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MODULE MODE_GRADIENT_M_PHY
IMPLICIT NONE
CONTAINS
! #########################################
SUBROUTINE GZ_M_W_PHY(D,PY,PDZZ,PGZ_M_W)
! #########################################
!
!!**** *GZ_M_W * - Compute the gradient along z direction for a
!! variable localized at a mass point
!!
!! PURPOSE
!! -------
! The purpose of this routine is to compute a gradient along x,y,z
! directions for a field PY localized at a mass point. The result PGZ_M_W
! is localized at a z-flux point (w point)
!
!
! dzm(PY)
! PGZ_M_W = -------
! d*zz
!
!!** METHOD
!! ------
!! We employ the Shuman operators to compute the derivatives and the
!! averages. The metric coefficients PDZZ are dummy arguments.
!!
!!
!! EXTERNAL
!! --------
!! FUNCTION DZM : compute a finite difference along the z
!! direction for a variable at a mass localization
!!
!! IMPLICIT ARGUMENTS
!! ------------------
!! Module MODI_SHUMAN : interface for the Shuman functions
!!
!! REFERENCE
!! ---------
!! Book2 of documentation (function GZ_M_W)
!!
!!
!! AUTHOR
!! ------
!! P. Hereil and J. Stein * Meteo France *
!!
!! MODIFICATIONS
!! -------------
!! Original 05/07/94
!! Modification 16/03/95 change the order of the arguments
!! 19/07/00 inlining(J. Stein)
!-------------------------------------------------------------------------------
!
!* 0. DECLARATIONS
! ------------
!
USE MODD_DIMPHYEX, ONLY: DIMPHYEX_t
!
IMPLICIT NONE
!
!* 0.1 Declarations of arguments and results
! -------------------------------------
!
TYPE(DIMPHYEX_t), INTENT(IN) :: D
!
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PDZZ !d*zz
!
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PY ! variable at mass
! localization
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(OUT) :: PGZ_M_W ! result at flux
! side
!
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INTEGER :: IKT,IKTB,IKTE,IIB,IJB,IIE,IJE,IKA,IKU,IKL
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INTEGER :: JI,JJ,JK
!-------------------------------------------------------------------------------
!
!* 1. COMPUTE THE GRADIENT ALONG Z
! -----------------------------
!
IKT=D%NKT
IKTB=D%NKTB
IKTE=D%NKTE
IIE=D%NIEC
IIB=D%NIBC
IJE=D%NJEC
IJB=D%NJBC
IKT=D%NKT
IKA=D%NKA
IKU=D%NKU
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IKL=D%NKL
!
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DO JK=IKTB,IKTE
DO JJ=IJB,IJE
DO JI=IIB,IIE
PGZ_M_W(JI,JJ,JK) = (PY(JI,JJ,JK)-PY(JI,JJ,JK-IKL )) / PDZZ(JI,JJ,JK)
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ENDDO
ENDDO
ENDDO
!$mnh_expand_array(JI=IIB:IIE,JJ=IJB:IJE)
PGZ_M_W(IIB:IIE,IJB:IJE,IKU)= (PY(IIB:IIE,IJB:IJE,IKU)-PY(IIB:IIE,IJB:IJE,IKU-IKL)) &
/ PDZZ(IIB:IIE,IJB:IJE,IKU)
PGZ_M_W(IIB:IIE,IJB:IJE,IKA)= PGZ_M_W(IIB:IIE,IJB:IJE,IKU) ! -999.
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!$mnh_end_expand_array(JI=IIB:IIE,JJ=IJB:IJE)
!
!-------------------------------------------------------------------------------
!
END SUBROUTINE GZ_M_W_PHY
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!
SUBROUTINE GX_M_M_PHY(D,OFLAT,PA,PDXX,PDZZ,PDZX,PGX_M_M)
USE PARKIND1, ONLY : JPRB
USE YOMHOOK , ONLY : LHOOK, DR_HOOK
! #######################################################
!
