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C $Header$ |
C $Header$ |
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C $Name$ |
C $Name$ |
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cc |
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#include "OBCS_OPTIONS.h" |
#include "OBCS_OPTIONS.h" |
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SUBROUTINE ORLANSKI_EAST( bi, bj, futureTime, |
SUBROUTINE ORLANSKI_EAST( bi, bj, futureTime, |
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I uVel, vVel, wVel, theta, salt, |
I uVel, vVel, wVel, theta, salt, |
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I myThid ) |
I myThid ) |
10 |
C /==========================================================\ |
C /==========================================================\ |
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C | SUBROUTINE ORLANSKI_EAST | |
C | SUBROUTINE ORLANSKI_EAST | |
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#include "EEPARAMS.h" |
#include "EEPARAMS.h" |
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#include "PARAMS.h" |
#include "PARAMS.h" |
24 |
#include "GRID.h" |
#include "GRID.h" |
25 |
#include "OBCS.h" |
#include "OBCS_PARAMS.h" |
26 |
|
#include "OBCS_GRID.h" |
27 |
|
#include "OBCS_FIELDS.h" |
28 |
#include "ORLANSKI.h" |
#include "ORLANSKI.h" |
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|
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C SPK 6/2/00: Added radiative OBC's for salinity. |
C SPK 6/2/00: Added radiative OBCs for salinity. |
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C SPK 6/6/00: Changed calculation of OB*w. When K=1, the |
C SPK 6/6/00: Changed calculation of OB*w. When K=1, the |
32 |
C upstream value is used. For example on the eastern OB: |
C upstream value is used. For example on the eastern OB: |
33 |
C IF (K.EQ.1) THEN |
C IF (K.EQ.1) THEN |
34 |
C OBEw(J,K,bi,bj)=wVel(I_obc-1,J,K,bi,bj) |
C OBEw(J,K,bi,bj)=wVel(I_obc-1,J,K,bi,bj) |
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C ENDIF |
C ENDIF |
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C |
C |
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C SPK 7/7/00: 1) Removed OB*w fix (see above). |
C SPK 7/7/00: 1) Removed OB*w fix (see above). |
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C 2) Added variable CMAX. Maximum diagnosed phase speed is now |
C 2) Added variable CMAX. Maximum diagnosed phase speed is now |
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C clamped to CMAX. For stability of AB-II scheme (CFL) the |
C clamped to CMAX. For stability of AB-II scheme (CFL) the |
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C (non-dimensional) phase speed must be <0.5 |
C (non-dimensional) phase speed must be <0.5 |
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C 3) (Sonya Legg) Changed application of uVel and vVel. |
C 3) (Sonya Legg) Changed application of uVel and vVel. |
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C uVel on the western OB is actually applied at I_obc+1 |
C uVel on the western OB is actually applied at I_obc+1 |
