1 |
m_bates |
1.14 |
C $Header: /u/gcmpack/MITgcm/pkg/gmredi/gmredi_k3d.F,v 1.13 2013/10/21 18:46:05 m_bates Exp $ |
2 |
m_bates |
1.1 |
C $Name: $ |
3 |
m_bates |
1.9 |
#include "CPP_OPTIONS.h" |
4 |
m_bates |
1.1 |
#include "GMREDI_OPTIONS.h" |
5 |
|
|
|
6 |
|
|
C !ROUTINE: GMREDI_K3D |
7 |
|
|
C !INTERFACE: |
8 |
|
|
SUBROUTINE GMREDI_K3D( |
9 |
|
|
I iMin, iMax, jMin, jMax, |
10 |
|
|
I sigmaX, sigmaY, sigmaR, |
11 |
m_bates |
1.4 |
I bi, bj, myTime, myThid ) |
12 |
m_bates |
1.1 |
|
13 |
|
|
C !DESCRIPTION: \bv |
14 |
|
|
C *==========================================================* |
15 |
|
|
C | SUBROUTINE GMREDI_K3D |
16 |
|
|
C | o Calculates the 3D diffusivity as per Bates et al. (2013) |
17 |
|
|
C *==========================================================* |
18 |
|
|
C \ev |
19 |
|
|
|
20 |
|
|
IMPLICIT NONE |
21 |
|
|
|
22 |
|
|
C == Global variables == |
23 |
|
|
#include "SIZE.h" |
24 |
|
|
#include "GRID.h" |
25 |
|
|
#include "DYNVARS.h" |
26 |
|
|
#include "EEPARAMS.h" |
27 |
|
|
#include "PARAMS.h" |
28 |
|
|
#include "GMREDI.h" |
29 |
|
|
|
30 |
|
|
C !INPUT/OUTPUT PARAMETERS: |
31 |
|
|
C == Routine arguments == |
32 |
|
|
C bi, bj :: tile indices |
33 |
|
|
C myThid :: My Thread Id. number |
34 |
|
|
|
35 |
|
|
INTEGER iMin,iMax,jMin,jMax |
36 |
|
|
_RL sigmaX(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
37 |
|
|
_RL sigmaY(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
38 |
|
|
_RL sigmaR(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
39 |
|
|
INTEGER bi, bj |
40 |
m_bates |
1.4 |
_RL myTime |
41 |
m_bates |
1.1 |
INTEGER myThid |
42 |
|
|
|
43 |
|
|
#ifdef GM_K3D |
44 |
|
|
|
45 |
m_bates |
1.4 |
C === Functions ==== |
46 |
|
|
LOGICAL DIFFERENT_MULTIPLE |
47 |
|
|
EXTERNAL DIFFERENT_MULTIPLE |
48 |
|
|
|
49 |
m_bates |
1.1 |
C !LOCAL VARIABLES: |
50 |
|
|
C == Local variables == |
51 |
m_bates |
1.4 |
INTEGER i,j,k,kk,m |
52 |
|
|
|
53 |
|
|
C update_modes :: Whether to update the eigenmodes |
54 |
|
|
LOGICAL update_modes |
55 |
|
|
|
56 |
|
|
C surfk :: index of the depth of the surface layer |
57 |
|
|
C kLow_C :: Local version of the index of deepest wet grid cell on tracer grid |
58 |
|
|
C kLow_U :: Local version of the index of deepest wet grid cell on U grid |
59 |
|
|
C kLow_V :: Local version of the index of deepest wet grid cell on V grid |
60 |
m_bates |
1.1 |
INTEGER surfk(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
61 |
|
|
INTEGER kLow_C(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
62 |
|
|
INTEGER kLow_U(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
63 |
|
|
INTEGER kLow_V(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
64 |
m_bates |
1.4 |
|
65 |
|
|
C N2loc :: local N**2 |
66 |
|
|
C slope :: local slope |
67 |
|
|
C Req :: local equatorial deformation radius (m) |
68 |
|
|
C deltaH :: local thickness of Eady integration (m) |
69 |
|
|
C g_reciprho_sq :: (gravity*recip_rhoConst)**2 |
70 |
|
|
C M4loc :: local M**4 |
71 |
|
|
C maxDRhoDz :: maximum value of d(rho)/dz (derived from GM_K3D_minN2) |
72 |
|
|
C sigx :: local d(rho)/dx |
73 |
|
|
C sigy :: local d(rho)/dy |
74 |
|
|
C sigz :: local d(rho)/dz |
75 |
|
|
C hsurf :: local surface layer depth |
76 |
|
|
C small :: a small number (to avoid floating point exceptions) |
77 |
m_bates |
1.10 |
_RL N2loc(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
78 |
m_bates |
1.1 |
_RL slope |
79 |
m_bates |
1.10 |
_RL slopeC(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
80 |
m_bates |
1.4 |
_RL Req |
81 |
m_bates |
1.10 |
_RL deltaH(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
82 |
m_bates |
1.1 |
_RL g_reciprho_sq |
83 |
m_bates |
1.10 |
_RL M4loc(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
84 |
m_bates |
1.13 |
_RL M4onN2(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
85 |
m_bates |
1.1 |
_RL maxDRhoDz |
86 |
|
|
_RL sigx, sigy, sigz |
87 |
|
|
_RL hsurf |
88 |
|
|
_RL small |
89 |
m_bates |
1.4 |
|
90 |
|
|
C dfdy :: gradient of the Coriolis paramter, df/dy, 1/(m*s) |
91 |
|
|
C dfdx :: gradient of the Coriolis paramter, df/dx, 1/(m*s) |
92 |
m_bates |
1.6 |
C gradf :: gradient of the Coriolis paramter at a cell centre, 1/(m*s) |
93 |
m_bates |
1.8 |
C Rurms :: a local mixing length used in calculation of urms (m) |
94 |
m_bates |
1.4 |
C RRhines :: The Rhines scale (m) |
95 |
|
|
C Rmix :: Mixing length |
96 |
|
|
C N2 :: Square of the buoyancy frequency (1/s**2) |
97 |
|
|
C N2W :: Square of the buoyancy frequency (1/s**2) averaged to west of grid cell |
98 |
|
|
C N2S :: Square of the buoyancy frequency (1/s**2) averaged to south of grid cell |
99 |
|
|
C N :: Buoyancy frequency, SQRT(N2) |
100 |
|
|
C BVint :: The vertical integral of N (m/s) |
101 |
|
|
C ubar :: Zonal velocity on a tracer point (m/s) |
102 |
|
|
C vbar :: Meridional velocity on a tracer point (m/s) |
103 |
|
|
C Ubaro :: Barotropic velocity (m/s) |
104 |
|
|
_RL dfdy( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
105 |
|
|
_RL dfdx( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
106 |
|
|
_RL gradf( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
107 |
|
|
_RL dummy( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
108 |
m_bates |
1.8 |
_RL Rurms( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
