Week 4 - CHT Analysis on Exhaust port
Aim:
· To give a brief description of why and where a CHT analysis is used.
· To maintain the y+ value according to the turbulence model and justify the results.
· To calculate the wall/surface heat transfer coefficient on the internal solid surface & show the velocity & temperature contours in appropriate areas.
· To get answer for how would you verify if the HTC predictions from the simulations are right? On what factors does the accuracy of the prediction depend on?
Introduction:
CHT Analysis and Its Importance
Conjugate heat transfer is a type of heat transfer analysis between solids and fluid. This type of heat transfer includes both convection (between fluids) and conductive (between solids) heat transfer, as well as both forced and natural convection. Common applications and use cases of this thermal simulation type include electronics cooling, heat exchangers, industrial machinery.
In solids, heat transfer typically occurs through conduction, while in fluids, it happens through convection. Conjugate heat transfer combines these two mechanisms to provide a comprehensive understanding of the thermal interactions between solids and fluids. For example, in a heat sink, heat is conducted through the solid material and then transferred to the surrounding fluid by convection.
Growth of the Boundary layer over the plate.

Y+ Value
Here y plus values are selected in accordance with the turbulence model we choose to solve the problem with. So particular. turbulence model have its own range of y plus values to get more accurate results
Y+> 500 for the outer layer
30<Y+<500 for log low region (High Reynolds number formulation hence K-epsilon is used)
5<Y+<30 for the buffer layer
Y+<5 for viscous sublayer (low Reynolds number formulation hence K-w or SST is used)
Y+ calculation by Matlab
clear all
close all
clc
Re = 67934; %Reynolds number
rho = 1.225; %density of the fluid
U = 6; %velocity
Yplus = 30
Mu = 1.7965e-5; %dynamic viscosity
Cf = 0.079*Re^(-0.25) %for internal flow, skin friction factor which is function of Reynolds number.
Tw = 0.5*(Cf*rho*U^2); % wall shear stress
Ut = (Tw/rho)^0.5 % frictional velocity
dy = (Yplus*Mu)/(rho*Ut) %first cell height
result

Matlab Calculation for Heat transfer coefficient
close all
clear all
clc
%input
rho= 1.225; % density kg/m^3
mu= 1.796e-5; %dynamic viscosity
U = 6; %velocity in m/s
D= 0.166; %Pipe diameter in m
Pr=0.746; %Prandtl number
L=D; %Characteristic length
k=0.0242; %thermal conductivity of the fluid
%Reynolds Number
Re=(rho*U*D)/mu
%Nusselt Number
Nu=0.023*(Re^0.8)*(Pr^0.4)
%heat transfer coefficient in W/m^2 K
h=Nu*(k/L)
Result
Physics /Mesh Setup
Geometry
· Model imported into the space claim
· By using volume extract option, extracted the volume.
· Share topology between solid and fluid volume enabled (pink circles ensures the share topology is enabled)
· Created new component from both the volumes.
Mesh
Case1



Case2
We have added inflation layer with first layer thickness 0.0015m as we calculated for Y+ value 30. Element size 0.05m.



Setting up of Physics,
Refference Values

Material Properties
Viscous Model
Hybrid Initialization selected.
Analysis of all the cases
Case 1
1.1 Description of the case 1
|
Description |
Values |
|
Flow type |
Steady state, pressure-based solver |
|
Turbulence \ Viscous model |
K- Epsilon |
|
Inlet Velocity |
6 m/s |
|
Y+ |
- |
|
Total Number of elements |
138020 |
|
First layer Thickness |
NA |
1.2 Line plot of Residual versus the iteration
1.3 Line plot of Nusselt number versus the iteration
1.4 Line plot of Yplus based of heat transfer coefficient versus the iteration
1.5 Line plot of heat transfer coefficient adjacent wall versus the iteration
1.6 Line plot of Temperature at outlet versus the iteration
1.7 Result

1.8 Contour plot of temperature
1.9 velocity stream line
1.10 velocity contour

1.10 velocity vector


Case 2
2.1 Description of the case 2
|
Description |
Values |
|
Flow type |
Steady state, pressure-based solver |
|
Turbulence \ Viscous model |
K- Epsilon |
|
Inlet Velocity |
6 m/s |
|
Y+ |
30 |
|
Total Number of elements |
4321111 |
|
First layer Thickness |
0.0015 |
2.2 Line plot of Residual versus the
iteration
2.3 Line plot of Nusselt number versus the iteration

2.4 Line plot of Yplus based of heat transfer coefficient versus the iteration
2.5 Line plot of heat transfer coefficient adjacent wall versus the iteration
2.6 Line plot of Temperature at outlet versus the iteration
2.7 Result

2.8 Contour plot of temperature
2.9 velocity stream line
2.10 velocity contour
2.11 velocity vector


Conclusion
From the base line mesh which doesn't have inflation layer and from the Refined mesh we can conclude that The model with inflation layer can trap better wall adjacent values and conditions. Thus it signifies the importance of the inflation layer in capturing near-wall phenomenon.
As a fact we know that finer the mesh accurate the values are. The viscous models and solvers should be chosen according to the requirements. A good understanding of solvers and models is needed for CHT analysis.
Y plus values should be maintained depending on the solvers. Comparing the contours of temperature between the baseline mesh and refined mesh, we have observed that temperature is more accurate in case of refined mesh with an inflation layer
To get answer for how would you verify if the HTC predictions from the simulations are right? On what factors does the accuracy of the prediction depend on?
|
HTC |
Nusselt Number |
Outlet temperature |
HTC Error |
|
|
Analytical |
21.98 |
150 |
- |
- |
|
Base mesh |
32.07 |
170 |
682 K |
10.09 |
|
Refined Mesh |
61.01 |
220 |
680 K |
39.03 |
Using the above data the calculation done can be validated as the values are closer to the analytical values. There was no much of difference spotted comparing both cases, there was only a little change in the values obtained










