SydU STAT3014 (2015) Second semester Dr. J. Chan 18
|
|
- Avice Gardner
- 5 years ago
- Views:
Transcription
1 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Stratified Random Samping.1 Introduction Description The popuation of size N is divided into mutuay excusive and exhaustive subpopuations caed strata of N 1, N,, N L units where N s are known. A simpe random sampe of size n is drawn from the -th stratum, = 1,, L. Tota sampe size : n = n. Reasons for Stratification: N 1 N N 3 n 1 n n 3 SRS 1 SRS SRS 3 ȳ 1 ȳ ȳ 3 1. Aow sub-estimates which can then be combined to give an overa estimate, e.g. district and state income eves.. Provide administrative convenience as strata may exist in natura, e.g. counties and branches. 3. Aow different samping fractions and methods in different stratum, e.g. sma/arge business, private/government housing, urban/rura househods. 4. Enabe efficient estimates if a heterogeneous popuation is divided into strata that are internay homogeneous. ȳ ȳ 1 ȳ ȳ 3 Gp 1 Gp Gp 3 s 1 s s 3 s i < s SydU STAT ) Second semester Dr. J. Chan 18
2 Notation Popuation N STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Sampe n Y i i = 1,, N y i, i = 1,, n i-th unit from stratum h Ȳ = 1 N Y i ȳ = 1 n y i N n i=1 S s i=1 Aso W = N N is the stratum weight and f = n is the samping fraction N for stratum.. Estimators of mean and variance For the popuation mean Ȳ = 1 N N Ȳ : Ȳ = ȳ st = 1 N N ȳ = W ȳ. For the popuation tota Y = NȲ : Ŷ = N ȳ st = N ȳ = N W ȳ. Ceary Eȳ st ) = Ȳ since Eȳ ) = Ȳ and the ȳ s are independent. Hence var Ȳ ) = W 1 n ) s = N n W s n 1 N W s SydU STAT ) Second semester Dr. J. Chan 19
3 varŷ ) = N STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe W 1 n ) s = N N n W s n N W s Estimators and variance estimates for a stratified SRS Parameter Estimator Variance Ordinary estimator s y = 1 n n 1 yi n ȳ ), W = N N i=1 Ratio R Rst = 1 X W ȳ var R st ) = 1 X W 1 n ) s y N n Mean Ȳ Ȳ st = L W ȳ var Ȳ st ) = 1 n ) s y Tota Y W Ŷ st = N L W ȳ varŷst) = N W N n 1 n ) s y N n SydU STAT ) Second semester Dr. J. Chan 0
4 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Exampe Cochran, 1963) A sampe of U.S. coeges was drawn to estimate the enroments in 1947 from 196 Teachers Coeges. These coeges were separated into 6 strata. Suppose the foowing sampe information is obtained. Compete the tabe and estimate tota enroment, its s.e. and coefficient of variation. N n ȳ N ȳ s N 1 n N ) s n = )31 9 = = )31 7 = = )15 11 = = )105 7 = = )9 14 = = ) = Tota Soution: We have N = 196 and Ŷ st = N ȳ = = varŷst) = i=1 i=1 N 1 n N ) s = ) n sdŷst) = = cvŷst) = sd Ȳ st ) Ȳ st = ) = = Read Tutoria 10 Q4c and Tutoria 11 Q1a,b. SydU STAT ) Second semester Dr. J. Chan 1
5 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe.3 Optima Aocation We consider 1. Choice of n = nw s to obtain maximum precision, for a given tota sampe size n or, more generay, a given tota cost. Here w is the desire aocation.. For a specified precision choice of the minimum n and corresponding n s. 1. Optimization Let K denote a cost function where C = C 0 + C n, C 0 0, C > 0, = 1,, L. Let V = Varȳ st ) = W S n 1 N W S. Note that if we take C 0 = 0, C = 1, 1 then C reduces to the tota sampe size n.. Theorem For a fixed vaue of C, V is minimized by the choices of n where n N S C, = 1,, L. The proportionaity constant is chosen in accordance with the fixed vaue of C. We shoud take a arger sampe from a statrum if SydU STAT ) Second semester Dr. J. Chan
6 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe 1) the stratum size N is arger; and/or ) the variabiity in terms of s.d. S is greater; and/or 3) the square root of the cost of samping a unit C is ower. 3. Best precision for specified tota sampe size Optima aocation: For fixed tota sampe size n, precision is greatest if N S / C n = N S / W S / ) C n = C W S / n, = 1,, L. C Neyman aocation: C 1 = C = = C L First determined by Aexander Chuprov 193), rediscovered by Neyman 1934). n = N ) S W S n = n, = 1,, L. N S W S Proportiona aocation: If S 1 = S = = S L, then n = N N n = W n, = 1,, L. SydU STAT ) Second semester Dr. J. Chan 3
7 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe 4. Minima Tota Sampe Size for Specified Precision If we require that is Pr{ ȳ st Ȳ δ µ} 1 α, { } ȳ st Pr Ȳ V arȳst ) δ µ 1 α V arȳst ) or δ µ V arȳst ) z α/ so Varȳ st ) δ µ zα/. For optima aocation, n = n L Varȳ st ) = 1 n n/ ) L W C S V + 1 N W S n 1 N W S / C W S /. C =1 W S ast eqt in P.19) W S = ) W S / C ) nw S / 1 W S C N ) = 1 W S W S C) 1 W S δ µ n C N z α/ W S C) W S C) W S C ) W S or n = n ) W S C ) W S C =1 W S C W S C 1 N 1 N W S C W S + δ µ z α/ 1 W S + δ µ z α/ W S C =1 V + 1 N. W S SydU STAT ) Second semester Dr. J. Chan 4 =1