109 |
m_bates |
1.4 |
_RL RRhines(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
110 |
|
|
_RL Rmix( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
111 |
|
|
_RL N2( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
112 |
|
|
_RL N2W( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
113 |
|
|
_RL N2S( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
114 |
|
|
_RL N( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
115 |
|
|
_RL BVint( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
116 |
|
|
_RL Ubaro( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
117 |
|
|
_RL ubar( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr,nSx,nSy) |
118 |
|
|
_RL vbar( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr,nSx,nSy) |
119 |
|
|
|
120 |
|
|
C Rmid :: Rossby radius (m) |
121 |
|
|
C KPV :: Diffusivity (m**2/s) |
122 |
m_bates |
1.13 |
C Kdqdx :: diffusivity multiplied by zonal PV gradient |
123 |
|
|
C Kdqdy :: diffusivity multiplied by meridional PV gradient |
124 |
m_bates |
1.4 |
C SlopeX :: isopycnal slope in x direction |
125 |
|
|
C SlopeY :: isopycnal slope in y direction |
126 |
|
|
C dSigmaDx :: sigmaX averaged onto tracer grid |
127 |
|
|
C dSigmaDy :: sigmaY averaged onto tracer grid |
128 |
|
|
C tfluxX :: thickness flux in x direction |
129 |
|
|
C tfluxY :: thickness flux in y direction |
130 |
|
|
C fCoriU :: Coriolis parameter averaged to U points |
131 |
|
|
C fCoriV :: Coriolis parameter averaged to V points |
132 |
|
|
C cori :: Coriolis parameter forced to be finite near the equator |
133 |
|
|
C coriU :: As for cori, but, at U point |
134 |
|
|
C coriV :: As for cori, but, at V point |
135 |
|
|
C surfkz :: Depth of surface layer (in r units) |
136 |
|
|
_RL Rmid(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
137 |
m_bates |
1.3 |
_RL KPV(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
138 |
m_bates |
1.13 |
_RL Kdqdy(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
139 |
|
|
_RL Kdqdx(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
140 |
m_bates |
1.1 |
_RL SlopeX(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
141 |
|
|
_RL SlopeY(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
142 |
|
|
_RL dSigmaDx(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
143 |
|
|
_RL dSigmaDy(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
144 |
|
|
_RL tfluxX(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
145 |
|
|
_RL tfluxY(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
146 |
|
|
_RL cori(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
147 |
|
|
_RL coriU(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
148 |
|
|
_RL coriV(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
149 |
|
|
_RL fCoriU(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
150 |
|
|
_RL fCoriV(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
151 |
|
|
_RL surfkz(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
152 |
m_bates |
1.4 |
|
153 |
|
|
C gradqx :: Potential vorticity gradient in x direction |
154 |
|
|
C gradqy :: Potential vorticity gradient in y direction |
155 |
|
|
C XimX :: Vertical integral of phi_m*K*gradqx |
156 |
|
|
C XimY :: Vertical integral of phi_m*K*gradqy |
157 |
|
|
C cDopp :: Quasi-Doppler shifted long Rossby wave speed (m/s) |
158 |
|
|
C umc :: ubar-c (m/s) |
159 |
|
|
C eady :: Eady growth rate (1/s) |
160 |
|
|
C urms :: the rms eddy velocity (m/s) |
161 |
|
|
C supp :: The suppression factor |
162 |
|
|
C ustar :: The eddy induced velocity in the x direction |
163 |
|
|
C vstar :: The eddy induced velocity in the y direction |
164 |
|
|
C Xix :: Xi in the x direction (m/s**2) |
165 |
|
|
C Xiy :: Xi in the y direction (m/s**2) |
166 |
m_bates |
1.1 |
_RL gradqx(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
167 |
|
|
_RL gradqy(1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
168 |
|
|
_RL XimX(GM_K3D_NModes,1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
169 |
|
|
_RL XimY(GM_K3D_NModes,1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
170 |
m_bates |
1.4 |
_RL cDopp(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
171 |
m_bates |
1.1 |
_RL umc( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
172 |
|
|
_RL eady( 1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
173 |
|
|
_RL urms( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
174 |
|
|
_RL supp( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
175 |
|
|
_RL ustar(1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
176 |
|
|
_RL vstar(1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
177 |
|
|
_RL Xix( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
178 |
|
|
_RL Xiy( 1-Olx:sNx+Olx,1-Oly:sNy+Oly,Nr) |
179 |
m_bates |
1.4 |
#ifdef GM_K3D_PASSIVE |
180 |
|
|
C psistar :: eddy induced streamfunction in the y direction |
181 |
m_bates |
1.1 |
_RL psistar(1-Olx:sNx+Olx,1-Oly:sNy+Oly,1:Nr) |
182 |
m_bates |
1.4 |
#endif |
183 |
m_bates |
1.1 |
|
184 |
|
|
|
185 |
|
|
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
186 |
|
|
|
187 |
|
|
C ====================================== |
188 |
|
|
C Initialise some variables |
189 |
|
|
C ====================================== |
190 |
|
|
small = TINY(zeroRL) |
