1 |
jmc |
1.8 |
C $Header: /u/gcmpack/MITgcm/pkg/thsice/thsice_solve4temp.F,v 1.7 2006/03/13 03:55:39 jmc Exp $ |
2 |
jmc |
1.1 |
C $Name: $ |
3 |
|
|
|
4 |
|
|
#include "THSICE_OPTIONS.h" |
5 |
|
|
|
6 |
|
|
CBOP |
7 |
|
|
C !ROUTINE: THSICE_SOLVE4TEMP |
8 |
|
|
C !INTERFACE: |
9 |
|
|
SUBROUTINE THSICE_SOLVE4TEMP( |
10 |
jmc |
1.8 |
I bi, bj, siLo, siHi, sjLo, sjHi, |
11 |
|
|
I iMin,iMax, jMin,jMax, dBugFlag, useBlkFlx, |
12 |
|
|
I iceMask, hIce, hSnow, tFrz, flxExSW, |
13 |
|
|
U flxSW, tSrf, qIc1, qIc2, |
14 |
|
|
O tIc1, tIc2, dTsrf, |
15 |
|
|
O sHeat, flxCnB, flxAtm, evpAtm, |
16 |
|
|
I myTime, myIter, myThid ) |
17 |
jmc |
1.1 |
C !DESCRIPTION: \bv |
18 |
|
|
C *==========================================================* |
19 |
|
|
C | S/R THSICE_SOLVE4TEMP |
20 |
|
|
C *==========================================================* |
21 |
|
|
C | Solve (implicitly) for sea-ice and surface temperature |
22 |
|
|
C *==========================================================* |
23 |
|
|
C \ev |
24 |
|
|
|
25 |
jmc |
1.8 |
C ADAPTED FROM: |
26 |
|
|
C LANL CICE.v2.0.2 |
27 |
|
|
C----------------------------------------------------------------------- |
28 |
|
|
C.. thermodynamics (vertical physics) based on M. Winton 3-layer model |
29 |
|
|
C.. See Bitz, C. M. and W. H. Lipscomb, 1999: "An energy-conserving |
30 |
|
|
C.. thermodynamic sea ice model for climate study." J. Geophys. |
31 |
|
|
C.. Res., 104, 15669 - 15677. |
32 |
|
|
C.. Winton, M., 1999: "A reformulated three-layer sea ice model." |
33 |
|
|
C.. Submitted to J. Atmos. Ocean. Technol. |
34 |
|
|
C.. authors Elizabeth C. Hunke and William Lipscomb |
35 |
|
|
C.. Fluid Dynamics Group, Los Alamos National Laboratory |
36 |
|
|
C----------------------------------------------------------------------- |
37 |
|
|
Cc****subroutine thermo_winton(n,fice,fsnow,dqice,dTsfc) |
38 |
|
|
C.. Compute temperature change using Winton model with 2 ice layers, of |
39 |
|
|
C.. which only the top layer has a variable heat capacity. |
40 |
|
|
|
41 |
jmc |
1.1 |
C !USES: |
42 |
|
|
IMPLICIT NONE |
43 |
|
|
|
44 |
|
|
C == Global variables === |
45 |
jmc |
1.5 |
#include "EEPARAMS.h" |
46 |
jmc |
1.1 |
#include "THSICE_SIZE.h" |
47 |
|
|
#include "THSICE_PARAMS.h" |
48 |
|
|
|
49 |
|
|
C !INPUT/OUTPUT PARAMETERS: |
50 |
|
|
C == Routine Arguments == |
51 |
jmc |
1.8 |
C siLo,siHi :: size of input/output array: 1rst dim. lower,higher bounds |
52 |
|
|
C sjLo,sjHi :: size of input/output array: 2nd dim. lower,higher bounds |
53 |
|
|
C bi,bj :: tile indices |
54 |
|
|