!!**** *GX_M_M* - Cartesian Gradient operator:
!! computes the gradient in the cartesian X
!! direction for a variable placed at the
!! mass point and the result is placed at
!! the mass point.
!! PURPOSE
!! -------
! The purpose of this function is to compute the discrete gradient
! along the X cartesian direction for a field PA placed at the
! mass point. The result is placed at the mass point.
!
!
! ( ______________z )
! ( (___x ) )
! 1 ( _x (d*zx dzm(PA) ) )
! PGX_M_M = ---- (dxf(PA) - (------------)) )
! ___x ( ( ) )
! d*xx ( ( d*zz ) )
!
!
!
!!** METHOD
!! ------
!! The Chain rule of differencing is applied to variables expressed
!! in the Gal-Chen & Somerville coordinates to obtain the gradient in
!! the cartesian system
!!
!! EXTERNAL
!! --------
!! MXM,MXF,MZF : Shuman functions (mean operators)
!! DXF,DZF : Shuman functions (finite difference operators)
!!
!! IMPLICIT ARGUMENTS
!! ------------------
!! MODD_CONF : LFLAT
!!
!! REFERENCE
!! ---------
!! Book2 of documentation of Meso-NH (GRAD_CAR operators)
!! A Turbulence scheme for the Meso-NH model (Chapter 6)
!!
!! AUTHOR
!! ------
!! Joan Cuxart *INM and Meteo-France*
!!
!! MODIFICATIONS
!! -------------
!! Original 18/07/94
!! 19/07/00 add the LFLAT switch (J. Stein)
!! J.Escobar : 15/09/2015 : WENO5 & JPHEXT <> 1
!-------------------------------------------------------------------------
!
!* 0. DECLARATIONS
!
!
USE MODD_DIMPHYEX, ONLY: DIMPHYEX_t
USE SHUMAN_PHY, ONLY: DXF_PHY, MZF_PHY, DZM_PHY, MXF_PHY, MXM_PHY
!
IMPLICIT NONE
!
!
!* 0.1 declarations of arguments and result
!
TYPE(DIMPHYEX_t), INTENT(IN) :: D
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PA ! variable at the mass point
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PDXX ! metric coefficient dxx
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PDZZ ! metric coefficient dzz
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PDZX ! metric coefficient dzx
LOGICAL, INTENT(IN) :: OFLAT
!
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(OUT) :: PGX_M_M ! result mass point
REAL, DIMENSION(D%NIT,D%NJT,D%NKT) :: ZWORK1, ZWORK2, ZWORK3, ZWORK4, ZWORK5, ZWORK6, ZMXF_PDXX
!
INTEGER :: IIB,IJB,IIE,IJE,IKT
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INTEGER :: JI,JJ,JK
!
!* 0.2 declaration of local variables
!
! NONE
!
!----------------------------------------------------------------------------
!
!* 1. DEFINITION of GX_M_M
! --------------------
!
REAL(KIND=JPRB) :: ZHOOK_HANDLE
IF (LHOOK) CALL DR_HOOK('GX_M_M',0,ZHOOK_HANDLE)
!
IIE=D%NIEC
IIB=D%NIBC
IJE=D%NJEC
IJB=D%NJBC
IKT=D%NKT
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!
CALL MXF_PHY(D,PDXX,ZMXF_PDXX)
CALL MXM_PHY(D,PA,ZWORK1)
CALL DXF_PHY(D,ZWORK1,ZWORK2)
!
