CFD2011 03 GTK NA62Micro channel Parametric study using

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CFD-2011 -03 -GTK NA-62(Micro channel) Parametric study using Empirical Results June 30 th 2011

CFD-2011 -03 -GTK NA-62(Micro channel) Parametric study using Empirical Results June 30 th 2011 Bdg 298 Enrico Da Riva, Vinod Singh Rao Enrico Da Riva , V. Rao 30 th June 2011 1

Estimation of the pressure drop in the Microchannel device PDdevice = PDmanifold + PDmicrochannels+

Estimation of the pressure drop in the Microchannel device PDdevice = PDmanifold + PDmicrochannels+ PDpipe where PD : Pressure Drop Enrico Da Riva , V. Rao 30 th June 2011 2

Estimation of pressure drop in manifold The pressure drop in a fluid flow is

Estimation of pressure drop in manifold The pressure drop in a fluid flow is proportional to the dynamic pressure as given by the relation: The value of K(=3*2. 1) is chosen according to the experimental data provided @15°C to obtain the pressure drop @ -25°C Enrico Da Riva , V. Rao 30 th June 2011 3

Estimation of pressure drop in the microchannel The pressure drop across the microchannel and

Estimation of pressure drop in the microchannel The pressure drop across the microchannel and the inlet-outlet pipe is calculated using churchill correlations flow in tubes. where Re : Reynolds number f: friction factor where Enrico Da Riva , V. Rao 30 th June 2011 L: Length w: Mass flow rate D: hydraulic diameter 4

Dimensions and flow regime in the microchannels Number of microchannels: 300 Length of microchannel:

Dimensions and flow regime in the microchannels Number of microchannels: 300 Length of microchannel: 40 mm Depth of microchannel: 100µm Width of channel: 100µm Mass flow rate: 7 g/s Density @ 15°C : 1700. 85 Kg/m 3 Kinematic viscosity @ 15°C : . 425 c. St Inlet velocity: 1. 75 m/s Inlet Reynolds number: 410. 99 Density @ -25°C : 1805. 25 Kg/m 3 Kinematic viscosity @ -25°C : . 8 c. St Inlet velocity: 1. 65 m/s Inlet Reynolds number: 205. 71 » Flow is laminar in the microchannels Enrico Da Riva , V. Rao 30 th June 2011 5

Effect of the mass flow rate on Pressure drop across the microchannels 5. 00

Effect of the mass flow rate on Pressure drop across the microchannels 5. 00 E+000 Pressure drop variation with mass flow rate 4. 50 E+000 4. 00 E+000 pressure drop(bars) 3. 50 E+000 3. 00 E+000 Temp=10 C Temp=15 C 2. 50 E+000 Temp=25 C 2. 00 E+000 Temp=-25 C 1. 50 E+000 1. 00 E+000 5. 00 E-001 0. 00 E+000 2. 00 E+000 4. 00 E+000 6. 00 E+000 8. 00 E+000 mass flow rate (g/sec) 1. 00 E+001 1. 20 E+001 The pressure drop varies linearly with the mass flow rate in the laminar region. The variation of the kinematic viscosity with temperature also has a huge effect on the pressure drop. The pressure drop at a lower temperature is quite high as compared to the higher temperature with same mass flow rate. Enrico Da Riva , V. Rao 30 th June 2011 6

Effect of the microchannel dimension/Number of microchannels on Pressure drop across the microchannels Length

Effect of the microchannel dimension/Number of microchannels on Pressure drop across the microchannels Length of microchannel: 40 mm Depth of microchannel: 100µm Fin-width: 100µm Mass flow rate: 7 g/sec 1. 20 E+001 pressure drop with number of channels pressure drop (bars) 1. 00 E+001 8. 00 E+000 Temp=-25 Temp=10 6. 00 E+000 Temp=15 Temp=25 4. 00 E+000 2. 00 E+000 0. 00 E+000 5. 00 E+001 1. 00 E+002 1. 50 E+002 2. 00 E+002 2. 50 E+002 3. 00 E+002 3. 50 E+002 4. 00 E+002 4. 50 E+002 number of channels Increasing the number of channels with fin-width constant increases the pressure drop exponentially as the hydraulic diameter decreases quite fast. Enrico Da Riva , V. Rao 30 th June 2011 7

