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Mixing Tee
Aim: To set up steady-state simulations and compare mixing efficiencies for short and long-mixing tees when the hot inlet temperature is 36°C and the Cold inlet is at 19°C.
Objective:
Problem setup:
case 2
Here the momentum ratio is defined as: momentum ratio=Velocity at cold inletVelocity at hot inlet
Computation domain
Comparison of the two mixing Tee geometries:
Geometry | Diameter inlet X | Diameter inlet Y | Length |
Short | 33.8761 mm | 16.9626 mm | 192.3778 mm |
Long | 33.8761 mm | 16.9626 mm | 268.328 mm |
So the difference in length between short and long tee geometry is 75.9502 mm.
Procedure:
Mesh independency test:
First, we are going to perform a mesh independency test for one case and then use the same mesh settings for all other cases. Selecting the case 1 short mixing tee with a momentum ratio of 2.
Element size | 10.219 mm | 5 mm | 2.5 mm | 1.5 mm |
Cell count | 12692 | 14249 | 61233 | 213011 |
No. of Iterations for Convergence | 89 | 113 | 102 | 86 |
Average Outlet Temperature °C | 30.251 | 30.247 | 30.28 | 30.337 |
Using the analytical solution Compare the Temperature at the outlet as a parameter.
As we can see from the plot the mesh size of 1.5mm is selected for the rest of the simulations.
K-epsilon | k-omega | |
Element size | 1.5 mm | 1.5 mm |
Cell count | 213011 | 213011 |
No of Iterations for Convergence | 86 | 78 |
Average Outlet Temperature °C | 30.337 | 30.445 |
Analytical solution | 30.3255 | 30.3255 |
Error | 0.04% | 0.39% |
Results:
Case | Cell count | Convergence | Average Temperature | Average Velocity | Standard deviation Temperature | Standard deviation Velocity | Analytical |
1a | 213011 | 86 | 30.337 | 4.5081 | 2.5641 | 0.64687 | 30.322 |
1b | 213011 | 202 | 27.613 | 6.0484 | 1.4527 | 0.57547 | 27.487 |
2a | 289669 | 82 | 30.403 | 4.5032 | 2.0693 | 0.7243 | 30.322 |
2b | 289669 | 132 | 27.472 | 6.0236 | 0.70678 | 0.62787 | 27.487 |
Case 1a
Residuals | ![]() |
Average outlet temperature | ![]() |
Average outlet velocity | ![]() |
Standard deviation of Temperature | ![]() |
Standard deviation of Velocity | ![]() |
Contour plots
Case 1b
Residuals | ![]() |
Average outlet temperature | ![]() |
Average outlet velocity | ![]() |
Standard deviation of Temperature | ![]() |
Standard deviation of Velocity | ![]() |
Contout plots
Case 2a
Residuals | ![]() |
Average outlet temperature | ![]() |
Average outlet velocity | ![]() |
Standard deviation of Temperature | ![]() |
Standard deviation of Velocity | ![]() |
Contour plot
s
Case 2b
Residuals | ![]() |
Average outlet temperature | ![]() |
Average outlet velocity | ![]() |
Standard deviation of Temperature | ![]() |
Standard deviation of Velocity | ![]() |
Contour plots
Effectiveness of Mixing
The high standard deviation implies better mixing. Observing the cases it shows that higher momentum ratio is giving lesser standard deviation
for cases 1a and 2a the SD is around 2 for Temperature.
But when Momentum ratio is 4 i.e., 1b and 2b standard deviation is less than the case 1a and 2a.
Case | Average Temperature | Average Velocity | Standard deviation Temperature | Standard deviation Velocity |
1a | 30.337 | 4.5081 | 2.5641 | 0.64687 |
1b | 27.613 | 6.0484 | 1.4527 | 0.57547 |
2a | 30.403 | 4.5032 | 2.0693 | 0.7243 |
2b | 27.472 | 6.0236 | 0.70678 | 0.62787 |
The length does not create any change in temperature.
When looking at the contour plots it is seen that the uniformity of temperature is better for long tee.
Conclusion:
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Week 1- Mixing Tee
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08 Jul 2023 06:07 PM IST
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