8 where V = δ µ L STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe z α/ ) L W S C V is the bound for variance. Ignoring fpc, ) W C S or n W S C For Neyman aocation, n = n W S / L 1 N ) W S W S + V or n = n Ignoring fpc, the formua is L ) W S V or n W S W S =1 =1 W S C =1 1 N L ) W S W S =1 V V W S. W S W S =1, = 1,, L., = 1,, L. W S + V =1, = 1,, L. For proportiona aocation, n = n W. Equating S fais because S in V arȳ st ) are not a equa. Instead we shoud consider Varȳ st ) = W S n 1 N W S = W S nw 1 N W S V W S W W S V + 1 N W S or n = n W V + 1 N =1, = 1,.., L. W S =1 SydU STAT ) Second semester Dr. J. Chan 5
9 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Sampe size determination for a SRS and stratified SRS SRS for mean Ŷ s.t. Pr y Y δ µ) = 0.95 and S = p1 p) for prop. P Sam. n NS Nδ µ/z α/ + S f=0 z α/ S δ µ = S V Stratified SRS for mean Ŷ s.t. Pr y st Y δ µ ) = 0.95 and V = δ µ zα/ Sizes Optimum Neyman Proportiona Strat. n Sam. n n = n L W S C i=1 W i S i Ci ) L W S C i=1 V + 1 N W S ) W Ci i S i n = n W S W i S i i=1 L ) W S V + 1 N W S n = nw W S V + 1 N W S 5. Confidence Intervas for specified tota sampe size Provided each n is moderatey arge ȳ st µ Varȳst ) N 0, 1), at east approximatey. Optima aocation for a given tota sampe size wi give the shortest 1 α) 100% CI with ength: z 1 α ) Var ȳst = z 1 α ) Varopt ȳ st SydU STAT ) Second semester Dr. J. Chan 6
10 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Exampe Cochran, 1963) The standard deviation for coege enroments, s, in a given stratum is estimated by the 1943 vaue. Stratum N S The tota enroment in 1943 was 56,47. For the 1947 study the aim is to obtain a coefficient of variation CV) which is a ratio of standard error to estimate to be approximatey 5%. Determine the sampe size n required and the Neyman aocation n of these vaues to strata as given previousy. Soution: We have N = 196, Ŷ = 56, 47 and seŷ ) = cv Ŷ = ) = 84 varŷ ) = 84 = 7, 974, 976 = N V We assume that C are a equa. Then Strat. N S N S N S ω = N S N S n = ω n roundn ) Tota SydU STAT ) Second semester Dr. J. Chan 7
11 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Take n = 58. = ) W S V + 1 N W S = ) N S V N + N S 6841) = Read Tutoria 10 Q4a,b and Tutoria 11 Q1e. SydU STAT ) Second semester Dr. J. Chan 8
12 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe.4 Doube samping for stratification In stratified SRS, the auxiiary variabe X for stratification can be known ony after samping, e.g. income eve or education eve. In other words, W = N N, = I,..., L are unknown before samping. Doube samping is a two-phase samping. For exampe, we may ca many voters in an opinion po to identify income eve phase 1 sampe), when ony a few coud be interviewed phase sampe) for purposes of competing a detaied questionnaire. Phase 1: Take a arge sampe of size n for obtaining preiminary information such as income eve of a voter) to identify strata with Ŵ = n n, = 1,..., L denote the proportion of the first sampe faing into stratum. Then Ŵ is an unbiased estimator of W = N N. Phase : A much smaer sampe of n eements are randomy samped from the n eements identified in stratum for coecting information on Y. Then the subsampe mean and variance, ȳ and s, are cacuated for each stratum. N X, Y, Sy SRS s s n n n 1 n L x, Ŵ Post-stratification n SRS n 1 n L x, ȳ, s SydU STAT ) Second semester Dr. J. Chan 9
13 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe An estimator of the popuation mean if the phase samping fractions n N are a sma and N is arge is Y st,ds = varŷ st,ds) = Ŵ ȳ n n 1 [ Ŵ Ŵ n ) ] s + Ŵȳ Ŷ st,ds) n n If n is so arge that Ŵ n varŷ st,ds) = is negigibe, this variance estimate reduces to ] [Ŵ s + Ŵȳ Ŷ st,ds) n n Ignoring fpc terms, the first part takes the usua form with w repacing N N. The second part is the additiona variance since we estimate the weights W from a sampe. It is not necessariy to make the second term sma because it means making the ȳ about equa which is not desirabe because stratification is more efficient than SRS when the ȳ are quite different. Thus, choosing strata that produce different ȳ sti may be better than a SRS, even though doube samping might have to be empoyed to estimate the W. SydU STAT ) Second semester Dr. J. Chan 30
14 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Exampe: Coege enroment) From a ist of enroments and facuty sizes for American 4-year coeges and universities, it is desired to estimate the average enroment for the academic year). Private institutions tend to be smaer than pubic ones, so stratification is in order. Whie the data indicate the type of coege or university, the ist is not broken up according to type. A 1-in-10 systematic sampe was done to obtain information on type of coege and the resuts are: Private Pubic Tota n 1 = 84 n = 57 n = 141 Subsampes of 11 private and 1 pubic coeges gave the foowing data on enroments and facuty size. Estimate the average enroment for American coeges and universities in Private Pubic n 1 = 11 n = 1 Enroment Facuty Enroment Facuty ȳ 1 = 1, s 1 = 1, 77.7 ȳ = 5, 85.7 s 1 = 5, SydU STAT ) Second semester Dr. J. Chan 31