191 |
m_bates |
1.4 |
update_modes=.FALSE. |
192 |
|
|
IF ( DIFFERENT_MULTIPLE(GM_K3D_vecFreq,myTime,deltaTClock) ) |
193 |
|
|
& update_modes=.TRUE. |
194 |
|
|
|
195 |
m_bates |
1.1 |
DO j=1-Oly,sNy+Oly |
196 |
|
|
DO i=1-Olx,sNx+Olx |
197 |
|
|
kLow_C(i,j) = kLowC(i,j,bi,bj) |
198 |
|
|
ENDDO |
199 |
|
|
ENDDO |
200 |
|
|
DO j=1-Oly,sNy+Oly |
201 |
|
|
DO i=1-Olx+1,sNx+Olx |
202 |
|
|
kLow_U(i,j) = MIN( kLow_C(i,j), kLow_C(i-1,j) ) |
203 |
|
|
ENDDO |
204 |
|
|
ENDDO |
205 |
|
|
DO j=1-Oly+1,sNy+Oly |
206 |
|
|
DO i=1-Olx,sNx+Olx |
207 |
|
|
kLow_V(i,j) = MIN( kLow_C(i,j), kLow_C(i,j-1) ) |
208 |
|
|
ENDDO |
209 |
|
|
ENDDO |
210 |
|
|
|
211 |
|
|
C Dummy values for the edges |
212 |
|
|
C This avoids weirdness in gmredi_calc_eigs |
213 |
|
|
i=1-Olx |
214 |
|
|
DO j=1-Oly,sNy+Oly |
215 |
|
|
kLow_U(i,j) = kLow_C(i,j) |
216 |
|
|
ENDDO |
217 |
|
|
j=1-Oly |
218 |
|
|
DO i=1-Olx,sNx+Olx |
219 |
|
|
kLow_V(i,j) = kLow_C(i,j) |
220 |
|
|
ENDDO |
221 |
|
|
|
222 |
|
|
g_reciprho_sq = (gravity*recip_rhoConst)**2 |
223 |
|
|
C Gradient of Coriolis |
224 |
|
|
DO j=1-Oly+1,sNy+Oly |
225 |
|
|
DO i=1-Olx+1,sNx+Olx |
226 |
|
|
dfdx(i,j) = ( fCori(i,j,bi,bj)-fCori(i-1,j,bi,bj) ) |
227 |
|
|
& *recip_dxC(i,j,bi,bj) |
228 |
|
|
dfdy(i,j) = ( fCori(i,j,bi,bj)-fCori(i,j-1,bi,bj) ) |
229 |
|
|
& *recip_dyC(i,j,bi,bj) |
230 |
|
|
ENDDO |
231 |
|
|
ENDDO |
232 |
|
|
|
233 |
|
|
C Coriolis at C points enforcing a minimum value so |
234 |
|
|
C that it is defined at the equator |
235 |
|
|
DO j=1-Oly,sNy+Oly |
236 |
|
|
DO i=1-Olx,sNx+Olx |
237 |
|
|
cori(i,j) = SIGN( MAX( ABS(fCori(i,j,bi,bj)),GM_K3D_minCori ), |
238 |
|
|
& fCori(i,j,bi,bj) ) |
239 |
|
|
ENDDO |
240 |
|
|
ENDDO |
241 |
|
|
C Coriolis at U and V points |
242 |
|
|
DO j=1-Oly+1,sNy+Oly |
243 |
|
|
DO i=1-Olx+1,sNx+Olx |
244 |
|
|
C Limited so that the inverse is defined at the equator |
245 |
|
|
coriU(i,j) = op5*( cori(i,j)+cori(i-1,j) ) |
246 |
|
|
coriU(i,j) = SIGN( MAX( ABS(coriU(i,j)),GM_K3D_minCori ), |
247 |
|
|
& coriU(i,j) ) |
248 |
|
|
|
249 |
|
|
coriV(i,j) = op5*( cori(i,j)+cori(i,j-1) ) |
250 |
|
|
coriV(i,j) = SIGN( MAX( ABS(coriV(i,j)),GM_K3D_minCori ), |
251 |
|
|
& coriV(i,j) ) |
252 |
|
|
|
253 |
|
|
C Not limited |
254 |
|
|
fCoriU(i,j) = op5*( fCori(i,j,bi,bj)+fCori(i-1,j,bi,bj) ) |
255 |
|
|
fCoriV(i,j) = op5*( fCori(i,j,bi,bj)+fCori(i,j-1,bi,bj) ) |
256 |
|
|
ENDDO |
257 |
|
|
ENDDO |
258 |
|
|
DO j=1-Oly,sNy+Oly |
259 |
|
|
DO i=1-Olx,sNx+Olx |
260 |
m_bates |
1.6 |
gradf(i,j) = recip_rSphere*fCoriCos(i,j,bi,bj) |
261 |
m_bates |
1.1 |
ENDDO |
262 |
|
|
ENDDO |
263 |
|
|
|
264 |
|
|
C Zeroing some cumulative fields |
265 |
|
|
DO j=1-Oly,sNy+Oly |
266 |
|
|
DO i=1-Olx,sNx+Olx |
267 |
m_bates |
1.10 |
eady(i,j) = zeroRL |
268 |
|
|
BVint(i,j) = zeroRL |
269 |
|
|
Ubaro(i,j) = zeroRL |
270 |
|
|
deltaH(i,j) = zeroRL |
271 |
|
|
ENDDO |
272 |
|
|
ENDDO |
273 |
|
|
DO k=1,Nr |
274 |
|
|
DO j=1-Oly,sNy+Oly |
275 |
|
|
DO i=1-Olx,sNx+Olx |
276 |
|
|
slopeC(i,j,k)=zeroRL |
277 |
|
|
ENDDO |
278 |
m_bates |
1.1 |
ENDDO |
279 |
|
|
ENDDO |
280 |
|
|
|
281 |
|
|
C Find the zonal velocity at the cell centre |
282 |
|
|
C The logicals here are, in order: 1/ go from grid to north/east directions |
283 |
|
|
C 2/ go from C to A grid and 3/ apply the mask |
284 |
m_bates |
1.9 |
#ifdef ALLOW_EDDYPSI |
285 |
|
|
IF (GM_InMomAsStress) THEN |
286 |
|
|
CALL rotate_uv2en_rl(uMean, vMean, ubar, vbar, .TRUE., .TRUE., |
287 |
|
|
& .TRUE.,Nr,mythid) |
288 |
|
|
ELSE |
289 |
|
|
#endif |
290 |
|
|
CALL rotate_uv2en_rl(uVel, vVel, ubar, vbar, .TRUE., .TRUE., |
291 |
|
|
& .TRUE.,Nr,mythid) |
292 |
|
|
#ifdef ALLOW_EDDYPSI |
293 |
|
|
ENDIF |
294 |
|
|
#endif |
295 |
m_bates |
1.1 |
|
296 |
|
|
C Square of the buoyancy frequency at the top of a grid cell |
297 |
|
|
DO k=2,Nr |
298 |
|
|
DO j=1-Oly,sNy+Oly |
299 |
|
|
DO i=1-Olx,sNx+Olx |
300 |
|
|
N2(i,j,k) = -gravity*recip_rhoConst*sigmaR(i,j,k) |
301 |
|
|
ENDDO |
302 |
|
|
ENDDO |
303 |
|
|
ENDDO |
304 |
|
|
C N2(k=1) is always zero |
305 |
|
|
k=1 |
306 |
|
|
DO j=1-Oly,sNy+Oly |
307 |
|
|
DO i=1-Olx,sNx+Olx |
308 |
|
|
N2(i,j,k) = 0.0 |
309 |
|
|
N(i,j,k) = 0.0 |
310 |
|
|
ENDDO |
311 |
|
|
ENDDO |
312 |
|
|
C Enforce a minimum N2 |
313 |
|
|
DO k=2,Nr |
314 |
|
|
DO j=1-Oly,sNy+Oly |
315 |
|
|
DO i=1-Olx,sNx+Olx |
316 |
|
|
IF (N2(i,j,k).LT.GM_K3D_minN2) N2(i,j,k)=GM_K3D_minN2 |
317 |
|
|
N(i,j,k) = SQRT(N2(i,j,k)) |
318 |
|
|
ENDDO |
319 |
|
|
ENDDO |
320 |
|
|
ENDDO |
321 |
|
|
C Calculate the minimum drho/dz |
322 |
|
|
maxDRhoDz = -rhoConst*GM_K3D_minN2/gravity |
323 |
|
|
|
324 |
|
|
C Calculate the barotropic velocity by vertically integrating |
325 |
|
|
C and the dividing by the depth of the water column |
326 |
|
|
C Note that Ubaro is on the U grid. |
327 |
|
|
DO k=1,Nr |
328 |
|
|
DO j=1-Oly,sNy+Oly |
329 |
|
|
DO i=1-Olx,sNx+Olx |
330 |
|
|
Ubaro(i,j) = Ubaro(i,j) + |
331 |
|
|
& maskW(i,j,k,bi,bj)*drF(k)*hfacC(i,j,k,bi,bj) |
332 |
|
|
& *ubar(i,j,k,bi,bj) |
333 |
|
|
ENDDO |
334 |
|
|
ENDDO |
335 |
|
|
ENDDO |
336 |
|
|
DO j=1-Oly,sNy+Oly |
337 |
|
|
DO i=1-Olx,sNx+Olx |
338 |
|
|
IF (kLow_C(i,j).GT.0) THEN |
339 |
|
|
C The minus sign is because r_Low<0 |
340 |
|
|
Ubaro(i,j) = -Ubaro(i,j)/r_Low(i,j,bi,bj) |
341 |
|
|
ENDIF |