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C while vVel on the southern OB is applied at J_obc+1. |
C while vVel on the southern OB is applied at J_obc+1. |
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C 4) (Sonya Legg) Added templates for forced OB's. |
C 4) (Sonya Legg) Added templates for forced OBs. |
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C |
C |
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C SPK 7/17/00: Non-uniform resolution is now taken into account in diagnosing |
C SPK 7/17/00: Non-uniform resolution is now taken into account in diagnosing |
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C phase speeds and time-stepping OB values. CL is still the |
C phase speeds and time-stepping OB values. CL is still the |
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C non-dimensional phase speed; CVEL is the dimensional phase |
C non-dimensional phase speed; CVEL is the dimensional phase |
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C speed: CVEL = CL*(dx or dy)/dt, where dx and dy is the |
C speed: CVEL = CL*(dx or dy)/dt, where dx and dy is the |
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C appropriate grid spacings. Note that CMAX (with which CL |
C appropriate grid spacings. Note that CMAX (with which CL |
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C is compared) remains non-dimensional. |
C is compared) remains non-dimensional. |
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C |
C |
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C SPK 7/18/00: Added code to allow filtering of phase speed following |
C SPK 7/18/00: Added code to allow filtering of phase speed following |
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C Blumberg and Kantha. There is now a separate array |
C Blumberg and Kantha. There is now a separate array |
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C CVEL_**, where **=Variable(U,V,T,S,W)Boundary(E,W,N,S) for |
C CVEL_**, where **=Variable(U,V,T,S,W)Boundary(E,W,N,S) for |
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C the dimensional phase speed. These arrays are initialized to |
C the dimensional phase speed. These arrays are initialized to |
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C zero in ini_obcs.F. CVEL_** is filtered according to |
C zero in ini_obcs.F. CVEL_** is filtered according to |
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C CVEL_** = fracCVEL*CVEL(new) + (1-fracCVEL)*CVEL_**(old). |
C CVEL_** = fracCVEL*CVEL(new) + (1-fracCVEL)*CVEL_**(old). |
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C fracCVEL=1.0 turns off filtering. |
C fracCVEL=1.0 turns off filtering. |
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C |
C |
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C SPK 7/26/00: Changed code to average phase speed. A new variable |
C SPK 7/26/00: Changed code to average phase speed. A new variable |
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C 'cvelTimeScale' was created. This variable must now be |
C 'cvelTimeScale' was created. This variable must now be |
