
m_bates |
1.13 |
& + hfacC(i,j,k,bi,bj)*drF(k)*M4onN2(i,j,k) |
562 |
m_bates |
1.10 |
deltaH(i,j) = deltaH(i,j) + drF(k) |
563 |
m_bates |
1.1 |
ENDIF |
564 |
|
|
ENDDO |
565 |
|
|
ENDDO |
566 |
|
|
ENDDO |
567 |
|
|
|
568 |
|
|
DO j=1-Oly,sNy+Oly |
569 |
|
|
DO i=1-Olx,sNx+Olx |
570 |
m_bates |
1.10 |
C If the minimum depth for the integration is deeper than the ocean |
571 |
jmc |
1.20 |
C bottom OR the mixed layer is deeper than the maximum depth of |
572 |
m_bates |
1.10 |
C integration, we set the Eady growth rate to something small |
573 |
|
|
C to avoid floating point exceptions. |
574 |
|
|
C Later, these areas will be given a small diffusivity. |
575 |
|
|
IF (deltaH(i,j).EQ.zeroRL) THEN |
576 |
m_bates |
1.1 |
eady(i,j) = small |
577 |
|
|
|
578 |
m_bates |
1.10 |
C Otherwise, divide over the integration and take the square root |
579 |
|
|
C to actually find the Eady growth rate. |
580 |
m_bates |
1.1 |
ELSE |
581 |
m_bates |
1.10 |
eady(i,j) = SQRT(eady(i,j)/deltaH(i,j)) |
582 |
jmc |
1.20 |
|
583 |
m_bates |
1.1 |
ENDIF |
584 |
|
|
|
585 |
|
|
ENDDO |
586 |
|
|
ENDDO |
587 |
|
|
|
588 |
|
|
C ====================================== |
589 |
|
|
C Calculate the diffusivity |
590 |
|
|
C ====================================== |
591 |
|
|
DO j=1-Oly+1,sNy+Oly |
592 |
|
|
DO i=1-Olx+1,sNx+Olx-1 |
593 |
|
|
C Calculate the Visbeck velocity |
594 |
m_bates |
1.13 |
Rurms(i,j) = MIN(Rdef(i,j,bi,bj),GM_K3D_Rmax) |
595 |
m_bates |
1.8 |
urms(i,j,1) = GM_K3D_Lambda*eady(i,j)*Rurms(i,j) |
596 |
m_bates |
1.1 |
C Set the bottom urms to zero |
597 |
|
|
k=kLow_C(i,j) |
598 |
|
|
IF (k.GT.0) urms(i,j,k) = 0.0 |
599 |
|
|
|
600 |
|
|
C Calculate the Rhines scale |
601 |
|
|
RRhines(i,j) = SQRT(urms(i,j,1)/gradf(i,j)) |
602 |
|
|
|
603 |
|
|
C Calculate the estimated length scale |
604 |
m_bates |
1.4 |
Rmix(i,j) = MIN(Rdef(i,j,bi,bj), RRhines(i,j)) |
605 |
m_bates |
1.13 |
Rmix(i,j) = MAX(Rmix(i,j),GM_K3D_Rmin) |
606 |
m_bates |
1.1 |
|
607 |
|
|
C Calculate the Doppler shifted long Rossby wave speed |
608 |
|
|
C Ubaro is on the U grid so we must average onto the M grid. |
609 |
m_bates |
1.21 |
cDopp(i,j) = Ubaro(i,j) |
610 |
m_bates |
1.4 |
& - gradf(i,j)*Rdef(i,j,bi,bj)*Rdef(i,j,bi,bj) |
611 |
m_bates |
1.1 |
C Limit the wave speed to the namelist variable GM_K3D_maxC |
612 |
|
|
IF (ABS(cDopp(i,j)).GT.GM_K3D_maxC) THEN |
613 |
|
|
cDopp(i,j) = MAX(GM_K3D_maxC, cDopp(i,j)) |
614 |
|
|
ENDIF |
615 |
|
|
|
616 |
|
|
ENDDO |
617 |
|
|
ENDDO |
618 |
|
|
|
619 |
|
|
C Project the surface urms to the subsurface using the first baroclinic mode |
620 |
m_bates |
1.4 |
CALL GMREDI_CALC_URMS( |
621 |
|
|
I iMin,iMax,jMin,jMax,bi,bj,N2,myThid, |
622 |
|
|
U urms) |
623 |
m_bates |
1.1 |
|
624 |
|
|
C Calculate the diffusivity (on the mass grid) |
625 |
|
|
DO k=1,Nr |
626 |
|
|
DO j=1-Oly,sNy+Oly |
627 |
|
|
DO i=1-Olx,sNx+Olx |
628 |
|
|
IF (k.LE.kLow_C(i,j)) THEN |
629 |
m_bates |
1.10 |
IF (deltaH(i,j).EQ.zeroRL) THEN |
630 |
m_bates |
1.1 |
K3D(i,j,k,bi,bj) = GM_K3D_smallK |
631 |
|
|
ELSE |
632 |
|
|
IF (urms(i,j,k).EQ.0.0) THEN |
633 |
|
|
K3D(i,j,k,bi,bj) = GM_K3D_smallK |
634 |
|
|
ELSE |
635 |
m_bates |
1.21 |
umc(i,j,k) =ubar(i,j,k) - cDopp(i,j) |
636 |
m_bates |
1.13 |
supp(i,j,k)=1/(1+GM_K3D_b1*umc(i,j,k)**2/urms(i,j,1)**2) |
637 |
|
|
C 2*Rmix gives the diameter |