IF (.NOT. OFLAT) THEN
CALL DZM_PHY(D,PA,ZWORK3)
CALL MXF_PHY(D,PDZX,ZWORK4)
!$mnh_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
ZWORK5(IIB:IIE,IJB:IJE,1:IKT) = ZWORK3(IIB:IIE,IJB:IJE,1:IKT) * ZWORK4(IIB:IIE,IJB:IJE,1:IKT) &
/ PDZZ(IIB:IIE,IJB:IJE,1:IKT)
!$mnh_end_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
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CALL MZF_PHY(D,ZWORK5,ZWORK6)
!$mnh_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
PGX_M_M(IIB:IIE,IJB:IJE,1:IKT)= (ZWORK2(IIB:IIE,IJB:IJE,1:IKT) - ZWORK6(IIB:IIE,IJB:IJE,1:IKT)) &
/ ZMXF_PDXX(IIB:IIE,IJB:IJE,1:IKT)
!$mnh_end_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
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ELSE
!$mnh_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
PGX_M_M(IIB:IIE,IJB:IJE,1:IKT)= ZWORK2(IIB:IIE,IJB:IJE,1:IKT) / ZMXF_PDXX(IIB:IIE,IJB:IJE,1:IKT)
!$mnh_end_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
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END IF
!
!----------------------------------------------------------------------------
!
IF (LHOOK) CALL DR_HOOK('GX_M_M',1,ZHOOK_HANDLE)
END SUBROUTINE GX_M_M_PHY
!
SUBROUTINE GY_M_M_PHY(D,OFLAT,PA,PDYY,PDZZ,PDZY,PGY_M_M)
USE PARKIND1, ONLY : JPRB
USE YOMHOOK , ONLY : LHOOK, DR_HOOK
! #######################################################
!
!!**** *GY_M_M* - Cartesian Gradient operator:
!! computes the gradient in the cartesian Y
!! direction for a variable placed at the
!! mass point and the result is placed at
!! the mass point.
!! PURPOSE
!! -------
! The purpose of this function is to compute the discrete gradient
! along the Y cartesian direction for a field PA placed at the
! mass point. The result is placed at the mass point.
!
!
! ( ______________z )
! ( (___y ) )
! 1 ( _y (d*zy dzm(PA) ) )
! PGY_M_M = ---- (dyf(PA) - (------------)) )
! ___y ( ( ) )
! d*yy ( ( d*zz ) )
!
!
!!** METHOD
!! ------
!! The Chain rule of differencing is applied to variables expressed
!! in the Gal-Chen & Somerville coordinates to obtain the gradient in
!! the cartesian system
!!
!! EXTERNAL
!! --------
!! MYM,MYF,MZF : Shuman functions (mean operators)
!! DYF,DZF : Shuman functions (finite difference operators)
!!
!! IMPLICIT ARGUMENTS
!! ------------------
!! MODD_CONF : LFLAT
!!
!! REFERENCE
!! ---------
!! Book2 of documentation of Meso-NH (GRAD_CAR operators)
!! A Turbulence scheme for the Meso-NH model (Chapter 6)
!!
!! AUTHOR
!! ------
!! Joan Cuxart *INM and Meteo-France*
!!
!! MODIFICATIONS
!! -------------
!! Original 18/07/94
!! 19/07/00 add the LFLAT switch (J. Stein)
!-------------------------------------------------------------------------
!
!* 0. DECLARATIONS
!
!
USE MODD_DIMPHYEX, ONLY: DIMPHYEX_t
USE SHUMAN_PHY, ONLY: DYF_PHY, MZF_PHY, DZM_PHY, MYF_PHY, MYM_PHY
!
IMPLICIT NONE
!
!
!* 0.1 declarations of arguments and result
!
TYPE(DIMPHYEX_t), INTENT(IN) :: D
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PA ! variable at the mass point
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PDYY ! metric coefficient dyy
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PDZZ ! metric coefficient dzz
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PDZY ! metric coefficient dzy
LOGICAL, INTENT(IN) :: OFLAT
!
REAL, DIMENSION(D%NIT,D%NJT,D%NKT),INTENT(OUT) :: PGY_M_M ! result mass point
REAL, DIMENSION(D%NIT,D%NJT,D%NKT) :: ZWORK1, ZWORK2, ZWORK3, ZWORK4, ZWORK5, ZMYF_PDYY
!
