426 lines
22 KiB
JavaScript
426 lines
22 KiB
JavaScript
// ════════════════════════════════════════════════════════════════════════
|
||
// physics.js — Physical constants and meteorological calculations.
|
||
//
|
||
// Exports:
|
||
// SIGMA, EPSILON_P, A_K, ALBEDO_GRASS (radiation constants)
|
||
// vaporPressureHpa(Ta, RH) Magnus formula → hPa
|
||
// solarElevationDeg(lat, lon, dateUTC) NOAA simplified solar position
|
||
// calcTmrt(Ta, dirRad, diffRad, globalRad, solElev) Mean radiant temp
|
||
// utciApprox(Ta, Tmrt, va10, ehPa) Bröde et al. 2012 polynomial
|
||
//
|
||
// Nothing in here should need editing unless the underlying science
|
||
// changes. All numbers are peer-reviewed constants or coefficients.
|
||
// ════════════════════════════════════════════════════════════════════════
|
||
|
||
// ═══════════════════════════════════════════════════════════════════
|
||
// PHYSICAL CONSTANTS
|
||
// ───────────────────────────────────────────────────────────────────
|
||
// These are real-world physics values — don't change them unless you
|
||
// have a peer-reviewed reason. They're used by calcTmrt() below to
|
||
// work out how much heat your skin actually absorbs from the sun.
|
||
// SIGMA — Stefan–Boltzmann constant (radiates heat)
|
||
// EPSILON_P — emissivity of human skin (~0.97)
|
||
// A_K — short-wave absorption coefficient for clothing
|
||
// ALBEDO_GRASS — how much sun grass reflects back at you (23%)
|
||
// ALBEDO_CONCRETE — how much sun concrete reflects back (30%)
|
||
// Concrete absorbs more net solar than grass and has
|
||
// no evaporative cooling, so its surface runs hot.
|
||
// ═══════════════════════════════════════════════════════════════════
|
||
export const SIGMA = 5.670374419e-8;
|
||
export const EPSILON_P = 0.97;
|
||
export const A_K = 0.7;
|
||
export const ALBEDO_GRASS = 0.23;
|
||
export const ALBEDO_CONCRETE = 0.30;
|
||
|
||
// ═══════════════════════════════════════════════════════════════════
|
||
// CONCRETE SURFACE TEMPERATURE (Urban profile)
|
||
// ───────────────────────────────────────────────────────────────────
|
||
// Estimates the surface temperature of exposed concrete using a
|
||
// simplified energy-balance approach:
|
||
// • Absorbed solar = globalRad × (1 − albedo)
|
||
// • No latent heat (no evaporation — concrete is dry)
|
||
// • Convective loss to air proportional to wind speed
|
||
// • Result is clamped to a physically plausible range
|
||
//
|
||
// This is what matters for contact heat stress in cities — the UTCI
|
||
// standard uses grass, which runs ~5–15 °C cooler than urban concrete
|
||
// on a sunny day because grass sweats (transpires).
|
||
// ═══════════════════════════════════════════════════════════════════
|
||
export function calcConcreteTemp(Ta, globalRad, windSpeed) {
|
||
if (globalRad == null || Ta == null) return null;
|
||
const absorbed = globalRad * (1 - ALBEDO_CONCRETE); // W/m²
|
||
// Convective heat transfer coefficient: ~5 W/m²K still air, rises with wind
|
||
const hc = 5 + 4.5 * Math.sqrt(Math.max(windSpeed || 0, 0));
|
||
// Surface temp: Ta + solar gain / convective loss
|
||
const Ts = Ta + absorbed / hc;
|
||
// Clamp: can't be cooler than air, cap at 85 °C (melting asphalt territory)
|
||
return Math.max(Ta, Math.min(Ts, 85));
|
||
}
|
||
|
||
// ═══════════════════════════════════════════════════════════════════
|
||
// UK HOUSE INDOOR TEMPERATURE (windows closed, no active cooling)
|
||
// ───────────────────────────────────────────────────────────────────
|
||
// Estimates the ambient indoor air temperature of a typical UK brick
|
||
// house with windows closed and no air conditioning.