342 |
|
|
ENDDO |
343 |
|
|
ENDDO |
344 |
|
|
|
345 |
|
|
C Integrate the buoyancy frequency vertically using the trapezoidal method. |
346 |
|
|
DO k=1,Nr |
347 |
|
|
DO j=1-Oly,sNy+Oly |
348 |
|
|
DO i=1-Olx,sNx+Olx |
349 |
|
|
IF (k.LT.kLow_C(i,j)) THEN |
350 |
|
|
BVint(i,j) = BVint(i,j) + hFacC(i,j,k,bi,bj)*drF(k) |
351 |
|
|
& *(N(i,j,k)+N(i,j,k+1)) |
352 |
|
|
ELSEIF (k.EQ.kLow_C(i,j)) THEN |
353 |
|
|
C Assume that N(z=-H)=0 |
354 |
|
|
BVint(i,j) = BVint(i,j) + hFacC(i,j,k,bi,bj)*drF(k)*N(i,j,k) |
355 |
|
|
ENDIF |
356 |
|
|
ENDDO |
357 |
|
|
ENDDO |
358 |
|
|
ENDDO |
359 |
|
|
DO j=1-Oly,sNy+Oly |
360 |
|
|
DO i=1-Olx,sNx+Olx |
361 |
|
|
BVint(i,j) = op5*BVint(i,j) |
362 |
|
|
ENDDO |
363 |
|
|
ENDDO |
364 |
|
|
|
365 |
|
|
C Calculate the eigenvalues and eigenvectors |
366 |
m_bates |
1.4 |
IF (update_modes) THEN |
367 |
|
|
CALL GMREDI_CALC_EIGS( |
368 |
|
|
I iMin,iMax,jMin,jMax,bi,bj,N2,myThid, |
369 |
|
|
I kLow_C, maskC(:,:,:,bi,bj), |
370 |
|
|
I hfacC(:,:,:,bi,bj), recip_hfacC(:,:,:,bi,bj), |
371 |
|
|
I R_Low(:,:,bi,bj), 1, .TRUE., |
372 |
|
|
O Rmid, modesC(:,:,:,:,bi,bj)) |
373 |
|
|
|
374 |
|
|
C Calculate the Rossby Radius |
375 |
|
|
DO j=1-Oly+1,sNy+Oly |
376 |
|
|
DO i=1-Olx+1,sNx+Olx |
377 |
|
|
Req = SQRT(BVint(i,j)/(2*pi*gradf(i,j))) |
378 |
|
|
Rdef(i,j,bi,bj) = MIN(Rmid(i,j),Req) |
379 |
|
|
ENDDO |
380 |
|
|
ENDDO |
381 |
|
|
ENDIF |
382 |
m_bates |
1.1 |
|
383 |
|
|
C Average dsigma/dx and dsigma/dy onto the centre points |
384 |
|
|
|
385 |
|
|
DO k=1,Nr |
386 |
|
|
DO j=1-Oly,sNy+Oly-1 |
387 |
|
|
DO i=1-Olx,sNx+Olx-1 |
388 |
|
|
dSigmaDx(i,j,k) = op5*(sigmaX(i,j,k)+sigmaX(i+1,j,k)) |
389 |
|
|
dSigmaDy(i,j,k) = op5*(sigmaY(i,j,k)+sigmaY(i,j+1,k)) |
390 |
|
|
ENDDO |
391 |
|
|
ENDDO |
392 |
|
|
ENDDO |
393 |
|
|
|
394 |
|
|
C =============================== |
395 |
|
|
C Calculate the Eady growth rate |
396 |
|
|
C =============================== |
397 |
|
|
DO k=1,Nr |
398 |
|
|
|
399 |
m_bates |
1.10 |
DO j=1-Oly,sNy+Oly-1 |
400 |
|
|
DO i=1-Olx,sNx+Olx-1 |
401 |
|
|
M4loc(i,j,k) = g_reciprho_sq*( dSigmaDx(i,j,k)**2 |
402 |
|
|
& +dSigmaDy(i,j,k)**2 ) |
403 |
|
|
IF (k.NE.kLow_C(i,j)) THEN |
404 |
|
|
N2loc(i,j,k) = op5*(N2(i,j,k)+N2(i,j,k+1)) |
405 |
|
|
ELSE |
406 |
|
|
N2loc(i,j,k) = op5*N2(i,j,k) |
407 |
|
|
ENDIF |
408 |
|
|
ENDDO |
409 |
|
|
ENDDO |
410 |
m_bates |
1.1 |
C The bottom of the grid cell is shallower than the top |
411 |
|
|
C integration level, so, advance the depth. |
412 |
m_bates |
1.10 |
IF (-rF(k+1) .LE. GM_K3D_EadyMinDepth) CYCLE |
413 |
m_bates |
1.1 |
|
414 |
jmc |
1.7 |
C Do not bother going any deeper since the top of the |
415 |
m_bates |
1.1 |
C cell is deeper than the bottom integration level |
416 |
|
|
IF (-rF(k).GE.GM_K3D_EadyMaxDepth) EXIT |
417 |
|
|
|
418 |
|
|
C We are in the integration depth range |
419 |
|
|
DO j=1-Oly,sNy+Oly-1 |
420 |
|
|
DO i=1-Olx,sNx+Olx-1 |
421 |
m_bates |
1.10 |
IF ( (kLow_C(i,j).GE.k) .AND. |
422 |
|
|
& (-hMixLayer(i,j,bi,bj).LE.-rC(k)) ) THEN |
423 |
m_bates |
1.1 |
|
424 |
m_bates |
1.12 |
slopeC(i,j,k) = SQRT(M4loc(i,j,k))/N2loc(i,j,k) |
425 |
m_bates |
1.1 |
C Limit the slope. Note, this is not all the Eady calculations. |
426 |
m_bates |
1.13 |
IF (slopeC(i,j,k).LE.GM_maxSlope) THEN |
427 |
|
|
M4onN2(i,j,k) = M4loc(i,j,k)/N2loc(i,j,k) |
428 |
m_bates |
1.1 |
ELSE |
429 |
m_bates |
1.13 |
slopeC(i,j,k) = GM_maxslope |
430 |
|
|
M4onN2(i,j,k) = SQRT(M4loc(i,j,k))*GM_maxslope |
431 |
m_bates |
1.1 |
ENDIF |
432 |
m_bates |
1.13 |
eady(i,j) = eady(i,j) |
433 |
|
|
& + hfacC(i,j,k,bi,bj)*drF(k)*M4onN2(i,j,k) |
434 |
m_bates |
1.10 |
deltaH(i,j) = deltaH(i,j) + drF(k) |
435 |
m_bates |
1.1 |
ENDIF |
436 |
|
|
ENDDO |
437 |
|
|
ENDDO |
438 |
|
|
ENDDO |
439 |
|
|
|
440 |
|
|
DO j=1-Oly,sNy+Oly |
441 |
|
|
DO i=1-Olx,sNx+Olx |
442 |
m_bates |
1.10 |
C If the minimum depth for the integration is deeper than the ocean |
443 |
|
|
C bottom OR the mixed layer is deeper than the maximum depth of |
444 |
|
|
C integration, we set the Eady growth rate to something small |
445 |
|
|
C to avoid floating point exceptions. |
446 |
|
|
C Later, these areas will be given a small diffusivity. |
447 |
|
|
IF (deltaH(i,j).EQ.zeroRL) THEN |
448 |
m_bates |
1.1 |
eady(i,j) = small |
449 |
|
|
|
450 |
m_bates |
1.10 |
C Otherwise, divide over the integration and take the square root |
451 |
|
|
C to actually find the Eady growth rate. |
452 |
m_bates |
1.1 |
ELSE |
453 |
m_bates |
1.10 |
eady(i,j) = SQRT(eady(i,j)/deltaH(i,j)) |
454 |
m_bates |
1.1 |
|
455 |
|
|
ENDIF |
456 |
|
|
|
457 |
|
|
ENDDO |
458 |
|
|
ENDDO |
459 |
|
|
|
460 |
|
|
C ====================================== |
461 |
|
|
C Calculate the diffusivity |
462 |
|
|
C ====================================== |
463 |
|
|
DO j=1-Oly+1,sNy+Oly |
464 |
|
|
DO i=1-Olx+1,sNx+Olx-1 |
465 |
|
|
C Calculate the Visbeck velocity |
466 |
m_bates |
1.13 |
Rurms(i,j) = MIN(Rdef(i,j,bi,bj),GM_K3D_Rmax) |
467 |
m_bates |
1.8 |
urms(i,j,1) = GM_K3D_Lambda*eady(i,j)*Rurms(i,j) |
468 |
m_bates |
1.1 |
C Set the bottom urms to zero |
469 |
|
|
k=kLow_C(i,j) |
470 |
|
|
IF (k.GT.0) urms(i,j,k) = 0.0 |
471 |
|
|
|
472 |
|
|
C Calculate the Rhines scale |
473 |
|
|
RRhines(i,j) = SQRT(urms(i,j,1)/gradf(i,j)) |
474 |
|
|
|
475 |
