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and Jackson Wolinsky (1996) introduced the concept of pairwise stability (known from the matching literature) as an equilibrium concept in models of network formation. This gave rise to a completely new strand of the literature focusing on the tension between stability and e ciency. Pairwise stability requires mutual consent of a pair of agents for link formation whereas links can be deleted unilaterally. Dutta and Muttuswami (1997) and Watts (2001) re ne the Jackson-Wolinksy framework further by introducing other stability concepts and derive implementation results for these concepts. Johnson and Gilles (2000) introduce a geographic dimension to the Jackson-Wolinsky model through spatial costs of link formation. For a recent survey of this literature see Jackson (2003). Several dynamic models using pairwise stability have been investigated as well, starting with Jackson and Watts (2002a). Jackson and Watts (2002b) and Goyal and Vega-Rodondo (1999) consider coordination games played on a network. The choice of partners in the game is endogenous and players are periodically allowed to add or sever links. Droste et al. (2000) also analyze coordination games played on a network with spatial costs of link formation. The non-cooperative version of network formation has rst been developed in two papers by Bala and Goyal (2000a, b). In all cases, agents choose to form links on the basis of costs and a (deterministic or stochastic) ow of bene ts that accrue from links. Bala and Goyal assume that a player can create a one-sided link with another player by making the appropriate investment. Their assumption di ers fundamentally from the concept of pairwise stability since mutual consent of both players is no longer required for link formation. They further investigate the reliability issue in networks by allowing links to fail independently of each other with a certain probability. Links are deterministic in Bala and Goyal (2000a). They are random, with identical probabilities of failure for all established links, in Bala and Goyal (2000b). Thus both their models deal with homogeneous agents. The corresponding static equilibrium outcomes are called Nash networks.2 Our model also belongs to the non-cooperative tradition and is a generalization of Bala and Goyal (2000b). We introduce agent heterogeneity by allowing for the probability of link failure (or success) to di er across 2 They also identify strict Nash networks and study the formation of Nash networks in a modi ed version of best-response dynamics. 3 links. This distinctive feature re ects the nature of the transmission technology or the quality of information. The generalization provides a richer model in terms of answering theoretical as well as practical questions: connectivity and super-connectivity, selection of central agents in star networks, e ciency, and Pareto-optimality. Besides imparting greater realism to the model, the introduction of heterogeneous agents allows us to check the robustness of the conclusions obtained in Bala and Goyal (2000b). Whereas their ndings still hold under certain conditions, heterogeneity gives rise to a greater variety of equilibrium outcomes, tends to alter results signi cantly and even generates some of the results of their deterministic model. Bala and Goyal show for both their models that Nash networks must be either connected or empty. With heterogeneous agents, this proves true only when the probabilities of success not are very di erent from each other. Another central nding of Bala and Goyal is that compared to information decay imperfect reliability has very di erent e ects on network formation. With information decay, minimally connected networks (notably the star) are Nash for a wide range of cost and decay parameters, independently of the size of society. In contrast, with imperfect reliability and small link formation costs, minimally connected networks tend to be replaced by superconnected networks (connected networks with redundant links) as the player set increases. However, with agent heterogeneity neither connectedness nor super-connectedness need arise asymptotically. Furthermore, in order for star networks to be Nash, probabilities must lie in a certain range (depending on costs) as in Bala and Goyal s setting. But we nd that as a rule, they have to satisfy additional conditions. In particular, it never pays in the Bala and Goyal framework to connect to the center of the star indirectly. In our context, however, such a connection might be bene cial and further conditions on probabilities are required to prevent these connections. Interestingly enough, heterogeneity helps resolve a particular ambiguity associated with the homogeneous model: Owing to the additional equilibrium conditions, the coordination problem inherent in