1 |
adcroft |
1.21 |
C $Header: /u/gcmpack/MITgcm/pkg/mom_vecinv/mom_vecinv.F,v 1.20 2004/06/02 13:23:55 adcroft Exp $ |
2 |
adcroft |
1.2 |
C $Name: $ |
3 |
adcroft |
1.1 |
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4 |
adcroft |
1.21 |
#include "MOM_VECINV_OPTIONS.h" |
5 |
adcroft |
1.1 |
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6 |
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SUBROUTINE MOM_VECINV( |
7 |
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I bi,bj,iMin,iMax,jMin,jMax,k,kUp,kDown, |
8 |
jmc |
1.4 |
I dPhiHydX,dPhiHydY,KappaRU,KappaRV, |
9 |
adcroft |
1.1 |
U fVerU, fVerV, |
10 |
jmc |
1.15 |
I myTime, myIter, myThid) |
11 |
adcroft |
1.1 |
C /==========================================================\ |
12 |
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C | S/R MOM_VECINV | |
13 |
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C | o Form the right hand-side of the momentum equation. | |
14 |
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C |==========================================================| |
15 |
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C | Terms are evaluated one layer at a time working from | |
16 |
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C | the bottom to the top. The vertically integrated | |
17 |
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C | barotropic flow tendency term is evluated by summing the | |
18 |
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C | tendencies. | |
19 |
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C | Notes: | |
20 |
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C | We have not sorted out an entirely satisfactory formula | |
21 |
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C | for the diffusion equation bc with lopping. The present | |
22 |
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C | form produces a diffusive flux that does not scale with | |
23 |
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C | open-area. Need to do something to solidfy this and to | |
24 |
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C | deal "properly" with thin walls. | |
25 |
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C \==========================================================/ |
26 |
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IMPLICIT NONE |
27 |
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28 |
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C == Global variables == |
29 |
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#include "SIZE.h" |
30 |
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#include "DYNVARS.h" |
31 |
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#include "EEPARAMS.h" |
32 |
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#include "PARAMS.h" |
33 |
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#include "GRID.h" |
34 |
jmc |
1.7 |
#ifdef ALLOW_TIMEAVE |
35 |
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#include "TIMEAVE_STATV.h" |
36 |
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#endif |
37 |
adcroft |
1.1 |
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38 |
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C == Routine arguments == |
39 |
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C fVerU - Flux of momentum in the vertical |
40 |
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C fVerV direction out of the upper face of a cell K |
41 |
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C ( flux into the cell above ). |
42 |
jmc |
1.4 |
C dPhiHydX,Y :: Gradient (X & Y dir.) of Hydrostatic Potential |
43 |
adcroft |
1.1 |
C bi, bj, iMin, iMax, jMin, jMax - Range of points for which calculation |
44 |
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C results will be set. |
45 |
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C kUp, kDown - Index for upper and lower layers. |
46 |
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C myThid - Instance number for this innvocation of CALC_MOM_RHS |
47 |
jmc |
1.4 |
_RL dPhiHydX(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
48 |
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_RL dPhiHydY(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
49 |
adcroft |
1.1 |
