Fitting Data in Mathematica

MSE 310/ECE 340. Instructor: Bill Knowlton. Initialize data Clear somedata, someplot. Place data in list somedata

MSE 3/ECE 340 Instructor: Bill Knowlton Examples of Plotting Functions ü Example 1: Using the command ListPlot[ ] to plot data in a scatter plot In[1]:= Initialize data Clear somedata someplot Place data

A Poor Example of a Project - But Gives Some Direction

A Poor Example of a Project - But Gives Some Direction Bill Knowlton Materials Science & Engineering Electrical & Computer Engineering Boise State Unversity The idea behind this example is two-fold: 1.

Concepts of Approximate Error: Approximate Error, Absolute Approximate Error, Relative Approximate Error, and Absolute Relative Approximate Error

Concepts of Approximate Error: Approximate Error, Absolute Approximate Error, Relative Approximate Error, and Absolute Relative Approximate Error Sean Rodby, Luke Snyder, Autar Kaw University of South

Chemical Kinetics and Equilibrium - An Overview - Key

Chemical Kinetics and Equilibrium - An Overview - Key The following questions are designed to give you an overview of the toics of chemical kinetics and chemical equilibrium. Although not comrehensive,

Alpha Decay. 1. Introduction. 2. Constants, Commands, and Functions. 2.1 Constants:

1. Introduction Alpha Decay One of the earliest and most convincing verifications of the validity of quantum mechanics was the resolution of the paradox of alpha decay observed in heavy nuclei. Gamow,

PHYS 301 HOMEWORK #9-- SOLUTIONS

PHYS 0 HOMEWORK #9-- SOLUTIONS. We are asked to use Dirichlet' s theorem to determine the value of f (x) as defined below at x = 0, ± /, ± f(x) = 0, - < x

Calculus I Homework: The Derivatives of Polynomials and Exponential Functions Page 1

Calculus I Homework: The Derivatives of Polynomials and Exponential Functions Page 1 Questions Example Differentiate the function y = ae v + b v + c v 2. Example Differentiate the function y = A + B x

Global Warming? Effects on Glaciers

This project has been funded with support from the European Commission. This publication reflects the views only of the author, and the Commission cannot be held responsible for any use which may be made

CHAPTER 6 : LITERATURE REVIEW

CHAPTER 6 : LITERATURE REVIEW Chapter : LITERATURE REVIEW 77 M E A S U R I N G T H E E F F I C I E N C Y O F D E C I S I O N M A K I N G U N I T S A B S T R A C T A n o n l i n e a r ( n o n c o n v e

P E R E N C O - C H R I S T M A S P A R T Y

L E T T I C E L E T T I C E I S A F A M I L Y R U N C O M P A N Y S P A N N I N G T W O G E N E R A T I O N S A N D T H R E E D E C A D E S. B A S E D I N L O N D O N, W E H A V E T H E P E R F E C T R

PHYSICS 301/MATH 355 HOMEWORK #8

PHYSICS 3/MATH 355 HOMEWORK #8 Solutions Question # We consider the integral : where m and n are both integers. We can evaluate this integral : Integrate@Cos@m xd Cos@n xd, 8x, π, π

Grain elevator. You need to convince your boss that this is a very inefficient system.

Grain elevator You are working for a grain storage comany over the summer, and they have a roblem with the grain elevator, that kees breaking down. This morning, your boss woke u feeling like a genius

T i t l e o f t h e w o r k : L a M a r e a Y o k o h a m a. A r t i s t : M a r i a n o P e n s o t t i ( P l a y w r i g h t, D i r e c t o r )

v e r. E N G O u t l i n e T i t l e o f t h e w o r k : L a M a r e a Y o k o h a m a A r t i s t : M a r i a n o P e n s o t t i ( P l a y w r i g h t, D i r e c t o r ) C o n t e n t s : T h i s w o

dn i where we have used the Gibbs equation for the Gibbs energy and the definition of chemical potential

Chem 467 Sulement to Lectures 33 Phase Equilibrium Chemical Potential Revisited We introduced the chemical otential as the conjugate variable to amount. Briefly reviewing, the total Gibbs energy of a system

