Vapour Absorption Refrigeration Systems Based on Ammonia- Water Pair
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Chapter 8 and 9 – Energy Balances
CBE2124, Levicky Chapter 8 and 9 – Energy Balances Reference States . Recall that enthalpy and internal energy are always defined relative to a reference state (Chapter 7). When solving energy balance problems, it is therefore necessary to define a reference state for each chemical species in the energy balance (the reference state may be predefined if a tabulated set of data is used such as the steam tables). Example . Suppose water vapor at 300 oC and 5 bar is chosen as a reference state at which Hˆ is defined to be zero. Relative to this state, what is the specific enthalpy of liquid water at 75 oC and 1 bar? What is the specific internal energy of liquid water at 75 oC and 1 bar? (Use Table B. 7). Calculating changes in enthalpy and internal energy. Hˆ and Uˆ are state functions , meaning that their values only depend on the state of the system, and not on the path taken to arrive at that state. IMPORTANT : Given a state A (as characterized by a set of variables such as pressure, temperature, composition) and a state B, the change in enthalpy of the system as it passes from A to B can be calculated along any path that leads from A to B, whether or not the path is the one actually followed. Example . 18 g of liquid water freezes to 18 g of ice while the temperature is held constant at 0 oC and the pressure is held constant at 1 atm. The enthalpy change for the process is measured to be ∆ Hˆ = - 6.01 kJ. -
A Comparative Energy and Economic Analysis Between a Low Enthalpy Geothermal Design and Gas, Diesel and Biomass Technologies for a HVAC System Installed in an Office Building
energies Article A Comparative Energy and Economic Analysis between a Low Enthalpy Geothermal Design and Gas, Diesel and Biomass Technologies for a HVAC System Installed in an Office Building José Ignacio Villarino 1, Alberto Villarino 1,* , I. de Arteaga 2 , Roberto Quinteros 2 and Alejandro Alañón 1 1 Department of Construction and Agronomy, Construction Engineering Area, High Polytechnic School of Ávila, University of Salamanca, Hornos Caleros, 50, 05003 Ávila, Spain; [email protected] (J.I.V.); [email protected] (A.A.) 2 Facultad de Ingeniería, Escuela de Ingeniería Mecánica, Pontificia Universidad Católica de Valparaíso, Av. Los Carrera 01567, Quilpué 2430000, Chile; [email protected] (I.d.A.); [email protected] (R.Q.) * Correspondence: [email protected]; Tel.: +34-920-353-500; Fax: +34-920-353-501 Received: 3 January 2019; Accepted: 25 February 2019; Published: 6 March 2019 Abstract: This paper presents an analysis of economic and energy between a ground-coupled heat pump system and other available technologies, such as natural gas, biomass, and diesel, providing heating, ventilation, and air conditioning to an office building. All the proposed systems are capable of reaching temperatures of 22 ◦C/25 ◦C in heating and cooling modes. EnergyPlus software was used to develop a simulation model and carry out the validation process. The first objective of the paper is the validation of the numerical model developed in EnergyPlus with the experimental results collected from the monitored building to evaluate the system in other operating conditions and to compare it with other available technologies. The second aim of the study is the assessment of the position of the low enthalpy geothermal system proposed versus the rest of the systems, from energy, economic, and environmental aspects. -
A Comprehensive Review of Thermal Energy Storage
sustainability Review A Comprehensive Review of Thermal Energy Storage Ioan Sarbu * ID and Calin Sebarchievici Department of Building Services Engineering, Polytechnic University of Timisoara, Piata Victoriei, No. 2A, 300006 Timisoara, Romania; [email protected] * Correspondence: [email protected]; Tel.: +40-256-403-991; Fax: +40-256-403-987 Received: 7 December 2017; Accepted: 10 January 2018; Published: 14 January 2018 Abstract: Thermal energy storage (TES) is a technology that stocks thermal energy by heating or cooling a storage medium so that the stored energy can be used at a later time for heating and cooling applications and power generation. TES systems are used particularly