Effect of the microchannel dimension/Number of microchannels on Pressure drop across the microchannels Length

Effect of the microchannel dimension/Number of microchannels on Pressure drop across the microchannels Length of microchannel: 40 mm Depth of mircochannel: 100µm Microchannel-width: 100µm Mass flow rate: 7 g/sec 5. 00 E+000 pressure drop variation with number of channels 4. 50 E+000 pressure drop(bars) 4. 00 E+000 3. 50 E+000 Temp=-25 3. 00 E+000 Temp=10 2. 50 E+000 Temp=15 2. 00 E+000 Temp=25 1. 50 E+000 1. 00 E+000 5. 00 E-001 0. 00 E+000 5. 00 E+001 1. 00 E+002 1. 50 E+002 2. 00 E+002 2. 50 E+002 3. 00 E+002 3. 50 E+002 4. 00 E+002 4. 50 E+002 number of channels Increasing the number of channels with channel width constant decreases the pressure drop as there is smaller mass flow rate in each channel. Enrico Da Riva , V. Rao 30 th June 2011 8

Effect of the mass flow rate on Pressure drop across the manifold Inlet mass

Effect of the mass flow rate on Pressure drop across the manifold Inlet mass flow rate: 7 g/s Inlet diameter: 1. 4 mm Manifold cross section: 280µm X 1. 7 mm Density @ 15°C : 1700. 85 Kg/m 3 Kinematic viscosity @ 15°C : . 425 c. St Inlet velocity: 2. 67 m/s Inlet Reynolds number: 8806. 94 Manifold velocity: 8. 64 m/s Manifold Reynolds number: 9781. 55 Density @ -25°C : 1805. 25 Kg/m 3 Kinematic viscosity @ -25°C : . 8 c. St Inlet velocity: 2. 51 m/s Inlet Reynolds number: 4408. 11 Manifold velocity: 8. 14 m/s Manifold Reynolds number: 4895. 93 Flow is turbulent in the manifold Enrico Da Riva , V. Rao 30 th June 2011 9

Effect of the mass flow rate on Pressure drop across the manifold Dimensions: Inlet

Effect of the mass flow rate on Pressure drop across the manifold Dimensions: Inlet diameter of the pipe: 1. 4 mm Depth of the manifold: 280 µm Width of the manifold: 1. 7 mm 12 Total pressure drop variation with mass flow pressure drop(bar) 10 8 calc. totalpressure drop 6 Corrected pressure drop(experimental) 4 2 0 0. 00 E+000 2. 00 E+000 4. 00 E+000 6. 00 E+000 8. 00 E+000 mass flow(g/sec) 1. 00 E+001 1. 20 E+001 Temperature: 15°C Enrico Da Riva , V. Rao 30 th June 2011 10

Effect of the mass flow rate on Pressure drop across the manifold. Pressure drop

Effect of the mass flow rate on Pressure drop across the manifold. Pressure drop variation with mass flow @ 15°C 1. 20 E+001 pressure drop(bar) 1. 00 E+001 8. 00 E+000 channels manifold 6. 00 E+000 calc. totalpressure drop 4. 00 E+000 2. 00 E+000 0. 00 E+000 2. 00 E+000 4. 00 E+000 6. 00 E+000 8. 00 E+000 1. 00 E+001 1. 20 E+001 mass flow(g/sec) Enrico Da Riva , V. Rao 30 th June 2011 11