C iMin,iMax :: computation domain: 1rst index range |
55 |
|
|
C jMin,jMax :: computation domain: 2nd index range |
56 |
|
|
C dBugFlag :: allow to print debugging stuff (e.g. on 1 grid point). |
57 |
|
|
C useBlkFlx :: use surf. fluxes from bulk-forcing external S/R |
58 |
|
|
C--- Input: |
59 |
|
|
C iceMask :: sea-ice fractional mask [0-1] |
60 |
|
|
C hIce (hi) :: ice height [m] |
61 |
|
|
C hSnow (hs) :: snow height [m] |
62 |
|
|
C tFrz (Tf) :: sea-water freezing temperature [oC] (function of S) |
63 |
|
|
C flxExSW (=) :: surf. heat flux (+=down) except SW, function of surf. temp Ts: |
64 |
|
|
C 0: Flx(Ts=0) ; 1: Flx(Ts=Ts^n) ; 2: d.Flx/dTs(Ts=Ts^n) |
65 |
|
|
C--- Modified (input&output): |
66 |
|
|
C flxSW (netSW) :: net Short-Wave flux (+=down) [W/m2]: input= at surface |
67 |
|
|
C (=) :: output= below sea-ice, into the ocean |
68 |
|
|
C tSrf (Tsf) :: surface (ice or snow) temperature |
69 |
|
|
C qIc1 (qicen) :: ice enthalpy (J/kg), 1rst level |
70 |
|
|
C qIc2 (qicen) :: ice enthalpy (J/kg), 2nd level |
71 |
|
|
C--- Output |
72 |
|
|
C tIc1 (Tice) :: temperature of ice layer 1 [oC] |
73 |
|
|
C tIc2 (Tice) :: temperature of ice layer 2 [oC] |
74 |
|
|
C dTsrf (dTsf) :: surf. temp adjusment: Ts^n+1 - Ts^n |
75 |
|
|
C sHeat(sHeating):: surf heating flux left to melt snow or ice (= Atmos-conduction) |
76 |
|
|
C flxCnB (=) :: heat flux conducted through the ice to bottom surface |
77 |
|
|
C flxAtm (=) :: net flux of energy from the atmosphere [W/m2] (+=down) |
78 |
|
|
C without snow precip. (energy=0 for liquid water at 0.oC) |
79 |
|
|
C evpAtm (=) :: evaporation to the atmosphere [kg/m2/s] (>0 if evaporate) |
80 |
|
|
C--- Input: |
81 |
|
|
C myTime :: current Time of simulation [s] |
82 |
|
|
C myIter :: current Iteration number in simulation |
83 |
|
|
C myThid :: my Thread Id number |
84 |
|
|
INTEGER siLo, siHi, sjLo, sjHi |
85 |
|
|
INTEGER bi,bj |
86 |
|
|
INTEGER iMin, iMax |
87 |
|
|
INTEGER jMin, jMax |
88 |
|
|
LOGICAL dBugFlag |
89 |
jmc |
1.1 |
LOGICAL useBlkFlx |
90 |
jmc |
1.8 |
_RL iceMask(siLo:siHi,sjLo:sjHi) |
91 |
|
|
_RL hIce (siLo:siHi,sjLo:sjHi) |
92 |
|
|
_RL hSnow (siLo:siHi,sjLo:sjHi) |
93 |
|
|
_RL tFrz (siLo:siHi,sjLo:sjHi) |
94 |
|
|
_RL flxExSW(iMin:iMax,jMin:jMax,0:2) |
95 |
|
|
_RL flxSW (siLo:siHi,sjLo:sjHi) |
96 |
|
|
_RL tSrf (siLo:siHi,sjLo:sjHi) |
97 |
|
|
_RL qIc1 (siLo:siHi,sjLo:sjHi) |
98 |
|
|
_RL qIc2 (siLo:siHi,sjLo:sjHi) |
99 |
|
|
_RL tIc1 (siLo:siHi,sjLo:sjHi) |
100 |
|
|
_RL tIc2 (siLo:siHi,sjLo:sjHi) |
101 |
|
|
c _RL dTsrf (siLo:siHi,sjLo:sjHi) |
102 |
|
|
