•  Home  •  Thesis  •  Incubus Fan Site  •  E-mail US  •

Menu

 Home
 Main

 Webmaster
 Thesis
 Misamis University 

     Mechanical Engineering
 Incubus Fan Site
 Web Links


 Thesis
 Abstract
 Title Page    

 Approval Sheet

 Acknowledgment

 Table of Contents

 List of Figures & Graphs

 Chapter I 

     Introduction

 Chapter II 

     Review of Related 

     Literature

 Chapter III 

     Theoretical Framework

 Chapter IV 

     Methodology

 Chapter V 

    Results and Discussions

 Chapter VI 

    Conclusions &  

    Recommendations

 Bibliography

 Appendices


  Guestbook

 Sign Guestbook

 View Guestbook

 

.: E-mail US :.  

THESIS 

 

Prepared and Submitted 

by 

Emmanuel M. Galleros 

Medandro Singidas

 

PROF. KARL EMPESO, MSME

Adviser

 A STUDY AND EVALUATION OF ADIABATIC SATURATION PROCESS

CHAPTER V

RESULTS AND DISCUSSIONS

            

            The performance of the adiabatic saturator was studied and evaluated. Results and data were gathered and recorded after a series of preliminary testing basing on the procedures that were presented in the earlier chapter. 

 

            Air that enters the saturator being the unsaturated air becomes saturated as it passes the re-circulated water and this process is believed to be adiabatic process. The saturated air having a lower temperature compared to the unsaturated air because it is said that when air is passed through the re-circulating water spray as shown in Figure 5 & 7 the adiabatic process reduces the air temperature and will pick up moisture causing it to fall in temperature. 

 

Figure 6 shows the adiabatic saturation process as water is sprayed, recycled and collected in the basin. A continuous flow of recycled water was evaluated for 5 days and at least 5 hours each day. Data such as the ambient temperature (unsaturated air), water temperature (wet bulb temperature) and the exhaust temperature (saturated air) are gathered and recorded every hour. Results were each compared to determine if a change or adiabatic cooling is achieved. 

 

The water spray shown in Figure 7 saturates the air. Some time after starting the equipment, when equilibrium exists, the water leaves the chamber at the same temperature at which it enters. The temperature of the water in the adiabatic saturator is the same as to temperature of the droplet of water and of the wet bulb thermometer when the thermometer is in contact with a stream of air.


Figure 5. Plastic water pipe used to spray re-cycled water.

 

Figure 6. Adiabatic Saturator without cover.

 

Figure 7. Adiabatic Saturator with cover.

 

5.1            Discussions and Results

 

On the first day that we have tested the adiabatic saturator we turned the power on for the water pump and the re-circulated water was sprayed. The fan was turned on then it started to suck and collect saturated air that passed through the water spray. During the first hour of our experiment, the reading was 26.67 °C ambient temperature, 26.11 °C for the water temperature, which is the wet bulb temperature and the exhaust air, had the temperature of 26.48 °C is our saturated air. For five hours the ambient temperature remained constant while the wet bulb temperature ranges from 26.11 °C to 23.9 °C and the exhaust temperature having a reading from 26.48 °C to 25 °C which is showed in Graph 1 or Table 1.

 

          On the second day, same process was done and this time with an ambient temperature of 28 °C which remained constant for 5 hours. Graph 2 or Table 2shows the falling of temperature as water was continuously sprayed in hours. There’s almost a point were the water temperature is almost identical as the exhaust temperature with very little difference during the first two hours. As the process was continued it shows that exhaust temperature was dropping and making it more cooler comparing to the ambient temperature.

 

          During the third day of our evaluation of the adiabatic saturator with the ambient temperature at 27 °C that remained the same for the next 5 hours with a reduction of 1.6 °C in temperature. Graph 3 or Table 3 shows that wet bulb temperature is always lower compared to exhaust temperature. As the re-circulated water continuously sprayed there is also a continuous falling of the temperature in the wet bulb temperature and exhaust temperature.

 

          Fourth day of evaluation with a starting ambient temperature of 27.79 °C and an increased to 28 °C during the next hour which stayed the same for the next 4 hours. A falling of temperature from 27.5 °C to 25 °C was achieved during 5 hours of observation. Graph 4 or Table 4revealed that there is little difference between the wet bulb and exhaust temperature but never with of the same reading because as mentioned in earlier chapters, the wet bulb temperature has always the lowest temperature.

 

During our last evaluation of the adiabatic saturator with a starting ambient temperature of 30 °C that remained the same during the next 5 hours had an exhaust temperature reduction from 28.5 °C to 26.5 °C, with a total reduction of 2 °C. Graph 5 or Table 5 shows that even though the ambient temperature remained the same but there was still a continuous falling of temperature as the re-circulated water was continuously spraying. 

 

          Five days of evaluating, gathering, and recording data we have concluded that adiabatic saturation can achieve adiabatic cooling. Thus adiabatic saturator can provide comfort cooling.

CLICK HERE FOR THE GRAPHS


Sign Guestbook | View Guestbook

News

· Manila Bulletin
· 
Philippine Star

· Philippine Daily Inquirer
· 
Manila Times

· ABS-CBN News

Copyright Galleros Janno ©
.: E-mail US :.