Quantum Mechanics using Matrix Methods

Quantum Mechanics using Matrix Methods Introduction and the simple harmonic oscillator In this notebook we study some problems in quantum mechanics using matrix methods. We know that we can solve quantum

School of Materials Science & Engineering

Problem Set 1 Solutions Reminder From Syllabus: Problem Set Format Checklist: At the top of the page, include your name, problem set number, course name & number, and date. Submitted problem sets must

GSOE9210 Engineering Decisions

GSOE9 Engineering Decisions Problem Set 5. Consider the river roblem described in lectures: f f V B A B + (a) For =, what is the sloe of the Bayes indifference line through A? (b) Draw the Bayes indifference

Lecture 8, the outline

Lecture, the outline loose end: Debye theory of solids more remarks on the first order hase transition. Bose Einstein condensation as a first order hase transition 4He as Bose Einstein liquid Lecturer:

Differentiation of Continuous Functions Central Difference Approximation of the First Derivative

Differentiation of Continuous Functions Central Difference Approximation of the First Derivative Ana Catalina Torres, Autar Kaw University of South Florida United States of America kaw@eng.usf.edu Introduction

HEAT, WORK, AND THE FIRST LAW OF THERMODYNAMICS

HET, ORK, ND THE FIRST L OF THERMODYNMIS 8 EXERISES Section 8. The First Law of Thermodynamics 5. INTERPRET e identify the system as the water in the insulated container. The roblem involves calculating

COMPUTING FOURIER SERIES

COMPUTING FOURIER SERIES Overview We have see i revious otes how we ca use the fact that si ad cos rereset comlete orthogoal fuctios over the iterval [-,] to allow us to determie the coefficiets of a Fourier

Chapter 20: Exercises: 3, 7, 11, 22, 28, 34 EOC: 40, 43, 46, 58

Chater 0: Exercises:, 7,,, 8, 4 EOC: 40, 4, 46, 8 E: A gasoline engine takes in.80 0 4 and delivers 800 of work er cycle. The heat is obtained by burning gasoline with a heat of combustion of 4.60 0 4.

Chapter 11. Molecular Composition of Gases

Chapter 11 Molecular Composition of Gases PART 1 Volume-Mass Relationships of Gases Avogadro s Law Equal volumes of gases at the same temperature and pressure contain equal numbers of molecules. Recall

Physicist's Introduction to Mathematica

Physicist's Introduction to Mathematica Laboratory 6 Part B Fitting Curves to Data Preliminary Remarks It is increasingly rare for your activity in the laboratory to be describable as "hands-on" production

Dumas Method. A method to determine the molar mass of a compound.

Dumas Method A method to determine the molar mass of a compound. The Dumas method uses the ideal gas law to determine the molar mass of a compound which is a liquid that has a boiling point between room

ME201/MTH21/ME400/CHE400 ASSIGNMENT #7 PROBLEM 1 Newton's Law of Cooling in Transient Conduction 1. Introduction This notebook uses Mathematica to solve problem 1 of Assignment #7, in which we analyze

( ) Chapter 12. Problem Problem Problem 12.3 G = T = 0 T = K. Mg CO3 = Mg O + CO2. We know that ( ) 10 amt

Chater Problem. We know that ( ) Mg 3 = Mg O + G = G + R ln Π= G + R ln ( ) r r in atm amt in atm Let us find temerature at which rg = =, and from able A- we know that rg 76 7 = 76 7 const7ln + = 76 =

Physics 2A (Fall 2012) Chapters 11:Using Energy and 12: Thermal Properties of Matter

Physics 2A (Fall 2012) Chaters 11:Using Energy and 12: Thermal Proerties of Matter "Kee in mind that neither success nor failure is ever final." Roger Ward Babson Our greatest glory is not in never failing,

Adequacy of Regression Models

nbm_reg_sim_adequacy.nb 1 Adequacy of Regression Models Autar Kaw, Jamie Trahan University of South Florida United States of America kaw@eng.usf.edu ClearAll; Introduction This worksheet allows you to

Thermal wind and temperature perturbations

Thermal wind and temerature erturbations Robert Lindsay Korty Massachusetts Institute of Technology October 15, 2002 Following the work of Bretherton (1966), we showed in class that a boundary otential