_RL dTsrf (iMin:iMax,jMin:jMax) |
103 |
|
|
_RL sHeat (siLo:siHi,sjLo:sjHi) |
104 |
|
|
_RL flxCnB (siLo:siHi,sjLo:sjHi) |
105 |
|
|
_RL flxAtm (siLo:siHi,sjLo:sjHi) |
106 |
|
|
_RL evpAtm (siLo:siHi,sjLo:sjHi) |
107 |
|
|
_RL myTime |
108 |
|
|
INTEGER myIter |
109 |
|
|
INTEGER myThid |
110 |
|
|
CEOP |
111 |
|
|
|
112 |
|
|
#ifdef ALLOW_THSICE |
113 |
|
|
C !LOCAL VARIABLES: |
114 |
|
|
C--- local copy of input/output argument list variables (see description above) |
115 |
|
|
c _RL flxExcSw(0:2) |
116 |
jmc |
1.1 |
_RL Tf |
117 |
|
|
_RL hi |
118 |
|
|
_RL hs |
119 |
jmc |
1.8 |
_RL netSW |
120 |
jmc |
1.1 |
_RL Tsf |
121 |
|
|
_RL qicen(nlyr) |
122 |
|
|
_RL Tice (nlyr) |
123 |
jmc |
1.8 |
c _RL sHeating |
124 |
|
|
c _RL flxCnB |
125 |
jmc |
1.1 |
_RL dTsf |
126 |
jmc |
1.8 |
c _RL flxAtm |
127 |
|
|
c _RL evpAtm |
128 |
jmc |
1.1 |
|
129 |
|
|
C == Local Variables == |
130 |
jmc |
1.8 |
INTEGER i,j |
131 |
jmc |
1.6 |
INTEGER k, iterMax |
132 |
jmc |
1.1 |
|
133 |
|
|
_RL frsnow ! fractional snow cover |
134 |
|
|
_RL fswpen ! SW penetrating beneath surface (W m-2) |
135 |
|
|
_RL fswdn ! SW absorbed at surface (W m-2) |
136 |
|
|
_RL fswint ! SW absorbed in ice (W m-2) |
137 |
|
|
_RL fswocn ! SW passed through ice to ocean (W m-2) |
138 |
|
|
_RL flxExceptSw ! net surface heat flux, except short-wave (W/m2) |
139 |
|
|
C evap :: evaporation over snow/ice [kg/m2/s] (>0 if evaporate) |
140 |
|
|
C dEvdT :: derivative of evap. with respect to Tsf [kg/m2/s/K] |
141 |
|
|
_RL evap, dEvdT |
142 |
|
|
_RL flx0 ! net surf heat flux, from Atmos. to sea-ice (W m-2) |
143 |
|
|
_RL fct ! heat conducted to top surface |
144 |
|
|
_RL df0dT ! deriv of flx0 wrt Tsf (W m-2 deg-1) |
145 |
|
|
_RL k12, k32 ! thermal conductivity terms |
146 |
|
|
_RL a10, b10 ! coefficients in quadratic eqn for T1 |
147 |
|
|
_RL a1, b1, c1 ! coefficients in quadratic eqn for T1 |
148 |
|
|
c _RL Tsf_start ! old value of Tsf |
149 |
|
|
_RL dt ! timestep |
150 |
jmc |
1.8 |
INTEGER iceornot |
151 |
jmc |
1.1 |
|
152 |
jmc |
1.8 |
C- define grid-point location where to print debugging values |
153 |
|
|
#include "THSICE_DEBUG.h" |
154 |
jmc |
1.1 |
|
155 |
jmc |
1.7 |
1010 FORMAT(A,I3,3F11.6) |
156 |
|
|
1020 FORMAT(A,1P4E14.6) |
157 |
jmc |
1.1 |
|
158 |
jmc |
1.8 |
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
159 |
|
|
|
160 |
jmc |
1.1 |
dt = thSIce_deltaT |
161 |
jmc |
1.8 |
DO j = jMin, jMax |
162 |
|
|
DO i = iMin, iMax |
163 |
|
|
IF ( iceMask(i,j).GT.0. _d 0) THEN |
164 |
|
|
hi = hIce(i,j) |
165 |
|
|
hs = hSnow(i,j) |
166 |
|
|
