SlideShare uma empresa Scribd logo
1 de 49
Chapter 12 Thermal Energy or How I Learned to Love Sweat
In this unit we are going to learn about the difference between heat and temperature.  Two hundred years ago that statement could not have been made.  The mid-eighteenth century saw the advance in a new theory to explain heat and temperature. The old theory that explained the difference between a hot body and cold one was called “caloric theory.”  Caloric was an invisible fluid that went into a body when it was warmed.  Hot bodies had more caloric than cold bodies.
This silly theory had a few problems.  The major one was to explain how two ice cubes could melt when rubbed together. The 18th century theory that replaced the caloric theory was (and is still) called the  kinetic molecular theory . This theory says the particles in a body are in motion.  In a hot body, the particles move faster, and thus have a higher energy than the particles in a cold body.
The internal motion of the particles in a body is its kinetic energy.  Because these particles are vibrating back and forth they have a potential energy as well.  The sum of the PE and KE of the particles is called the  thermal energy  of the object. Remember that the kinetic theory says that a hot body has more thermal energy than a cold body.  The hot body has a higher total sum of PE and KE than a cold body.  p.314 .
The number of particles also affects the amount of thermal energy in a body. Once you know that a hot body has more thermal energy than a cold body, you can understand temperature. Temperature is a measure of the  average  kinetic energy of the particles in a body. Temperature is independent of number of particles in the body. If 1-kg mass is same temperature as 2-kg mass, both have same average KE, although 2-kg mass has more thermal energy and KE than 1-kg mass.
Thermometers measure temperature, but how do they work? ,[object Object],[object Object],[object Object],[object Object]
Energy is transferred from your skin to the glass particles by the process of  conduction , the transfer of kinetic energy when particles collide.
[object Object]
Most thermometers operate with some property that changes with temperature.  Hotter thermometer = larger volume of material inside alcohol, mercury, and gas are  most common materials inside  thermometers. The first scale to measure  temperature was developed by  Anders Celsius   The Celsius scale has 0°C as  freezing point of water and  boiling point of pure water at  100°C. (Body temperature is 37°C)
 
Heat and Thermal Energy One way to increase the temperature of an object is to place it in contact with a hotter object.  The thermal energy of the hotter object is decreased, and the thermal energy of the cooler object is increased.  Energy always flows from the hotter object to the cooler object.  Energy never flows from a colder object to a hotter object.  Heat  is the energy that flows between two objects as a result of a difference in temperature.  The symbol  Q  is used to represent the amount of heat.
If  Q  has a negative value, heat has left the object; if  Q  has a positive value, heat has been absorbed by the object.  Heat, like other forms of energy, is measured in joules.
You have already learned one way that heat flows from a warmer body to a colder one.  If you place one end of a metal rod in a flame, it becomes hot.  The other end also becomes warm very quickly.  Heat is conducted because the particles in the rod are in direct contact. Thermal energy transfer
[object Object]
A second means of thermal transfer involves particles that are not in direct contact.   Have you ever looked in a pot of water just about to boil?  You can see motion of water, as water heated by conduction at the bottom of the pot flows up and the colder water at top sinks.  Heat flows between the rising hotter water and the descending colder water.  This motion of fluid, whether liquid or gas, caused by temperature differences, is  convection
 
 
The third method of thermal transfer, unlike the first two, does not depend on the presence of matter.  The sun warms us from over 150 million kilometers via  radiation , the transfer of energy by electromagnetic waves.  These waves carry the energy from the hot sun to the much cooler Earth.
When heat flows into an object, its thermal energy increases, and so does its temperature.   The amount of the increase depends on the size of the object.  It also depends on the material from which the object is made.  The   specific heat  of a material is the amount of energy that must be added to the material to raise the temperature of a unit mass one temperature unit.   Specific heat
In SI units, specific heat, represented by C (not to be confused with °C), is measured in J/kg·K. Water has a high specific heat compared to those of other substances, even ice and steam.  One kilogram of water requires the addition of 4180 J of energy to increase its temperature by one kelvin.  The same mass of copper requires only 385 J to increase its temperature by one kelvin.  The 4180 J of energy needed to raise the temperature of one kilogram of water by one kelvin would increase the temperature of the same mass of copper by 11 K.
The high specific heat of water is the reason water is used in car radiators to remove thermal energy from the engine block. The heat gained or lost by an object as its temperature changes depends on the mass, the change in temperature, and the specific heat of the substance.  The amount of heat transferred can be determined using the following equation: Q = mC  T = mC(T final  - T initial ) where  Q  is the heat gained or lost,  m  is the mass of the object,  C  is the specific heat of the substance, and   T  is the change in temperature.
When the temperature of 10.0 kg of water is increased by 5.0 K, the heat absorbed,  Q,  is Q = ( 10.0  kg)( 4180  J/kg · K)( 5.0  K) =  2.1 X 10 5  J. Because one Celsius degree is equal in magnitude to one kelvin, temperature changes can be measured in either kelvins or Celsius degrees.
Calorimetry A  calorimeter  is a device used to measure changes in thermal energy.  A calorimeter is carefully insulated so that heat transfer is very small.  A measured mass of a substance is placed in the calorimeter and heated to a high temperature.  The calorimeter contains a known mass of cold water at a measured temperature.  The heat released by the substance is transferred to the cooler water.  For the resulting increase in water temperature, the change in thermal energy of the substance is calculated.
 