INTEGER :: IIB,IJB,IIE,IJE,IKT
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INTEGER :: JI,JJ,JK
!
!* 0.2 declaration of local variables
!
REAL(KIND=JPRB) :: ZHOOK_HANDLE
IF (LHOOK) CALL DR_HOOK('GY_M_M',0,ZHOOK_HANDLE)
!
IIE=D%NIEC
IIB=D%NIBC
IJE=D%NJEC
IJB=D%NJBC
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IKT=D%NKT
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!
!----------------------------------------------------------------------------
!
!* 1. DEFINITION of GY_M_M
! --------------------
!
CALL MYM_PHY(D,PA,ZWORK1)
CALL DYF_PHY(D,ZWORK1,ZWORK2)
CALL MYF_PHY(D,PDYY,ZMYF_PDYY)
!
IF (.NOT. OFLAT) THEN
!
CALL DZM_PHY(D,PA,ZWORK3)
CALL MYF_PHY(D,PDZY,ZWORK4)
!$mnh_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
ZWORK5(IIB:IIE,IJB:IJE,1:IKT) = ZWORK4(IIB:IIE,IJB:IJE,1:IKT) * ZWORK3(IIB:IIE,IJB:IJE,1:IKT) &
/ PDZZ(IIB:IIE,IJB:IJE,1:IKT)
!$mnh_end_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
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CALL MZF_PHY(D,ZWORK5,ZWORK4)
!$mnh_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
PGY_M_M(IIB:IIE,IJB:IJE,1:IKT)= (ZWORK2(IIB:IIE,IJB:IJE,1:IKT)-ZWORK4(IIB:IIE,IJB:IJE,1:IKT)) &
/ZMYF_PDYY(IIB:IIE,IJB:IJE,1:IKT)
!$mnh_end_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
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ELSE
!$mnh_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
PGY_M_M(IIB:IIE,IJB:IJE,1:IKT) = ZWORK2(IIB:IIE,IJB:IJE,1:IKT)/ZMYF_PDYY(IIB:IIE,IJB:IJE,1:IKT)
!$mnh_end_expand_array(JI=IIB:IIE,JJ=IJB:IJE,JK=1:IKT)
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ENDIF
!
!----------------------------------------------------------------------------
!
IF (LHOOK) CALL DR_HOOK('GY_M_M',1,ZHOOK_HANDLE)
END SUBROUTINE GY_M_M_PHY
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!
! #######################################################
SUBROUTINE GX_M_U_PHY(D,OFLAT,PY,PDXX,PDZZ,PDZX,PGX_M_U)
USE PARKIND1, ONLY : JPRB
USE YOMHOOK , ONLY : LHOOK, DR_HOOK
! ##################################################
!
!!**** *GX_M_U * - Compute the gradient along x for a variable localized at
!! a mass point
!!
!! PURPOSE
!! -------
! The purpose of this routine is to compute a gradient along x
! direction for a field PY localized at a mass point. The result PGX_M_U
! is localized at a x-flux point (u point).
!
! ( ____________z )
! ( ________x )
! 1 ( dzm(PY) )
! PGX_M_U = ---- (dxm(PY) - d*zx -------- )
! d*xx ( d*zz )
!
!
!
!!** METHOD
!! ------
!! We employ the Shuman operators to compute the derivatives and the
!! averages. The metric coefficients PDXX,PDZX,PDZZ are dummy arguments.
!!
!!
!! EXTERNAL
!! --------
!! FUNCTION DXM: compute a finite difference along the x direction for
!! a variable at a mass localization
!! FUNCTION DZM: compute a finite difference along the y direction for
!! a variable at a mass localization
!! FUNCTION MXM: compute an average in the x direction for a variable
!! at a mass localization
!! FUNCTION MZF: compute an average in the z direction for a variable
!! at a flux side
!!