|
|
C Calculate the estimated length scale |
476 |
m_bates |
1.4 |
Rmix(i,j) = MIN(Rdef(i,j,bi,bj), RRhines(i,j)) |
477 |
m_bates |
1.13 |
Rmix(i,j) = MAX(Rmix(i,j),GM_K3D_Rmin) |
478 |
m_bates |
1.1 |
|
479 |
|
|
C Calculate the Doppler shifted long Rossby wave speed |
480 |
|
|
C Ubaro is on the U grid so we must average onto the M grid. |
481 |
|
|
cDopp(i,j) = op5*( Ubaro(i,j)+Ubaro(i+1,j) ) |
482 |
m_bates |
1.4 |
& - gradf(i,j)*Rdef(i,j,bi,bj)*Rdef(i,j,bi,bj) |
483 |
m_bates |
1.1 |
C Limit the wave speed to the namelist variable GM_K3D_maxC |
484 |
|
|
IF (ABS(cDopp(i,j)).GT.GM_K3D_maxC) THEN |
485 |
|
|
cDopp(i,j) = MAX(GM_K3D_maxC, cDopp(i,j)) |
486 |
|
|
ENDIF |
487 |
|
|
|
488 |
|
|
ENDDO |
489 |
|
|
ENDDO |
490 |
|
|
|
491 |
|
|
C Project the surface urms to the subsurface using the first baroclinic mode |
492 |
m_bates |
1.4 |
CALL GMREDI_CALC_URMS( |
493 |
|
|
I iMin,iMax,jMin,jMax,bi,bj,N2,myThid, |
494 |
|
|
U urms) |
495 |
m_bates |
1.1 |
|
496 |
|
|
C Calculate the diffusivity (on the mass grid) |
497 |
|
|
DO k=1,Nr |
498 |
|
|
DO j=1-Oly,sNy+Oly |
499 |
|
|
DO i=1-Olx,sNx+Olx |
500 |
|
|
IF (k.LE.kLow_C(i,j)) THEN |
501 |
m_bates |
1.10 |
IF (deltaH(i,j).EQ.zeroRL) THEN |
502 |
m_bates |
1.1 |
K3D(i,j,k,bi,bj) = GM_K3D_smallK |
503 |
|
|
ELSE |
504 |
|
|
IF (urms(i,j,k).EQ.0.0) THEN |
505 |
|
|
K3D(i,j,k,bi,bj) = GM_K3D_smallK |
506 |
|
|
ELSE |
507 |
m_bates |
1.13 |
umc(i,j,k) =ubar(i,j,k,bi,bj) - cDopp(i,j) |
508 |
|
|
supp(i,j,k)=1/(1+GM_K3D_b1*umc(i,j,k)**2/urms(i,j,1)**2) |
509 |
|
|
C 2*Rmix gives the diameter |
510 |
m_bates |
1.1 |
K3D(i,j,k,bi,bj) = GM_K3D_gamma*urms(i,j,k) |
511 |
m_bates |
1.13 |
& *2*Rmix(i,j)*supp(i,j,k) |
512 |
m_bates |
1.1 |
ENDIF |
513 |
|
|
|
514 |
|
|
C Enforce lower and upper bounds on the diffusivity |
515 |
|
|
IF (K3D(i,j,k,bi,bj).LT.GM_K3D_smallK) |
516 |
|
|
& K3D(i,j,k,bi,bj) = GM_K3D_smallK |
517 |
|
|
IF (K3D(i,j,k,bi,bj).GT.GM_maxK3D) |
518 |
|
|
& K3D(i,j,k,bi,bj) = GM_maxK3D |
519 |
|
|
ENDIF |
520 |
|
|
ENDIF |
521 |
|
|
ENDDO |
522 |
|
|
ENDDO |
523 |
|
|
ENDDO |
524 |
|
|
|
525 |
|
|
C ====================================== |
526 |
|
|
C Find the PV gradient |
527 |
|
|
C ====================================== |
528 |
m_bates |
1.3 |
C Calculate the surface layer thickness. |
529 |
|
|
C Use hMixLayer (calculated in model/src/calc_oce_mxlayer) |
530 |
|
|
C for the mixed layer depth. |
531 |
m_bates |
1.1 |
|
532 |
m_bates |
1.3 |
C Enforce a minimum surface layer depth |
533 |
m_bates |
1.1 |
DO j=1-Oly,sNy+Oly |
534 |
|
|
DO i=1-Olx,sNx+Olx |
535 |
m_bates |
1.3 |
surfkz(i,j) = MIN(-GM_K3D_surfMinDepth,-hMixLayer(i,j,bi,bj)) |
536 |
|
|
surfkz(i,j) = MAX(surfkz(i,j),R_low(i,j,bi,bj)) |
537 |
|
|
IF(maskC(i,j,1,bi,bj).EQ.0.0) surfkz(i,j)=0.0 |
538 |
|
|
surfk(i,j) = 0 |
539 |
m_bates |
1.1 |
ENDDO |
540 |
|
|
ENDDO |
541 |
m_bates |
1.4 |
DO k=1,Nr |
542 |
m_bates |
1.1 |
DO j=1-Oly,sNy+Oly |
543 |
|
|
DO i=1-Olx,sNx+Olx |
544 |
m_bates |
1.3 |
IF (rF(k).GT.surfkz(i,j) .AND. surfkz(i,j).GE.rF(k+1)) |
545 |
|
|
& surfk(i,j) = k |
546 |
m_bates |
1.1 |
ENDDO |
547 |
|
|
ENDDO |
548 |
|
|
ENDDO |
549 |
m_bates |
1.3 |
|
550 |
m_bates |
1.1 |
C Calculate the isopycnal slope |
551 |
|
|
DO j=1-Oly,sNy+Oly-1 |
552 |
|
|
DO i=1-Olx,sNx+Olx-1 |
553 |
|
|
SlopeX(i,j,1) = zeroRL |
554 |
|
|
SlopeY(i,j,1) = zeroRL |
555 |
|
|
ENDDO |
556 |
|
|
ENDDO |
557 |
|
|
DO k=2,Nr |
558 |
|
|
DO j=1-Oly+1,sNy+Oly |
559 |
|
|
DO i=1-Olx+1,sNx+Olx |
560 |
|
|
IF(surfk(i,j).GE.kLowC(i,j,bi,bj)) THEN |
561 |
|
|
C If the surface layer is thinner than the water column |
562 |
|
|
C the set the slope to zero to avoid problems. |
563 |
|
|
SlopeX(i,j,k) = zeroRL |
564 |
|
|
SlopeY(i,j,k) = zeroRL |
565 |
|
|
|
566 |
|
|
ELSE |
567 |
|
|
C Calculate the zonal slope at the western cell face (U grid) |
568 |
m_bates |
1.4 |
sigz = MIN( op5*(sigmaR(i,j,k)+sigmaR(i-1,j,k)), maxDRhoDz ) |
569 |
m_bates |
1.1 |
sigx = op5*( sigmaX(i,j,k)+sigmaX(i,j,k-1) ) |
570 |
|
|
slope = sigx/sigz |
571 |
|
|
IF(ABS(slope).GT.GM_maxSlope) |
572 |
|
|
& slope = SIGN(GM_maxSlope,slope) |
573 |
|
|
SlopeX(i,j,k)=-maskW(i,j,k-1,bi,bj)*maskW(i,j,k,bi,bj)*slope |
574 |
|
|
|
575 |
|
|
C Calculate the meridional slope at the southern cell face (V grid) |
576 |
m_bates |
1.4 |
sigz = MIN( op5*(sigmaR(i,j,k)+sigmaR(i,j-1,k)), maxDRhoDz ) |
577 |
m_bates |
1.1 |
sigy = op5*( sigmaY(i,j,k) + sigmaY(i,j,k-1) ) |
578 |
|
|
slope = sigy/sigz |
579 |
|
|
IF(ABS(slope).GT.GM_maxSlope) |
580 |
|
|
& slope = SIGN(GM_maxSlope,slope) |
581 |
|
|
SlopeY(i,j,k)=-maskS(i,j,k-1,bi,bj)*maskS(i,j,k,bi,bj)*slope |
582 |
|
|
ENDIF |
583 |
|
|
ENDDO |
584 |
|
|
ENDDO |
585 |
|
|
ENDDO |
586 |
|
|
|
587 |
m_bates |
1.14 |
C Calculate the thickness flux and diffusivity. These may be altered later |
588 |
|
|
C depending on namelist options. |
589 |
m_bates |
1.1 |
C Enforce a zero slope bottom boundary condition for the bottom most cells (k=Nr) |
590 |
|
|
k=Nr |
591 |
|
|
DO j=1-Oly,sNy+Oly |
592 |
|
|
DO i=1-Olx,sNx+Olx |
593 |
|
|
C Zonal thickness flux at the western cell face |
594 |
|
|
tfluxX(i,j,k) = -fCoriU(i,j)*SlopeX(i,j,k) |
595 |
|
|
& *recip_drF(k)*recip_hFacW(i,j,k,bi,bj) |
596 |
|
|
C Meridional thickness flux at the southern cell face |
597 |
