Gas Processes. Gas Process The thermodynamic state of a gas is defined by pressure, volume, and temperature. A “gas process” describes how gas gets from.

Slides:



Advertisements
Similar presentations
Chapter 12: Laws of Thermo
Advertisements

Ideal Monatomic Gas C v = 3/2R C p = C v + R = 5/2 R Polyatomic Gas C v > 3/2R C p > 5/2 R All Ideal Gases  E = q + w w = -P ext  V (for now)  E = nC.
Do Now (11/7/13): What are the major topics and concepts from our unit on Fluids and Heat?
Chapter 18: Heat,Work,the First Law of Thermodynamics
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.
Thermodynamics April 27, 2015April 27, 2015April 27, 2015.
Standards/Plan.
First Law of Thermodynamics
Physics 52 - Heat and Optics Dr. Joseph F
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.
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.
Dr. Jie ZouPHY Chapter 20 Heat and the First Law of Thermodynamics (cont.)
First law of thermodynamics
The First Law of Thermodynamics
First Law of Thermodynamics Physics 102 Professor Lee Carkner Lecture 5 (Session: )
Fig The infinitesimal work done by the system (gas) during the small expansion dx is dW = p A dx.
Knight: Chapter 17 Work, Heat, & the 1st Law of Thermodynamics
Fig The net work done by the system in the process aba is –500 J.
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:
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.
1 Adiabatic Flame Temperature Reaction Q W P 2 =P a T 2 =T a Consider the case where the cylinder is perfectly insulated so the process is adiabatic (
Matter and Energy. Drill Answer the following: 1) List the 3 types of energy: 2) The air inside of a basketball left outside on a cold day cools and contracts.
The Laws of Thermodynamics
The first law of thermodynamics Deduce an expression for the work involved in a volume change of a gas at constant pressure State the first.
1 Thermal Physics 13 - Temperature & Kinetic Energy 15 - Laws of Thermodynamics.
Warm up!  What is the difference between Isothermal and Adiabatic?  Describe the difference using the relationship between Internal energy(  U), heat(Q),
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.
What affects the behavior of a gas? u The number of particles present u Volume (the size of the container) u Temperature 2.
Thermodynamics. Thermodynamic Process in which energy is transferred as heat and work.
Thermodynamic Quantities Defined Internal Energy = U = the sum of all the energy held by the molecules: * the PE stored in their chemical bonds, attractions.
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.
CHAPTER 16 : THERMODYNAMICS
17.4 State Variables State variables describe the state of a system
Chapter 15 Thermodynamics.
1 Introduction Physics 313 Professor Lee Carkner Lecture 1.
Chapter 15: Thermodynamics
The Laws of Thermodynamics
Chemistry. Chemical energetics-1 Session Objectives.
b The good news is that you don’t have to remember all three gas laws! Since they are all related to each other, we can combine them into a single equation.
Thermodynamics How Energy Is Transferred As Heat and Work Animation Courtesy of Louis Moore.
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.
when system is subdivided? Intensive variables: T, P Extensive variables: V, E, H, heat capacity C.
The Laws of Thermodynamics
حرارة وديناميكا حرارية
Ch15 Thermodynamics Zeroth Law of Thermodynamics If two systems are in thermal equilibrium with a third system, then they are in thermal equilibrium with.
Ideal Gases. Ideal Gas vs. Real Gas Gases are “most ideal”… at low P & high T in nonpolar atoms/molecules Gases are “real”… Under low T & high P when.
Gas Cycles 2 nd Law of Thermodynamics. Work done by a cycle When a gas undergoes a complete cycle, it starts and ends in the same state. The gas is identical.
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
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.
Option B - Thermodynamics Year 13 SL Physics. Thermodynamics System – Environment of activity Surroundings – Factors impacting the system Boundary (wall)
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:
What volume will 1 mole of a gas occupy at STP? STP = 273K, 1.013x10 5 Pa One mole of any ideal gas occupies a volume of 22.4L at STP.
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.
The First Law of Thermodynamics Ideal Gas Processes
Chapter 15 Thermodynamics Thermodynamic Systems and Their Surroundings Thermodynamics is the branch of physics that is built upon the fundamental.
Work in Thermodynamic Processes
THERMODYNAMICS THE NEXT STEP. THERMAL PROPERTIES OF MATTER STATE VARIABLES – DESCRIBE THE SUBSTANCE –PRESSURE –TEMPERATURE –VOLUME –QUANITY OF SUBSTANCE.
Lecture #20: Thermodynamics AP Physics B. Work done by a gas Suppose you had a piston filled with a specific amount of gas. As you add heat, the temperature.
Energy. Energy is classified: Kinetic energy – energy of motion Potential energy – energy of position Both energies can be transferred from one object.
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.
How much wood… ? U -W Q.
Chapter 2 The First Law Unit 3 adiabatic process
AP PHYSICS AP ME to TE problem.
Physics 2 – March 9, 2017 P3 Challenge – What is the sign of W, the work done by a gas during a) an expansion, and b) a compression. Today’s Objective:
Ch 15: laws of Thermo Includes ideas about energy and work associated with a working gas in a piston/cylinder arrangement.
A THERMODYNAMIC SYSTEM
Consider an isothermal reversible expansion of an ideal gas
Presentation transcript:

Gas Processes

Gas Process The thermodynamic state of a gas is defined by pressure, volume, and temperature. A “gas process” describes how gas gets from one state to another state. Processes depend on the behavior of the boundary and the environment more than they depend on the behavior of the gas.

T1T1 T2T2 T3T3 Gas “isotherms” Isothermal Process (constant temperature) P V PV = nRT  T = 0 (constant T) Initial State of Gas Final State of Gas Isothermal Process

Isobaric Process (constant pressure) P V T1T1 T2T2 T3T3 PV = nRT  P = 0 (constant P) Isobaric Expansion Isobaric Contraction

Isometric Process (constant volume) P V T1T1 T2T2 T3T3  V = 0 (constant V) PV = nRT

Adiabatic process (insulated) P V T isotherm adiabat Q = 0 (no heat enters or leaves) Temperature, pressure, and volume all change in an adiabatic process. PV = nRT

Work Calculation of work done on a system (or by a system) is an important part of thermodynamic calculations. Work depends upon volume change. Work also depends upon the pressure at which the volume change occurs.

p Work done BY gas VV p W gas = p  V W env = -p  V Positive work Negative work

p Work done ON gas VV p W gas = p  V W ext = -p  V Negative since  V is negative Positive since  V is negative

Sample problem Calculate the work done by a gas that expands from m 3 to 0.80 m 3 at constant atmospheric pressure. How much work is done by the environment when the gas expands this much?

Sample problem What is the change in volume of a cylinder operating at atmospheric pressure if its internal energy decreases by 230 J when 120 J of heat are removed from it?

W CD = p 1  V Work (isobaric) P V P2P2 V1V1 A V2V2 B P1P1 C D W AB > W CD Where we are considering work done BY the gas W AB = p 2  V

W ACD Work is path dependent P V P2P2 V1V1 A V2V2 B P1P1 C D W ABD > W ACD Where we are considering work done BY the gas W ABD

Problem One mole of a gas goes from state A (200 kPa and 0.5 m 3 ) to state B (150 kPa and 1.5 m 3 ). – A) What is the change in temperature of the gas during this process?

Problem One mole of a gas goes from state A (200 kPa and 0.5 m 3 ) to state B (150 kPa and 1.5 m 3 ). – B) Draw this process, assuming the smoothest possible transition (straight line) for the process. – C) Estimate the work done by the gas during the process. – D) Estimate the work done by the environment during the process.

Sample Problem Draw the gas process from state A (200 kPa and 0.5 m3) to state B (150 kPa and 1.5 m3).