Experimental Procedure and Design Simulation of Filing Sequence and Solidification Time for Cast Metal Matrix Composite by Low Pressure Die Casting.

Copyright © 2011 Praise Worthy Prize S.r.l. - All rights reserved International Review of Mechanical Engineering, Vol. 5, N. 2 Special Issue on Heat Transfer 281 The installation comprised two thermal solar collectors constructed of aluminum profile, with single cover glass and black-painted absorber plate, each of area 2,2 m². Solar collectors were oriented to south having tilt angle of 30 o with horizontal plane. They were also connected to a pump and a water storage tank of 1000 lt as shown in Fig. 1. They were also connected to boilers each of 132lt. Cold water supply to the system was achieved from the water storage tank through plastic tubes under forced circulation conditions open circuit. The return of hot water from the system to the same water storage tank was done under natural circulation conditions through well insulated plastic tubes. Anti-freeze solution was used in the closed circuit consisting of water and antifreeze chemical. 30.6l of PCM were placed inside the boiler of one of the solar collectors in 17 metal tubes of 0.95m length and 0.05m diameter with complement of 85 which were sealed to avoid possible leakages. The PCM used was paraffin. The thermo physical properties of the paraffin wax are given in Tables I, II. The insulation material of the boiler was glass wool. TABLE I P ROPERTIES O F M ATERIALS F OR B OTH B OILERS BOILER WITH PCM no Material Volume Density Mass Cp Heat fusion Heat capacity lt kg kJkgK kJkg kJK 1 Water 96,19 0,996 95,81 4,186 401,05 2 PCM 30,60 0,850 26,01 2,130 214 5621,54 3 Steel 5,21 7,850 40,87 0,480 19,62 Total 132,00 162,69 6042,21 Theoretical capacity for energy storage m x c +m x ∆Η x ∆ 3600 kWh 59,89 Experimental capacity for energy storage kWh 26,32 PCM fraction melted 39,15 26,32 PCM thermal diffusivity k ρ c 1,10E-07 BOILER WITHOUT PCM no Material Volume Density Mass Specific heat Heat of fusion Heat capacity lt kg kJkgK JK 1 water 132 0,996 131,47 4,186 550,34 Total 132 131,47 550,34 Theoretical capacity for energy storage m x c x ∆ 3600 5,22 Experimental capacity for energy storage kWh 5,22 TABLE II PCM T HERMOPHYSICAL P ROPERTIES Melting Temperature o C 58 Heat capacity kJkgK 2,13 Thermal conductivity WmK 0,2 Latent Heat kJkg 214 Solid density kgm 3 850 Liquid density kgm 3 775 Temperature was recorded at the open circuit inlet and outlet, closed circuit inlet and outlet, and inside the boiler as depicted in Fig. 1. The measurement system included T type thermocouples, two ADAM 4018 modules connected to a PC to enable the continuous recording of the temperature readings. A meteorological station was placed 5m away from the solar collectors measuring environmental temperature, relative humidity, direct and diffuse radiation, wind velocity and direction, total sunshine duration. Data recording has been scheduled every ten minutes. Pump’s flow rate of the open circuit was calculated 0,246m 3 h. The experiments were conducted during June at the campus. This site is located at 38°3440.42N and 23°3834.52E with an altitude of around 42 m. Table III shows meteorological data of the campus area. The climate at the campus area is typically Mediterranean and is characterized by around 2851h of sunshine per year. TABLE III M ETEOROLOGICAL D ATA O F T HE C AMPUS A REA M ea n da il y m in im u m a ir te m pe ra ture o C M ea n da il y m ax im u m a ir te m pe ra ture o C S uns hi ne dur at ion h m ont h S uns hi ne dur at ion h d ay Re la ti ve hum idi ty Irra d ia ti o n o f gl oba l r adi at ion hor iz ont al kW h m 2 Jan 3,6 11,9 135 4,4 79 63 Feb 3,3 13,6 142 5,1 75 70 Mar 5,1 16,0 186 6,0 69 107 Apr 8,1 19,8 236 7,9 64 154 May 12,9 25,3 299 9,7 58 193 Jun 16,4 30,1 339 11,3 52 205 Jul 19,1 32,6 371 12,0 50 215 Aug 18,9 32,1 352 11,3 52 197 Sep 15,2 28,2 281 9,4 59 154 Oct 11,6 22,6 216 7,0 69 98 Nov 8,0 17,5 160 5,3 77 62 Dec 5,4 13,5 133 4,3 79 48 Year 1561