8.6 Recursion and Computer Algebra Systems

8.6 Recursion and Computer Algebra Systems There is frequently debate as to if how and when computers should be introduced teaching a topic such as recurrence relations. We have chosen to append this information

Class 4: More Pendulum results

Class 4: More Pendulum results The pendulum is a mechanical problem with a long and interesting history, from Galileo s first ansatz that the period was independent of the amplitude based on watching priests

Thermodynamics in combustion

Thermodynamics in combustion 2nd ste in toolbox Thermodynamics deals with a equilibrium state and how chemical comosition can be calculated for a system with known atomic or molecular comosition if 2 indeendent

December 18, 2017 Section W Nandyalam

Mathematica Gift #11 Problem Complete the following 15 exercises in a Mathematica notebook. You should write the problem in a text cell and show your work below the question. Questions Question 1 Compute

Sample Mathematica code for the paper "Modeling a Diving Board"

Sample Mathematica code for the paper "Modeling a Diving Board" Michael A. Karls and Brenda M. Skoczelas, Department of Mathematical Sciences, Ball State University, Muncie, IN 47306 Beam Data Original

ATM The thermal wind Fall, 2016 Fovell

ATM 316 - The thermal wind Fall, 2016 Fovell Reca and isobaric coordinates We have seen that for the synotic time and sace scales, the three leading terms in the horizontal equations of motion are du dt

ME 406 Bifurcations VII Subcritical Hopf Bifurcation

ME 406 Bifurcations VII Subcritical Hopf Bifurcation sysid Mathematica 4.1.2, DynPac 10.66, 3ê5ê2002 intreset; plotreset; 1. Introduction In this notebook, the seventh in a series of notebooks on bifurcations,

PHYS1001 PHYSICS 1 REGULAR Module 2 Thermal Physics Chapter 17 First Law of Thermodynamics

PHYS1001 PHYSICS 1 REGULAR Module Thermal Physics Chater 17 First Law of Thermodynamics References: 17.1 to 17.9 Examles: 17.1 to 17.7 Checklist Thermodynamic system collection of objects and fields. If

ME201/MTH281/ME400/CHE400 Newton's Law of Cooling

ME1/MTH281/ME0/CHE0 Newton's Law of Cooling 1. Introduction This notebook uses Mathematica to solve the problem presented in class, in section 5.1 of the notes. The problem is one of transient heat conduction

Efficiencies. Damian Vogt Course MJ2429. Nomenclature. Symbol Denotation Unit c Flow speed m/s c p. pressure c v. Specific heat at constant J/kgK

Turbomachinery Lecture Notes 1 7-9-1 Efficiencies Damian Vogt Course MJ49 Nomenclature Subscrits Symbol Denotation Unit c Flow seed m/s c Secific heat at constant J/kgK ressure c v Secific heat at constant

ME201/MTH281/ME400/CHE400 Zeros of Bessel Function Derivatives

ME201/MTH281/ME400/CHE400 Zeros of Bessel Function Derivatives In[42]:= We write code here to find the n th zero of the derivative of the Bessel function J m. Here n is a positive integer, and m is any

HW #6. 1. Inflaton. (a) slow-roll regime. HW6.nb 1

HW6.nb HW #6. Inflaton (a) slow-roll regime In the slow-roll regime, we neglect the kinetic energy as well as f ÿÿ term in the equation of motion. Then H = ÅÅÅ 8 p 3 G N ÅÅÅ m f, 3 H f ÿ + m f = 0. We

6.7 Thermal wind in pressure coordinates

176 CHAPTER 6. THE EQUATIONS OF FLUID MOTION 6.7 Thermal wind in ressure coordinates The thermal wind relation aroriate to the atmoshere is untidy when exressed with height as a vertical coordinate (because

The Second Law: The Machinery

The Second Law: The Machinery Chater 5 of Atkins: The Second Law: The Concets Sections 3.7-3.9 8th Ed, 3.3 9th Ed; 3.4 10 Ed.; 3E 11th Ed. Combining First and Second Laws Proerties of the Internal Energy