The operation of a calorimeter depends on the conservation of energy in isolated, closed systems.   Energy can neither enter nor leave an isolated system.  As a result of the isolation, if the energy of one part of the system increases, the energy of another part must decrease by the same amount.   Consider a system composed of two blocks of metal, block A and block B.  The total energy of the system is constant. E A  + E B  =  constant
Suppose that the two blocks are initially separated but can be placed in contact.  If the thermal energy of block A changes by an amount E A , then the change in thermal energy of block B,  E B , must be related by the following equation: E A  +  E B  = 0 Which means that the following relationship is true: E A  = -  E B The change in energy of one block is positive, while the change in energy of the other block is negative.  If the thermal energy change is positive, the temperature of that block rises.  If the change is negative, the temperature falls.
Assume that the initial temperatures of the two blocks are different.  When the blocks are brought together, heat flows from the hotter block to the colder block.  The flow continues until the blocks are in thermal equilibrium.  The blocks then have the same temperature. In a calorimeter, the change in thermal energy is equal to the heat transferred because no work is done.  Therefore, the change in energy can be expressed by the following equation: E = Q =  m C  T
The increase in thermal energy of block A is equal to the decrease in thermal energy of block B.  Thus, the following relationship is true: m A C A   T A  +  m B   C B   T B  = 0 The change in temperature is the difference between the final and initial temperatures, that is,  T = T f -T i .  If the temperature of a block increases, T f  >T i , and  T is positive.  If the temperature of the block decrease, Tf<Ti, and  T is negative.  The final temperatures of the two blocks are equal.  The equation for the transfer of energy is m A C A (T f  - T Ai ) +  m B C B (T f  - T Bi ) = 0 .  (2) (1)
To solve for T f , expand the equation. m A C A T f  -  m A C A T Ai   + m B C B T f  - m B C B T Bi  = 0 T f  ( m A C A  +  m B C B ) =  m A C A T Ai  +  m B C B T Bi T f  =  m A C A T Ai  +  m B C B T Bi m A C A  +  m B C B
CHANGE OF STATE AND LAWS OF THERMODYNAMICS
Change of State ,[object Object],[object Object],[object Object],[object Object],[object Object]
At some point, the added thermal energy causes the particles to move rapidly enough that their motion overcomes the forces holding the particles together in a fixed location.  The particles are still touching, but they have more freedom of movement.  Eventually, the particles become free enough to slide past each other.  At this point, the substance has changed from a solid to a liquid.  The temperature at which this change occurs is the  melting point .   When a substance is melting, all of the added thermal energy goes to overcome the forces holding the particles together in the solid state.
None of the added thermal energy increases the kinetic energy of the particles.  Since the kinetic energy of the particles does not increase, the temperature does not increase here.
Once the solid is completely melted, there are no more forces holding the particles in the solid state and the added thermal energy again increases the motion of the particles, and the temperature rises.   As the temperature increases, some particles in the liquid acquire enough energy to break free from other particles.  At a specific temperature, known as the  boiling point , further addition for energy causes another change of state where all the added thermal energy converts the material from the liquid state to the gas state.   Boiling Point
The motion of the particles does not increase so the temperature is not raised during this transition. p.323 – copy graph
The amount of energy needed to melt one kilogram of a substance is called the  heat of fusion  of that substance.  The added energy causes a change in state but not in temperature. Heat of fusion
At normal atmosphere pressure, water boils at 373 K.  The thermal energy needed to vaporize one kilogram of a liquid is called the  heat of vaporization .   Each substance has a characteristic heat of vaporization.   Heat of vaporization
The heat,  Q , required to melt a solid of mass  m  is given by the equation, Q = m H f where H f  is the heat of fusion.  Similarly, the heat,  Q , required to vaporize a mass,  m , of liquid is given by the equation, Q = m H v where H v  is the heat of vaporization.  When a liquid freezes, an amount of heat  Q  = - m H f  must be removed from the liquid to turn it into a solid.
The negative sign indicates the heat is transferred from the sample to the environment. When a vapor condenses to a liquid, an amount of heat,  Q  = - m H v , must be removed.
The First Law of Thermodynamics ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
The conversion of mechanical energy to thermal energy, as when you rub your hands together, is easy.  The reverse process, conversion of thermal to mechanical energy, is more difficult.  A device able to convert thermal energy to mechanical energy continuously is called a  heat engine . Heat engine requires a high temperature source from which thermal energy can be removed, a low temperature receptacle, called a sink, into which thermal energy can be delivered, and a way to convert the thermal energy into work.
 
