Challenge

Week 6: Conjugate Heat Transfer Simulation

Aim:- Conjugate Heat Transfer Simulation

objective:-

  • Setup a flow simulation through a pipe
  • Inlet Reynolds number should be 7,000
  • Turbulence modelling - K-Epsilon
  • Supercycling parameters
  • Grid dependence test

    • Start with an initial base grid
    • Run grid dependence test on 3 grids and show that the outlet temperature converges to a particular value

    Effect of supercycle stage interval

    • Set supercyle stage interval to 0.01,0.02 and 0.03

theory:-

Conjugate Heat Transfer(CHT):-

Conjugate heat transfer corresponds with the combination of heat transfer in solids and heat transfer in fluids. In solids, conduction often dominates whereas in fluids, convection usually dominates. Conjugate heat transfer is observed in many situations. For example, heat sinks are optimized to combine heat transfer by conduction in the heat sink with the convection in the surrounding fluid.

Heat Transfer in a Solid:

heat transfer in solids, if only due to conduction, is described by Fourier’s law defining the conductive heat flux, q, proportional to the temperature gradient

`q=-k*gradT`

For a time-dependent problem, the temperature field in an immobile solid verifies the following form of the heat equation:

`rho*C_p(dT)/dt=grad*(k*gradT)+Q`

here Q is heat generation per volume if bogy generating heat

Heat Transfer in a Fluid

Due to the fluid motion, three contributions to the heat equation are included:

  1. The transport of fluid implies energy transport too, which appears in the heat equation as the convective contribution. Depending on the thermal properties on the fluid and on the flow regime, either the convective or the conductive heat transfer can dominate.
  2. The viscous effects of the fluid flow produce fluid heating. This term is often neglected, nevertheless, its contribution is noticeable for fast flow in viscous fluids.
  3. As soon as a fluid density is temperature-dependent, a pressure work term contributes to the heat equation. This accounts for the well-known effect that, for example, compressing air produces heat.

Radiation: transfer of energy by electromagnetic waves between surfaces with different temperatures, separated by a medium that is at least partially transparent to the (infrared) radiation. Radiation is especially important at high temperatures, e.g. during combustion processes, but can also have a measurable effect at room temperatures.

supercycle modling:

converge offer several time control methd for CHT in which supercycling is one option

here converge iterate b/w fully couple transient for fluid and stedy sate solustion for solid only

this method is highly recommend for combution simulation

during super cycling

  1. intially solver solves fluid and solid using transient solver and store the heat transfer coeffient(HTC) and tepratuer on the interface during this precess
  2. freezes the fluid solver: time avrging the HTCs and temp and applies them as boundary conction at the interface
  3. solver the solid temp untilll it reaches steady state
  4. update the solid temp field and unfreeze the flluid solver
  5. repeat untill solid temp converge
simulation setup:
open converge application and create a cylender with radius 0.015 and length 0.2m in z direction and thickness to it of 0.005 m
once cylanfder is created check the diagnossis if any error present the resolve them
boundary flag
case setup:
case setup tree
matrials : select prefine mixture as air
in solid simulation select aluminium from predefine data
in spicies
in solid section select aluminium and in gas section select N2 and O2
simulation parameter
boundary condtion
regions and intialization
here need to create 2 region 1 for solids and another for fluid
physical model
base grid control
output and post processing
after case setup final validate the setup if any errors are present selove them once agine run the diagnossis if no error present export the input file to peticular folder
now open cygwin navigate to the folder where input files are saved run the command
mpiexec.exe -n 8 converge.exe restricted
wait till simulation runs and look for results and post precess result
result:-
once the simulation runs gove to converge studion line plot section to see he plots
super cycle stage interval 0.03 and base grid 0.004
mass flow rate, temp, pressure and velocity plots
cell count in each region
super cycle temp output at points
wall temp
super cycle 0.02 base grid 0.004
mass flow rate , pressure, temprature andd velocity result plot
cell count in each region
temp at each super cycle point
mean temp of solid wall
super cycle 0.01 base grid 0.004
mass flow rate , pressure, temp and velocity resul plot
cell count
super cycle poittemp
mean temp of solid wall
super cycle inteval 0.01 base grid 0.03
mass flow rate, pressure, temp and velocity result plot
cell count in each region
super cycle at each point
temp of solid wall
super cyycle interval 0.01 base circle 0.02
mass flow rate , pressure , temp and velocity plot
cell count in each region
super cycle temp at each point
solid wall temp
at lower supe cycle value the chane in solid wall temp is quick
post processing
the output file which are save in output older are converted to readble file for paraview to see post procssong result
now open parview and open converted file to see result
super cycle 0.03 base grid 0.004
density with mesh
temprature distribution
velocity
pressure
super cyce 0.02 base grid 0.004
density
temperatuere
pressure
y+ value
velocity
super cycle 0.02 base grid 0.004
density
pressure
temprature
y+ value
velocity
scper cycle 0.01 base grid 0.003
density
pressure
temp
y+ value
velocity
super cycle 0.01 and grid control 0.002
density
temp
pressure
y+ value
velocity
conclusion
as grid size reduce more number of cell as well as there is reduction in solid wall temp and temp of fluid is more
with change in super cycle less the value more quick change in wall temp
as the grid size reduce less will be the y+value
animation which support conclusion are attached in zip file
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