_RL KappaRU(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr) |
50 |
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_RL KappaRV(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr) |
51 |
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_RL fVerU(1-OLx:sNx+OLx,1-OLy:sNy+OLy,2) |
52 |
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_RL fVerV(1-OLx:sNx+OLx,1-OLy:sNy+OLy,2) |
53 |
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INTEGER kUp,kDown |
54 |
jmc |
1.15 |
_RL myTime |
55 |
adcroft |
1.2 |
INTEGER myIter |
56 |
adcroft |
1.1 |
INTEGER myThid |
57 |
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INTEGER bi,bj,iMin,iMax,jMin,jMax |
58 |
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59 |
edhill |
1.11 |
#ifdef ALLOW_MOM_VECINV |
60 |
jmc |
1.7 |
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61 |
adcroft |
1.2 |
C == Functions == |
62 |
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LOGICAL DIFFERENT_MULTIPLE |
63 |
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EXTERNAL DIFFERENT_MULTIPLE |
64 |
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65 |
adcroft |
1.1 |
C == Local variables == |
66 |
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_RL aF (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
67 |
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_RL vF (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
68 |
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_RL vrF (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
69 |
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_RL uCf (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
70 |
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_RL vCf (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
71 |
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_RL mT (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
72 |
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_RL pF (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
73 |
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_RL del2u(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
74 |
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_RL del2v(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
75 |
adcroft |
1.3 |
_RL tension(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
76 |
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_RL strain(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
77 |
adcroft |
1.1 |
_RS hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
78 |
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_RS r_hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
79 |
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_RS xA(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
80 |
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_RS yA(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
81 |
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_RL uFld(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
82 |
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_RL vFld(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
83 |
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_RL dStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
84 |
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_RL zStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
85 |
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_RL uDiss(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
86 |
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_RL vDiss(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
87 |
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C I,J,K - Loop counters |
88 |
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INTEGER i,j,k |
89 |
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C rVelMaskOverride - Factor for imposing special surface boundary conditions |
90 |
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C ( set according to free-surface condition ). |
91 |
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C hFacROpen - Lopped cell factos used tohold fraction of open |
92 |
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C hFacRClosed and closed cell wall. |
93 |
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_RL rVelMaskOverride |
94 |