An automobile internal combustion engine is one example of a heat engine.  In the automobile, a mixture of air and gasoline vapor is ignited, producing a high-temperature flame.  Heat flows from the flame to the air in the cylinder.  The hot air expands and pushes on a piston, changing thermal energy into mechanical energy.  In order to obtain continuous mechanical energy, the engine must be returned to its starting condition.  The heated air is expelled and replaced by new air, and the piston is returned to the top of the cylinder.  The entire cycle is repeated many times each minute.  The thermal energy from the gasoline is converted into mechanical energy that eventually results in the movement of the car.
The Second Law of Thermodynamics Many processes that are consistent with the first law of thermodynamics have never been observed to occur spontaneously. For example, the first law of thermodynamics does not prohibit heat flowing from a cold object to a hot object. However, when hot objects have been placed in contact with cold object the hot object have never been observed to become hotter. Similarly, the cold objects have never been observed to become colder.
Entropy If heat engines completely converted thermal energy into mechanical energy with no waste heat, then the first law of thermodynamics would be obeyed. However, waste heat is always generated, and randomly distributed particles of a gas are not observed to spontaneously arrange themselves in specific ordered patterns. This is best described in terms of a quantity called  entropy , which is a measure of the disorder of a system.
When a baseball is dropped and falls due to gravity, it possesses potential and kinetic energies that can be recovered to do work. However, when the baseball fall through the air, it collides with many air molecules that absorb some of its energy. This causes air molecules to move in random directions and at random speeds. The energy absorbed from the baseball causes more disorder among the molecules. The greater range of speeds exhibited by the molecules, the greater the disorder, which in turn increase the entropy. Entropy, like thermal energy, is contained in an object.
If heat is added to an object, entropy is increased. If heat is removed from an object, entropy is decreased. If an object does work with no change in temperature, the entropy does not change, as long as friction is ignored. The change in entropy, ∆S, is expressed by the following equation, in which entropy has units of J/K and the temperature is measured in kelvins. The  second law of thermodynamics  states that natural processes go in a direction that maintains or increases the total entropy of the universe. That is, all things will become more and more disordered unless some action is taken to keep them ordered.
The second law of thermodynamics predicts that heat flows spontaneously only from a hot object to a cold object. The entropy of the final state is greater than that of the initial state.
 

Mais conteúdo relacionado

Mais procurados

W4_Lecture_Transient heat conduction.ppt
W4_Lecture_Transient heat conduction.pptW4_Lecture_Transient heat conduction.ppt
W4_Lecture_Transient heat conduction.ppt
Mike275736
 

Mais procurados (20)

Heat transfer by convection
Heat transfer by convectionHeat transfer by convection
Heat transfer by convection
 
Heat Transfer
Heat TransferHeat Transfer
Heat Transfer
 
Heat and Mass Transfer Basics
Heat and Mass Transfer BasicsHeat and Mass Transfer Basics
Heat and Mass Transfer Basics
 
Micro pulsating heat pipe
Micro pulsating heat pipeMicro pulsating heat pipe
Micro pulsating heat pipe
 
ME6301 ENGINEERING THERMODYNAMICS - LECTURE NOTES
ME6301 ENGINEERING THERMODYNAMICS - LECTURE NOTESME6301 ENGINEERING THERMODYNAMICS - LECTURE NOTES
ME6301 ENGINEERING THERMODYNAMICS - LECTURE NOTES
 
Extended surface fins
Extended surface finsExtended surface fins
Extended surface fins
 
Tons of Refrigeration
Tons of RefrigerationTons of Refrigeration
Tons of Refrigeration
 
Heat 4e chap03_lecture
Heat 4e chap03_lectureHeat 4e chap03_lecture
Heat 4e chap03_lecture
 
Thermodynamics - Unit - II
Thermodynamics - Unit - II Thermodynamics - Unit - II
Thermodynamics - Unit - II
 
Cartesian Coordinates Derivation.pdf
Cartesian Coordinates Derivation.pdfCartesian Coordinates Derivation.pdf
Cartesian Coordinates Derivation.pdf
 
Chapter 1 introduction of heat transfer
Chapter 1 introduction of heat transferChapter 1 introduction of heat transfer
Chapter 1 introduction of heat transfer
 
Lecture 1 introduction of engineering thermodynamics
Lecture 1 introduction of engineering thermodynamicsLecture 1 introduction of engineering thermodynamics
Lecture 1 introduction of engineering thermodynamics
 
(3) heat conduction equation [compatibility mode]
(3) heat conduction equation [compatibility mode](3) heat conduction equation [compatibility mode]
(3) heat conduction equation [compatibility mode]
 
Heat 4e chap11_lecture
Heat 4e chap11_lectureHeat 4e chap11_lecture
Heat 4e chap11_lecture
 
Radiation heat transfer
Radiation heat transferRadiation heat transfer
Radiation heat transfer
 
W4_Lecture_Transient heat conduction.ppt
W4_Lecture_Transient heat conduction.pptW4_Lecture_Transient heat conduction.ppt
W4_Lecture_Transient heat conduction.ppt
 
Heat exchanger
Heat exchanger Heat exchanger
Heat exchanger
 
Principles of temperature measurement
Principles of temperature measurementPrinciples of temperature measurement
Principles of temperature measurement
 
Heat Transfer Applications
Heat Transfer ApplicationsHeat Transfer Applications
Heat Transfer Applications
 
Chapter 6 FUNDAMENTALS OF CONVECTION
Chapter 6FUNDAMENTALS OF CONVECTIONChapter 6FUNDAMENTALS OF CONVECTION
Chapter 6 FUNDAMENTALS OF CONVECTION
 

Destaque

5th grade chapter 14 section 4 - what is thermal energy
5th grade chapter 14 section 4 - what is thermal energy5th grade chapter 14 section 4 - what is thermal energy
5th grade chapter 14 section 4 - what is thermal energy
hinsz
 
Thermal Energy & Heat Transfer
Thermal Energy & Heat TransferThermal Energy & Heat Transfer
Thermal Energy & Heat Transfer
Alan Wrafter
 
