ISAT Module III: Building Energy Efficiency

Slides:



Advertisements
Similar presentations
Chapter 11 Refrigeration Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel.
Advertisements

Chapter 9 REFRIGERATION AND LIQUEFACTION
Refrigeration Cycles د/ محمود عبدالوهاب.
Refrigeration Cycles CHAPTER 11: PTT 201/4 THERMODYNAMICS
REFRIGERATION Refrigeration may be defined as the process of removing heat from a substance under controlled conditions and reducing and maintaining the.
10 CHAPTER Refrigeration Cycles.
Moisture to water converter. Out Line : Abstract Introduction Heat Pump Heat Pump Components Conclusion.
Refrigeration and Heat Pump Systems
14. REFRIGERATION.
Refrigeration Cycles Chapter 11.
Gas – Vapor Mixtures & Air – Conditioning
Building Energy Efficiency
Vapor and Combined Power Cycles
9 CHAPTER Vapor and Combined Power Cycles.
Chapter 1 VAPOR AND COMBINED POWER CYCLES
EXERCISE 1 CHAPTER 11.
1 Vapour compression cycle Refrigerator Air conditioning plant Heat pump (“ ENERGY MANAGEMENT HANDBOOK” Sixth Edition, Chapter 8)
Throttling Thermodynamics Professor Lee Carkner Lecture 22.
HOT COLD HOT COLD The Ideal Vapor-Compression Refrigeration Cycle 1-2 Isentropic compression in a compressor 2-3 Constant-pressure heat rejection in.
Advanced Thermodynamics Note 8 Refrigeration and Liquefaction
Atmospheric Moisture: Relative Humidity and Dew Point
EGR 334 Thermodynamics Chapter 10:
Refrigerators and Heat Pumps
1 ISAT Module III: Building Energy Efficiency Topic 9:Advanced Heat Pumps  Heat Pump Water Heater  Heat Recovery from a Swimming Pool Using a Heat.
Pacific School Of Engineering. Guided By:- Asst.Prof.Vatsal patel Submitted by:-  Kotadiya Reshma :  Ladva Piyush : 
Refrigeration Cycles Chapter 11: ERT 206/4 THERMODYNAMICS
REFRIGERATION, COMPRESSED AIR SYSTEMS & EFFICIENT USE OF ENERGY
ISAT Module V: Industrial Systems
Chapter 11 Refrigeration Cycles
Refrigeration Terms Cooling Load, Cooling Capacity – Q in Compressor Load – W in Condenser Load – Q out Tons of Refrigeration – Rate of Heat Input Refrigerant.
Vapor and Combined Power Cycles (2)
Chapter10 Refrigeration Cycle 10-1 Vapor-Compression Cycle The Reversed Carnot Cycle T s THTH TLTL Coefficient of Performance.
Heat Transfer Equations For “thin walled” tubes, A i = A o.
Refrigeration Basics 101.
Chapter 11 Refrigeration Cycles
Vapour Compression Refrigeration Systems
The Refrigeration Process
Last Time Where did all these equations come from?
Energy and the Environment Fall 2013 Instructor: Xiaodong Chu : Office Tel.:
Refrigeration Cycles (YAC: 7-13 trough 7-16)
Chapter 11 Refrigeration Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 8th edition by Yunus A. Çengel.
Heat Transfer Equations For “thin walled” tubes, A i = A o.
Refrigeration Cycles A Carnot cycle in reverse QL QH T s 2
HW2 AHU problems: Book: 8.5, 8.25, 8.27, 8.28, 8.22 Cooling Cycles Problems: - Book: 3.1 (page 69), - Book: 3.5 ((page 70), - Out of book: Same like 3.5.
Chapter 9. Refrigeration and Liquefaction (냉동과 액화)
Basic Refrigeration. Star Refrigeration Wednesday 12 September 2007.
VAPOUR ABSORPTION REFRIGERATION SYSTEM
Prepared by:- B.S.Bhandari Faculty HNBGU.  Refrigeration is a science of producing and maintaining temperature below that of the surrounding temperature.
Chapter 11 Refrigeration Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 7th edition by Yunus A. Çengel.
Chapter 14 Gas-Vapor Mixtures and Air-Conditioning Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 8th edition.
Refrigeration & air conditioning
REFRIGERATION CYCLES ERT 206 THERMODYNAMICS.
Refrigeration and Heat Pump Systems
SNS COLLEGE OF ENGINEERING Coimbatore-107 Subject: Thermal Engineering
Objectives Introduce the concepts of refrigerators and heat pumps and the measure of their performance. Analyze the ideal vapor-compression refrigeration.
Introduction to Food Engineering
HVAC EQUIPMENT: COOLING SOURCES (see Chapter 16)
Automotive Heating And Air Conditioning
TOPIC:- VAPOUR CYCLES CREATED BY:
High Temperature Reservoir Low Temperature Reservoir
Mohamed Iqbal Pallipurath
The Second Law of Thermodynamics: Kelvin–Planck Statement
Chapter 11 Refrigeration Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel.
9 CHAPTER Vapor and Combined Power Cycles.
Objectives Learn about Cooling towers Cooling cycles.
Psychrometry & Air-conditioning
Chapter 11 Refrigeration Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel.
Objectives Solve one more example related to the psychometrics in AHU and building systems Learn about the psychometrics related to the cooling towers.
10 CHAPTER Refrigeration Cycles.
“THERMODYNAMIC AND HEAT TRANSFER”
Presentation transcript:

ISAT 413 - Module III: Building Energy Efficiency Topic 3: Refrigeration, Heat Pumps and Air Conditioning Evaporating Cooling Vapor-Compression Refrigeration Vapor-Absorption Refrigeration Other Refrigeration Systems The Heat Pump Air Conditioning

Evaporative Cooling (Eastop, Example 4.8) In a cooling tower the water to be cooled enters near the top of the tower and flows down through packing in counter flow to an air stream as shown diagrammatically in Fig. 4.34. Air is induced from the base of the tower by a fan mounted on the top of the tower. Using the data given below and neglecting heat losses and pressure losses, calculate: (i) the required mass flow rate of air induced by the fan for the given cooling duty; (ii) the mass flow rate of make-up water required.

Cooling Tower (Evaporative Cooling)

Data: Water: Mass flow rate, 15 kg/s; temperature of water at entry, 27oC; temperature of water at exit, 21oC; mean specific heat, 4.18 kJ/kg.K. Air: Ambient conditions, 1,01325 bar, 23oC dry bulb (DB), 17oC wet bulb (WB); air at exit, saturated with water vapor at 25oC; mean specific heat of dry air, 1.005 kJ/kg.K; fan air power input, 5 kW. Assumptions: For air at standard atmospheric pressure it can be assumed that the vapor pressure is given by: For water vapor at low vapor pressure it is a good approximation to assume that the enthalpy is equal to the saturated value at the same dry bulb temperature.

(i) the required mass flow rate of air induced by the fan for the given cooling duty

Vapor-Compression Refrigeration P-h Diagram of an Ideal Vapor-Compression Refrigeration Cycle

Schematic and T-s Diagram for Ideal Vapor-Compression Refrigeration Cycle

Schematic and T-s Diagram for Actual Vapor-Compression Refrigeration Cycle

The performance of refrigerators and heat pumps is expressed in terms of coefficient of performance (COP), defined as

The standard of comparison for refrigeration cycles is the reversed Carnot cycle. A refrigerator or heat pump that operates on the reversed Carnot cycle is called a Carnot refrigerator or a Carnot heat pump, and their COPs are

The transfer of heat from lower temperature regions to higher temperature ones is called refrigeration. Devices that produce refrigeration are called refrigerators, and the cycles on which they operate are called refrigeration cycles. The working fluids used in refrigerators are called refrigerants. Refrigerators used for the purpose of heating a space by transferring heat from a cooler medium are called heat pumps.

The most widely used refrigeration cycle is the vapor-compression refrigeration cycle. In an ideal vapor-compression refrigeration cycle, the refrigerant enters the compressor as a saturated vapor and is cooled to the saturated liquid state in the condenser. It is then throttled to the evaporator pressure and vaporizes as it absorbs heat from the refrigerated space.