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C specified. Then, fracCVEL=deltaT/cvelTimeScale. |
C specified. Then, fracCVEL=deltaT/cvelTimeScale. |
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C Since the goal is to smooth out the 'singularities' in the |
C Since the goal is to smooth out the 'singularities' in the |
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C diagnosed phase speed, cvelTimeScale could be picked as the |
C diagnosed phase speed, cvelTimeScale could be picked as the |
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C duration of the singular period in the unfiltered case. Thus, |
C duration of the singular period in the unfiltered case. Thus, |
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C for a plane wave cvelTimeScale might be the time take for the |
C for a plane wave cvelTimeScale might be the time take for the |
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C wave to travel a distance DX, where DX is the width of the region |
C wave to travel a distance DX, where DX is the width of the region |
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C near which d(phi)/dx is small. |
C near which d(phi)/dx is small. |
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C |
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C JBG 4/10/03: Fixed phase speed at western boundary (as suggested by |
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C Dale Durran in his MWR paper). Fixed value (in m/s) is |
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C passed in as variable CFIX in data.obcs. |
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C also now allow choice of Orlanski or fixed wavespeed |
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C (by means of new booleans useFixedCEast and |
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C useFixedCWest) without having to recompile each time |
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C |
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C == Routine arguments == |
C == Routine arguments == |
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INTEGER bi, bj |
INTEGER bi, bj |
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INTEGER myThid |
INTEGER myThid |
88 |
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|
89 |
#ifdef ALLOW_ORLANSKI |
#ifdef ALLOW_ORLANSKI |
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|
#ifdef ALLOW_OBCS_EAST |
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|
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C == Local variables == |
C == Local variables == |
93 |
INTEGER J, K, I_obc |
INTEGER J, K, I_obc |
99 |
/* cvelTimeScale is averaging period for phase speed in sec. */ |
/* cvelTimeScale is averaging period for phase speed in sec. */ |
100 |
|
|
101 |
fracCVEL = deltaT/cvelTimeScale /* fraction of new phase speed used*/ |
fracCVEL = deltaT/cvelTimeScale /* fraction of new phase speed used*/ |
102 |
f1 = fracCVEL /* don't change this. Set cvelTimeScale */ |
f1 = fracCVEL /* dont change this. Set cvelTimeScale */ |
103 |
f2 = 1.0-fracCVEL /* don't change this. set cvelTimeScale */ |
f2 = 1.0-fracCVEL /* dont change this. set cvelTimeScale */ |