in buildings and in industrial processes. This paper is focused on TES technologies that provide a way of valorizing solar heat and reducing the energy demand of buildings. The principles of several energy storage methods and calculation of storage capacities are described. Sensible heat storage technologies, including water tank, underground, and packed-bed storage methods, are briefly reviewed. Additionally, latent-heat storage systems associated with phase-change materials for use in solar heating/cooling of buildings, solar water heating, heat-pump systems, and concentrating solar power plants as well as thermo-chemical storage are discussed. Finally, cool thermal energy storage is also briefly reviewed and outstanding information on the performance and costs of TES systems are included. Keywords: storage system; phase-change materials; chemical storage; cold storage; performance 1. Introduction Recent projections predict that the primary energy consumption will rise by 48% in 2040 [1]. On the other hand, the depletion of fossil resources in addition to their negative impact on the environment has accelerated the shift toward sustainable energy sources. -
Cryogenicscryogenics Forfor Particleparticle Acceleratorsaccelerators Ph
CryogenicsCryogenics forfor particleparticle acceleratorsaccelerators Ph. Lebrun CAS Course in General Accelerator Physics Divonne-les-Bains, 23-27 February 2009 Contents • Low temperatures and liquefied gases • Cryogenics in accelerators • Properties of fluids • Heat transfer & thermal insulation • Cryogenic distribution & cooling schemes • Refrigeration & liquefaction Contents • Low temperatures and liquefied gases ••• CryogenicsCryogenicsCryogenics ininin acceleratorsacceleratorsaccelerators ••• PropertiesPropertiesProperties ofofof fluidsfluidsfluids ••• HeatHeatHeat transfertransfertransfer &&& thermalthermalthermal insulationinsulationinsulation ••• CryogenicCryogenicCryogenic distributiondistributiondistribution &&& coolingcoolingcooling schemesschemesschemes ••• RefrigerationRefrigerationRefrigeration &&& liquefactionliquefactionliquefaction • cryogenics, that branch of physics which deals with the production of very low temperatures and their effects on matter Oxford English Dictionary 2nd edition, Oxford University Press (1989) • cryogenics, the science and technology of temperatures below 120 K New International Dictionary of Refrigeration 3rd edition, IIF-IIR Paris (1975) Characteristic temperatures of cryogens Triple point Normal boiling Critical Cryogen [K] point [K] point [K] Methane 90.7 111.6 190.5 Oxygen 54.4 90.2 154.6 Argon 83.8 87.3 150.9 Nitrogen 63.1 77.3 126.2 Neon 24.6 27.1 44.4 Hydrogen 13.8 20.4 33.2 Helium 2.2 (*) 4.2 5.2 (*): λ Point Densification, liquefaction & separation of gases LNG Rocket fuels LIN & LOX 130 000 m3 LNG carrier with double hull Ariane 5 25 t LHY, 130 t LOX Air separation by cryogenic distillation Up to 4500 t/day LOX What is a low temperature? • The entropy of a thermodynamical system in a macrostate corresponding to a multiplicity W of microstates is S = kB ln W • Adding reversibly heat dQ to the system results in a change of its entropy dS with a proportionality factor T T = dQ/dS ⇒ high temperature: heating produces small entropy change ⇒ low temperature: heating produces large entropy change L. -
Matching Energy Consumption and Photovoltaic Production in a Retrofitted Dwelling in Subtropical Climate Without a Backup System
energies Article Matching Energy Consumption and Photovoltaic Production in a Retrofitted Dwelling in Subtropical Climate without a Backup System Sergio Gómez Melgar 1,* , Antonio Sánchez Cordero 2 , Marta Videras Rodríguez 2 and José Manuel Andújar Márquez 1 1 TEP192 Control y Robótica, Escuela Técnica Superior de Ingeniería, Universidad de Huelva, CP. 21007 Huelva, Spain; [email protected] 2 Programa de Ciencia y Tecnología Industrial y Ambiental, Escuela Técnica Superior de Ingeniería, Universidad de Huelva, CP. 21007 Huelva, Spain; [email protected] (A.S.C.); [email protected] (M.V.R.) * Correspondence: [email protected] Received: 4 October 2020; Accepted: 16 November 2020; Published: 18 November 2020 Abstract: The construction sector is a great contributor to global warming both in new and existing buildings. Minimum energy buildings (MEBs) demand as little energy as possible, with an optimized architectural design, which includes passive solutions. In addition, these buildings consume as low energy as possible introducing efficient facilities. Finally, they produce renewable energy on-site to become zero energy buildings (ZEBs) or even plus zero energy buildings (+ZEB). In this paper, a deep analysis of the energy use and renewable energy production of a social dwelling was carried out based on data measurements. Unfortunately, in residential buildings, most renewable energy production occurs at a different time than energy demand. Furthermore, energy storage batteries for these facilities are expensive and require significant maintenance. The present research proposes a strategy, which involves rescheduling energy demand by changing the habits of the occupants in terms of domestic hot water (DHW) consumption, cooking, and washing. -
Installation, Setup & Troubleshooting Supplement
EconoMi$er X F a c t o r y --- I n s t a l l e d O p t i o n Low Leak Economizer for 2 Speed SAV (Staged Air Volume) Systems Installation, Setup & Troubleshooting Supplement This document is a supplemental installation instruction for the factory-installed EconoMi$er X (low leak economizer) option. It is to be used with the base unit Installation Instructions for 48/50TC, 50TCQ, 48/50HC, and 50HCQ 2-Stage cooling units, sizes 08 – 30. Units equipped with the EconoMi$er X option are identified by an indicator in the unit's model number (see the unit's nameplate). Use Table 1 (on page 2) to identify whether or not a given unit is equipped with the factory-installed EconoMi$er X. NOTE: Read the entire instruction manual before starting the installation. TABLE OF CONTENTS SAFETY CONSIDERATIONS SAFETY CONSIDERATIONS.................... 1 Improper installation, adjustment, alteration, service, maintenance, or use can cause explosion, fire, electrical GENERAL.................................... 2 shock or other conditions which may cause personal injury Identifying Factory Option...................... 2 or property damage. Consult a qualified installer, service EconoMi$er X................................ 3 agency, or your distributor or branch for information or assistance. The qualified installer or agency must use W7220 Economizer Controller................... 3 factory--authorized kits or accessories when modifying this User Interface................................ 3 product. Refer to the individual instructions packaged with Menu Structure............................... 3 the kits or accessories when installing. Checkout Tests............................... 7 Follow all safety codes. Wear safety glasses and work gloves. Use quenching cloths for brazing operations and SETUP AND CONFIGURATION................ -
Thermodynamics the Study of the Transformations of Energy from One Form Into Another
Thermodynamics the study of the transformations of energy from one form into another First Law: Heat and Work are both forms of Energy. in any process, Energy can be changed from one form to another (including heat and work), but it is never created or distroyed: Conservation of Energy Second Law: Entropy is a measure of disorder; Entropy of an isolated system Increases in any spontaneous process. OR This law also predicts that the entropy of an isolated system always increases with time. Third Law: The entropy of a perfect crystal approaches zero as temperature approaches absolute zero. ©2010, 2008, 2005, 2002 by P. W. Atkins and L. L. Jones ©2010, 2008, 2005, 2002 by P. W. Atkins and L. L. Jones A Molecular Interlude: Internal Energy, U, from translation, rotation, vibration •Utranslation = 3/2 × nRT •Urotation = nRT (for linear molecules) or •Urotation = 3/2 × nRT (for nonlinear molecules) •At room temperature, the vibrational contribution is small (it is of course zero for monatomic gas at any temperature). At some high temperature, it is (3N-5)nR for linear and (3N-6)nR for nolinear molecules (N = number of atoms in the molecule. Enthalpy H = U + PV Enthalpy is a state function and at constant pressure: ∆H = ∆U + P∆V and ∆H = q At constant pressure, the change in enthalpy is equal to the heat released or absorbed by the system. Exothermic: ∆H < 0 Endothermic: ∆H > 0 Thermoneutral: ∆H = 0 Enthalpy of Physical Changes For phase transfers at constant pressure Vaporization: ∆Hvap = Hvapor – Hliquid Melting (fusion): ∆Hfus = Hliquid – -
