University of Anbar College of Engineering Mechanical Engineering Department Refrigeration & Air-Conditioning Laboratory Experiment No.1 Psychometric Process Cooling with Dehumidification By Mohammed Hashim Abdulhassan Supervisor Asst. Prof. Dr. Obaid T. Fadhil Turn in date 9/11/2022 Mechanical Engineering Department Air Conditioning Report Abstract The purpose of the experiment is to better understand how air conditioners work as well as how much heat and moisture is present in the air. In addition, the experiment enables students to understand and calculate the necessary heat exchanges to produce the desired air condition. Introduction Dry air (which includes gases like O2, N2, CO2, etc.) and water vapor are combined to create moist air. A psychrometric chart is a useful tool for researching and examining the thermodynamic characteristics of wet air. Air conditioning is necessary to provide thermal comfort cooling in occupied environments. The methods of air conditioning can include sensible heating or cooling, dehumidifying, humidifying, etc. depending on the interior requirement and the indoor temperature. This experiment aims to demonstrate the practical applications of the psychrometric chart and to investigate some of the air conditioning processes from the viewpoint of thermodynamics. Objectives • To study the components of air conditioning systems. • To carry out performance test on typical air conditioning processes. Page | 1 Mechanical Engineering Department Air Conditioning Report Theory and Principles The cooling and dehumidifying process is one of the fundamental air conditioning techniques that is widely used in hot, humid locations. Utilizing a cooling coil, this process is accomplished. Direct expansion (DX) type or chilled water type cooling coils are both options. To chill and dehumidify moist air, it must pass over a cooling coil whose surface temperature is lower than the incoming air's dew point temperature or equal to it. Two thermometers are installed at each condition in our experimental unit to measure the temperatures of the dry and wet bulbs. This will make it simpler to find the states on the map. The air system is set up as a once-through configuration because the air damper is closed. Equipment and Instruments • A660 Air Conditioning Laboratory Unit Fig.1 • Sling psychrometer Procedure Turn on the main power switch of the unit and adjust a fan speed around medium level. Start the refrigeration circuit turning on its switch. Increase the power inputs of Preheater, Re-heater and Boiler from minimum to maximum for each test. Collect the data which are seen on the observation sheet while the system is running. Page | 2 Mechanical Engineering Department Air Conditioning Report Fig. 1 Fig. 2 Page | 3 Mechanical Engineering Department Air Conditioning Report Calculations and Results πΈπΉπ = πΜπ (ππ − ππ ) … … … … . . πππ. π πΈπΉπ = πΜπ (ππ − ππ ) … … … … . . πππ. π πΜπ = πΜπ (ππ − ππ ) … … … … . . πππ. π Where W1 , W2 : moisture content for outlet and inlet πππππππ πππππ Because of losses Q1 ≠ Q2 πΜπ = π. πππππ√π ∗ ππ … … … … . . πππ. π ππ = 1 … … … … . . πππ’. 5 π£π Readings 1 2 Manometer H (mmH2O) 6.6 4.6 db 30 31 wb 19.1 17 db 23 21 wb 14 14.9 Cooling liquid mass flow rate mΜr (g/s) 17 16.8 Cooling liquid pressure after condenser Pc (Kpa) 1260 1240 Cooling liquid pressure after evaporator Pe (Kpa) 295 270 Cooling liquid Temperature before condenser tc (°C) 43 49 Cooling liquid Temperature after evaporator te (°C) 9 9 Inlet air Temperature (°C) Outlet air Temperature (°C) Page | 4 Mechanical Engineering Department Air Conditioning Report From psychometric chart for first readings at (tdb ,twb) and crossing the readings: h2 = 41 kj/kg ,h1 = 53.5 kj/kg ,π€1 = 9.4 ∗ 10−3 , π€2 = 7.3 ∗ 10−3 1 1 π£ 0.848 H = 6.6 mmH2O , ππ = = From equ.4 = 1.179 ππ π3 πΜπ = 0.05048 √6.6 ∗ 1.179 = 0.152899 ππ π ∴ ππ 1 = πΜπ (β1 − β2 ) = 0.152899(53.5 − 41) = 1.911 ππ€ ππ€ = ππ (π€1 − π€2 ) = 1.911(9.4 − 7.3) ∗ 10−3 = 4.0131 ∗ 10−3 ππ π And similarly, for second readings h1 = 48 kj/kg ,h2 = 42 kj/kg ,π€1 = 6.4 ∗ 10−3 ,π€2 = 8.3 ∗ 10−3 1 1 π£ 0.848 H = 4.6 mmH2O , ππ = = From equ.4 = 1.179 ππ π3 πΜπ = 0.05048 √4.6 ∗ 1.179 = 0.14678 ππ π ∴ ππ 1 = πΜπ (β1 − β2 ) = 0.14678(48 − 42) = 0.88068 ππ€ ππ€ = ππ (π€1 − π€2 ) = 0.14678(6.4 − 8.3) ∗ 10−3 = −2.78882 ∗ 10−4 ππ π From R12 Table after the condenser for first readings at (tdb ,twb) hb = 242.2 kj/kg ,ha = 356.7 kj/kg from equ.2 ππ 2 = πΜπ (βπ − βπ ) = 17 ∗ 10−3 (356.7 − 242.2) = 1.94 ππ€ And similarly, for second readings hb = 220.3 kj/kg ,ha = 356.7 kj/kg ππ 2 = πΜπ (βπ − βπ ) = 16.8 ∗ 10−3 (356.7 − 220.3) = 2.29 ππ€ Page | 5 Mechanical Engineering Department Air Conditioning Report Discussion The results of the tests demonstrate that there is a considerable difference in the air qualities before and after the cooling coil, with the enthalpy before the coil being (53.5 KJ/kg) and after the coil being (41 KJ/kg) for the first measurement, and when converted into a percentage it becomes β1 −β2 β1 = 53.5−41 53.5 ∗ 100% = 23.36% For the first reading and the second reading, there is a 23% difference. β1 − β2 48 − 42 = ∗ 100% = 12.5% β1 48 The same happens for the second measurement the difference is 12.5% . We can also see the heat rejected from the air and taken by the cooling liquid, indicating that there is a difference in heat exchange rate which shows the actual work of the cooling system. And that is the expected outcome that the air became cooler and less humid. Because of various flaws and uncertainties, the results obtained were not reliable. However, it can be said that the experiment's primary goal was met and that a complete understanding of the air conditioning system, the refrigeration cycle, and heat transfer was acquired. Page | 6