|
|
tfluxY(i,j,k) = -fCoriV(i,j)*SlopeY(i,j,k) |
598 |
|
|
& *recip_drF(k)*recip_hFacS(i,j,k,bi,bj) |
599 |
m_bates |
1.14 |
|
600 |
|
|
C Use the interior diffusivity. Note: if we are using a |
601 |
|
|
C constant diffusivity KPV is overwritten later |
602 |
|
|
KPV(i,j,k) = K3D(i,j,k,bi,bj) |
603 |
|
|
|
604 |
m_bates |
1.1 |
ENDDO |
605 |
|
|
ENDDO |
606 |
|
|
|
607 |
m_bates |
1.14 |
C Calculate the thickness flux and diffusivity and for other cells (k<Nr) |
608 |
m_bates |
1.1 |
DO k=Nr-1,1,-1 |
609 |
m_bates |
1.14 |
DO j=1-Oly,sNy+Oly |
610 |
|
|
DO i=1-Olx,sNx+Olx |
611 |
|
|
C Zonal thickness flux at the western cell face |
612 |
|
|
tfluxX(i,j,k)=-fCoriU(i,j)*(SlopeX(i,j,k)-SlopeX(i,j,k+1)) |
613 |
|
|
& *recip_drF(k)*recip_hFacW(i,j,k,bi,bj) |
614 |
|
|
& *maskW(i,j,k,bi,bj) |
615 |
|
|
|
616 |
|
|
C Meridional thickness flux at the southern cell face |
617 |
|
|
tfluxY(i,j,k)=-fCoriV(i,j)*(SlopeY(i,j,k)-SlopeY(i,j,k+1)) |
618 |
|
|
& *recip_drF(k)*recip_hFacS(i,j,k,bi,bj) |
619 |
|
|
& *maskS(i,j,k,bi,bj) |
620 |
|
|
|
621 |
|
|
C Use the interior diffusivity. Note: if we are using a |
622 |
|
|
C constant diffusivity KPV is overwritten later |
623 |
|
|
KPV(i,j,k) = K3D(i,j,k,bi,bj) |
624 |
|
|
ENDDO |
625 |
|
|
ENDDO |
626 |
|
|
ENDDO |
627 |
|
|
|
628 |
|
|
|
629 |
|
|
C Special treatment for the surface layer (if necessary), which overwrites |
630 |
|
|
C values in the previous loops. |
631 |
|
|
IF (GM_K3D_ThickSheet .OR. GM_K3D_surfK) THEN |
632 |
|
|
DO k=Nr-1,1,-1 |
633 |
|
|
DO j=1-Oly,sNy+Oly |
634 |
|
|
DO i=1-Olx,sNx+Olx |
635 |
|
|
IF(k.LE.surfk(i,j)) THEN |
636 |
|
|
C We are in the surface layer. Change the thickness flux |
637 |
|
|
C and diffusivity as necessary. |
638 |
|
|
|
639 |
|
|
IF (GM_K3D_ThickSheet) THEN |
640 |
|
|
C We are in the surface layer, so set the thickness flux |
641 |
|
|
C based on the average slope over the surface layer |
642 |
|
|
C If we are on the edge of a "cliff" the surface layer at the |
643 |
|
|
C centre of the grid point could be deeper than the U or V point. |
644 |
|
|
C So, we ensure that we always take a sensible slope. |
645 |
|
|
IF(kLow_U(i,j).LT.surfk(i,j)) THEN |
646 |
|
|
kk=kLow_U(i,j) |
647 |
|
|
hsurf = -rLowW(i,j,bi,bj) |
648 |
|
|
ELSE |
649 |
|
|
kk=surfk(i,j) |
650 |
|
|
hsurf = -surfkz(i,j) |
651 |
|
|
ENDIF |
652 |
|
|
IF(kk.GT.0) THEN |
653 |
|
|
IF(kk.EQ.Nr) THEN |
654 |
|
|
tfluxX(i,j,k) = -fCoriU(i,j)*maskW(i,j,k,bi,bj) |
655 |
|
|
& *SlopeX(i,j,kk)/hsurf |
656 |
|
|
ELSE |
657 |
|
|
tfluxX(i,j,k) = -fCoriU(i,j)*maskW(i,j,k,bi,bj) |
658 |
|
|
& *( SlopeX(i,j,kk)-SlopeX(i,j,kk+1) )/hsurf |
659 |
|
|
ENDIF |
660 |
|
|
ELSE |
661 |
|
|
tfluxX(i,j,k) = zeroRL |
662 |
|
|
ENDIF |
663 |
|
|
|
664 |
|
|
IF(kLow_V(i,j).LT.surfk(i,j)) THEN |
665 |
|
|
kk=kLow_V(i,j) |
666 |
|
|
hsurf = -rLowS(i,j,bi,bj) |
667 |
|
|
ELSE |
668 |
|
|
kk=surfk(i,j) |
669 |
|
|
hsurf = -surfkz(i,j) |
670 |
|
|
ENDIF |
671 |
|
|
IF(kk.GT.0) THEN |
672 |
|
|
IF(kk.EQ.Nr) THEN |
673 |
|
|
tfluxY(i,j,k) = -fCoriV(i,j)*maskS(i,j,k,bi,bj) |
674 |
|
|
& *SlopeY(i,j,kk)/hsurf |
675 |
|
|
ELSE |
676 |
|
|
tfluxY(i,j,k) = -fCoriV(i,j)*maskS(i,j,k,bi,bj) |
677 |
|
|
& *( SlopeY(i,j,kk)-SlopeY(i,j,kk+1) )/hsurf |
678 |
|
|
ENDIF |
679 |
|
|
ELSE |
680 |
|
|
tfluxY(i,j,k) = zeroRL |
681 |
|
|
ENDIF |
682 |
m_bates |
1.4 |
ENDIF |
683 |
m_bates |
1.1 |
|
684 |
m_bates |
1.14 |
IF (GM_K3D_surfK) THEN |
685 |
|
|
C Use a constant K in the surface layer. |
686 |
|
|
KPV(i,j,k) = GM_K3D_constK |
687 |
m_bates |
1.4 |
ENDIF |
688 |
m_bates |
1.1 |
ENDIF |
689 |
m_bates |
1.14 |
ENDDO |
690 |
|
|
ENDDO |
691 |
m_bates |
1.1 |
ENDDO |
692 |
m_bates |
1.14 |
ENDIF |
693 |
m_bates |
1.1 |
|
694 |
|
|
C Calculate gradq |
695 |
m_bates |
1.5 |
IF (GM_K3D_likeGM .OR. GM_K3D_beta_eq_0) THEN |
696 |
|
|
C Ignore beta in the calculation of grad(q) |
697 |
m_bates |
1.2 |
DO k=1,Nr |
698 |
|
|
DO j=1-Oly+1,sNy+Oly |
699 |
|
|
DO i=1-Olx+1,sNx+Olx |
700 |
|
|
gradqx(i,j,k) = maskW(i,j,k,bi,bj)*tfluxX(i,j,k) |
701 |
|
|
gradqy(i,j,k) = maskS(i,j,k,bi,bj)*tfluxY(i,j,k) |
702 |
|
|
ENDDO |
703 |
|
|
ENDDO |
704 |
|
|
ENDDO |
705 |
|
|
|
706 |
|
|
ELSE |
707 |
|
|
C Do not ignore beta |
708 |
|
|
DO k=1,Nr |
709 |
|
|
DO j=1-Oly+1,sNy+Oly |
710 |
|
|
DO i=1-Olx+1,sNx+Olx |
711 |
|
|
gradqx(i,j,k) = maskW(i,j,k,bi,bj)*(dfdx(i,j)+tfluxX(i,j,k)) |
712 |
|
|
gradqy(i,j,k) = maskS(i,j,k,bi,bj)*(dfdy(i,j)+tfluxY(i,j,k)) |
713 |
|
|
ENDDO |
714 |
|
|
ENDDO |
715 |
m_bates |
1.1 |
ENDDO |
716 |
m_bates |
1.2 |
ENDIF |
717 |
m_bates |
1.1 |
|
718 |
|
|
C ====================================== |
719 |
|
|
C Find Xi and the eddy induced velocities |
720 |
|
|
C ====================================== |
721 |
|
|
C Find the buoyancy frequency at the west and south faces of a cell |
722 |
|
|
C This is necessary to find the eigenvectors at those points |
723 |
|
|
DO k=1,Nr |
724 |
|
|
DO j=1-Oly+1,sNy+Oly |
725 |
|
|
DO i=1-Olx+1,sNx+Olx |
726 |
|
|
N2W(i,j,k) = maskW(i,j,k,bi,bj) |
727 |
|
|
& *( N2(i,j,k)+N2(i-1,j,k) ) |
728 |
|
|
N2S(i,j,k) = maskS(i,j,k,bi,bj) |
729 |
|
|
& *( N2(i,j,k)+N2(i,j-1,k) ) |
730 |
|
|
ENDDO |
731 |
|
|
ENDDO |
732 |
|
|
C This fudge is necessary to avoid division by zero in gmredi_calc_eigs. |
733 |
jmc |
1.7 |
