1. Review of Probability.
|
|
- Amie Tyler
- 5 years ago
- Views:
Transcription
1 1. Review of Pobability. What is pobability? Pefom an expeiment. The esult is not pedictable. One of finitely many possibilities R 1, R 2,, R k can occu. Some ae pehaps moe likely than othes. We assign nonnegative numbes p i P [R i ] such that p i 0 and i p i 1. The intepetation is that we know (fom expeience?) that, if we epeated the expeiment a lage numbe of times, these events would occus moe o less in these these ppotions. In othe wods if we epeat the expeiment N times, fo lage N, #(R i ) N p i Often when thee is no eason to pefe one ove the othes we may set P (R i ) 1 k. 1. Examples. Toss a coin. H o T. P (H) P (T ) Thow a die. 1, 2,..., 6. P (1) P (2) P (6) 1 6 Repeated Expeiments. Toss a coin twice. P (HH) P (HT ) P (T H) P (T T ) 1 4. Independence. If P [R i ] p i, then if we epeat twice unde the assumption of independence we have P [R i R j ] P [R i ]P [R j ]. They can be diffeent expeiments. P [R i S j ] P [R i ]P [S j ] You can have many expeiments that ae mutually independent. Fo example fo any sting of length n, P [HHT T HT T H T T ] 1 2 n Absactly X is a finite set of points {x} o {x 1,..., x k } and {p(x)} o {p i } ae numbes adding up to 1. We extend the definition to subsets A X. P (A) i:x i A p i i:x A p(x) P has the popeties 0 P (A) 1. P (X) 1. P ( ) 0 and if A B, then P (A B) P (A) + P (B). 1
2 Wehn diagams. P (A B) P (A) + P (B) P (A B). Mappings. F : X Y. Thee is a natual Q on Y defined by Q(B) P (F 1 A) p i p(x) i:f (x i ) B x:f (x) B If Y R then F is called andom vaiable. Example x {HHT T H} a sting of length n. p(x) 1 2. F is the numbe of heads. {x : F (x) } n has ( n ) stings in it. So ( n ) P [F ] 2 n The heads and tails may have unequal pobabilities. P (H) p and P (T ) 1 p. Then p(x) p F (x) n F (x) (1 p) Theefoe P [F ] ( ) n p (1 p) n Expectations. If X R, then the mean of the distibution p is defined as m x xp (x) Moe geneally if F is andom vaiable then E[F (x)] x F (x)p(x) y yq(y) whee q(y) P [F (x) y] x:f (x)y p(x). If F and G ae andom vaiables then E[aF + bg] ae[f ] + be[g] If P is on X and Q is on Y, then on Z X Y R P Q is the poduct distibution defined by ({x, y}) p(x)q(y). Then it is easy to veify that E[F (x)g(y)] x,y F (x)g(y)p(x)q(y) [ x F (x)p(x)] [ y G(y)q(y)] E[F (x)]e[g(y)] 2
3 Fo the Binomial Distibution m ( ) n p (1 p) n np F F 1 + F F n. Each F i 1 o 0 with pobability p and E[F i ] p and E[F ] n p. Waiting Times; Suppose we have independent tosses with P (H) p and P (T ) 1 p, F is the numbe of ties befoe a Head shows up, (including the last one), then we obtain the Geometic distibution. Fo the Geometic Distibution P [F ] p(1 p) 1 E[F ] p(1 p) 1 1 p Could you have guessed it? Conditional Pobability. P (A B) P (A B) P (B) Example. Dawing without eplacement. We have an un containing ed and g geen ball. A ball is dawn at andom. Then anothe ball is dawn at andom with out eplacement. A is the event that the fist ball is ed. B is the event that the second ball is geen. It is clea that What about P (A B)? P (B A) g g + 1 P (A B) P (A B) P (B) P (A)P (B A) P (B) + g 1 3