selecting the central agent of a star is mitigated to a certain degree. We also investigate e ciency issues and nd that Nash networks may be nested and Pareto-ranked. We demonstrate by example that ine cient Nash networks can be Pareto-optimal. A further example shows that Nash networks do not always exist with non-uniform link success probabilities. Criticisms of the non-cooperative approach to network formation are addressed as well. We extend the model to allow for duplication of links 4 and to analyze Nash networks with incomplete information. Regarding the rst extension, it turns out that double links enable the formation of some networks that could not occur in the single links model. In the second extension, we nd that redundant links will be established when the agents beliefs about the probabilities of the indirect links are lower than the actual probabilities. Finally, the implications of mutual consent and endogenous success probabilities for Nash networks are discussed and explored. The network literature almost completely lacks models with heterogeneous agents, with the notable exception of Johnson and Gilles (2000) and Droste et al. (2000) who introduce spatial heterogeneity of agents and obtain results substantially di erent from both static and dynamic versions of homogeneous-agent pairwise stability models. Their model and ours di er in two respects: the kind of agent heterogeneity and the equilibrium concept. They follow Jackson and Wolinsky (1996) and use pairwise stability as the equilibrium concept. We analyze Nash networks. In a recent paper, Galeotti and Goyal (2002) also incorporate heterogeneity in the context of Nash networks. In their model di erent links may have di erent costs, and the bene ts of obtaining information from other players also varies across agents. They nd that equilibrium networks continue to have some of the key features identi ed by Bala and Goyal (2000a), i.e., centrality, centersponsorship and short network diameter occur in equilibrium despite the presence of heterogeneous players.3 These properties depend on the fa
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LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES Stable Networks and Convex Payoffs Robert P. Gilles Virginia Tech University Sudipta Sarangi Louisiana State University Working Paper 2005-13 http:/www.bus.lsu.edu/economics/papers/pap05_13.pdf Departme...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES Technology Diffusion through Trade with Heterogeneous Firms Bulent Unel Department of Economics Louisiana State University email: bunel@lsu.edu Working Paper 2006-15 http:/www.bus.lsu.edu/economics/pape...
LSU >> ECON >> 4445 (Summer, 2008)
Longevity and the Life Cycle Zsolt Becsi Federal Reserve Bank of Atlanta and Louisiana State University November 2001 Abstract The life-cycle model is extended to analyze the causes of longer lifespans. In contrast to previous work, the extension d...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES The Role of Beliefs and Confidence in Building Social Networks Robert P. Gilles Virginia Tech University Sudipta Sarangi Louisiana State University Working Paper 2005-15 http:/www.bus.lsu.edu/economics...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES Capitalization of Parent, School, and Peer Group Components of School Quality into House Price David Brasington Louisiana State University Donald R. Haurin Ohio State University Working Paper 2005-04 http...
LSU >> ECON >> 4445 (Summer, 2008)
Estimating the Effects of Monetary Policy Shocks: Does Lag Structure Matter? Keuk-Soo Kim Korea International Trade Association 159-1, Sam-Sung Dong, Kang-Nam Gu Seoul, Korea email: kimksoo@kotis.net W. Douglas McMillin Department of Economics Louis...
LSU >> ECON >> 4445 (Summer, 2008)
The Effects of Japanese Foreign Exchange Intervention GARCH Estimation and Change Point Detection1 ERIC HILLEBRAND Department of Economics, Louisiana State University, Baton Rouge, LA 70803, USA, Tel. +1 225 578 3795, FAX. +1 225 578 3807 erhil@lsu....
LSU >> ECON >> 4445 (Summer, 2008)
IN MEMORIAM WILLIAM J. MOORE William Jefferson Moore passed away on March 15, 2006 at his home in Baton Rouge at the age of 64. Moore was the Gulf Coast Coca-Cola Distinguished Professor of Economics. He had been a member of the LSU faculty for more ...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES International Transmission of Fiscal Shocks: An Empirical Investigation K. Peren Arin Massey University Faik Koray Louisiana State University Working Paper 2006-03 http:/www.bus.lsu.edu/economics/paper...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES Existence of Nash Networks in One-Way Flow Models Pascal Billand CREUSET, Jean Monnet University Christophe Bravard CREUSET, Jean Monnet University Sudipta Sarangi Louisiana State University Working Pap...
