上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 23-24_Introducing 2nd law, concept of irreversibilities

上游充通大学 SHANGHAI JIAO TONG UNIVERSITY Engineering Thermodynamics I Lecture 23-24 Chapter 6 The second law of Thermodynamics (Section6.1-6.3,6.6) Spring,2017 强 Prof.,Dr.Yonghua HUANG http://cc.sjtu.edu.cn/G2S/site/thermo.html 1日G
Engineering Thermodynamics I Lecture 23-24 Spring, 2017 Prof., Dr. Yonghua HUANG Chapter 6 The second law of Thermodynamics (Section 6.1- 6.3, 6.6) http://cc.sjtu.edu.cn/G2S/site/thermo.html

Why need the second law? First law-energy conservation (Quantity) dt How about the Quality of the energy? 4C61676666 C61676656 100 100 好好学习 上游究通大学 Mar/29,Wed,2017 2 SHANGHAI JIAO TONG UNIVERSITY
Mar/29, Wed, 2017 2 Why need the second law? First law – energy conservation How about the Quality of the energy? (Quantity)

Quality of energy 1 kJ electricity power <-1kJ heat 1 kJ chemical energy <-1kJ heat 300 上游充通大学 Mar/29,Wed,2017 3 SHANGHAI JLAO TONG UNIVERSITY
Mar/29, Wed, 2017 3 Quality of energy 1 kJ electricity power 1kJ heat 1 kJ chemical energy 1kJ heat

Spontaneous processes Atmospheric air at To Body at Time Time ToTo 10 Valve7 Air at Air Pi>Po Air at po<p<pi Po Mass z<Z Mass 上游充通大学 Mar/29,Wed,2017 4 SHANGHAI JIAO TONG UNIVERSITY
Mar/29, Wed, 2017 4 Spontaneous processes

The inverse process Heat Tl,raising? Heat Not violate the 1st law!! IWn-9 TT,current output 上游充通大 Mar/29,Wed,2017 5 SHANGHAI JIAO TONG UNIVERSITY
Mar/29, Wed, 2017 5 The inverse process Q Q' ? Not violate the 1st law!! T↓, raising ? T↑, current output ?

Summary Spontaneous process: processes proceed in a certain direction initial condition of the system can be restored,but not in a spontaneous process.Some auxiliary devices would be required (a permanent change in the condition of the surroundings would result.) satisfying the first law does not ensure that the process can actually occur 上游充通大学 Mar/29,Wed,2017 6 SHANGHAI JLAO TONG UNIVERSITY
Mar/29, Wed, 2017 6 Summary Spontaneous process: • processes proceed in a certain direction • initial condition of the system can be restored, but not in a spontaneous process. Some auxiliary devices would be required (a permanent change in the condition of the surroundings would result.). • satisfying the first law does not ensure that the process can actually occur

Relations?:quality of energy -spontaneous Quality degrading spontaneous. Quality upgrading>need compensation. But overall effect:quality degrading. Hot reservoir Hot reservoir T T Wnet Wnet R Q21 Cold reservoir Cold reservoir T2 T2 Fully convertible energy-mechanical /electrical energy Direction of energy conversion energy quality difference Partially convertible energy-heat t T≠To Unconvertible energy-internal energy in surrounding 上游充通大 Mar/29,Wed,2017 7 SHANGHAI JIAO TONG UNIVERSITY
Mar/29, Wed, 2017 7 Relations?: quality of energy – spontaneous Quality degrading spontaneous. Quality upgrading need compensation. But overall effect: quality degrading. Hot reservoir T1 E Cold reservoir T2 Q1 Q2 Wnet Hot reservoir T1 R Cold reservoir T2 Q1 Q2 Wnet Direction of energy conversion = energy quality difference Fully convertible energy—mechanical /electrical energy Partially convertible energy—heat T T0 Unconvertible energy—internal energy in surrounding

Calling another principle-2nd law Only the first law is inadequate to identify whether a process can take place. Another guiding principle would be helpful.This is provided by the 2nd law The above inverse processes violate the 2nd law, so not spontaneous. A process cannot occur unless it satisfies both the first and the second laws of thermodynamics 上游充通大学 Mar/29,Wed,2017 8 SHANGHAI JLAO TONG UNIVERSITY
Mar/29, Wed, 2017 8 Calling another principle- 2 nd law Only the first law is inadequate to identify whether a process can take place. Another guiding principle would be helpful. This is provided by the 2nd law The above inverse processes violate the 2nd law, so not spontaneous. A process cannot occur unless it satisfies both the first and the second laws of thermodynamics

Opportunities for developing work Spontaneous process: imbalance equilibrium:possible to retrieve work Examples:Spontaneous cooling direct cooling System undergoing a thermodynamic cycle What is the theoretical maximum value for the work Hot that could be obtained? reservoir Wasted (uncontrolled way) .What are the factors that would Weyele=CH-ec preclude the realization of the maximum value? Cold reservoir -friction... 上游充通大 Mar/29,Wed,2017 9 SHANGHAI JLAO TONG UNIVERSITY
Mar/29, Wed, 2017 9 Opportunities for developing work Spontaneous process: • imbalance equilibrium: possible to retrieve work • Examples: Spontaneous cooling Wasted (uncontrolled way) • What is the theoretical maximum value for the work that could be obtained? • What are the factors that would preclude the realization of the maximum value? -friction…

