Document ZndmMN0aaZ0OpZKL9q2oZBGQZ

ni i 22 CHAPTER 2 1952 Guide 76. Scale Trap 80.6 Evaporator Pressure -Q-. Regulating, Throt tling Type (Evapo rator Side)' 77.' Spray Pond 78. Thermal Bulb 79..Thermostat (Remote .... Bulb) . 80. Valves ..80.L Automatic Expan sion 80.2 Compressor. Suction ' Pressure Limiting, : Throttling Type (Compressor Side) 80.3 Constant Pressure, Suction 80.4 Evaporator Pressure Regelating, Snap Action 80.5 Evaporator Pressure iRegulating, Thermo static Throttling Type ^1 80.7 Hand Expansion 80.8 Magnetic Stop 80.9 Snap Action 80.10 Suction Vapor Regulating 80.11 Thermo Suction 80.12 Thermostatic Ex pansion 80.13 Water 81. Vibration Absorber* Line (m) IDENTIFICATION OF PIPING SYSTEMS BY COLOR The color scheme for identification of piping systems, based on material carried,'as listed, in the following table and shown in Fig. 1, is reprinted from1 Part V, Fourth Edition, of the Engineering Standards of the Heat ing, Pi-ping and Air Conditioning Contractors National AssociationJ Class F--Fire-protection D--Dangerous materials S--Safe Materials and, when required . P--Protective materials , V--Extra valuable materials CoLOB Red Yellow or Orange Green (or the achromatic black, gray or aluminum) colors, white, Bright blue Deep purple ----------- Stfi Fig. 1. Main Classification by Colob * See Scheme for Identification of Piping Systems. A13-1928, American Standard) Aesociation. CHAPTER 3 THERMODYNAMICS Mass and Energy Balances; Thermodynamic Properties of Moist Air; Formulas and Tables; Thermodynamic Properties of Water, Formulas and Tables; Degree of Saturation; A.S.H.V.E. Psychrometric Chart; Solution of Air Conditioning Problems by Use of Tables and Psychrometric Chart; U. S. Standard Atmosphere - 1 THERMODYNAMICS is that, branch of natural science which deals with energy and its transformations into various forms. In this chap ter the discussion will be limited to thermodynamics as it affects the. arts of heating and air conditioning. This will necessarily presume some knowledge of the fundamentals of the science on the part of the reader who.may also find it desirable to refer to a standard text on the subject, preferably one published after 1930. MASS AND ENERGY BALANCES The First Law of Thermodynamics is a . statement of the'Principle of Conservation of Energy. It may be stated as follows: The energy added to a system is equal to the increase or decrease of the energy stored in the system, plus the energy which leaves the system. For a completely contained, or non-flow system, this may be restated as: The heat added to a non-flow system is equal to .the change in the internal energy of the system, plus the work done by the system. iq = Ut -- Ui + w (1) For a constant pressure process where iq> = Hi -- Hj -. (2) iq> = energy added between points 1 and 2. U = internal energy of system, w = work done by syBtem. . H = enthalpy of system. Subscripts 1 and 2 refer to sections of the system between which a change takes place. For engineering problems, a more important application of the. First Law is its use in cases in which, in addition to energy, one or more fluids aje crossing the boundaries of the syBtem. The most simple of- these is the steady flow system, in which the.rates of energy and mass flow across the boundaries of the system are constant, and no mass or energy is stored or released by the system. Consider a system as illustrated in Fig. 1. The fluid crossing the boundaries of the system carries with it potential energy by reason of its elevation above some convenient datum, kinetic energy by reason of its 23