LSU >> ECON >> 4445 (Summer, 2008)
Economics Update www.bus.lsu.edu/economics Fall 2005 Division of Economic Development Completes over $3 Million in Funded Research The Division of Economic Development has completed over $3 million in funded research projects since its inception in...
LSU >> ECON >> 4445 (Summer, 2008)
Table of Contents Welcome Letter .2 E. J. Ourso College of Business - Administration and Staff.3 Where do you go? Whom do you call?.4 Degree Programs Offered .4 What makes up a degree from the E. J. Ourso College? .5 How do I get into the E. J. Ourso...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES Diseases and Development Shankha Chakraborty University of Oregon Chris Papageorgiou Louisiana State University Fidel Perez-Sebastian Universidad de Alicante Working Paper 2005-12 http:/www.bus.lsu.edu/...
LSU >> ECON >> 4445 (Summer, 2008)
International Technology Diusion and Growth in the Manufacturing Sector of Developing Economies Andreas Savvides Marios Zachariadis October 2002 Abstract This paper evaluates various channels through which foreign technology diuses to the manufactur...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES Preference-Theoretic Weak Complementarity: Getting More with Less David G. Brown Louisiana State University Working Paper 2008-09 http:/www.bus.lsu.edu/economics/papers/pap08_09.pdf Department of Econo...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES Do Adolescents with Emotional or Behavioral Problems Respond to Cigarette Prices? Erdal Tekin Georgia State University and NBER Naci Mocan Louisiana State University and NBER Lan Liang Agency for Healthc...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES Analyzing Skilled and Unskilled Labor Efficiencies in US Bulent Unel Department of Economics Louisiana State University Baton Rouge, LA 70803-6306 bunel@lsu.edu Working Paper 2007-11 http:/www.bus.lsu.e...
LSU >> ECON >> 4445 (Summer, 2008)
Nonlinearities in Capital-Skill Complementarity Chris Papageorgiou Department of Economics Louisiana State University Baton Rouge, LA 70803 Email: cpapa@lsu.edu Viera Chmelarova Department of Economics Louisiana State University Baton Rouge, LA 70803...
LSU >> ECON >> 4445 (Summer, 2008)
IN MEMORIAM LEE J. MELTON Professor Emeritus Lee J. Melton died on December 12, 2006, five days short of his 86th birthday. Professor Melton served in the Faculty of Economics at Louisiana State University for 32 years, rising through the ranks from...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS Economics 4445 Internship Description Form Registration date _ _ _ Semester Year Section _ /_ Name ID Number __ /_ Campus Address Campus Phone _ /_ Home Address Home Phone _ E-mail Address Brief description of the proposed...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES Early Starts, Reversals, and Catchup in the Process of Economic Development Areendam Chanda Louisiana State University Louis Putterman Brown University Working Paper 2005-06 http:/www.bus.lsu.edu/economi...
LSU >> ECON >> 4445 (Summer, 2008)
@T|@*5!* L4T*i4i?|@h|)q ,_i?Ui uhL4 @ @?i* Lu L ?|hit aL ? # g) #iT@h|4i?| Lu ,UL?L4Ut N?iht|) Lu |tM h} |tM h} c D2Sf ,4@*G _ g)9T|i_ ht @T@}iLh}L #iT@h|4i?| Lu ,UL?L4Ut wL t@?@ 5|@|i N?iht|) @|L? +L }ic w .fHf ,4@*G UT@T@9*t i_ 6_i* ihi35iM@t|@?...
LSU >> ECON >> 4445 (Summer, 2008)
ABSTRACT Macroeconomic Stabilization and Economic Growth: Analysis of Reform Policies in Tanzania1 by Andrew Feltenstein International Monetary Fund Washington, DC 20431 and Sudipta Sarangi Department of Economics Louisiana State University Baton Rou...
