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FORCED CONVECTION SIMULATION FOR HT2 EXPERIMENT

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Properties: use average values over temperature range. Reynolds no. ~ 100,000 ... Post-Processing Step ... Post-Processing Step. Velocity vectors in the first ... – PowerPoint PPT presentation

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Title: FORCED CONVECTION SIMULATION FOR HT2 EXPERIMENT


1
FORCED CONVECTION SIMULATION FOR HT2 EXPERIMENT
  • MAE 427
  • Mechanical Aerospace Engineering
  • Cornell University

2
Experiment vs. Modeling
  • Modeling Well use FlowLab software
  • FlowLab uses the computational modeling approach
    to obtain an approximate solution to the
    governing equations. Referred to as Computational
    Fluid Dynamics (CFD).
  • Will use nominal data in simulation. You need to
    redo with your data.

3
Strategy of CFD
  • Eg. Continuous Domain p p(x), 0ltxlt1
    Discrete Domain pi p(xi), i1,2,,N
  • Truncation error introduced. Can be reduced by
    refining the grid.
  • Grid refinement study required to assess the
    level of truncation error.

4
Geometry Step
  • Assume flow is axisymmetric. Hence, domain is
    rectangular.
  • Rotate the rectangle 360o about the axis to get
    the full pipe geometry

5
Geometry Step
  • Length of pipe included in the simulation From A
    to D
  • Tip To restore original views, use the following
    buttons at the bottom right of the GUI

6
Physics Step
  • Incompressible ideal gas Neglect variations in
    absolute pressure in ideal gas law
  • Properties use average values over temperature
    range
  • Reynolds no. 100,000 Turbulent flow regime

7
Physics Step Turbulence
  • Cannot resolve rapid fluctuations in turbulent
    flow
  • We solve only for averaged quantities
  • Need to augment governing equations with
    turbulence model equations (additional
    approximation!).

8
Physics Step Turbulence
  • Will use k-e turbulence model.
  • Workhorse in engineering calculations (but has
    problems).
  • k turbulent kinetic energy Measure of the
    kinetic energy of velocity fluctuations u, v
    and w.
  • e turbulent dissipationMeasure of the
    dissipation of k into internal energy.
  • See lab manual for more details.

9
Physics Step
  • Operating condition
  • Gauge pressure Absolute pressure Reference
    pressure
  • Inlet boundary condition (BC)
  • Assume velocity is constant across cross-section.
  • Use guess values of k and e. Well specify low
    turbulence levels.
  • Axis BC FlowLab imposes symmetry conditions.

10
Physics Step
  • Outlet BC
  • Outlet pressure needs to be specified. Use
    measured gauge pressure at D.
  • Outlet velocity and temperature come out of the
    simulation.
  • Wall BC
  • FlowLab imposes no-slip condition for velocity.
  • We specify the measured (constant) heat flux in
    the heated section.
  • Well assume wall is smooth ((wall thickness
    0).
  • Well neglect heat conduction within pipe wall
    (wall thickness 0).

11
Solve Step
  • Since governing equations are nonlinear,
    iterations are required to solve the equations.

12
Post-Processing Step
  • Temperature contours Is the flow well-mixed at
    the end of the adiabatic mixing section?

13
Post-Processing Step
  • Velocity vectors in the first section showing
    flow development.

14
Reports Step
  • Pressure variation along pipe axis. Yellow
    symbols represent experimental values.
  • Can export these values in Excel format.

15
Reports Step
  • Temperature variation along pipe axis. Yellow
    symbols represent experimental values.

16
Reports Step
  • Wall temperature variation. Shows thermal
    entrance length effects.

17
Reports Step
  • Nusselt number distribution.
  • Can average values in the heated section to
    compare with experiment.
  • Dont use friction factor values from FlowLab.

18
Reports Step
  • Axial velocity profiles at various locations.
  • Plot shows flow is nearly fully developed as it
    enters the heated section.
  • Shows flow is accelerated in the heated section.

19
Reports Step
  • Temperature profiles at various locations.
  • Plot shows temperature is nearly uniform at the
    outlet (end of the mixing section).
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