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|
|
105 |
C Eastern OB (Orlanski Radiation Condition) |
C Eastern OB (Orlanski Radiation Condition) |
106 |
DO K=1,Nr |
DO K=1,Nr |
107 |
DO J=1-Oly,sNy+Oly |
DO J=1-OLy,sNy+OLy |
108 |
I_obc=OB_Ie(J,bi,bj) |
I_obc=OB_Ie(J,bi,bj) |
109 |
IF (I_obc.ne.0) THEN |
IF ( I_obc.NE.OB_indexNone ) THEN |
110 |
C uVel |
C uVel |
111 |
IF ((UE_STORE_2(J,K,bi,bj).eq.0.).and. |
IF ((UE_STORE_2(J,K,bi,bj).eq.0.).and. |
112 |
& (UE_STORE_3(J,K,bi,bj).eq.0.)) THEN |
& (UE_STORE_3(J,K,bi,bj).eq.0.)) THEN |
120 |
ELSEIF (CL.gt.CMAX) THEN |
ELSEIF (CL.gt.CMAX) THEN |
121 |
CL=CMAX |
CL=CMAX |
122 |
ENDIF |
ENDIF |
123 |
CVEL_UE(J,K,bi,bj) = f1*(CL*dxF(I_obc-2,J,bi,bj)/deltaT)+ |
IF (useFixedCEast) THEN |
124 |
& f2*CVEL_UE(J,K,bi,bj) |
C Fixed phase speed (ignoring all of that painstakingly |
125 |
|
C saved data...) |
126 |
|
CVEL_UE(J,K,bi,bj) = CFIX |
127 |
|
ELSE |
128 |
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CVEL_UE(J,K,bi,bj) = f1*(CL*dxF(I_obc-2,J,bi,bj)/deltaT |
129 |
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& )+f2*CVEL_UE(J,K,bi,bj) |
130 |
|
ENDIF |
131 |
C update OBC to next timestep |
C update OBC to next timestep |
132 |
OBEu(J,K,bi,bj)=uVel(I_obc,J,K,bi,bj)- |
OBEu(J,K,bi,bj)=uVel(I_obc,J,K,bi,bj)- |
133 |
& CVEL_UE(J,K,bi,bj)*(deltaT/dxF(I_obc-1,J,bi,bj))* |
& CVEL_UE(J,K,bi,bj)*(deltaT*recip_dxF(I_obc-1,J,bi,bj))* |
134 |
& (ab1*(uVel(I_obc,J,K,bi,bj)-uVel(I_obc-1,J,K,bi,bj)) + |
& (ab1*(uVel(I_obc,J,K,bi,bj)-uVel(I_obc-1,J,K,bi,bj)) + |
135 |
& ab2*(UE_STORE_4(J,K,bi,bj)-UE_STORE_1(J,K,bi,bj))) |
& ab2*(UE_STORE_4(J,K,bi,bj)-UE_STORE_1(J,K,bi,bj))) |
136 |
C vVel |
C vVel |
140 |
ELSE |
ELSE |
141 |
CL=-(vVel(I_obc-1,J,K,bi,bj)-VE_STORE_1(J,K,bi,bj))/ |
CL=-(vVel(I_obc-1,J,K,bi,bj)-VE_STORE_1(J,K,bi,bj))/ |
142 |
& (ab1*VE_STORE_2(J,K,bi,bj) + ab2*VE_STORE_3(J,K,bi,bj)) |
& (ab1*VE_STORE_2(J,K,bi,bj) + ab2*VE_STORE_3(J,K,bi,bj)) |
143 |
ENDIF |
ENDIF |
144 |
IF (CL.lt.0.) THEN |
IF (CL.lt.0.) THEN |
145 |
CL=0. |
CL=0. |
146 |
ELSEIF (CL.gt.CMAX) THEN |
ELSEIF (CL.gt.CMAX) THEN |
147 |
CL=CMAX |
CL=CMAX |
148 |
ENDIF |
ENDIF |
149 |
CVEL_VE(J,K,bi,bj) = f1*(CL*dxV(I_obc-1,J,bi,bj)/deltaT)+ |
IF (useFixedCEast) THEN |
150 |
& f2*CVEL_VE(J,K,bi,bj) |
C Fixed phase speed (ignoring all of that painstakingly |
151 |
|
C saved data...) |
152 |
|
CVEL_VE(J,K,bi,bj) = CFIX |
153 |
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ELSE |
154 |
|
CVEL_VE(J,K,bi,bj) = f1*(CL*dxV(I_obc-1,J,bi,bj) |
155 |
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$ /deltaT)+f2*CVEL_VE(J,K,bi,bj) |
156 |
|
ENDIF |
157 |
C update OBC to next timestep |
C update OBC to next timestep |
158 |
OBEv(J,K,bi,bj)=vVel(I_obc,J,K,bi,bj)- |
OBEv(J,K,bi,bj)=vVel(I_obc,J,K,bi,bj)- |
159 |
& CVEL_VE(J,K,bi,bj)*(deltaT/dxV(I_obc,J,bi,bj))* |
& CVEL_VE(J,K,bi,bj)*(deltaT*recip_dxV(I_obc,J,bi,bj))* |
160 |
& (ab1*(vVel(I_obc,J,K,bi,bj)-vVel(I_obc-1,J,K,bi,bj)) + |
& (ab1*(vVel(I_obc,J,K,bi,bj)-vVel(I_obc-1,J,K,bi,bj)) + |
161 |
& ab2*(VE_STORE_4(J,K,bi,bj)-VE_STORE_1(J,K,bi,bj))) |
& ab2*(VE_STORE_4(J,K,bi,bj)-VE_STORE_1(J,K,bi,bj))) |