638 |
m_bates |
1.1 |
K3D(i,j,k,bi,bj) = GM_K3D_gamma*urms(i,j,k) |
639 |
m_bates |
1.13 |
& *2*Rmix(i,j)*supp(i,j,k) |
640 |
m_bates |
1.1 |
ENDIF |
641 |
|
|
|
642 |
|
|
C Enforce lower and upper bounds on the diffusivity |
643 |
|
|
IF (K3D(i,j,k,bi,bj).LT.GM_K3D_smallK) |
644 |
|
|
& K3D(i,j,k,bi,bj) = GM_K3D_smallK |
645 |
|
|
IF (K3D(i,j,k,bi,bj).GT.GM_maxK3D) |
646 |
|
|
& K3D(i,j,k,bi,bj) = GM_maxK3D |
647 |
|
|
ENDIF |
648 |
|
|
ENDIF |
649 |
|
|
ENDDO |
650 |
|
|
ENDDO |
651 |
|
|
ENDDO |
652 |
|
|
|
653 |
|
|
C ====================================== |
654 |
|
|
C Find the PV gradient |
655 |
|
|
C ====================================== |
656 |
m_bates |
1.3 |
C Calculate the surface layer thickness. |
657 |
jmc |
1.20 |
C Use hMixLayer (calculated in model/src/calc_oce_mxlayer) |
658 |
m_bates |
1.3 |
C for the mixed layer depth. |
659 |
m_bates |
1.1 |
|
660 |
m_bates |
1.3 |
C Enforce a minimum surface layer depth |
661 |
m_bates |
1.1 |
DO j=1-Oly,sNy+Oly |
662 |
|
|
DO i=1-Olx,sNx+Olx |
663 |
m_bates |
1.3 |
surfkz(i,j) = MIN(-GM_K3D_surfMinDepth,-hMixLayer(i,j,bi,bj)) |
664 |
|
|
surfkz(i,j) = MAX(surfkz(i,j),R_low(i,j,bi,bj)) |
665 |
|
|
IF(maskC(i,j,1,bi,bj).EQ.0.0) surfkz(i,j)=0.0 |
666 |
|
|
surfk(i,j) = 0 |
667 |
m_bates |
1.1 |
ENDDO |
668 |
|
|
ENDDO |
669 |
m_bates |
1.4 |
DO k=1,Nr |
670 |
m_bates |
1.1 |
DO j=1-Oly,sNy+Oly |
671 |
|
|
DO i=1-Olx,sNx+Olx |
672 |
jmc |
1.20 |
IF (rF(k).GT.surfkz(i,j) .AND. surfkz(i,j).GE.rF(k+1)) |
673 |
m_bates |
1.3 |
& surfk(i,j) = k |
674 |
m_bates |
1.1 |
ENDDO |
675 |
|
|
ENDDO |
676 |
|
|
ENDDO |
677 |
m_bates |
1.3 |
|
678 |
m_bates |
1.1 |
C Calculate the isopycnal slope |
679 |
|
|
DO j=1-Oly,sNy+Oly-1 |
680 |
|
|
DO i=1-Olx,sNx+Olx-1 |
681 |
|
|
SlopeX(i,j,1) = zeroRL |
682 |
|
|
SlopeY(i,j,1) = zeroRL |
683 |
|
|
ENDDO |
684 |
|
|
ENDDO |
685 |
|
|
DO k=2,Nr |
686 |
|
|
DO j=1-Oly+1,sNy+Oly |
687 |
|
|
DO i=1-Olx+1,sNx+Olx |
688 |
|
|
IF(surfk(i,j).GE.kLowC(i,j,bi,bj)) THEN |
689 |
|
|
C If the surface layer is thinner than the water column |
690 |
|
|
C the set the slope to zero to avoid problems. |
691 |
|
|
SlopeX(i,j,k) = zeroRL |
692 |
|
|
SlopeY(i,j,k) = zeroRL |
693 |
|
|
|
694 |
|
|
ELSE |
695 |
|
|
C Calculate the zonal slope at the western cell face (U grid) |
696 |
m_bates |
1.4 |
sigz = MIN( op5*(sigmaR(i,j,k)+sigmaR(i-1,j,k)), maxDRhoDz ) |
697 |
m_bates |
1.1 |
sigx = op5*( sigmaX(i,j,k)+sigmaX(i,j,k-1) ) |
698 |
|
|
slope = sigx/sigz |
699 |
|
|
IF(ABS(slope).GT.GM_maxSlope) |
700 |
|
|
& slope = SIGN(GM_maxSlope,slope) |
701 |
|
|
SlopeX(i,j,k)=-maskW(i,j,k-1,bi,bj)*maskW(i,j,k,bi,bj)*slope |
702 |
jmc |
1.20 |
|
703 |
m_bates |
1.1 |
C Calculate the meridional slope at the southern cell face (V grid) |
704 |
m_bates |
1.4 |
sigz = MIN( op5*(sigmaR(i,j,k)+sigmaR(i,j-1,k)), maxDRhoDz ) |
705 |
m_bates |
1.1 |
sigy = op5*( sigmaY(i,j,k) + sigmaY(i,j,k-1) ) |
706 |
|
|
slope = sigy/sigz |
707 |
|
|
IF(ABS(slope).GT.GM_maxSlope) |
708 |
|
|
& slope = SIGN(GM_maxSlope,slope) |
709 |
|
|
SlopeY(i,j,k)=-maskS(i,j,k-1,bi,bj)*maskS(i,j,k,bi,bj)*slope |
710 |
|
|
ENDIF |
711 |
|
|
ENDDO |
712 |
|
|
ENDDO |
713 |
|
|
ENDDO |
714 |
|
|
|
715 |
jmc |
1.20 |
C Calculate the thickness flux and diffusivity. These may be altered later |
716 |
m_bates |
1.14 |