15 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Soution: From the data given above, Y [ 84 st,ds = ȳ st,ds = Ŵ ȳ = 141 = 3, varŷ st,ds) = 1 n 1 Ŵ1s 1 ) + 1 n Ŵs ) + 1, ] 5, n [Ŵ1ȳ 1 ȳ st,ds ) + Ŵȳ ȳ st,ds ) ] = 1 ) ) [ , , 367.4) + 57 ] 5, , 367.4) 141 = 553, , = 583, seŷ st,ds) = 583, = The second part of the variance is due to estimating the true stratum weights. The standard deviation of Ŷ st,ds is sti quite arge due to the sma sampe sizes and arge variation among coege enroments, but it is much smaer than the error associated with a singe SRS of 3 coeges from the ist. Y srs = varŷ srs) = n n ȳ = 1 n N [ 11 3 seŷ srs) = 965, = ] 5, , = 3, ) s n = 1 3 ), 576, 503 = 965, where s is cacuated using the combined 1 SRS) sampe and N = SydU STAT ) Second semester Dr. J. Chan 3
16 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Doube samping estimator based on -stage samping Parameter Estimator Variance [ ] Mean Y Y w st,ds = w ȳ varŷ st,ds) = s + w ȳ Ŷ st,ds) n n w = n n If n & N are arge and n N are a sma SydU STAT ) Second semester Dr. J. Chan 33
Jan van den Brakel Department of Statistical Methods, Statistics Netherlands
Survey Research Methods (2010) Vo.4, No.2, pp. 103-119 ISSN 1864-3361 http://www.surveymethods.org c European Survey Research Association Samping and estimation techniques for the impementation of new
More informationGeneral Certificate of Education Advanced Level Examination June 2010
Genera Certificate of Education Advanced Leve Examination June 2010 Human Bioogy HBI6T/P10/task Unit 6T A2 Investigative Skis Assignment Task Sheet The effect of temperature on the rate of photosynthesis
More informationSydU STAT3014 (2015) Second semester Dr. J. Chan 1
Refereces STAT3014/3914 Appied Statistics-Sampig Preimiary 1. Cochra, W.G. 1963) Sampig Techiques, Wiey, ew York.. Kish, L. 1995) Survey Sampig, Wiey Iter. Sciece. 3. Lohr, S.L. 1999) Sampig: Desig ad
More informationDo Schools Matter for High Math Achievement? Evidence from the American Mathematics Competitions Glenn Ellison and Ashley Swanson Online Appendix
VOL. NO. DO SCHOOLS MATTER FOR HIGH MATH ACHIEVEMENT? 43 Do Schoos Matter for High Math Achievement? Evidence from the American Mathematics Competitions Genn Eison and Ashey Swanson Onine Appendix Appendix
More informationCS229 Lecture notes. Andrew Ng
CS229 Lecture notes Andrew Ng Part IX The EM agorithm In the previous set of notes, we taked about the EM agorithm as appied to fitting a mixture of Gaussians. In this set of notes, we give a broader view
More informationGeneral Certificate of Education Advanced Level Examination June 2010
Genera Certificate of Education Advanced Leve Examination June 2010 Human Bioogy HBI6T/Q10/task Unit 6T A2 Investigative Skis Assignment Task Sheet The effect of using one or two eyes on the perception
More informationSEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l
Probem 7. Simpe Penduum SEMINAR. PENDULUMS A simpe penduum means a mass m suspended by a string weightess rigid rod of ength so that it can swing in a pane. The y-axis is directed down, x-axis is directed
More informationProblem set 6 The Perron Frobenius theorem.
Probem set 6 The Perron Frobenius theorem. Math 22a4 Oct 2 204, Due Oct.28 In a future probem set I want to discuss some criteria which aow us to concude that that the ground state of a sef-adjoint operator
More information8 APPENDIX. E[m M] = (n S )(1 exp( exp(s min + c M))) (19) E[m M] n exp(s min + c M) (20) 8.1 EMPIRICAL EVALUATION OF SAMPLING
8 APPENDIX 8.1 EMPIRICAL EVALUATION OF SAMPLING We wish to evauate the empirica accuracy of our samping technique on concrete exampes. We do this in two ways. First, we can sort the eements by probabiity
More informationSome Measures for Asymmetry of Distributions
Some Measures for Asymmetry of Distributions Georgi N. Boshnakov First version: 31 January 2006 Research Report No. 5, 2006, Probabiity and Statistics Group Schoo of Mathematics, The University of Manchester
More informationNEW DEVELOPMENT OF OPTIMAL COMPUTING BUDGET ALLOCATION FOR DISCRETE EVENT SIMULATION
NEW DEVELOPMENT OF OPTIMAL COMPUTING BUDGET ALLOCATION FOR DISCRETE EVENT SIMULATION Hsiao-Chang Chen Dept. of Systems Engineering University of Pennsyvania Phiadephia, PA 904-635, U.S.A. Chun-Hung Chen
More informationSAMPLING II BIOS 662. Michael G. Hudgens, Ph.D. mhudgens :37. BIOS Sampling II
SAMPLING II BIOS 662 Michael G. Hudgens, Ph.D. mhudgens@bios.unc.edu http://www.bios.unc.edu/ mhudgens 2008-11-17 14:37 BIOS 662 1 Sampling II Outline Stratified sampling Introduction Notation and Estimands
More information(This is a sample cover image for this issue. The actual cover is not yet available at this time.)
