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...15. Ch Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - work on system Liu UCD Phy1B 07 2 II. Heat Engine Efficiency (x100%) e=W/QH =(QH-QL)/QH =1- QL/QH e<1 Liu UCD Phy1B 07 3 Engine Steam Liu UCD Phy1B 07 4 Combustion Engine Liu UCD Phy1B 07 5 Carnot Engine Ideal engine, reversible process...
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15. Ch Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - work on system Liu UCD Phy1B 07 2 II. Heat Engine Efficiency (x100%) e=W/QH =(QH-QL)/QH =1- QL/QH e<1 Liu UCD Phy1B 07 3 Engine Steam Liu UCD Phy1B 07 4 Combustion Engine Liu UCD Phy1B 07 5 Carnot Engine Ideal engine, reversible process QH ~ TH QL ~ TL eideal =1- QL/QH=1- TL/TH (in Kelvin) Real engine e< eideal <100% Second law of thermodynamics: No device can transfer a given amount of heat completely into work Liu UCD Phy1B 07 6 III. Refrigerator, ac, heat pump Liu UCD Phy1B 07 7
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UC Davis >> PHY >> 14 (Fall, 2008)
Ch 15. Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - wo...
UC Davis >> PHY >> 15 (Fall, 2008)
Ch 15. Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - wo...
UC Davis >> PHY >> 16 (Fall, 2008)
Ch 15. Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - wo...
UC Davis >> PHY >> 17 (Fall, 2008)
Ch 15. Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - wo...
UC Davis >> PHY >> 18 (Fall, 2008)
Ch 15. Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - wo...
UC Davis >> PHY >> 2 (Fall, 2008)
Ch 15. Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - wo...
UC Davis >> PHY >> 20 (Fall, 2008)
Ch 15. Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - wo...
UC Davis >> PHY >> 23 (Fall, 2008)
Ch 15. Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - wo...
UC Davis >> PHY >> 3 (Fall, 2008)
Ch 15. Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - wo...
UC Davis >> PHY >> 49 (Fall, 2008)
Ch 15. Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - wo...
UC Davis >> PHY >> 6 (Fall, 2008)
Ch 15. Thermodynamics Liu UCD Phy1B 07 1 I. The First Law of Thermodynamics Closed system: U=Q-W U U Q W Internal energy: all the energy of the molecules change in internal energy + for heat added; - for heat lost + work done by the system; - wo...
UC Davis >> PHY >> 115a (Fall, 2008)
Physics 115A Spring 2006 Problem Set 4 Due by 4:00 pm Wednesday, 5/17 (in class, at my oce, or in my mailbox) 1. Finite barrier (25 points) Consider the nite potential barrier V (x) = V0 for a < x < a 0 for |x| > a with V0 > 0. Suppose a particle ...
UC Davis >> PHY >> 115a (Fall, 2008)
The harmonic oscillator April 24, 2006 In what follows, we will be making use of the following key results: a = 1 (m x i) p 2 m h a n = nn1 (1) (2) (3) (4) (5) [ , a+ ] = 1 a a+ n = n + 1 n , m n dx = mn 1 H = h a+ a + 2 We can use (1) ...
UC Davis >> PHY >> 115a (Fall, 2008)
Some Useful Facts for Physics 115A Probabilities: Prob(a < x < b at time t) = t ( ) = x J, b a (x, t)(x, t)dx h 2im Probability current: Expectation values: Uncertainties: x = p2 2m with J(x) = x x O(x, p) = x2 x (x, t)O(x,...
UC Davis >> PHY >> 115a (Fall, 2008)
Physics 115A Spring 2005 Problem Set 6 Due by 4:00 pm Wednesday, 5/31 (in class, at my oce, or in my mailbox) 1. Simultaneous eigenvectors: an example (10 points) Consider the two matrices M1 = ab 0c , M2 = de fg with a = c a. Find the eigenvector...
UC Davis >> PHY >> 115a (Fall, 2008)
Physics 115A Spring 2006 Professor: Steve Carlip Room 437 (Physics-Geology) Oce hours TW 11-12 (or email for an appointment: carlip@physics.ucdavis.edu) TA: TBA Oce hours TBA TA/grader: TBA Oce hours TBA (for questions about grading) Required text:...