4 Bayes ule; B i ae disjoint and thee union is X the whole space. Then P (A) i P (B i A) i P (B i )P (A B i ) In the pevious example P (B) P (B A)P (A) + P (B A c )P (A c ) g g + 1 g + + g 1 g + 1 g g + Conditional Expectation. g g + If F (x) is a andom vaiable on X {x} with pobbailities {p(x)}, the expectation of F on any A can be defined as x A E[F A] F (x)p(x) x A p(x) 1 F (x)p(x) P (A) If X and Y ae two andom vaiables then E[Y X] f(x) x A whee f(x) is defined fo evey x with P [X x] > 0 by the fomula It is easy to check that f(x) E[Y X x] yp [Y y X x] 1 yp [X x, Y y] P [X x] y E[Y ] E[f(X)] E[E[Y X]] Mean and Vaiance. 4
5 Let X {x} be a be a finite set with associated pobabilities {p(x)}. We saw that if Y f(x) is a andom vaiable then, with q(y) P [Y y] x:yf(x) p(x), E[Y ] E[f(x)] yq(y) x f(x)p(x) We can similaly define E[Y 2 ] y y2 q(y). The Vaiance of Y is defined as E[[Y E[Y ]] 2 ] E[Y 2 ] 2[E[Y ]] 2 + [E[Y ]] 2 E[Y 2 ] [E[Y ]] 2 Measues the spead. V (ax + b) a 2 V (X). If X and Y ae independent andom vaiables the V a(x +Y ) V a(x)+ V a(y ). If we expand [X E(X) + Y E(Y )] 2 we get an additional coss tem 2[X E(X)][Y E(Y )] and if X and Y ae independent E[[X E(X)][Y E(Y )]] E[[X E(X)]] E[[Y E(Y )]] 0 Some impotant Discete distibutions. 1. Binomial Distibution. {1, 2,..., n}. P () ( n ) p (1 p) n. Mean np. Vaiance np(1 p). One way to compute is the use of geneating functions. E[e θx ] M(θ) 0 θ E[X ]! e θ ( n M (θ) n(pe θ + 1 p) n 1 pe θ ) p (1 p) n (pe θ + q) n M (θ) n(n 1)(pe θ + 1 p) n 2 p 2 e 2θ + n(pe θ + 1 p) n 1 pe θ Mean M (0) np. Vaiance M (0) [M (0)] 2 n(n 1)p 2 + np n 2 p 2 np np 2 np(1 p) 5
6 2. Geometic Distibution. {0, 1, 2,...,...}. P () p(1 p) 1 M(θ) 1 p(1 p) 1 e θ pe θ 1 (1 p)e θ p p + e θ 1 M (0) 1 p Mean 1 p. Vaiance 1 p 2 M (0) 2 p 2 1 p 1 p 1 p p 2. λ λ 2. Poisson Distibution. {0, 1, 2,...,...}. P () e! M(θ) e λ e λeθ Mean M (0) λ, Vaiance λ. Binomial p << 1, n >> 1 np λ, then as n,p 0, np λ np(1 p) λ. ( n )p (1 p) n λ λ e! Sums of Independent Random vaiables. P [X ] p() P [Y ] q(). X and Y ae independent. π() P [X + Y ] a+b p(a)q(b). π p q is the convolution of p and q. Pobability geneating functions. P (z) p()z. Replace e θ by z. Binomial: (p + qz) n Geomteic: pz 1 (1 p)z Poisson: e λ(z 1). Bin(n, p) Bin(m, p) Bin(n + m, p) P oisson(λ) P oisson(µ) P oisson(λ + µ) [ Negative Binomial: Convolutions of Geometic. P n [X n + ] ( ) n+ 1 (1 p) p n pz 1 (1 p)z Distibution functions. F X (t) P [X t] x t P [X x] 6 ] n
7 If X and Y ae independent and Z max{x, Y }, then F Z (t) F X (t)f Y (t). Assignment 1. k dice ae thown. Assume that all the sides have the same pobability of showing up and the scoes {X 1,..., X k } of the k dice ae independent. What is the pobability distibution of F max 1 i k X i? Calculate E[F ] and V (F ). What happens when k is lage? 7
6 PROBABILITY GENERATING FUNCTIONS
6 PROBABILITY GENERATING FUNCTIONS Cetain deivations pesented in this couse have been somewhat heavy on algeba. Fo example, detemining the expectation of the Binomial distibution (page 5.1 tuned out to
More informationRandom Variables and Probability Distribution Random Variable
Random Vaiables and Pobability Distibution Random Vaiable Random vaiable: If S is the sample space P(S) is the powe set of the sample space, P is the pobability of the function then (S, P(S), P) is called
More information1) (A B) = A B ( ) 2) A B = A. i) A A = φ i j. ii) Additional Important Properties of Sets. De Morgan s Theorems :
Additional Impotant Popeties of Sets De Mogan s Theoems : A A S S Φ, Φ S _ ( A ) A ) (A B) A B ( ) 2) A B A B Cadinality of A, A, is defined as the numbe of elements in the set A. {a,b,c} 3, { }, while
More informationand the correct answer is D.