Physicist's Introduction to Mathematica

Physicist's Introduction to Mathematica Physics 200 Physics 50 Lab Revised for V6.0 Fall Semester 2000 Spring Semester 2006 Summer 2007 Nicholas Wheeler John Boccio John Boccio REED COLLEGE Swarthmore

CHAPTER 16. Basic Concepts. Basic Concepts. The Equilibrium Constant. Reaction Quotient & Equilibrium Constant. Chemical Equilibrium

Proerties of an Equilibrium System CHAPTER 6 Chemial Equilibrium Equilibrium systems are DYNAMIC (in onstant motion) REVERSIBLE an be aroahed from either diretion Pink to blue Co(H O) 6 Cl ---> > Co(H

MODULE 2: DIFFUSION LECTURE NO DIFFUSION COEFFICIENT: MEASUREMENT AND PREDICTION

NPTEL Chemical ass Transfer Oeration OULE : IFFUSION LECTURE NO. 4.4 IFFUSION COEFFICIENT: ESUREENT N PREICTION The roortionality factor of Fick s law is called diffusivity or diffusion coefficient which

5 Linear Homotopy. 5-1 Introduction

Algebraic Geodesy and Geoinformatics - 2009 PART I METHODS 5 Linear Homotopy 5-1 Introduction Most often, there exist a fundamental task of solving systems of equations in geodesy. In such cases, many

Project 2 by Kayli-Anna Barriteau

Project 2 by Kayli-Anna Barriteau Decay of quinine in a malaria patient Data for the decay of a mg dose of quinine in a patient suffering from malaria is given in Mathematica format below. The first number

Problem Set 5 Solution

Problem Set 5 Solution Friday, 14 October 011 Physics 111 Proble The Setup For a pair of point masses, and m, interacting via a conservative force directed along the line joining the masses, show that

FUGACITY. It is simply a measure of molar Gibbs energy of a real gas.

FUGACITY It is simly a measure of molar Gibbs energy of a real gas. Modifying the simle equation for the chemical otential of an ideal gas by introducing the concet of a fugacity (f). The fugacity is an

f(r) = a d n) d + + a0 = 0

Math 400-00/Foundations of Algebra/Fall 07 Polynomials at the Foundations: Roots Next, we turn to the notion of a root of a olynomial in Q[x]. Definition 8.. r Q is a rational root of fx) Q[x] if fr) 0.

AP Chem Chapter 12 Notes: Gaseous Equilibrium

AP Chem Chapter 12 Notes: Gaseous Equilibrium Equilibrium I. Equilibrium is reached when both the and reactions are occurring at. A. Dynamic Equilibrium: reactions are still occurring but the of reactants

THE FIRST LAW OF THERMODYNAMICS

THE FIRST LA OF THERMODYNAMIS 9 9 (a) IDENTIFY and SET UP: The ressure is constant and the volume increases (b) = d Figure 9 Since is constant, = d = ( ) The -diagram is sketched in Figure 9 The roblem

The extreme case of the anisothermal calorimeter when there is no heat exchange is the adiabatic calorimeter.

.4. Determination of the enthaly of solution of anhydrous and hydrous sodium acetate by anisothermal calorimeter, and the enthaly of melting of ice by isothermal heat flow calorimeter Theoretical background

HW5.nb 1. , we find d t = - ÅÅÅÅÅ

HW5.nb HW #5. Boltzmann equation

Isothermal vs. adiabatic compression

Isothermal vs. adabatc comresson 1. One and a half moles of a datomc gas at temerature 5 C are comressed sothermally from a volume of 0.015 m to a volume of 0.0015 m. a. Sketch the rocess on a dagram and

Problem Set 1 Solution

Problem Set 1 Solution Friday, 9 September 2011 Physics 111 Exercise 1 Watch the 20-minute Wolfram tutorial introducing Mathematica at http://url. wolfram.com/fgkkpc/. Even if you already know how to use

2 EC-wave propagation using Mathematica. 2.1 O-X propagation for 2nd harmonic resonance for KSTAR tokamak with low density

2 EC-wave propagation using Mathematica 2.1 O-X propagation for 2nd harmonic resonance for KSTAR tokamak with low density 8 OX-propagation-2ndHarm-lowDensity.nb 1 Propagation of 84-GHz Microwave in KSTAR

STK4900/ Lecture 7. Program

STK4900/9900 - Lecture 7 Program 1. Logistic regression with one redictor 2. Maximum likelihood estimation 3. Logistic regression with several redictors 4. Deviance and likelihood ratio tests 5. A comment

1 14a. 1 14a is always a repellor, according to the derivative criterion.