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C xxxFac - On-off tracer parameters used for switching terms off. |
95 |
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_RL uDudxFac |
96 |
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_RL AhDudxFac |
97 |
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_RL A4DuxxdxFac |
98 |
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_RL vDudyFac |
99 |
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_RL AhDudyFac |
100 |
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_RL A4DuyydyFac |
101 |
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_RL rVelDudrFac |
102 |
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_RL ArDudrFac |
103 |
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_RL fuFac |
104 |
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_RL phxFac |
105 |
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_RL mtFacU |
106 |
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_RL uDvdxFac |
107 |
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_RL AhDvdxFac |
108 |
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_RL A4DvxxdxFac |
109 |
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_RL vDvdyFac |
110 |
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_RL AhDvdyFac |
111 |
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_RL A4DvyydyFac |
112 |
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_RL rVelDvdrFac |
113 |
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_RL ArDvdrFac |
114 |
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_RL fvFac |
115 |
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_RL phyFac |
116 |
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_RL vForcFac |
117 |
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_RL mtFacV |
118 |
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_RL wVelBottomOverride |
119 |
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LOGICAL bottomDragTerms |
120 |
jmc |
1.15 |
LOGICAL writeDiag |
121 |
adcroft |
1.1 |
_RL KE(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
122 |
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_RL omega3(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
123 |
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_RL vort3(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
124 |
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_RL hDiv(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
125 |
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126 |
heimbach |
1.9 |
#ifdef ALLOW_AUTODIFF_TAMC |
127 |
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C-- only the kDown part of fverU/V is set in this subroutine |
128 |
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C-- the kUp is still required |
129 |
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C-- In the case of mom_fluxform Kup is set as well |
130 |
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C-- (at least in part) |
131 |
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fVerU(1,1,kUp) = fVerU(1,1,kUp) |
132 |
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fVerV(1,1,kUp) = fVerV(1,1,kUp) |
133 |
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#endif |
134 |
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135 |
adcroft |
1.1 |
rVelMaskOverride=1. |
136 |
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IF ( k .EQ. 1 ) rVelMaskOverride=freeSurfFac |
137 |
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wVelBottomOverride=1. |
138 |
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IF (k.EQ.Nr) wVelBottomOverride=0. |
139 |
jmc |
1.15 |
writeDiag = DIFFERENT_MULTIPLE(diagFreq, myTime, |
140 |
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& myTime-deltaTClock) |
141 |
adcroft |
1.1 |
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142 |
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C Initialise intermediate terms |
143 |
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DO J=1-OLy,sNy+OLy |
144 |
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DO I=1-OLx,sNx+OLx |
145 |
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aF(i,j) = 0. |
146 |
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vF(i,j) = 0. |
147 |
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vrF(i,j) = 0. |
