Convert ignition_chamulak to new reactions scheme (#1296)

Author: maximumcats

networks/ignition_chamulak/Make.package

@@ -1,10 +1,7 @@
 CEXE_headers += network_properties.H
 
 ifeq ($(USE_REACT),TRUE)
-  CEXE_sources += actual_network_data.cpp
   CEXE_headers += actual_network.H
-
-  CEXE_sources += actual_rhs_data.cpp
   CEXE_headers += actual_rhs.H
 
   USE_SCREENING = TRUE

networks/ignition_chamulak/actual_network.H

@@ -1,31 +1,144 @@
 #ifndef actual_network_H
 #define actual_network_H
 
+#define NEW_NETWORK_IMPLEMENTATION
+
 #include <AMReX_REAL.H>
 #include <AMReX_Vector.H>
 #include <AMReX_Array.H>
 
 #include <fundamental_constants.H>
 #include <network_properties.H>
+#include <rhs_type.H>
 
 using namespace amrex;
 
-void actual_network_init();
+AMREX_INLINE
+void actual_network_init() {}
 
 const std::string network_name = "ignition_chamulak";
 
-namespace network
-{
-    // M12_chamulak is the effective number of C12 nuclei destroyed per
-    // reaction
-    const Real M12_chamulak = 2.93e0_rt;
-}
-
 namespace Rates
 {
     enum NetworkRates {
-        NumRates = 1
+        chamulak_rate = 1,
+        NumRates = chamulak_rate
     };
 };
 
+namespace RHS {
+
+    AMREX_GPU_HOST_DEVICE AMREX_INLINE
+    constexpr rhs_t rhs_data (int rate)
+    {
+        using namespace Species;
+        using namespace Rates;
+
+        rhs_t data;
+
+        switch (rate) {
+
+        case chamulak_rate:
+            data.species_A = C12;
+            data.species_D = Ash;
+
+            // The composite "ash" particle we are creating has a A = 18,
+            // while we are consuming 2 C12 nucleons to create it. In order
+            // to conserve mass, we need to scale the number of ash particles
+            // created by 24 / 18 = 4 / 3.
+
+            data.number_A = 2.0_rt;
+            data.number_D = 4.0_rt / 3.0_rt;
+
+            data.exponent_A = 2;
+            data.exponent_D = 1;
+
+            // For each reaction, we lose 2.93 C12 nuclei (for a single rate,
+            // C12+C12, we would lose 2. In Chamulak et al. (2008), they say a
+            // value of 2.93 captures the energetics from a larger network.
+
+            data.forward_branching_ratio = 2.93e0_rt / 2.0_rt;
+            break;
+
+        }
+
+        return data;
+    }
+
+    template<int rate>
+    AMREX_GPU_HOST_DEVICE AMREX_INLINE
+    void evaluate_analytical_rate (const rhs_state_t& state, rate_t& rates)
+    {
+        using namespace Species;
+        using namespace Rates;
+
+        if constexpr (rate == chamulak_rate) {
+            // compute some often used temperature constants
+            Real T9     = state.tf.t9;
+            Real dT9dt  = 1.0_rt / 1.0e9_rt;
+            Real T9a    = T9 / (1.0_rt + 0.0396e0_rt * T9);
+            Real dT9adt = (T9a / T9 - (T9a / (1.0_rt + 0.0396e0_rt * T9)) * 0.0396e0_rt) * dT9dt;
+
+            // compute the CF88 rate
+            Real scratch    = std::pow(T9a, 1.0_rt / 3.0_rt);
+            Real dscratchdt = (1.0_rt / 3.0_rt) * std::pow(T9a, -2.0_rt / 3.0_rt) * dT9adt;
+
+            Real a    = 4.27e26_rt * std::pow(T9a, 5.0_rt / 6.0_rt) * std::pow(T9, -1.5e0_rt);
+            Real dadt = (5.0_rt / 6.0_rt) * (a / T9a) * dT9adt - 1.5e0_rt * (a / T9) * dT9dt;
+
+            Real b    = std::exp(-84.165e0_rt / scratch - 2.12e-3_rt * T9 * T9 * T9);
+            Real dbdt = (84.165e0_rt * dscratchdt / (scratch * scratch) - 3.0_rt * 2.12e-3_rt * T9 * T9 * dT9dt) * b;
+
+            rates.fr = a * b;
+            rates.frdt = dadt * b + a * dbdt;
+
+            rates.rr = 0.0_rt;
+            rates.rrdt = 0.0_rt;
+        }
+    }
+
+    template<int rate>
+    AMREX_GPU_HOST_DEVICE AMREX_INLINE
+    void postprocess_rate (const rhs_state_t& state, rate_t& rates,
+                           rate_t& rates1, rate_t& rates2, rate_t& rates3)
+    {
+        // Nothing to do for this network.
+    }
+
+    template<int spec>
+    AMREX_GPU_HOST_DEVICE AMREX_INLINE
+    Real ener_gener_rate (const rhs_state_t& rhs_state, Real const& dydt)
+    {
+        // Chamulak et al. provide the q-value resulting from C12 burning,
+        // given as 3 different values (corresponding to 3 different densities).
+        // Here we do a simple quadratic fit to the 3 values provided (see
+        // Chamulak et al., p. 164, column 2).
+
+        // our convention is that the binding energies are negative.  We convert
+        // from the MeV values that are traditionally written in astrophysics
+        // papers by multiplying by 1.e6 eV/MeV * 1.60217646e-12 erg/eV.  The
+        // MeV values are per nucleus, so we divide by aion to make it per
+        // nucleon and we multiple by Avogardo's # (6.0221415e23) to get the
+        // value in erg/g
+        Real rho9 = rhs_state.rho / 1.0e9_rt;
+
+        // q_eff is effective heat evolved per reaction (given in MeV)
+        Real q_eff = 0.06e0_rt * rho9 * rho9 + 0.02e0_rt * rho9 + 8.83e0_rt;
+
+        // convert from MeV to ergs / gram.  Here 2.93 is the
+        // number of C12 nuclei destroyed in a single reaction and 12.0 is
+        // the mass of a single C12 nuclei.  Also note that our convention
+        // is that binding energies are negative.
+        Real ebin_C12 = -q_eff * C::MeV2eV * C::ev2erg * C::n_A / (2.93e0_rt * 12.0e0_rt);
+
+        if constexpr (spec == Species::C12) {
+            return dydt * NetworkProperties::aion(spec) * ebin_C12;
+        }
+        else {
+            return 0.0_rt;
+        }
+    }
+
+} // namespace RHS
+
 #endif