18.9 A Closer Look at Heat and Work. 18.10 The First Law of Thermodynamics You have just seen that when a system changes from a given initial state to.

Slides:



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

Work and Heat in Thermodynamic Processes
Chapter 12 The Laws of Thermodynamics. Work in a Gas Cylinder.
Temperature, Heat, and the First Law of Thermodynamics
Chapter 18: Heat,Work,the First Law of Thermodynamics
Kinetic Theory and Thermodynamics
Temperature, Heat, and the First Law of Thermodynamics
Unit 3 Temperature, Heat, and the First Law of Thermodynamics.
Chapter 10 Thermodynamics
Dr. Jie ZouPHY Chapter 20 Heat and the First Law of Thermodynamics (cont.)
Chapter 12 The Laws of Thermodynamics. Work in Thermodynamic Processes Work is an important energy transfer mechanism in thermodynamic systems Work is.
Fig The infinitesimal work done by the system (gas) during the small expansion dx is dW = p A dx.
Entropy and the Second Law of Thermodynamics
Fig The net work done by the system in the process aba is –500 J.
First Law of Thermodynamics Physics 202 Professor Lee Carkner Lecture 13.
Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley PowerPoint ® Lectures for University Physics, Twelfth Edition – Hugh D. Young.
Chapter 5 The First Law of Thermodynamics
Temperature, Heat, and the First Law of Thermodynamics Chapter 18 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 16 Physics, 4 th Edition James S. Walker.
Thermodynamics AP Physics 2.
Chapter 18 Temperature, Heat, and the First Law of Thermodynamics.
Topic 10 Sections 2 and 3.  Statement Number Assessment Statement Deduce an expression for the work involved in a volume change of a gas at constant.
Work and heat oWhen an object is heated and its volume is allowed to expand, then work is done by the object and the amount of work done depends generally.
17.4 State Variables State variables describe the state of a system
1 Introduction Physics 313 Professor Lee Carkner Lecture 1.
Preview Objectives Heat, Work, and Internal Energy Thermodynamic Processes Chapter 10 Section 1 Relationships Between Heat and Work.
Chapter 15: Thermodynamics
Q19.1 A system can be taken from state a to state b along any of the three paths shown in the pV–diagram. If state b has greater internal energy than state.
T062:Q10. A metal rod has a length of 7.30 m at 15  C and a length of 7.40 m at 95  C. What is the temperature of the rod when its length is 7.21.
Chapter-18 Temperature, Heat and the First Law of Thermodynamics.
The internal energy of a substance can be changed in different ways. Work can transfer energy to a substance and increase its internal energy.
Preview Objectives Heat, Work, and Internal Energy Thermodynamic Processes Chapter 10 Section 1 Relationships Between Heat and Work.
Preview Objectives Heat, Work, and Internal Energy Thermodynamic Processes Chapter 10 Section 1 Relationships Between Heat and Work.
Deduce an expression for the work involved in a volume change of a gas at constant pressure State the first law of thermodynamics. 1 Students.
Chapter 4 Macroscopic Parameters & Their Measurement
Temperature, Heat, and the First Law of Thermodynamics
Temperature, Heat, and the First Law of Thermodynamics
Chapter 10 Preview Objectives Heat, Work, and Internal Energy
Heat & The First Law of Thermodynamics
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.
First Law of Thermodynamics
1 Second Law of Thermodynamics - Entropy. 2 Introduction The second low often leads to expressions that involve inequalities.
B2 Thermodynamics Ideal gas Law Review PV=nRT P = pressure in Pa V = volume in m3 n = # of moles T= temperature in Kelvin R = 8.31 J K -1 mol -1 m = mass.
Thermodynamics. Definitions Thermodynamics is the study of processes in which energy is transferred as work and heat The system is a set of particles.
Thermodynamic Processes
In review, the 1 st law of thermodynamics indicates that all energy entering and leaving the system is accounted for and is conserved. 2.
The First Law of Thermodynamics Ideal Gas Processes
AP Physics B Ch. 12: Laws of Thermodynamics. Internal energy (U) Sum of the kinetic energy of all particles in a system. For an ideal gas: U = N K ave.
Chapter 16 Temperature and Heat.  Definition of heat: Heat is the energy transferred between objects because of a temperature difference.  Objects are.
Chapter 11 Thermodynamics Worksheet
Chapter 13 The Transfer of Heat.
Chapter 2 Heat, Temperature and the First Law of Thermodynamics
The Absorption of Heat by Solids and Liquids
and Statistical Physics
You have 1 kg ice (at 0o C) in a well-insulated container
Temperature, Heat, and the First Law of Thermodynamics
Temperature, Heat and Thermal Expansion
Thermal 3.
D. |Q| is the same for all three paths.
Temperature, Heat, and the First Law of Thermodynamics
Temperature, Heat, and the First Law of Thermodynamics
Quasistatic processes The relation of heat and work
Temperature, Heat, and the First Law of Thermodynamics
18.9 A Closer Look at Heat and Work
Chapter 16 Temperature and Heat.
Temperature, Heat , and the First law of thermodynamics
Temperature, Heat and the First Law of Thermodynamics
First Law of Thermodynamics
Temperature, Heat, and the First Law of Thermodynamics
Thermodynamic Processes
Presentation transcript:

18.9 A Closer Look at Heat and Work

18.10 The First Law of Thermodynamics You have just seen that when a system changes from a given initial state to a given final state, both the work W and the heat Q depend on the nature of the process. Experimentally, however, we find a surprising thing. The quantity, is the same for all processes.

Some Special Cases of the First Law of Thermodynamics Adiabatic processes. An adiabatic process is one that occurs so rapidly or occurs in a system that is so well insulated that no transfer of energy as heat occurs between the system and its environment. Constant-volume processes. If the volume of a system (such as a gas) is held constant, that system can do no work. Cyclical processes. There are processes in which, after certain interchanges of heat and work, the system is restored to its initial state. In that case, no intrinsic property of the system—including its internal energy—can possibly change. Free expansions. These are adiabatic processes in which no transfer of heat occurs between the system and its environment and no work is done on or by the system.

P 44. A thermodynamic system is taken from state A to state B to state C, and then back to A, as shown in the p-V diagram. The vertical scale is set by p s = 40 Pa, and the horizontal scale is set by. (a)–(g) Complete the table below by inserting a plus sign, a minus sign, or a zero in each indicated cell. (h) What is the net work done by the system as it moves once through the cycle ABCA?

18.12 Heat Transfer Mechanisms Conduction Thermal Resistance to Conduction (R-Value)

Radiation The rate P rad at which an object emits energy via electromagnetic radiation depends on the object’s surface area A and the temperature T of that area in kelvins and is given by The symbol represents the emissivity of the object’s surface, which has a value between 0 and 1, depending on the composition of the surface. The rate P abs at which an object absorbs energy via thermal radiation from its environment, which we take to be at uniform temperature T env (in kelvins), is