Thermal energy
Thermal energyThermal energy
Thermal energy
theMrNeale
 
Compact Thermal Energy Storage
Compact Thermal Energy StorageCompact Thermal Energy Storage
Compact Thermal Energy Storage
Leonardo ENERGY
 
Sci 10 4.2 early theories of heat
Sci 10 4.2 early theories of heatSci 10 4.2 early theories of heat
Sci 10 4.2 early theories of heat
Sherry Heschuk
 
Synopsis of steam power plant system
Synopsis of steam power plant systemSynopsis of steam power plant system
Synopsis of steam power plant system
mundaa
 
Thermal energy transfer notes without highlights
Thermal energy transfer notes without highlightsThermal energy transfer notes without highlights
Thermal energy transfer notes without highlights
xmaldonado
 

Destaque (20)

Thermal Energy PPT
Thermal Energy PPTThermal Energy PPT
Thermal Energy PPT
 
5th grade chapter 14 section 4 - what is thermal energy
5th grade chapter 14 section 4 - what is thermal energy5th grade chapter 14 section 4 - what is thermal energy
5th grade chapter 14 section 4 - what is thermal energy
 
Thermal Energy & Heat Transfer
Thermal Energy & Heat TransferThermal Energy & Heat Transfer
Thermal Energy & Heat Transfer
 
Transfer of Thermal Energy
Transfer of Thermal EnergyTransfer of Thermal Energy
Transfer of Thermal Energy
 
Thermal energy
Thermal energyThermal energy
Thermal energy
 
Thermal energy
Thermal energyThermal energy
Thermal energy
 
Compact Thermal Energy Storage
Compact Thermal Energy StorageCompact Thermal Energy Storage
Compact Thermal Energy Storage
 
Coduction, convection and radiation
Coduction, convection and radiationCoduction, convection and radiation
Coduction, convection and radiation
 
Presentation on Geothermal Energy
Presentation on Geothermal EnergyPresentation on Geothermal Energy
Presentation on Geothermal Energy
 
Heat Transfer
Heat TransferHeat Transfer
Heat Transfer
 
Thermal power point
Thermal power pointThermal power point
Thermal power point
 
Sci 10 4.2 early theories of heat
Sci 10 4.2 early theories of heatSci 10 4.2 early theories of heat
Sci 10 4.2 early theories of heat
 
SPM Phyiscs - Thermal energy
SPM Phyiscs - Thermal energySPM Phyiscs - Thermal energy
SPM Phyiscs - Thermal energy
 
Publikasi Karya Ilmiah Tahun 2014 (Jurnal Internasional)
Publikasi Karya Ilmiah Tahun 2014 (Jurnal Internasional)Publikasi Karya Ilmiah Tahun 2014 (Jurnal Internasional)
Publikasi Karya Ilmiah Tahun 2014 (Jurnal Internasional)
 
Heat
HeatHeat
Heat
 
Synopsis of steam power plant system
Synopsis of steam power plant systemSynopsis of steam power plant system
Synopsis of steam power plant system
 
Thermal energy transfer notes without highlights
Thermal energy transfer notes without highlightsThermal energy transfer notes without highlights
Thermal energy transfer notes without highlights
 
solar thermal energy
solar thermal energysolar thermal energy
solar thermal energy
 
Heat powerpoint
Heat powerpointHeat powerpoint
Heat powerpoint
 
Synopsis of solar tracker and charging monitor
Synopsis of solar tracker and charging monitorSynopsis of solar tracker and charging monitor
Synopsis of solar tracker and charging monitor
 

Semelhante a Chapter 12 - Thermal Energy

Minooka Atoms and Elements Part 1
Minooka Atoms and Elements Part 1Minooka Atoms and Elements Part 1
Minooka Atoms and Elements Part 1
Jeanne Erfft
 
02-20-08 - Thermodynamics
02-20-08 - Thermodynamics02-20-08 - Thermodynamics
02-20-08 - Thermodynamics
wjerlinger
 
Unit 3 pp #2, #3, and #4 7th grade
Unit 3 pp #2, #3, and #4 7th gradeUnit 3 pp #2, #3, and #4 7th grade
Unit 3 pp #2, #3, and #4 7th grade
Tarina Medford
 
Heat Lecture Slides
Heat Lecture SlidesHeat Lecture Slides
Heat Lecture Slides
Ed Stermer
 

Semelhante a Chapter 12 - Thermal Energy (20)

4_5994635259759561834.pdf
4_5994635259759561834.pdf4_5994635259759561834.pdf
4_5994635259759561834.pdf
 
3 1
3 13 1
3 1
 
Minooka Atoms and Elements Part 1
Minooka Atoms and Elements Part 1Minooka Atoms and Elements Part 1
Minooka Atoms and Elements Part 1
 
02-20-08 - Thermodynamics
02-20-08 - Thermodynamics02-20-08 - Thermodynamics
02-20-08 - Thermodynamics
 
Thermo
ThermoThermo
Thermo
 
Thermal Properties of Material presentation
Thermal Properties of Material presentationThermal Properties of Material presentation
Thermal Properties of Material presentation
 