Effect of the mass flow rate on Pressure drop across the manifold. Pressure drop

Effect of the mass flow rate on Pressure drop across the manifold. Pressure drop variation with mass flow rate @ -25°C 14 12 pressure drop(bars) 10 8 manifold Pressure drop channel Pressure drop total pressure drop 6 4 2 0 0. 00 E+000 2. 00 E+000 4. 00 E+000 6. 00 E+000 8. 00 E+000 mass flow(g/sec) 1. 00 E+001 1. 20 E+001 With decrease in temperature , the pressure drop in microchannel become more prominent but for the current operating point, manifold pressure drop is quite important. Enrico Da Riva , V. Rao 30 th June 2011 12

Effect of the mass flow rate on Pressure drop across the inlet-outlet pipes. pressure

Effect of the mass flow rate on Pressure drop across the inlet-outlet pipes. pressure drop in pipe @15 °C 0. 7 pressure drop (bars) 0. 6 0. 5 0. 4 pressure drop in pipe(data from georg) pressure drop in pipe calculated 0. 3 0. 2 0. 1 0 0 1 Enrico Da Riva , V. Rao 2 3 mass flow(g/sec) 4 30 th June 2011 5 6 13

Effect of the mass flow rate on Pressure drop across the Pipes. pressure drop

Effect of the mass flow rate on Pressure drop across the Pipes. pressure drop in pipe @ -25 °C 1. 60 E+000 1. 40 E+000 pressure drop (bars) 1. 20 E+000 1. 00 E+000 pressure drop in pipe 8. 00 E-001 6. 00 E-001 4. 00 E-001 2. 00 E-001 0. 00 E+000 2. 00 E+000 4. 00 E+000 6. 00 E+000 mass flow(g/sec) 8. 00 E+000 1. 00 E+001 1. 20 E+001 The change in the steepness of the curve may be due to the transition from laminar region to turbulent flow. Enrico Da Riva , V. Rao 30 th June 2011 14

Conclusions & Suggestions 1. ) The pressure drop in the manifold would be dominant

Conclusions & Suggestions 1. ) The pressure drop in the manifold would be dominant at the design temperature and design mass flow rate. 2. ) The problem is due to the small cross section of the manifold. 3. ) Before looking at the microchannels, we must work on the manifold. 4. ) Temperature has a strong influence on the pressure drop in the microchannel, but this is not so important with the present design since the dominant pressure drop is in the manifold. 5. ) Using multiple inlet-outlet system to reduce pressure drop in the manifold. Enrico Da Riva , V. Rao 30 th June 2011 15

Pressure drop with dual inlet-outlet Working fluid perflourohexane @Temperature -25 °C Mass flow: 7

Pressure drop with dual inlet-outlet Working fluid perflourohexane @Temperature -25 °C Mass flow: 7 g/s or 2*3. 5 g/s Manifold velocity: 4. 07 m/s Inlet velocity: 1. 25 m/s Manifold Reynolds number: 2447 Inlet Reynolds number: 2204 Enrico Da Riva , V. Rao 30 th June 2011 16

Pressure drop with dual inlet-outlet Pressure drop variation with mass flow rate 7 6

Pressure drop with dual inlet-outlet Pressure drop variation with mass flow rate 7 6 5 4 manifold Pressure drop channel Pressure drop total pressure drop(bars) 3 2 1 0 0. 00 E+000 2. 00 E+000 4. 00 E+000 6. 00 E+000 mass flow(g/sec)8. 00 E+000 1. 00 E+001 1. 20 E+001 The required pressure drop for mass flow rate of 7 g/s is about 4 bar Enrico Da Riva , V. Rao 30 th June 2011 17

Heat transfer coefficient For laminar flow Nusselt number : 3. 2 Hydraulic diameter of

Heat transfer coefficient For laminar flow Nusselt number : 3. 2 Hydraulic diameter of channels : 100 µm Thermal conductivity of Perflourohexane @ -25 °C: . 06275 W/(m-k) Heat transfer coefficient (Perflourohexane): 2008 W/(m 2 k) Enrico Da Riva , V. Rao 30 th June 2011 18