LSU >> ECON >> 4445 (Summer, 2008)
Imitation in a non-scale R&D growth model Chris Papageorgiou Department of Economics Louisiana State University email: cpapa@lsu.edu tel: (225) 578-3790 fax: (225) 578-3807 April 2002 Abstract. Motivated by recent empirical evidence this paper extend...
LSU >> ECON >> 4445 (Summer, 2008)
ECONOMICS What is Economics? Areas Research/ Forecasting Economic Advising Teaching All Levels Economics is the study of how people make choices. It examines these choices and provides a way of understanding how to make best use of natural resource...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES R&D Spillovers Through Trade in a Panel of OECD Industries Bulent Unel Department of Economics Louisiana State University email: bunel@lsu.edu Working Paper 2006-14 http:/www.bus.lsu.edu/economics/paper...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES Educational Outcomes and House Values: A Test of the Value-Added Approach David Brasington Louisiana State University Donald R. Haurin Ohio State University Working Paper 2005-03 http:/www.bus.lsu.edu/eco...
LSU >> ECON >> 4445 (Summer, 2008)
DEPARTMENT OF ECONOMICS WORKING PAPER SERIES Estimating the Inflation-Output Variability Frontier with Inflation Targeting: A VAR Approach James S. Fackler Department of Economics University of Kentucky Lexington, KY 40506-0034 James.Fackler@gmail....
LSU >> PHYS >> 1002 (Fall, 2008)
Chapter 22 22.1 Electromagnetic Induction This phenomenon is the process of bringing about or inducing an emf in a circuit which in turn induces a current. This occurs in a coil of wire connected within a circuit. It occurs when (1) a magnetic field...
LSU >> PHYS >> 1002 (Fall, 2008)
Chapter 9 I. Electrostatics Electrical charges that does not flow through an object, but sit stationary on the surface of an object. Usually it is isolated on the surface, but can transfer from object to object by contact. Protons and Electrons both...
LSU >> PHYS >> 1002 (Fall, 2008)
CHAPTER 20 ELECTRIC CIRCUITS A Circuit is a closed-loop conducting path for electrons to flow between a source and a resistance (device that uses electricity) which are connected by a conducting material (usually wire). When electrons are allowed to ...
LSU >> PHYS >> 1002 (Fall, 2008)
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LSU >> PHYS >> 1100 (Fall, 2008)
Phys 2101 Review problems In the figure below, block 1 of mass m1 slides from rest along a frictionless ramp from height h = 3.00 m and then collides with stationary block 2, which has mass m2 = 2m1. After the collision, block 2 slides into a region...
LSU >> PHYS >> 2101 (Fall, 2008)
Phys 2101 Review problems In the figure below, block 1 of mass m1 slides from rest along a frictionless ramp from height h = 3.00 m and then collides with stationary block 2, which has mass m2 = 2m1. After the collision, block 2 slides into a region...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Fall 2008 I. Using the Principle of Superposition A. 1-dimensional B. 2-dimensional II. g from Fg III. Gravitational Potential Energy PHYS 2101 Fall 2008 CT1: Two particles lie along the x-axis separated by a distance 2d, as shown be...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Fall 2008 I. Universal Law of Gravitation m1m 2 g A. F = G r 2 r B. Shell Theorem QuickTime and a TIFF (Uncompressed) decompressor are needed to see this picture. II. Superposition of Forces PHYS 2101 Fall 2008 CT1: A particle is p...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Fall 2008 I. II. Rotational Inertia & Rolling Static Equilibrium A. P= constant ( F = 0) B. L= constant ( = 0 ) C. P= 0 PHYS 2101 Fall 2008 CT1: The figure below shows the overhead views of a series of uniform rods on which for...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Fall 2008 I. Buoyancy Force PHYS 2101 Fall 2008 CT1: You insert a straw of length L into a tall glass of your favorite beverage. You place your finger over the top of the straw so that no air can get in or out and the lift the straw f...
