1 of 17

Streamwise periodic flow solver with iso-thermal boundaries in SU2.

3rd Annual SU2 Conference

September 5 - 7, 2022

Nitish Anand, Carlo de Servi

ETE-THES, VITO, EnergyVille.

vito.be

©VITO – Not for distribution

2 of 17

Motivation & Background

1

©VITO – Not for distribution

3 of 17

Why a periodic flow solver?

Reduced-order Modeling

vito.be

©VITO – Not for distribution

4 of 17

Periodic Flow Solver in SU2

Momentum and Mass Equations

©VITO – Not for distribution

4

5/09/2022

vito.be

©VITO – Not for distribution

5 of 17

Periodic Flow Solver in SU2

Energy Equation

 

Turbulent source term

(Kattmann, 2021)

Laminar source term

 

Only one side of the HEX 🡪 Boundary Condition needed!

Constant heat flux @ walls

vito.be

©VITO – Not for distribution

6 of 17

Periodic Flow Solver in SU2

Energy Equation

Only one side of the HEX 🡪 Boundary Condition needed!

Constant heat flux @ walls

  • Heat sinks
  • Thermally balanced HEXs �(e.g recuperators)

temperature

length

Counterflow + Ch = Cc

Constant T @ walls

  • Condensers & Evaporators
  • HEXs where Ch >> Cc or viceversa

temperature

length

vito.be

©VITO – Not for distribution

7 of 17

Streamwise Periodic Energy Equation for Isothermal Walls

Derivation

2

©VITO – Not for distribution

8 of 17

Boundary Condition: Iso-thermal Wall

Temperature periodicity

Observation:

Exponential decay of mean T

 

 

 

Suitable temperature scaling

(Patankar, �1977)

 

 

 

vito.be

©VITO – Not for distribution

9 of 17

Boundary Condition: Iso-thermal Wall

 

Suitable temperature scaling

Energy Equation

Turbulent source terms

(original contribution)

Laminar source terms

(same as that of Buckinx, 2017,

Stalio et Al.)

 

 

 

 

 

Temperature periodicity

vito.be

©VITO – Not for distribution

10 of 17

Boundary Condition: Iso-thermal Wall

 

Suitable temperature scaling

Energy Equation

 

 

 

 

 

Temperature periodicity

 

 

vito.be

©VITO – Not for distribution

11 of 17

Preliminary Results

3

©VITO – Not for distribution

12 of 17

Code Verification

Laminar Regime

vito.be

©VITO – Not for distribution

13 of 17

Code Verification

Adjoint gradients

Laminar Regime (Re = 100)

Turbulent Regime (Re = 5000)

vito.be

©VITO – Not for distribution

14 of 17

Conclusions & Way Forward

4

©VITO – Not for distribution

15 of 17

Conclusions and Perspective

  • Implementation of periodic flow solver for iso-thermal walls in SU2 accomplished

  • Code verified for laminar flow regime

  • Setting up high-fidelity flow solver for verification study in turbulent regime in progress

  • Optimization framework using SU2 in near future

LES - Teaser

vito.be

©VITO – Not for distribution

16 of 17

Thank you!

Dr.ir. Nitish Anand

nitish.anand@vito.be

Dr.ir. Carlo de Servi

carlo.deservi@vito.be

vito.be

©VITO – Not for distribution

17 of 17

References

1. T. Kattmann, “Streamwise periodic boundary conditions in SU2.” Unpublished notes (2021).

2. S. Patankar, C. Liu, and E. M. Sparrow, “Fully developed flow and heat transfer in ducts having streamwise-periodic variations of cross-sectional area.” J. Heat Transf. 99, 180–187 (1977).

3. G. Buckinx, “Macro-scale flow and heat transfer in systems with periodic solid structures.” PhD Thesis, KU Leuven (2017).

4. E. Stalio and M. Piller, “Direct numerical simulation of heat transfer in converging-diverging wavy channels.” J. Heat Transf. 129, 769–777 (2007).

vito.be

©VITO – Not for distribution