Maharishi - ENGLISH - 0058

POE AND ROMANTICISMBy Karna Upadhyay My favorite Edgar Allen Poe story was The Tell Tale Heart because of the effortless ways he includes the five Romantic techniques and the suspense woven so skillfully throughout the entire story. The Tell Tale Heart w

Clarkson - MA - 232

CHAPTER1First-Order Differential Equations1.1Dynamical Systems: ModelingConstants of Proportionality 1. 3. 5.dA = kA dt(k < 0)2. 4.dA = kA dt(k < 0)dP = kP(20,000 P ) dtdA kA = dt tdG kN = dt AA Walking Model6.Because d = t where d = dista

Clarkson - MA - 232

CHAPTER6Linear Systems of Differential Equations6.1Theory of Linear DE SystemsBreaking Out Systems 1. x1 = x1 + 2 x2 x2 = 4 x1 x2 x1 = 4 x1 + 3 x2 + e t x2 = x1 x22. x1 = x1 x2 = x2 + 1 x1 = x2 x2 = x3 x3 = 2 x1 + x2 + 3x3 + sin t3.4.Checking

Clarkson - PH - 132

Clarkson - PH - 132

Clarkson - PH - 132

Clarkson - PH - 132

Clarkson - PH - 132

Clarkson - PH - 132

Clarkson - PH - 132

Clarkson - PH - 132

Clarkson - PH - 132

Clarkson - PH - 132

Clarkson - PH - 132

Clarkson - PH - 132

Clarkson - PH - 132

fctYP ll'l m+sI\b' ~d.'a1-11-12:'0lI_~II+I~-(J)40PH 132 Labs ., PH 132: Pre-lab 3 arrangement of the ""2. Fig 3.4B shows an" incomplete" breadboard schematic circuit of Fig 3.4A. Drawin Fig 3.4Blines (representing connecting wires)to complet

NYU - MORSE - V55.038503

Katherine Ling Conversations of the West: 19th C and Antiquity David Levene October 5, 2009 Essay #1 Creon vs. Agamemnon Creon and Agamemnon are both characters with very caricatural personalities. They possess exaggerated pride and obstinancy, which make

UIllinois - STAT - 410

STAT 410Examples for 06/27/2008Summer 2008In general, if X 1 , X 2 , , X n is a random sample of size n from a continuous distribution with cumulative distribution function F ( x ) and probability density function f ( x ), thenF max X ( x ) = P ( max

UIllinois - STAT - 410

STAT 410Examples for 10/06/2008Fall 2008In general, if X 1 , X 2 , , X n is a random sample of size n from a continuous distribution with cumulative distribution function F ( x ) and probability density function f ( x ), thenF max X ( x ) = P ( max X

UIllinois - STAT - 410

STAT 410Examples for 10/15/2008Fall 2008Normal (Gaussian) Distribution:1.Let X be normally distributed with mean and standard deviation . Find the moment-generating function of X, M X ( t ). MX( t ) = E( etX ) = =et x e1 2z 2 22 e ( x )22dxe

UIllinois - STAT - 410

STAT 410Examples for 10/15/2008Fall 2008Gamma Distribution:f (x ) =( )x 1 e x ,0x<ORf (x) =1 ( )x 1 e x,0x<If T has a Gamma ( , =1/ ) distribution, where is an integer, thenF T ( t ) = P ( T t ) = P ( X t ), where X t has a Poisson ( t )

Purdue - CHM - 111

Chemistry 11500 - MDr. Marcy Towns Mtowns@purdue.edu1 Models Nuclear energy Drugs as molecules Nanotech BiofuelsLectures CHM 11500 - M01 MF 11:30 - 12:20 CHM 11500 - M02 MF 2:30 - 3:202 Models Nuclear energy Drugs as molecules Nanotech BiofuelsCH

Purdue - CHM - 111

CH M 11500-M CHLectur e 2Dr. Marcy Towns Lectures: M, F Section M-01 at 11:30 AM Section M-02 at 2:30 PMFor next lectureReview sections: section 1.6, pp. 25-32 section 1.8, pp. 38-42 section 2.3-2.5, pp. 69-76 section 3.3, pp. 103-107 section 3.5, pp

Purdue - CHM - 111

CHM 11500-M01 and M02 STUDENT HANDOUTDr. Towns Lectures: M, F 11:30, 2:30 Lecture 31CPS Questions #1, 2 and 32Buddy Question #43Potential and Kinetic Energy Energy is stored in molecules. As stored energy it is potential energy. Some molecules st

Purdue - CHM - 111

CHM 11500-M01 and M02 STUDENT HANDOUTDr. TownsLectures: M, F 11:30, 2:30Lecture 4Nuclear ChemistryQuestion #1Nuclear equationsa. 9843Tc 98Ru + 0-1e 44b. 229m90Th 22990Th + c. 21284Po 208Pb + 42He 82Generating Electricity CombustionGenerating