Tf = tFrz(i,j) |
167 |
|
|
netSW = flxSW(i,j) |
168 |
|
|
Tsf = tSrf(i,j) |
169 |
|
|
qicen(1)= qIc1(i,j) |
170 |
|
|
qicen(2)= qIc2(i,j) |
171 |
|
|
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
172 |
|
|
#ifdef ALLOW_DBUG_THSICE |
173 |
|
|
IF ( dBug(i,j,bi,bj) ) WRITE(6,'(A,2I4,2I2)') |
174 |
|
|
& 'ThSI_SOLVE4T: i,j=',i,j,bi,bj |
175 |
|
|
#endif |
176 |
jmc |
1.6 |
IF ( hi.LT.himin ) THEN |
177 |
jmc |
1.1 |
C If hi < himin, melt the ice. |
178 |
jmc |
1.3 |
STOP 'THSICE_SOLVE4TEMP: should not enter if hi<himin' |
179 |
jmc |
1.6 |
ENDIF |
180 |
jmc |
1.1 |
|
181 |
|
|
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
182 |
|
|
|
183 |
|
|
C fractional snow cover |
184 |
|
|
frsnow = 0. _d 0 |
185 |
jmc |
1.6 |
IF (hs .GT. 0. _d 0) frsnow = 1. _d 0 |
186 |
jmc |
1.1 |
|
187 |
|
|
C Compute SW flux absorbed at surface and penetrating to layer 1. |
188 |
jmc |
1.8 |
fswpen = netSW * (1. _d 0 - frsnow) * i0 |
189 |
jmc |
1.1 |
fswocn = fswpen * exp(-ksolar*hi) |
190 |
|
|
fswint = fswpen - fswocn |
191 |
|
|
|
192 |
jmc |
1.8 |
fswdn = netSW - fswpen |
193 |
jmc |
1.1 |
|
194 |
|
|
C Compute conductivity terms at layer interfaces. |
195 |
|
|
|
196 |
|
|
k12 = 4. _d 0*kice*ksnow / (ksnow*hi + 4. _d 0*kice*hs) |
197 |
|
|
k32 = 2. _d 0*kice / hi |
198 |
|
|
|
199 |
|
|
C compute ice temperatures |
200 |
|
|
a1 = cpice |
201 |
|
|
b1 = qicen(1) + (cpwater-cpice )*Tmlt1 - Lfresh |
202 |
|
|
c1 = Lfresh * Tmlt1 |
203 |
jmc |
1.6 |
Tice(1) = 0.5 _d 0 *(-b1 - SQRT(b1*b1-4. _d 0*a1*c1))/a1 |
204 |
jmc |
1.1 |
Tice(2) = (Lfresh-qicen(2)) / cpice |
205 |
|
|
|
206 |
jmc |
1.6 |
IF (Tice(1).GT.0. _d 0 .OR. Tice(2).GT.0. _d 0) THEN |
207 |
|
|
WRITE (6,*) 'BBerr Tice(1) > 0 = ',Tice(1) |
208 |
|
|
WRITE (6,*) 'BBerr Tice(2) > 0 = ',Tice(2) |
209 |
|
|
ENDIF |
210 |
jmc |
1.8 |
#ifdef ALLOW_DBUG_THSICE |
211 |
|
|
IF ( dBug(i,j,bi,bj) ) WRITE(6,1010) |
212 |
|
|
& 'ThSI_SOLVE4T: k, Ts, Tice=',0,Tsf,Tice |
213 |
|
|
#endif |
214 |
jmc |
1.1 |
|
215 |
|
|
C Compute coefficients used in quadratic formula. |
216 |
|
|
|
217 |
|
|
a10 = rhoi*cpice *hi/(2. _d 0*dt) + |
218 |
|
|
& k32 * (4. _d 0*dt*k32 + rhoi*cpice *hi) |
219 |
|
|
& / (6. _d 0*dt*k32 + rhoi*cpice *hi) |
220 |
|
|
b10 = -hi* |
221 |
|
|
& (rhoi*cpice*Tice(1)+rhoi*Lfresh*Tmlt1/Tice(1)) |
222 |
|
|
& /(2. _d 0*dt) |
223 |
|
|
& - k32 * (4. _d 0*dt*k32*Tf+rhoi*cpice *hi*Tice(2)) |
224 |
|
|
& / (6. _d 0*dt*k32 + rhoi*cpice *hi) - fswint |
225 |
|
|
c1 = rhoi*Lfresh*hi*Tmlt1 / (2. _d 0*dt) |
226 |
|
|
|
227 |
jmc |
1.4 |
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