162 |
C Temperature |
C Temperature |
163 |
IF ((TE_STORE_2(J,K,bi,bj).eq.0.).and. |
IF ((TE_STORE_2(J,K,bi,bj).eq.0.).and. |
164 |
& (TE_STORE_3(J,K,bi,bj).eq.0.)) THEN |
& (TE_STORE_3(J,K,bi,bj).eq.0.)) THEN |
166 |
ELSE |
ELSE |
167 |
CL=-(theta(I_obc-1,J,K,bi,bj)-TE_STORE_1(J,K,bi,bj))/ |
CL=-(theta(I_obc-1,J,K,bi,bj)-TE_STORE_1(J,K,bi,bj))/ |
168 |
& (ab1*TE_STORE_2(J,K,bi,bj) + ab2*TE_STORE_3(J,K,bi,bj)) |
& (ab1*TE_STORE_2(J,K,bi,bj) + ab2*TE_STORE_3(J,K,bi,bj)) |
169 |
ENDIF |
ENDIF |
170 |
IF (CL.lt.0.) THEN |
IF (CL.lt.0.) THEN |
171 |
CL=0. |
CL=0. |
172 |
ELSEIF (CL.gt.CMAX) THEN |
ELSEIF (CL.gt.CMAX) THEN |
173 |
CL=CMAX |
CL=CMAX |
174 |
ENDIF |
ENDIF |
175 |
CVEL_TE(J,K,bi,bj) = f1*(CL*dxC(I_obc-1,J,bi,bj)/deltaT)+ |
IF (useFixedCEast) THEN |
176 |
& f2*CVEL_TE(J,K,bi,bj) |
C Fixed phase speed (ignoring all of that painstakingly |
177 |
|
C saved data...) |
178 |
|
CVEL_TE(J,K,bi,bj) = CFIX |
179 |
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ELSE |
180 |
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CVEL_TE(J,K,bi,bj) = f1*(CL*dxC(I_obc-1,J,bi,bj) |
181 |
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$ /deltaT)+f2*CVEL_TE(J,K,bi,bj) |
182 |
|
ENDIF |
183 |
C update OBC to next timestep |
C update OBC to next timestep |
184 |
OBEt(J,K,bi,bj)=theta(I_obc,J,K,bi,bj)- |
OBEt(J,K,bi,bj)=theta(I_obc,J,K,bi,bj)- |
185 |
& CVEL_TE(J,K,bi,bj)*(deltaT/dxC(I_obc,J,bi,bj))* |
& CVEL_TE(J,K,bi,bj)*(deltaT*recip_dxC(I_obc,J,bi,bj))* |
186 |
& (ab1*(theta(I_obc,J,K,bi,bj)-theta(I_obc-1,J,K,bi,bj))+ |
& (ab1*(theta(I_obc,J,K,bi,bj)-theta(I_obc-1,J,K,bi,bj))+ |
187 |
& ab2*(TE_STORE_4(J,K,bi,bj)-TE_STORE_1(J,K,bi,bj))) |
& ab2*(TE_STORE_4(J,K,bi,bj)-TE_STORE_1(J,K,bi,bj))) |
188 |
C Salinity |
C Salinity |
189 |
IF ((SE_STORE_2(J,K,bi,bj).eq.0.).and. |
IF ((SE_STORE_2(J,K,bi,bj).eq.0.).and. |
192 |
ELSE |
ELSE |
193 |
CL=-(salt(I_obc-1,J,K,bi,bj)-SE_STORE_1(J,K,bi,bj))/ |
CL=-(salt(I_obc-1,J,K,bi,bj)-SE_STORE_1(J,K,bi,bj))/ |
194 |
& (ab1*SE_STORE_2(J,K,bi,bj) + ab2*SE_STORE_3(J,K,bi,bj)) |
& (ab1*SE_STORE_2(J,K,bi,bj) + ab2*SE_STORE_3(J,K,bi,bj)) |
195 |
ENDIF |
ENDIF |
196 |
IF (CL.lt.0.) THEN |
IF (CL.lt.0.) THEN |
197 |
CL=0. |
CL=0. |
198 |
ELSEIF (CL.gt.CMAX) THEN |
ELSEIF (CL.gt.CMAX) THEN |
199 |
CL=CMAX |
CL=CMAX |
200 |
ENDIF |
ENDIF |
201 |
CVEL_SE(J,K,bi,bj) = f1*(CL*dxC(I_obc-1,J,bi,bj)/deltaT)+ |
IF (useFixedCEast) THEN |
202 |
& f2*CVEL_SE(J,K,bi,bj) |
C Fixed phase speed (ignoring all of that painstakingly |
203 |
|
C saved data...) |
204 |
|
CVEL_SE(J,K,bi,bj) = CFIX |
205 |
|
ELSE |
206 |
|
CVEL_SE(J,K,bi,bj) = f1*(CL*dxC(I_obc-1,J,bi,bj) |
207 |
|
$ /deltaT)+f2*CVEL_SE(J,K,bi,bj) |
208 |
|
ENDIF |
209 |
C update OBC to next timestep |
C update OBC to next timestep |
210 |
OBEs(J,K,bi,bj)=salt(I_obc,J,K,bi,bj)- |
OBEs(J,K,bi,bj)=salt(I_obc,J,K,bi,bj)- |
211 |
& CVEL_SE(J,K,bi,bj)*(deltaT/dxC(I_obc,J,bi,bj))* |
& CVEL_SE(J,K,bi,bj)*(deltaT*recip_dxC(I_obc,J,bi,bj))* |
212 |
& (ab1*(salt(I_obc,J,K,bi,bj)-salt(I_obc-1,J,K,bi,bj))+ |
& (ab1*(salt(I_obc,J,K,bi,bj)-salt(I_obc-1,J,K,bi,bj))+ |
213 |
& ab2*(SE_STORE_4(J,K,bi,bj)-SE_STORE_1(J,K,bi,bj))) |
