debojyoti ghosh adviser: dr. james baeder alf dlfred ...rvbalan/.../midyrdebojyotighosh.pdf ·...
TRANSCRIPT
![Page 1: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/1.jpg)
Debojyoti Ghosh
Adviser: Dr. James Baederlf d fAlfred Gessow Rotorcraft Center
Department of Aerospace Engineering
![Page 2: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/2.jpg)
To study the Dynamic Stalling of rotor blade cross-sections
Unsteady Aerodynamics:y y
Time varying angle of attack and free-stream velocities.
Affects the lift drag and pitching moment of the rotorAffects the lift, drag and pitching moment of the rotor
Numerical Simulation:
Solution of the Navier Stokes equations with an appropriate
turbulence model
“First Step” → Solve the Euler Equations (inviscid
aerodynamics)aerodynamics)
![Page 3: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/3.jpg)
Airfoil:
Wing / Rotor cross section – basic 2D lifting surface
Lift and Drag are functions of angle of attack, free-streamfluid velocity and shape of the airfoilfluid velocity and shape of the airfoil
Higher velocities on upper surface create pressurediff l i i d i fdifference resulting in aerodynamic forces
Inviscid flow over airfoil → only pressure forces, no shearstresses on the surface
Inviscid drag less than actual dragg g
![Page 4: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/4.jpg)
Governing Equations: Euler EquationsConservation of Mass, Momentum and Energy, gy
Obtained from the Navier Stokes equations by l ti i it d h t d tineglecting viscosity and heat conduction
Importance: (High Speed Flows)gFlow around any solid body = viscous “boundary layer” + outer flow
Flow away from the surface can be approximated as inviscid flow (negligible cross-derivatives of fluid velocity)flow (negligible cross-derivatives of fluid velocity)
![Page 5: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/5.jpg)
Discretizations based the Integral form of the governing equation
∂∫∫
u 0. =+∂∂
∫∫∂VV
dSdVt
nFu )
Also called as “Conservation form” since u is a conserved
variable
Does not assume smooth solutions (unlike differential form)
→ More appropriate for hyperbolic systems with discontinuous
solutionssolutions
![Page 6: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/6.jpg)
C ti f f th E l E tiConservation form of the Euler Equations
+==∇+∂∂ ˆˆ;0. jg(u)if(u)F(u)Fu
t
⎥⎤
⎢⎡
⎥⎤
⎢⎡
⎥⎤
⎢⎡∂
vu2
ρρρt
⎥⎥⎥⎥
⎢⎢⎢⎢
+=
⎥⎥⎥⎥
⎢⎢⎢⎢ +
=
⎥⎥⎥⎥
⎢⎢⎢⎢
=pv
uv,
uvpu
,vu
2
2
ρ
ρ
ρρ
ρρ
g(u)f(u)u
ρ - Density, (u, v) – Velocity components,
⎥⎥⎦⎢
⎢⎣ +⎥
⎥⎦⎢
⎢⎣ +
⎥⎦
⎢⎣ p)v(Ep)u(EE
ρ y, ( , ) y p ,p - Pressure, E – Internal Energy
)(1p 22Equation of State )vρ(u
21
1γpE 22 ++−
=
![Page 7: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/7.jpg)
Semi-discrete equation using the FV formulation:dd uu
Fl C i l ll i f
),(0ˆ jidt
ddS
dtd ij
faces
ij Resu
nF.u
=⇒=+ ∑Flux Computation normal to cell interfaces
Upwinded to account for wave nature of the solutionUpwinded to account for wave nature of the solution
Essentially Non Oscillatory Schemes (2nd, 3rd order)
Time Marching using Total Variation Diminishingd dRunge Kutta (2nd, 3rd order) schemes
![Page 8: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/8.jpg)
2D Riemann Problems on Cartesian gridsDiscontinuous initial data on a square domainDiscontinuous initial data on a square domain
Unsteady problems
M h 2 9 Obli Sh k R fl ti blMach 2.9 Oblique Shock Reflection problemOblique shock wave at 30o reflects off a flat wall
Supersonic flow on 15o compression rampCompression ramp causes an oblique shock followed by an expansion
Inviscid flow around the NACA0012 airfoilSubsonic and Transonic cases studied and validated
Results validated with UM TURNS codedeveloped and used by the Rotorcraft Center
Implicit time – stepping with MUSCL-type reconstruction
![Page 9: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/9.jpg)
M lt3rd Order1st Order My results
“Configuration 6” (Density)
Results from Kurganov TadmorResults from Kurganov-Tadmor
![Page 10: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/10.jpg)
Oblique Shock Pressure Contours and Streamlines
Exact Solution obtained through Oblique Shock relationsg q
3rd order ENO +3rd order TVD Runge Kutta
Mach 2.9 Inflow
![Page 11: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/11.jpg)
2nd order ENO + 2nd order TVD Runge Kutta
M h 3 3 I fl
Compression Ramp Pressure Contours and Streamlines
Mach 3.3 Inflow
Compression Ramp Pressure Contours and StreamlinesSolution validated with exact solution obtained from oblique shock relations
and Prandtl-Myer expansion fan relations
![Page 12: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/12.jpg)
Magnified view of mesh aroundi f il ( it h d)airfoil (unit chord)
C-Type Structured Mesh withoutside boundary 20 chords away
Curved Wall Boundary Conditions Freestream boundary conditions on outer boundary
at Airfoil Surface
![Page 13: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/13.jpg)
- Coefficient of Pressure /2uρppC2
p∞∞
∞−=
- Results validated with TURNS code
i h d h i k
/2uρ ∞∞
Higher order schemes capture suction peak better than 1st order
Pressure and streamlinesaround the airfoil at Mach 0.63and 2 degrees angle of attackg g
![Page 14: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/14.jpg)
Results validated with TURNS code
Higher order schemes show bettershock resolution than 1st order
Pressure and streamlinesaround the airfoil at Mach 0.85and 1 degrees angle of attack
![Page 15: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/15.jpg)
2D Euler code validated for various cases
Next steps:Incorporating viscosity terms in the code to make in a Navier Stokes solver
Validation of the Navier Stokes solver on 2D problems (Cartesian and non –Cartesian)
Incorporating a turbulence model
Timeline → Running slightly late but will make upFinished with building and validating 2D Euler code
Started reading up on solution to Navier Stokes equations
Have coded in the viscous terms for the Navier Stokes solver (will startvalidating soon)
![Page 16: Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred ...rvbalan/.../MidYrDebojyotiGhosh.pdf · Debojyoti Ghosh Adviser: Dr. James Baeder Alf dlfred Gessow Rotorcraft Center Department](https://reader034.vdocuments.mx/reader034/viewer/2022050506/5f976d9bf5bcdc37692ac9f3/html5/thumbnails/16.jpg)