Very low temperatures can be achieved by operating two or more vapor-compression Systems in series, called cascading. The COP of a refrigeration system also increases as a result of cascading.

Another way of improving the performance of a vapor-compression refrigeration system is by using multistage compression with regenerative cooling. A refrigerator with a single compressor can provide refrigeration at several temperatures by throttling the refrigerant in stages. The vapor-compression refrigeration cycle can also be used to liquefy gases after some modifications Q: Cycles? Components? Working Fluids?

Working Fluids – Refrigerants The designation of CFCs (ChloroFluoroCarbons) is by a two or three digit number: The digit on the right represents the number of fluorine (F) atoms; The middle digit represents one more than the number of hydrogen (H) atoms; The digit on the left represents one less than the number of carbon (C) atoms and omitted when there is only one carbon atom. CHClF2 (R22) or called HCFC 22

Some Common CFC, HCFC Refrigerants: CCl3F (R11), CCl2F2 (R12), and CHClF2 (R22), HFC 134a, CCl2FCClF2 (R113) and CClF2CClF2 (R114) R502 which is an azeotropic mixture (acts as a single substance and cannot be separated into its components by distillation.) of R22 and R115 The commonly accepted designation for refrigerants other than halocarbons (compounds containing carbon, fluorine and chlorine in varying proportions, known as CFCs) is to put the digit 7 in front of the relative molecular mass (e.g. NH3 (R717), CO2 ( R744).) (Notice that researches are now underway to develop acceptable alternatives.)

Vapor-Absorption Refrigeration Ammonia Absorption Refrigeration Cycle

Another form of refrigeration that becomes economically attractive when there is a source of inexpensive heat energy at a temperature of 100 to 2000C is absorption refrigeration, where the refrigerant is absorbed by a transport medium and compressed in liquid form. The most widely used absorption refrigeration system is the ammonia-water system, where ammonia serves as the refrigerant and water as the transport medium. The work input to the pump is usually very small, and the COP of absorption refrigeration systems is defined as

The maximum COP an absorption refrigeration system can have is determined by assuming totally reversible conditions, which yields where T0, TL, and Ts are the absolute temperatures of the environment, refrigerated space, and heat source, respectively.

Other Refrigeration Systems Schematic of Simple Thermoelectric Power Generator

A Thermoelectric Refrigerator 10-13 A Thermoelectric Refrigerator (Fig. 10-28)

A refrigeration effect can also be achieved without using any moving parts by simply passing a small current through a closed circuit made up of two dissimilar materials. This effect is called the Peltier effect, and a refrigerator that works on this principle is called a thermoelectric refrigerator.

Refrigerator and Heat Pump Objectives The Heat Pump Refrigerator and Heat Pump Objectives The objective of a refrigerator is to remove heat (QL) from the cold medium; the objective of a heat pump is to supply heat (QH) to a warm medium.

Heat Pump Heats a House in Winter and Cools it in Summer

Air Conditioning (Eastop, Example 4.11) An air conditioning plant is designed to maintain a room at 20oC, percentage saturation 50%, which an air supply to the room of 1.8 kg/s at 14oC, percentage saturation 60%. The design outside air conditions are 27oC,percentage saturation 70%. The plant consists of a mixing chamber for re-circulated and fresh air, a cooling coil supplied with chilled water, heating coil, and a supply fan. The ratio of re-circulated air to fresh air is 3; the cooling coil has an apparatus dew point of 5oC, and the refrigeration unit supplying the chilled water has an overall coefficient of performance 2. Neglecting all losses and fan and pump work, calculate:

(i) the total air conditioning load for the room; (ii) the required total energy input; (iii) the required energy input if the energy to the heating coil is supplied from the refrigeration plant condenser cooling water.

(i) the total air conditioning load for the room;

(ii) the required total energy input;

(iii) the required energy input if the energy to the heating coil is supplied from the refrigeration plant condenser cooling water.