148 |
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uCf(i,j) = 0. |
149 |
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vCf(i,j) = 0. |
150 |
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mT(i,j) = 0. |
151 |
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pF(i,j) = 0. |
152 |
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del2u(i,j) = 0. |
153 |
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del2v(i,j) = 0. |
154 |
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dStar(i,j) = 0. |
155 |
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zStar(i,j) = 0. |
156 |
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uDiss(i,j) = 0. |
157 |
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vDiss(i,j) = 0. |
158 |
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vort3(i,j) = 0. |
159 |
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omega3(i,j) = 0. |
160 |
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ke(i,j) = 0. |
161 |
heimbach |
1.8 |
#ifdef ALLOW_AUTODIFF_TAMC |
162 |
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strain(i,j) = 0. _d 0 |
163 |
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tension(i,j) = 0. _d 0 |
164 |
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#endif |
165 |
adcroft |
1.1 |
ENDDO |
166 |
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ENDDO |
167 |
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168 |
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C-- Term by term tracer parmeters |
169 |
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C o U momentum equation |
170 |
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uDudxFac = afFacMom*1. |
171 |
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AhDudxFac = vfFacMom*1. |
172 |
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A4DuxxdxFac = vfFacMom*1. |
173 |
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vDudyFac = afFacMom*1. |
174 |
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AhDudyFac = vfFacMom*1. |
175 |
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A4DuyydyFac = vfFacMom*1. |
176 |
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rVelDudrFac = afFacMom*1. |
177 |
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ArDudrFac = vfFacMom*1. |
178 |
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mTFacU = mtFacMom*1. |
179 |
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fuFac = cfFacMom*1. |
180 |
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phxFac = pfFacMom*1. |
181 |
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C o V momentum equation |
182 |
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uDvdxFac = afFacMom*1. |
183 |
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AhDvdxFac = vfFacMom*1. |
184 |
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A4DvxxdxFac = vfFacMom*1. |
185 |
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vDvdyFac = afFacMom*1. |
186 |
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AhDvdyFac = vfFacMom*1. |
187 |
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A4DvyydyFac = vfFacMom*1. |
188 |
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rVelDvdrFac = afFacMom*1. |
189 |
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ArDvdrFac = vfFacMom*1. |
190 |
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mTFacV = mtFacMom*1. |
191 |
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fvFac = cfFacMom*1. |
192 |
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phyFac = pfFacMom*1. |
193 |
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vForcFac = foFacMom*1. |
194 |
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195 |
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IF ( no_slip_bottom |
196 |
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& .OR. bottomDragQuadratic.NE.0. |
197 |
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& .OR. bottomDragLinear.NE.0.) THEN |
198 |
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bottomDragTerms=.TRUE. |
199 |
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ELSE |
200 |
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bottomDragTerms=.FALSE. |
201 |
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ENDIF |
202 |
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203 |