!! IMPLICIT ARGUMENTS
!! ------------------
!! MODD_CONF : LFLAT
!!
!! REFERENCE
!! ---------
!! Book2 of documentation (function GX_M_U)
!!
!!
!! AUTHOR
!! ------
!! P. Hereil and J. Stein * Meteo France *
!!
!! MODIFICATIONS
!! -------------
!! Original 05/07/94
!! Modification 16/03/95 change the order of the arguments
!! 19/07/00 add the LFLAT switch + inlining(J. Stein)
!! 20/08/00 optimization (J. Escobar)
!-------------------------------------------------------------------------------
!
!* 0. DECLARATIONS
! ------------
!
USE MODD_DIMPHYEX, ONLY: DIMPHYEX_t
USE MODD_PARAMETERS, ONLY : JPHEXT, JPVEXT_TURB
!
IMPLICIT NONE
!
!* 0.1 Declarations of arguments and result
! ------------------------------------
!
TYPE(DIMPHYEX_t), INTENT(IN) :: D
LOGICAL, INTENT(IN) :: OFLAT
REAL, DIMENSION(D%NIT*D%NJT*D%NKT), INTENT(IN) :: PY ! variable at the mass point
REAL, DIMENSION(D%NIT*D%NJT*D%NKT), INTENT(IN) :: PDXX ! metric coefficient dyy
REAL, DIMENSION(D%NIT*D%NJT*D%NKT), INTENT(IN) :: PDZZ ! metric coefficient dzz
REAL, DIMENSION(D%NIT*D%NJT*D%NKT), INTENT(IN) :: PDZX ! metric coefficient dzy
!
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(OUT) :: PGX_M_U ! result at flux
! side
REAL, DIMENSION(D%NIT*D%NJT*D%NKT) :: ZGX_M_U
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REAL, DIMENSION(D%NIT,D%NJT,D%NKT):: ZY, ZDXX
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INTEGER IIU,IKU,JI,JK,IKL, IKA
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!
INTEGER :: JJK,IJU
INTEGER :: JIJK,JIJKOR,JIJKEND
INTEGER :: JI_1JK, JIJK_1, JI_1JK_1, JIJKP1, JI_1JKP1
!
!
!-------------------------------------------------------------------------------
!
!* 1. COMPUTE THE GRADIENT ALONG X
! -----------------------------
!
REAL(KIND=JPRB) :: ZHOOK_HANDLE
IF (LHOOK) CALL DR_HOOK('GX_M_U',0,ZHOOK_HANDLE)
IIU=D%NIT
IJU=D%NJT
IKU=D%NKT
IKL=D%NKL
IKA=D%NKA
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!
CALL D1D_TO_3D(D,PDXX,ZDXX)
CALL D1D_TO_3D(D,PY,ZY)
!
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IF (.NOT. OFLAT) THEN
JIJKOR = 1 + JPHEXT + IIU*IJU*(JPVEXT_TURB+1 - 1)
JIJKEND = IIU*IJU*(IKU-JPVEXT_TURB)
!CDIR NODEP
!OCL NOVREC
DO JIJK=JIJKOR , JIJKEND
! indexation
JI_1JK = JIJK - 1
JIJK_1 = JIJK - IIU*IJU*IKL
JI_1JK_1 = JIJK - 1 - IIU*IJU*IKL
JIJKP1 = JIJK + IIU*IJU*IKL
JI_1JKP1 = JIJK - 1 + IIU*IJU*IKL
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!
ZGX_M_U(JIJK)= &
( PY(JIJK)-PY(JI_1JK) &
-( (PY(JIJK)-PY(JIJK_1)) / PDZZ(JIJK) &
+(PY(JI_1JK)-PY(JI_1JK_1)) / PDZZ(JI_1JK) &
) * PDZX(JIJK)* 0.25 &
-( (PY(JIJKP1)-PY(JIJK)) / PDZZ(JIJKP1) &
+(PY(JI_1JKP1)-PY(JI_1JK)) / PDZZ(JI_1JKP1) &
) * PDZX(JIJKP1)* 0.25 &
) / PDXX(JIJK)
END DO
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!