C depending on namelist options. |
717 |
m_bates |
1.1 |
C Enforce a zero slope bottom boundary condition for the bottom most cells (k=Nr) |
718 |
|
|
k=Nr |
719 |
|
|
DO j=1-Oly,sNy+Oly |
720 |
|
|
DO i=1-Olx,sNx+Olx |
721 |
|
|
C Zonal thickness flux at the western cell face |
722 |
|
|
tfluxX(i,j,k) = -fCoriU(i,j)*SlopeX(i,j,k) |
723 |
|
|
& *recip_drF(k)*recip_hFacW(i,j,k,bi,bj) |
724 |
|
|
C Meridional thickness flux at the southern cell face |
725 |
|
|
tfluxY(i,j,k) = -fCoriV(i,j)*SlopeY(i,j,k) |
726 |
|
|
& *recip_drF(k)*recip_hFacS(i,j,k,bi,bj) |
727 |
m_bates |
1.14 |
|
728 |
jmc |
1.20 |
C Use the interior diffusivity. Note: if we are using a |
729 |
m_bates |
1.14 |
C constant diffusivity KPV is overwritten later |
730 |
|
|
KPV(i,j,k) = K3D(i,j,k,bi,bj) |
731 |
|
|
|
732 |
m_bates |
1.1 |
ENDDO |
733 |
|
|
ENDDO |
734 |
|
|
|
735 |
m_bates |
1.14 |
C Calculate the thickness flux and diffusivity and for other cells (k<Nr) |
736 |
m_bates |
1.1 |
DO k=Nr-1,1,-1 |
737 |
m_bates |
1.14 |
DO j=1-Oly,sNy+Oly |
738 |
|
|
DO i=1-Olx,sNx+Olx |
739 |
|
|
C Zonal thickness flux at the western cell face |
740 |
|
|
tfluxX(i,j,k)=-fCoriU(i,j)*(SlopeX(i,j,k)-SlopeX(i,j,k+1)) |
741 |
|
|
& *recip_drF(k)*recip_hFacW(i,j,k,bi,bj) |
742 |
|
|
& *maskW(i,j,k,bi,bj) |
743 |
jmc |
1.20 |
|
744 |
m_bates |
1.14 |
C Meridional thickness flux at the southern cell face |
745 |
|
|
tfluxY(i,j,k)=-fCoriV(i,j)*(SlopeY(i,j,k)-SlopeY(i,j,k+1)) |
746 |
|
|
& *recip_drF(k)*recip_hFacS(i,j,k,bi,bj) |
747 |
|
|
& *maskS(i,j,k,bi,bj) |
748 |
jmc |
1.20 |
|
749 |
|
|
C Use the interior diffusivity. Note: if we are using a |
750 |
m_bates |
1.14 |
C constant diffusivity KPV is overwritten later |
751 |
|
|
KPV(i,j,k) = K3D(i,j,k,bi,bj) |
752 |
|
|
ENDDO |
753 |
|
|
ENDDO |
754 |
|
|
ENDDO |
755 |
|
|
|
756 |
jmc |
1.20 |
C Special treatment for the surface layer (if necessary), which overwrites |
757 |
m_bates |
1.14 |
C values in the previous loops. |
758 |
|
|
IF (GM_K3D_ThickSheet .OR. GM_K3D_surfK) THEN |
759 |
|
|
DO k=Nr-1,1,-1 |
760 |
|
|
DO j=1-Oly,sNy+Oly |
761 |
|
|
DO i=1-Olx,sNx+Olx |
762 |
jmc |
1.20 |
IF(k.LE.surfk(i,j)) THEN |
763 |
|
|
C We are in the surface layer. Change the thickness flux |
764 |
m_bates |
1.14 |
C and diffusivity as necessary. |
765 |
|
|
|
766 |
|
|
IF (GM_K3D_ThickSheet) THEN |
767 |
|
|
C We are in the surface layer, so set the thickness flux |
768 |
|
|
C based on the average slope over the surface layer |
769 |
|
|
C If we are on the edge of a "cliff" the surface layer at the |
770 |
jmc |
1.20 |
C centre of the grid point could be deeper than the U or V point. |
771 |
m_bates |
1.14 |
C So, we ensure that we always take a sensible slope. |
772 |
|
|
IF(kLow_U(i,j).LT.surfk(i,j)) THEN |
773 |
|
|
kk=kLow_U(i,j) |
774 |
|
|
hsurf = -rLowW(i,j,bi,bj) |
775 |
|
|
ELSE |
776 |
|
|
kk=surfk(i,j) |
777 |
|
|
hsurf = -surfkz(i,j) |
778 |
|
|
ENDIF |
779 |
|
|
IF(kk.GT.0) THEN |
780 |
|
|
IF(kk.EQ.Nr) THEN |
781 |
|
|
tfluxX(i,j,k) = -fCoriU(i,j)*maskW(i,j,k,bi,bj) |
782 |
|
|
& *SlopeX(i,j,kk)/hsurf |
783 |
|
|
ELSE |
784 |
|
|
tfluxX(i,j,k) = -fCoriU(i,j)*maskW(i,j,k,bi,bj) |
785 |
|
|
& *( SlopeX(i,j,kk)-SlopeX(i,j,kk+1) )/hsurf |
786 |
|
|
ENDIF |
787 |
|
|
ELSE |
788 |
|
|
tfluxX(i,j,k) = zeroRL |
789 |
|
|
ENDIF |
790 |
jmc |
1.20 |
|
791 |
m_bates |
1.14 |