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C-- with stagger time stepping, grad Phi_Hyp is directly incoporated in TIMESTEP |
204 |
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IF (staggerTimeStep) THEN |
205 |
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phxFac = 0. |
206 |
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phyFac = 0. |
207 |
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ENDIF |
208 |
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209 |
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C-- Calculate open water fraction at vorticity points |
210 |
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CALL MOM_CALC_HFACZ(bi,bj,k,hFacZ,r_hFacZ,myThid) |
211 |
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212 |
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C---- Calculate common quantities used in both U and V equations |
213 |
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C Calculate tracer cell face open areas |
214 |
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DO j=1-OLy,sNy+OLy |
215 |
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DO i=1-OLx,sNx+OLx |
216 |
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xA(i,j) = _dyG(i,j,bi,bj) |
217 |
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& *drF(k)*_hFacW(i,j,k,bi,bj) |
218 |
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yA(i,j) = _dxG(i,j,bi,bj) |
219 |
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& *drF(k)*_hFacS(i,j,k,bi,bj) |
220 |
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ENDDO |
221 |
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ENDDO |
222 |
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223 |
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C Make local copies of horizontal flow field |
224 |
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DO j=1-OLy,sNy+OLy |
225 |
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DO i=1-OLx,sNx+OLx |
226 |
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uFld(i,j) = uVel(i,j,k,bi,bj) |
227 |
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vFld(i,j) = vVel(i,j,k,bi,bj) |
228 |
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ENDDO |
229 |
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ENDDO |
230 |
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231 |
jmc |
1.7 |
C note (jmc) : Dissipation and Vort3 advection do not necesary |
232 |
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C use the same maskZ (and hFacZ) => needs 2 call(s) |
233 |
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c CALL MOM_VI_HFACZ_DISS(bi,bj,k,hFacZ,r_hFacZ,myThid) |
234 |
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235 |
adcroft |
1.16 |
CALL MOM_CALC_KE(bi,bj,k,2,uFld,vFld,KE,myThid) |
236 |
adcroft |
1.1 |
|
237 |
adcroft |
1.17 |
CALL MOM_CALC_HDIV(bi,bj,k,2,uFld,vFld,hDiv,myThid) |
238 |
adcroft |
1.1 |
|
239 |
adcroft |
1.18 |
CALL MOM_CALC_RELVORT3(bi,bj,k,uFld,vFld,hFacZ,vort3,myThid) |
240 |
adcroft |
1.1 |
|
241 |
adcroft |
1.20 |
IF (useAbsVorticity) |
242 |
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& CALL MOM_CALC_ABSVORT3(bi,bj,k,vort3,omega3,myThid) |
243 |
adcroft |
1.1 |
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244 |
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IF (momViscosity) THEN |
245 |
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C Calculate del^2 u and del^2 v for bi-harmonic term |
246 |
adcroft |
1.19 |
IF (viscA4.NE.0. |
247 |
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& .OR. viscA4Grid.NE.0. |
248 |
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& .OR. viscC4leith.NE.0. |
249 |
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& ) THEN |
250 |
adcroft |
1.2 |
CALL MOM_VI_DEL2UV(bi,bj,k,hDiv,vort3,hFacZ, |
251 |
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O del2u,del2v, |
252 |
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& myThid) |
253 |
adcroft |
1.17 |
CALL MOM_CALC_HDIV(bi,bj,k,2,del2u,del2v,dStar,myThid) |
254 |
adcroft |
1.18 |
CALL MOM_CALC_RELVORT3( |
255 |
adcroft |
1.2 |
& bi,bj,k,del2u,del2v,hFacZ,zStar,myThid) |
256 |
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ENDIF |
257 |
adcroft |
1.1 |
C Calculate dissipation terms for U and V equations |
258 |
