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Heat Temperature and the Zeroth and First Laws of Thermodynamics Thermodynamics A principle branch of physics and engineering is Thermodynamics: the study and application of thermal energy-often called internal energy of systems First we study in terms of bulk properties of matter then on the microscopic scale, ie we will define temperature in terms of kinetic energy in ch. 19 One of the principle concept is...
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Heat Temperature and the Zeroth and First Laws of Thermodynamics
Thermodynamics
A principle branch of physics and engineering is Thermodynamics: the study and application of thermal energy-often called internal energy of systems First we study in terms of bulk properties of matter then on the microscopic scale, ie we will define temperature in terms of kinetic energy in ch. 19 One of the principle concept is temperature Temperature and internal energy are related through the concept of the transfer of this energy in the form of heat and work done a system We will quantify these notions in studying systems with many particles These systems exist in various phases: ie liquid, solid and gas or vapor
Questions that are addressed in thermodynamics & the notion of temperature
Examples of how thermodynamics figures into everyday engineering and physics is countless
Heating of a car engine Heating of your dinner in a microwave oven or a conventional oven How a thermometer works!
Thermoscope
Based on the fact that many bodies change as we alter their temperature by heating or cooling ie vol...
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Penn State - PHYS - 212
Chapter 27 DC CircuitsDC Circuits Combining Resistors and Capacitors Time Dependent CircuitsWork done by a battery on charge Here=B > AW = [volts!] q dW = = [volts!] dqReal Battery and Single Loop circuits. What's the current ?Conservatio
Penn State - PHYS - 2
Prob 32.reviewRecall Motion 1-Dim @ Constant AccelerationEquations:We can also combine these equations so as to eliminate t:Review .Chapter 3 Kinematics in Two Dimension-VectorsUnits of Chapter 3 Vectors and Scalars Addition of Vectors
Penn State - PHYS - 250
Prob 32.reviewRecall Motion 1-Dim @ Constant AccelerationEquations:We can also combine these equations so as to eliminate t:Review .Chapter 3 Kinematics in Two Dimension-VectorsUnits of Chapter 3 Vectors and Scalars Addition of Vectors
Penn State - PHYS - 2
Chapter 17 Electric PotentialUnits of Chapter 17 Electric Potential Energy and Potential Difference Relation between Electric Potential and Electric Field Equipotential Lines The Electron Volt, a Unit of Energy Electric Potential Due to Point Char
Penn State - PHYS - 212
Chapter 22 Electric-FieldWhat is a FIELD? Region of space influenced by some physical phenomena; e.g., temperature, gravity, electric, magnetic behaviorsElectric Field Region of space where another charge would be influenced by a charge or distri
Penn State - PHYS - 213
WavesWave Function characteristicsSnapshots wavelength and Time dependenceT Traveling wavesThe Wave Equation from Newton 2nd Lawd 2 y ( x, t ) 1 d 2 y ( x , t ) = 2 2 d x v d 2tSuperposition Interference of traveling waves Creati
Penn State - PHYS - 211
Chapter 3 Vectors Physics deals with many quantities that have bothSize Direction VECTORS !y r(x,y) (r,)xE.g. Displacement, Velocity, Acceleration, Force, Torquex and y components of motion are independent-"LINEARITY"Componets v x =
Penn State - PHYS - 213