UC Davis >> PHY >> 115a (Fall, 2008)
Physics 115a Quantum Mechanics Spring 2007 Tues-Thurs 1:40-3pm 130 P/G Prof. Andreas Albrecht General Information This course is the first quarter of upper division quantum mechanics. The course will cover the first three chapters of Griffiths in de...
UC Davis >> PHY >> 115a (Fall, 2008)
Info Sheet for the Final Exam PHY 115a Wed June 13 2007 1:30pm 130 P/G Andreas Albrecht Basics: Date of midterm: Wed June 13 2007 Time: 1:30pm-3:30pm Place: 130 P/G Bring: Your own *blank* bluebooks (any size) and your own pen(s). Calculators: Are li...
UC Davis >> PHY >> 115a (Fall, 2008)
Physics 115a Homework 1 (due April 5 at start of class) Assigned March 29 1.1) Consider a particle wavefunction which at a fixed time ( t = 0 ) has the form Aeikx 1 < x < 1 ( x, 0 ) = x 1 0 where A is real. a) Find the value of A for which is n...
UC Davis >> PHY >> 115a (Fall, 2008)
Physics 115a Homework 2 (due April 12 at start of class) Assigned April 5 2.1) Problem 1.10 from Griffiths 2.2) Show that 1 ( t ) 2 ( t ) = 1 ( 0 ) 2 ( 0 ) . You may assume time evolution is given by Eqn 3.24 or 3.26 of the notes (use notes ...
UC Davis >> PHY >> 116c (Fall, 2008)
Physics 116A Notes Fall 2004 David E. Pellett Draft v.0.9 beta Notes Copyright 2004 David E. Pellett unless stated otherwise. References: Text for course: Fundamentals of Electrical Engineering, second edition, by Leonard S. Bobrow, published by O...
UC Davis >> PHY >> 116c (Fall, 2008)
TABLE OF CONTENTS Release Notes . 1. INTRODUCTION .. 1. TYPES OF ANALYSIS . 1. DC Analysis .. 2. AC Small-Signal Analysis . 3. Transient Analysis .. 4. Pole-Zero Analysis . 5. Small-Signal Distortion Analysis . 6. Sensitivity Analysis . 7. Noise Ana...
UC Davis >> PHY >> 116c (Fall, 2008)
...
UC Davis >> PHY >> 116c (Fall, 2008)
Physics 116A Notes Fall 2004 David E. Pellett Draft v.0.9 Notes Copyright 2004 David E. Pellett unless stated otherwise. References: Text for course: Fundamentals of Electrical Engineering, second edition, by Leonard S. Bobrow, published by Oxford...
UC Davis >> PHY >> 116c (Fall, 2008)
Lab 1: Introduction to Lab Equipment U.C. Davis Physics 116A INTRODUCTION The purpose of this first lab is to become familiar with the standard equipment of an electronics lab. You will use the multimeter, function generator, and oscilloscope. 3. U...
UC Davis >> PHY >> 116c (Fall, 2008)
Physics 116A Notes Fall 2004 David E. Pellett Draft v.0.9 Notes Copyright 2004 David E. Pellett unless stated otherwise. References: Text for course: Fundamentals of Electrical Engineering, second edition, by Leonard S. Bobrow, published by Oxford...
UC Davis >> PHY >> 116c (Fall, 2008)
Amplier Frequency Response, Feedback, Oscillations; Op-Amp Block Diagram and Gain-Bandwidth Product Physics116A,12/4/06 Draft Rev. 1, 12/12/06 D. Pellett 2 Negative Feedback and Voltage Amplier AB is called the loop gain. (see solutions to Prob. 1...
UC Davis >> PHY >> 116c (Fall, 2008)
Lab 3: Passive Components U.C. Davis Physics 116A 10/8/2003 INTRODUCTION In this lab you will build a Thvenin equivalent circuit and a low-pass filter and will characterize each. 1. THVENIN EQUIVALENT CIRCUIT In this section, you will build a circui...
UC Davis >> PHY >> 116c (Fall, 2008)
Lab 5: Diodes U.C. Davis Physics 116A INTRODUCTION The purpose of this lab is to measure the properties of a diode and a zener diode. You will make I-V curves for each and will see how a diode can be used as a voltage rectifier. 1. DIODE I-V CU R V...
UC Davis >> PHY >> 116c (Fall, 2008)
Lab 6: Transistors (Part 1, BJT\'s) U.C. Davis Physics 116A INTRODUCTION The purpose of this lab is to measure some characteristics of a transistor (a bipolar junction transistor, or BJT) in two useful circuit configurations, the emitter follower amp...
