Auto-Ignition

Auto-ignition is a spontaneous ignition of the combustible mixture, without an external source of ignition. Pre-ignition kinetics are not directly resolved by the ECFM model—an ignition delay is computed and used to establish the time when ignition occurs.

Simcenter STAR-CCM+ provides two auto-ignition models:

  • ECFM Standard Auto-Ignition
  • ECFM TKI Auto-Ignition

ECFM Standard Auto-Ignition

The ECFM standard auto-ignition model provides source terms for the species, such as fuel, according to:

Figure 1. EQUATION_DISPLAY
ω ˙ f = A [ F ] b f [ O 2 ] b o e T c , a c t T b
(4019)
where b f and b o are the fuel exponent and oxygen exponent, respectively, for the ignition reaction. A is the ignition reaction pre-exponential factor, T c , a c t is the fuel consumption reaction activation temperature, and T b is the temperature of the burnt gasses.

The auto-ignition delay τ d is calculated based on semi-empirical correlations.

Compression Ignition
τ d is calculated as:
Figure 2. EQUATION_DISPLAY
τ d [ c o m p r e s s i o n ] = A d [ F ] a f [ O 2 ] a o ρ a ρ ( F c n C N ) e T d , a c t / T u
(4020)
where a f , a o , and a ρ are the delay fuel, delay oxidizer, and delay density exponents, respectively. [ F ] and [ O 2 ] are the molar concentrations of the fuel and oxygen respectively. F c n is the delay cetane number factor and C N is the cetane number (maximum value = 60).
Knock
τ d is calculated as:
Figure 3. EQUATION_DISPLAY
τ d [ k n o c k ] = A d ( R O N F o n ) a o n [ p 1 + X r e s ] a p e T d , a c t / T u
(4021)
where a o n and a p are the delay octane number exponent and delay pressure exponent respectively. R O N is the octane number, F o n is the delay octane number factor, X r e s is the mole fraction of the residual gases, and ρ is the density.

A d is the delay pre-exponent factor, T d , a c t is the reaction-delay activation temperature, and T u is the unburnt temperature.

An ignition progress variable function Y i g i is defined to track the development of the reactions prior to autoignition:
Figure 4. EQUATION_DISPLAY
d Y i g i d t = Y u , f F ( τ d )
The condition for auto-ignition is:
Figure 4. EQUATION_DISPLAY
c i g i = { 1 Y i g i > Y u , f a n d Y u , f > 1 e 10 0 o t h e r w i s e
(4023)
(4022)

ECFM TKI Auto-Ignition

The alternative is to use Tabulated Kinetic Ignition (TKI) tables. With this approach, the ignition delay is derived by taking values from pre-computed tables based on complex chemistry. If required, these values can be adjusted by multiplying with a delay factor. The auto-ignition saturation coupling option takes into account the local equivalence ratio profile near fuel droplets and uses this as input for the TKI libraries. Ignition delay and auto-ignition reaction rates (DELAY and DCDT in the TKI tables output respectively) are derived from the pre-computed TKI tables based on complex chemistry. The TKI libraries are fuel dependant.

When using the ECFM TKI auto-ignition model, the TKI tables provide source terms for the species.

When adjusting the auto-ignition reaction rates with a burning rate factor, the auto-ignition reaction rate that is used in the CFD simulation ( d c d t C F D ) is calculated by:
Figure 6. EQUATION_DISPLAY
d c d t C F D = d c d t F b r
(4024)
where d c d t is the DCDT value in the TKI table output and F b r is the burning rate factor.
An ignition progress variable function Y i g i is defined to track the development of the reactions prior to auto-ignition:
Figure 7. EQUATION_DISPLAY
d Y i g i d t = Y u , f F ( τ d )
(4025)
where F ( τ d ) is a function of auto-ignition delay τ d (DELAY in the TKI table output).
When adjusting the auto-ignition delay with a delay factor, the ignition delay that is used in the CFD simulation ( τ d , C F D ) is calculated by:
Figure 8. EQUATION_DISPLAY
τ d , C F D = τ d F τ d
(4026)
where F τ d is the auto-ignition delay factor.
Once a delay criterion is reached, for example:
Figure 9. EQUATION_DISPLAY
Y i g i > Y u , f
(4027)
an extra flame surface area Σ i n i t is added to the existing flame surface within the unburnt gases:
Figure 10. EQUATION_DISPLAY
Σ i n i t = max [ Σ , min ( c i g i | c | , V 1 / 3 ) ]
(4028)
where V is the ignition cell volume and:
Figure 11. EQUATION_DISPLAY
c i g i = { 1 Y i g i > 0.99 Y u , f a n d Y u , f > 1 e 4 0 o t h e r w i s e
(4029)

where Y u , f is the subgrid mixed-level unburnt fuel conditional mass fraction.