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| module | mom_bulk_mixed_layer |
| | Build mixed layer parameterization.
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| integer | mom_bulk_mixed_layer::id_clock_detrain =0 |
| | CPU clock IDs. More...
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| integer | mom_bulk_mixed_layer::id_clock_mech =0 |
| | CPU clock IDs. More...
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| integer | mom_bulk_mixed_layer::id_clock_conv =0 |
| | CPU clock IDs. More...
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| integer | mom_bulk_mixed_layer::id_clock_adjustment =0 |
| | CPU clock IDs. More...
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| integer | mom_bulk_mixed_layer::id_clock_eos =0 |
| | CPU clock IDs. More...
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| integer | mom_bulk_mixed_layer::id_clock_resort =0 |
| | CPU clock IDs. More...
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| integer | mom_bulk_mixed_layer::id_clock_pass =0 |
| | CPU clock IDs. More...
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| subroutine, public | mom_bulk_mixed_layer::bulkmixedlayer (h_3d, u_3d, v_3d, tv, fluxes, dt, ea, eb, G, GV, US, CS, optics, Hml, aggregate_FW_forcing, dt_diag, last_call) |
| | This subroutine partially steps the bulk mixed layer model. The following processes are executed, in the order listed. More...
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| subroutine | mom_bulk_mixed_layer::convective_adjustment (h, u, v, R0, Rcv, T, S, eps, d_eb, dKE_CA, cTKE, j, G, GV, US, CS, nz_conv) |
| | This subroutine does instantaneous convective entrainment into the buffer layers and mixed layers to remove hydrostatic instabilities. Any water that is lighter than currently in the mixed- or buffer- layer is entrained. More...
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| subroutine | mom_bulk_mixed_layer::mixedlayer_convection (h, d_eb, htot, Ttot, Stot, uhtot, vhtot, R0_tot, Rcv_tot, u, v, T, S, R0, Rcv, eps, dR0_dT, dRcv_dT, dR0_dS, dRcv_dS, netMassInOut, netMassOut, Net_heat, Net_salt, nsw, Pen_SW_bnd, opacity_band, Conv_En, dKE_FC, j, ksort, G, GV, US, CS, tv, fluxes, dt, aggregate_FW_forcing) |
| | This subroutine causes the mixed layer to entrain to the depth of free convection. The depth of free convection is the shallowest depth at which the fluid is denser than the average of the fluid above. More...
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| subroutine | mom_bulk_mixed_layer::find_starting_tke (htot, h_CA, fluxes, Conv_En, cTKE, dKE_FC, dKE_CA, TKE, TKE_river, Idecay_len_TKE, cMKE, dt, Idt_diag, j, ksort, G, GV, US, CS) |
| | This subroutine determines the TKE available at the depth of free convection to drive mechanical entrainment. More...
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| subroutine | mom_bulk_mixed_layer::mechanical_entrainment (h, d_eb, htot, Ttot, Stot, uhtot, vhtot, R0_tot, Rcv_tot, u, v, T, S, R0, Rcv, eps, dR0_dT, dRcv_dT, cMKE, Idt_diag, nsw, Pen_SW_bnd, opacity_band, TKE, Idecay_len_TKE, j, ksort, G, GV, US, CS) |
| | This subroutine calculates mechanically driven entrainment. More...
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| subroutine | mom_bulk_mixed_layer::sort_ml (h, R0, eps, G, GV, CS, ksort) |
| | This subroutine generates an array of indices that are sorted by layer density. More...
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| subroutine | mom_bulk_mixed_layer::resort_ml (h, T, S, R0, Rcv, RcvTgt, eps, d_ea, d_eb, ksort, G, GV, CS, dR0_dT, dR0_dS, dRcv_dT, dRcv_dS) |
| | This subroutine actually moves properties between layers to achieve a resorted state, with all of the resorted water either moved into the correct interior layers or in the top nkmb layers. More...
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| subroutine | mom_bulk_mixed_layer::mixedlayer_detrain_2 (h, T, S, R0, Rcv, RcvTgt, dt, dt_diag, d_ea, j, G, GV, US, CS, dR0_dT, dR0_dS, dRcv_dT, dRcv_dS, max_BL_det) |
| | This subroutine moves any water left in the former mixed layers into the two buffer layers and may also move buffer layer water into the interior isopycnal layers. More...
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| subroutine | mom_bulk_mixed_layer::mixedlayer_detrain_1 (h, T, S, R0, Rcv, RcvTgt, dt, dt_diag, d_ea, d_eb, j, G, GV, US, CS, dRcv_dT, dRcv_dS, max_BL_det) |
| | This subroutine moves any water left in the former mixed layers into the single buffer layers and may also move buffer layer water into the interior isopycnal layers. More...
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| subroutine, public | mom_bulk_mixed_layer::bulkmixedlayer_init (Time, G, GV, US, param_file, diag, CS) |
| | This subroutine initializes the MOM bulk mixed layer module. More...
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| real function | mom_bulk_mixed_layer::ef4 (Ht, En, I_L, dR_de) |
| | This subroutine returns an approximation to the integral R = exp(-L*(H+E)) integral(LH to L(H+E)) L/(1-(1+x)exp(-x)) dx. The approximation to the integrand is good to within -2% at x~.3 and +25% at x~3.5, but the exponential deemphasizes the importance of large x. When L=0, EF4 returns E/((Ht+E)*Ht). More...
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1.8.16