@. Assume the pobability of a boy being bon is the same as a gil. The pobability that in a family of 5 childen thee o moe childen will be gils is given by A) B) C) D) Solution: The pobability of a gil
More information1 Random Variable. Why Random Variable? Discrete Random Variable. Discrete Random Variable. Discrete Distributions - 1 DD1-1
Rando Vaiable Pobability Distibutions and Pobability Densities Definition: If S is a saple space with a pobability easue and is a eal-valued function defined ove the eleents of S, then is called a ando
More information3.1 Random variables
3 Chapte III Random Vaiables 3 Random vaiables A sample space S may be difficult to descibe if the elements of S ae not numbes discuss how we can use a ule by which an element s of S may be associated
More informationThe Substring Search Problem
The Substing Seach Poblem One algoithm which is used in a vaiety of applications is the family of substing seach algoithms. These algoithms allow a use to detemine if, given two chaacte stings, one is
More informationProbability Distribution (Probability Model) Chapter 2 Discrete Distributions. Discrete Random Variable. Random Variable. Why Random Variable?
Discete Distibutions - Chapte Discete Distibutions Pobability Distibution (Pobability Model) If a balanced coin is tossed, Head and Tail ae equally likely to occu, P(Head) = = / and P(Tail) = = /. Rando
More informationST 501 Course: Fundamentals of Statistical Inference I. Sujit K. Ghosh.
ST 501 Couse: Fundamentals of Statistical Infeence I Sujit K. Ghosh sujit.ghosh@ncsu.edu Pesented at: 2229 SAS Hall, Depatment of Statistics, NC State Univesity http://www.stat.ncsu.edu/people/ghosh/couses/st501/
More informationTHE NUMBER OF TWO CONSECUTIVE SUCCESSES IN A HOPPE-PÓLYA URN
TH NUMBR OF TWO CONSCUTIV SUCCSSS IN A HOPP-PÓLYA URN LARS HOLST Depatment of Mathematics, Royal Institute of Technology S 100 44 Stocholm, Sweden -mail: lholst@math.th.se Novembe 27, 2007 Abstact In a
More informationGoodness-of-fit for composite hypotheses.
Section 11 Goodness-of-fit fo composite hypotheses. Example. Let us conside a Matlab example. Let us geneate 50 obsevations fom N(1, 2): X=nomnd(1,2,50,1); Then, unning a chi-squaed goodness-of-fit test
More information1 Notes on Order Statistics
1 Notes on Ode Statistics Fo X a andom vecto in R n with distibution F, and π S n, define X π by and F π by X π (X π(1),..., X π(n) ) F π (x 1,..., x n ) F (x π 1 (1),..., x π 1 (n)); then the distibution
More informationON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0},
ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION E. J. IONASCU and A. A. STANCU Abstact. We ae inteested in constucting concete independent events in puely atomic pobability
More informationWhen two numbers are written as the product of their prime factors, they are in factored form.
10 1 Study Guide Pages 420 425 Factos Because 3 4 12, we say that 3 and 4 ae factos of 12. In othe wods, factos ae the numbes you multiply to get a poduct. Since 2 6 12, 2 and 6 ae also factos of 12. The
More information16 Modeling a Language by a Markov Process
K. Pommeening, Language Statistics 80 16 Modeling a Language by a Makov Pocess Fo deiving theoetical esults a common model of language is the intepetation of texts as esults of Makov pocesses. This model
More informationSection 5.3 Arrangements and Selections with repetitions
Section 5.3 Aangements and Selections with epetitions Example 1: The numbe of aangements of BANANA? Thm 1: Given n objects, 1 of type 1, 2 of type 2,..., m of type m, with n = 1 + 2 + m, then the numbe
More informationMath 151. Rumbos Spring Solutions to Assignment #7
Math. Rumbos Sping 202 Solutions to Assignment #7. Fo each of the following, find the value of the constant c fo which the given function, p(x, is the pobability mass function (pmf of some discete andom
More informationStanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012
Stanfod Univesity CS59Q: Quantum Computing Handout 8 Luca Tevisan Octobe 8, 0 Lectue 8 In which we use the quantum Fouie tansfom to solve the peiod-finding poblem. The Peiod Finding Poblem Let f : {0,...,
More informationInformation Retrieval Advanced IR models. Luca Bondi
Advanced IR models Luca Bondi Advanced IR models 2 (LSI) Pobabilistic Latent Semantic Analysis (plsa) Vecto Space Model 3 Stating point: Vecto Space Model Documents and queies epesented as vectos in the
More informationPearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms
Peason s Chi-Squae Test Modifications fo Compaison of Unweighted and Weighted Histogams and Two Weighted Histogams Univesity of Akueyi, Bogi, v/noduslód, IS-6 Akueyi, Iceland E-mail: nikolai@unak.is Two
More informationNew problems in universal algebraic geometry illustrated by boolean equations
New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic
More information763620SS STATISTICAL PHYSICS Solutions 2 Autumn 2012
763620SS STATISTICAL PHYSICS Solutions 2 Autumn 2012 1. Continuous Random Walk Conside a continuous one-dimensional andom walk. Let w(s i ds i be the pobability that the length of the i th displacement
More informationIn statistical computations it is desirable to have a simplified system of notation to avoid complicated formulas describing mathematical operations.