IF(kLow_V(i,j).LT.surfk(i,j)) THEN |
792 |
|
|
kk=kLow_V(i,j) |
793 |
|
|
hsurf = -rLowS(i,j,bi,bj) |
794 |
|
|
ELSE |
795 |
|
|
kk=surfk(i,j) |
796 |
|
|
hsurf = -surfkz(i,j) |
797 |
|
|
ENDIF |
798 |
|
|
IF(kk.GT.0) THEN |
799 |
|
|
IF(kk.EQ.Nr) THEN |
800 |
|
|
tfluxY(i,j,k) = -fCoriV(i,j)*maskS(i,j,k,bi,bj) |
801 |
|
|
& *SlopeY(i,j,kk)/hsurf |
802 |
|
|
ELSE |
803 |
|
|
tfluxY(i,j,k) = -fCoriV(i,j)*maskS(i,j,k,bi,bj) |
804 |
|
|
& *( SlopeY(i,j,kk)-SlopeY(i,j,kk+1) )/hsurf |
805 |
|
|
ENDIF |
806 |
|
|
ELSE |
807 |
|
|
tfluxY(i,j,k) = zeroRL |
808 |
|
|
ENDIF |
809 |
m_bates |
1.4 |
ENDIF |
810 |
m_bates |
1.1 |
|
811 |
m_bates |
1.14 |
IF (GM_K3D_surfK) THEN |
812 |
|
|
C Use a constant K in the surface layer. |
813 |
|
|
KPV(i,j,k) = GM_K3D_constK |
814 |
m_bates |
1.4 |
ENDIF |
815 |
m_bates |
1.1 |
ENDIF |
816 |
m_bates |
1.14 |
ENDDO |
817 |
|
|
ENDDO |
818 |
m_bates |
1.1 |
ENDDO |
819 |
m_bates |
1.14 |
ENDIF |
820 |
m_bates |
1.1 |
|
821 |
|
|
C Calculate gradq |
822 |
m_bates |
1.21 |
IF (GM_K3D_beta_eq_0) THEN |
823 |
m_bates |
1.5 |
C Ignore beta in the calculation of grad(q) |
824 |
m_bates |
1.2 |
DO k=1,Nr |
825 |
|
|
DO j=1-Oly+1,sNy+Oly |
826 |
|
|
DO i=1-Olx+1,sNx+Olx |
827 |
|
|
gradqx(i,j,k) = maskW(i,j,k,bi,bj)*tfluxX(i,j,k) |
828 |
|
|
gradqy(i,j,k) = maskS(i,j,k,bi,bj)*tfluxY(i,j,k) |
829 |
|
|
ENDDO |
830 |
|
|
ENDDO |
831 |
|
|
ENDDO |
832 |
jmc |
1.20 |
|
833 |
m_bates |
1.2 |
ELSE |
834 |
|
|
C Do not ignore beta |
835 |
|
|
DO k=1,Nr |
836 |
|
|
DO j=1-Oly+1,sNy+Oly |
837 |
|
|
DO i=1-Olx+1,sNx+Olx |
838 |
|
|
gradqx(i,j,k) = maskW(i,j,k,bi,bj)*(dfdx(i,j)+tfluxX(i,j,k)) |
839 |
|
|
gradqy(i,j,k) = maskS(i,j,k,bi,bj)*(dfdy(i,j)+tfluxY(i,j,k)) |
840 |
|
|
ENDDO |
841 |
|
|
ENDDO |
842 |
m_bates |
1.1 |
ENDDO |
843 |
m_bates |
1.2 |
ENDIF |
844 |
m_bates |
1.1 |
|
845 |
|
|
C ====================================== |
846 |
|
|
C Find Xi and the eddy induced velocities |
847 |
|
|
C ====================================== |
848 |
|
|
C Find the buoyancy frequency at the west and south faces of a cell |
849 |
|
|
C This is necessary to find the eigenvectors at those points |
850 |
|
|
DO k=1,Nr |
851 |
|
|
DO j=1-Oly+1,sNy+Oly |
852 |
|
|
DO i=1-Olx+1,sNx+Olx |
853 |
|
|
N2W(i,j,k) = maskW(i,j,k,bi,bj) |
854 |
|
|
& *( N2(i,j,k)+N2(i-1,j,k) ) |
855 |
|
|
N2S(i,j,k) = maskS(i,j,k,bi,bj) |
856 |
|
|
& *( N2(i,j,k)+N2(i,j-1,k) ) |
857 |
|
|
ENDDO |
858 |
|
|
ENDDO |
859 |
|
|
ENDDO |
860 |
|
|
|
861 |
m_bates |
1.21 |
C If GM_K3D_use_constK=.TRUE., the diffusivity for the eddy transport is |
862 |
m_bates |
1.14 |
C set to a constant equal to GM_K3D_constK. |
863 |
m_bates |
1.11 |
C If the diffusivity is constant the method here is the same as GM. |
864 |
m_bates |
1.14 |
C If GM_K3D_constRedi=.TRUE. K3D will be set equal to GM_K3D_constK later. |
865 |
m_bates |
1.21 |
IF(GM_K3D_use_constK) THEN |
866 |
m_bates |
1.3 |
DO k=1,Nr |
867 |
|
|
DO j=1-Oly,sNy+Oly |
868 |
|
|
DO i=1-Olx,sNx+Olx |
869 |
|
|
KPV(i,j,k) = GM_K3D_constK |
870 |
|
|
ENDDO |
871 |
m_bates |
1.2 |
ENDDO |
872 |
|
|
ENDDO |
873 |
m_bates |
1.3 |
ENDIF |
874 |
m_bates |
1.2 |
|
875 |
m_bates |
1.3 |
IF (.NOT. GM_K3D_smooth) THEN |
876 |
|
|
C Do not expand K grad(q) => no smoothing |
877 |
jmc |
1.20 |
C May only be done with a constant K, otherwise the |
878 |