IV. Experimental Procedure and

Calculations The experimental procedure lasts 24h and is divided in two stages, charging and discharging. The charging stage starts when both boilers have been filled with cold water from the water storage tank. This corresponds to about 09:00am in the morning when solar radiation Copyright © 2011 Praise Worthy Prize S.r.l. - All rights reserved International Review of Mechanical Engineering, Vol. 5, N. 2 Special Issue on Heat Transfer 282 significantly increases and lasts until the sunset. As solar radiation levels increase during the day, water temperature inside the boiler increases. Simultaneously, paraffin wax temperature increases. Paraffin begins to melt at 55-58 o C where latent heat storage begins. The latter heat will be emitted again to the water when paraffin will be solidified. As tubes material is of high thermal conductivity, it has been assumed that paraffin wax temperature does not deviate from that of water inside boiler. Discharging begins when solar radiation levels are low sunset, circuit valves open and hot water returns back to the water storage tank. It lasts until the end of the 24h cycle. During discharging stage water flows at the open circuit and temperature is recorded at its outlet. It is expected that the boiler with PCM will require more time to reduce water temperature in comparison with that of water at the boiler without PCM outlet as in the first case the PCM latent heat will be emitted again to the water when PCM will be solidified. For the evaluation of the system and the energy storage during charging and discharging stages the following calculations were applied: Charging w ,c ,b w ,o ,b st PCM ,S w,c,b P w,o,b P s ,ch ch st p PCM p sensible heat - PCM at solid state PCM L ,PCM latent heat absorption from PCM during its melting w,c,b m C m C T Q m C m C t m Q t m C + + ⎧ ⎫ ∆ ⎪ ⎪ = + ⎨ ⎬ + + ∆ ⎪ ⎪ ⎩ ⎭ + ∆ + + w,c ,b w ,o ,b st PCM ,L P w,o,b P l ,ch st p PCM p sensible heat - PCM at liquid state m C T m C m C t + + ⎧ ⎫ ∆ ⎪ ⎪ ⎨ ⎬ + + ∆ ⎪ ⎪ ⎩ ⎭ 3 where w,c,b m : is anti-freeze solution from closed circuit mass inside boiler kg, w,c ,b P C : is specific heat capacity of anti-freeze solution inside boiler JkgK, w,o,b m : is water mass from open circuit inside boiler kg, w,o ,b P C : is specific heat capacity of water mass from open circuit inside boiler JkgK, st m : is mass of steel tubes that contain PCM kg, st P C : is specific heat capacity of steel tubes that contain PCM JkgK, PCM m : is PCM mass kg, PCM ,S P C : is specific heat capacity of PCM at solid state JkgK, PCM ,L P C : is specific heat capacity of PCM at liquid state JkgK, L,PCM Q : is PCM heat of fusion Jkg, ∆T s,ch : is temperature difference during charging until PCM melting K, ∆T l,ch : is temperature difference after melting during charging where PCM is at liquid state K. Closed circuit: Heat inlet from closed circuit is calculated by: ch,c c p ,c c ch Q m C T t = ∆ ∆ 4 • c m , anti-freeze solution feed rate from closed circuit kgs • p ,c C , anti-freeze solution specific heat JkgK • ∆ Τ c , temperature change of anti-freeze solution boiler inlet-outlet – closed circuit Κ • ch t ∆ , charging time Open circuit: ch,o Q = Discharging w,c ,b w,o ,b st PCM ,L w,c,b P w,o,b P l ,dis st p PCM p sensible heat - PCM at liquid state PCM L,PCM latent heat emmision from PCM during its solidification m C m C T Q m C m C t m Q t + + ⎧ ⎫ ∆ ⎪ ⎪ = + ⎨ ⎬ + + ∆ ⎪ ⎪ ⎩ ⎭ − ∆ + + w ,c ,b w ,o ,b st PCM ,S w,c,b P w,o,b P s ,dis st p PCM p sensible heat - PCM at solid state m C m C T m C m C t + + ⎧ ⎫ ∆ ⎪ ⎪ ⎨ ⎬ + + ∆ ⎪ ⎪ ⎩ ⎭ 5 where w,c,b m : is anti-freeze solution mass inside boiler kg, w ,c ,b P C : is specific heat capacity of anti-freeze solution inside boiler JkgK, w,o,b m : is water mass from open circuit inside boiler kg, w ,o ,b P C : is specific heat capacity of water mass from open circuit inside boiler JkgK, st m : is mass of steel tubes that contain PCM kg, st P C : is specific heat capacity of steel tubes that contain PCM JkgK, PCM m : is PCM mass kg, PCM ,S P C : is specific heat capacity of PCM at solid state JkgK, PCM ,L P C : is specific heat capacity of PCM at liquid state JkgK, L,PCM Q : is PCM heat of fusion Jkg, ∆T s,dis : temperature difference for a certain time period ∆t during discharging after PCM solidification K, ∆T l,dis : temperature difference after melting during discharging where PCM is at liquid state K Open circuit: dis,o o p ,o o dis Q m C T t = ∆ ∆ Copyright © 2011 Praise Worthy Prize S.r.l. - All rights reserved International Review of Mechanical Engineering, Vol. 5, N. 2 Special Issue on Heat Transfer 283 • o m , water feed rate discharging at the open circuit kgs • p ,o C , water specific heat at the open circuit JkgK • ∆ Τ ο , water temperature change at the open circuit boiler inlet-outlet- open circuit Κ • dis t ∆ , discharging time Closed circuit: dis ,c Q =

V. Results and Discussion