Skip to main content

Direct Numerical Simulation of Autoignition in Turbulent Non-premixed Combustion

  • Chapter
  • First Online:
Modeling and Simulation of Turbulent Combustion

Part of the book series: Energy, Environment, and Sustainability ((ENENSU))

  • 2582 Accesses

Abstract

Combustion in a CI engine is initiated by self-ignition of fuel–air mixture caused by high pressure and high temperature; a process known as autoignition. Autoignition is a challenging problem to simulate as the temperature increases from initial temperature to the adiabatic flame temperature in a very short duration. Numerical study of a turbulent flow using RANS/LES encounters a closure problem. Accuracy of closure models can be improved through experimental results, theoretical reasoning and direct numerical simulation (DNS) data. A review of DNS of autoignition in a turbulent non-premixed medium is presented in this chapter. As observed from DNS study, autoignition sites in a turbulent non-premixed medium are not randomly distributed but follow a pattern in the mixture fraction-scalar dissipation rate space. Turbulent flow is always three-dimensional in nature. 2D DNS of autoignition shows that ignition delay time increases with increase in initial turbulence intensity, which contradicts with the experimental observation. 3D DNS of autoignition resolves this conflict. The conflict is mainly due to the absence of vortex-stretching phenomenon in 2D DNS. Homogeneous charge compression ignition (HCCI) is being considered as one of the strategies toward improving performance of conventional CI engines. However, HCCI engines suffer from drawbacks like lack of control over combustion and limited operating regime. One of the modifications suggested in the HCCI technology to overcome these drawbacks is the use of stratification in the fuel–air mixture. Therefore, a few DNS studies on autoignition in the stratified medium have been discussed here. Further, discussion on the conditional moment closure (CMC) model and its validation using DNS data has been presented. Ignition delay time predicted by CMC was found to be in good agreement with DNS predictions.

This is a preview of subscription content, log in via an institution to check access.

Access this chapter

Chapter
USD 29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD 189.00
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD 249.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book
USD 249.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Institutional subscriptions

Abbreviations

CFD:

Computational Fluid Dynamics

CI:

Compression Ignition

CMC:

Conditional Moment Closure

DNS:

Direct Numerical Simulation

HCCI:

Homogeneous Charge Compression Ignition

HRR:

Heat Release Rate

LES:

Large Eddy Simulation

MR:

Most Reactive

RANS:

Reynolds-Averaged Navier–Stokes

SI:

Spark Ignition

TDC:

Top Dead Center

2D/3D:

Two Dimensional/Three Dimensional

\( c_{P} \) :

Specific heat at constant pressure

D :

Fickian diffusion coefficient

Da :

Damköhler Number

Ea :

Activation energy of a reaction

h r :

Heat of reaction

Δh α :

Heat of formation of a species

H F :

Heat of combustion of fuel

N S :

Number of species

\( Q(\eta ;x,t) \) :

Conditional average of any scalar Y on ξ = η

R :

Universal gas constant

T :

Temperature

T a :

Activation temperature of a reaction (E a /R)

T in :

Initial Temperature

u rms :

Root mean square value of velocity fluctuations

Y i :

Mass fraction of ith species

α, β :

Indices of species

η :

Sample space of ξ

\( \theta \) :

Excess temperature given by \( (T - T_{in} )c_{P} /h_{r} \)

λ:

Thermal Diffusivity

ξ:

Mixture fraction (Eq.  2 )

ρ :

Density

σ 2 :

Conditional variance of excess temperature θ

τ ign :

Ignition delay

τ t :

Integral timescale of turbulence

τ 0 :

Ignition delay in homogeneous mixture (or other reference timescale)

φ αβ :

Factor defined by Eq.  11

χ:

Scalar dissipation rate (Eq. 1)

\( \dot{\omega }_{i} \) :

Chemical source term of ith species

\( {\bigwedge } \) :

Integral length scale of turbulence

\( {\bigwedge }_{k} \) :

Kolmogorov scale of turbulence

\( \wedge_{\upxi} \) :

Integral scale of initial scalar distribution

\( \mho \) :

Vortex locating index (Sect. 10.2.1)

References

Download references

Acknowledgements

Most of these works were carried out by one of the authors, during his PhD, under the supervision of Prof. K. N. Lakshmisha, IISc, Bangalore.

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to S. Sreedhara .

Editor information

Editors and Affiliations

Rights and permissions

Reprints and permissions

Copyright information

© 2018 Springer Nature Singapore Pte Ltd.

About this chapter

Check for updates. Verify currency and authenticity via CrossMark

Cite this chapter

Bhide, K.G., Sreedhara, S. (2018). Direct Numerical Simulation of Autoignition in Turbulent Non-premixed Combustion. In: De, S., Agarwal, A., Chaudhuri, S., Sen, S. (eds) Modeling and Simulation of Turbulent Combustion. Energy, Environment, and Sustainability. Springer, Singapore. https://doi.org/10.1007/978-981-10-7410-3_10

Download citation

  • DOI: https://doi.org/10.1007/978-981-10-7410-3_10

  • Published:

  • Publisher Name: Springer, Singapore

  • Print ISBN: 978-981-10-7409-7

  • Online ISBN: 978-981-10-7410-3

  • eBook Packages: EngineeringEngineering (R0)

Publish with us

Policies and ethics