m_bates |
1.3 |
C integral constraint is violated. |
879 |
m_bates |
1.2 |
DO k=1,Nr |
880 |
|
|
DO j=1-Oly,sNy+Oly |
881 |
|
|
DO i=1-Olx,sNx+Olx |
882 |
m_bates |
1.3 |
Xix(i,j,k) = -maskW(i,j,k,bi,bj)*KPV(i,j,k)*gradqx(i,j,k) |
883 |
|
|
Xiy(i,j,k) = -maskS(i,j,k,bi,bj)*KPV(i,j,k)*gradqy(i,j,k) |
884 |
m_bates |
1.2 |
ENDDO |
885 |
|
|
ENDDO |
886 |
|
|
ENDDO |
887 |
|
|
|
888 |
|
|
ELSE |
889 |
m_bates |
1.3 |
C Expand K grad(q) in terms of baroclinic modes to smooth |
890 |
|
|
C and satisfy the integral constraint |
891 |
m_bates |
1.2 |
|
892 |
m_bates |
1.1 |
C Start with the X direction |
893 |
|
|
C ------------------------------ |
894 |
|
|
C Calculate the eigenvectors at the West face of a cell |
895 |
m_bates |
1.4 |
IF (update_modes) THEN |
896 |
|
|
CALL GMREDI_CALC_EIGS( |
897 |
|
|
I iMin,iMax,jMin,jMax,bi,bj,N2W,myThid, |
898 |
|
|
I kLow_U,maskW(:,:,:,bi,bj), |
899 |
|
|
I hfacW(:,:,:,bi,bj),recip_hfacW(:,:,:,bi,bj), |
900 |
|
|
I rLowW(:,:,bi,bj),GM_K3D_NModes,.FALSE., |
901 |
|
|
O dummy,modesW(:,:,:,:,bi,bj)) |
902 |
|
|
ENDIF |
903 |
jmc |
1.20 |
|
904 |
m_bates |
1.1 |
C Calculate Xi_m at the west face of a cell |
905 |
|
|
DO j=1-Oly,sNy+Oly |
906 |
|
|
DO i=1-Olx,sNx+Olx |
907 |
|
|
DO m=1,GM_K3D_NModes |
908 |
|
|
XimX(m,i,j) = zeroRL |
909 |
|
|
ENDDO |
910 |
|
|
ENDDO |
911 |
|
|
ENDDO |
912 |
|
|
DO k=1,Nr |
913 |
|
|
DO j=1-Oly,sNy+Oly |
914 |
|
|
DO i=1-Olx,sNx+Olx |
915 |
|
|
DO m=1,GM_K3D_NModes |
916 |
m_bates |
1.13 |
Kdqdx(i,j,k) = KPV(i,j,k)*gradqx(i,j,k) |
917 |
jmc |
1.20 |
XimX(m,i,j) = XimX(m,i,j) |
918 |
m_bates |
1.13 |
& - maskW(i,j,k,bi,bj)*drF(k)*hfacW(i,j,k,bi,bj) |
919 |
|
|
& *Kdqdx(i,j,k)*modesW(m,i,j,k,bi,bj) |
920 |
m_bates |
1.1 |
ENDDO |
921 |
|
|
ENDDO |
922 |
|
|
ENDDO |
923 |
|
|
ENDDO |
924 |
jmc |
1.20 |
|
925 |
m_bates |
1.1 |
C Calculate Xi in the X direction at the west face |
926 |
|
|
DO k=1,Nr |
927 |
|
|
DO j=1-Oly,sNy+Oly |
928 |
|
|
DO i=1-Olx,sNx+Olx |
929 |
|
|
Xix(i,j,k) = zeroRL |
930 |
|
|
ENDDO |
931 |
|
|
ENDDO |
932 |
|
|
ENDDO |
933 |
|
|
DO k=1,Nr |
934 |
|
|
DO j=1-Oly,sNy+Oly |
935 |
|
|
DO i=1-Olx,sNx+Olx |
936 |
|
|
DO m=1,GM_K3D_NModes |
937 |
jmc |
1.20 |
Xix(i,j,k) = Xix(i,j,k) |
938 |
m_bates |
1.4 |
& + maskW(i,j,k,bi,bj)*XimX(m,i,j)*modesW(m,i,j,k,bi,bj) |
939 |
m_bates |
1.1 |
ENDDO |
940 |
|
|
ENDDO |
941 |
|
|
ENDDO |
942 |
|
|
ENDDO |
943 |
|
|
|
944 |
|
|
C Now the Y direction |
945 |
|
|
C ------------------------------ |
946 |
|
|
C Calculate the eigenvectors at the West face of a cell |
947 |
m_bates |
1.4 |
IF (update_modes) THEN |
948 |
|
|
CALL GMREDI_CALC_EIGS( |
949 |
|
|
I iMin,iMax,jMin,jMax,bi,bj,N2S,myThid, |
950 |
|
|
I kLow_V,maskS(:,:,:,bi,bj), |
951 |
|
|
I hfacS(:,:,:,bi,bj),recip_hfacS(:,:,:,bi,bj), |
952 |
|
|
I rLowS(:,:,bi,bj), GM_K3D_NModes, .FALSE., |
953 |
|
|
O dummy,modesS(:,:,:,:,bi,bj)) |
954 |
|
|
ENDIF |
955 |
|
|
|
956 |
m_bates |
1.1 |
DO j=1-Oly,sNy+Oly |
957 |
|
|
DO i=1-Olx,sNx+Olx |
958 |
|
|
DO m=1,GM_K3D_NModes |
959 |
|
|
XimY(m,i,j) = zeroRL |
960 |
|
|
ENDDO |
961 |
|
|
ENDDO |
962 |
|
|
ENDDO |
963 |
|
|
DO k=1,Nr |
964 |
|
|
DO j=1-Oly,sNy+Oly |
965 |
|
|
DO i=1-Olx,sNx+Olx |
966 |
|
|
DO m=1,GM_K3D_NModes |
967 |
m_bates |
1.13 |
Kdqdy(i,j,k) = KPV(i,j,k)*gradqy(i,j,k) |
968 |
m_bates |
1.3 |
XimY(m,i,j) = XimY(m,i,j) |
