Physics 207: Lecture 24, Pg 1 Lecture 24 Goals: Chapter 17 Chapter 17  Apply heat and energy transfer processes  Recognize adiabatic processes Chapter.

Slides:



Advertisements
Similar presentations
The Kinetic Theory of Gases
Advertisements

As close to chemistry as we can get
Physics Subject Area Test Thermodynamics. There are three commonly used temperature scales, Fahrenheit, Celsius and Kelvin.
Thermodynamics April 27, 2015April 27, 2015April 27, 2015.
James Joule and the mechanical equivalent of heat
Energy in Thermal Processes
Temperature, Heat, and the First Law of Thermodynamics
Temperature, Heat, and the Thermal Behavior of Matter
Energy in Thermal Processes
Energy in Thermal Processes
Dr.Salwa Al Saleh Work and Heat Lecture 3.
Chapter 5 TEMPERATURE AND HEAT Dr. Babar Ali.
MECHANISMS OF HEAT TRANSFER
1 Thermal Physics 13 - Temperature & Kinetic Energy 15 - Laws of Thermodynamics.
Energy in Thermal Processes
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 16 Physics, 4 th Edition James S. Walker.
Heat. Heat and Temperature Kinetic Molecular Theory – Is the theory that matter is made up of atoms (smallest piece of matter) and that these atoms are.
Chapter 18 Temperature, Heat, and the First Law of Thermodynamics.
Heat Transfer There are 3 ways that heat can move from one place to another: radiation conduction convection.
Chapter 10 Thermal Physics. Temperature Thermodynamics – branch of physics studying thermal energy of systems Temperature ( T ), a scalar – measure of.
Chapter 11 Energy in Thermal Processes. Energy Transfer When two objects of different temperatures are placed in thermal contact, the temperature of the.
Energy in Thermal Processes
Chapter 13 States of Matter
Chapter 6.  Temperature ◦ Is something hot or cold? ◦ Relative measure.
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.
The Laws 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.
© 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.
Heat. Heat As Energy Transfer Internal Energy Specific Heat Calorimetry – Solving Problems Latent Heat Heat Transfer: Conduction Heat Transfer: Convection.
14-1 Heat As Energy Transfer If heat is a form of energy, it ought to be possible to equate it to other forms. The experiment below found the mechanical.
Thermal Physics Modes of Heat Transfer.
HEAT & THERMAL ENERGY CH. 16. State indicator 17. Demonstrate that thermal energy can be transferred by conduction, convection or radiation (e.g., through.
Unit 6 : Part 3 Heat. Outline Definition and Units of Heat Specific Heat and Calorimetry Phase Changes and Latent Heat Heat Transfer.
Physics 1501: Lecture 35, Pg 1 Physics 1501: Lecture 35 Today’s Agenda l Announcements çHomework #11 (Dec. 2) and #12 (Dec. 9): 2 lowest dropped l Honors’
Thermal contact Two systems are in thermal (diathermic) contact, if they can exchange energy without performing macroscopic work. This form of energy.
Heat – Thermal Energy ISCI What is Heat? Place your finger on the handle of a ‘hot’ pan. Ouch! Heat is energy that is transferred from one ‘system’
Chapter 20 Heat and the First Law of Thermodynamics.
Physics 207: Lecture 26, Pg 1 Physics 207, Lecture 26, Dec. 4 Exams will be returned at your next discussion section Regrades: Write down, on a separate.
Thermodynamics. What is Temperature Temperature is a measure of the kinetic energy of matter. Collision between molecules causes energy transfer Motion.
THERMAL ENERGY AND HEAT SPH4C April THERMAL ENERGY James Prescott Joule ( ) spent much of his honeymoon studying waterfalls. He noticed.
College Physics, 7th Edition
Use pV diagrams for ideal-gas processes. Chapter 17
Limitations to basic mechanics Deformable bodies (liquids, gas, soft matter) Temperature’s influence on motion Electric charge’s influence on motion Phase.
1 Work and Heat Readings: Chapter Internal Energy -Initial kinetic energy is lost due to friction. -This is not completely true, the initial kinetic.
Physics 207: Lecture 27, Pg 1 Physics 207, Lecture 27, Dec. 6 l Agenda: Ch. 20, 1 st Law of Thermodynamics, Ch. 21  1 st Law of thermodynamics (  U=
The First Law of Thermodynamics The Law of Conservation of Energy.
Temperature and Heat Temperature & Scales Thermometry Thermal Expansion Heat and Internal Energy Heat Transfer Heat and Temperature Change, Specific.
Halliday/Resnick/Walker Fundamentals of Physics
Physics 207: Lecture 24, Pg 1 Lecture 24 Goals: Chapter 17 Chapter 17  Employ heat (Q) and energy transfer in materials  Recognize adiabatic processes.
AP Physics B: Lecture #21 Second Law of Thermodynamics “Heat will not flow spontaneously from a colder body to a warmer body AND heat energy cannot be.
Chemical Thermodynamics Lecture 1. Chemical Thermodynamics Prepared by PhD Halina Falfushynska.
Ying Yi PhD Chapter 11 Energy in Thermal Processes 1 PHYS HCCS.
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 11 Energy in Thermal Processes. Energy Transfer When two objects of different temperatures are placed in thermal contact, the temperature of the.
Chapter 11 Energy in Thermal Processes. Energy Transfer When two objects of different temperatures are placed in thermal contact, the temperature of the.
Physics 141Mechanics Lecture 24 Heat and Temperature Yongli Gao So far we have concentrated on mechanical energy, including potential and kinetic energy.
PHY 151: Lecture 20B 20.4 Work and Heat in Thermodynamic Processes 20.5 First Law of Thermodynamics 20.6 Some Applications of the First Law of Thermodynamics.
Chapter 10 Heat 10-1 Temperature and Thermal Equilibrium.
College Physics, 7th Edition
Chapters 17, thermodynamics
UNIT - 4 HEAT TRANSFER.
Apply heat and energy transfer processes Recognize adiabatic processes
Chapter 14 Heat © 2014 Pearson Education, Inc..
Figure 20.1  Joule’s experiment for determining the mechanical equivalent of heat. The falling blocks rotate the paddles, causing the temperature of the.
Figure 20.1  Joule’s experiment for determining the mechanical equivalent of heat. The falling blocks rotate the paddles, causing the temperature of the.
Chapter 14 Heat.
Heat Physics 2053 Lecture Notes Heat 14 (01 of 32)
Chapter 20: Heat and the First Law of Thermodynamics
ChemE 260 Work and Heat Dr. William Baratuci Senior Lecturer
The Transfer of Heat Chapter 13.
Presentation transcript:

Physics 207: Lecture 24, Pg 1 Lecture 24 Goals: Chapter 17 Chapter 17  Apply heat and energy transfer processes  Recognize adiabatic processes Chapter 18 Chapter 18  Follow the connection between temperature, thermal energy, and the average translational kinetic energy molecules  Understand the molecular basis for pressure and the ideal- gas law.  To predict the molar specific heats of gases and solids. Assignment Assignment  HW10, Due Wednesday 9:00 AM  For Thursday, Read through all of Chapter 18

Physics 207: Lecture 24, Pg 2 (4) Isobaric (3) Isothermal (2) Isochoric (1) Adiabatic Paths on the pV diagram p V T1T1 T2T2 T3T3 T4T4 W = - p  V ???? W = 0 ???? Ideal gas

Physics 207: Lecture 24, Pg 3 Isothermal processes l Work done when PV = nRT = constant  P = nRT / V p V 3 T1T1 T2T2 T3T3 T4T4

Physics 207: Lecture 24, Pg 4 Adiabatic Processes l An adiabatic process is process in which there is no thermal energy transfer to or from a system (Q = 0) l A reversible adiabatic process involves a “worked” expansion in which we can return all of the energy transferred. l In this case PV  = const. l All real processes are not. p V T1T1 T2T2 T3T3 T4T4

Physics 207: Lecture 24, Pg 5 Work and Ideal Gas Processes (on system) l Isothermal l Isobaric l Isochoric l FYI: Adiabatic (and reversible)

Physics 207: Lecture 24, Pg 6 Combinations of Isothermal & Adiabatic Processes All engines employ a thermodynamic cycle W = ± (area under each pV curve) W cycle = area shaded in turquoise Watch sign of the work!