adcroft |
1.2 |
C in terms of vorticity and divergence |
259 |
adcroft |
1.19 |
IF (viscAh.NE.0. .OR. viscA4.NE.0. |
260 |
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& .OR. viscAhGrid.NE.0. .OR. viscA4Grid.NE.0. |
261 |
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& .OR. viscC2leith.NE.0. .OR. viscC4leith.NE.0. |
262 |
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& ) THEN |
263 |
adcroft |
1.2 |
CALL MOM_VI_HDISSIP(bi,bj,k,hDiv,vort3,hFacZ,dStar,zStar, |
264 |
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O uDiss,vDiss, |
265 |
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& myThid) |
266 |
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ENDIF |
267 |
adcroft |
1.3 |
C or in terms of tension and strain |
268 |
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IF (viscAstrain.NE.0. .OR. viscAtension.NE.0.) THEN |
269 |
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CALL MOM_CALC_TENSION(bi,bj,k,uFld,vFld, |
270 |
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O tension, |
271 |
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I myThid) |
272 |
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CALL MOM_CALC_STRAIN(bi,bj,k,uFld,vFld,hFacZ, |
273 |
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O strain, |
274 |
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I myThid) |
275 |
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CALL MOM_HDISSIP(bi,bj,k, |
276 |
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I tension,strain,hFacZ,viscAtension,viscAstrain, |
277 |
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O uDiss,vDiss, |
278 |
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I myThid) |
279 |
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ENDIF |
280 |
adcroft |
1.1 |
ENDIF |
281 |
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|
282 |
jmc |
1.7 |
C- Return to standard hfacZ (min-4) and mask vort3 accordingly: |
283 |
|
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c CALL MOM_VI_MASK_VORT3(bi,bj,k,hFacZ,r_hFacZ,vort3,myThid) |
284 |
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285 |
adcroft |
1.1 |
C---- Zonal momentum equation starts here |
286 |
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287 |
|
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C-- Vertical flux (fVer is at upper face of "u" cell) |
288 |
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289 |
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C Eddy component of vertical flux (interior component only) -> vrF |
290 |
|
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IF (momViscosity.AND..NOT.implicitViscosity) |
291 |
|
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& CALL MOM_U_RVISCFLUX(bi,bj,k,uVel,KappaRU,vrF,myThid) |
292 |
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293 |
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C Combine fluxes |
294 |
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DO j=jMin,jMax |
295 |
|
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DO i=iMin,iMax |
296 |
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fVerU(i,j,kDown) = ArDudrFac*vrF(i,j) |
297 |
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ENDDO |
298 |
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ENDDO |
299 |
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300 |
|
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C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
301 |
|
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DO j=2-Oly,sNy+Oly-1 |
302 |
|
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DO i=2-Olx,sNx+Olx-1 |
303 |
|
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gU(i,j,k,bi,bj) = uDiss(i,j) |
304 |
|
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& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k) |
305 |
|
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& *recip_rAw(i,j,bi,bj) |
306 |
|
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& *( |
307 |
|
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& +fVerU(i,j,kUp)*rkFac - fVerU(i,j,kDown)*rkFac |
308 |
|
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& ) |
309 |
jmc |
1.4 |
& - phxFac*dPhiHydX(i,j) |
310 |
adcroft |
1.1 |
ENDDO |
311 |
|
|
ENDDO |
312 |
|
|
|
313 |
|
|