C It does not affect the end result since it is in the overlap region. |
734 |
m_bates |
1.1 |
j=1-Oly |
735 |
|
|
DO i=1-Olx,sNx+Olx |
736 |
|
|
N2W(i,j,k) = GM_K3D_minN2 |
737 |
|
|
N2S(i,j,k) = GM_K3D_minN2 |
738 |
|
|
ENDDO |
739 |
|
|
i=1-Olx |
740 |
|
|
DO j=1-Oly,sNy+Oly |
741 |
|
|
N2W(i,j,k) = GM_K3D_minN2 |
742 |
|
|
N2S(i,j,k) = GM_K3D_minN2 |
743 |
|
|
ENDDO |
744 |
|
|
ENDDO |
745 |
|
|
|
746 |
m_bates |
1.14 |
C If GM_K3D_likeGM=.TRUE., the diffusivity for the eddy transport is |
747 |
|
|
C set to a constant equal to GM_K3D_constK. |
748 |
m_bates |
1.11 |
C If the diffusivity is constant the method here is the same as GM. |
749 |
m_bates |
1.14 |
C If GM_K3D_constRedi=.TRUE. K3D will be set equal to GM_K3D_constK later. |
750 |
m_bates |
1.2 |
IF(GM_K3D_likeGM) THEN |
751 |
m_bates |
1.3 |
DO k=1,Nr |
752 |
|
|
DO j=1-Oly,sNy+Oly |
753 |
|
|
DO i=1-Olx,sNx+Olx |
754 |
|
|
KPV(i,j,k) = GM_K3D_constK |
755 |
|
|
ENDDO |
756 |
m_bates |
1.2 |
ENDDO |
757 |
|
|
ENDDO |
758 |
m_bates |
1.3 |
ENDIF |
759 |
m_bates |
1.2 |
|
760 |
m_bates |
1.3 |
IF (.NOT. GM_K3D_smooth) THEN |
761 |
|
|
C Do not expand K grad(q) => no smoothing |
762 |
|
|
C May only be done with a constant K, otherwise the |
763 |
|
|
C integral constraint is violated. |
764 |
m_bates |
1.2 |
DO k=1,Nr |
765 |
|
|
DO j=1-Oly,sNy+Oly |
766 |
|
|
DO i=1-Olx,sNx+Olx |
767 |
m_bates |
1.3 |
Xix(i,j,k) = -maskW(i,j,k,bi,bj)*KPV(i,j,k)*gradqx(i,j,k) |
768 |
|
|
Xiy(i,j,k) = -maskS(i,j,k,bi,bj)*KPV(i,j,k)*gradqy(i,j,k) |
769 |
m_bates |
1.2 |
ENDDO |
770 |
|
|
ENDDO |
771 |
|
|
ENDDO |
772 |
|
|
|
773 |
|
|
ELSE |
774 |
m_bates |
1.3 |
C Expand K grad(q) in terms of baroclinic modes to smooth |
775 |
|
|
C and satisfy the integral constraint |
776 |
m_bates |
1.2 |
|
777 |
m_bates |
1.1 |
C Start with the X direction |
778 |
|
|
C ------------------------------ |
779 |
|
|
C Calculate the eigenvectors at the West face of a cell |
780 |
m_bates |
1.4 |
IF (update_modes) THEN |
781 |
|
|
CALL GMREDI_CALC_EIGS( |
782 |
|
|
I iMin,iMax,jMin,jMax,bi,bj,N2W,myThid, |
783 |
|
|
I kLow_U,maskW(:,:,:,bi,bj), |
784 |
|
|
I hfacW(:,:,:,bi,bj),recip_hfacW(:,:,:,bi,bj), |
785 |
|
|
I rLowW(:,:,bi,bj),GM_K3D_NModes,.FALSE., |
786 |
|
|
O dummy,modesW(:,:,:,:,bi,bj)) |
787 |
|
|
ENDIF |
788 |
m_bates |
1.1 |
|
789 |
|
|
C Calculate Xi_m at the west face of a cell |
790 |
|
|
DO j=1-Oly,sNy+Oly |
791 |
|
|
DO i=1-Olx,sNx+Olx |
792 |
|
|
DO m=1,GM_K3D_NModes |
793 |
|
|
XimX(m,i,j) = zeroRL |
794 |
|
|
ENDDO |
795 |
|
|
ENDDO |
796 |
|
|
ENDDO |
797 |
|
|
DO k=1,Nr |
798 |
|
|
DO j=1-Oly,sNy+Oly |
799 |
|
|
DO i=1-Olx,sNx+Olx |
800 |
|
|
DO m=1,GM_K3D_NModes |
801 |
m_bates |
1.13 |
Kdqdx(i,j,k) = KPV(i,j,k)*gradqx(i,j,k) |
802 |
|
|
XimX(m,i,j) = XimX(m,i,j) |
803 |
|
|
& - maskW(i,j,k,bi,bj)*drF(k)*hfacW(i,j,k,bi,bj) |
804 |
|
|
& *Kdqdx(i,j,k)*modesW(m,i,j,k,bi,bj) |
805 |
m_bates |
1.1 |
ENDDO |
806 |
|
|
ENDDO |
807 |
|
|
ENDDO |
808 |
|
|
ENDDO |
809 |
|
|
|
810 |
|
|
C Calculate Xi in the X direction at the west face |
811 |
|
|
DO k=1,Nr |
812 |
|
|
DO j=1-Oly,sNy+Oly |
813 |
|
|
DO i=1-Olx,sNx+Olx |
814 |
|
|
Xix(i,j,k) = zeroRL |
815 |
|
|
ENDDO |
816 |
|
|
ENDDO |
817 |
|
|
ENDDO |
818 |
|
|
DO k=1,Nr |
819 |
|
|
DO j=1-Oly,sNy+Oly |
820 |
|
|
DO i=1-Olx,sNx+Olx |
821 |
|
|
DO m=1,GM_K3D_NModes |
822 |
|
|
Xix(i,j,k) = Xix(i,j,k) |
823 |
m_bates |
1.4 |
& + maskW(i,j,k,bi,bj)*XimX(m,i,j)*modesW(m,i,j,k,bi,bj) |
824 |
m_bates |
1.1 |
ENDDO |
825 |
|
|
ENDDO |
826 |
|
|
ENDDO |
827 |
|
|
ENDDO |
828 |
|
|
|
829 |
|
|
C Now the Y direction |
830 |
|
|
C ------------------------------ |
831 |
|
|
C Calculate the eigenvectors at the West face of a cell |
832 |
m_bates |
1.4 |
IF (update_modes) THEN |
833 |
|
|
CALL GMREDI_CALC_EIGS( |
834 |
|
|
I iMin,iMax,jMin,jMax,bi,bj,N2S,myThid, |
835 |
|
|
I kLow_V,maskS(:,:,:,bi,bj), |
836 |
|
|
I hfacS(:,:,:,bi,bj),recip_hfacS(:,:,:,bi,bj), |
837 |
|
|
I rLowS(:,:,bi,bj), GM_K3D_NModes, .FALSE., |
838 |
|
|
O dummy,modesS(:,:,:,:,bi,bj)) |
839 |
|
|
ENDIF |
840 |
|
|
|
841 |
m_bates |
1.1 |
DO j=1-Oly,sNy+Oly |
842 |
|
|
DO i=1-Olx,sNx+Olx |
843 |
|
|
DO m=1,GM_K3D_NModes |
844 |
|
|
XimY(m,i,j) = zeroRL |
845 |
|
|
ENDDO |
846 |
|
|
ENDDO |
847 |
|
|
ENDDO |
848 |
|
|
DO k=1,Nr |
849 |
|
|
DO j=1-Oly,sNy+Oly |
850 |
|
|
DO i=1-Olx,sNx+Olx |
851 |
|
|
DO m=1,GM_K3D_NModes |
852 |
m_bates |
1.13 |
Kdqdy(i,j,k) = KPV(i,j,k)*gradqy(i,j,k) |
853 |
m_bates |
1.3 |
XimY(m,i,j) = XimY(m,i,j) |
854 |
|
|
& - drF(k)*hfacS(i,j,k,bi,bj) |
855 |
m_bates |
1.13 |
& *Kdqdy(i,j,k)*modesS(m,i,j,k,bi,bj) |
856 |
m_bates |
1.1 |
ENDDO |
857 |
|
|
ENDDO |
858 |
|
|
ENDDO |
859 |
|
|
ENDDO |
860 |
|
|
|
861 |
|
|
C Calculate Xi for Y direction at the south face |
862 |
|
|
DO k=1,Nr |
863 |
|
|
DO j=1-Oly,sNy+Oly |
864 |
|
|
DO i=1-Olx,sNx+Olx |
865 |
|
|
Xiy(i,j,k) = zeroRL |
866 |
|
|
ENDDO |
867 |
|
|
ENDDO |
868 |
|
|
ENDDO |
869 |
|
|
DO k=1,Nr |
870 |
|
|
DO j=1-Oly,sNy+Oly |
871 |
|
|
DO i=1-Olx,sNx+Olx |
872 |
|
|
DO m=1,GM_K3D_NModes |
873 |
|
|
Xiy(i,j,k) = Xiy(i,j,k) |
874 |
m_bates |
1.4 |
& + maskS(i,j,k,bi,bj)*XimY(m,i,j)*modesS(m,i,j,k,bi,bj) |
875 |
m_bates |
1.1 |
ENDDO |
876 |
|
|
ENDDO |
877 |
|
|
ENDDO |
878 |
|
|
ENDDO |
879 |
|
|
|
880 |
m_bates |