Physics 207: Lecture 24, Pg 7 Relationship between energy transfer and T

Physics 207: Lecture 24, Pg 8 Heat and Latent Heat l Latent heat of transformation L is the energy required for 1 kg of substance to undergo a phase change. (J / kg) Q = ±ML l Specific heat c of a substance is the energy required to raise the temperature of 1 kg by 1 K. (Units: J / K kg ) Q = M c ΔT l Molar specific heat C of a gas at constant volume is the energy required to raise the temperature of 1 mol by 1 K. Q = n C V ΔT If a phase transition involved then the heat transferred is Q = ±ML+M c ΔT

Physics 207: Lecture 24, Pg 9 Q : Latent heat and specific heat l The molar specific heat of gasses depends on the process path l C V = molar specific heat at constant volume l C p = molar specific heat at constant pressure l C p = C V +R (R is the universal gas constant)

Physics 207: Lecture 24, Pg 10 Mechanical equivalent of heat l Heating liquid water:  Q = amount of heat that must be supplied to raise the temperature by an amount  T.  [Q] = Joules or calories.  calorie: energy to raise 1 g of water from 14.5 to 15.5 °C (James Prescott Joule found the mechanical equivalent of heat.) 1 Cal = J 1 kcal = 1 Cal = 4186 J Sign convention: +Q : heat gained - Q : heat lost

Physics 207: Lecture 24, Pg 11 Exercise l The specific heat (Q = M c ΔT) of aluminum is about twice that of iron. Consider two blocks of equal mass, one made of aluminum and the other one made of iron, initially in thermal equilibrium. l Heat is added to each block at the same constant rate until it reaches a temperature of 500 K. Which of the following statements is true? (a) The iron takes less time than the aluminum to reach 500 K (b) The aluminum takes less time than the iron to reach 500 K (c) The two blocks take the same amount of time to reach 500 K

Physics 207: Lecture 24, Pg 12 Heat and Ideal Gas Processes (on system) l Isothermal Expansion/Contraction l Isobaric l Isochoric l Adiabatic

Physics 207: Lecture 24, Pg 13 Two process are shown that take an ideal gas from state 1 to state 3. Compare the work done by process A to the work done by process B. A. W A > W B B. W A < W B C. W A = W B = 0 D. W A = W B but neither is zero ON BY A 1  3 W 1  2 = 0 (isochoric) B 1  2 W 1  2 = -½ (p 1 +p 2 )(V 2 -V 1 ) 0 B 2  3 W 2  3 = -½ (p 2 +p 3 )(V 1 -V 2 ) > 0 -W 2  3 < 0 B 1  3 = ½ (p 3 - p 1 )(V 2 -V 1 ) > 0 < 0

Physics 207: Lecture 24, Pg 14 l Most people were at least once burned by hot water or steam. l Assume that water and steam, initially at 100°C, are cooled down to skin temperature, 37°C, when they come in contact with your skin. Assume that the steam condenses extremely fast, and that the specific heat c = 4190 J/ kg K is constant for both liquid water and steam. l Under these conditions, which of the following statements is true? (a) Steam burns the skin worse than hot water because the thermal conductivity of steam is much higher than that of liquid water. (b) Steam burns the skin worse than hot water because the latent heat of vaporization is released as well. (c) Hot water burns the skin worse than steam because the thermal conductivity of hot water is much higher than that of steam. (d) Hot water and steam both burn skin about equally badly. Exercise Latent Heat

Physics 207: Lecture 24, Pg 15 Energy transfer mechanisms l Thermal conduction (or conduction) l Convection l Thermal Radiation For a material of cross-section area A and length L, spanning a temperature difference ΔT = T H – T C, the rate of heat transfer is where k is the thermal conductivity, which characterizes whether the material is a good conductor of heat or a poor conductor. Q /  t = k A  T /  x

Physics 207: Lecture 24, Pg 16 Energy transfer mechanisms l Thermal conduction (or conduction):  Energy transferred by direct contact.  e.g.: energy enters the water through the bottom of the pan by thermal conduction.  Important: home insulation, etc. l Rate of energy transfer ( J / s or W )  Through a slab of area A and thickness  x, with opposite faces at different temperatures, T c and T h Q /  t = k A (T h - T c ) /  x  k :Thermal conductivity ( J / s m °C)

Physics 207: Lecture 24, Pg 17 Thermal Conductivities Aluminum238Air0.0234Asbestos0.25 Copper397Helium0.138Concrete1.3 Gold314Hydrogen0.172Glass0.84 Iron79.5Nitrogen0.0234Ice1.6 Lead34.7Oxygen0.0238Water0.60 Silver427Rubber0.2Wood0.10 J/s m °C

