Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 1.

Slides:



Advertisements
Similar presentations
QUICK QUIZ 22.1 (end of section 22.1)
Advertisements

Operated by the Southeastern Universities Research Association for the U.S. Depart. Of Energy Thomas Jefferson National Accelerator Facility Strained superlattice.
IB Physics Topic 3 & 10 Mr. Jean May 7 th, The plan: Video clip of the day Thermodynamics Carnot Cycle Second Law of Thermodynamics Refrigeration.
Chapter 11 Refrigeration Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel.
Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 1.
Refrigeration Cycles Chapter 11.
L 19 - Thermodynamics [4] Change of phase ice  water  steam
Phy 212: General Physics II Chapter 20: Entropy & Heat Engines Lecture Notes.
Vapor and Combined Power Cycles
EXERCISE 1 CHAPTER 11.
The Second Law of Thermodynamics Physics 102 Professor Lee Carkner Lecture 6.
The Second Law of Thermodynamics Physics 102 Professor Lee Carkner Lecture 7.
Second Law Thermodynamics Professor Lee Carkner Lecture 11.
Thermo & Stat Mech - Spring 2006 Class 5 1 Thermodynamics and Statistical Mechanics Heat Engines and Refrigerators.
Thermo & Stat Mech - Spring 2006 Class 6 1 Thermodynamics and Statistical Mechanics Entropy and the Second Law of Thermodynamics.
For next time: Read: § 8-6 to 8-7 HW11 due Wednesday, November 12, 2003 Outline: Isentropic efficiency Air standard cycle Otto cycle Important points:
Reversible Processes The second law of thermodynamics state that no heat engine can have an efficiency of 100%. Then one may ask, what is the highest efficiency.
Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 1.
Dr.Salwa Al Saleh Lecture 9 Thermodynamic Systems Specific Heat Capacities Zeroth Law First Law.
Chapter 15: Thermodynamics
The Laws of Thermodynamics
Second Law of Thermodynamics.  No cyclic process that converts heat entirely into work is possible.  W can never be equal to Q.  Some energy must always.
Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 1.
A Vapor Power Cycle Boiler T Turbine Compressor (pump) Heat exchanger
The Second Law of Thermodynamics Chapter 6. The Second Law  The second law of thermodynamics states that processes occur in a certain direction, not.
Lecture Outline Chapter 12 College Physics, 7 th Edition Wilson / Buffa / Lou © 2010 Pearson Education, Inc.
Sajjad Ahmed Memon S.S./ Health Physicist NIMRA 1.
The Thermodynamic Cycle. Heat engines and refrigerators operate on thermodynamic cycles where a gas is carried from an initial state through a number.
Gas Turbines for Aircraft Propulsion. AIR CRAFT ENGINE The turbojet engine consists of three main sections: the diffuser, the gas generator, and the nozzle.
Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 1.
Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 1.
PHY1039 Properties of Matter Heat Engines, Thermodynamic Efficiency, and Carnot Cycles April 30 and May 3, 2012 Lectures 17 and 18.
Chapter 11 Refrigeration Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 8th edition by Yunus A. Çengel.
Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 1.
Thermodynamics Internal energy of a system can be increased either by adding energy to the system or by doing work on the system Remember internal energy.
Presentation on HEAT ENGINE PREPARED BY: CHAUHAN SATISH(EN. NO: ) GAUTAM ASHISH(EN. NO: ) KETUL PATEL(EN. NO: ) SUB:
1 Second Law of Thermodynamics Engines and Refrigerators.
Reversible and irreversible processes Physics Entropy 28 September 2011.
1 Heat Engines and Refregerators Readings: Chapter 19.
APPLIED THERMODYNAMICS UNIT- 2 Gas power cycle 1 Department of Mechanical Engineering,A.I.E.T.,Mijar 3)Air Standard Diesel Cycle/ Constant Pressure cycle:
Thermodynamics Thermodynamics is a branch of physics concerned with heat and temperature and their relation to energy and work.
Chapter 15 Thermodynamics Thermodynamic Systems and Their Surroundings Thermodynamics is the branch of physics that is built upon the fundamental.
Lecture 26: Thermodynamics II l Heat Engines l Refrigerators l Entropy l 2 nd Law of Thermodynamics l Carnot Engines.
Chapter 12 Laws of Thermodynamics. Chapter 12 Objectives Internal energy vs heat Work done on or by a system Adiabatic process 1 st Law of Thermodynamics.
Unit 61: Engineering Thermodynamics Lesson 9: Carnot Engine Cycles.
Dr. Owen Clarkin School of Mechanical & Manufacturing Engineering Summary of Energy Topics Chapter 1: Thermodynamics / Energy Introduction Chapter 2: Systems.
Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 1.
1 Summer Training On Refrigeration and Air Conditioning From:-Amber Enterprises PVT.LTD.
Chapter 7 THE SECOND LAW OF THERMODYNAMICS
1 Reversible Processes The second law of thermodynamics state that no heat engine can have an efficiency of 100%. Then one may ask, what is the highest.
Chapter 11 Refrigeration Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 7th edition by Yunus A. Çengel.
Date of download: 9/30/2017 Copyright © ASME. All rights reserved.
Solar collectors for water heating
Indian Institute of Technology Bombay
BRAYTON CYCLE AND EFFECT OF INTERCOOLING , REHEAT AND REGENRATION
SNS COLLEGE OF ENGINEERING Coimbatore-107 Subject: Thermal Engineering
Mohamed Iqbal Pallipurath
LAXMI INSTITUTE OF TECHNOLOGY
An iso certified institute
Presentation Title “Reversed Carnot Cycle”
REVERSIBLE AND IRREVERSIBLE PROCESSES
The Laws of Thermodynamics
Chapter 11 Refrigeration Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel.
Objectives Learn about Cooling towers Cooling cycles.
Z.E. Z.E. Z.E. IE 211 INTRODUCTION TO ENGINEERING THERMODYNAMICS
Chapter 11 Refrigeration Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel.
Chapter 18,19and20 Thermodynamics.
Second Law of Thermodynamics
10 CHAPTER Refrigeration Cycles.
Presentation transcript:

Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 1 2. Carnot Helium Refrigeration and Liquefaction Systems Clausius (In)equality

Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 2 Carnot Helium Refrigeration and Liquefaction Systems (Cont.) Carnot Refrigeration System: Minimum required input work for a given rate of thermal energy transfer between two thermal reservoirs. The work input for the Carnot system expressed as: This is a very powerful equation. The terms are as follows: is the heat rejected to the environment or, the input power to an isothermal compressor is the heat absorbed or the ideal refrigeration or, the ideal work output from an ideal expander is the ideal net input work required which is the difference between (a) and (b) above

Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 3 Carnot Helium Refrigeration and Liquefaction Systems (Cont.) A refrigerator transfers heat energy from a low temperature reservoir to a higher temperature reservoir. Most helium refrigerators transfer heat energy from approximately 4.22K (or in some cases at sub-atmospheric pressures). A liquefier is different from a refrigerator since the objective is to cool a quantity (flow rate) of high (or ambient) temperature fluid to a specified low (or load) temperature, which then leaves the cycle (at a low temperature). What leaves the cycle is the liquefaction flow, and may be returned at a higher or ambient temperature. In comparison to the refrigerator, in a liquefier the temperature at which the heat energy is being transferred (removed) is constantly varying (decreasing as it is being cooled), although it is rejected at the same (high or ambient) temperature reservoir.

Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 4 Carnot Helium Refrigeration and Liquefaction Systems (Cont.) Carnot Helium Refrigerator Carnot Helium Liquefier

Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 5 Carnot Helium Refrigeration and Liquefaction Systems (Cont.) Carnot work required for a given liquefaction load

Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 6 Carnot Helium Refrigeration and Liquefaction Systems (Cont.) Carnot work required for liquefaction load for a given temperature range

Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Page 7 Carnot Helium Refrigeration and Liquefaction Systems (Cont.) Carnot work for different fluids