Adiabatic Processes. Pressure/Temp and Vol/Temp Adiabatic Compression If I compress air at atmospheric pressure and room temperature by a factor of 10.

Slides:



Advertisements
Similar presentations
Chapter 12: Laws of Thermo
Advertisements

APHY201 5/31/ The First Law of Thermodynamics A systems internal energy can be changed by doing work or by the addition/removal of heat: ΔU.
Derivation of thermodynamic equations
PV Diagrams THERMODYNAMICS.
Work and Heat in Thermodynamic Processes
Using the “Clicker” If you have a clicker now, and did not do this last time, please enter your ID in your clicker. First, turn on your clicker by sliding.
Ch15 Thermodynamics Zeroth Law of Thermodynamics
Thermodynamic Processes Lecturer: Professor Stephen T. Thornton.
The Laws of Thermodynamics Chapter 12. Principles of Thermodynamics Energy is conserved FIRST LAW OF THERMODYNAMICS Examples: Engines (Internal -> Mechanical)
Lecture 5 First Law of Thermodynamics. You can’t get something for nothing. Nothing is for free. We will discuss these statements later…
Heat Flow. Constant Volume  Fixing the piston keeps the volume constant.  If heat flows in then temperature remains the same. heat flows at base to.
1 UCT PHY1025F: Heat and Properties of Matter Physics 1025F Heat & Properties of Matter Dr. Steve Peterson THERMODYNAMICS.
Chem Ch 19/#1 Today’s To Do List l Start Chapter 19: 1st Law P-V work State Functions 1st Law Adiabatic Processes.
PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 19. First Law of Thermodynamics Work done by/on a gas Last Lecture.
General Relations Thermodynamics Professor Lee Carkner Lecture 24.
First Law of Thermodynamics Physics 202 Professor Lee Carkner Lecture 11.
First Law of Thermodynamics Physics 102 Professor Lee Carkner Lecture 6 “of each the work shall become manifest, for the day shall declare it, because.
PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 18. The Laws of Thermodynamics Chapter 12.
1 Lec 9: Heat and work. 2 For next time: –Look at practice exams and pick questions for next time –HW5 due on Thursday, October 2nd at the exam Outline:
Internal Energy Physics 202 Professor Lee Carkner Lecture 14.
Engines Physics 202 Professor Lee Carkner Lecture 18.
Fig The net work done by the system in the process aba is –500 J.
Copyright © 2009 Pearson Education, Inc. Lecture 11: Laws of Thermodynamics.
How much work is done when the ideal gas is expanded from V 1 to V 2 at constant pressure? A] 0 B] nRT 2 C] nRT 1 D] nR(T 2 -T 1 ) E] it depends on whether.
MHS Physics Department AP Unit II C 2 Laws of Thermodynamics Ref: Chapter 12.
9.6 Work A change in the state of the system is usually accompanied by the transfer of heat and or work between the system and the surroundings. Work and.
Thermodynamics. Thermodynamic Process in which energy is transferred as heat and work.
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.
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.
Preview Objectives Heat, Work, and Internal Energy Thermodynamic Processes Chapter 10 Section 1 Relationships Between Heat and Work.
Heat, Work, and Internal Energy Thermodynamic Processes.
Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 10 Heat, Work, and Internal Energy Heat and work are energy.
Some common processes Isobaric Isobaric. Some common processes Isovolumetric Isovolumetric.
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.
Chapter 19. “A theory is the more impressive the greater the simplicity of its premises, the more different kinds of things it relates, and the more extended.
The Laws of Thermodynamics Applied to Refrigerators and Heat Engines.
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.
Thermodynamics. System / environment Diathermal / adiabatic Walls between the system and surroundings are called diathermal if they permit energy flow.
METR February Review Hydrostatic balance Pressure decreases exponentially with height, isothermal atmosphere: Zeroth law of thermodynamics:
1 Chapter 7. Applications of the Second Law. 2 Consider entropy changes in various reversible (!!!) processes We have: (a) Adiabatic process Hence a reversible.
Chapter 10 Preview Objectives Heat, Work, and Internal Energy
Ch15 Thermodynamics Zeroth Law of Thermodynamics If two systems are in thermal equilibrium with a third system, then they are in thermal equilibrium with.
CHAPTER 15 Thermodynamics Thermodynamic Systems and Their Surroundings Thermodynamics is the branch of physics that is built upon the fundamental.
Thermodynamics Chapter 10
Constant volume (isochoric) process No work is done by the gas: W = 0. The P-V diagram is a vertical line, going up if heat is added, and going down if.
First Law of Thermodynamics
First Law of Thermodynamics
Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Section 1 Relationships Between Heat and Work Chapter 10 Objectives.
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 Davidson College APSI Ideal Gas Equations P 1 V 1 / T 1 = P 2 V 2 / T 2 PV = n R T (using moles) P V = N k B T (using molecules)  P:
First Law of Thermodynamics Conservation of Energy for Thermal Systems.
Thermodynamic Processes
H. Saibi January 20 th,  The internal Energy of an Ideal Gas  Work and the PV Diagram for a Gas  Heat capacities of Gases  Heat capacities of.
Chapter 4 ENERGY ANALYSIS OF CLOSED SYSTEMS
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley. Chapter 15. Work, Heat, and the First Law of Thermodynamics.
The First Law of Thermodynamics Ideal Gas Processes
Lecture 29: 1st Law of Thermodynamics
Lecture Outline Chapter 12 College Physics, 7 th Edition Wilson / Buffa / Lou © 2010 Pearson Education, Inc.
On expanding isothermally from 2L to 4L, an ideal gas does 6J of work, as the pressure drops from 2 atm to 1 atm. By how much must it expand to do an additional.
The Laws of Thermodynamics Enrolment No.: Noble Group of Institutions - Junagadh.
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.
D. |Q| is the same for all three paths.
Quasistatic processes The relation of heat and work
The First Law of Thermodynamics
This pV–diagram shows two ways to take a system from state a (at lower left) to state c (at upper right): • via state b (at upper left), or • via state.
Thermodynamics Section 1.
Pressure - Volume Graph
Heat Flow.
Presentation transcript:

Adiabatic Processes

Pressure/Temp and Vol/Temp

Adiabatic Compression If I compress air at atmospheric pressure and room temperature by a factor of 10 the temperature will go up by 1. Less than 10 degrees C 2. Between 10 and 50 degrees C 3. Between 50 and 100 degrees C 4. More than 100 degrees C

Blow on your hand

Malachi 2:10 Have we not all one father? hath not one God created us? why do we deal treacherously every man against his brother, by profaning the covenant of our fathers?

The first law of thermodynamics ∆E int = Q + W The internal energy of an ideal gas depends only on the temperature of the gas. Change of internal energy = heat put into system + work done on system

For an ideal gas... Always!!!!!

Deriving the Adiabatic Equation i.e. Going way beyond what you need to know for the homework and exams because you will hopefully learn something and, with luck, gain a greater appreciation of the power of differential calculus...

Three things changing, but in a defined way such that if I know how one changes, I should know others. To get rid of an unknown, I need another equation – here it is! But I need to write it in terms of P, V, and T. And what do I do with the integral in it? If I have a piston whose location is x, or a balloon with a radius x, or a basketball being squished into the floor by an amount x, I should be able to tell you any one just in terms of initial conditions and x. How do things change with x?

They each only have one “T” thing (P and V show up twice, as P and dP, V and dV, in the left equation), so that’s the easy one to solve for and eliminate. Take all the constants to one side and simplify. Then to keep things tidy, call it gamma.

Get P stuff on one side, V on other, integrate. Remember, when V is equal to its initial value, P is equal to its initial value. When V is its final value, P is its final value.

The path shown below is isothermal (ΔT= 0). The change in internal energy of the gas is A. Positive B. Negative C. zero P V

The path shown below is isothermal (ΔT= 0). The heat flow is A. Into the gas B. Out of the gas C. zero P V

The path shown below is adiabatic (Q = 0). The change in internal energy of the gas is A. Positive B. Negative C. zero P V

The two lines below represent an isotherm and an adiabat. Which one is the isotherm? A. The upper one B. The lower one P V

The two lines below represent an isotherm and an adiabat. Which one is the isotherm? A. The upper one B. The lower one P V