Thermo
ThermoThermo
Thermo
 
Module No. 31
Module No. 31Module No. 31
Module No. 31
 
Thermodynamics
ThermodynamicsThermodynamics
Thermodynamics
 
Heat and Calorie
Heat and CalorieHeat and Calorie
Heat and Calorie
 
12C W9 Thermal physics.pptx
12C W9 Thermal physics.pptx12C W9 Thermal physics.pptx
12C W9 Thermal physics.pptx
 
Thermo dynamics
Thermo dynamicsThermo dynamics
Thermo dynamics
 
Measurement and effects of heat
Measurement and effects of heatMeasurement and effects of heat
Measurement and effects of heat
 
Physics Thermodynamics Notes Grade 11
Physics Thermodynamics Notes Grade 11Physics Thermodynamics Notes Grade 11
Physics Thermodynamics Notes Grade 11
 
Ch14 S1and2
Ch14 S1and2Ch14 S1and2
Ch14 S1and2
 
Chapter 14 heat and heat transfer methods
Chapter 14   heat and heat transfer methodsChapter 14   heat and heat transfer methods
Chapter 14 heat and heat transfer methods
 
for publishing.pptx
for publishing.pptxfor publishing.pptx
for publishing.pptx
 
Unit 3 pp #2, #3, and #4 7th grade
Unit 3 pp #2, #3, and #4 7th gradeUnit 3 pp #2, #3, and #4 7th grade
Unit 3 pp #2, #3, and #4 7th grade
 
Heat Lecture Slides
Heat Lecture SlidesHeat Lecture Slides
Heat Lecture Slides
 
Presentation 1.pdf
Presentation 1.pdfPresentation 1.pdf
Presentation 1.pdf
 

Mais de Galen West

Mais de Galen West (18)

Chapter 14 - Gases
Chapter 14 - GasesChapter 14 - Gases
Chapter 14 - Gases
 
Chapter 4 - The Atom
Chapter 4 - The AtomChapter 4 - The Atom
Chapter 4 - The Atom
 
Chapter 18 Lenses And Refraction
Chapter 18   Lenses And RefractionChapter 18   Lenses And Refraction
Chapter 18 Lenses And Refraction
 
Chapter 12 Stoichiometry
Chapter 12   StoichiometryChapter 12   Stoichiometry
Chapter 12 Stoichiometry
 
Chap16 Light
Chap16   LightChap16   Light
Chap16 Light
 
Chapter 11 - Reaction Types
Chapter 11 - Reaction TypesChapter 11 - Reaction Types
Chapter 11 - Reaction Types
 
Chapter 10 - Chemical Quantities
Chapter 10 - Chemical QuantitiesChapter 10 - Chemical Quantities
Chapter 10 - Chemical Quantities
 
Energy, Work, and Simple Machines - Chapter 10
Energy, Work, and Simple Machines - Chapter 10Energy, Work, and Simple Machines - Chapter 10
Energy, Work, and Simple Machines - Chapter 10
 
Covalent Bonding - Chapter 8
Covalent Bonding - Chapter 8Covalent Bonding - Chapter 8
Covalent Bonding - Chapter 8
 
Chapter7 - Test A Answers
Chapter7 - Test A AnswersChapter7 - Test A Answers
Chapter7 - Test A Answers
 
Ionic Bonds - Chapter 7
Ionic Bonds  - Chapter 7Ionic Bonds  - Chapter 7
Ionic Bonds - Chapter 7
 
Momentum - Chapter 9
Momentum - Chapter 9Momentum - Chapter 9
Momentum - Chapter 9
 
Chemistry Jeopardy
Chemistry JeopardyChemistry Jeopardy
Chemistry Jeopardy
 
Physics Jeopardy
Physics JeopardyPhysics Jeopardy
Physics Jeopardy
 
Universal Gravitation
Universal GravitationUniversal Gravitation
Universal Gravitation
 
Periodic Table Chapter 14
Periodic Table   Chapter 14Periodic Table   Chapter 14
Periodic Table Chapter 14
 
Friction
FrictionFriction
Friction
 
Models
ModelsModels
Models
 

Último

Cloud Frontiers: A Deep Dive into Serverless Spatial Data and FME
Cloud Frontiers:  A Deep Dive into Serverless Spatial Data and FMECloud Frontiers:  A Deep Dive into Serverless Spatial Data and FME
Cloud Frontiers: A Deep Dive into Serverless Spatial Data and FME
Safe Software
 
+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...
+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...
+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...
?#DUbAI#??##{{(☎️+971_581248768%)**%*]'#abortion pills for sale in dubai@
 

Último (20)

Boost Fertility New Invention Ups Success Rates.pdf
Boost Fertility New Invention Ups Success Rates.pdfBoost Fertility New Invention Ups Success Rates.pdf
Boost Fertility New Invention Ups Success Rates.pdf
 
Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...
Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...
Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...
 
TrustArc Webinar - Unlock the Power of AI-Driven Data Discovery
TrustArc Webinar - Unlock the Power of AI-Driven Data DiscoveryTrustArc Webinar - Unlock the Power of AI-Driven Data Discovery
TrustArc Webinar - Unlock the Power of AI-Driven Data Discovery
 
Apidays New York 2024 - Accelerating FinTech Innovation by Vasa Krishnan, Fin...
Apidays New York 2024 - Accelerating FinTech Innovation by Vasa Krishnan, Fin...Apidays New York 2024 - Accelerating FinTech Innovation by Vasa Krishnan, Fin...
Apidays New York 2024 - Accelerating FinTech Innovation by Vasa Krishnan, Fin...
 