969 |
|
|
& - drF(k)*hfacS(i,j,k,bi,bj) |
970 |
m_bates |
1.13 |
& *Kdqdy(i,j,k)*modesS(m,i,j,k,bi,bj) |
971 |
m_bates |
1.1 |
ENDDO |
972 |
|
|
ENDDO |
973 |
|
|
ENDDO |
974 |
|
|
ENDDO |
975 |
jmc |
1.20 |
|
976 |
m_bates |
1.1 |
C Calculate Xi for Y direction at the south face |
977 |
|
|
DO k=1,Nr |
978 |
|
|
DO j=1-Oly,sNy+Oly |
979 |
|
|
DO i=1-Olx,sNx+Olx |
980 |
|
|
Xiy(i,j,k) = zeroRL |
981 |
|
|
ENDDO |
982 |
|
|
ENDDO |
983 |
|
|
ENDDO |
984 |
|
|
DO k=1,Nr |
985 |
|
|
DO j=1-Oly,sNy+Oly |
986 |
|
|
DO i=1-Olx,sNx+Olx |
987 |
|
|
DO m=1,GM_K3D_NModes |
988 |
jmc |
1.20 |
Xiy(i,j,k) = Xiy(i,j,k) |
989 |
m_bates |
1.4 |
& + maskS(i,j,k,bi,bj)*XimY(m,i,j)*modesS(m,i,j,k,bi,bj) |
990 |
m_bates |
1.1 |
ENDDO |
991 |
|
|
ENDDO |
992 |
|
|
ENDDO |
993 |
|
|
ENDDO |
994 |
|
|
|
995 |
m_bates |
1.11 |
C ENDIF (.NOT. GM_K3D_smooth) |
996 |
m_bates |
1.1 |
ENDIF |
997 |
|
|
|
998 |
m_bates |
1.15 |
C Calculate the renormalisation factor |
999 |
|
|
DO j=1-Oly,sNy+Oly |
1000 |
|
|
DO i=1-Olx,sNx+Olx |
1001 |
|
|
uInt(i,j)=zeroRL |
1002 |
|
|
vInt(i,j)=zeroRL |
1003 |
|
|
KdqdyInt(i,j)=zeroRL |
1004 |
|
|
KdqdxInt(i,j)=zeroRL |
1005 |
|
|
uKdqdyInt(i,j)=zeroRL |
1006 |
|
|
vKdqdxInt(i,j)=zeroRL |
1007 |
|
|
uXiyInt(i,j)=zeroRL |
1008 |
|
|
vXixInt(i,j)=zeroRL |
1009 |
m_bates |
1.16 |
Renorm(i,j)=oneRL |
1010 |
|
|
RenormU(i,j)=oneRL |
1011 |
|
|
RenormV(i,j)=oneRL |
1012 |
m_bates |
1.15 |
ENDDO |
1013 |
|
|
ENDDO |
1014 |
|
|
DO k=1,Nr |
1015 |
|
|
DO j=1-Oly,sNy+Oly-1 |
1016 |
|
|
DO i=1-Olx,sNx+Olx-1 |
1017 |
|
|
centreX = op5*(uVel(i,j,k,bi,bj)+uVel(i+1,j,k,bi,bj)) |
1018 |
|
|
centreY = op5*(Kdqdy(i,j,k) +Kdqdy(i,j+1,k) ) |
1019 |
|
|
C For the numerator |
1020 |
jmc |
1.20 |
uInt(i,j) = uInt(i,j) |
1021 |
m_bates |
1.15 |
& + centreX*hfacC(i,j,k,bi,bj)*drF(k) |
1022 |
|
|
KdqdyInt(i,j) = KdqdyInt(i,j) |
1023 |
|
|
& + centreY*hfacC(i,j,k,bi,bj)*drF(k) |
1024 |
|
|
uKdqdyInt(i,j) = uKdqdyInt(i,j) |
1025 |
|
|
& + centreX*centreY*hfacC(i,j,k,bi,bj)*drF(k) |
1026 |
|
|
C For the denominator |
1027 |
|
|
centreY = op5*(Xiy(i,j,k) + Xiy(i,j+1,k)) |
1028 |
|
|
uXiyInt(i,j) = uXiyInt(i,j) |
1029 |
|
|
& + centreX*centreY*hfacC(i,j,k,bi,bj)*drF(k) |
1030 |
|
|
|
1031 |
|
|
centreX = op5*(Kdqdx(i,j,k) +Kdqdx(i+1,j,k)) |
1032 |
|
|
centreY = op5*(vVel(i,j,k,bi,bj)+vVel(i,j+1,k,bi,bj) ) |
1033 |
|
|
C For the numerator |
1034 |
|
|
vInt(i,j) = vInt(i,j) |
1035 |
|
|
& + centreY*hfacC(i,j,k,bi,bj)*drF(k) |
1036 |
|
|
KdqdxInt(i,j) = KdqdxInt(i,j) |
1037 |
|
|
& + CentreX*hfacC(i,j,k,bi,bj)*drF(k) |
1038 |
|
|
vKdqdxInt(i,j) = vKdqdxInt(i,j) |
1039 |
|
|
& + centreY*centreX*hfacC(i,j,k,bi,bj)*drF(k) |
1040 |
|
|
C For the denominator |
1041 |
|
|
centreX = op5*(Xix(i,j,k) + Xix(i+1,j,k)) |
1042 |
|
|
vXixInt(i,j) = vXixInt(i,j) |
1043 |
|
|
& + centreY*centreX*hfacC(i,j,k,bi,bj)*drF(k) |
1044 |
|
|
|
1045 |
|
|
ENDDO |
1046 |
|
|
ENDDO |
1047 |
|
|
ENDDO |
1048 |
|
|
|
1049 |
|
|
DO j=1-Oly,sNy+Oly-1 |
1050 |
|
|
DO i=1-Olx,sNx+Olx-1 |
1051 |
|
|
IF (kLowC(i,j,bi,bj).GT.0) THEN |
1052 |
jmc |
1.20 |
numerator = |
1053 |
m_bates |
1.15 |
& (uKdqdyInt(i,j)-uInt(i,j)*KdqdyInt(i,j)/R_low(i,j,bi,bj)) |
1054 |
|
|
& -(vKdqdxInt(i,j)-vInt(i,j)*KdqdxInt(i,j)/R_low(i,j,bi,bj)) |
1055 |
|
|
denominator = uXiyInt(i,j) - vXixInt(i,j) |
1056 |
jmc |
1.20 |