(This is a sampe cover image for this issue The actua cover is not yet avaiabe at this time) This artice appeared in a journa pubished by Esevier The attached copy is furnished to the author for interna
More informationLaboratory Exercise 1: Pendulum Acceleration Measurement and Prediction Laboratory Handout AME 20213: Fundamentals of Measurements and Data Analysis
Laboratory Exercise 1: Penduum Acceeration Measurement and Prediction Laboratory Handout AME 20213: Fundamentas of Measurements and Data Anaysis Prepared by: Danie Van Ness Date exercises to be performed:
More informationGOYAL BROTHERS PRAKASHAN
Assignments in Mathematics Cass IX (Term 2) 14. STATISTICS IMPORTANT TERMS, DEFINITIONS AND RESULTS The facts or figures, which are numerica or otherwise, coected with a definite purpose are caed data.
More informationStochastic Variational Inference with Gradient Linearization
Stochastic Variationa Inference with Gradient Linearization Suppementa Materia Tobias Pötz * Anne S Wannenwetsch Stefan Roth Department of Computer Science, TU Darmstadt Preface In this suppementa materia,
More informationPhysics Dynamics: Springs
F A C U L T Y O F E D U C A T I O N Department of Curricuum and Pedagogy Physics Dynamics: Springs Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund
More informationInteractive Fuzzy Programming for Two-level Nonlinear Integer Programming Problems through Genetic Algorithms
Md. Abu Kaam Azad et a./asia Paciic Management Review (5) (), 7-77 Interactive Fuzzy Programming or Two-eve Noninear Integer Programming Probems through Genetic Agorithms Abstract Md. Abu Kaam Azad a,*,
More informationPartial permutation decoding for MacDonald codes
Partia permutation decoding for MacDonad codes J.D. Key Department of Mathematics and Appied Mathematics University of the Western Cape 7535 Bevie, South Africa P. Seneviratne Department of Mathematics
More informationXSAT of linear CNF formulas
XSAT of inear CN formuas Bernd R. Schuh Dr. Bernd Schuh, D-50968 Kön, Germany; bernd.schuh@netcoogne.de eywords: compexity, XSAT, exact inear formua, -reguarity, -uniformity, NPcompeteness Abstract. Open
More informationIn-plane shear stiffness of bare steel deck through shell finite element models. G. Bian, B.W. Schafer. June 2017
In-pane shear stiffness of bare stee deck through she finite eement modes G. Bian, B.W. Schafer June 7 COLD-FORMED STEEL RESEARCH CONSORTIUM REPORT SERIES CFSRC R-7- SDII Stee Diaphragm Innovation Initiative
More informationAlgorithms to solve massively under-defined systems of multivariate quadratic equations
Agorithms to sove massivey under-defined systems of mutivariate quadratic equations Yasufumi Hashimoto Abstract It is we known that the probem to sove a set of randomy chosen mutivariate quadratic equations
More information12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes
Maima and Minima 1. Introduction In this Section we anayse curves in the oca neighbourhood of a stationary point and, from this anaysis, deduce necessary conditions satisfied by oca maima and oca minima.
More informationCryptanalysis of PKP: A New Approach
Cryptanaysis of PKP: A New Approach Éiane Jaumes and Antoine Joux DCSSI 18, rue du Dr. Zamenhoff F-92131 Issy-es-Mx Cedex France eiane.jaumes@wanadoo.fr Antoine.Joux@ens.fr Abstract. Quite recenty, in
More informationc 2007 Society for Industrial and Applied Mathematics
SIAM REVIEW Vo. 49,No. 1,pp. 111 1 c 7 Society for Industria and Appied Mathematics Domino Waves C. J. Efthimiou M. D. Johnson Abstract. Motivated by a proposa of Daykin [Probem 71-19*, SIAM Rev., 13 (1971),
More informationHaar Decomposition and Reconstruction Algorithms
Jim Lambers MAT 773 Fa Semester 018-19 Lecture 15 and 16 Notes These notes correspond to Sections 4.3 and 4.4 in the text. Haar Decomposition and Reconstruction Agorithms Decomposition Suppose we approximate
More informationModal analysis of a multi-blade system undergoing rotational motion
Journa of Mechanica Science and Technoogy 3 (9) 5~58 Journa of Mechanica Science and Technoogy www.springerin.com/content/738-494x DOI.7/s6-9-43-3 Moda anaysis of a muti-bade system undergoing rotationa
More informationarxiv:quant-ph/ v3 6 Jan 1995
arxiv:quant-ph/9501001v3 6 Jan 1995 Critique of proposed imit to space time measurement, based on Wigner s cocks and mirrors L. Diósi and B. Lukács KFKI Research Institute for Partice and Nucear Physics
More informationLecture Note 3: Stationary Iterative Methods
MATH 5330: Computationa Methods of Linear Agebra Lecture Note 3: Stationary Iterative Methods Xianyi Zeng Department of Mathematica Sciences, UTEP Stationary Iterative Methods The Gaussian eimination (or
More informationTwo-sample inference for normal mean vectors based on monotone missing data
Journa of Mutivariate Anaysis 97 (006 6 76 wwweseviercom/ocate/jmva Two-sampe inference for norma mean vectors based on monotone missing data Jianqi Yu a, K Krishnamoorthy a,, Maruthy K Pannaa b a Department
More informationCourse 2BA1, Section 11: Periodic Functions and Fourier Series
Course BA, 8 9 Section : Periodic Functions and Fourier Series David R. Wikins Copyright c David R. Wikins 9 Contents Periodic Functions and Fourier Series 74. Fourier Series of Even and Odd Functions...........