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
314 |
|
|
IF (momViscosity.AND.no_slip_sides) THEN |
315 |
|
|
C- No-slip BCs impose a drag at walls... |
316 |
|
|
CALL MOM_U_SIDEDRAG(bi,bj,k,uFld,del2u,hFacZ,vF,myThid) |
317 |
|
|
DO j=jMin,jMax |
318 |
|
|
DO i=iMin,iMax |
319 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j) |
320 |
|
|
ENDDO |
321 |
|
|
ENDDO |
322 |
|
|
ENDIF |
323 |
heimbach |
1.8 |
|
324 |
adcroft |
1.1 |
C- No-slip BCs impose a drag at bottom |
325 |
|
|
IF (momViscosity.AND.bottomDragTerms) THEN |
326 |
|
|
CALL MOM_U_BOTTOMDRAG(bi,bj,k,uFld,KE,KappaRU,vF,myThid) |
327 |
|
|
DO j=jMin,jMax |
328 |
|
|
DO i=iMin,iMax |
329 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j) |
330 |
|
|
ENDDO |
331 |
|
|
ENDDO |
332 |
|
|
ENDIF |
333 |
|
|
|
334 |
|
|
C-- Metric terms for curvilinear grid systems |
335 |
|
|
c IF (usingSphericalPolarMTerms) THEN |
336 |
|
|
C o Spherical polar grid metric terms |
337 |
|
|
c CALL MOM_U_METRIC_NH(bi,bj,k,uFld,wVel,mT,myThid) |
338 |
|
|
c DO j=jMin,jMax |
339 |
|
|
c DO i=iMin,iMax |
340 |
|
|
c gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mTFacU*mT(i,j) |
341 |
|
|
c ENDDO |
342 |
|
|
c ENDDO |
343 |
|
|
c ENDIF |
344 |
|
|
|
345 |
|
|
C---- Meridional momentum equation starts here |
346 |
|
|
|
347 |
|
|
C-- Vertical flux (fVer is at upper face of "v" cell) |
348 |
|
|
|
349 |
|
|
C Eddy component of vertical flux (interior component only) -> vrF |
350 |
|
|
IF (momViscosity.AND..NOT.implicitViscosity) |
351 |
|
|
& CALL MOM_V_RVISCFLUX(bi,bj,k,vVel,KappaRV,vrf,myThid) |
352 |
|
|
|
353 |
|
|
C Combine fluxes -> fVerV |
354 |
|
|
DO j=jMin,jMax |
355 |
|
|
DO i=iMin,iMax |
356 |
|
|
fVerV(i,j,kDown) = ArDvdrFac*vrF(i,j) |
357 |
|
|
ENDDO |
358 |
|
|
ENDDO |
359 |
|
|
|
360 |
|
|
C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
361 |
|
|
DO j=jMin,jMax |
362 |
|
|
DO i=iMin,iMax |
363 |
|
|
gV(i,j,k,bi,bj) = vDiss(i,j) |
364 |
|
|
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k) |
365 |
|
|
& *recip_rAs(i,j,bi,bj) |
366 |
|
|
& *( |
367 |
|
|
& +fVerV(i,j,kUp)*rkFac - fVerV(i,j,kDown)*rkFac |
368 |
|
|
& ) |
369 |
jmc |
1.4 |
& - phyFac*dPhiHydY(i,j) |
370 |
adcroft |
1.1 |
ENDDO |
371 |
|
|
ENDDO |
372 |
|
|
|
373 |
|
|
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
374 |
|
|
IF (momViscosity.AND.no_slip_sides) THEN |
375 |
|
|
C- No-slip BCs impose a drag at walls... |
376 |
|
|
CALL MOM_V_SIDEDRAG(bi,bj,k,vFld,del2v,hFacZ,vF,myThid) |
377 |
|
|
DO j=jMin,jMax |
378 |
|
|
DO i=iMin,iMax |
379 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vF(i,j) |
380 |
|
|
ENDDO |
381 |
|
|
ENDDO |
382 |
|
|
ENDIF |
383 |
|
|
C- No-slip BCs impose a drag at bottom |
384 |
|
|
IF (momViscosity.AND.bottomDragTerms) THEN |
385 |
|
|
CALL MOM_V_BOTTOMDRAG(bi,bj,k,vFld,KE,KappaRV,vF,myThid) |
386 |
|
|
DO j=jMin,jMax |
387 |
|
|
DO i=iMin,iMax |
388 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vF(i,j) |
389 |
|
|
ENDDO |
390 |
|
|
ENDDO |
391 |
|
|
ENDIF |
392 |
|
|
|
393 |
|
|
C-- Metric terms for curvilinear grid systems |
394 |
|
|
c IF (usingSphericalPolarMTerms) THEN |
395 |
|
|
C o Spherical polar grid metric terms |
396 |
|
|
c CALL MOM_V_METRIC_NH(bi,bj,k,vFld,wVel,mT,myThid) |
397 |
|
|
c DO j=jMin,jMax |
398 |
|
|
c DO i=iMin,iMax |
399 |
|
|
c gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mTFacV*mT(i,j) |
400 |
|
|
c ENDDO |
401 |
|
|
c ENDDO |
402 |
|
|
c ENDIF |
403 |
|
|
|
404 |
jmc |
1.5 |
C-- Horizontal Coriolis terms |
405 |
adcroft |
1.20 |
IF (useCoriolis .AND. .NOT.useCDscheme |
406 |
|
|
& .AND. .NOT. useAbsVorticity) THEN |
407 |
|
|
CALL MOM_VI_CORIOLIS(bi,bj,k,uFld,vFld,hFacZ,r_hFacZ, |
408 |
jmc |
1.5 |
& uCf,vCf,myThid) |
409 |
|
|
DO j=jMin,jMax |
410 |
|
|
DO i=iMin,iMax |
411 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j) |
412 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j) |
413 |
|
|
ENDDO |
414 |
adcroft |
1.1 |
ENDDO |
415 |
jmc |
1.15 |
IF ( writeDiag ) THEN |
416 |
|
|
CALL WRITE_LOCAL_RL('fV','I10',1,uCf,bi,bj,k,myIter,myThid) |
417 |
|
|
CALL WRITE_LOCAL_RL('fU','I10',1,vCf,bi,bj,k,myIter,myThid) |
418 |
|
|
ENDIF |
419 |
jmc |
1.5 |
ENDIF |
420 |
adcroft |
1.1 |
|
421 |
jmc |
1.5 |
IF (momAdvection) THEN |
422 |
|
|
C-- Horizontal advection of relative vorticity |
423 |
adcroft |
1.20 |