FWD Group - Insurer Innovation Award 2024
FWD Group - Insurer Innovation Award 2024FWD Group - Insurer Innovation Award 2024
FWD Group - Insurer Innovation Award 2024
 
Cloud Frontiers: A Deep Dive into Serverless Spatial Data and FME
Cloud Frontiers:  A Deep Dive into Serverless Spatial Data and FMECloud Frontiers:  A Deep Dive into Serverless Spatial Data and FME
Cloud Frontiers: A Deep Dive into Serverless Spatial Data and FME
 
"I see eyes in my soup": How Delivery Hero implemented the safety system for ...
"I see eyes in my soup": How Delivery Hero implemented the safety system for ..."I see eyes in my soup": How Delivery Hero implemented the safety system for ...
"I see eyes in my soup": How Delivery Hero implemented the safety system for ...
 
AWS Community Day CPH - Three problems of Terraform
AWS Community Day CPH - Three problems of TerraformAWS Community Day CPH - Three problems of Terraform
AWS Community Day CPH - Three problems of Terraform
 
Axa Assurance Maroc - Insurer Innovation Award 2024
Axa Assurance Maroc - Insurer Innovation Award 2024Axa Assurance Maroc - Insurer Innovation Award 2024
Axa Assurance Maroc - Insurer Innovation Award 2024
 
Navi Mumbai Call Girls 🥰 8617370543 Service Offer VIP Hot Model
Navi Mumbai Call Girls 🥰 8617370543 Service Offer VIP Hot ModelNavi Mumbai Call Girls 🥰 8617370543 Service Offer VIP Hot Model
Navi Mumbai Call Girls 🥰 8617370543 Service Offer VIP Hot Model
 
+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...
+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...
+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...
 
presentation ICT roal in 21st century education
presentation ICT roal in 21st century educationpresentation ICT roal in 21st century education
presentation ICT roal in 21st century education
 
Apidays Singapore 2024 - Scalable LLM APIs for AI and Generative AI Applicati...
Apidays Singapore 2024 - Scalable LLM APIs for AI and Generative AI Applicati...Apidays Singapore 2024 - Scalable LLM APIs for AI and Generative AI Applicati...
Apidays Singapore 2024 - Scalable LLM APIs for AI and Generative AI Applicati...
 
Repurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost Saving
Repurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost SavingRepurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost Saving
Repurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost Saving
 
Real Time Object Detection Using Open CV
Real Time Object Detection Using Open CVReal Time Object Detection Using Open CV
Real Time Object Detection Using Open CV
 
EMPOWERMENT TECHNOLOGY GRADE 11 QUARTER 2 REVIEWER
EMPOWERMENT TECHNOLOGY GRADE 11 QUARTER 2 REVIEWEREMPOWERMENT TECHNOLOGY GRADE 11 QUARTER 2 REVIEWER
EMPOWERMENT TECHNOLOGY GRADE 11 QUARTER 2 REVIEWER
 
Powerful Google developer tools for immediate impact! (2023-24 C)
Powerful Google developer tools for immediate impact! (2023-24 C)Powerful Google developer tools for immediate impact! (2023-24 C)
Powerful Google developer tools for immediate impact! (2023-24 C)
 
A Year of the Servo Reboot: Where Are We Now?
A Year of the Servo Reboot: Where Are We Now?A Year of the Servo Reboot: Where Are We Now?
A Year of the Servo Reboot: Where Are We Now?
 
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobe
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, AdobeApidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobe
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobe
 
Artificial Intelligence Chap.5 : Uncertainty
Artificial Intelligence Chap.5 : UncertaintyArtificial Intelligence Chap.5 : Uncertainty
Artificial Intelligence Chap.5 : Uncertainty
 

