subsurface/core/gas-model.c
Berthold Stoeger 2a966ac2a9 Cleanup: replace macro by inline function in gas-model.c
Replace a macro calculating a degree-three polynomial by an
inline function.

Moreover, calculate the powers 1, 2 and 3 of the pressure inside
the function. The compiler will be smart enough to optimize this
to the same code. The only important thing is to write "x*x*x*coeff"
instead of "coeff*x*x*x". The compiler can't optimize the latter
because ... wonderful floating point semantics.

Signed-off-by: Berthold Stoeger <bstoeger@mail.tuwien.ac.at>
2019-08-08 15:22:09 -07:00

92 lines
2.6 KiB
C
Raw Blame History

This file contains ambiguous Unicode characters

This file contains Unicode characters that might be confused with other characters. If you think that this is intentional, you can safely ignore this warning. Use the Escape button to reveal them.

// SPDX-License-Identifier: GPL-2.0
/* gas-model.c */
/* gas compressibility model */
#include <stdio.h>
#include <stdlib.h>
#include "dive.h"
/* "Virial minus one" - the virial cubic form without the initial 1.0 */
static double virial_m1(const double coeff[], double x)
{
return x*coeff[0] + x*x*coeff[1] + x*x*x*coeff[2];
}
/*
* Z = pV/nRT
*
* Cubic virial least-square coefficients for O2/N2/He based on data from
*
* PERRYS CHEMICAL ENGINEERS HANDBOOK SEVENTH EDITION
*
* with the lookup and curve fitting by Lubomir.
*
* The "virial" form of the compression factor polynomial is
*
* Z = 1.0 + C[0]*P + C[1]*P^2 + C[2]*P^3 ...
*
* and these tables do not contain the initial 1.0 term.
*
* NOTE! Helium coefficients are a linear mix operation between the
* 323K and one for 273K isotherms, to make everything be at 300K.
*/
double gas_compressibility_factor(struct gasmix gas, double bar)
{
static const double o2_coefficients[3] = {
-7.18092073703e-04,
+2.81852572808e-06,
-1.50290620492e-09
};
static const double n2_coefficients[3] = {
-2.19260353292e-04,
+2.92844845532e-06,
-2.07613482075e-09
};
static const double he_coefficients[3] = {
+4.87320026468e-04,
-8.83632921053e-08,
+5.33304543646e-11
};
int o2, he;
double Z;
/*
* The curve fitting range is only [0,500] bar.
* Anything else is way out of range for cylinder
* pressures.
*/
if (bar < 0) bar = 0;
if (bar > 500) bar = 500;
o2 = get_o2(gas);
he = get_he(gas);
Z = virial_m1(o2_coefficients, bar) * o2 +
virial_m1(he_coefficients, bar) * he +
virial_m1(n2_coefficients, bar) * (1000 - o2 - he);
/*
* We add the 1.0 at the very end - the linear mixing of the
* three 1.0 terms is still 1.0 regardless of the gas mix.
*
* The * 0.001 is because we did the linear mixing using the
* raw permille gas values.
*/
return Z * 0.001 + 1.0;
}
/* Compute the new pressure when compressing (expanding) volome v1 at pressure p1 bar to volume v2
* taking into account the compressebility (to first order) */
double isothermal_pressure(struct gasmix gas, double p1, int volume1, int volume2)
{
double p_ideal = p1 * volume1 / volume2 / gas_compressibility_factor(gas, p1);
return p_ideal * gas_compressibility_factor(gas, p_ideal);
}
double gas_density(struct gasmix gas, int pressure)
{
int density = gas.he.permille * HE_DENSITY + gas.o2.permille * O2_DENSITY + (1000 - gas.he.permille - gas.o2.permille) * N2_DENSITY;
return density * (double) pressure / gas_compressibility_factor(gas, pressure / 1000.0) / SURFACE_PRESSURE / 1000000.0;
}