Chapter 18. The table shows the properties of four gases, each having the same number of molecules. Rank in order, from largest to smallest, the mean.

Slides:



Advertisements
Similar presentations
The Kinetic Theory of Gases
Advertisements

Kinetic Theory of Gases I
The Kinetic Theory of Gases
Ideal gas and kinetic gas theory Boltzmann constant.
Physics for Scientists and Engineers, 6e
The Kinetic Theory of Gases
Chapter 21 The Kinetic Theory of Gases EXAMPLES. Chapter 21 The Kinetic Theory of Gases: Examples.
Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley Atomic/molecular collisions and pressure The kinetic-molecular theory relates.
Nankai University Song Feng Chapter 4 Boltzman Distribution in infirm-coupling system Prof. Song
Kinetic Theory and Thermodynamics
Physics 207: Lecture 25, Pg 1 Lecture 25Goals: Chapters 18, micro-macro connection Chapters 18, micro-macro connection Third test on Thursday at 7:15 pm.
Gases and Heat Chapter 18.
Knight: Chapter 18 The Micro/Macro Connection
Physics 207: Lecture 27, Pg 1 Lecture 26Goals: Chapters 18, entropy and second law of thermodynamics Chapters 18, entropy and second law of thermodynamics.
Entropy Physics 202 Professor Lee Carkner Lecture 17 “Entropy isn’t what it used to be.” --Anonymous.
Lecture 344/24/06. Entropy (Measurement of disorder) Related to number of microstates ∆S universe = ∆S system + ∆S surroundings 2 nd Law of Thermodynamics.
MSEG 803 Equilibria in Material Systems 8: Statistical Ensembles Prof. Juejun (JJ) Hu
AME Int. Heat Trans. D. B. GoSlide 1 Non-Continuum Energy Transfer: Gas Dynamics.
Internal Energy Physics 202 Professor Lee Carkner Lecture 14.
Internal Energy Physics 202 Professor Lee Carkner Lecture 16.
Thermal Properties of Matter
Chapter 18 Lecture.
Knight: Chapter 18 The Micro/Macro Connection
Dr. Jie ZouPHY Chapter 21 The Kinetic Theory of Gases.
For the cyclic process shown, W is:D A] 0, because it’s a loop B] p 0 V 0 C] - p 0 V 0 D] 2 p 0 V 0 E] 6 p 0 V 0 For the cyclic process shown,  U is:
AP Physics Mr. Jean November 8 th, Problems: A segment of steel railroad track has a length of m when the temperature is at 0.0 o C. What.
The Kinetic Theory of Gases Chapter 19 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Gas molar specific heats Mean kinetic energy of a gas molecule: If we have n moles of gas: Then molar specific heat at constant volume should be: What.
Chapter 10 Thermal Physics. Temperature Thermodynamics – branch of physics studying thermal energy of systems Temperature ( T ), a scalar – measure of.
PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, & Dr. Derrick Boucher Assoc. Prof. of Physics Session 24, Chapter 18.
CHAPTER 15 : KINETIC THEORY OF GASSES
Results from kinetic theory, 1 1. Pressure is associated with collisions of gas particles with the walls. Dividing the total average force from all the.
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
講者: 許永昌 老師 1. Contents Molecular Speeds and Collisions Pressure Temperature Thermal energy and Specific heat Thermal interaction and Heat Irreversible.
Q19. Second Law of Thermodynamics
Thermal Physics Thermal Physics is the study of temperature and heat and how they effect matter. Heat leads to change in internal energy which shows as.
President UniversityErwin SitompulThermal Physics 5/1 Lecture 5 Thermal Physics Dr.-Ing. Erwin Sitompul President University
Physics 207: Lecture 26, Pg 1 Lecture 26 Goals: Chapter 18 Chapter 18  Understand the molecular basis for pressure and the ideal- gas law.  Predict the.
THERMOCHEMISTRY Courtesy of lab-initio.com. Definitions #1 Energy: The capacity to do work or produce heat. Potential Energy: Energy due to position or.
Thermal Energy Heat & Temperature. Definitions  Energy  Can do work  Kinetic Energy  Energy associated with the motion of objects, large or small.
Chapter 19 The Kinetic Theory of Gases To study p, V, E int, T, …etc. from a “molecular” approach 19.1 A new way to look at gases: Warm up: How many moles.
Temperature and Kinetic Theory
The Kinetic Theory of Gases
Ludwid Boltzmann 1844 – 1906 Contributions to Kinetic theory of gases Electromagnetism Thermodynamics Work in kinetic theory led to the branch of.
Thermal Physics Chapter 10. Thermal Physics Thermal physics looks at temperature, heat, and internal energy Heat and temperature are not the same thing.
Chapter 10 Thermal Physics. Thermal physics is the study of Temperature Heat How these affect matter.
Temperature & the Laws of Thermodynamics Lecture Notes
PHY1039 Properties of Matter Equation-of-State for an Ideal Gas 13 February, 2012 Lecture 3.
Heat & The First Law of Thermodynamics
Thermodynamic Nature of Energy P M V Subbarao Professor Mechanical Engineering Department The Root Cause behind All Thermodynamic Actions…..
The Kinetic Theory of Gases
Thermodynamics. Thermodynamic Systems, States and Processes Objectives are to: define thermodynamics systems and states of systems explain how processes.
CHE 116 No. 1 Chapter Nineteen Copyright © Tyna L. Meeks All Rights Reserved.
Halliday/Resnick/Walker Fundamentals of Physics
Micro & Macro Descriptions of Internal Energy P M V Subbarao Professor Mechanical Engineering Department Important Form of Energy for Engineering Systems.
Chapter 23 The First Law of Thermodynamics. Thermal Physics Macroscopic Microscopic The Diffusion The Viscous The Transfer of Heat Exchange molecule T.
Q18. First Law of Thermodynamics. 1.A quantity of an ideal gas is compressed to half its initial volume. The process may be adiabatic, isothermal or isobaric.
Chapter 9 Heat.
THE SECOND LAW OF THERMODYNAMICS Entropy. Entropy and the direction of time Microscopically the eqs. of physics are time reversible ie you can turn the.
The Kinetic Theory of Gases
Ch18 The Micro/Macro Connection
Q18.1 A quantity of an ideal gas is contained in a balloon. Initially the gas temperature is 27°C. You double the pressure on the balloon and change the.
Lecture 25 Goals: Chapter 18
The Kinetic Theory of Gases
Ideal Gases Kinetic Theory of Gases
Thermal Properties of Matter
Understand the molecular basis for pressure and the ideal-gas law.
Entropy & the 2nd Law of Thermodynamics
The Distribution of Molecular Speeds
The Micro/Macro Connection
Presentation transcript:

Chapter 18

The table shows the properties of four gases, each having the same number of molecules. Rank in order, from largest to smallest, the mean free paths of molecules in these gases. GasABCD VolumeV2V2VVV Atomic massmm2m2mm Atomic radiusrrr2r2r

The table shows the properties of four gases, each having the same number of molecules. Rank in order, from largest to smallest, the mean free paths of molecules in these gases. GasABCD VolumeV2V2VVV Atomic massmm2m2mm Atomic radiusrrr2r2r

The speed of every molecule in a gas is suddenly increased by a factor of 4. As a result, v rms increases by a factor of >4 but not necessarily <4, but not necessarily

The speed of every molecule in a gas is suddenly increased by a factor of 4. As a result, v rms increases by a factor of >4 but not necessarily <4, but not necessarily

1. 1 mol of He at p = 1 atm, T = 300 K 2. 2 mol of N 2 at p = 0.5 atm, T = 450 K 3. 2 mol of He at p = 2 atm, T = 300 K 4. 1 mol of Ar at p = 0.5 atm, T = 450 K 5. 1 mol of N 2 at p = 0.5 atm, T = 600 K Which system has the largest average translational kinetic energy per molecule?

1. 1 mol of He at p = 1 atm, T = 300 K 2. 2 mol of N 2 at p = 0.5 atm, T = 450 K 3. 2 mol of He at p = 2 atm, T = 300 K 4. 1 mol of Ar at p = 0.5 atm, T = 450 K 5. 1 mol of N 2 at p = 0.5 atm, T = 600 K

How many degrees of freedom does a bead on a wire have?

How many degrees of freedom does a bead on a wire have?

Systems A and B are interacting thermally. At this instant of time, 1. T A = T B. 2. T A > T B. 3. T A < T B.

Systems A and B are interacting thermally. At this instant of time, 1. T A = T B. 2. T A > T B. 3. T A < T B.

Two identical boxes each contain 1,000,000 molecules. In box A, 750,000 molecules happen to be in the left half the box while 250,000 are in the right half. In box B. 499,900 molecules happen to be in the left half the box while 500,100 are in the right half. At this instant of time, 1. The entropy of box A is smaller than the entropy of box B. 2. The entropy of box A is equal to the entropy of box B. 3. The entropy of box A is larger than the entropy of box B.

Two identical boxes each contain 1,000,000 molecules. In box A, 750,000 molecules happen to be in the left half the box while 250,000 are in the right half. In box B. 499,900 molecules happen to be in the left half the box while 500,100 are in the right half. At this instant of time, 1. The entropy of box A is smaller than the entropy of box B. 2. The entropy of box A is equal to the entropy of box B. 3. The entropy of box A is larger than the entropy of box B.

Chapter 18 Reading Quiz

What is the name of the quantity represented as v rms ? 1. random-measured-step viscosity 2. root-mean-squared speed 3. relative-mean-system velocity 4. radial-maser-system volume

What is the name of the quantity represented as v rms ? 1. random-measured-step viscosity 2. root-mean-squared speed 3. relative-mean-system velocity 4. radial-maser-system volume

What additional kind of energy makes C V larger for a diatomic than for a monatomic gas? 1. Charismatic energy 2. Translational energy 3. Heat energy 4. Rotational energy 5. Solar energy

What additional kind of energy makes C V larger for a diatomic than for a monatomic gas? 1. Charismatic energy 2. Translational energy 3. Heat energy 4. Rotational energy 5. Solar energy

The second law of thermodynamics says that 1. the entropy of an isolated system never decreases. 2. heat never flows spontaneously from cold to hot. 3. the total thermal energy of an isolated system is constant. 4. both 1 and both 1 and 3.

The second law of thermodynamics says that 1. the entropy of an isolated system never decreases. 2. heat never flows spontaneously from cold to hot. 3. the total thermal energy of an isolated system is constant. 4. both 1 and both 1 and 3.

1. both microscopic and macroscopic processes are reversible. 2. both microscopic and macroscopic processes are irreversible. 3. microscopic processes are reversible and macroscopic processes are irreversible. 4. microscopic processes are irreversible and macroscopic processes are reversible. In general,

1. both microscopic and macroscopic processes are reversible. 2. both microscopic and macroscopic processes are irreversible. 3. microscopic processes are reversible and macroscopic processes are irreversible. 4. microscopic processes are irreversible and macroscopic processes are reversible. In general,