228 |
jmc |
1.1 |
C Compute new surface and internal temperatures; iterate until |
229 |
|
|
C Tsfc converges. |
230 |
|
|
|
231 |
jmc |
1.6 |
IF ( useBlkFlx ) THEN |
232 |
|
|
iterMax = nitMaxTsf |
233 |
|
|
ELSE |
234 |
|
|
iterMax = 1 |
235 |
|
|
ENDIF |
236 |
|
|
dTsf = Terrmax |
237 |
|
|
|
238 |
jmc |
1.1 |
C ----- begin iteration ----- |
239 |
jmc |
1.6 |
DO k = 1,iterMax |
240 |
|
|
IF ( ABS(dTsf).GE.Terrmax ) THEN |
241 |
jmc |
1.1 |
|
242 |
|
|
C Save temperatures at start of iteration. |
243 |
|
|
c Tsf_start = Tsf |
244 |
|
|
|
245 |
|
|
IF ( useBlkFlx ) THEN |
246 |
|
|
C Compute top surface flux. |
247 |
jmc |
1.6 |
IF (hs.GT.3. _d -1) THEN |
248 |
jmc |
1.1 |
iceornot=2 |
249 |
jmc |
1.6 |
ELSE |
250 |
jmc |
1.1 |
iceornot=1 |
251 |
jmc |
1.6 |
ENDIF |
252 |
jmc |
1.1 |
CALL THSICE_GET_BULKF( |
253 |
|
|
I iceornot, Tsf, |
254 |
|
|
O flxExceptSw, df0dT, evap, dEvdT, |
255 |
|
|
I i,j,bi,bj,myThid ) |
256 |
|
|
ELSE |
257 |
jmc |
1.8 |
flxExceptSw = flxExSW(i,j,1) |
258 |
|
|
df0dT = flxExSW(i,j,2) |
259 |
jmc |
1.1 |
ENDIF |
260 |
jmc |
1.7 |
flx0 = fswdn + flxExceptSw |
261 |
jmc |
1.8 |
#ifdef ALLOW_DBUG_THSICE |
262 |
|
|
IF ( dBug(i,j,bi,bj) ) WRITE(6,1020) |
263 |
|
|
& 'ThSI_SOLVE4T: flx0,df0dT,k12,D=', flx0,df0dT,k12,k12-df0dT |
264 |
|
|
#endif |
265 |
jmc |
1.1 |
|
266 |
|
|
C Compute new top layer and surface temperatures. |
267 |
|
|
C If Tsfc is computed to be > 0 C, fix Tsfc = 0 and recompute T1 |
268 |
jmc |
1.7 |
C with different coefficients. |
269 |
jmc |
1.1 |
|
270 |
|
|
a1 = a10 - k12*df0dT / (k12-df0dT) |
271 |
|
|
b1 = b10 - k12*(flx0-df0dT*Tsf) / (k12-df0dT) |
272 |
jmc |
1.6 |
Tice(1) = -(b1 + SQRT(b1*b1-4. _d 0*a1*c1))/(2. _d 0*a1) |
273 |
jmc |
1.1 |
dTsf = (flx0 + k12*(Tice(1)-Tsf)) / (k12-df0dT) |
274 |
|
|
Tsf = Tsf + dTsf |
275 |
jmc |
1.6 |
IF (Tsf .GT. 0. _d 0) THEN |
276 |
jmc |
1.8 |
#ifdef ALLOW_DBUG_THSICE |
277 |
|
|
IF ( dBug(i,j,bi,bj) ) WRITE(6,1010) |
278 |
|
|
& 'ThSI_SOLVE4T: k,ts,t1,dTs=', k,Tsf,Tice(1),dTsf |
279 |
|
|
#endif |
280 |
jmc |
1.1 |
a1 = a10 + k12 |
281 |
|
|
b1 = b10 ! note b1 = b10 - k12*Tf0 |
282 |
jmc |
1.6 |
Tice(1) = (-b1 - SQRT(b1*b1-4. _d 0*a1*c1))/(2. _d 0*a1) |
283 |
jmc |
1.1 |
Tsf = 0. _d 0 |
284 |
|
|
IF ( useBlkFlx ) THEN |
285 |
jmc |
1.6 |
IF (hs.GT.3. _d -1) THEN |
286 |
jmc |
1.1 |
iceornot=2 |
287 |
jmc |
1.6 |
ELSE |
288 |
jmc |
1.1 |
iceornot=1 |
289 |
jmc |
1.6 |
ENDIF |
290 |
jmc |
1.1 |
CALL THSICE_GET_BULKF( |
291 |
|
|
I iceornot, Tsf, |
292 |
|
|
O flxExceptSw, df0dT, evap, dEvdT, |
293 |
|
|
I i,j,bi,bj,myThid ) |