Energy and Enthalpy Thermodynamics
Energy and Energy and Enthalpy Thermodynamics The internal energy (E) of a system consists of The energy change of a reaction the kinetic energy of all the particles (related to is measured at constant temperature) plus the potential energy of volume (in a bomb interaction between the particles and within the calorimeter). particles (eg bonding). We can only measure the change in energy of the system (units = J or Nm). More conveniently reactions are performed at constant Energy pressure which measures enthalpy change, ∆H. initial state final state ∆H ~ ∆E for most reactions we study. final state initial state ∆H < 0 exothermic reaction Energy "lost" to surroundings Energy "gained" from surroundings ∆H > 0 endothermic reaction < 0 > 0 2 o Enthalpy of formation, fH Hess’s Law o Hess's Law: The heat change in any reaction is the The standard enthalpy of formation, fH , is the change in enthalpy when one mole of a substance is formed from same whether the reaction takes place in one step or its elements under a standard pressure of 1 atm. several steps, i.e. the overall energy change of a reaction is independent of the route taken. The heat of formation of any element in its standard state is defined as zero. o The standard enthalpy of reaction, H , is the sum of the enthalpy of the products minus the sum of the enthalpy of the reactants. Start End o o o H = prod nfH - react nfH 3 4 Example Application – energy foods! Calculate Ho for CH (g) + 2O (g) CO (g) + 2H O(l) Do you get more energy from the metabolism of 1.0 g of sugar or -
Fundamentals of Refrigeration 3.1
Fundamentals of Refrigeration of Fundamentals Fundamentals of Refrigeration Changing the way you think about refrigeration LI 001 V3 001 LI ™® The following are tradenames or registered trademarks of their respective companies: BACnet from ASHRAE; Mod- bus from Schneider Electric Ltd; MicroTech III, Open Choices, from Daikin Applied; LONMARK, LonTalk, and LONWORKS are managed, granted and used by LONMARK International under a license granted by Echelon Corporation. 800.432.1342 ©2016 Daikin Applied www.DaikinApplied.com LI 001 (06/16) 001_Refrigeration_Cover_Wrap.indd All Pages 5/27/2016 12:33:11 PM Fundamentals of Refrigeration 3.1 Refrigeration Cycles 3 A refrigeration system moves heat from a space, fluid or material for the purpose of lowering its temperature. In the past, this was done by collecting ice in the winter and using its specific heat to cool as the ice melted. When 1 pound of ice melts, it absorbs 144 Btu, as latent energy. When 1 ton (2000 lbs) melts over a 24-hour period: Q = 2000 lbs × 144 Btu/lb/24 hrs = 12,000 Btu/h This is the definition of 1 ton of refrigeration. Ideal Basic Refrigeration Cycle The ideal basic refrigeration cycle consists of four components, connected by piping with refrigerant flowing through the system. Figure 13 shows the components in the cycle and Figure 14 shows the basic cycle on the Ph diagram. 1 ton of cooling is the effect of 1 ton of ice melting over a 24 hour period. 4 CONDENSER 3 COMPRESSOR EXPANSION DEVICE 2 EVAPORATOR 1 Figure 13 Basic Refrigeration Cycle The evaporator is between points 1 and 2. -
Analysis of Heat Transfer in Air Cooled Condensers
Analysis of Heat Transfer in Air Cooled Condensers Sigríður Bára Ingadóttir FacultyFaculty of of Industrial Industrial Engineering, Engineering, Mechanical Mechanical Engineering Engineering and and ComputerComputer Science Science UniversityUniversity of of Iceland Iceland 20142014 ANALYSIS OF HEAT TRANSFER IN AIR COOLED CONDENSERS Sigríður Bára Ingadóttir 30 ECTS thesis submitted in partial fulfillment of a Magister Scientiarum degree in Mechanical Engineering Advisors Halldór Pálsson, Associate Professor, University of Iceland Óttar Kjartansson, Green Energy Group AS Gestur Bárðarson, Green Energy Group AS Faculty Representative Ármann Gylfason, Associate Professor, Reykjavík University Faculty of Industrial Engineering, Mechanical Engineering and Computer Science School of Engineering and Natural Sciences University of Iceland Reykjavik, May 2014 Analysis of Heat Transfer in Air Cooled Condensers Analysis of Heat