Purdue - CHM - 111

CHM 11500-M01 and M02Dr. Towns Lecture 5, 9-12-08Reading was: 23.3 - 23.51Runaway Nuclear ReactionsWhy didnt these reactors explode like an atomic bomb? Nuclear fuel: 3% U-235 Weapon grade uranium: 97% U-235 Different design and geometries2Yucca Mo

Purdue - CHM - 111

CHM 11500Lecture 7 9-19-081Reading Expected for Today Chapter 7, pp 294-312, 318-3232Question #13Think/Pair/Share Question #24Key terms: wavelength, (nm) frequency, (s-1 = Hz) c= 5Amplitude (intensity) of a waveKey terms: wavelength amplitud

Purdue - CHM - 111

Chem 11500 Lecture 8Reading was Chapter 8.4-8.71This week: Lab: From Element to Salt Prepare alum, KAl(SO4)2 q 12H2O and find the % yield. Techniques: Filtration, crystallization Homework due on Friday.2Exam 1: Tuesday 9/30, 6:30 PM Elliot Hall of M

Purdue - CHM - 111

PHYS 172: Modern MechanicsFall 2009Lecture 2 - Momentum & RelativityRead: 1.5-1.11Agenda for today: Clicker questions Review of syllabus points Interactions Vectors: position, displacement, velocity. Momentum A word about RelativityClicker question 1

Purdue - CHM - 111

PHYS 172: Modern MechanicsFall 2009Lecture 4 Conservation of MomentumRead 2.72.14C L IC K E R Q U E S T IO N # 1Reading Question (Sections 2.7 2.14) (This is a closed-book quiz, no consulting with neighbors, etc.) Which of the following are always co

Purdue - CHM - 111

PHYS 172: Modern MechanicsFall 2009Lecture 6 Fundamental Forces, ReciprocityRead 3.9 3.14Exam 1 - Tuesday September 15, 8:00-10:00 PM Elliott Hall of Music1. T h e e x a m w ill b e w r itte n a s a s ta n d a r d 1 h o u r e x a m , b u t y o u w il

Purdue - CHM - 111

PHYS 172: Modern MechanicsFall 2009Lecture 9 Buoyancy, The Energy PrincipleRead 5.1 5.7C L IC K E R Q U E S T IO N # 1Reading Question (Sections 5.1 5.7) (This is a closed-book quiz, no consulting with neighbors, etc.) The Moon is in circular orbit a

Purdue - CHM - 111

PHYS 172: Modern MechanicsFall 2009Lecture 10 The Energy Principle: Multiparticle SystemsRead 5.8 5.15R e a d in g Q u e s tio n : A little c a lc u lu s r e v ie w . C o n s id e r a p u r e ly o n e - d im e n s io n a l p r o b le m , w h e r e a p

Purdue - CHM - 111

PHYS 172: Modern MechanicsFall 2009Lecture 12 Energy AccountingRead 6.5 6.9C L IC K E R Q U E S T IO N # 1Reading Question (Sections 6.5 6.9) (This is a closed-book quiz, no consulting with neighbors, etc.) Consider a system containing only an object

Purdue - CHM - 111

PHYS 172: Modern MechanicsFall 2009Lecture 13 Friction, Driven Oscillations, and ResonanceRead 6.10 6.14C L IC K E R Q U E S T IO N # 1Reading Question (Sections 6.10 6.14) (This is a closed-book quiz, no consulting with neighbors, etc.)Y o u th r o

Purdue - CHM - 111

PHYS 172: Modern MechanicsFall 2009Lecture 15 - Multiple Particle SystemsRead 8.1 - 8.5Review of What Weve Covered Thus FarCh 1 Changes imply interactions Vectors are used to describe many changes Momentum is fundamental: p=mv. Ch 2 The momentum prin

Purdue - CHM - 111

PHYSICS 272 Electric & Magnetic InteractionsProf. Andrew Hirsch Hirsch@purdue.edu Room: 178, Phone: 42218Course ContentThis course deals with electric and magnetic interactions, which are central to the structure of matter, to chemical and biological p

Purdue - CHM - 111

Example ProblemA particle with charge +2 nC (1 nanoCoulomb=10-9 C) is located at the origin. What is the electric field due to this particle at a location <-0.2,-0.2,-0.2> m?Solution:1. Distance and direction: r E1 =1 q1 r 2 4 0 r r = observed _ lo

Purdue - CHM - 111

Polarization of Atoms+ Force due to E created by E positive charge shifts electron cloud and nucleus in opposite directions: electric dipole.An atom is said to be polarized when its electron cloud has been shifted by it is not a permanent dipole the inf

Purdue - CHM - 111

Chapter 15Electric Field of Distributed ChargesDistributed Charges( x ', y ', z ') E ( x, y, z ) =1 Qi r 2 ri 4 0 i =1 iN( x ', y ', z ')( x, y, z ) E ( x, y, z ) =1 4 0 ( x ', y ', z ')rdx ' dy ' dz ' 2 rUniformly Charged Thin RodLength: L C