|
||
//
|
||
// Two heat pathways are modelled:
|
||
//
|
||
// 1. WALL CONDUCTION
|
||
// Heat conducts through brick cavity walls and roof. UK Part L
|
||
// compliant walls have a U-value around 0.28–0.45 W/m²K; older
|
||
// solid-brick stock runs higher. A representative mid-stock value
|
||
// is used. This drives a slow, steady heat transfer proportional
|
||
// to the difference between outdoor and indoor air temperature.
|
||
//
|
||
// 2. WINDOW SOLAR GAIN
|
||
// A typical UK semi has ~15–18% glazing ratio. Solar energy
|
||
// transmits through glass, is absorbed by floors and furniture,
|
||
// and heats the indoor air. Gain is averaged across orientations
|
||
// (not all windows face south). Diffuse radiation contributes
|
||
// regardless of sun angle.
|
||
//
|
||
// THERMAL LAG
|
||
// Brick and concrete have high thermal mass — the house responds
|
||
// slowly to outdoor temperature swings. This function takes a
|
||
// weighted average of the current hour's heat load and the
|
||
// previous few hours', giving the characteristic lag where indoor
|
||
// temperature peaks 2–4 hours after the outdoor peak.
|
||
// Call calcIndoorTempPass() on the full hourly arrays after
|
||
// building rows — it returns a per-hour indoor temp array.
|
||
//
|
||
// No mechanical cooling. Minimal infiltration (windows closed).
|
||
// Internal heat gains (people, appliances) are not modelled.
|
||
//
|
||
// Colour thresholds:
|
||
// < 20 °C — cool, may need heating
|
||
// 20–26 °C — comfortable
|
||
// 26–32 °C — warm; WHO heatwave advisory threshold for sleeping
|
||
// > 32 °C — hot; risk for elderly and vulnerable occupants
|
||
// ═══════════════════════════════════════════════════════════════════
|
||
|
||
// Single-hour instantaneous heat load (W/m² effective, indoor side).
|
||
// Used internally by calcIndoorTempPass — not exported.
|
||
function _houseHeatLoad(Ta, globalRad, solElev) {
|
||
// Wall + roof conduction: U-value ~0.35 W/m²K × effective envelope area ratio
|
||
// We express as a gain-per-degree-delta — applied against Ti later in the pass.
|
||
// (See calcIndoorTempPass for how this feeds the lag model.)
|
||
|
||
// Window solar gain: glazing ratio 0.16, g-value 0.63 (standard double glazing),
|
||
// averaged across orientations (0.5 factor — not all windows face the sun).
|
||
const glazingRatio = 0.16;
|
||
const gValue = 0.63;
|
||
const orientFactor = 0.50;
|
||
const solarGain = globalRad * glazingRatio * gValue * orientFactor;
|
||
|
||
return { conductionDelta: Ta, solarGain };
|
||
}
|
||
|
||
// Two-pass function: call with the full arrays of hourly Ta and globalRad.
|
||
// Returns an array of indoor temperatures, one per hour.
|
||
export function calcIndoorTempPass(TaArr, globArr, elevArr) {
|
||
const n = TaArr.length;
|
||
const result = new Array(n);
|
||
|
||
// Thermal resistance of the building envelope (°C per W/m² of heat load)
|
||
// Lower = faster response to outdoor changes. UK brick mid-stock ~0.45.
|
||
const uWall = 0.35; // W/m²K effective wall U-value
|
||
// Thermal mass time constant: heavier = longer lag.
|
||
// ~4 h lag for typical UK brick semi (expressed as exponential decay weight).
|
||
const lagHours = 4;
|
||
const alpha = 1 - Math.exp(-1 / lagHours); // per-hour blending weight
|
||
|
||
// Seed indoor temp to first outdoor temp
|
||
let Ti = TaArr[0] ?? 15;
|
||
|
||
for (let i = 0; i < n; i++) {
|
||
const Ta = TaArr[i] ?? Ti;
|
||
const glob = globArr[i] ?? 0;
|
||
const solElev = elevArr[i] ?? 0;
|
||
|
||
// Solar gain through windows (W/m² effective)
|
||
const glazingRatio = 0.16;
|
||
const gValue = 0.63;
|
||
const orientFactor = 0.50;
|
||
const solarGain = glob * glazingRatio * gValue * orientFactor;
|
||
|
||
// Conductive heat flow through walls: proportional to (Ta - Ti)
|
||
// uWall drives how quickly the indoor temp chases outdoor temp.