& ab2*(SE_STORE_4(J,K,bi,bj)-SE_STORE_1(J,K,bi,bj))) |
|
C wVel |
|
214 |
#ifdef ALLOW_NONHYDROSTATIC |
#ifdef ALLOW_NONHYDROSTATIC |
215 |
IF ((WE_STORE_2(J,K,bi,bj).eq.0.).and. |
IF ( nonHydrostatic ) THEN |
216 |
& (WE_STORE_3(J,K,bi,bj).eq.0.)) THEN |
C wVel |
217 |
CL=0. |
IF ((WE_STORE_2(J,K,bi,bj).eq.0.).and. |
218 |
ELSE |
& (WE_STORE_3(J,K,bi,bj).eq.0.)) THEN |
219 |
CL=-(wVel(I_obc-1,J,K,bi,bj)-WE_STORE_1(J,K,bi,bj))/ |
CL=0. |
220 |
& (ab1*WE_STORE_2(J,K,bi,bj)+ab2*WE_STORE_3(J,K,bi,bj)) |
ELSE |
221 |
ENDIF |
CL=-(wVel(I_obc-1,J,K,bi,bj)-WE_STORE_1(J,K,bi,bj))/ |
222 |
IF (CL.lt.0.) THEN |
& (ab1*WE_STORE_2(J,K,bi,bj)+ab2*WE_STORE_3(J,K,bi,bj)) |
223 |
CL=0. |
ENDIF |
224 |
ELSEIF (CL.gt.CMAX) THEN |
IF (CL.lt.0.) THEN |
225 |
CL=CMAX |
CL=0. |
226 |
ENDIF |
ELSEIF (CL.gt.CMAX) THEN |
227 |
CVEL_WE(J,K,bi,bj)=f1*(CL*dxC(I_obc-1,J,bi,bj)/deltaT) |
CL=CMAX |
228 |
|
ENDIF |
229 |
|
IF (useFixedCEast) THEN |
230 |
|
C Fixed phase speed (ignoring all of that painstakingly |
231 |
|
C saved data...) |
232 |
|
CVEL_WE(J,K,bi,bj) = CFIX |
233 |
|
ELSE |
234 |
|
CVEL_WE(J,K,bi,bj)=f1*(CL*dxC(I_obc-1,J,bi,bj)/deltaT) |
235 |
& + f2*CVEL_WE(J,K,bi,bj) |
& + f2*CVEL_WE(J,K,bi,bj) |
236 |
C update OBC to next timestep |
ENDIF |
237 |
OBEw(J,K,bi,bj)=wVel(I_obc,J,K,bi,bj)- |
C update OBC to next timestep |
238 |
& CVEL_WE(J,K,bi,bj)*(deltaT/dxC(I_obc,J,bi,bj))* |
OBEw(J,K,bi,bj)=wVel(I_obc,J,K,bi,bj)- |
239 |
& (ab1*(wVel(I_obc,J,K,bi,bj)-wVel(I_obc-1,J,K,bi,bj))+ |
& CVEL_WE(J,K,bi,bj)*(deltaT*recip_dxC(I_obc,J,bi,bj))* |
240 |
& ab2*(WE_STORE_4(J,K,bi,bj)-WE_STORE_1(J,K,bi,bj))) |
& (ab1*(wVel(I_obc,J,K,bi,bj)-wVel(I_obc-1,J,K,bi,bj))+ |
241 |
#endif |
& ab2*(WE_STORE_4(J,K,bi,bj)-WE_STORE_1(J,K,bi,bj))) |
242 |
|
ENDIF |
243 |
|
#endif /* ALLOW_NONHYDROSTATIC */ |
244 |
C update/save storage arrays |
C update/save storage arrays |
245 |
C uVel |
C uVel |
246 |
C copy t-1 to t-2 array |
C copy t-1 to t-2 array |
274 |
& salt(I_obc-2,J,K,bi,bj) |
& salt(I_obc-2,J,K,bi,bj) |
275 |
SE_STORE_1(J,K,bi,bj)=salt(I_obc-1,J,K,bi,bj) |
SE_STORE_1(J,K,bi,bj)=salt(I_obc-1,J,K,bi,bj) |
276 |
SE_STORE_4(J,K,bi,bj)=salt(I_obc,J,K,bi,bj) |
SE_STORE_4(J,K,bi,bj)=salt(I_obc,J,K,bi,bj) |
|
C wVel |
|
277 |
#ifdef ALLOW_NONHYDROSTATIC |
#ifdef ALLOW_NONHYDROSTATIC |
278 |
|
IF ( nonHydrostatic ) THEN |
279 |
|
C wVel |
280 |
C copy t-1 to t-2 array |
C copy t-1 to t-2 array |
281 |
WE_STORE_3(J,K,bi,bj)=WE_STORE_2(J,K,bi,bj) |
WE_STORE_3(J,K,bi,bj)=WE_STORE_2(J,K,bi,bj) |
282 |
C copy (current time) t to t-1 arrays |
C copy (current time) t to t-1 arrays |
284 |
& wVel(I_obc-2,J,K,bi,bj) |
& wVel(I_obc-2,J,K,bi,bj) |
285 |
WE_STORE_1(J,K,bi,bj)=wVel(I_obc-1,J,K,bi,bj) |
WE_STORE_1(J,K,bi,bj)=wVel(I_obc-1,J,K,bi,bj) |
286 |
WE_STORE_4(J,K,bi,bj)=wVel(I_obc,J,K,bi,bj) |
WE_STORE_4(J,K,bi,bj)=wVel(I_obc,J,K,bi,bj) |
287 |
#endif |
ENDIF |
288 |
|
#endif /* ALLOW_NONHYDROSTATIC */ |
289 |
ENDIF |
ENDIF |
290 |
ENDDO |
ENDDO |
291 |
ENDDO |
ENDDO |
292 |
|
|
293 |
|
#endif |
294 |
#endif /* ALLOW_ORLANSKI */ |
#endif /* ALLOW_ORLANSKI */ |
295 |
RETURN |
RETURN |
296 |
END |
END |