UC Davis >> PHY >> 116c (Fall, 2008)
Experiment 4 Op-Amp Resonant Bandpass Filter Physics 116A, D. Pellett v. 1.2, Oct. 19, 2003 1 Introduction In this experiment you will become familiar with a bandpass lter made with an op-amp (active lter). You will compare experimental results on...
UC Davis >> PHY >> 116c (Fall, 2008)
Lab 2: Op Amp Circuits U.C. Davis Physics 116A INTRODUCTION This lab introduces the operational amplifier or \"op amp\". The circuit is already constructed for you on a single IC (integrated circuit) and in this lab we will use the IC in several of it...
UC Davis >> PHY >> 116c (Fall, 2008)
Physics 116A Fall 2008 Introduction to Analog Electronics Preliminary Outline 9/26/08 Class meets MWF at 12:10 PM in 140 Physics/Geology Week 0 1 2 Monday Topics/Notes First class is Friday, September 26 (Sept 22) Overview: Scope of course (Fri. 9/26...
UC Davis >> PHY >> 116c (Fall, 2008)
SPICE3 Version 3f3 Users Manual May, 1993 T. Quarles A.R.Newton, D.O.Pederson, A.Sangiovanni-Vincentelli Department of Electrical Engineering and Computer Sciences University of California Berkeley, Ca., 94720 Copyright 1990, 1991, 1992, 1993 Regent...
UC Davis >> PHY >> 116c (Fall, 2008)
Physics 116A Notes Fall 2004 David E. Pellett Draft v.0.9 Notes Copyright 2003 David E. Pellett unless stated otherwise. References: Text for course: Fundamentals of Electrical Engineering, second edition, by Leonard S. Bobrow, published by Oxford...
UC Davis >> PHY >> 116c (Fall, 2008)
Physics 116A Notes Fall 2004 David E. Pellett Draft v.0.9 Notes Copyright 2004 David E. Pellett unless stated otherwise. References: Text for course: Fundamentals of Electrical Engineering, second edition, by Leonard S. Bobrow, published by Oxford...
UC Davis >> PHY >> 116c (Fall, 2008)
Physics 116A Fall 2006: Final Exam 12/13/2006 Closed book and notes except for four 8.5 in x 11 in sheets of paper. Show reasoning for full credit. There are 6 problems and 200 points. Complex quantities are shown as boldface. Note: transistor high f...
UC Davis >> PHY >> 116c (Fall, 2008)
1. INTRODUCTION SPICE is a general-purpose circuit simulation program for nonlinear dc, nonlinear transient, and linear ac analyses. Circuits may contain resistors, capacitors, inductors, mutual inductors, independent voltage and current sources, fou...
UC Davis >> PHY >> 116c (Fall, 2008)
Lab 8: INTRODUCTION Differential Amplifier 2. DC ANALYSIS Construct the circuit of figure 1, for which you have already calculated the voltages at the lettered nodes. Leaving v1 and v2 unconnected, measure the voltages at the lettered nodes and comp...
UC Davis >> PHY >> 116c (Fall, 2008)
Physics 116A: Diode Problem 11/11/08 The gure above is a diagram of a silicon junction diode connected to a source of bias voltage V at T = 300 K. 1. Would phosphorus be a suitable dopant for the p-type material? Explain briey. 2. Let V = 0. Make a ...
UC Davis >> PHY >> 116c (Fall, 2008)
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UC Davis >> PHY >> 116c (Fall, 2008)
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UC Davis >> PHY >> 116c (Fall, 2008)
Lab 10: Feedback and Oscillation U.C. Davis Physics 116A INTRODUCTION This lab consists of two parts. Both show some property of feedback. The Wien bridge oscillator illustrates how a feedback amplifier can become an oscillator. The class B output s...
UC Davis >> PHY >> 116c (Fall, 2008)
ON Semiconductort JFET VHF Amplifier NChannel Depletion MPF102 MAXIMUM RATINGS Rating DrainSource Voltage DrainGate Voltage GateSource Voltage Gate Current Total Device Dissipation @ TA = 25C Derate above 25C Junction Temperature Range Storage Te...