|
||
const conductionGain = uWall * (Ta - Ti);
|
||
|
||
// Target indoor temp this hour if there were no thermal mass:
|
||
// Ti_instant = Ti + conduction + solar load / heat capacity proxy
|
||
// heatCap proxy: how many degrees does 1 W/m² raise the indoor air?
|
||
// For a typical 90 m² house, ~0.15 °C per W/m² effective.
|
||
const heatCapProxy = 0.15;
|
||
const Ti_instant = Ti + (conductionGain + solarGain) * heatCapProxy;
|
||
|
||
// Apply thermal lag: blend toward Ti_instant slowly
|
||
Ti = Ti + alpha * (Ti_instant - Ti);
|
||
|
||
// Can't be colder than outdoor (house doesn't actively cool)
|
||
// Cap at 55 °C (physically implausible above this for a house interior)
|
||
result[i] = Math.max(Math.min(Ti, 55), Math.min(Ta, Ti));
|
||
}
|
||
|
||
return result;
|
||
}
|
||
|
||
// ═══════════════════════════════════════════════════════════════════
|
||
// VEHICLE INTERIOR CABIN TEMPERATURE (seated occupant, not in sunbeam)
|
||
// ───────────────────────────────────────────────────────────────────
|
||
// Models the ambient cabin air temperature experienced by an occupant
|
||
// seated out of direct sunlight inside a sealed, parked vehicle.
|
||
// Two heat sources are combined:
|
||
//
|
||
// 1. PANEL CONDUCTION
|
||
// Aluminium body panels absorb solar radiation and conduct heat
|
||
// into the cabin. Albedo ~0.25 (mid-point for typical mixed-colour
|
||
// fleet; dark paint ~0.10, silver/white ~0.40).
|
||
// Panel surface temp → conductive gain into cabin air.
|
||
//
|
||
// 2. SIDE-WINDOW GLAZING GAIN (sun-angle dependent)
|
||
// When solar elevation is between ~10° and ~60°, the sun's rays
|
||
// cut through the side glass at an angle that allows significant
|
||
// transmission into the cabin (rather than hitting the roof or
|
||
// reflecting off at a shallow angle). This warms the cabin air
|
||
// but the occupant is modelled as NOT sitting in the beam —
|
||
// so it adds to ambient cabin temp, not direct radiant load.
|
||
// Above 60° the sun mostly hits the roof; below 10° it reflects.
|
||
//
|
||
// Wind is ignored (vehicle is sealed). No evaporative cooling.
|
||
// Steady-state reached after ~45–60 min of parking.
|
||
//
|
||
// Colour thresholds in the table:
|
||
// < 35 °C — warm but tolerable for short periods
|
||
// 35–45 °C — dangerous for children/pets (hyperthermia risk)
|
||
// > 45 °C — potentially fatal within minutes
|
||
// ═══════════════════════════════════════════════════════════════════
|
||
export function calcVehicleInteriorTemp(Ta, globalRad, solElev) {
|
||
if (globalRad == null || Ta == null) return null;
|
||
|
||
// ── 1. Panel conduction ──────────────────────────────────────────
|
||
const albedoPanel = 0.25; // typical mixed fleet
|
||
const panelAbsorbed = globalRad * (1 - albedoPanel); // W/m² absorbed by bodywork
|
||
// Panel surface temp: absorbed solar / convective loss to outside air
|
||
// hOut ~10 W/m²K (light breeze over panel surface even when parked)
|
||
const hOut = 10;
|
||
const panelSurfaceTemp = Ta + panelAbsorbed / hOut;
|
||
// Conductive gain into cabin: panel-to-cabin air, ~4 W/m²K through metal + trim
|
||
const hCabin = 4;
|
||
const conductionGain = hCabin * (panelSurfaceTemp - Ta); // W/m²
|
||
|
||
// ── 2. Side-window glazing gain (angle-dependent) ─────────────────
|
||
// Glazing transmission for auto glass ~0.70
|
||
const tau = 0.70;
|
||
let glazingGain = 0;
|
||
if (solElev != null && solElev > 10 && solElev < 60) {
|
||
// Scale factor: peaks around 30–40° elevation (sun cuts squarely
|
||
// through side glass), tapers off toward 10° (shallow/reflected)
|
||
// and 60° (sun increasingly hitting roof not side glass).
