Combustion and Reactions Chapter 4: Turbulent Combustion

This chapter introduces turbulent combustion as the realistic regime for most engineering systems, where turbulence and chemical reactions interact strongly. It develops the conceptual and mathematical tools needed to model this interaction: DNS, RANS, LES, Favre averaging, scalar statistics, and PDF methods. The focus is on understanding why turbulence fundamentally changes combustion behavior and why modeling becomes significantly more complex

 

Context and Motivation

In real engineering devices, combustion is almost always turbulent by design:

  • Gas turbines

  • IC engines

  • Industrial burners

  • Fires

Reason:
→ Turbulence enhances mixing and heat transfer, leading to faster and more stable combustion

Physically, this means:

  • Reactants are brought together faster

  • Heat is redistributed more efficiently

  • Flames become stronger but more complex

However, turbulence introduces:

  • Random fluctuations

  • Wide range of length/time scales

  • Strong coupling with chemistry

This makes turbulent combustion one of the most difficult problems in CFD.


Main Concepts

Turbulence–Chemistry Interaction

The defining feature:
Two-way coupling

  • Turbulence affects combustion:

    • Enhances mixing → increases reaction rates

  • Combustion affects turbulence:

    • Heat release → changes density, viscosity, velocity fields

Physically:

  • The flame is not independent of the flow

  • The flow is not independent of the flame

They evolve together.

Time Scale Competition (Key Idea)

The central parameter is the ratio of:

  • Mixing time (turbulence)

  • Chemical time (reaction)

This ratio defines combustion regimes.

Damköhler number (Da):

  • High Da → fast chemistry → thin flame sheets

  • Low Da → slow chemistry → distributed reaction

Interpretation:

  • If mixing is slow → reaction limited by mixing

  • If chemistry is slow → reaction limited by kinetics

Turbulent Combustion Regimes

1. Flamelet regime (fast chemistry)

  • Reaction zones remain thin

  • Turbulence wrinkles and stretches flames

  • Flame behaves like many laminar flamelets

2. Distributed regime (slow chemistry)

  • Reaction occurs over a larger volume

  • No clear flame front

  • Strong turbulence–chemistry coupling

These regimes directly determine which model to use


Modeling Framework / Formulations

1. DNS, RANS, LES (Core CFD Approaches)

DNS (Direct Numerical Simulation)

  • Resolves all turbulence scales

  • No modeling assumptions

Reality:

  • Computationally infeasible for real systems

  • Only small domains and simple chemistry possible

Use:
→ Fundamental research

RANS (Reynolds-Averaged)

  • Solves time-averaged fields

  • All turbulence effects are modeled

Implications:

  • Fast and practical

  • Loses instantaneous fluctuations

Main issue:
→ Introduces closure problems, especially for reaction terms

LES (Large Eddy Simulation)

  • Resolves large turbulent structures

  • Models only small scales

Key idea:

  • Large eddies control mixing → directly resolved

Advantages:

  • More accurate than RANS for mixing-driven processes

  • Captures unsteady flame behavior

Limitation:

  • Expensive, especially near walls

Engineering Insight:

  • Large eddies contain most energy

  • Small eddies dissipate energy

LES resolves:
→ The most physically important structures for combustion

2. Favre Averaging (Variable Density Flows)

Why Needed

In combustion:

  • Density varies strongly due to heat release

Standard averaging creates:

  • Complex additional correlation terms

Favre Averaging Idea

Instead of simple averaging:
→ Use density-weighted averaging

Physically:

  • Gives more importance to high-density regions

Result:

  • Simplifies governing equations

  • Reduces complexity of turbulent correlations

Interpretation:

Favre averaging:
→ Separates variables into:

  • Mean value

  • Fluctuations relative to density

This is essential for:

  • Species transport

  • Energy equations

3. Closure Problem (Core Difficulty)

After averaging:

  • New unknown terms appear:

    • Turbulent fluxes

    • Reaction source terms

The biggest challenge:
→ Chemical reaction terms

Reason:

  • Reaction rates depend nonlinearly on:

    • Temperature

    • Species concentrations

Therefore:

  • Mean reaction ≠ reaction at mean conditions

This is the turbulence–chemistry interaction problem

4. Statistical Description: PDF Approach

Why PDFs?

In turbulence:

  • Variables fluctuate strongly

Instead of single values:
→ Use probability distributions

Concept

The PDF gives:

  • Probability of finding a certain value (e.g., mixture fraction, temperature)

Importance

Reaction rates depend on:
→ Full distribution, not just averages

This allows:

  • More accurate modeling of nonlinear chemistry

Types

  • Assumed PDF models (simplified shapes)

  • Transported PDF models (solve transport equation)

Trade-off:

  • Accuracy vs computational cost


Numerical / CFD Aspects

Main Challenges

From CFD perspective:

  • Many species equations

  • Stiff chemistry

  • Wide range of scales

  • Strong nonlinear coupling

Model Choices in Practice

From Fluent:

Fast chemistry models (Da >> 1):

  • Eddy Dissipation Model

  • Non-premixed model

Finite-rate models:

  • Eddy Dissipation Concept (EDC)

  • Finite-rate chemistry

  • Flamelet models

  • PDF models

LES Workflow Insight

From LES application chapter:

  • Mesh must resolve large eddies

  • Time step must capture unsteady behavior

  • Sub-grid models handle smallest scales

Important:
→ LES becomes more accurate as resolution increases


Physical Interpretation and Engineering Intuition

Mixing Controls Everything

In turbulent combustion:
→ Mixing is often the limiting factor

Large eddies:

  • Stretch and fold scalar fields

  • Create thin layers → intense reactions

Flame Structure

Instead of smooth laminar flames:

  • Flames become:

    • Wrinkled

    • Intermittent

    • Unsteady

Physically:

  • Flame surface area increases → higher burning rate

Unsteady Behavior Matters

From LES examples:

  • Large-scale structures strongly affect mixing and combustion

Time-averaged (RANS) results:
→ May miss important physics

Engineering Judgment

  • Use RANS for:

    • Design iterations

    • Steady predictions

  • Use LES for:

    • Flame instability

    • Detailed mixing

    • Research-level accuracy


Applications

  • Gas turbines (lean premixed combustion)

  • IC engines (diesel, SI engines)

  • Industrial furnaces

  • Fire dynamics

  • Rocket propulsion


Limitations and Assumptions

RANS

  • Cannot capture transient flame structures

  • Strong modeling dependence

LES

  • High computational cost

  • Difficult near walls

DNS

  • Not practical for engineering

All Models

  • Require turbulence–chemistry closure

  • Sensitive to modeling assumptions


Study Priorities

If short on time:

  1. Turbulence–chemistry interaction concept

  2. Damköhler number interpretation

  3. DNS vs RANS vs LES differences

  4. Favre averaging (why it exists)

  5. Closure problem (reaction term)

  6. PDF concept and purpose


Key Takeaways

  • Turbulent combustion is dominated by mixing–chemistry interaction

  • The Damköhler number defines combustion regime

  • DNS, RANS, LES differ by how turbulence is treated

  • Favre averaging is essential for variable-density flows

  • The reaction source term closure is the central challenge

  • PDF methods capture nonlinear effects of fluctuations

  • LES provides the best balance between accuracy and feasibility for modern CFD

Next
Next

Combustion and Reactions Chapter 3: Laminar Non-premixed flames