1.11 |
C ENDIF (.NOT. GM_K3D_smooth) |
881 |
m_bates |
1.1 |
ENDIF |
882 |
|
|
|
883 |
|
|
|
884 |
|
|
C Calculate the eddy induced velocity in the X direction at the west face |
885 |
|
|
DO k=1,Nr |
886 |
|
|
DO j=1-Oly+1,sNy+Oly |
887 |
|
|
DO i=1-Olx+1,sNx+Olx |
888 |
|
|
ustar(i,j,k) = -Xix(i,j,k)/coriU(i,j) |
889 |
|
|
ENDDO |
890 |
|
|
ENDDO |
891 |
|
|
ENDDO |
892 |
|
|
|
893 |
|
|
C Calculate the eddy induced velocity in the Y direction at the south face |
894 |
|
|
DO k=1,Nr |
895 |
|
|
DO j=1-Oly+1,sNy+Oly |
896 |
|
|
DO i=1-Olx+1,sNx+Olx |
897 |
|
|
vstar(i,j,k) = -Xiy(i,j,k)/coriV(i,j) |
898 |
|
|
ENDDO |
899 |
|
|
ENDDO |
900 |
|
|
ENDDO |
901 |
|
|
|
902 |
|
|
C ====================================== |
903 |
|
|
C Calculate the eddy induced overturning streamfunction |
904 |
|
|
C ====================================== |
905 |
|
|
#ifdef GM_K3D_PASSIVE |
906 |
|
|
k=Nr |
907 |
|
|
DO j=1-Oly,sNy+Oly |
908 |
|
|
DO i=1-Olx,sNx+Olx |
909 |
|
|
psistar(i,j,Nr) = -hfacS(i,j,k,bi,bj)*drF(k)*vstar(i,j,k) |
910 |
|
|
ENDDO |
911 |
|
|
ENDDO |
912 |
|
|
DO k=Nr-1,1,-1 |
913 |
|
|
DO j=1-Oly,sNy+Oly |
914 |
|
|
DO i=1-Olx,sNx+Olx |
915 |
|
|
psistar(i,j,k) = psistar(i,j,k+1) |
916 |
|
|
& - hfacS(i,j,k,bi,bj)*drF(k)*vstar(i,j,k) |
917 |
|
|
ENDDO |
918 |
|
|
ENDDO |
919 |
|
|
ENDDO |
920 |
|
|
|
921 |
|
|
#else |
922 |
|
|
|
923 |
|
|
IF (GM_AdvForm) THEN |
924 |
|
|
k=Nr |
925 |
|
|
DO j=1-Oly+1,sNy+1 |
926 |
|
|
DO i=1-Olx+1,sNx+1 |
927 |
|
|
GM_PsiX(i,j,k,bi,bj) = -hfacW(i,j,k,bi,bj)*drF(k)*ustar(i,j,k) |
928 |
|
|
GM_PsiY(i,j,k,bi,bj) = -hfacS(i,j,k,bi,bj)*drF(k)*vstar(i,j,k) |
929 |
|
|
ENDDO |
930 |
|
|
ENDDO |
931 |
|
|
DO k=Nr-1,1,-1 |
932 |
|
|
DO j=1-Oly+1,sNy+1 |
933 |
|
|
DO i=1-Olx+1,sNx+1 |
934 |
|
|
GM_PsiX(i,j,k,bi,bj) = GM_PsiX(i,j,k+1,bi,bj) |
935 |
|
|
& - hfacW(i,j,k,bi,bj)*drF(k)*ustar(i,j,k) |
936 |
|
|
GM_PsiY(i,j,k,bi,bj) = GM_PsiY(i,j,k+1,bi,bj) |
937 |
|
|
& - hfacS(i,j,k,bi,bj)*drF(k)*vstar(i,j,k) |
938 |
|
|
ENDDO |
939 |
|
|
ENDDO |
940 |
|
|
ENDDO |
941 |
|
|
|
942 |
|
|
ENDIF |
943 |
|
|
#endif |
944 |
|
|
|
945 |
|
|
#ifdef ALLOW_DIAGNOSTICS |
946 |
|
|
C Diagnostics |
947 |
|
|
IF ( useDiagnostics ) THEN |
948 |
|
|
CALL DIAGNOSTICS_FILL(K3D, 'GM_K3D ',0,Nr,0,1,1,myThid) |
949 |
m_bates |
1.14 |
CALL DIAGNOSTICS_FILL(KPV, 'GM_KPV ',0,Nr,0,1,1,myThid) |
950 |
m_bates |
1.1 |
CALL DIAGNOSTICS_FILL(urms, 'GM_URMS ',0,Nr,0,1,1,myThid) |
951 |
|
|
CALL DIAGNOSTICS_FILL(Rdef, 'GM_RDEF ',0, 1,0,1,1,myThid) |
952 |
m_bates |
1.8 |
CALL DIAGNOSTICS_FILL(Rurms, 'GM_RURMS',0, 1,0,1,1,myThid) |
953 |
|
|
CALL DIAGNOSTICS_FILL(RRhines,'GM_RRHNS',0, 1,0,1,1,myThid) |
954 |
m_bates |
1.1 |
CALL DIAGNOSTICS_FILL(Rmix, 'GM_RMIX ',0, 1,0,1,1,myThid) |
955 |
|
|
CALL DIAGNOSTICS_FILL(supp, 'GM_SUPP ',0,Nr,0,1,1,myThid) |
956 |
|
|
CALL DIAGNOSTICS_FILL(Xix, 'GM_Xix ',0,Nr,0,1,1,myThid) |
957 |
|
|
CALL DIAGNOSTICS_FILL(Xiy, 'GM_Xiy ',0,Nr,0,1,1,myThid) |
958 |
|
|
CALL DIAGNOSTICS_FILL(cDopp, 'GM_C ',0, 1,0,1,1,myThid) |
959 |
|
|
CALL DIAGNOSTICS_FILL(Ubaro, 'GM_UBARO',0, 1,0,1,1,myThid) |
960 |
|
|
CALL DIAGNOSTICS_FILL(eady, 'GM_EADY ',0, 1,0,1,1,myThid) |
961 |
|
|
CALL DIAGNOSTICS_FILL(SlopeX, 'GM_Sx ',0,Nr,0,1,1,myThid) |
962 |
|
|
CALL DIAGNOSTICS_FILL(SlopeY, 'GM_Sy ',0,Nr,0,1,1,myThid) |
963 |
|
|
CALL DIAGNOSTICS_FILL(tfluxX, 'GM_TFLXX',0,Nr,0,1,1,myThid) |
964 |
|
|
CALL DIAGNOSTICS_FILL(tfluxY, 'GM_TFLXY',0,Nr,0,1,1,myThid) |
965 |
|
|
CALL DIAGNOSTICS_FILL(gradqx, 'GM_dqdx ',0,Nr,0,1,1,myThid) |
966 |
|
|
CALL DIAGNOSTICS_FILL(gradqy, 'GM_dqdy ',0,Nr,0,1,1,myThid) |
967 |
m_bates |
1.13 |
CALL DIAGNOSTICS_FILL(Kdqdy, 'GM_Kdqdy',0,Nr,0,1,1,myThid) |
968 |
|
|
CALL DIAGNOSTICS_FILL(Kdqdx, 'GM_Kdqdx',0,Nr,0,1,1,myThid) |
969 |
m_bates |
1.1 |
CALL DIAGNOSTICS_FILL(surfkz, 'GM_SFLYR',0, 1,0,1,1,myThid) |
970 |
|
|
CALL DIAGNOSTICS_FILL(ustar, 'GM_USTAR',0,Nr,0,1,1,myThid) |
971 |
|
|
CALL DIAGNOSTICS_FILL(vstar, 'GM_VSTAR',0,Nr,0,1,1,myThid) |
972 |
|
|
CALL DIAGNOSTICS_FILL(umc, 'GM_UMC ',0,Nr,0,1,1,myThid) |
973 |
|
|
CALL DIAGNOSTICS_FILL(ubar, 'GM_UBAR ',0,Nr,0,1,1,myThid) |
974 |
m_bates |
1.4 |
CALL DIAGNOSTICS_FILL(modesC(1,:,:,:,bi,bj), |
975 |
|
|
& 'GM_MODEC',0,Nr,0,1,1,myThid) |
976 |
m_bates |
1.10 |
CALL DIAGNOSTICS_FILL(M4loc, 'GM_M4 ',0,Nr,0,1,1,myThid) |
977 |
|
|
CALL DIAGNOSTICS_FILL(N2loc, 'GM_N2 ',0,Nr,0,1,1,myThid) |
978 |
m_bates |
1.13 |
CALL DIAGNOSTICS_FILL(M4onN2, 'GM_M4_N2',0,Nr,0,1,1,myThid) |
979 |
m_bates |
1.10 |
CALL DIAGNOSTICS_FILL(slopeC, 'GM_SLOPE',0,Nr,0,1,1,myThid) |
980 |
|
|
|
981 |
m_bates |
1.1 |
ENDIF |
982 |
|
|
#endif |
983 |
|
|
|
984 |
m_bates |
1.11 |
C For the Redi diffusivity, we set K3D to a constant if |
985 |
m_bates |
1.14 |
C GM_K3D_constRedi=.TRUE. |
986 |
|
|
IF (GM_K3D_constRedi) THEN |
987 |
m_bates |
1.11 |
DO k=1,Nr |
988 |
|
|
DO j=1-Oly,sNy+Oly |
989 |
|
|
DO i=1-Olx,sNx+Olx |
990 |
|
|
K3D(i,j,k,bi,bj) = GM_K3D_constK |
991 |
|
|
ENDDO |
992 |
|
|
ENDDO |
993 |
|
|
ENDDO |
994 |
|
|
ENDIF |
995 |
|
|
|
996 |
m_bates |
1.14 |
#ifdef ALLOW_DIAGNOSTICS |
997 |
|
|
IF ( useDiagnostics ) |
998 |
|
|
& CALL DIAGNOSTICS_FILL(K3D, 'GM_K3D_T',0,Nr,0,1,1,myThid) |
999 |
|
|
#endif |
1000 |
|
|
|
1001 |
m_bates |
1.1 |
#endif /* GM_K3D */ |
1002 |
|
|
RETURN |
1003 |
|
|
END |