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-rw-r--r--vcpkg/ports/if97/relax-encoding.diff48
1 files changed, 48 insertions, 0 deletions
diff --git a/vcpkg/ports/if97/relax-encoding.diff b/vcpkg/ports/if97/relax-encoding.diff
new file mode 100644
index 0000000..e48ae2b
--- /dev/null
+++ b/vcpkg/ports/if97/relax-encoding.diff
@@ -0,0 +1,48 @@
+diff --git a/IF97.h b/IF97.h
+index 864f3a0..4e6cab5 100644
+--- a/IF97.h
++++ b/IF97.h
+@@ -52,7 +52,7 @@ namespace IF97
+ // IF97 Constants
+ const double Tcrit = 647.096; // K
+ const double Pcrit = 22.064*p_fact; // MPa*
+- const double Rhocrit = 322.0; // kg/m³
++ const double Rhocrit = 322.0; // kg/m^3
+ const double Scrit = 4.41202148223476*R_fact; // kJ*/kg-K (needed for backward eqn. in Region 3(a)(b)
+ const double Ttrip = 273.16; // K
+ const double Ptrip = 0.000611656*p_fact; // MPa*
+@@ -2394,7 +2394,7 @@ namespace IF97
+ // The equation is rearranged to solve for rho and turned
+ // into functions f(T,P,rho0) and f'(T,P,rho0) for the
+ // Newton-Raphson technique. Functions for
+- // dphi/ddelta and d²phi/ddelta² were also required. These
++ // dphi/ddelta and d^2phi/ddelta^2 were also required. These
+ // additional Taylor functions are defined above.
+ //
+ double f(double T, double p, double rho0) const{
+@@ -4172,7 +4172,7 @@ namespace IF97
+ return RegionOutput( IF97_HMASS,RegionOutputBackward(Pmax,s,IF97_SMASS),Pmax, NONE);
+ else {
+ // Determining H(s) along Tmax is difficult because there is no direct p(T,s) formulation.
+- // This linear combination fit h(s)=a*ln(s)+b/s+c/s²+d is not perfect, but it's close
++ // This linear combination fit h(s)=a*ln(s)+b/s+c/s^2+d is not perfect, but it's close
+ // and can serve as a limit along that Tmax boundary. Coefficients in HTmaxdata above.
+ // There is a better way to do this using Newton-Raphson on Tmax = T(p,s), but it is iterative and slow.
+ double ETA = Hmax_n[0]*log(sigma) + Hmax_n[1]/sigma + Hmax_n[2]/pow(sigma,2) +Hmax_n[3];
+@@ -4323,14 +4323,14 @@ namespace IF97
+ inline double cvmass_Tp(double T, double p){ return RegionOutput( IF97_CVMASS, T, p, NONE); };
+ /// Get the speed of sound [m/s] as a function of T [K] and p [Pa]
+ inline double speed_sound_Tp(double T, double p){ return RegionOutput( IF97_W, T, p, NONE); };
+- /// Get the [d(rho)/d(p)]T [kg/m³/Pa] as a function of T [K] and p [Pa]
++ /// Get the [d(rho)/d(p)]T [kg/m^3/Pa] as a function of T [K] and p [Pa]
+ inline double drhodp_Tp(double T, double p){ return RegionOutput( IF97_DRHODP, T, p, NONE); };
+
+ // ******************************************************************************** //
+ // Transport Properties //
+ // ******************************************************************************** //
+
+- /// Get the viscosity [Pa-s] as a function of T [K] and Rho [kg/m³]
++ /// Get the viscosity [Pa-s] as a function of T [K] and Rho [kg/m^3]
+ inline double visc_TRho(double T, double rho) {
+ // Since we have density, we don't need to determine the region for viscosity.
+ static Region1 R1; // All regions use base region equations for visc(T,rho).