C We can have troubles with floating point exceptions if the denominator |
1057 |
|
|
C of the renormalisation if the ocean is resting (e.g. intial conditions). |
1058 |
m_bates |
1.16 |
C So we make the renormalisation factor one if the denominator is very small |
1059 |
|
|
C The renormalisation factor is supposed to correct the error in the extraction of |
1060 |
|
|
C potential energy associated with the truncation of the expansion. Thus, we |
1061 |
|
|
C enforce a minimum value for the renormalisation factor. |
1062 |
|
|
C We also enforce a maximum renormalisation factor. |
1063 |
|
|
IF (denominator.GT.small) THEN |
1064 |
m_bates |
1.15 |
Renorm(i,j) = ABS(numerator/denominator) |
1065 |
m_bates |
1.16 |
Renorm(i,j) = MAX(Renorm(i,j),GM_K3D_minRenorm) |
1066 |
|
|
Renorm(i,j) = MIN(Renorm(i,j),GM_K3D_maxRenorm) |
1067 |
m_bates |
1.15 |
ENDIF |
1068 |
|
|
ENDIF |
1069 |
|
|
ENDDO |
1070 |
|
|
ENDDO |
1071 |
|
|
C Now put it back on to the velocity grids |
1072 |
|
|
DO j=1-Oly+1,sNy+Oly-1 |
1073 |
|
|
DO i=1-Olx+1,sNx+Olx-1 |
1074 |
|
|
RenormU(i,j) = op5*(Renorm(i-1,j)+Renorm(i,j)) |
1075 |
|
|
RenormV(i,j) = op5*(Renorm(i,j-1)+Renorm(i,j)) |
1076 |
|
|
ENDDO |
1077 |
|
|
ENDDO |
1078 |
|
|
|
1079 |
m_bates |
1.1 |
C Calculate the eddy induced velocity in the X direction at the west face |
1080 |
|
|
DO k=1,Nr |
1081 |
|
|
DO j=1-Oly+1,sNy+Oly |
1082 |
|
|
DO i=1-Olx+1,sNx+Olx |
1083 |
m_bates |
1.16 |
ustar(i,j,k) = -RenormU(i,j)*Xix(i,j,k)/coriU(i,j) |
1084 |
m_bates |
1.1 |
ENDDO |
1085 |
|
|
ENDDO |
1086 |
jmc |
1.20 |
ENDDO |
1087 |
m_bates |
1.1 |
|
1088 |
|
|
C Calculate the eddy induced velocity in the Y direction at the south face |
1089 |
|
|
DO k=1,Nr |
1090 |
|
|
DO j=1-Oly+1,sNy+Oly |
1091 |
|
|
DO i=1-Olx+1,sNx+Olx |
1092 |
m_bates |
1.16 |
vstar(i,j,k) = -RenormV(i,j)*Xiy(i,j,k)/coriV(i,j) |
1093 |
m_bates |
1.1 |
ENDDO |
1094 |
|
|
ENDDO |
1095 |
jmc |
1.20 |
ENDDO |
1096 |
m_bates |
1.1 |
|
1097 |
|
|
C ====================================== |
1098 |
|
|
C Calculate the eddy induced overturning streamfunction |
1099 |
|
|
C ====================================== |
1100 |
|
|
#ifdef GM_K3D_PASSIVE |
1101 |
|
|
k=Nr |
1102 |
|
|
DO j=1-Oly,sNy+Oly |
1103 |
|
|
DO i=1-Olx,sNx+Olx |
1104 |
|
|
psistar(i,j,Nr) = -hfacS(i,j,k,bi,bj)*drF(k)*vstar(i,j,k) |
1105 |
|
|
ENDDO |
1106 |
|
|
ENDDO |
1107 |
|
|
DO k=Nr-1,1,-1 |
1108 |
|
|
DO j=1-Oly,sNy+Oly |
1109 |
|
|
DO i=1-Olx,sNx+Olx |
1110 |
|
|
psistar(i,j,k) = psistar(i,j,k+1) |
1111 |
|
|
& - hfacS(i,j,k,bi,bj)*drF(k)*vstar(i,j,k) |
1112 |
|
|
ENDDO |
1113 |
|
|
ENDDO |
1114 |
|
|
ENDDO |
1115 |
jmc |
1.20 |
|
1116 |
m_bates |
1.1 |
#else |
1117 |
|
|
|
1118 |
|
|
IF (GM_AdvForm) THEN |
1119 |
|
|
k=Nr |
1120 |
|
|
DO j=1-Oly+1,sNy+1 |
1121 |
|
|
DO i=1-Olx+1,sNx+1 |
1122 |
|
|
GM_PsiX(i,j,k,bi,bj) = -hfacW(i,j,k,bi,bj)*drF(k)*ustar(i,j,k) |
1123 |
|
|
GM_PsiY(i,j,k,bi,bj) = -hfacS(i,j,k,bi,bj)*drF(k)*vstar(i,j,k) |
1124 |
|
|
ENDDO |
1125 |
|
|
ENDDO |
1126 |
|
|
DO k=Nr-1,1,-1 |
1127 |
|
|
DO j=1-Oly+1,sNy+1 |
1128 |
|
|
DO i=1-Olx+1,sNx+1 |
1129 |
|
|
GM_PsiX(i,j,k,bi,bj) = GM_PsiX(i,j,k+1,bi,bj) |
1130 |
|
|
& - hfacW(i,j,k,bi,bj)*drF(k)*ustar(i,j,k) |
1131 |
|
|
GM_PsiY(i,j,k,bi,bj) = GM_PsiY(i,j,k+1,bi,bj) |
1132 |
|
|
& - hfacS(i,j,k,bi,bj)*drF(k)*vstar(i,j,k) |
1133 |
|
|
ENDDO |
1134 |
|
|