UC Davis >> PHY >> 200b (Fall, 2008)
Physics 200C Dr. Cebra Final Exam 11-June-07 Name: _ Instructions: Work all parts of each problem (each problem worth 50 points). No notes, calculators, etc. Please write your name on every page they WILL be separated. Staple additional sheet to ...
UC Davis >> PHY >> 200b (Fall, 2008)
Physics 200C Dr. Cebra Mid Term Exam 05-May-08 Name: _ Instructions: Work all parts of each problems (each problem worth 50 points). No notes, calculators, etc. Please write your name on every page they could be separated. Staple additional sheet...
UC Davis >> PHY >> 200b (Fall, 2008)
Physics 200C Dr. Cebra Final Exam 16-Jun-04 Name: _ Instructions: Work all parts of each problem (each problem worth 50 points). No notes, calculators, etc. Please write your name on every page. Staple additional sheets to the page to which they r...
UC Davis >> PHY >> 200b (Fall, 2008)
Physics 200C Dr. Cebra Final Exam 11-Jun-05 Name: _ Instructions: Work all parts of each problem (each problem worth 50 points). No notes, calculators, etc. Please write your name on every page. Staple additional sheets to the page to which they r...
UC Davis >> PHY >> 219a (Fall, 2008)
Problem I (10 points) Consider a system of N distinguishable particles. Each particle can occupy only one of the two levels 1 or 2, where 1< 2. Assume N is very large. You can distribute the particles in such way that n particles reside on level 2 wh...
UC Davis >> PHY >> 219a (Fall, 2008)
Pure Appl. Chem., Vol. 73, No. 8, pp. 13491380, 2001. 2001 IUPAC INTERNATIONAL UNION OF PURE AND APPLIED CHEMISTRY PHYSICAL CHEMISTRY DIVISION COMMISSION ON THERMODYNAMICS* USE OF LEGENDRE TRANSFORMS IN CHEMICAL THERMODYNAMICS (IUPAC Technical Repo...
UC Davis >> PHY >> 219a (Fall, 2008)
Winter 2007 PHY 250 Signals & Noise 3 UNITS CRN 57655 T Th 10:30-11:50 Room PHY 525 Instructor: Prof. Tony Tyson, Department of Physics, tyson@physics.ucdavis.edu Research in physics and other fields often deals with signals which are buried in rando...
UC Davis >> PHY >> 219a (Fall, 2008)
q o d m io no n io o g y po d r io grn o d dr c o d m i y tr sxUfpX1\'|Xn svv f|i y p y \'fhe|Xd q tX}Uf y } y Xpi h\'fGpXo m i o n q o y o r q q r v pX#|~fgxfXd#|i y y siU~i x e si`r zvv rt y svv y rf tX tf Q YY R gr...
UC Davis >> PHY >> 219a (Fall, 2008)
INTERNAL FELLOWSHIP APPLICATION FOR PROSPECTIVE STUDENTS 00008 SECTION ONE Graduate program: Student name: Phone number: Address: City: Country of citizenship: For tuition purposes, are you a legal resident of California? Cumulative undergraduate GPA...
UC Davis >> PHY >> 230a (Spring, 2008)
A Brief Introduction to Relativistic Quantum Mechanics Hsin-Chia Cheng, U.C. Davis 1 Introduction In Physics 215AB, you learned non-relativistic quantum mechanics, e.g., Schrdinger o equation, E= p2 + V, 2m , p i , Ei t 2 2 i = + V . t 2m (1)...
UC Davis >> PHY >> 230a (Spring, 2008)
5 Lorentz Covariance of the Dirac Equation = c = 1 from now on. We will set In E&M, we write down Maxwells equations in a given inertial frame, x, t, with the electric and magnetic elds E, B. Maxwells equations are covariant with respecct to Loren...
UC Davis >> PHY >> 230a (Spring, 2008)
Class Notes for Quantum Field Theory: Section I Introduction to 2nd Quantization, Lagrangian and Equations of Motion, Conservation Laws, the Klein Gordon eld, the Dirac eld, Spin-Statistics connection, Feynman Propagators, Electromagnetic elds Notes...
UC Davis >> PHY >> 230a (Spring, 2008)
Class Notes for Quantum Field Theory: Section II S-Matrix, Wicks Theorem, Feynman Rules, Specic Sample Calculations Primary Reference: Mandl & Shaw, Quantum Field Theory See also: Peskin and Schroeder, Quantum Field Theory Jack Gunion U.C. Davis 230...