THE SECOND LAW OF THERMODYNAMICS EntropyEntropy and the direction of time Microscopically the eqs. of physics are time reversible ie you can turn the arrow of time around.! Macroscopically there is an arrow to time what's going on. ie processes a
Penn State - PHYS - 2
Chapter 5 Circular Motion; GravitationUnits of Chapter 5Kinematics of Uniform Circular Motion Dynamics of Uniform Circular Motion Highway Curves, Banked and Unbanked Nonuniform Circular Motion Centrifugation Newton's Law of Universal Gravitation
Penn State - PHYS - 250
Chapter 5 Circular Motion; GravitationUnits of Chapter 5Kinematics of Uniform Circular Motion Dynamics of Uniform Circular Motion Highway Curves, Banked and Unbanked Nonuniform Circular Motion Centrifugation Newton's Law of Universal Gravitation
Penn State - PHYS - 2
Chapter 21 Electromagnetic Induction and Faradays LawUnits of Chapter 21 Induced EMF Faradays Law of Induction; Lenzs Law EMF Induced in a Moving Conductor Changing Magnetic Flux Produces an Electric Field Electric Generators Transformers and
Penn State - PHYS - 250
Chapter 21 Electromagnetic Induction and Faradays LawUnits of Chapter 21 Induced EMF Faradays Law of Induction; Lenzs Law EMF Induced in a Moving Conductor Changing Magnetic Flux Produces an Electric Field Electric Generators Transformers and
Penn State - PHYS - 2
Chapter 16 Electric Charge and Electric FieldUnits of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors Induced Charge; the Electroscope Coulomb's Law Solving Problems In
Penn State - PHYS - 250
Chapter 16 Electric Charge and Electric FieldUnits of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors Induced Charge; the Electroscope Coulomb's Law Solving Problems In
Penn State - PHYS - 212
Experiment 6: MEASURING THE TIME CONSTANT OF AN RC CIRCUIT Object: The object of this experiment is to study the behavior of the time dependent potential difference across a capacitor in a simple RC series circuit. Prior to Lab: From the information
Penn State - PHYS - 212
Experiment 10 RC and RL circuits: Measuring the time constant.Object: The object of this lab is to measure the time constant of an RC circuit and a LR circuit. In addition, one can observe the characteristics of these two circuits and compare them.
Penn State - PHYS - 211
Physics 211"Physics" with Calculus Concurrent minimal requirement: Math 140 "First Semester Calculus" Text: Halliday Resnick Walker, Fundamentals of Physics, Extended, 7th EditionPhysics 211Introduction to Mechanics Course Overview Requiremen
Penn State - PHYS - 211
Pre-Lab Excel Problem Read and follow the instructions carefully! Below you are given a problem which you are to solve using Excel. If you have not used the Excel spreadsheet a limited tutorial is given in Appendix A. You are to hand in the enclosed
Penn State - PHYS - 211
Experiment #3: Computer Analysis of Projectile MotionObject: To use Videopoint to analyze the digital video of an object in flight, to study its horizontal and vertical motion, and to model the two-dimensional motion of the object. Prior to Lab: The
Penn State - PHYS - 2
Chapter 2 Describing Motion: Kinematics in One DimensionEquations of Constant AccelerationT equations we need to solve constantacceleration problemsv(t ) = v0 + at 1 2 x(t ) = x0 + v0 t + at 2 2 2 v (t ) = v0 + 2a( x - x0 ) v(t ) + v0 v= 2Kine
Penn State - PHYS - 250
Chapter 2 Describing Motion: Kinematics in One DimensionEquations of Constant AccelerationT equations we need to solve constantacceleration problemsv(t ) = v0 + at 1 2 x(t ) = x0 + v0 t + at 2 2 2 v (t ) = v0 + 2a( x - x0 ) v(t ) + v0 v= 2Kine