Transfer in ACCs 30 ECTS thesis submitted in partial fulfillment of a M.Sc. degree in Mechanical Engi- neering Copyright c 2014 Sigríður Bára Ingadóttir All rights reserved Faculty of Industrial Engineering, Mechanical Engineering and Computer Science School of Engineering and Natural Sciences University of Iceland VRII, Hjardarhagi 2-6 107, Reykjavik, Reykjavik Iceland Telephone: 525 4000 Bibliographic information: Sigríður Bára Ingadóttir, 2014, Analysis of Heat Transfer in Air Cooled Condensers, M.Sc. thesis, Faculty of Industrial Engineering, Mechanical Engineering and Computer Science, University of Iceland. Printing: Háskólaprent, Fálkagata 2, 107 Reykjavík Reykjavik, Iceland, May 2014 Abstract Condensing units at geothermal power plants containing surface condensers and cooling towers utilize great amounts of water. Air cooled condensers (ACCs) are not typically paired with dry or flash steam geothermal power plants, but can be a viable solution to eliminate the extensive water usage and vapor emissions related to water cooled systems. -
Topic 4 Thermodynamics Thermodynamics
Topic 4 Thermodynamics Thermodynamics • We need thermodynamic data to: – Determine the heat release in a combustion process (need enthalpies and heat capacities) – Calculate the equilibrium constant for a reaction – this allows us to relate the rate coefficients for forward and reverse reactions (need enthalpies, entropies (and hence Gibbs energies), and heat capacities. • This lecture considers: – Classical thermodynamics and statistical mechanics – relationships for thermodynamic quantities – Sources of thermodynamic data – Measurement of enthalpies of formation for radicals – Active Thermochemical Tables – Representation of thermodynamic data for combustion models Various thermodynamic relations are needed to determine heat release and the relations between forward and reverse rate coefficients A statement of Hess’s Law ni is the stoichiometric coefficient Hess’s Law: The standard enthalpy of an overall reaction is the sum of the standard enthalpies of the individual reactions into which the reaction may be divided Tabulated thermodynamic quantities. 1. Standard enthalpy of formation o Standard enthalpy change of formation, fH The standard enthalpy change when 1 mol of a substance is formed from its elements in their reference states, at a stated temperature (usually 298 K). The reference state is the most stable state at that temperature, and at a pressure of 1 bar. o e.g. C(s) + 2H2(g) CH4(g) fH = -74.8 kJ mol-1 The standard enthalpies of formation of C(s) and H2(g) are both zero The reference state for carbon is graphite. Standard -
Mass and Energy Balances
Mass and Energy Balances Outline • Terminology – Specific heat, enthalpy, heat, sensible heat, latent heat, saturation temperature & pressure, saturated liquid & vapor • Phase diagram of water (liquid and vapor phases) – Sub-cooled liquid, condensate, steam (saturated steam: mix of condensate & vapor), vapor, superheated steam • Steam table • Steam quality • Superheated steam • Energy content (or enthalpy) – Liquid products, steam • Mass and energy balances – Batch & continuous processes (mixing & heating); direct & indirect contact heating; indirect contact cooling; determination of steam quality Terminology • Specific heat (cp: J/kg K) – Energy required to raise the temperature of unit mass of a substance by unit value – It varies with temperature; however, for approximate calculations, cp of water is assumed to be 4180 J/kg K • Enthalpy (H: J/kg) – Heat content of a system • It is always expressed relative to a reference state (usually 0 °C) – Generally, enthalpy is assumed to be zero at 0 °C – For most liquids, H ~ cp (Tin °C) • Heat (Q: J) – Energy transferred due to temperature difference between system and surroundings • When energy transferred is represented per unit time, its units are J/s or W • The energy transferred may be utilized as sensible heat or latent heat Terminology (contd.) • Sensible heat (Q: J or J/s) – Energy transferred from hot to cold object • For a batch system: Q = m c T Q is in J p . • For a continuous system: Q = m cp T Q is in J/s or W • Latent heat (Q: J or J/s) – Energy transferred during phase change without any temperature change • For a batch system: Q = m Q is in J .