IF (useAbsVorticity) THEN |
424 |
|
|
CALL MOM_VI_U_CORIOLIS(bi,bj,K,vFld,omega3,hFacZ,r_hFacZ, |
425 |
|
|
& uCf,myThid) |
426 |
|
|
ELSE |
427 |
|
|
CALL MOM_VI_U_CORIOLIS(bi,bj,k,vFld,vort3,hFacZ,r_hFacZ, |
428 |
|
|
& uCf,myThid) |
429 |
|
|
ENDIF |
430 |
jmc |
1.5 |
c CALL MOM_VI_U_CORIOLIS_C4(bi,bj,K,vFld,vort3,r_hFacZ,uCf,myThid) |
431 |
|
|
DO j=jMin,jMax |
432 |
|
|
DO i=iMin,iMax |
433 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j) |
434 |
|
|
ENDDO |
435 |
adcroft |
1.1 |
ENDDO |
436 |
adcroft |
1.20 |
IF (useAbsVorticity) THEN |
437 |
|
|
CALL MOM_VI_V_CORIOLIS(bi,bj,K,uFld,omega3,hFacZ,r_hFacZ, |
438 |
|
|
& vCf,myThid) |
439 |
|
|
ELSE |
440 |
|
|
CALL MOM_VI_V_CORIOLIS(bi,bj,k,uFld,vort3,hFacZ,r_hFacZ, |
441 |
|
|
& vCf,myThid) |
442 |
|
|
ENDIF |
443 |
jmc |
1.5 |
c CALL MOM_VI_V_CORIOLIS_C4(bi,bj,K,uFld,vort3,r_hFacZ,vCf,myThid) |
444 |
|
|
DO j=jMin,jMax |
445 |
|
|
DO i=iMin,iMax |
446 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j) |
447 |
|
|
ENDDO |
448 |
adcroft |
1.1 |
ENDDO |
449 |
|
|
|
450 |
jmc |
1.15 |
IF ( writeDiag ) THEN |
451 |
|
|
CALL WRITE_LOCAL_RL('zV','I10',1,uCf,bi,bj,k,myIter,myThid) |
452 |
|
|
CALL WRITE_LOCAL_RL('zU','I10',1,vCf,bi,bj,k,myIter,myThid) |
453 |
|
|
ENDIF |
454 |
jmc |
1.7 |
#ifdef ALLOW_TIMEAVE |
455 |
dimitri |
1.13 |
#ifndef HRCUBE |
456 |
jmc |
1.7 |
IF (taveFreq.GT.0.) THEN |
457 |
|
|
CALL TIMEAVE_CUMUL_1K1T(uZetatave,vCf,deltaTClock, |
458 |
|
|
& Nr, k, bi, bj, myThid) |
459 |
|
|
CALL TIMEAVE_CUMUL_1K1T(vZetatave,uCf,deltaTClock, |
460 |
|
|
& Nr, k, bi, bj, myThid) |
461 |
|
|
ENDIF |
462 |
dimitri |
1.13 |
#endif /* ALLOW_TIMEAVE */ |
463 |
|
|
#endif /* ndef HRCUBE */ |
464 |
jmc |
1.7 |
|
465 |
jmc |
1.5 |
C-- Vertical shear terms (-w*du/dr & -w*dv/dr) |
466 |
jmc |
1.12 |
IF ( .NOT. momImplVertAdv ) THEN |
467 |
|
|
CALL MOM_VI_U_VERTSHEAR(bi,bj,K,uVel,wVel,uCf,myThid) |
468 |
|
|
DO j=jMin,jMax |
469 |
|
|
DO i=iMin,iMax |
470 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j) |
471 |
|
|
ENDDO |
472 |
jmc |
1.5 |
ENDDO |
473 |
jmc |
1.12 |
CALL MOM_VI_V_VERTSHEAR(bi,bj,K,vVel,wVel,vCf,myThid) |
474 |
|
|
DO j=jMin,jMax |
475 |
|
|
DO i=iMin,iMax |
476 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j) |
477 |
|
|
ENDDO |
478 |
jmc |
1.5 |
ENDDO |
479 |
jmc |
1.12 |
ENDIF |
480 |
adcroft |
1.1 |
|
481 |
|
|
C-- Bernoulli term |
482 |
jmc |
1.5 |
CALL MOM_VI_U_GRAD_KE(bi,bj,K,KE,uCf,myThid) |
483 |
|
|
DO j=jMin,jMax |
484 |
|
|
DO i=iMin,iMax |
485 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j) |
486 |
|
|
ENDDO |
487 |
|
|
ENDDO |
488 |
|
|
CALL MOM_VI_V_GRAD_KE(bi,bj,K,KE,vCf,myThid) |
489 |
|
|
DO j=jMin,jMax |
490 |
|
|
DO i=iMin,iMax |
491 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j) |
492 |
|
|
ENDDO |
493 |
adcroft |
1.1 |
ENDDO |
494 |
jmc |
1.15 |
IF ( writeDiag ) THEN |
495 |
|
|
CALL WRITE_LOCAL_RL('KEx','I10',1,uCf,bi,bj,k,myIter,myThid) |
496 |
|
|
CALL WRITE_LOCAL_RL('KEy','I10',1,vCf,bi,bj,k,myIter,myThid) |
497 |
|
|
ENDIF |
498 |
|
|
|
499 |
jmc |
1.5 |
C-- end if momAdvection |
500 |
|
|
ENDIF |
501 |
|
|
|
502 |
|
|
C-- Set du/dt & dv/dt on boundaries to zero |
503 |
adcroft |
1.1 |
DO j=jMin,jMax |
504 |
|
|
DO i=iMin,iMax |
505 |
jmc |
1.5 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)*_maskW(i,j,k,bi,bj) |
506 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)*_maskS(i,j,k,bi,bj) |
507 |
adcroft |
1.1 |
ENDDO |
508 |
|
|
ENDDO |
509 |
jmc |
1.5 |
|
510 |
adcroft |
1.2 |
|
511 |
jmc |
1.15 |
IF ( writeDiag ) THEN |
512 |
adcroft |
1.3 |
CALL WRITE_LOCAL_RL('Ds','I10',1,strain,bi,bj,k,myIter,myThid) |
513 |
|
|
CALL WRITE_LOCAL_RL('Dt','I10',1,tension,bi,bj,k,myIter,myThid) |
514 |
adcroft |
1.2 |
CALL WRITE_LOCAL_RL('Du','I10',1,uDiss,bi,bj,k,myIter,myThid) |
515 |
|
|
CALL WRITE_LOCAL_RL('Dv','I10',1,vDiss,bi,bj,k,myIter,myThid) |
516 |
adcroft |
1.3 |
CALL WRITE_LOCAL_RL('Z3','I10',1,vort3,bi,bj,k,myIter,myThid) |
517 |
adcroft |
1.20 |
CALL WRITE_LOCAL_RL('W3','I10',1,omega3,bi,bj,k,myIter,myThid) |
518 |
adcroft |
1.3 |
CALL WRITE_LOCAL_RL('KE','I10',1,KE,bi,bj,k,myIter,myThid) |
519 |
|
|
CALL WRITE_LOCAL_RL('D','I10',1,hdiv,bi,bj,k,myIter,myThid) |
520 |
adcroft |
1.1 |
ENDIF |
521 |
jmc |
1.7 |
|
522 |
edhill |
1.11 |
#endif /* ALLOW_MOM_VECINV */ |
523 |
adcroft |
1.1 |
|
524 |
|
|
RETURN |
525 |
|
|
END |