Chapter 12 - Thermal Energy

  • 1. Chapter 12 Thermal Energy or How I Learned to Love Sweat
  • 2. In this unit we are going to learn about the difference between heat and temperature. Two hundred years ago that statement could not have been made. The mid-eighteenth century saw the advance in a new theory to explain heat and temperature. The old theory that explained the difference between a hot body and cold one was called “caloric theory.” Caloric was an invisible fluid that went into a body when it was warmed. Hot bodies had more caloric than cold bodies.
  • 3. This silly theory had a few problems. The major one was to explain how two ice cubes could melt when rubbed together. The 18th century theory that replaced the caloric theory was (and is still) called the kinetic molecular theory . This theory says the particles in a body are in motion. In a hot body, the particles move faster, and thus have a higher energy than the particles in a cold body.
  • 4. The internal motion of the particles in a body is its kinetic energy. Because these particles are vibrating back and forth they have a potential energy as well. The sum of the PE and KE of the particles is called the thermal energy of the object. Remember that the kinetic theory says that a hot body has more thermal energy than a cold body. The hot body has a higher total sum of PE and KE than a cold body. p.314 .
  • 5. The number of particles also affects the amount of thermal energy in a body. Once you know that a hot body has more thermal energy than a cold body, you can understand temperature. Temperature is a measure of the average kinetic energy of the particles in a body. Temperature is independent of number of particles in the body. If 1-kg mass is same temperature as 2-kg mass, both have same average KE, although 2-kg mass has more thermal energy and KE than 1-kg mass.
  • 6.
  • 7. Energy is transferred from your skin to the glass particles by the process of conduction , the transfer of kinetic energy when particles collide.
  • 8.
  • 9. Most thermometers operate with some property that changes with temperature. Hotter thermometer = larger volume of material inside alcohol, mercury, and gas are most common materials inside thermometers. The first scale to measure temperature was developed by Anders Celsius The Celsius scale has 0°C as freezing point of water and boiling point of pure water at 100°C. (Body temperature is 37°C)
  • 10.  
  • 11. Heat and Thermal Energy One way to increase the temperature of an object is to place it in contact with a hotter object. The thermal energy of the hotter object is decreased, and the thermal energy of the cooler object is increased. Energy always flows from the hotter object to the cooler object. Energy never flows from a colder object to a hotter object. Heat is the energy that flows between two objects as a result of a difference in temperature. The symbol Q is used to represent the amount of heat.
  • 12. If Q has a negative value, heat has left the object; if Q has a positive value, heat has been absorbed by the object. Heat, like other forms of energy, is measured in joules.
  • 13. You have already learned one way that heat flows from a warmer body to a colder one. If you place one end of a metal rod in a flame, it becomes hot. The other end also becomes warm very quickly. Heat is conducted because the particles in the rod are in direct contact. Thermal energy transfer
  • 14.
  • 15. A second means of thermal transfer involves particles that are not in direct contact. Have you ever looked in a pot of water just about to boil? You can see motion of water, as water heated by conduction at the bottom of the pot flows up and the colder water at top sinks. Heat flows between the rising hotter water and the descending colder water. This motion of fluid, whether liquid or gas, caused by temperature differences, is convection
  • 16.  
  • 17.  
  • 18. The third method of thermal transfer, unlike the first two, does not depend on the presence of matter. The sun warms us from over 150 million kilometers via radiation , the transfer of energy by electromagnetic waves. These waves carry the energy from the hot sun to the much cooler Earth.
  • 19. When heat flows into an object, its thermal energy increases, and so does its temperature. The amount of the increase depends on the size of the object. It also depends on the material from which the object is made. The specific heat of a material is the amount of energy that must be added to the material to raise the temperature of a unit mass one temperature unit. Specific heat
  • 20. In SI units, specific heat, represented by C (not to be confused with °C), is measured in J/kg·K. Water has a high specific heat compared to those of other substances, even ice and steam. One kilogram of water requires the addition of 4180 J of energy to increase its temperature by one kelvin. The same mass of copper requires only 385 J to increase its temperature by one kelvin. The 4180 J of energy needed to raise the temperature of one kilogram of water by one kelvin would increase the temperature of the same mass of copper by 11 K.
  • 21. The high specific heat of water is the reason water is used in car radiators to remove thermal energy from the engine block. The heat gained or lost by an object as its temperature changes depends on the mass, the change in temperature, and the specific heat of the substance. The amount of heat transferred can be determined using the following equation: Q = mC  T = mC(T final - T initial ) where Q is the heat gained or lost, m is the mass of the object, C is the specific heat of the substance, and  T is the change in temperature.
  • 22. When the temperature of 10.0 kg of water is increased by 5.0 K, the heat absorbed, Q, is Q = ( 10.0 kg)( 4180 J/kg · K)( 5.0 K) = 2.1 X 10 5 J. Because one Celsius degree is equal in magnitude to one kelvin, temperature changes can be measured in either kelvins or Celsius degrees.
  • 23. Calorimetry A calorimeter is a device used to measure changes in thermal energy. A calorimeter is carefully insulated so that heat transfer is very small. A measured mass of a substance is placed in the calorimeter and heated to a high temperature. The calorimeter contains a known mass of cold water at a measured temperature. The heat released by the substance is transferred to the cooler water. For the resulting increase in water temperature, the change in thermal energy of the substance is calculated.
  • 24.  
  • 25. The operation of a calorimeter depends on the conservation of energy in isolated, closed systems. Energy can neither enter nor leave an isolated system. As a result of the isolation, if the energy of one part of the system increases, the energy of another part must decrease by the same amount. Consider a system composed of two blocks of metal, block A and block B. The total energy of the system is constant. E A + E B = constant
  • 26. Suppose that the two blocks are initially separated but can be placed in contact. If the thermal energy of block A changes by an amount E A , then the change in thermal energy of block B, E B , must be related by the following equation: E A + E B = 0 Which means that the following relationship is true: E A = - E B The change in energy of one block is positive, while the change in energy of the other block is negative. If the thermal energy change is positive, the temperature of that block rises. If the change is negative, the temperature falls.