Chapte 1 STATISTICAL NOTATION AND ORGANIZATION 11 Summation Notation fo a One-Way Classification In statistical computations it is desiable to have a simplified system of notation to avoid complicated
More informationMacro Theory B. The Permanent Income Hypothesis
Maco Theoy B The Pemanent Income Hypothesis Ofe Setty The Eitan Beglas School of Economics - Tel Aviv Univesity May 15, 2015 1 1 Motivation 1.1 An econometic check We want to build an empiical model with
More informationn 1 Cov(X,Y)= ( X i- X )( Y i-y ). N-1 i=1 * If variable X and variable Y tend to increase together, then c(x,y) > 0
Covaiance and Peason Coelation Vatanian, SW 540 Both covaiance and coelation indicate the elationship between two (o moe) vaiables. Neithe the covaiance o coelation give the slope between the X and Y vaiable,
More informationCSCE 478/878 Lecture 4: Experimental Design and Analysis. Stephen Scott. 3 Building a tree on the training set Introduction. Outline.
In Homewok, you ae (supposedly) Choosing a data set 2 Extacting a test set of size > 3 3 Building a tee on the taining set 4 Testing on the test set 5 Repoting the accuacy (Adapted fom Ethem Alpaydin and
More informationRevision of Lecture Eight
Revision of Lectue Eight Baseband equivalent system and equiements of optimal tansmit and eceive filteing: (1) achieve zeo ISI, and () maximise the eceive SNR Thee detection schemes: Theshold detection
More informationElementary Statistics and Inference. Elementary Statistics and Inference. 11. Regression (cont.) 22S:025 or 7P:025. Lecture 14.
Elementay tatistics and Infeence :05 o 7P:05 Lectue 14 1 Elementay tatistics and Infeence :05 o 7P:05 Chapte 10 (cont.) D. Two Regession Lines uppose two vaiables, and ae obtained on 100 students, with
More information6 Matrix Concentration Bounds
6 Matix Concentation Bounds Concentation bounds ae inequalities that bound pobabilities of deviations by a andom vaiable fom some value, often its mean. Infomally, they show the pobability that a andom
More informationPhysics 211: Newton s Second Law
Physics 211: Newton s Second Law Reading Assignment: Chapte 5, Sections 5-9 Chapte 6, Section 2-3 Si Isaac Newton Bon: Januay 4, 1643 Died: Mach 31, 1727 Intoduction: Kinematics is the study of how objects
More informationLecture 28: Convergence of Random Variables and Related Theorems
EE50: Pobability Foundations fo Electical Enginees July-Novembe 205 Lectue 28: Convegence of Random Vaiables and Related Theoems Lectue:. Kishna Jagannathan Scibe: Gopal, Sudhasan, Ajay, Swamy, Kolla An
More informationLab #4: Newton s Second Law
Lab #4: Newton s Second Law Si Isaac Newton Reading Assignment: bon: Januay 4, 1643 Chapte 5 died: Mach 31, 1727 Chapte 9, Section 9-7 Intoduction: Potait of Isaac Newton by Si Godfey Knelle http://www.newton.cam.ac.uk/at/potait.html
More informationCentral Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution
Statistics Reseach Lettes Vol. Iss., Novembe Cental Coveage Bayes Pediction Intevals fo the Genealized Paeto Distibution Gyan Pakash Depatment of Community Medicine S. N. Medical College, Aga, U. P., India
More informationMath 151 Homework 2 Solutions (Winter 2015)
Math 5 Homewo 2 Solutions (Winte 25 Polem 3. (a Let A and A 2 e the events that the fist and the second selected alls, espectively, ae white. Also let B and B 2 e the events that the thid and the fouth
More informationA Multivariate Normal Law for Turing s Formulae
A Multivaiate Nomal Law fo Tuing s Fomulae Zhiyi Zhang Depatment of Mathematics and Statistics Univesity of Noth Caolina at Chalotte Chalotte, NC 28223 Abstact This pape establishes a sufficient condition
More informationMODULE 5a and 5b (Stewart, Sections 12.2, 12.3) INTRO: In MATH 1114 vectors were written either as rows (a1, a2,..., an) or as columns a 1 a. ...