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CALL D1D_TO_3D(D,ZGX_M_U,PGX_M_U)
!
DO JI=1+JPHEXT,IIU
PGX_M_U(JI,:,IKU)= ( ZY(JI,:,IKU)-ZY(JI-1,:,IKU) ) / ZDXX(JI,:,IKU)
PGX_M_U(JI,:,IKA)= -999.
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END DO
ELSE
! PGX_M_U = DXM(PY) / PDXX
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PGX_M_U(1+1:IIU,:,:) = ( ZY(1+1:IIU,:,:)-ZY(1:IIU-1,:,:) ) &
/ ZDXX(1+1:IIU,:,:)
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!
ENDIF
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DO JI=1,JPHEXT
PGX_M_U(JI,:,:)=PGX_M_U(IIU-2*JPHEXT+JI,:,:) ! for reprod JPHEXT <> 1
END DO
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!
!-------------------------------------------------------------------------------
!
IF (LHOOK) CALL DR_HOOK('GX_M_U',1,ZHOOK_HANDLE)
END SUBROUTINE GX_M_U_PHY
!
SUBROUTINE GY_M_V_PHY(D,OFLAT,PY,PDYY,PDZZ,PDZY,PGY_M_V)
USE PARKIND1, ONLY : JPRB
USE YOMHOOK , ONLY : LHOOK, DR_HOOK
! ##################################################
!
!!**** *GY_M_V * - Compute the gradient along y for a variable localized at
!! a mass point
!!
!! PURPOSE
!! -------
! The purpose of this routine is to compute a gradient along y
! direction for a field PY localized at a mass point. The result PGY_M_V
! is localized at a y-flux point (v point).
!
! ( ____________z )
! ( ________y )
! 1 ( dzm(PY) )
! PGY_M_V = ---- (dym(PY) - d*zy -------- )
! d*yy ( d*zz )
!
!
!
!
!!** METHOD
!! ------
!! We employ the Shuman operators to compute the derivatives and the
!! averages. The metric coefficients PDYY,PDZY,PDZZ are dummy arguments.
!!
!!
!! EXTERNAL
!! --------
!! FUNCTION DYM: compute a finite difference along the y direction for
!! a variable at a mass localization
!! FUNCTION DZM: compute a finite difference along the y direction for
!! a variable at a mass localization
!! FUNCTION MYM: compute an average in the x direction for a variable
!! at a mass localization
!! FUNCTION MZF: compute an average in the z direction for a variable
!! at a flux side
!!
!! IMPLICIT ARGUMENTS
!! ------------------
!! MODD_CONF : LFLAT
!!
!! REFERENCE
!! ---------
!! Book2 of documentation (function GY_M_V)
!!
!!
!! AUTHOR
!! ------
!! P. Hereil and J. Stein * Meteo France *
!!
!! MODIFICATIONS
!! -------------
!! Original 05/07/94
!! Modification 16/03/95 change the order of the arguments
!! 19/07/00 add the LFLAT switch + inlining(J. Stein)
!-------------------------------------------------------------------------------
!
!* 0. DECLARATIONS
! ------------
!
USE MODD_DIMPHYEX, ONLY: DIMPHYEX_t
USE MODD_PARAMETERS, ONLY : JPHEXT, JPVEXT_TURB
!
IMPLICIT NONE
!
!* 0.1 Declarations of arguments and results
! -------------------------------------
!