|
||
// Use a simple tent function peaking at 35°.
|
||
const peak = 35;
|
||
const halfWidth = 25; // degrees either side
|
||
const factor = Math.max(0, 1 - Math.abs(solElev - peak) / halfWidth);
|
||
// Diffuse radiation also enters through glass regardless of angle
|
||
glazingGain = tau * globalRad * factor * 0.5; // occupant not in beam → 50% ambient
|
||
} else {
|
||
// Outside the side-window zone: diffuse only (scattered sky light)
|
||
glazingGain = tau * (globalRad * 0.15); // ~15% diffuse fraction
|
||
}
|
||
|
||
// ── Combine into cabin air temperature ───────────────────────────
|
||
// Total heat input per m² of cabin surface
|
||
const totalGain = conductionGain + glazingGain;
|
||
// Cabin heat loss: poor natural ventilation in sealed car ~2.0 W/m²K
|
||
const hCabinLoss = 2.0;
|
||
const Ti = Ta + totalGain / hCabinLoss;
|
||
|
||
// Clamp: can't be cooler than outside air; physical cap at 90 °C
|
||
return Math.max(Ta, Math.min(Ti, 90));
|
||
}
|
||
|
||
// Vapour pressure (Magnus → hPa)
|
||
export function vaporPressureHpa(Ta, RH) {
|
||
const es = 6.105 * Math.exp((17.27 * Ta) / (237.7 + Ta));
|
||
return es * (RH / 100);
|
||
}
|
||
|
||
// Solar elevation (NOAA simplified, degrees)
|
||
export function solarElevationDeg(lat, lon, dateUTC) {
|
||
const start = Date.UTC(dateUTC.getUTCFullYear(), 0, 0);
|
||
const diff = dateUTC - start;
|
||
const DOY = Math.floor(diff / 86400000);
|
||
const hourUTC =
|
||
dateUTC.getUTCHours() +
|
||
dateUTC.getUTCMinutes() / 60 +
|
||
dateUTC.getUTCSeconds() / 3600;
|
||
const gamma = ((2 * Math.PI) / 365) * (DOY - 1 + (hourUTC - 12) / 24);
|
||
const eqtime =
|
||
229.18 *
|
||
(0.000075 +
|
||
0.001868 * Math.cos(gamma) -
|
||
0.032077 * Math.sin(gamma) -
|
||
0.014615 * Math.cos(2 * gamma) -
|
||
0.040849 * Math.sin(2 * gamma));
|
||
const decl =
|
||
0.006918 -
|
||
0.399912 * Math.cos(gamma) +
|
||
0.070257 * Math.sin(gamma) -
|
||
0.006758 * Math.cos(2 * gamma) +
|
||
0.000907 * Math.sin(2 * gamma) -
|
||
0.002697 * Math.cos(3 * gamma) +
|
||
0.00148 * Math.sin(3 * gamma);
|
||
const timeOffset = eqtime + 4 * lon;
|
||
const tst = hourUTC * 60 + timeOffset;
|
||
const ha = (((tst / 4) - 180) * Math.PI) / 180;
|
||
const latRad = (lat * Math.PI) / 180;
|
||
const cosZenith =
|
||
Math.sin(latRad) * Math.sin(decl) +
|
||
Math.cos(latRad) * Math.cos(decl) * Math.cos(ha);
|
||
const zenith = Math.acos(Math.max(-1, Math.min(1, cosZenith)));
|
||
return (Math.PI / 2 - zenith) * (180 / Math.PI);
|
||
}
|
||
|
||
// Mean radiant temperature
|
||
export function calcTmrt(Ta, dirRad, diffRad, globalRad, solElev) {
|
||
const TaK = Ta + 273.15;
|
||
let fp = 0;
|
||
if (solElev > 0) {
|
||
const h2 = solElev;
|
||
fp = 0.308 * Math.cos((Math.PI / 180) * h2 * (0.998 - (h2 * h2) / 50000));
|
||
}
|
||
let DNI = 0;
|
||
if (solElev > 1) {
|
||
DNI = dirRad / Math.sin((solElev * Math.PI) / 180);
|
||
DNI = Math.min(DNI, 1100);
|
||
}
|
||
const Sshort = A_K * (fp * DNI + 0.5 * diffRad + 0.5 * ALBEDO_GRASS * globalRad);
|
||
const Slong = EPSILON_P * SIGMA * Math.pow(TaK, 4);
|
||
const TmrtK = Math.pow((Sshort + Slong) / (EPSILON_P * SIGMA), 0.25);
|
||
return TmrtK - 273.15;
|
||
}
|
||
|
||
// ═══════════════════════════════════════════════════════════════════
|
||
// UTCI POLYNOMIAL — DO NOT EDIT (or be VERY careful if you do)
|
||
// ───────────────────────────────────────────────────────────────────
|
||
// This is the official 210-term Bröde et al. (2012) approximation.