MODULE 5a and 5b (Stewat, Sections 2.2, 2.3) INTRO: In MATH 4 vectos wee witten eithe as ows (a, a2,..., an) o as columns a a 2... a n and the set of all such vectos of fixed length n was called the vecto
More informationEncapsulation theory: the transformation equations of absolute information hiding.
1 Encapsulation theoy: the tansfomation equations of absolute infomation hiding. Edmund Kiwan * www.edmundkiwan.com Abstact This pape descibes how the potential coupling of a set vaies as the set is tansfomed,
More informationq i i=1 p i ln p i Another measure, which proves a useful benchmark in our analysis, is the chi squared divergence of p, q, which is defined by
CSISZÁR f DIVERGENCE, OSTROWSKI S INEQUALITY AND MUTUAL INFORMATION S. S. DRAGOMIR, V. GLUŠČEVIĆ, AND C. E. M. PEARCE Abstact. The Ostowski integal inequality fo an absolutely continuous function is used
More informationSolutions to Problem Set 8
Massachusetts Institute of Technology 6.042J/18.062J, Fall 05: Mathematics fo Compute Science Novembe 21 Pof. Albet R. Meye and Pof. Ronitt Rubinfeld evised Novembe 27, 2005, 858 minutes Solutions to Poblem
More informationSurveillance Points in High Dimensional Spaces
Société de Calcul Mathématique SA Tools fo decision help since 995 Suveillance Points in High Dimensional Spaces by Benad Beauzamy Januay 06 Abstact Let us conside any compute softwae, elying upon a lage
More information(A) 2log( tan cot ) [ ], 2 MATHEMATICS. 1. Which of the following is correct?
MATHEMATICS. Which of the following is coect? A L.P.P always has unique solution Evey L.P.P has an optimal solution A L.P.P admits two optimal solutions If a L.P.P admits two optimal solutions then it
More informationMarkscheme May 2017 Calculus Higher level Paper 3
M7/5/MATHL/HP3/ENG/TZ0/SE/M Makscheme May 07 Calculus Highe level Pape 3 pages M7/5/MATHL/HP3/ENG/TZ0/SE/M This makscheme is the popety of the Intenational Baccalaueate and must not be epoduced o distibuted
More informationRandom variables (discrete)
Random variables (discrete) Saad Mneimneh 1 Introducing random variables A random variable is a mapping from the sample space to the real line. We usually denote the random variable by X, and a value that
More informationHypothesis Test and Confidence Interval for the Negative Binomial Distribution via Coincidence: A Case for Rare Events
Intenational Jounal of Contempoay Mathematical Sciences Vol. 12, 2017, no. 5, 243-253 HIKARI Ltd, www.m-hikai.com https://doi.og/10.12988/ijcms.2017.7728 Hypothesis Test and Confidence Inteval fo the Negative
More information3.6 Applied Optimization
.6 Applied Optimization Section.6 Notes Page In this section we will be looking at wod poblems whee it asks us to maimize o minimize something. Fo all the poblems in this section you will be taking the
More informationF-IF Logistic Growth Model, Abstract Version
F-IF Logistic Gowth Model, Abstact Vesion Alignments to Content Standads: F-IFB4 Task An impotant example of a model often used in biology o ecology to model population gowth is called the logistic gowth
More informationAppendix A. Appendices. A.1 ɛ ijk and cross products. Vector Operations: δ ij and ɛ ijk
Appendix A Appendices A1 ɛ and coss poducts A11 Vecto Opeations: δ ij and ɛ These ae some notes on the use of the antisymmetic symbol ɛ fo expessing coss poducts This is an extemely poweful tool fo manipulating
More information2 x 8 2 x 2 SKILLS Determine whether the given value is a solution of the. equation. (a) x 2 (b) x 4. (a) x 2 (b) x 4 (a) x 4 (b) x 8