Penn State - PHYS - 2
Prob 32reviewRecall Motion 1-Dim @ Constant AccelerationEquations:We can also combine these equations so as to eliminate t:Review Chapter 3 Kinematics in Two Dimension-VectorsUnits of Chapter 3 Vectors and Scalars Addition of Vectors G
Penn State - PHYS - 250
Prob 32reviewRecall Motion 1-Dim @ Constant AccelerationEquations:We can also combine these equations so as to eliminate t:Review Chapter 3 Kinematics in Two Dimension-VectorsUnits of Chapter 3 Vectors and Scalars Addition of Vectors G
Penn State - PHYS - 2
Chapter 2 Describing Motion: Kinematics in One DimensionEquations of Constant AccelerationT equations we need to solve constantacceleration problemsv( t ) = v0 + at 1 2 x( t ) = x0 + v0 t + at 2 2 2 v ( t ) = v0 + 2a( x - x0 ) v( t ) + v0 v= 2
Penn State - PHYS - 250
Chapter 2 Describing Motion: Kinematics in One DimensionEquations of Constant AccelerationT equations we need to solve constantacceleration problemsv( t ) = v0 + at 1 2 x( t ) = x0 + v0 t + at 2 2 2 v ( t ) = v0 + 2a( x - x0 ) v( t ) + v0 v= 2
Penn State - PHYS - 2
Chapter 8 Rotational MotionUnits of Chapter 8Angular Quantities Constant Angular Acceleration Torque Rotational Dynamics; Torque and Rotational Inertia Solving Problems in Rotational DynamicsUnits of Chapter 8Rotational Kinetic Energy Angular M
Penn State - PHYS - 250
Chapter 8 Rotational MotionUnits of Chapter 8Angular Quantities Constant Angular Acceleration Torque Rotational Dynamics; Torque and Rotational Inertia Solving Problems in Rotational DynamicsUnits of Chapter 8Rotational Kinetic Energy Angular M
Penn State - PHYS - 2
Chapter 11 Vibrations and WavesUnits of Chapter 11Simple Harmonic Motion Energy in the Simple Harmonic Oscillator The Period and Sinusoidal Nature of SHM The Simple Pendulum Damped Harmonic Motion Forced Vibrations; Resonance Wave Motion Types of
Penn State - PHYS - 250
Chapter 11 Vibrations and WavesUnits of Chapter 11Simple Harmonic Motion Energy in the Simple Harmonic Oscillator The Period and Sinusoidal Nature of SHM The Simple Pendulum Damped Harmonic Motion Forced Vibrations; Resonance Wave Motion Types of
Penn State - PHYS - 212
Chapter 31 INDUCTIVE CIRCUITS LR circuit LC circuit exponential growth and decay Free oscillations Damped oscillations LRC circuit Forced Oscillations Resonance conditionPut them together!Electro-magnetic Energy LRC circuits Explored the
Penn State - PHYS - 2
Chapter 9 Static Equilibrium; Elasticity and FractureEx. 9-7Units of Chapter 9The Conditions for Equilibrium Solving Statics Problems Applications to Muscles and Joints Stability and Balance Elasticity; Stress and Strain Fracture Spanning a Spac
Penn State - PHYS - 250
Chapter 9 Static Equilibrium; Elasticity and FractureEx. 9-7Units of Chapter 9The Conditions for Equilibrium Solving Statics Problems Applications to Muscles and Joints Stability and Balance Elasticity; Stress and Strain Fracture Spanning a Spac
Penn State - PHYS - 212
FARADAY'S LAW Michael Faraday and Joseph Henry discovered it in 1831 Changing magnetic flux produces an emf Or Changing B-Field produces E-Field The rate of change of magnetic flux is requiredInduced EMF produced by a changing Magnetic Flux!d
Penn State - PHYS - 213
The Dual PersonalityParticle or Wave?Evidence for Wave Behavior Solution to Maxwell's Equations Interference Diffraction Polarization explained Adequately explains geometric opticsClassical Wave Theory Cannot Explain Photoelectric Effect