|
||
// It takes air temp, mean radiant temp, wind, and humidity and returns
|
||
// the "felt" temperature. Every number is a peer-reviewed coefficient.
|
||
// Scroll past it — there's nothing here you'll want to change.
|
||
// ═══════════════════════════════════════════════════════════════════
|
||
export function utciApprox(Ta, Tmrt, va10, ehPa) {
|
||
const va = Math.max(0.5, Math.min(17, va10));
|
||
const D_Tmrt = Tmrt - Ta;
|
||
const Pa = ehPa / 10;
|
||
const T = Ta, V = va, D = D_Tmrt, P = Pa;
|
||
const T2=T*T, T3=T2*T, T4=T3*T, T5=T4*T, T6=T5*T;
|
||
const V2=V*V, V3=V2*V, V4=V3*V, V5=V4*V, V6=V5*V;
|
||
const D2=D*D, D3=D2*D, D4=D3*D, D5=D4*D, D6=D5*D;
|
||
const P2=P*P, P3=P2*P, P4=P3*P, P5=P4*P, P6=P5*P;
|
||
return T +
|
||
6.07562052e-1 +
|
||
-2.27712343e-2 * T + 8.06470249e-4 * T2 + -1.54271372e-4 * T3 +
|
||
-3.24651735e-6 * T4 + 7.32602852e-8 * T5 + 1.35959073e-9 * T6 +
|
||
-2.25836520e0 * V + 8.80326035e-2 * T*V + 2.16844454e-3 * T2*V +
|
||
-1.53347087e-5 * T3*V + -5.72983704e-7 * T4*V + -2.55090145e-9 * T5*V +
|
||
-7.51269505e-1 * V2 + -4.08350271e-3 * T*V2 + -5.21670675e-5 * T2*V2 +
|
||
1.94544667e-6 * T3*V2 + 1.14099531e-8 * T4*V2 +
|
||
1.58137256e-1 * V3 + -6.57263143e-5 * T*V3 + 2.22697524e-7 * T2*V3 +
|
||
-4.16117031e-8 * T3*V3 +
|
||
-1.27762753e-2 * V4 + 9.66891875e-6 * T*V4 + 2.52785852e-9 * T2*V4 +
|
||
4.56306672e-4 * V5 + -1.74202546e-7 * T*V5 +
|
||
-5.91491269e-6 * V6 +
|
||
3.98374029e-1 * D + 1.83945314e-4 * T*D + -1.73754510e-4 * T2*D +
|
||
-7.60781159e-7 * T3*D + 3.77830287e-8 * T4*D + 5.43079673e-10 * T5*D +
|
||
-2.00518269e-2 * V*D + 8.92859837e-4 * T*V*D + 3.45433048e-6 * T2*V*D +
|
||
-3.77925774e-7 * T3*V*D + -1.69699377e-9 * T4*V*D +
|
||
1.69992415e-4 * V2*D + -4.99204314e-5 * T*V2*D + 2.47417178e-7 * T2*V2*D +
|
||
1.07596466e-8 * T3*V2*D +
|
||
8.49242932e-5 * V3*D + 1.35191328e-6 * T*V3*D + -6.21531254e-9 * T2*V3*D +
|
||
-4.99410301e-6 * V4*D + -1.89489258e-8 * T*V4*D +
|
||
8.15300114e-8 * V5*D +
|
||
7.55043090e-4 * D2 + -5.65095215e-5 * T*D2 + -4.52166564e-7 * T2*D2 +
|
||
2.46688878e-8 * T3*D2 + 2.42674348e-10 * T4*D2 +
|
||