In[3]:= f Functionx, x^ a; Solvex fx, x Out[4]= x 4a, x 4a So the fixed points are x 4a and x 4a. f'x x f' 4a 4a f' 4a 4a Since f ' 4a 4a is always greater than (due to the fact that 4a 0 when a0), we

Homework 3 and Mid-term

Homework 3 and Mid-term ECE 4339 Spring 2014 Han Q. Le (copyrighted) U. of Houston Choose a combination of problems so that the total >= 100 pts to submit as part 1. Then the rest can be submitted a week

A comparison of two barometers: Nicholas Fortin versus Robert Bosch

Isn t that a daisy? Doc Holliday A comarison of two barometers: Nicholas Fortin versus Robert Bosch Andrew Mosedale I have heard the whisers. I know the rumors. I attend to the gossi. Does it even work?

Stability of critical points in Linear Systems of Ordinary Differential Equations (SODE)

Stability of critical points in Linear Systems of Ordinary Differential Equations (SODE) In this chapter Mathematica will be used to study the stability of the critical points of twin equation linear SODE.

Laboratory exercise 2. FY2302 Biophysics I Department of Physics NTNU, Enzyme kinetics

Laoratory exercise. FY0 Biohysics I Deartment of Physics NTNU, 0 Enzyme kinetics Overview In this laoratory you will monitor the conversion of hydrogen eroxide (H O ) to water and oxygen gas y the enzyme

Apply the concept of percent yield to stoichiometric problems. Methanol can be produced through the reaction of CO and H 2 in the presence of a

Apply the concept of percent yield to stoichiometric problems. Methanol can be produced through the reaction of CO and H 2 in the presence of a catalyst. CO (g) + H 2 (g) CH 3 OH (l) If 75.0 g of CO reacts

Subject: Modeling of Thermal Rocket Engines; Nozzle flow; Control of mass flow. p c. Thrust Chamber mixing and combustion

16.50 Leture 6 Subjet: Modeling of Thermal Roket Engines; Nozzle flow; Control of mass flow Though onetually simle, a roket engine is in fat hysially a very omlex devie and diffiult to reresent quantitatively

Lecture 28: Kinetics of Oxidation of Metals: Part 1: rusting, corrosion, and

Lecture 8: Kinetics of xidation of etals: Part 1: rusting, corrosion, and the surface rotection, all about chemistry Today s toics hemical rocesses of oxidation of metals: the role layed by oxygen. How

CarnotVDWA.nb 1. Carnot Knowledge. Hal Harris Department of Chemistry University of Missouri-St. Louis St. Louis, Missouri

CarnotVDWA.nb 1 Carnot Knowledge This is the first part of this worksheet and describes the Carnot cycle for an ideal gas Hal Harris Department of Chemistry University of Missouri-St. Louis St. Louis,

A Review of Trigonometry

A Review of Trigonometr 0 Kenneth Levasseur Mathematical Sciences UMass Lowell Kenneth_Levasseur@uml.edu Introduction Trigonometr is often introduced as a sstem of ratios of sides of right triangles. Although

Differentiation 1. The METRIC Project, Imperial College. Imperial College of Science Technology and Medicine, 1996.