More information17 Lecture 17: Recombination and Dark Matter Production
PYS 652: Astrophysics 88 17 Lecture 17: Recombination and Dark Matter Production New ideas pass through three periods: It can t be done. It probaby can be done, but it s not worth doing. I knew it was
More informationMore Scattering: the Partial Wave Expansion
More Scattering: the Partia Wave Expansion Michae Fower /7/8 Pane Waves and Partia Waves We are considering the soution to Schrödinger s equation for scattering of an incoming pane wave in the z-direction
More informationBayesian Learning. You hear a which which could equally be Thanks or Tanks, which would you go with?
Bayesian Learning A powerfu and growing approach in machine earning We use it in our own decision making a the time You hear a which which coud equay be Thanks or Tanks, which woud you go with? Combine
More informationMARKOV CHAINS AND MARKOV DECISION THEORY. Contents
MARKOV CHAINS AND MARKOV DECISION THEORY ARINDRIMA DATTA Abstract. In this paper, we begin with a forma introduction to probabiity and expain the concept of random variabes and stochastic processes. After
More informationChapter 4. Moving Observer Method. 4.1 Overview. 4.2 Theory
Chapter 4 Moving Observer Method 4.1 Overview For a compete description of traffic stream modeing, one woud reuire fow, speed, and density. Obtaining these parameters simutaneousy is a difficut task if
More informationA. Distribution of the test statistic
A. Distribution of the test statistic In the sequentia test, we first compute the test statistic from a mini-batch of size m. If a decision cannot be made with this statistic, we keep increasing the mini-batch
More informationHYDROGEN ATOM SELECTION RULES TRANSITION RATES
DOING PHYSICS WITH MATLAB QUANTUM PHYSICS Ian Cooper Schoo of Physics, University of Sydney ian.cooper@sydney.edu.au HYDROGEN ATOM SELECTION RULES TRANSITION RATES DOWNLOAD DIRECTORY FOR MATLAB SCRIPTS
More information(1 ) = 1 for some 2 (0; 1); (1 + ) = 0 for some > 0:
Answers, na. Economics 4 Fa, 2009. Christiano.. The typica househod can engage in two types of activities producing current output and studying at home. Athough time spent on studying at home sacrices
More informationof being selected and varying such probability across strata under optimal allocation leads to increased accuracy.
5 Sampling with Unequal Probabilities Simple random sampling and systematic sampling are schemes where every unit in the population has the same chance of being selected We will now consider unequal probability
More informationDiscrete Applied Mathematics
Discrete Appied Mathematics 159 (2011) 812 825 Contents ists avaiabe at ScienceDirect Discrete Appied Mathematics journa homepage: www.esevier.com/ocate/dam A direct barter mode for course add/drop process
More informationMultiple Beam Interference
MutipeBeamInterference.nb James C. Wyant 1 Mutipe Beam Interference 1. Airy's Formua We wi first derive Airy's formua for the case of no absorption. ü 1.1 Basic refectance and transmittance Refected ight
More informationSTA 216 Project: Spline Approach to Discrete Survival Analysis
: Spine Approach to Discrete Surviva Anaysis November 4, 005 1 Introduction Athough continuous surviva anaysis differs much from the discrete surviva anaysis, there is certain ink between the two modeing
More informationUnit 48: Structural Behaviour and Detailing for Construction. Deflection of Beams
Unit 48: Structura Behaviour and Detaiing for Construction 4.1 Introduction Defection of Beams This topic investigates the deformation of beams as the direct effect of that bending tendency, which affects
More informationInference Using Biased Coin Randomization. Victoria Plamadeala
Inference Using Biased Coin Randomization A dissertation submitted in partia fufiment of the requirements for the degree of Doctor of Phiosophy at George Mason University By Victoria Pamadeaa Master of
More informationProcess Capability Proposal. with Polynomial Profile
Contemporary Engineering Sciences, Vo. 11, 2018, no. 85, 4227-4236 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ces.2018.88467 Process Capabiity Proposa with Poynomia Profie Roberto José Herrera
More information1. Measurements and error calculus
EV 1 Measurements and error cacuus 11 Introduction The goa of this aboratory course is to introduce the notions of carrying out an experiment, acquiring and writing up the data, and finay anayzing the
More informationResearch of Data Fusion Method of Multi-Sensor Based on Correlation Coefficient of Confidence Distance
Send Orders for Reprints to reprints@benthamscience.ae 340 The Open Cybernetics & Systemics Journa, 015, 9, 340-344 Open Access Research of Data Fusion Method of Muti-Sensor Based on Correation Coefficient
More informationEnergy-Efficient Task Scheduling on Multiple Heterogeneous Computers: Algorithms, Analysis, and Performance Evaluation
IEEE TRANSACTIONS ON SUSTAINABLE COMPUTING, VOL., NO., JANUARY-JUNE 206 7 Energy-Efficient Tas Scheduing on Mutipe Heterogeneous Computers: Agorithms, Anaysis, and Performance Evauation Keqin Li, Feow,
