!====================== include file "xbt.h" =========================== ! Each XBT station is located at latitude "xbtlat" and longitude ! "xbtlon". Data is collected at each grid point from the first ! level down through the nearest model level corresponding to a ! depth of "xbtdpt" cm. Actually, all coordinates are converted to ! the nearest model temperature grid point. ! All basic quantities as well as all terms in the momentum, ! temperature, and salinity equations are averaged over the time ! period specified by "xbtint". ! The maximum number of XBTs may be increased by changing parameter ! "maxxbt" below. ! inputs: ! maxxbt = maximum number of XBTs allowed. ! kmxbt = maximum number of levels from surface downward (<=km) ! set kmxbt < km to save space ! xbtlat = real latitude of XBTs in degrees ! xbtlon = real longitude of XBTs in degrees ! xbtdpt = real depths of XBTs in cm ! items = number of items in the XBT ! xname = character*12 names of XBT quantities ! outputs: ! numxbt = actual number of XBTs used ! nxbtts = current number of time steps in accumulated XTB data ! ixbt = longitude index of nearest model temperature grid point ! corresponding to "xbtlon" ! jxbt = latitude index of nearest model temperature grid point ! corresponding to "xbtlat" ! kxbt = depth index of nearest model temperature grid point ! corresponding to "xbtdpt" ! nsxbt = starting number for the XBTs on each latitude ! nexbt = ending number for the XBTs on each latitude ! txbt = accumulator array for time rate of change of ! tracers. the total time rate of change ! is broken down into components as follows: ! the form is d( )/dt = terms (2) ... (10) where each ! term has the units of "tracer units/sec" using ! schematic terms for illustration. ! (1) = total time rate of change for the tracer ! (2) = change due to zonal nonlinear term (UT)x ! (3) = change due to meridional nonlinear term (VT)y ! (4) = change due to vertical nonlinear term (WT)z ! (5) = change due to zonal diffusion: Ah*Txx ! (6) = change due to meridional diffusion: Ah*Tyy ! (7) = change due to vertical diffusion: kappa_h*Tzz ! (8) = change due to source term ! (9) = change due to explicit convection ! (10) = change due to filtering ! the nonlinear terms can be broken into two parts: advection and a ! continuity part: The physically meaningful part is advection. ! eg: Zonal advection of tracer "A" is -U(A)x = A(Ux) - (UA)x ! (11) = zonal advection U(Ax) ! (12) = meridional advection V(Ay) ! (13) = vertical advection W(Az) ! (14) = change of tracer variance ! (15) = average tracer within volume (tracer units) ! uxbt = accumulator array for time rate of change of ! momentum. the total time rate of change ! is broken down into components as follows: ! the form is d( )/dt = terms (2) ... (13) where each ! term has the units of "cm/sec**2" and "Q" is the ! momentum component {zonal or meridional} using ! schematic terms for illustration. ! (1) = total time rate of change for the momentum ! (2) = change due to the pressure gradient: grad_p ! without the surface pressure gradients ! (i.e., for computing the internal modes) ! (3) = change due to zonal nonlinear term: (UQ)x ! (4) = change due to meridional nonlinear term: (VQ)y ! (5) = change due to vertical nonlinear term: (wQ)z ! (6) = change due to zonal viscosity: Am*Qxx ! (7) = change due to meridional viscosity: Am*Qyy ! (8) = change due to vertical viscosity: kappa_m*Qzz ! (9) = change due to metric terms ! (10) = change due to coriolis terms: fQ ! (11) = change due to source terms ! (12) = change due to surface pressure gradient ! this is obtained after solving the external mode ! in the stream function technique. It is solved ! directly from the elliptic equation for the ! prognostic surface pressure technique ! (13) = change due to metric advection ! the nonlinear terms can be broken into two parts: advection and a ! continuity part: The physically meaningful part is advection. ! eg: Zonal advection of vel component "Q" is -U(Q)x = Q(U)x - (UQ)x ! (14) = zonal advection U(Qx) ! (15) = meridional advection V(Qy) ! (16) = vertical advection W(Qz) ! (17) = average velocity component ! xbtw = accumulator array for vertical velocity. (cm/sec) ! this is the average of adv_vbu at top and bottom of cell ! txbtsf = accumulator array for tracer surface flux terms. ! tracer (#1,#2) units = (cal/cm**2/sec, gm/cm**2/sec) ! uxbtsf = accumulator array for wind stress terms. (dynes/cm**2) ! ntxbt = number of terms for tracers ! nuxbt = number of terms for velocity integer maxxbt, kmxbt, ntxbt, nuxbt parameter (maxxbt=3, kmxbt=4) parameter (ntxbt=15, nuxbt=17) integer nxbtts, numxbt, nsxbt, nexbt, ixbt, jxbt, kxbt common /cxbt_i/ nxbtts, numxbt, nsxbt(jmt), nexbt(jmt) common /cxbt_i/ ixbt(maxxbt), jxbt(maxxbt), kxbt(maxxbt) character(12) :: xnamet, xnameu, xnamex common /cxbt_c/ xnamet(ntxbt), xnameu(nuxbt,2), xnamex(4) real xbtlat, xbtlon, xbtdpt, txbt, txbtsf, uxbt, uxbtsf, xbtw common /cxbt_r/ xbtlat(maxxbt), xbtlon(maxxbt), xbtdpt(maxxbt) common /cxbt_r/ txbt(kmxbt,ntxbt,nt,maxxbt), txbtsf(nt,maxxbt) common /cxbt_r/ uxbt(kmxbt,nuxbt,2,maxxbt), uxbtsf(2,maxxbt) common /cxbt_r/ xbtw(kmxbt,maxxbt)