Penn State - CM - 2002
Cold Molecules 2002:Ultracold Molecules and Bose-Einstein Condensation Les Houches, March 3-8, 2002Progress in trapping cold rubidium moleculesA. Fioretti, M. Mazzoni* and C. Gabbanini Istituto dei Processi Chimico-Fisici del CNR Via G. Moruzzi 1,
Penn State - CM - 2002
Ultracold collisions in spinspinpolarised Li + Li2Marko T. Cvitas, Pavel Soldn, and Jeremy M. HutsonDepartment of Chemistry, University of Durham, EnglandPascal Honvault and Jean-Michel LaunayUMR 6627 du CNRS, University of Rennes, FranceIntro
Penn State - CM - 2002
Interactions of Lithium Atoms in a Resonator-Enhanced Dipole TrapS. Jochim, M. Bartenstein, G. Hendl, J. Hecker Denschlag, A. Mosk1, M. Weidemller2 and R. Grimm Institut fr Experimentalphysik, Universitt Innsbruck, Austria 1FOM Instituut Rijnhuizen,
Penn State - CM - 2002
H6nGP S 6 B BE U z| BE U z uEIs 6 6 P zs U 6 QI to$6k&Q$6F tPCEu E {EG}GQaQe{ECu{u@yFGv6 eo$PCz@x X F nAa0 Ew86 x zI z z X xIEI I X R acSd~idE}CEH@F X zGEx H@F s X }Gs H@F s X X x {@ 10 10-12X sX @ sI X @ X E
Penn State - CM - 2002
A new magnetic trap for ultra-cold atoms and molecules - status reportO. Pradl, D. Weise, R. Hauschild, J. Mlynek, A. PetersUniversity of Konstanz, Fachbereich Physik, Fach M696, D-78457 Konstanz, GermanyTrapping of neutral species in magnetic tr
Penn State - CM - 2002
Sympathetic Cooling with Two Atomic Species in an Optical TrapS. Kraft, M. Mudrich, J. Lange, M. Eichhorn, K. Singer, A. Mosk, R. Grimm*, and M. WeidemllerMax-Planck-Institut fr Kernphysik, 69029 Heidelberg, Germanyhttp:/www.mpi-hd.mpg.de/ato/lase
Penn State - CM - 2002
Development of a mixed optical and magnetic trap for Bose-Einstein condensation of cesium atomsS. Boussen, N. Hoang, S. Guibal, D. Marescaux, L. Pruvost, J. Pinard, P. Pillet Laboratoire Aim Cotton, CNRS, Campus universitaire d'Orsay, Bt 505, 91405
Penn State - CM - 2002
Photoassociation of heteronuclear lithiumUlrike Schlder, Christian Silber, Thomas Deuschle, and Claus Zimmermann Physikalisches Institut der Universitt Tbingen, Auf der Morgenstelle 14, 72076 Tbingen, GermanyHomonuclear photoassociationE S +PSy
Penn State - CM - 2002
Institute of Quantum Optics University of Hannover Welfengarten 1 30167 Hannover Germany www.iqo.uni-hannover.deExperiments with a Molecular Matterwave Interferometer for Studying Cold Collisions between Atoms and MoleculesM. Frank, S. Jung, C. Li
Penn State - CM - 2002
Lu-Fano plot for the interpretation of photoassociation spectra*Department of Physics and JILA, University of Colorado, Boulder, Colorado 80309-0440, USA Laboratoire Aim Cotton, Universit Paris XI and CNRS II, Orsay 91405, France Photoassociation sp
Penn State - CM - 2002
Method for theoretical treatment of dissociative recombination of three-atomic moleculesV. Kokoouline, C.H. Greene, and B.D.IntroductionMotivation Dissociative recombination of three-atomic molecules:* EsryDepartment of Physics and JILA, Unive
Penn State - CM - 2002
Preparation, Storage and Investigation of sympathetically cooled MoleculesA. Ostendorf, U. Frhlich, C. Lmmerzahl, B. Roth, S. Schiller Institut fr Experimentalphysik , Heinrich-Heine-Universitt Dsseldorf, GermanyAbstractWe use the method of sympa
Penn State - CM - 2002
A new magnetic trap for ultra-cold atoms and molecules - status reportUniversitt KonstanzO. Pradl, D. Weise, R. Hauschild, J. Mlynek, and A. PetersFachbereich Physik and Optik-Zentrum Konstanz, Universitt Konstanz, Fach M696, 78457 Konstanz, GERM
Penn State - CM - 2002