More informationPhysics 127c: Statistical Mechanics. Fermi Liquid Theory: Collective Modes. Boltzmann Equation. The quasiparticle energy including interactions
Physics 27c: Statistica Mechanics Fermi Liquid Theory: Coective Modes Botzmann Equation The quasipartice energy incuding interactions ε p,σ = ε p + f(p, p ; σ, σ )δn p,σ, () p,σ with ε p ε F + v F (p p
More information6.434J/16.391J Statistics for Engineers and Scientists May 4 MIT, Spring 2006 Handout #17. Solution 7
6.434J/16.391J Statistics for Engineers and Scientists May 4 MIT, Spring 2006 Handout #17 Soution 7 Probem 1: Generating Random Variabes Each part of this probem requires impementation in MATLAB. For the
More informationAsymptotic Properties of a Generalized Cross Entropy Optimization Algorithm
1 Asymptotic Properties of a Generaized Cross Entropy Optimization Agorithm Zijun Wu, Michae Koonko, Institute for Appied Stochastics and Operations Research, Caustha Technica University Abstract The discrete
More informationRadiation Fields. Lecture 12
Radiation Fieds Lecture 12 1 Mutipoe expansion Separate Maxwe s equations into two sets of equations, each set separatey invoving either the eectric or the magnetic fied. After remova of the time dependence
More informationStatistical Inference, Econometric Analysis and Matrix Algebra
Statistica Inference, Econometric Anaysis and Matrix Agebra Bernhard Schipp Water Krämer Editors Statistica Inference, Econometric Anaysis and Matrix Agebra Festschrift in Honour of Götz Trenker Physica-Verag
More informationChemical Kinetics Part 2
Integrated Rate Laws Chemica Kinetics Part 2 The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates the rate
More informationLecture 6: Moderately Large Deflection Theory of Beams
Structura Mechanics 2.8 Lecture 6 Semester Yr Lecture 6: Moderatey Large Defection Theory of Beams 6.1 Genera Formuation Compare to the cassica theory of beams with infinitesima deformation, the moderatey
More informationAlberto Maydeu Olivares Instituto de Empresa Marketing Dept. C/Maria de Molina Madrid Spain
CORRECTIONS TO CLASSICAL PROCEDURES FOR ESTIMATING THURSTONE S CASE V MODEL FOR RANKING DATA Aberto Maydeu Oivares Instituto de Empresa Marketing Dept. C/Maria de Moina -5 28006 Madrid Spain Aberto.Maydeu@ie.edu
More informationComponentwise Determination of the Interval Hull Solution for Linear Interval Parameter Systems
Componentwise Determination of the Interva Hu Soution for Linear Interva Parameter Systems L. V. Koev Dept. of Theoretica Eectrotechnics, Facuty of Automatics, Technica University of Sofia, 1000 Sofia,
More information4 Separation of Variables
4 Separation of Variabes In this chapter we describe a cassica technique for constructing forma soutions to inear boundary vaue probems. The soution of three cassica (paraboic, hyperboic and eiptic) PDE
More informationMath 124B January 31, 2012
Math 124B January 31, 212 Viktor Grigoryan 7 Inhomogeneous boundary vaue probems Having studied the theory of Fourier series, with which we successfuy soved boundary vaue probems for the homogeneous heat
More informationTesting for the Existence of Clusters
Testing for the Existence of Custers Caudio Fuentes and George Casea University of Forida November 13, 2008 Abstract The detection and determination of custers has been of specia interest, among researchers
More information(Refer Slide Time: 2:34) L C V
Microwave Integrated Circuits Professor Jayanta Mukherjee Department of Eectrica Engineering Indian Intitute of Technoogy Bombay Modue 1 Lecture No 2 Refection Coefficient, SWR, Smith Chart. Heo wecome
More informationPHYS 110B - HW #1 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased
PHYS 110B - HW #1 Fa 2005, Soutions by David Pace Equations referenced as Eq. # are from Griffiths Probem statements are paraphrased [1.] Probem 6.8 from Griffiths A ong cyinder has radius R and a magnetization
More informationCandidate Number. General Certificate of Education Advanced Level Examination January 2012
entre Number andidate Number Surname Other Names andidate Signature Genera ertificate of Education dvanced Leve Examination January 212 Physics PHY4/1 Unit 4 Fieds and Further Mechanics Section Tuesday
More informationHow the backpropagation algorithm works Srikumar Ramalingam School of Computing University of Utah
How the backpropagation agorithm works Srikumar Ramaingam Schoo of Computing University of Utah Reference Most of the sides are taken from the second chapter of the onine book by Michae Nieson: neuranetworksanddeepearning.com
More informationSure Shot 2016 Electric Current By M K Ezaz
Sure Shot 06 Eectric Current B M K Ezaz. A 0 V batter of negigibe interna resistance is connected across a 00 V batter and a resistance of 38 Ω. Find the vaue of the current in circuit. () E 00 0 A: I
More informationOnline Appendices for The Economics of Nationalism (Xiaohuan Lan and Ben Li)
Onine Appendices for The Economics of Nationaism Xiaohuan Lan and Ben Li) A. Derivation of inequaities 9) and 10) Consider Home without oss of generaity. Denote gobaized and ungobaized by g and ng, respectivey.