1.54547250e-4 * V*D2 + 5.24110970e-6 * T*V*D2 + -8.75874982e-8 * T2*V*D2 +
|
||
-1.50743064e-9 * T3*V*D2 +
|
||
-1.56236307e-5 * V2*D2 + -1.33895614e-7 * T*V2*D2 + 2.49709824e-9 * T2*V2*D2 +
|
||
6.51711721e-7 * V3*D2 + 1.94960053e-9 * T*V3*D2 +
|
||
-1.00361113e-8 * V4*D2 +
|
||
-1.21206673e-5 * D3 + -2.18203660e-7 * T*D3 + 7.51269482e-9 * T2*D3 +
|
||
9.79063848e-11 * T3*D3 +
|
||
1.25006734e-6 * V*D3 + -1.81584736e-9 * T*V*D3 + -3.52197671e-10 * T2*V*D3 +
|
||
-3.36514630e-8 * V2*D3 + 1.35908359e-10 * T*V2*D3 +
|
||
4.17032620e-10 * V3*D3 +
|
||
-1.30369025e-9 * D4 + 4.13908461e-10 * T*D4 + 9.22652254e-12 * T2*D4 +
|
||
-5.08220384e-9 * V*D4 + -2.24730961e-11 * T*V*D4 +
|
||
1.17139133e-10 * V2*D4 +
|
||
6.62154879e-10 * D5 + 4.03863260e-13 * T*D5 + 1.95087203e-12 * V*D5 +
|
||
-4.73602469e-12 * D6 +
|
||
5.12733497e0 * P + -3.12788561e-1 * T*P + -1.96701861e-2 * T2*P +
|
||
9.99690870e-4 * T3*P + 9.51738512e-6 * T4*P + -4.66426341e-7 * T5*P +
|
||
5.48050612e-1 * V*P + -3.30552823e-3 * T*V*P + -1.64119440e-3 * T2*V*P +
|
||
-5.16670694e-6 * T3*V*P + 9.52692432e-7 * T4*V*P +
|
||
-4.29223622e-2 * V2*P + 5.00845667e-3 * T*V2*P + 1.00601257e-6 * T2*V2*P +
|
||
-1.81748644e-6 * T3*V2*P +
|
||
-1.25813502e-3 * V3*P + -1.79330391e-4 * T*V3*P + 2.34994441e-6 * T2*V3*P +
|
||
1.29735808e-4 * V4*P + 1.29064870e-6 * T*V4*P +
|
||
-2.28558686e-6 * V5*P +
|
||
-3.69476348e-2 * D*P + 1.62325322e-3 * T*D*P + -3.14279680e-5 * T2*D*P +
|
||
2.59835559e-6 * T3*D*P + -4.77136523e-8 * T4*D*P +
|
||
8.64203390e-3 * V*D*P + -6.87405181e-4 * T*V*D*P + -9.13863872e-6 * T2*V*D*P +
|
||
5.15916806e-7 * T3*V*D*P +
|
||
-3.59217476e-5 * V2*D*P + 3.28696511e-5 * T*V2*D*P + -7.10542454e-7 * T2*V2*D*P +
|
||
-1.24382300e-5 * V3*D*P + -7.38584400e-9 * T*V3*D*P +
|
||
2.20609296e-7 * V4*D*P +
|
||
-7.32469180e-4 * D2*P + -1.87381964e-5 * T*D2*P + 4.80925239e-6 * T2*D2*P +
|
||
-8.75492040e-8 * T3*D2*P +
|
||
2.77862930e-5 * V*D2*P + -5.06004592e-6 * T*V*D2*P + 1.14325367e-7 * T2*V*D2*P +
|
||
2.53016723e-6 * V2*D2*P + -1.72857035e-8 * T*V2*D2*P +
|
||
-3.95079398e-8 * V3*D2*P +
|
||
-3.59413173e-7 * D3*P + 7.04388046e-7 * T*D3*P + -1.89309167e-8 * T2*D3*P +
|
||