ENDDO |
1135 |
|
|
ENDDO |
1136 |
|
|
|
1137 |
|
|
ENDIF |
1138 |
|
|
#endif |
1139 |
|
|
|
1140 |
|
|
#ifdef ALLOW_DIAGNOSTICS |
1141 |
|
|
C Diagnostics |
1142 |
|
|
IF ( useDiagnostics ) THEN |
1143 |
jmc |
1.20 |
CALL DIAGNOSTICS_FILL(K3D, 'GM_K3D ',0,Nr,1,bi,bj,myThid) |
1144 |
|
|
CALL DIAGNOSTICS_FILL(KPV, 'GM_KPV ',0,Nr,2,bi,bj,myThid) |
1145 |
|
|
CALL DIAGNOSTICS_FILL(urms, 'GM_URMS ',0,Nr,2,bi,bj,myThid) |
1146 |
|
|
CALL DIAGNOSTICS_FILL(Rdef, 'GM_RDEF ',0, 1,1,bi,bj,myThid) |
1147 |
|
|
CALL DIAGNOSTICS_FILL(Rurms, 'GM_RURMS',0, 1,2,bi,bj,myThid) |
1148 |
|
|
CALL DIAGNOSTICS_FILL(RRhines,'GM_RRHNS',0, 1,2,bi,bj,myThid) |
1149 |
|
|
CALL DIAGNOSTICS_FILL(Rmix, 'GM_RMIX ',0, 1,2,bi,bj,myThid) |
1150 |
|
|
CALL DIAGNOSTICS_FILL(supp, 'GM_SUPP ',0,Nr,2,bi,bj,myThid) |
1151 |
|
|
CALL DIAGNOSTICS_FILL(Xix, 'GM_Xix ',0,Nr,2,bi,bj,myThid) |
1152 |
|
|
CALL DIAGNOSTICS_FILL(Xiy, 'GM_Xiy ',0,Nr,2,bi,bj,myThid) |
1153 |
|
|
CALL DIAGNOSTICS_FILL(cDopp, 'GM_C ',0, 1,2,bi,bj,myThid) |
1154 |
|
|
CALL DIAGNOSTICS_FILL(Ubaro, 'GM_UBARO',0, 1,2,bi,bj,myThid) |
1155 |
|
|
CALL DIAGNOSTICS_FILL(eady, 'GM_EADY ',0, 1,2,bi,bj,myThid) |
1156 |
|
|
CALL DIAGNOSTICS_FILL(SlopeX, 'GM_Sx ',0,Nr,2,bi,bj,myThid) |
1157 |
|
|
CALL DIAGNOSTICS_FILL(SlopeY, 'GM_Sy ',0,Nr,2,bi,bj,myThid) |
1158 |
|
|
CALL DIAGNOSTICS_FILL(tfluxX, 'GM_TFLXX',0,Nr,2,bi,bj,myThid) |
1159 |
|
|
CALL DIAGNOSTICS_FILL(tfluxY, 'GM_TFLXY',0,Nr,2,bi,bj,myThid) |
1160 |
|
|
CALL DIAGNOSTICS_FILL(gradqx, 'GM_dqdx ',0,Nr,2,bi,bj,myThid) |
1161 |
|
|
CALL DIAGNOSTICS_FILL(gradqy, 'GM_dqdy ',0,Nr,2,bi,bj,myThid) |
1162 |
|
|
CALL DIAGNOSTICS_FILL(Kdqdy, 'GM_Kdqdy',0,Nr,2,bi,bj,myThid) |
1163 |
|
|
CALL DIAGNOSTICS_FILL(Kdqdx, 'GM_Kdqdx',0,Nr,2,bi,bj,myThid) |
1164 |
|
|
CALL DIAGNOSTICS_FILL(surfkz, 'GM_SFLYR',0, 1,2,bi,bj,myThid) |
1165 |
|
|
CALL DIAGNOSTICS_FILL(ustar, 'GM_USTAR',0,Nr,2,bi,bj,myThid) |
1166 |
|
|
CALL DIAGNOSTICS_FILL(vstar, 'GM_VSTAR',0,Nr,2,bi,bj,myThid) |
1167 |
|
|
CALL DIAGNOSTICS_FILL(umc, 'GM_UMC ',0,Nr,2,bi,bj,myThid) |
1168 |
|
|
CALL DIAGNOSTICS_FILL(ubar, 'GM_UBAR ',0,Nr,2,bi,bj,myThid) |
1169 |
|
|
CALL DIAGNOSTICS_FILL(modesC, 'GM_MODEC',0,Nr,1,bi,bj,myThid) |
1170 |
|
|
CALL DIAGNOSTICS_FILL(M4loc, 'GM_M4 ',0,Nr,2,bi,bj,myThid) |
1171 |
|
|
CALL DIAGNOSTICS_FILL(N2loc, 'GM_N2 ',0,Nr,2,bi,bj,myThid) |
1172 |
|
|
CALL DIAGNOSTICS_FILL(M4onN2, 'GM_M4_N2',0,Nr,2,bi,bj,myThid) |
1173 |
|
|
CALL DIAGNOSTICS_FILL(slopeC, 'GM_SLOPE',0,Nr,2,bi,bj,myThid) |
1174 |
|
|
CALL DIAGNOSTICS_FILL(Renorm, 'GM_RENRM',0, 1,2,bi,bj,myThid) |
1175 |
m_bates |
1.1 |
ENDIF |
1176 |
|
|
#endif |
1177 |
|
|
|
1178 |
jmc |
1.20 |
C For the Redi diffusivity, we set K3D to a constant if |
1179 |
m_bates |
1.14 |
C GM_K3D_constRedi=.TRUE. |
1180 |
|
|
IF (GM_K3D_constRedi) THEN |
1181 |
m_bates |
1.11 |
DO k=1,Nr |
1182 |
|
|
DO j=1-Oly,sNy+Oly |
1183 |
|
|
DO i=1-Olx,sNx+Olx |
1184 |
|
|
K3D(i,j,k,bi,bj) = GM_K3D_constK |
1185 |
|
|
ENDDO |
1186 |
|
|
ENDDO |
1187 |
|
|
ENDDO |
1188 |
|
|
ENDIF |
1189 |
|
|
|
1190 |
m_bates |
1.14 |
#ifdef ALLOW_DIAGNOSTICS |
1191 |
jmc |
1.20 |
IF ( useDiagnostics ) |
1192 |
|
|
& CALL DIAGNOSTICS_FILL(K3D, 'GM_K3D_T',0,Nr,1,bi,bj,myThid) |
1193 |
m_bates |
1.14 |
#endif |
1194 |
|
|
|
1195 |
m_bates |
1.1 |
#endif /* GM_K3D */ |
1196 |
|
|
RETURN |
1197 |
|
|
END |