More informationChapter 7 PRODUCTION FUNCTIONS. Copyright 2005 by South-Western, a division of Thomson Learning. All rights reserved.
Chapter 7 PRODUCTION FUNCTIONS Copyright 2005 by South-Western, a division of Thomson Learning. A rights reserved. 1 Production Function The firm s production function for a particuar good (q) shows the
More informationChemical Kinetics Part 2. Chapter 16
Chemica Kinetics Part 2 Chapter 16 Integrated Rate Laws The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates
More informationTarget Location Estimation in Wireless Sensor Networks Using Binary Data
Target Location stimation in Wireess Sensor Networks Using Binary Data Ruixin Niu and Pramod K. Varshney Department of ectrica ngineering and Computer Science Link Ha Syracuse University Syracuse, NY 344
More informationu(x) s.t. px w x 0 Denote the solution to this problem by ˆx(p, x). In order to obtain ˆx we may simply solve the standard problem max x 0
Bocconi University PhD in Economics - Microeconomics I Prof M Messner Probem Set 4 - Soution Probem : If an individua has an endowment instead of a monetary income his weath depends on price eves In particuar,
More informationSeparation of Variables and a Spherical Shell with Surface Charge
Separation of Variabes and a Spherica She with Surface Charge In cass we worked out the eectrostatic potentia due to a spherica she of radius R with a surface charge density σθ = σ cos θ. This cacuation
More informationOn colorings of the Boolean lattice avoiding a rainbow copy of a poset arxiv: v1 [math.co] 21 Dec 2018
On coorings of the Booean attice avoiding a rainbow copy of a poset arxiv:1812.09058v1 [math.co] 21 Dec 2018 Baázs Patkós Afréd Rényi Institute of Mathematics, Hungarian Academy of Scinces H-1053, Budapest,
More informationApproximate Bandwidth Allocation for Fixed-Priority-Scheduled Periodic Resources (WSU-CS Technical Report Version)
Approximate Bandwidth Aocation for Fixed-Priority-Schedued Periodic Resources WSU-CS Technica Report Version) Farhana Dewan Nathan Fisher Abstract Recent research in compositiona rea-time systems has focused
More informationarxiv:hep-ph/ v1 15 Jan 2001
BOSE-EINSTEIN CORRELATIONS IN CASCADE PROCESSES AND NON-EXTENSIVE STATISTICS O.V.UTYUZH AND G.WILK The Andrzej So tan Institute for Nucear Studies; Hoża 69; 00-689 Warsaw, Poand E-mai: utyuzh@fuw.edu.p
More informationAutomobile Prices in Market Equilibrium. Berry, Pakes and Levinsohn
Automobie Prices in Market Equiibrium Berry, Pakes and Levinsohn Empirica Anaysis of demand and suppy in a differentiated products market: equiibrium in the U.S. automobie market. Oigopoistic Differentiated
More informationStochastic Complement Analysis of Multi-Server Threshold Queues. with Hysteresis. Abstract
Stochastic Compement Anaysis of Muti-Server Threshod Queues with Hysteresis John C.S. Lui The Dept. of Computer Science & Engineering The Chinese University of Hong Kong Leana Goubchik Dept. of Computer
More informationFlorida State University Libraries
Forida State University Libraries Eectronic Theses, Treatises and Dissertations The Graduate Schoo Construction of Efficient Fractiona Factoria Mixed-Leve Designs Yong Guo Foow this and additiona works
More informationMATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES
MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES Separation of variabes is a method to sove certain PDEs which have a warped product structure. First, on R n, a inear PDE of order m is
More informationSection 6: Magnetostatics
agnetic fieds in matter Section 6: agnetostatics In the previous sections we assumed that the current density J is a known function of coordinates. In the presence of matter this is not aways true. The
More informationMath 1600 Lecture 5, Section 2, 15 Sep 2014
1 of 6 Math 1600 Lecture 5, Section 2, 15 Sep 2014 Announcements: Continue reading Section 1.3 and aso the Exporation on cross products for next cass. Work through recommended homework questions. Quiz
More informationCentralized Coded Caching of Correlated Contents
Centraized Coded Caching of Correated Contents Qianqian Yang and Deniz Gündüz Information Processing and Communications Lab Department of Eectrica and Eectronic Engineering Imperia Coege London arxiv:1711.03798v1
More informationMerging to ordered sequences. Efficient (Parallel) Sorting. Merging (cont.)