ADIABATIC CHANNEL APPROXIMATION IN THE DYNAMIC AND STOCHASTIC DESCRIPTION OF THE ATOM-DIATOM COMPLEX FORMATION AT LOW ENERGIES.Elena I. Dashevskayaa), Evgueni E. Nikitina), Ilya D. Litvina,b), Itzhak Orefa) and Jrgen Troeb)a) b) Department of Chemi
Penn State - CM - 2002
Penn State - CM - 2002
Fine structure transitions in atom-atom and atom-molecule collisions at ultracold temperaturesR. Krems and A. DalgarnoITAMP, Harvard-Smithsonian Center for Astrophysics 60 Garden Street, Cambridge, MassachusettsUltracold collisions of He atoms wit
Penn State - CM - 2002
Development of a mixed optical and magnetic trap for cesium atoms N. Hoang, S. Boussen, S. Guibal, D. Marescaux, L. Pruvost, J. Pinard, P. Pillet Laboratoire Aim Cotton, CNRS, Bt. 505, Campus dOrsay,91405 Orsay, FranceWe describe a novel trap desig
Penn State - CM - 2002
Numerical treatment of diatomic molecules Alejandro Saenz Fachbereich Chemie, Universit t Konstanz, Fach M 721, 78 457 Konstanz, Germany. a The interest in theoretical and experimental investigations of diatomic molecules is recently increasing due t
Penn State - CM - 2002
Multichannel asymptotic model for the study of cold-atom interactionsBenot TJampens, Anne Crubellier Laboratoire Aim Cotton, e B t. 505, Campus dOrsay a F-91405 Orsay C dex eIntroductionPrecise knowledge of cold-atom collision properties is es
Penn State - CM - 2002
*=Universiteit-Utrecht1 2Quantum phases in an optical latticeDebye Institute, Utrecht University Postbus 80.000, 3508 TA Utrecht, The Netherlands Institute for Theoretical Physics, Utrecht University Postbus 80.006, 3508 TA Utrecht, The Netherlan
Penn State - PHYS - 213
Physics 214 Laboratory Interference of Light Theory: Light that is incident upon two or more slits will interfere and produce an interference pattern on a distant screen. If coherent light with wavelength is incident upon two slits the light will in
Penn State - PHYS - 212
Experiment 12: Elements of AC Circuits - The Series RLC circuitPurpose: To study the phase relationship and resonance conditions for a resistor, capacitor and inductor in a series ac circuit. Prior to Lab: Sketch a phasor diagram for an ideal LRC ci
Penn State - PHYS - 213
Physic 214 Polarization of LightEquipment 60 cm optical bench Pasco light source (OS-8517A) Light Sensor with exit slits mounted to optics holder 2 Polarizers with Holders One additional mounted polarizer with attached Rotary Motion Sensor Pasco spe
Penn State - PHYS - 2
Chapter 20 MagnetismUnits of Chapter 20 Magnets and Magnetic Fields Electric Currents Produce Magnetic Fields Force on an Electric Current in a Magnetic Field; Definition of B Force on Electric Charge Moving in a Magnetic Field Magnetic Field
Penn State - PHYS - 250
Chapter 20 MagnetismUnits of Chapter 20 Magnets and Magnetic Fields Electric Currents Produce Magnetic Fields Force on an Electric Current in a Magnetic Field; Definition of B Force on Electric Charge Moving in a Magnetic Field Magnetic Field
Penn State - PHSC - 410
Introduction PHSC 410Relationship between Work done by a force and ENERGYTo obtain a measure of the forces experienced by a penguin (here a particle ie rigid and looking only at center of mass.) moving between x1 and x2 we introduce the notion
Penn State - PHYS - 213
Chapter 36 Diffraction Part 1Single Slit Diffraction Diffraction and the Double Slit apparatus Intensity Formula for single and double slitDefinition and Types of Diffraction Diffraction is the bending of a wave around an object accompanied by an