Note
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Symmetric premixed twin flame#
Simulate two counter-flow jets of reactants shooting into each other. This simulation differs from the similar premixed_counterflow_flame.py example as the latter simulates a jet of reactants shooting into products.
Requires: cantera >= 3.0
import sys
from pathlib import Path
import numpy as np
import cantera as ct
# Differentiation function for data that has variable grid spacing Used here to
# compute normal strain-rate
def derivative(x, y):
dydx = np.zeros(y.shape, y.dtype.type)
dx = np.diff(x)
dy = np.diff(y)
dydx[0:-1] = dy/dx
dydx[-1] = (y[-1] - y[-2])/(x[-1] - x[-2])
return dydx
def computeStrainRates(oppFlame):
# Compute the derivative of axial velocity to obtain normal strain rate
strainRates = derivative(oppFlame.grid, oppFlame.velocity)
# Obtain the location of the max. strain rate upstream of the pre-heat zone.
# This is the characteristic strain rate
maxStrLocation = abs(strainRates).argmax()
minVelocityPoint = oppFlame.velocity[:maxStrLocation].argmin()
# Characteristic Strain Rate = K
strainRatePoint = abs(strainRates[:minVelocityPoint]).argmax()
K = abs(strainRates[strainRatePoint])
return strainRates, strainRatePoint, K
def computeConsumptionSpeed(oppFlame):
Tb = max(oppFlame.T)
Tu = min(oppFlame.T)
rho_u = max(oppFlame.density)
integrand = oppFlame.heat_release_rate/oppFlame.cp
total_heat_release = np.trapz(integrand, oppFlame.grid)
Sc = total_heat_release/(Tb - Tu)/rho_u
return Sc
# This function is called to run the solver
def solveOpposedFlame(oppFlame, massFlux=0.12, loglevel=1,
ratio=2, slope=0.3, curve=0.3, prune=0.05):
"""
Execute this function to run the Opposed Flow Simulation This function
takes a CounterFlowTwinPremixedFlame object as the first argument
"""
oppFlame.reactants.mdot = massFlux
oppFlame.set_refine_criteria(ratio=ratio, slope=slope, curve=curve, prune=prune)
oppFlame.show()
oppFlame.solve(loglevel, auto=True)
# Compute the strain rate, just before the flame. This is not necessarily
# the maximum We use the max. strain rate just upstream of the pre-heat zone
# as this is the strain rate that computations compare against, like when
# plotting Su vs. K
strainRates, strainRatePoint, K = computeStrainRates(oppFlame)
return np.max(oppFlame.T), K, strainRatePoint
# Select the reaction mechanism
gas = ct.Solution('gri30.yaml')
# Create a CH4/Air premixed mixture with equivalence ratio=0.75, and at room
# temperature and pressure.
gas.set_equivalence_ratio(0.75, 'CH4', {'O2': 1.0, 'N2': 3.76})
gas.TP = 300, ct.one_atm
# Set the velocity
axial_velocity = 2.0 # in m/s
# Domain half-width of 2.5 cm, meaning the whole domain is 5 cm wide
width = 0.025
# Done with initial conditions
# Compute the mass flux, as this is what the Flame object requires
massFlux = gas.density * axial_velocity # units kg/m2/s
# Create the flame object
oppFlame = ct.CounterflowTwinPremixedFlame(gas, width=width)
# Uncomment the following line to use a Multi-component formulation. Default is
# mixture-averaged
# oppFlame.transport_model = 'multicomponent'
# Now run the solver. The solver returns the peak temperature, strain rate and
# the point which we ascribe to the characteristic strain rate.
(T, K, strainRatePoint) = solveOpposedFlame(oppFlame, massFlux, loglevel=1)
# You can plot/see all state space variables by calling oppFlame.foo where foo
# is T, Y[i], etc. The spatial variable (distance in meters) is in oppFlame.grid
# Thus to plot temperature vs distance, use oppFlame.grid and oppFlame.T
Sc = computeConsumptionSpeed(oppFlame)
if "native" in ct.hdf_support():
output = Path() / "premixed_counterflow_twin_flame.h5"
else:
output = Path() / "premixed_counterflow_twin_flame.yaml"
output.unlink(missing_ok=True)
oppFlame.save(output, name="mix")
print(f"Peak temperature: {T:.1f} K")
print(f"Strain Rate: {K:.1f} 1/s")
print(f"Consumption Speed: {Sc * 100:.2f} cm/s")
oppFlame.save("premixed_counterflow_twin_flame.csv", basis="mole", overwrite=True)
# Generate plots to see results, if user desires
if '--plot' in sys.argv:
import matplotlib.pyplot as plt
plt.figure(figsize=(8, 6), facecolor='white')
# Axial Velocity Plot
plt.subplot(1, 2, 1)
plt.plot(oppFlame.grid, oppFlame.velocity, 'r', lw=2)
plt.xlim(oppFlame.grid[0], oppFlame.grid[-1])
plt.xlabel('Distance (m)')
plt.ylabel('Axial Velocity (m/s)')
# Identify the point where the strain rate is calculated
plt.plot(oppFlame.grid[strainRatePoint],
oppFlame.velocity[strainRatePoint], 'gs')
plt.annotate('Strain-Rate point',
xy=(oppFlame.grid[strainRatePoint],
oppFlame.velocity[strainRatePoint]),
xytext=(0.001, 0.1),
arrowprops={'arrowstyle': '->'})
# Temperature Plot
plt.subplot(1, 2, 2)
plt.plot(oppFlame.grid, oppFlame.T, 'b', lw=2)
plt.xlim(oppFlame.grid[0], oppFlame.grid[-1])
plt.xlabel('Distance (m)')
plt.ylabel('Temperature (K)')
plt.tight_layout()
plt.show()
else:
print('************')
print('Plotting option not enabled. Re-run script with --plot to see key plots.')
print('************')