TYPE(DIMPHYEX_t), INTENT(IN) :: D
LOGICAL, INTENT(IN) :: OFLAT
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PDYY !d*yy
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PDZY !d*zy
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PDZZ !d*zz
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: PY ! variable at mass
! localization
REAL, DIMENSION(D%NIT,D%NJT,D%NKT),INTENT(OUT) :: PGY_M_V ! result at flux
! side
!REAL, DIMENSION(D%NIT*D%NJT*D%NKT) :: ZGY_M_V
!REAL, DIMENSION(D%NIT,D%NJT,D%NKT):: ZY, ZDYY,ZDZZ,ZDZY
RODIER Quentin
committed
INTEGER IJU,IKU,JI,JJ,JK,IKL, IKA
RODIER Quentin
committed
!
!-------------------------------------------------------------------------------
!
!* 1. COMPUTE THE GRADIENT ALONG Y
! ----------------------------
!
REAL(KIND=JPRB) :: ZHOOK_HANDLE
IF (LHOOK) CALL DR_HOOK('GY_M_V',0,ZHOOK_HANDLE)
IJU=D%NJT
IKU=D%NKT
IKL=D%NKL
IKA=D%NKA
IKU=D%NKU
RODIER Quentin
committed
IF (.NOT. OFLAT) THEN
! PGY_M_V = ( DYM(PY) - MZF ( MYM( DZM(PY) /PDZZ ) * PDZY ) )/PDYY
DO JK=1+JPVEXT_TURB,IKU-JPVEXT_TURB
DO JJ=1+JPHEXT,IJU
PGY_M_V(:,JJ,JK)= &
( PY(:,JJ,JK)-PY(:,JJ-1,JK) &
-( (PY(:,JJ,JK)-PY(:,JJ,JK-IKL)) / PDZZ(:,JJ,JK) &
+(PY(:,JJ-1,JK)-PY(:,JJ-IKL,JK-IKL)) / PDZZ(:,JJ-1,JK) &
RODIER Quentin
committed
) * PDZY(:,JJ,JK)* 0.25 &
-( (PY(:,JJ,JK+IKL)-PY(:,JJ,JK)) / PDZZ(:,JJ,JK+IKL) &
+(PY(:,JJ-1,JK+IKL)-PY(:,JJ-1,JK)) / PDZZ(:,JJ-1,JK+IKL) &
) * PDZY(:,JJ,JK+IKL)* 0.25 &
RODIER Quentin
committed
) / PDYY(:,JJ,JK)
END DO
END DO
!
DO JJ=1+JPHEXT,IJU
PGY_M_V(:,JJ,IKU)= ( PY(:,JJ,IKU)-PY(:,JJ-1,IKU) ) / PDYY(:,JJ,IKU)
PGY_M_V(:,JJ,IKA)= -999.
RODIER Quentin
committed
END DO
!
ELSE
! PGY_M_V = DYM(PY)/PDYY
RODIER Quentin
committed
PGY_M_V(:,1+1:IJU,:) = ( PY(:,1+1:IJU,:)-PY(:,1:IJU-1,:) ) &
/ PDYY(:,1+1:IJU,:)
RODIER Quentin
committed
!
ENDIF
RODIER Quentin
committed
DO JJ=1,JPHEXT
PGY_M_V(:,JJ,:)=PGY_M_V(:,IJU-2*JPHEXT+JJ,:)
END DO
RODIER Quentin
committed
!
!-------------------------------------------------------------------------------
!
IF (LHOOK) CALL DR_HOOK('GY_M_V',1,ZHOOK_HANDLE)
END SUBROUTINE GY_M_V_PHY
!
SUBROUTINE D1D_TO_3D (D,P1D,P3D)
USE MODD_DIMPHYEX, ONLY: DIMPHYEX_t
IMPLICIT NONE
TYPE(DIMPHYEX_t), INTENT(IN) :: D
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(IN) :: P1D
REAL, DIMENSION(D%NIT,D%NJT,D%NKT), INTENT(OUT) :: P3D
P3D = P1D
END SUBROUTINE D1D_TO_3D
RODIER Quentin
committed
END MODULE MODE_GRADIENT_M_PHY