-4.79768731e-7 * V*D3*P + 7.96079978e-9 * T*V*D3*P +
|
||
1.62897058e-9 * V2*D3*P +
|
||
3.94367674e-8 * D4*P + -1.18566247e-9 * T*D4*P +
|
||
3.34678041e-10 * V*D4*P +
|
||
-1.15606447e-10 * D5*P +
|
||
-2.80626406e0 * P2 + 5.48712484e-1 * T*P2 + -3.99428410e-3 * T2*P2 +
|
||
-9.54009191e-4 * T3*P2 + 1.93090978e-5 * T4*P2 +
|
||
-3.08806365e-1 * V*P2 + 1.16952364e-2 * T*V*P2 + 4.95271903e-4 * T2*V*P2 +
|
||
-1.90710882e-5 * T3*V*P2 +
|
||
2.10787756e-3 * V2*P2 + -6.98445738e-4 * T*V2*P2 + 2.30109073e-5 * T2*V2*P2 +
|
||
4.17856590e-4 * V3*P2 + -1.27043871e-5 * T*V3*P2 +
|
||
-3.04620472e-6 * V4*P2 +
|
||
5.14507424e-2 * D*P2 + -4.32510997e-3 * T*D*P2 + 8.99281156e-5 * T2*D*P2 +
|
||
-7.14663943e-7 * T3*D*P2 +
|
||
-2.66016305e-4 * V*D*P2 + 2.63789586e-4 * T*V*D*P2 + -7.01199003e-6 * T2*V*D*P2 +
|
||
-1.06823306e-4 * V2*D*P2 + 3.61341136e-6 * T*V2*D*P2 +
|
||
2.29748967e-7 * V3*D*P2 +
|
||
3.04788893e-4 * D2*P2 + -6.42070836e-5 * T*D2*P2 + 1.16257971e-6 * T2*D2*P2 +
|
||
7.68023384e-6 * V*D2*P2 + -5.47446896e-7 * T*V*D2*P2 +
|
||
-3.59937910e-8 * V2*D2*P2 +
|
||
-4.36497725e-6 * D3*P2 + 1.68737969e-7 * T*D3*P2 +
|
||
2.67489271e-8 * V*D3*P2 +
|
||
3.23926897e-9 * D4*P2 +
|
||
-3.53874123e-2 * P3 + -2.21201190e-1 * T*P3 + 1.55126038e-2 * T2*P3 +
|
||
-2.63917279e-4 * T3*P3 +
|
||
4.53433455e-2 * V*P3 + -4.32943862e-3 * T*V*P3 + 1.45389826e-4 * T2*V*P3 +
|
||
2.17508610e-4 * V2*P3 + -6.66724702e-5 * T*V2*P3 +
|
||
3.33217140e-5 * V3*P3 +
|
||
-2.26921615e-3 * D*P3 + 3.80261982e-4 * T*D*P3 + -5.45314314e-9 * T2*D*P3 +
|
||
-7.96355448e-4 * V*D*P3 + 2.53458034e-5 * T*V*D*P3 +
|
||
-6.31223658e-6 * V2*D*P3 +
|
||
3.02122035e-4 * D2*P3 + -4.77403547e-6 * T*D2*P3 +
|
||
1.73825715e-6 * V*D2*P3 +
|
||
-4.09087898e-7 * D3*P3 +
|
||
6.14155345e-1 * P4 + -6.16755931e-2 * T*P4 + 1.33374846e-3 * T2*P4 +
|
||
3.55375387e-3 * V*P4 + -5.13027851e-4 * T*V*P4 +
|
||
1.02449757e-4 * V2*P4 +
|
||
-1.48526421e-3 * D*P4 + -4.11469183e-5 * T*D*P4 +
|
||
-6.80434415e-6 * V*D*P4 +
|
||
-9.77675906e-6 * D2*P4 +
|
||
8.82773108e-2 * P5 + -3.01859306e-3 * T*P5 +
|
||
1.04452989e-3 * V*P5 +
|
||
2.47090539e-4 * D*P5 +
|
||
1.48348065e-3 * P6;
|
||
}
|