Differentiation 1 The METRIC Project, Imperial College. Imperial College of Science Technology and Medicine, 1996. 1 Launch Mathematica. Type

Physics 101: Lecture 27 Thermodynamics

Final hysics 101: Lecture 27 Thermodynamics Today s lecture will cover Textbook Chapter 15.1-15.6 Check your grades in grade book!! hysics 101: Lecture 27, g 1 0 N=81 Mean=76.5 Number of students 20 10

MODULE 2: DIFFUSION LECTURE NO. 2

PTEL Chemical Mass Transfer Oeration MODULE : DIFFUSIO LECTURE O.. STEDY STTE MOLECULR DIFFUSIO I FLUIDS UDER STGT D LMIR FLOW CODITIOS.. Steady state diffusion through a constant area Steady state diffusion

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Introduction to Optimization (Spring 2004) Midterm Solutions

MASSAHUSTTS INSTITUT OF THNOLOGY 15.053 Introduction to Otimization (Sring 2004) Midterm Solutions Please note that these solutions are much more detailed that what was required on the midterm. Aggregate

Towards understanding the Lorenz curve using the Uniform distribution. Chris J. Stephens. Newcastle City Council, Newcastle upon Tyne, UK

Towards understanding the Lorenz curve using the Uniform distribution Chris J. Stehens Newcastle City Council, Newcastle uon Tyne, UK (For the Gini-Lorenz Conference, University of Siena, Italy, May 2005)

Introduction to Stoichiometry

Introduction to Stoichiometry Objectives: Introduction to concepts of stoichiometry. How we use the coefficients How to determine the limiting reactant How mass figures into stoichiometry How to determine

We now turn to considerations of mixtures. To keep our discussion reasonably simple,

143 Lecture 23 We now turn to considerations of mixtures. To kee our discussion reasonably simle, we will limit our discussion to non-reacting systems, and to non-ionic systems. In other words, we will

Internal Energy in terms of Properties

Lecture #3 Internal Energy in terms of roerties Internal energy is a state function. A change in the state of the system causes a change in its roerties. So, we exress the change in internal energy in

CarnotVDWB.nb 1. Carnot Knowledge. Hal Harris Department of Chemistry University of Missouri-St. Louis St. Louis, Missouri

CarnotVDWB.nb 1 Carnot Knowledge This is the second part of this worksheet and describes the Carnot cycle for methane Hal Harris Department of Chemistry University of Missouri-St. Louis St. Louis, Missouri

Accessibility of the lower-hybrid resonance

Accessibility of the lower-hybrid resonance [Sec. 4.1, Stix] Mathematica initialization Basic definitions Ion-to-electron mass ratio: Μ = All frequencies are assumed measured in units of Ωpe, so: Ωpi :=

Notes on the Unicycle Puzzle (PoW 1248)

Notes on the Unicycle Puzzle (PoW 248) Stan Wagon, wagon@macalester.edu, Sept. 207. The basic idea here is due to David Finn. Here are papers on the subject. D. Finn, Can a bicycle create a unicycle track,

Equilibrium point of any reaction is characterized by a single number: K eq is the equilibrium constant for the reaction

Lecture 19 Equilibrium Constant Equilibrium oint of any reaction is characterized by a single number: K eq is the equilibrium constant for the reaction In general: ja + kb R + qs K eq [ R] [ S] [ A] [

JPEG BMP. jpeg1.nb 1 JPEG. [Reference] /10/ /10/21 Takuichi Hirano (Tokyo Institute of Technology)

peg1.nb 1 JPEG JPEG [Reference] http://en.wikipedia.org/wiki/jpeg 2006/10/21 2006/10/21 Takuichi Hirano (Tokyo Institute of Technology) BMP In[1]:= Out[1]= SetDirectory@"d:êhira2êpublic_htmlêhobbyêeduêpeg"D

NY Times 11/25/03 Physics L 22 Frank Sciulli slide 1

NY Times /5/03 slide Thermodynamics and Gases Last Time specific heats phase transitions Heat and Work st law of thermodynamics heat transfer conduction convection radiation Today Kinetic Theory of Gases

Chemistry Tuesday, February 14 Wednesday, February 15, 2017

Chemistry Tuesday, February 14 Wednesday, February 15, 2017 Do-Now: BrainPOP: Moles 1. Write down today s FLT 2. What are the units of molar mass? 3. Use your periodic table to find the molar mass of NaOH.