Summary:duty of the second law 1.predicting the direction of processes. 2.establishing conditions for equilibrium. 0 3.determining the best theoretical performance of cycles, engines,and other devices. 4.evaluating quantitatively the factors that preclude the attainment of the best theoretical performance level. >how to briefly and accurately state the 2nd law? 上游通大学 Mar/29,Wed,2017 10 HANGHAI JIAO TONG UNIVERSITY
Mar/29, Wed, 2017 10 Summary: duty of the second law 1. predicting the direction of processes. 2. establishing conditions for equilibrium. 3. determining the best theoretical performance of cycles, engines, and other devices. 4. evaluating quantitatively the factors that preclude the attainment of the best theoretical performance level. how to briefly and accurately state the 2nd law?
按次数下载不扣除下载券;
注册用户24小时内重复下载只扣除一次;
顺序:VIP每日次数-->可用次数-->下载券;
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 22_Transient analysis of Energy.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 20-21_Illustrations_3 Heat exchangers, throttling devices, System integration.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 19_Illustrations_2 Compressors, pumps.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 18_Illustrations_1 Nozzles, diffusers, turbines.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 17_Control volume analysis - energy conservation.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 16_Control volume analysis - mass conservation.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 15_Polytropic process.pdf
- 上海交通大学:《传热学》课程教学资源(课件讲稿)第五章 对流传热的理论基础 5-1 对流传热概说 5-2 对流换热问题的数学描写.pdf
- 上海交通大学:《传热学》课程教学资源(课件讲稿)第四章 导热问题的数值解法 §4-4 非稳态导热问题的数值解法.pdf
- 上海交通大学:《传热学》课程教学资源(课件讲稿)第三章 非稳态导热 § 3-3 典型一维物体非稳态导热的分析解 §3-4 半无限大物体的非稳态导热 第四章 导热问题的数值解法 4-1 导热问题数值求解的基本思想 4-2 内节点离散方程的建立方法 4-3 边界结点离散方程的建立及代数方程的求解.pdf
- 上海交通大学:《传热学》课程教学资源(课件讲稿)第二章 导热基本定律及稳态导热 2-5 具有内热源的一维导热问题 2-6 多维稳态导热的求解 第三章 非稳态导热 3-1 非稳态导热的基本概念 3-2 零维问题的分析法——集中参数法.pdf
- 上海交通大学:《传热学》课程教学资源(课件讲稿)第二章 导热基本定律及稳态导热 2-5 具有内热源的一维导热问题 2-6 多维稳态导热的求解 第三章 非稳态导热 3-1 非稳态导热的基本概念 3-2 零维问题的分析法——集中参数法.pdf
- 上海交通大学:《传热学》课程教学资源(课件讲稿)第二章 导热基本定律及稳态导热 §2-3 典型一维稳态导热问题的分析解 2-4 通过肋片的导热.pdf
- 上海交通大学:《传热学》课程教学资源(课件讲稿)第二章 导热基本定律及稳态导热 2-1 导热基本定律 2-2 导热问题的数学描写.pdf
- 上海交通大学:《传热学》课程教学资源(课件讲稿)第五章 对流传热的理论基础 5-3 边界层型对流传热问题的数学描写 5-4 流体外掠平板传热层流分析解及比拟理论 第六章 单相对流传热的实验关联式 6-1 相似原理与量纲分析.pdf
- 上海交通大学:《传热学》课程教学资源(课件讲稿)传热传质学 Heat and Mass Transfer 第一章 绪论(王平阳).pdf
- 上海交通大学:《能源物理》教学资源(课件讲义)第一章 质点运动学.pdf
- 上海中医药大学:《物理学》课程教学资源(PPT课件)第十四章 原子光谱与分子光谱.ppt
- 上海中医药大学:《物理学》课程教学资源(PPT课件)第十二章 光学基本知识与药用光学仪器.ppt
- 上海中医药大学:《物理学》课程教学资源(PPT课件)第十三章 量子力学基础.ppt
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 27-28_Applying 2nd law to thermodynamic cycles, Maximum performance.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 29_Carnot Cycle.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 30_Clausius inequality and Entropy.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 31_Retrieve entropy data.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 32_Internally reversible processes, Closed system entropy balance.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 33_Entropy increase principle.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 34_Entropy balance to open systems.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 35_Isentropic processes, Isentropic efficiencies.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 36_Heat transfer and Work of internal reversible, ss flow.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 37-38_Concept of exergy and apply to CM&CV systems.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 39-40_vapor power cycles.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 43_superheat and reaheat.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 44_Vapor-compression refrigeration, Heat pump systems.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 45_Air standard cycle, internal combustion engines, Otto cycle.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 46_Diesel cycle and dual cycle.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 47_Compressor, compression with intercooling.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 48_Review and Final Exam.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)中意楼位置.pptx
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 01-02_Course Introduction.pdf
- 上海交通大学:《热力学 Thermodynamics(I)》课程教学资源(课件讲义)Lecture 03-04_Concepts.pdf