Efficient (Paae) Soting One of the most fequent opeations pefomed by computes is oganising (soting) data The access to soted data is moe convenient/faste Thee is a constant need fo good soting agoithms
More informationAnalysis of rounded data in mixture normal model
Stat Papers (2012) 53:895 914 DOI 10.1007/s00362-011-0395-0 REGULAR ARTICLE Anaysis of rounded data in mixture norma mode Ningning Zhao Zhidong Bai Received: 13 August 2010 / Revised: 9 June 2011 / Pubished
More informationAkaike Information Criterion for ANOVA Model with a Simple Order Restriction
Akaike Information Criterion for ANOVA Mode with a Simpe Order Restriction Yu Inatsu * Department of Mathematics, Graduate Schoo of Science, Hiroshima University ABSTRACT In this paper, we consider Akaike
More informationSequential Decoding of Polar Codes with Arbitrary Binary Kernel
Sequentia Decoding of Poar Codes with Arbitrary Binary Kerne Vera Miosavskaya, Peter Trifonov Saint-Petersburg State Poytechnic University Emai: veram,petert}@dcn.icc.spbstu.ru Abstract The probem of efficient
More informationFinal Marking Guidelines 2011 examination June series. Biology Unit 6T A2 Investigative Skills Assignment. General Certificate of Education
Genera Certificate of Education Bioogy Unit 6T A Investigative Skis Assignment BIO6T/P11/MG Fina Marking Guideines 011 examination June series WMP/Jun11/BIO6T/P11/MG Bioogy - AQA GCE BIO6T/P11 /Marking
More informationReliability: Theory & Applications No.3, September 2006
REDUNDANCY AND RENEWAL OF SERVERS IN OPENED QUEUING NETWORKS G. Sh. Tsitsiashvii M.A. Osipova Vadivosto, Russia 1 An opened queuing networ with a redundancy and a renewa of servers is considered. To cacuate
More informationMONOCHROMATIC LOOSE PATHS IN MULTICOLORED k-uniform CLIQUES
MONOCHROMATIC LOOSE PATHS IN MULTICOLORED k-uniform CLIQUES ANDRZEJ DUDEK AND ANDRZEJ RUCIŃSKI Abstract. For positive integers k and, a k-uniform hypergraph is caed a oose path of ength, and denoted by
More informationMaintenance activities planning and grouping for complex structure systems
Maintenance activities panning and grouping for compex structure systems Hai Canh u, Phuc Do an, Anne Barros, Christophe Bérenguer To cite this version: Hai Canh u, Phuc Do an, Anne Barros, Christophe
More informationApplied Nuclear Physics (Fall 2006) Lecture 7 (10/2/06) Overview of Cross Section Calculation
22.101 Appied Nucear Physics (Fa 2006) Lecture 7 (10/2/06) Overview of Cross Section Cacuation References P. Roman, Advanced Quantum Theory (Addison-Wesey, Reading, 1965), Chap 3. A. Foderaro, The Eements
More informationConservation of Circulations in Turbulent Flow
(D) Conservation of Circuations in Turbuent Fow We have emphasized the importance of deveoping a better understanding of the dynamica & statistica origin of the positivity of vortex-stretching rate ω S
More informationA Brief Introduction to Markov Chains and Hidden Markov Models
A Brief Introduction to Markov Chains and Hidden Markov Modes Aen B MacKenzie Notes for December 1, 3, &8, 2015 Discrete-Time Markov Chains You may reca that when we first introduced random processes,
More informationOn Non-Optimally Expanding Sets in Grassmann Graphs
ectronic Cooquium on Computationa Compexity, Report No. 94 (07) On Non-Optimay xpanding Sets in Grassmann Graphs Irit Dinur Subhash Khot Guy Kinder Dor Minzer Mui Safra Abstract The paper investigates
More informationElements of Kinetic Theory
Eements of Kinetic Theory Statistica mechanics Genera description computation of macroscopic quantities Equiibrium: Detaied Baance/ Equipartition Fuctuations Diffusion Mean free path Brownian motion Diffusion
More informationFormulas for Angular-Momentum Barrier Factors Version II
BNL PREPRINT BNL-QGS-06-101 brfactor1.tex Formuas for Anguar-Momentum Barrier Factors Version II S. U. Chung Physics Department, Brookhaven Nationa Laboratory, Upton, NY 11973 March 19, 2015 abstract A
More informationElements of Kinetic Theory
Eements of Kinetic Theory Statistica mechanics Genera description computation of macroscopic quantities Equiibrium: Detaied Baance/ Equipartition Fuctuations Diffusion Mean free path Brownian motion Diffusion
More informationTHE OUT-OF-PLANE BEHAVIOUR OF SPREAD-TOW FABRICS
ECCM6-6 TH EUROPEAN CONFERENCE ON COMPOSITE MATERIALS, Sevie, Spain, -6 June 04 THE OUT-OF-PLANE BEHAVIOUR OF SPREAD-TOW FABRICS M. Wysocki a,b*, M. Szpieg a, P. Heström a and F. Ohsson c a Swerea SICOMP
More informationModule 22: Simple Harmonic Oscillation and Torque
Modue : Simpe Harmonic Osciation and Torque.1 Introduction We have aready used Newton s Second Law or Conservation of Energy to anayze systems ike the boc-spring system that osciate. We sha now use torque
More informationWidth of Percolation Transition in Complex Networks
APS/23-QED Width of Percoation Transition in Compex Networs Tomer Kaisy, and Reuven Cohen 2 Minerva Center and Department of Physics, Bar-Ian University, 52900 Ramat-Gan, Israe 2 Department of Computer
More information