Ideal Gas Law Stoichiometry

Assume you had the following, simple, chemical reaction: A B Volume of A (in Liters) Mass of A (in grams) Atoms, Molecules, or Particles of A Divide by Molar Mass Divide by 22.4L/mol Moles of A Divide

Chemistry 531 Spring 2009 Problem Set 6 Solutions

Chemistry 531 Sring 2009 Problem Set 6 Solutions 1. In a thermochemical study of N 2, the following heat caacity data were found: t 0 C,m d 27.2Jmol 1 K 1 f t b f C,m d 23.4Jmol 1 K 1 C,m d 11.4Jmol 1

ME 406 Assignment #9 Solutions

ME 06 Assignment #9 Solutions sysid Mathematica 6.0., DynPac.0, ê8ê009 intreset; plotreset; imsize = 50; Problem The equations are x = -x, y = x +y, z = x + z. Let F = x + y +z. To show that the surface

Mathematica Project 3

Mathematica Project 3 Name: Section: Date: On your class s Sakai site, your instructor has placed 5 Mathematica notebooks. Please use the following table to determine which file you should select based

Conservation of Energy Thermodynamic Energy Equation

Conseration of Energy Thermodynamic Energy Equation The reious two sections dealt with conseration of momentum (equations of motion) and the conseration of mass (continuity equation). This section addresses

Mathematica for Calculus II (Version 9.0)

Mathematica for Calculus II (Version 9.0) C. G. Melles Mathematics Department United States Naval Academy December 31, 013 Contents 1. Introduction. Volumes of revolution 3. Solving systems of equations

A short note on Reitlinger thermodynamic cycles

short note on Reitlinger thermodynamic cycles melia arolina Saravigna eartment of lied Science and echnology, Politecnico di orino, orino, Italy bstract: It is well known that arnot cycle is the thermodynamic

Thermodynamics and Atomic Physics II

Thermodynamics and Atomic Physics II 1. Heat from a source at 550 K is added to the working fluid of an engine operating at a steady rate. The temperature of the surroundings is 300 K. The efficiency of

Videos 1. Crash course Partial pressures: YuWy6fYEaX9mQQ8oGr 2. Crash couse Effusion/Diffusion:

Videos 1. Crash course Partial pressures: https://youtu.be/jbqtqcunyza?list=pl8dpuualjxtphzz YuWy6fYEaX9mQQ8oGr 2. Crash couse Effusion/Diffusion: https://youtu.be/tlrzafu_9kg?list=pl8dpuualjxtph zzyuwy6fyeax9mqq8ogr

The Equilibrium Constant, K P

The Equilibrium Constant, K Consider the gas-phase reaction: aa + bb yy + zz The thermodynamic equilibrium constant K is Yy z Z K = aa b B (standard state is 1 bar pressure) And by the same argument used

pv = nrt Where n is the number of moles of gas and R, the molar constant of gases, with a value of

Experiment 11 IDEAL GAS Objectives 1. To set up a thermal machine laboratory model, 2. To raise an object of a given mass using the thermal machine model, and 3. To describe and explain the operation of

CHAPTER 14: The Behavior of Gases

Name: CHAPTER 14: The Behavior of Gases Period: RELATIONSHIPS BETWEEN PRESSURE, VOLUME & TEMPERATURE OF A GAS Boyle s Law-Pressure and Volume Volume (ml) Pressure ( ) 60 50 40 30 20 10 Practice problem:

Step-by-step explanation of FEM with second order elements in Mathematica

Step-by-step explanation of FEM with second order elements in Mathematica José Luis Gómez Muñoz http://homepage.cem.itesm.mx/jose.luis.gomez Based on the work of John H. Mathews http://math.fullerton.edu/mathews/n2003/galerkinmod.html

Factorial Studies. Factor A I levels Factor B J levels o I*J Treatment groups o n ij values for each treatment combination

Factorial tudies Factor A I levels Factor B J levels o I*J Treatment grous o n ij values for each treatment combination B1 B.. BJ A1 n 11 n 1 n 1J A n 1 n n 1J AI n I1 n I n IJ Equal relication, n relicates,

Analyzing a Tennis Game with Markov Chains

Analyzing a Tennis Game with Markov Chains What is a Markov Chain? A Markov chain is a way to model a system in which: 1) The system itself consists of a number of states, and the system can only be in