294 |
|
|
dTsf = 0. _d 0 |
295 |
|
|
ELSE |
296 |
jmc |
1.8 |
flxExceptSw = flxExSW(i,j,0) |
297 |
jmc |
1.1 |
dTsf = 1000. |
298 |
|
|
df0dT = 0. |
299 |
|
|
ENDIF |
300 |
jmc |
1.7 |
flx0 = fswdn + flxExceptSw |
301 |
jmc |
1.6 |
ENDIF |
302 |
jmc |
1.1 |
|
303 |
|
|
C Check for convergence. If no convergence, then repeat. |
304 |
|
|
C |
305 |
jmc |
1.7 |
C Convergence test: Make sure Tsfc has converged, within prescribed error. |
306 |
jmc |
1.1 |
C (Energy conservation is guaranteed within machine roundoff, even |
307 |
|
|
C if Tsfc has not converged.) |
308 |
|
|
C If no convergence, then repeat. |
309 |
|
|
|
310 |
jmc |
1.8 |
#ifdef ALLOW_DBUG_THSICE |
311 |
|
|
IF ( dBug(i,j,bi,bj) ) WRITE(6,1010) |
312 |
|
|
& 'ThSI_SOLVE4T: k,ts,t1,dTs=', k,Tsf,Tice(1),dTsf |
313 |
|
|
#endif |
314 |
jmc |
1.6 |
IF ( useBlkFlx .AND. k.EQ.nitMaxTsf |
315 |
|
|
& .AND. ABS(dTsf).GE.Terrmax ) THEN |
316 |
|
|
WRITE (6,*) 'BB: thermw conv err ',i,j,bi,bj,dTsf |
317 |
|
|
WRITE (6,*) 'BB: thermw conv err, iceheight ', hi |
318 |
|
|
WRITE (6,*) 'BB: thermw conv err: Tsf, flx0', Tsf,flx0 |
319 |
|
|
IF (Tsf.LT.-70. _d 0) STOP |
320 |
jmc |
1.1 |
ENDIF |
321 |
|
|
|
322 |
|
|
100 continue ! surface temperature iteration |
323 |
jmc |
1.6 |
ENDIF |
324 |
|
|
ENDDO |
325 |
jmc |
1.1 |
150 continue |
326 |
|
|
C ------ end iteration ------------ |
327 |
|
|
|
328 |
|
|
C Compute new bottom layer temperature. |
329 |
|
|
|
330 |
|
|
Tice(2) = (2. _d 0*dt*k32*(Tice(1)+2. _d 0*Tf) |
331 |
|
|
& + rhoi*cpice *hi*Tice(2)) |
332 |
|
|
& /(6. _d 0*dt*k32 + rhoi*cpice *hi) |
333 |
jmc |
1.8 |
#ifdef ALLOW_DBUG_THSICE |
334 |
|
|
IF ( dBug(i,j,bi,bj) ) WRITE(6,1010) |
335 |
|
|
& 'ThSI_SOLVE4T: k, Ts, Tice=',k,Tsf,Tice |
336 |
|
|
#endif |
337 |
jmc |
1.1 |
|
338 |
|
|
C Compute final flux values at surfaces. |
339 |
|
|
|
340 |
|
|
fct = k12*(Tsf-Tice(1)) |
341 |
jmc |
1.8 |
flxCnB(i,j) = 4. _d 0*kice *(Tice(2)-Tf)/hi |
342 |
jmc |
1.1 |
flx0 = flx0 + df0dT*dTsf |
343 |
|
|
IF ( useBlkFlx ) THEN |
344 |
|
|
C-- needs to update also Evap (Tsf changes) since Latent heat has been updated |
345 |
jmc |
1.8 |
evpAtm(i,j) = evap + dEvdT*dTsf |
346 |
jmc |
1.1 |
ELSE |
347 |
jmc |
1.7 |
C- WARNING: Evap & +Evap*Lfresh are missing ! (but only affects Diagnostics) |
348 |
jmc |
1.8 |
evpAtm(i,j) = 0. |
349 |
jmc |
1.1 |
ENDIF |
350 |
jmc |
1.7 |
C- energy flux to Atmos: use net short-wave flux at surf. and |
351 |
|
|
C use latent heat = Lvap (energy=0 for liq. water at 0.oC) |
352 |
jmc |
1.8 |
flxAtm(i,j) = netSW + flxExceptSw |
353 |
|