UC Davis >> PHY >> 252b (Fall, 2008)
The Tevatron and the Higgs John Conway Rutgers University LHC Advanced Study - Prague July 2003 CDF New double sided silicon central drift chamber plug calorimeter DAQ system trigger front end Detector fully commissioned Detector fully commis...
UC Davis >> PHY >> 252b (Fall, 2008)
Calorimetry: Energy Measurements Measuring particles energies through Electromagnetic and Hadronic interactions Prof. Robin D. Erbacher University of California, Davis References: R. Fernow, Introduction to Experimental Particle Physics, Ch. 11 D. G...
UC Davis >> PHY >> 252b (Fall, 2008)
Top Mass Measurement at the Tevatron Koji Sato (Univ. of Tsukuba) for CDF and D0 Collaborations HEP2005 Europhysics Conference Lisboa, Portugal, June 22, 2005 Top Quark Mass - Introduction Top mass is a fundamental parameter of the Standard Model....
UC Davis >> PHY >> 252b (Fall, 2008)
Preparing for Final Project: Working with ROOT on the lifshitz cluster Using LHC Olympics files Were going to set ourselves up to look at the LHC Olympics calibration files and an example analysis macro in ROOT. Bob McElrath has set up some code to g...
UC Davis >> PHY >> 252b (Fall, 2008)
Searchesforexotica withtheDetector MgeKaragznel OxfordUniversity fortheCDFCollaboration SUSY05Conference,IPPP,Durham July1823,2005 TheMillenniumWindow,DurhamCathedral 7/21/05 MotivationandStrategy: ManyquestionsunexplainedbySM:needBSM! Whatcanbe(no...
UC Davis >> PHY >> 252b (Fall, 2008)
Physics 252b, Homework #1 (Please feel free to collaborate with each other. It is your own responsibility to learn it.) 1) Fernow problem 1.1 2) Fernow problem 1.2 3) Fernow problem 1.8 (Just give it your best shot, nothing fancy.) 4) What is rapidi...
UC Davis >> PHY >> 252b (Fall, 2008)
Detecting Particles: How to see without seeing Interactions of Particles with Matter: Electromagnetic and Nuclear Interactions Prof. Robin D. Erbacher University of California, Davis References: R. Fernow, Introduction to Experimental Particle Physi...
UC Davis >> PHY >> 252b (Fall, 2008)
Searches for New Physics at Colliders Giorgio Chiarelli INFN Sezione di Pisa, Via F.Buonarroti 2, I-56127 Pisa Abstract. In this paper I present the most recent results of the ongoing searches, mainly from Tevatron Collider experiments, for new physi...
UC Davis >> PHY >> 252b (Fall, 2008)
Homework #2 - Statistics and Data Analysis - Probability Distributions 1. A certain isotope has an lifetime of 1 year. If you have 1 mole of this isotope, what is the activity of the sample, in counts per second? 2. If you have beam collisions at a...
UC Davis >> PHY >> 252b (Fall, 2008)
Development of Photon Detectors at UC Davis Daniel Ferenc Eckart Lorenz Alvin Laille Physics Department, University of California Davis Work supported partly by DOE, National Nuclear Security Administration (NNSA), Office of Nonproliferation Researc...
UC Davis >> PHY >> 252b (Fall, 2008)
Neutrino Cross Sections and Scattering Physics Bonnie Fleming Yale University, New Haven, CT. Abstract. Large ux uncertainties and small cross sections have made neutrino scattering physics a challenge. However, a worthwhile challenge, as these tiny ...
UC Davis >> ECS >> 120 (Fall, 2008)
ECS 120: Theory of Computation UC Davis Phillip Rogaway Handout MS1 February 21, 2002 Midterm Solutions Section 1 1 Short Answer [45 points] (1) Let M1 be an n1 -state DFA and let M2 be an n2 -state DFA. Using the procedures given in class and i...
UC Davis >> ECS >> 120 (Fall, 2008)
ECS 120: Theory of Computation UC Davis Phillip Rogaway Handout 9 March 7, 2002 Problem Set 10 Due Thursday, March 14, 2002 Problem 1. Let INFINITE = { M : M is a TM and L(M ) is innite}. Let REGULAR = { M : M is a TM and L(M ) is context free}. ...
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