Add C kernel for BSSN-EM (Maxwell/electromagnetic field) RHS computation
New bssn_em_rhs_c.C computes EM field RHS (E,B,Kpsi,Kphi) and stress-energy tensor, then calls the C BSSN RHS kernel with source terms. Replaces empart.f90 when USE_CXX_EM_KERNEL=1. Supports all ghost_width orders via existing derivative kernels. Controlled by USE_CXX_EM_KERNEL switch (default 0, experimental). Co-Authored-By: Claude Opus 4.7 <noreply@anthropic.com>
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@@ -32,6 +32,24 @@ $(error USE_CXX_ESCALAR_KERNEL=1 requires USE_CXX_KERNELS=1 because bssn_escalar
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endif
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endif
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ifeq ($(USE_CXX_EM_KERNEL),1)
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ifeq ($(ABE_TYPE),3)
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EFFECTIVE_USE_CXX_EM_KERNEL = 1
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else
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EFFECTIVE_USE_CXX_EM_KERNEL = 0
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endif
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else
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EFFECTIVE_USE_CXX_EM_KERNEL = 0
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endif
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ifeq ($(EFFECTIVE_USE_CXX_EM_KERNEL),1)
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ifeq ($(USE_CXX_KERNELS),0)
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$(error USE_CXX_EM_KERNEL=1 requires USE_CXX_KERNELS=1 because bssn_em_rhs_c.C reuses the C BSSN kernel)
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endif
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endif
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EM_KERNEL_FLAG = -DBSSN_USE_EM_C_KERNEL=$(EFFECTIVE_USE_CXX_EM_KERNEL)
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## polint(ordn=6) kernel selector:
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## 1 (default): barycentric fast path
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## 0 : fallback to Neville path
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@@ -102,6 +120,9 @@ fdderivs_shc_c.o: fdderivs_shc_c.C
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kodiss_sh_c.o: kodiss_sh_c.C
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${CXX} $(CXXAPPFLAGS) -c $< $(filein) -o $@
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bssn_em_rhs_c.o: bssn_em_rhs_c.C
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${CXX} $(CXXAPPFLAGS) -c $< $(filein) -o $@
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z4c_rhs_c.o: z4c_rhs_c.C
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${CXX} $(CXXAPPFLAGS) -c $< $(filein) -o $@
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@@ -112,7 +133,7 @@ z4c_rhs_c.o: z4c_rhs_c.C
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TP_PROFDATA = /home/$(shell whoami)/AMSS-NCKU/pgo_profile/TwoPunctureABE.profdata
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TP_OPTFLAGS = -O3 -xHost -fp-model fast=2 -fma -ipo \
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-fprofile-instr-use=$(TP_PROFDATA) \
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-Dfortran3 -Dnewc -I$(OMPI_ROOT)/include
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-Dfortran3 -Dnewc $(filein_real)
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TwoPunctures.o: TwoPunctures.C
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${CXX} $(TP_OPTFLAGS) -qopenmp -c $< -o $@
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@@ -132,6 +153,9 @@ CFILES = bssn_rhs_c.o fderivs_c.o fdderivs_c.o kodiss_c.o lopsided_c.o lopsided_
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ifeq ($(EFFECTIVE_USE_CXX_ESCALAR_KERNEL),1)
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CFILES += bssn_escalar_rhs_c.o
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endif
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ifeq ($(EFFECTIVE_USE_CXX_EM_KERNEL),1)
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CFILES += bssn_em_rhs_c.o
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endif
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endif
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ifeq ($(USE_CXX_Z4C_KERNELS),1)
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