|
& + df0dT*dTsf + evpAtm(i,j)*Lfresh |
354 |
jmc |
1.7 |
C- excess of energy @ surface (used for surface melting): |
355 |
jmc |
1.8 |
sHeat(i,j) = flx0 - fct |
356 |
jmc |
1.1 |
|
357 |
|
|
C- SW flux at sea-ice base left to the ocean |
358 |
jmc |
1.8 |
flxSW(i,j) = fswocn |
359 |
jmc |
1.1 |
|
360 |
jmc |
1.8 |
#ifdef ALLOW_DBUG_THSICE |
361 |
|
|
IF ( dBug(i,j,bi,bj) ) WRITE(6,1020) |
362 |
|
|
& 'ThSI_SOLVE4T: flx0,fct,Dif,flxCnB=', |
363 |
|
|
& flx0,fct,flx0-fct,flxCnB(i,j) |
364 |
|
|
#endif |
365 |
jmc |
1.1 |
|
366 |
|
|
C Compute new enthalpy for each layer. |
367 |
|
|
|
368 |
jmc |
1.7 |
qicen(1) = -cpwater*Tmlt1 + cpice *(Tmlt1-Tice(1)) |
369 |
|
|
& + Lfresh*(1. _d 0-Tmlt1/Tice(1)) |
370 |
jmc |
1.1 |
qicen(2) = -cpice *Tice(2) + Lfresh |
371 |
|
|
|
372 |
|
|
C Make sure internal ice temperatures do not exceed Tmlt. |
373 |
|
|
C (This should not happen for reasonable values of i0.) |
374 |
|
|
|
375 |
jmc |
1.7 |
IF (Tice(1) .GE. Tmlt1) THEN |
376 |
jmc |
1.6 |
WRITE (6,'(A,2I4,2I3,1P2E14.6)') |
377 |
jmc |
1.1 |
& 'BBerr - Bug: IceT(1) > Tmlt',i,j,bi,bj,Tice(1),Tmlt1 |
378 |
jmc |
1.6 |
ENDIF |
379 |
|
|
IF (Tice(2) .GE. 0. _d 0) THEN |
380 |
|
|
WRITE (6,'(A,2I4,2I3,1P2E14.6)') |
381 |
jmc |
1.1 |
& 'BBerr - Bug: IceT(2) > 0',i,j,bi,bj,Tice(2) |
382 |
jmc |
1.6 |
ENDIF |
383 |
jmc |
1.1 |
|
384 |
jmc |
1.8 |
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
385 |
|
|
C-- Update Sea-Ice state : |
386 |
|
|
tSrf(i,j) = Tsf |
387 |
|
|
tIc1(i,j) = Tice(1) |
388 |
|
|
tic2(i,j) = Tice(2) |
389 |
|
|
qIc1(i,j) = qicen(1) |
390 |
|
|
qIc2(i,j) = qicen(2) |
391 |
|
|
c dTsrf(i,j) = dTsf |
392 |
|
|
IF ( .NOT.useBlkFlx ) dTsrf(i,j) = dTsf |
393 |
|
|
c sHeat(i,j) = sHeating |
394 |
|
|
c flxCnB(i,j)= flxCnB |
395 |
|
|
c flxAtm(i,j)= flxAtm |
396 |
|
|
c evpAtm(i,j)= evpAtm |
397 |
|
|
#ifdef ALLOW_DBUG_THSICE |
398 |
|
|
IF ( dBug(i,j,bi,bj) ) THEN |
399 |
|
|
WRITE(6,1020) 'ThSI_SOLV_4T: Tsf, Tice(1,2), dTsurf=', |
400 |
|
|
& Tsf, Tice, dTsf |
401 |
|
|
WRITE(6,1020) 'ThSI_SOLV_4T: sHeat, flxCndBt, Qice =', |
402 |
|
|
& sHeat(i,j), flxCnB(i,j), qicen |
403 |
|
|
WRITE(6,1020) 'ThSI_SOLV_4T: flxA, evpA, fxSW_bf,af=', |
404 |
|
|
& flxAtm(i,j), evpAtm(i,j), netSW, flxSW(i,j) |
405 |
|
|
ENDIF |
406 |
|
|
#endif |
407 |
|
|
ELSE |
408 |
|
|
IF ( .NOT.useBlkFlx ) dTsrf(i,j) = 0. _d 0 |
409 |
|
|
ENDIF |
410 |
|
|
ENDDO |
411 |
|
|
ENDDO |
412 |
jmc |
1.1 |
#endif /* ALLOW_THSICE */ |
413 |
|
|
|
414 |
|
|
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
415 |
|
|
|
416 |
|
|
RETURN |
417 |
|
|
END |