  • 27. Assume that the initial temperatures of the two blocks are different. When the blocks are brought together, heat flows from the hotter block to the colder block. The flow continues until the blocks are in thermal equilibrium. The blocks then have the same temperature. In a calorimeter, the change in thermal energy is equal to the heat transferred because no work is done. Therefore, the change in energy can be expressed by the following equation: E = Q = m C T
  • 28. The increase in thermal energy of block A is equal to the decrease in thermal energy of block B. Thus, the following relationship is true: m A C A T A + m B C B T B = 0 The change in temperature is the difference between the final and initial temperatures, that is, T = T f -T i . If the temperature of a block increases, T f >T i , and T is positive. If the temperature of the block decrease, Tf<Ti, and T is negative. The final temperatures of the two blocks are equal. The equation for the transfer of energy is m A C A (T f - T Ai ) + m B C B (T f - T Bi ) = 0 . (2) (1)
  • 29. To solve for T f , expand the equation. m A C A T f - m A C A T Ai + m B C B T f - m B C B T Bi = 0 T f ( m A C A + m B C B ) = m A C A T Ai + m B C B T Bi T f = m A C A T Ai + m B C B T Bi m A C A + m B C B
  • 30. CHANGE OF STATE AND LAWS OF THERMODYNAMICS
  • 31.
  • 32. At some point, the added thermal energy causes the particles to move rapidly enough that their motion overcomes the forces holding the particles together in a fixed location. The particles are still touching, but they have more freedom of movement. Eventually, the particles become free enough to slide past each other. At this point, the substance has changed from a solid to a liquid. The temperature at which this change occurs is the melting point . When a substance is melting, all of the added thermal energy goes to overcome the forces holding the particles together in the solid state.
  • 33. None of the added thermal energy increases the kinetic energy of the particles. Since the kinetic energy of the particles does not increase, the temperature does not increase here.
  • 34. Once the solid is completely melted, there are no more forces holding the particles in the solid state and the added thermal energy again increases the motion of the particles, and the temperature rises. As the temperature increases, some particles in the liquid acquire enough energy to break free from other particles. At a specific temperature, known as the boiling point , further addition for energy causes another change of state where all the added thermal energy converts the material from the liquid state to the gas state. Boiling Point
  • 35. The motion of the particles does not increase so the temperature is not raised during this transition. p.323 – copy graph
  • 36. The amount of energy needed to melt one kilogram of a substance is called the heat of fusion of that substance. The added energy causes a change in state but not in temperature. Heat of fusion
  • 37. At normal atmosphere pressure, water boils at 373 K. The thermal energy needed to vaporize one kilogram of a liquid is called the heat of vaporization . Each substance has a characteristic heat of vaporization. Heat of vaporization
  • 38. The heat, Q , required to melt a solid of mass m is given by the equation, Q = m H f where H f is the heat of fusion. Similarly, the heat, Q , required to vaporize a mass, m , of liquid is given by the equation, Q = m H v where H v is the heat of vaporization. When a liquid freezes, an amount of heat Q = - m H f must be removed from the liquid to turn it into a solid.
  • 39. The negative sign indicates the heat is transferred from the sample to the environment. When a vapor condenses to a liquid, an amount of heat, Q = - m H v , must be removed.
  • 40.
  • 41. The conversion of mechanical energy to thermal energy, as when you rub your hands together, is easy. The reverse process, conversion of thermal to mechanical energy, is more difficult. A device able to convert thermal energy to mechanical energy continuously is called a heat engine . Heat engine requires a high temperature source from which thermal energy can be removed, a low temperature receptacle, called a sink, into which thermal energy can be delivered, and a way to convert the thermal energy into work.
  • 42.  
  • 43. An automobile internal combustion engine is one example of a heat engine. In the automobile, a mixture of air and gasoline vapor is ignited, producing a high-temperature flame. Heat flows from the flame to the air in the cylinder. The hot air expands and pushes on a piston, changing thermal energy into mechanical energy. In order to obtain continuous mechanical energy, the engine must be returned to its starting condition. The heated air is expelled and replaced by new air, and the piston is returned to the top of the cylinder. The entire cycle is repeated many times each minute. The thermal energy from the gasoline is converted into mechanical energy that eventually results in the movement of the car.
  • 44. The Second Law of Thermodynamics Many processes that are consistent with the first law of thermodynamics have never been observed to occur spontaneously. For example, the first law of thermodynamics does not prohibit heat flowing from a cold object to a hot object. However, when hot objects have been placed in contact with cold object the hot object have never been observed to become hotter. Similarly, the cold objects have never been observed to become colder.
  • 45. Entropy If heat engines completely converted thermal energy into mechanical energy with no waste heat, then the first law of thermodynamics would be obeyed. However, waste heat is always generated, and randomly distributed particles of a gas are not observed to spontaneously arrange themselves in specific ordered patterns. This is best described in terms of a quantity called entropy , which is a measure of the disorder of a system.
  • 46. When a baseball is dropped and falls due to gravity, it possesses potential and kinetic energies that can be recovered to do work. However, when the baseball fall through the air, it collides with many air molecules that absorb some of its energy. This causes air molecules to move in random directions and at random speeds. The energy absorbed from the baseball causes more disorder among the molecules. The greater range of speeds exhibited by the molecules, the greater the disorder, which in turn increase the entropy. Entropy, like thermal energy, is contained in an object.
  • 47. If heat is added to an object, entropy is increased. If heat is removed from an object, entropy is decreased. If an object does work with no change in temperature, the entropy does not change, as long as friction is ignored. The change in entropy, ∆S, is expressed by the following equation, in which entropy has units of J/K and the temperature is measured in kelvins. The second law of thermodynamics states that natural processes go in a direction that maintains or increases the total entropy of the universe. That is, all things will become more and more disordered unless some action is taken to keep them ordered.
  • 48. The second law of thermodynamics predicts that heat flows spontaneously only from a hot object to a cold object. The entropy of the final state is greater than that of the initial state.
  • 49.