Purdue - CHM - 111

Electric Field of a Spherical Shell of Charge Field inside: E = 0 1Q r Field outside: E = 2 4 0 r(like point charge)Qualitative approach IntegrationE of a Sphere Outside Direction: radial - due to the symmetryDivide into 6 areas: E6 E5E1+E4E2 E3E

Purdue - CHM - 111

Potential EnergyIntroduced the concept of electric field E to deal with forces Introduced electric potential V to deal with work and energy Electric potential: electric potential energy per unit charge Potential energy is associated with pairs of interac

Purdue - CHM - 111

Potential at a Certain Location1. Add up the contribution of all point charges at this point q2 r2 r1 A1 qi VA = i 4 0 riq12. Travel along a path from point very far away to the location of interest and add up E dl at each step:dl E VA = E dlA q2

Purdue - CHM - 111

Biot-Savart Law for a Single Charge Electric field of a point charge: E = 1q r 2 4 0 rMoving charge makes a curly magnetic field: B units: T (tesla) = kg s-2A-1 0 qv r B= 4 r 2 0 T m2 = 107 4 C m/sJean-Baptiste Biot (1774-1862) Felix Savart (1791-1841

Purdue - CHM - 111

The Atomic Structure of MagnetsThe magnetic field of a current loop and the magnetic field of a bar magnet look the same.Batom0 2 = , 3 4 z = R2 IWhat is the direction? One loop: What is the average current I?e current=charge/second: I = t ev 2 R I=

Purdue - CHM - 111

Chapter 19Capacitors, Resistors and BatteriesCapacitor: Charging and DischargingExperiment 1 Experiment 2Capacitor: Construction and SymbolsThe capacitor in your set is similar to a large two-disk capacitor s There is no connecting path through a cap

McGill - CHEM - CHEM120

CARBON DIOXIDE FROM AN ANTACID TABLET EXPERIMENT #1% Calcium carbonate reacts with acid and produces carbon dioxide 1. CaCO3 + 2HCl Ca2+ + 2Cl + H2O + CO2 OR 2. CO32= + 2H+ H2O + CO2Apparatus and Chemicals: 3- 125mL Erlenmeyer flasks 3- small vials 1- s

McMaster - CAS - 701

6-1Semantics of Predicate Logic (contd) I: Evaluation of TermsWe will dene a value function ValA : Tm( ) State(A) A We also write [t]A =df so that ValA (t, ) A[t]A : State(A) A.The def. of [t]A is by structural induction on t: [x]A = (x) [c]A = cA [f

McMaster - CAS - 701

5-1Semantics of Predicate Logic1 -structures Given a signature = cfw_ c : s, . . . , f : sn s, . . . , p : sm , . . . a -structure or -interpretation A consists of a non-empty set (e.g., dom(N ) = dom(A) = A), for each c : s in , an element cA A, for

McMaster - CAS - 701

4-1Substitution and -equivalenceI. Substitution in Terms r x/t : replace all free occurrences of x in r by t. Denition, by structural induction on r: (a) (b) (c) Q: Is x x/t y x/t c x/t t y c f (r1 x/t , . . . , rn x/t ) r x2 /t2 x1 /t1 ? (y x)f (r1 ,

McMaster - CAS - 701

3-1Math Digression 2: Binary relationsDenition 1. A (binary) relation R on a set A is a subset of A2 .We write, for all x, y A: (x, y ) R R(x, y ) xRy Examples of relations on A. IA = the identity or diagonal relation on A = UA = = the universal relati

McMaster - CAS - 701

2-1Predicate Logic1 Examples of AxiomatizationsExample 1: Group Theory. Axioms: (i) Associative: xy z (x y ) z = x (y z ) (ii) Right Identity: e(x(x e = x) (iii) Right Inverse: xy (x y = e) Q: Is e a constant or a variable ? Now we can prove theorems of

McMaster - CAS - 701

McMaster - CAS - 701

McMaster - SGS - 1

SGS101 Part 3 Responsibilities & Research Record-Keeping Methods MethodsDoug Welch Sep 23, 2008Principles PrinciplesOwnership Responsibility Organization Standard of recording Preservation of intermediate results Routine backup of research information

McMaster - SGS - 1

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McMaster - SGS - 1

SGS101 Part 2 Research Ethics ResearchDr Karen Szala-Meneok Sep 23, 2008Research Ethics Board ResearchWhy does my research dealing with humans need to Why dealing be approved by a Research Ethics Board (REB)? beThe Research Ethics Boards looks at it f

McMaster - SGS - 1

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McMaster - SGS - 1

To receive credit for SGS101, you must: youRegister for the course Register Show your student card and sign-in at the tables outside the lecture hall if you havent already done so, DO THIS NOW! havent Attend the full three hours Attend Write the quiz Wri

McMaster - SGS - 1

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McMaster - SGS - 1

SGS 101 September 2008 SeptemberAndrea Thyret-Kidd Academic Integrity Officer McMaster UniversityThis presentation was created by: This Academic Integrity Office Academic Andrea Thyret-Kidd Andrea Centre for Leadership in Learning Erika Kudstra Centre f