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MFC
Exascale flow solver
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Integer bounds for variables. More...
Public Attributes | |
| integer | beg |
| integer | end |
| real(wp) | vb1 |
| real(wp) | vb2 |
| real(wp) | vb3 |
| real(wp) | ve1 |
| real(wp) | ve2 |
| real(wp) | ve3 |
| real(wp) | pres_in |
| real(wp) | pres_out |
| real(wp), dimension(3) | vel_in |
| real(wp), dimension(3) | vel_out |
| real(wp), dimension(num_fluids_max) | alpha_rho_in |
| real(wp), dimension(num_fluids_max) | alpha_in |
| logical | grcbc_in |
| logical | grcbc_out |
| logical | grcbc_vel_out |
| real(wp) | vel_in_ramp |
| Smooth start-up of a GRCBC inflow: the inflow velocity is scaled by f(t) = vel_in_frac0 + (1 - vel_in_frac0) (1 + tanh(6 (t - t0)/tau - 3))/2, so it leaves vel_in_frac0 of its final value at t0 and reaches it after vel_in_ramp. Inactive when the ramp duration is zero. | |
| real(wp) | vel_in_t0 |
| real(wp) | vel_in_frac0 |
| logical | isothermal_in |
| logical | isothermal_out |
| real(wp) | twall_in |
| real(wp) | twall_out |
Integer bounds for variables.
Definition at line 429 of file m_derived_types.fpp.f90.
| real(wp), dimension(num_fluids_max) m_derived_types::int_bounds_info::alpha_in |
Definition at line 440 of file m_derived_types.fpp.f90.
| real(wp), dimension(num_fluids_max) m_derived_types::int_bounds_info::alpha_rho_in |
Definition at line 440 of file m_derived_types.fpp.f90.
| integer m_derived_types::int_bounds_info::beg |
Definition at line 430 of file m_derived_types.fpp.f90.
| integer m_derived_types::int_bounds_info::end |
Definition at line 431 of file m_derived_types.fpp.f90.
| logical m_derived_types::int_bounds_info::grcbc_in |
Definition at line 441 of file m_derived_types.fpp.f90.
| logical m_derived_types::int_bounds_info::grcbc_out |
Definition at line 441 of file m_derived_types.fpp.f90.
| logical m_derived_types::int_bounds_info::grcbc_vel_out |
Definition at line 441 of file m_derived_types.fpp.f90.
| logical m_derived_types::int_bounds_info::isothermal_in |
Definition at line 446 of file m_derived_types.fpp.f90.
| logical m_derived_types::int_bounds_info::isothermal_out |
Definition at line 446 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::pres_in |
Definition at line 438 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::pres_out |
Definition at line 438 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::twall_in |
Definition at line 447 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::twall_out |
Definition at line 447 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::vb1 |
Definition at line 432 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::vb2 |
Definition at line 433 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::vb3 |
Definition at line 434 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::ve1 |
Definition at line 435 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::ve2 |
Definition at line 436 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::ve3 |
Definition at line 437 of file m_derived_types.fpp.f90.
| real(wp), dimension(3) m_derived_types::int_bounds_info::vel_in |
Definition at line 439 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::vel_in_frac0 |
Definition at line 445 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::vel_in_ramp |
Smooth start-up of a GRCBC inflow: the inflow velocity is scaled by f(t) = vel_in_frac0 + (1 - vel_in_frac0) (1 + tanh(6 (t - t0)/tau - 3))/2, so it leaves vel_in_frac0 of its final value at t0 and reaches it after vel_in_ramp. Inactive when the ramp duration is zero.
Definition at line 445 of file m_derived_types.fpp.f90.
| real(wp) m_derived_types::int_bounds_info::vel_in_t0 |
Definition at line 445 of file m_derived_types.fpp.f90.
| real(wp), dimension(3) m_derived_types::int_bounds_info::vel_out |
Definition at line 439 of file m_derived_types.fpp.f90.