LSU >> PHYS >> 2101 (Fall, 2008)
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LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Exam #1 Fall 2008 1. A small child of mass 31 kg swings back and forth on a rope swing whose length is 3.8 m. At the bottom of each swing (i.e., when the rope is vertical), her speed is 4.2 m/s. What is the magnitude of the tension in the...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 General Physics for Technical Students Fall 2008 The Big Idea for Unit 2 The rst goal of this unit is to understand the importance and utility of the concepts of energy and momentum and use the laws of the conservation of energy and con...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Fall 2008 I. Kinematics 1-dimensional 2-dimensional Graphical Finishing Forces A. Stooges B. Friction C. Centripetal III. Multiplying Vectors PHYS 2101 Fall 2008 EX1: Two cars approach each other on a straight stretch of highwa...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Fall 2008 Energy in SHM Examples of SHM A. Spring-Mass System B. Torsion Pendulum C. Simple Pendulum D. Physical Pendulum PHYS 2101 Fall 2008 EX1: A block of mass 980 g is fastened to a spring with a spring constant of 196 N/m. The...
LSU >> PHYS >> 2101 (Fall, 2008)
Chapter 15 Questions 1. (Question 15.3) Which of the following describe for the SHM of Fig. 15-20a: x (a) < < /2. (b) < < 3/2. (c) 3/2 < < . -t 6 2. (a) What is the phase constant for the harmonic oscillation with the acceleration function a(t...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Fall 2008 I. Potential Energy A. U g = mg(y - y 0 ) 1 B. U s = k(x - x 0 ) 2 QuickTime and a TIFF (Uncompressed) decompressor are needed to see this picture. Conservation of Energy A. Ug only B. Us only C. Both Ug and Us PHYS 2101 F...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Fall 2008 Angular Momentum and Torque II. Conservation of Angular Momentum QuickTime and a TIFF (Uncompressed) decompressor are needed to see this picture. PHYS 2101 Fall 2008 EX1: A penguin of mass m falls from rest from the edge...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Fall 2008 Summing Vectors Newtons Laws 1-Dimensional Kinematics PHYS 2101 Fall 2008 EX1: Calculate: A ( B) +B 20 25 |A| = 12 m |B| = 5 m 20 PHYS 2101 Fall 2008 EX4: EX3: EX2: What is the acceleration of a ball as it has be...
LSU >> PHYS >> 2101 (Fall, 2008)
Chapter 7 and 8 Questions 1. In the gure below, a greased trunk can slide to the ground along the three frictionless slides, starting from rest. Rank the slides according to (a) how much work the gravitational force does on the trunk during the decen...
LSU >> PHYS >> 2101 (Fall, 2008)
Chapter 11 Questions 1. A cannonball rolls down an incline without sliding. If the roll is now repeated with an incline that is less steep but of the same height as the rst incline, are (a) the balls time to reach the bottom and (b) its translational...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Fall 2008 1. Speed of a Wave l v= T v = fl w v= k Waves on a String t v= Transverse Velocity m y u= t PHYS 2101 Fall 2008 EX1: A wave traveling along a string is given by: y(x,t) = 0.024 sin(14.6x - 3.2t) with y and x in meters...
LSU >> PHYS >> 2101 (Fall, 2008)
PHYS 2101 Fall 2008 I. Fluids A. Density B. Pressure C. Using Static Equilibrium D. Buoyancy Force PHYS 2101 Fall 2008 EX1: A U-tube contains two liquids in static equilibrium: water of density w (998 kg/m3) in the right arm and oil of an unkno...
