Challenge

Simulating the mixing of hot and cold fluids in a Mixing Tee

OBJECTIVE: To study the effectivness of mixing of hot and clod fluids inside two different types of mixing tee for different Boundary conditions

CASE-1: SHORT MIXING TEE

Plots and contour using k-epsilon model

Momentum Ratio-2

                                                           Temperature Contour

                                                            Velocity Contour

Momentum Ratio-4

                                                          Temperature contour

                                                                 Velocity contour

Plots and contour using k-epsilon model

Momentum Ratio - 2

NOTE :We employed two distinct turbulence solvers for it: k-omega SST and realized k-epsilon.Since the answer was converged after only a few iterations using the k-epsilon model rather than the k-omega model, the outcomes in this case are better. In investigating fluid behavior close to walls, K-omega is preferable, however this is not the case here. Therefore, in future circumstances, the k-epsilon model is advised for the analysis of fluid in the flow zone that is far from the wall.

CASE-2: LONG MIXING TEE

Momentum Ratio-2

                                                                         Temperature Contour

                                                                                    Velocity Contour

Momentum Ratio-4

                                                                   Temperature Contour

                                                                       Velocity Contour

Results: The following table shows the different parameters obtained from the simulation of the two different mixing tees

CASE set up no. of cell count Averrage outlet temperarture (degree celcius) No. of iterations for convergence Standard deviation of temperature
short mixing tee, mr=2 14400 30.25 152 1.4
short mixing tee, mr=4 14400 27.54 350 1.6
Long mixing tee, mr=2 18069 30.28 150 1.5
Long mixing tee, mr=4 18069 27.5 191 0.65
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