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Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchez University of California San Diego, La Jolla CA APS DFD 2016

Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchezasanchez.ucsd.edu/wp-content/uploads/2016/09/APSDFD2016.pdf · Prabakaran Rajamanickam, Wilfried Coenen & Antonio L

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Page 1: Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchezasanchez.ucsd.edu/wp-content/uploads/2016/09/APSDFD2016.pdf · Prabakaran Rajamanickam, Wilfried Coenen & Antonio L

Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchez

University of California San Diego, La Jolla CA

APS DFD 2016

Page 2: Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchezasanchez.ucsd.edu/wp-content/uploads/2016/09/APSDFD2016.pdf · Prabakaran Rajamanickam, Wilfried Coenen & Antonio L

F. Kimura, K. Kitamura, M. Yamaguchi, T. Asami, Fluid flow and heat transfer of natural convection adjacent to upward-facing, inclined,

heated plates, Heat Transfer - Asian Research. 32 (3) (2003) 278–291

Vortex instability

Crossover point Wave instability

Page 3: Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchezasanchez.ucsd.edu/wp-content/uploads/2016/09/APSDFD2016.pdf · Prabakaran Rajamanickam, Wilfried Coenen & Antonio L

Low Mach number equations

Boussinesq approximation is justified when

Parameters

• Inclination angle

• Wall-to-ambient temperature ratio

• Local Grashof number

• Prandtl number

Page 4: Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchezasanchez.ucsd.edu/wp-content/uploads/2016/09/APSDFD2016.pdf · Prabakaran Rajamanickam, Wilfried Coenen & Antonio L

Similarity variables

Governing equations

Streamwise

velocity

TemperatureTransverse

velocity

Page 5: Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchezasanchez.ucsd.edu/wp-content/uploads/2016/09/APSDFD2016.pdf · Prabakaran Rajamanickam, Wilfried Coenen & Antonio L

Vortex instability

Base flow in local coordinates

Wave instability

Eigenvalue problem

P. Jeschke, H. Beer, J. Fluid Mech. 432 (2001) 313–339.

Local coordinates

Page 6: Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchezasanchez.ucsd.edu/wp-content/uploads/2016/09/APSDFD2016.pdf · Prabakaran Rajamanickam, Wilfried Coenen & Antonio L

• Principle of exchange of instabilities

holds

Haaland & Sparrow(1970)

Page 7: Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchezasanchez.ucsd.edu/wp-content/uploads/2016/09/APSDFD2016.pdf · Prabakaran Rajamanickam, Wilfried Coenen & Antonio L

• Two dimensional disturbance,

• Travelling waves

Page 8: Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchezasanchez.ucsd.edu/wp-content/uploads/2016/09/APSDFD2016.pdf · Prabakaran Rajamanickam, Wilfried Coenen & Antonio L

Streamwise vortices Travelling waves

Boussinesq Grashof number For Ideal gas,

Page 9: Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchezasanchez.ucsd.edu/wp-content/uploads/2016/09/APSDFD2016.pdf · Prabakaran Rajamanickam, Wilfried Coenen & Antonio L

For wave mode prevails for all angles

Plot base

velocity

here,

Put a dot for

Boussinesq

Page 10: Prabakaran Rajamanickam, Wilfried Coenen & Antonio L. Sánchezasanchez.ucsd.edu/wp-content/uploads/2016/09/APSDFD2016.pdf · Prabakaran Rajamanickam, Wilfried Coenen & Antonio L

▪ The dependence of wall temperature in characterizing the stability mechanisms is studied explicitly since Boussinesqapproximations cease to be valid when

▪ Wave modes are found to be more sensitive to non-Boussinesqeffects compared to vortex mode.

▪ At higher temperatures, wave modes are most likely to prevail in reality for a wide of inclination angles, predicted by this work.

▪ The current work is an initial step towards non-Boussinesqnature of the concerned flow, which requires additional work for the development of heat transfer and other real life applications.