LSU >> PHYS >> 2102 (Fall, 2008)
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LSU >> PHYS >> 2102 (Fall, 2008)
Physics 2102 Section 003 Gaarde February 21, 2008 Quiz 10 Name (print): The figure shows four situations in which positive and negative charges move horizontally, and gives the rate at which each charge moves. (i) For each situation, indicate the di...
LSU >> PHYS >> 2102 (Fall, 2008)
Physics 2102 Section 003 Activity 1, January 29, 2008 The figure shows four solid spheres, each with charge Q uniformly distributed through its volume. Rank the spheres according to the magnitude of the electric field they produce at the point P: (i...
LSU >> PHYS >> 2102 (Fall, 2008)
Physics 2102 Section 003 Activity 1, April 15, 2008 The figure shows an ac generator connected to a black box through a pair of terminals. The box contains an RLC circuit whose elements and connections we do not know. Measurements reveal that and ...
LSU >> PHYS >> 2102 (Fall, 2008)
Physics 2102 Section 003 Gaarde February 7, 2008 Quiz 6 Name (print): The figure shows a family of parallel equipotential surfaces (in cross section) and five paths along which an electron is moved from one surface to another. (a) What is the direct...
LSU >> PHYS >> 2102 (Fall, 2008)
Physics 2102 Section 003 Gaarde February 26, 2008 Quiz 11 Name (print): The figure shows the current i in a single loop circuit with a battery B and a resistance R (and wires of negligible resistance). (i) Should the emf arrow at B be pointing leftw...
LSU >> PHYS >> 2102 (Fall, 2008)
Name: Solution Key ID No.: Instructor: Louisiana State University Physics 2102, Exam 2, October 14, 2004 Please, be sure to write your name, student ID number, and class instructor above. For the problems: Show your reasoning and your work. Th...
LSU >> PHYS >> 2102 (Fall, 2008)
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LSU >> PHYS >> 2102 (Fall, 2008)
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LSU >> PHYS >> 2102 (Fall, 2008)
Electric Flux Flux out: 3 + 10 + 5 = 18 Flux in: -3 - 4 - 6 = -13 Total flux: +18 - 13 = +5 > 0 Gauss law S1: S2: 1 > 0 2 < 0 3 = 0 4 = 0 S3: S4: ...
LSU >> PHYS >> 2102 (Fall, 2008)
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LSU >> PHYS >> 2102 (Fall, 2008)
Physics 2102 Section 003 March 6, 2008 Quiz 14 Gaarde Name (print): The figure shows the path of an proton that passes through two regions containing uniform magnetic fields of magnitudes B1 and B2. Its path in each region is a half-circle. (a) Wh...
LSU >> PHYS >> 2102 (Fall, 2008)
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LSU >> PHYS >> 2102 (Fall, 2008)
2/14/01 Your ID No. 2102 Test 1 Class No. Print your name: SOLUTIONS By signing below, I give my permission for my grades to be posted using my social security number as identification. Your signature: NOTE You must show your work including your s...
LSU >> PHYS >> 2102 (Fall, 2008)
PHYS-2102 Class Schedule * Gustav Revisions * August 17 - September 27, 2008 Sunday Monday Tuesday Wednesday Thursday Friday Saturday Aug 17 Aug 18 Aug 19 Aug 20 Aug 21 Aug 22 Aug 23 Freshman/Transfer Orientation Aug 24 Aug 25 Classes Begin...
LSU >> PHYS >> 2102 (Fall, 2008)
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LSU >> PHYS >> 2102 (Fall, 2008)
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LSU >> PHYS >> 2102 (Fall, 2008)
Physics 2102 Second Exam Formula Sheet Units: 1 min = 60 s 1 hr = 60 min 1 day = 24 hr 1 eV = 1.602x10-19 J 360o = 2 rad 1 N = 0.225 lb 1 m = 39.4 in = 3.28 ft Constants: Acceleration due to gravity (g) = 9.81 m/s2 = 32 ft/s2 G = 6.67x10-11 m3/kg s2...
LSU >> PHYS >> 2102 (Fall, 2008)
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