Physics 207: Lecture 24, Pg 18 (B) T top = T bottom (A) T top > T bottom (C) T top < T bottom 100 C T joint l Two identically shaped bars (one blue and one green) are placed between two different thermal reservoirs. The thermal conductivity coefficient k is twice as large for the blue as the green. l You measure the temperature at the joint between the green and blue bars. Which of the following is true? Home Exercise Thermal Conduction 300 C (D) need to know k

Physics 207: Lecture 24, Pg 19 l Two identically shaped bars (one blue and one green) are placed between two different thermal reservoirs. The thermal conductivity coefficient k is twice as large for the blue as the green. Home Exercise Thermal Conduction 100 C T joint 300 C Top: P green = P blue = Q /  t = 2 k A (T high - T j ) /  x= k A (T j - T low ) /  x 2 (T high - T j ) = (T j - T low )  3 T j(top) = 2 T high – T low By analogy for the bottom: 3 T j(bottom) = 2 T low – T high 3 (T j(top) - T j(bottom ) = 3 T high – 3 T low > 0 (A) T top > T bottom

Physics 207: Lecture 24, Pg C l Two thermal conductors (possibly inhomogeneous) are butted together and in contact with two thermal reservoirs held at the temperatures shown. l Which of the temperature vs. position plots below is most physical? Exercise Thermal Conduction 300 C Position Temperature Position Temperature Position Temperature (A) (B) (C)

Physics 207: Lecture 24, Pg 21 Energy transfer mechanisms l Convection:  Energy is transferred by flow of substance 1. Heating a room (air convection) 2. Warming of North Altantic by warm waters from the equatorial regions  Natural convection: from differences in density  Forced convection: from pump of fan l Radiation:  Energy is transferred by photons e.g.: infrared lamps  Stefan’s Law   = 5.7  W/m 2 K 4, T is in Kelvin, and A is the surface area  e is a constant called the emissivity P =  A e T 4 (power radiated)

Physics 207: Lecture 24, Pg 22 Minimizing Energy Transfer l The Thermos bottle, also called a Dewar flask is designed to minimize energy transfer by conduction, convection, and radiation. The standard flask is a double-walled Pyrex glass with silvered walls and the space between the walls is evacuated. Vacuum Silvered surfaces Hot or coldliquid

Physics 207: Lecture 24, Pg 23 Anti-global warming or the nuclear winter scenario l Assume P/A = I = 1340 W/m 2 from the sun is incident on a thick dust cloud above the Earth and this energy is absorbed, equilibrated and then reradiated towards space where the Earth’s surface is in thermal equilibrium with cloud. Let e (the emissivity) be unity for all wavelengths of light. l What is the Earth’s temperature?   P =  A T 4 =  (4  r 2 ) T 4 = I  r 2  T = [I / (4 x  )] ¼    = 5.7  W/m 2 K 4  T = 277 K (A little on the chilly side.)

Physics 207: Lecture 24, Pg 24 Ch. 18, Macro-micro connection Molecular Speeds and Collisions A real gas consists of a vast number of molecules, each moving randomly and undergoing millions of collisions every second. Despite the apparent chaos, averages, such as the average number of molecules in the speed range 600 to 700 m/s, have precise, predictable values. The “micro/macro” connection is built on the idea that the macroscopic properties of a system, such as temperature or pressure, are related to the average behavior of the atoms and molecules.

Physics 207: Lecture 24, Pg 25 Molecular Speeds and Collisions A view of a Fermi chopper

Physics 207: Lecture 24, Pg 26 Molecular Speeds and Collisions

Physics 207: Lecture 24, Pg 27 Mean Free Path If a molecule has N coll collisions as it travels distance L, the average distance between collisions, which is called the mean free path λ (lowercase Greek lambda), is

Physics 207: Lecture 24, Pg 28 Macro-micro connection l Assumptions for ideal gas:  # of molecules N is large  They obey Newton’s laws  Short-range interactions with elastic collisions  Elastic collisions with walls (an impulse…..pressure) l What we call temperature T is a direct measure of the average translational kinetic energy l What we call pressure p is a direct measure of the number density of molecules, and how fast they are moving (v rms )

Physics 207: Lecture 24, Pg 29 Lecture 24 Assignment Assignment  HW10, Due Wednesday (9:00 AM)  Tuesday review  Reading assignment through all of Chapter 18