Challenge

Week 5: Prandtl Meyer Shock problem

Prandtl Meyer Shock problem

OBJECTIVE-

  • Simulate a nozzle inside which air is flowing at subsonic and supersonic velocity
  • simulation is steady state
  • observe variation of velocity and pressure along the geometry and throughout the geometry
  • use of adaptive mesh refinement

What is a shock wave?

Shock waves are formed when a pressure front moves at supersonic speeds and pushes on the surrounding air. When the speed of a source exceeds the speed of sound (v > c) the wave fronts lag behind the source in a cone-shaped region with the source at the vertex. The edge of the cone forms a supersonic wave front with an unusually large amplitude called a "shock wave". When a shock wave reaches an observer a "sonic boom" is heard.

shock waves can be created in both liquid and air, primary condition for generation of shock wave is that source velocity should be greater than sound velocity.

shock waves are waves of long amplitude. In above figure at vetex is a source whose velocity is more than sound velocity, so we can see the rythmic long amplitude shock waves created, which starts at vertex goes to end forming a triangle or pyramid shape.

Mach number - Ratio of velocity of source to velocity of sound is called mach number. When mach > 1 supersonic waves are created and when mach < 1 subsonic waves are created.

Shock flow boundary conditions

Dirichlet boundary condition - This condition specifies the value that the unknown function needs to take on along the boundary of the domain. y(x) = f(x)

Neumann boundary condition - Neumann boundary when imposed on an ordinary (ODE) or a partial differential equation (PDE), it specifies the values that the derivative of a solution is going to take on the boundary of the domain. dy/dn = f

Robin boundary condition - This boundary condition consists of a linear combination of the values of the field and its derivatives on the boundary or this boundary condition is combination of dirichiletand neumann boundary condition

What is neuman boundary condition

The Neumann boundary condition specifies the normal derivative at a boundary to be zero or a constant. When the boundary is a plane normal to an axis, say the x axis, zero normal derivative represents an adiabatic boundary, in the case of a heat diffusion problem. Conduction heat flux is zero at the boundary.
This boundary condition when the input or outputs are unknown , like we dont know exact value of input velocity because that velocity is from of ODE or PDE.

NOZZLE

This is a 2D supersonic nozzle, velocity inside supersonic nozzle is more than velocity of sound.

SIMULATION PARAMETERS

Run parameters

simulation is a steady-state solver and hence we are using full hydrodynamic mode.

solver parametrs

Time parameters

start time -0

end time - 25000

time step - 1e-09

Boundary conditions-

Inlet - inflow, at inlet we will use specied value for all three boundary condition.

outlet - outflow , at outlet all three boundary conditions are zero gradient because we dont know final velocity , temprature and pressure so in such cases where outlet values are unknown we use neumann boundary condition

top-bottom - wall, It is slip boundary condition because it is solid , when we use wall it is going to be slip or no slip boundary condition.

inlet

velocity is 680m/s in x-direction which is supersonic speed

outlet

Top-bottom

Regions and initialisation

Grids

adaptive mesh refinement

why adaptive mesh refinement?

For large-size application problems. Due to the large size of many application problems, it is infeasible to solve the entire problem on a uniform grid that is fine enough to achieve the desired accuracy. For this reason, the code incorporates the ability to perform adaptive mesh refinement (AMR).

Supersonic problems are large size application problem and to get better results we use finer grids in combustion area

VELOCITY CONTOUR

PRESSURE CONTOUR

PLOTS

Average velocity at outlet

velocity observes a sudden rise , this usually happens in case of supersonic problems

average density at outlet

Density decreases as object moving at supersonic speed reduces density of its surroundings

static pressure at outlet

Increase in velocity leds to decrease in pressure.

Mass flow rate at outlet

Mach no

Mach no greater than 2 represnts supersonic flow

Velocity variation setup in paraview

https://drive.google.com/file/d/1nXB0PFYVa_-Hv2vhuoJiLlMpvI5SO3Se/view?usp=sharing

Pressure variation setup in paraview

https://drive.google.com/file/d/1EFwqutUQrbLg2SwWhXQ6hMmtVqwjqu9b/view?usp=sharing

SUBSONIC FLOW-

Everything would same except velocity, change velocity to 100m/s

velocity contour

pressure contour

Animation of velocity

https://drive.google.com/file/d/1OvIYX4_Qi23y9bokfXyL6crfYWTFDe-o/view?usp=sharing

PLOTS

mass flow

velocity

total cellls

mach no

Conclusion-

  • Pressure, density drops at supersonic flow.
  • velocity expriences sudden increase in magnitude in supersonic flow.
  • mach no increass to more than 2
  • neumann boundary are used while dealing with supersonic flows.
  • supersonic flow has mach no over 2 whereas subsonic flowa has mach no less than 1.
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