5 CHAPTER Fundamentals When solving equations that involve absolute values, we usually take cases. EXAMPLE An Absolute Value Equation Solve the equation 0 x 5 0 3. SOLUTION By the definition of absolute
More informationChem 453/544 Fall /08/03. Exam #1 Solutions
Chem 453/544 Fall 3 /8/3 Exam # Solutions. ( points) Use the genealized compessibility diagam povided on the last page to estimate ove what ange of pessues A at oom tempeatue confoms to the ideal gas law
More informationPulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects
Pulse Neuton Neuton (PNN) tool logging fo poosity Some theoetical aspects Intoduction Pehaps the most citicism of Pulse Neuton Neuon (PNN) logging methods has been chage that PNN is to sensitive to the
More informationInverse Square Law and Polarization
Invese Squae Law and Polaization Objectives: To show that light intensity is invesely popotional to the squae of the distance fom a point light souce and to show that the intensity of the light tansmitted
More information-Δ u = λ u. u(x,y) = u 1. (x) u 2. (y) u(r,θ) = R(r) Θ(θ) Δu = 2 u + 2 u. r = x 2 + y 2. tan(θ) = y/x. r cos(θ) = cos(θ) r.
The Laplace opeato in pola coodinates We now conside the Laplace opeato with Diichlet bounday conditions on a cicula egion Ω {(x,y) x + y A }. Ou goal is to compute eigenvalues and eigenfunctions of the
More informationMath Section 4.2 Radians, Arc Length, and Area of a Sector
Math 1330 - Section 4. Radians, Ac Length, and Aea of a Secto The wod tigonomety comes fom two Geek oots, tigonon, meaning having thee sides, and mete, meaning measue. We have aleady defined the six basic
More informationA Bijective Approach to the Permutational Power of a Priority Queue
A Bijective Appoach to the Pemutational Powe of a Pioity Queue Ia M. Gessel Kuang-Yeh Wang Depatment of Mathematics Bandeis Univesity Waltham, MA 02254-9110 Abstact A pioity queue tansfoms an input pemutation
More information9.1 The multiplicative group of a finite field. Theorem 9.1. The multiplicative group F of a finite field is cyclic.
Chapte 9 Pimitive Roots 9.1 The multiplicative goup of a finite fld Theoem 9.1. The multiplicative goup F of a finite fld is cyclic. Remak: In paticula, if p is a pime then (Z/p) is cyclic. In fact, this
More informationEXTRA HOTS PROBLEMS. (5 marks) Given : t 3. = a + (n 1)d = 3p 2q + (n 1) (q p) t 10. = 3p 2q + (10 1) (q p) = 3p 2q + 9 (q p) = 3p 2q + 9q 9p = 7q 6p
MT EDUCARE LTD. EXTRA HOTS PROBLEMS HOTS SUMS CHAPTER : - ARITHMETIC PROGRESSION AND GEOMETRIC PROGRESSION. If 3 d tem of an A.P. is p and the 4 th tem is q. Find its n th tem and hence find its 0 th tem.
More informationExploration of the three-person duel
Exploation of the thee-peson duel Andy Paish 15 August 2006 1 The duel Pictue a duel: two shootes facing one anothe, taking tuns fiing at one anothe, each with a fixed pobability of hitting his opponent.
More informationThe geometric construction of Ewald sphere and Bragg condition:
The geometic constuction of Ewald sphee and Bagg condition: The constuction of Ewald sphee must be done such that the Bagg condition is satisfied. This can be done as follows: i) Daw a wave vecto k in
More information10/04/18. P [P(x)] 1 negl(n).
Mastemath, Sping 208 Into to Lattice lgs & Cypto Lectue 0 0/04/8 Lectues: D. Dadush, L. Ducas Scibe: K. de Boe Intoduction In this lectue, we will teat two main pats. Duing the fist pat we continue the
More informationİstanbul Kültür University Faculty of Engineering. MCB1007 Introduction to Probability and Statistics. First Midterm. Fall
İstanbul Kültü Univesity Faculty of Engineeing MCB007 Intoduction to Pobability and Statistics Fist Midtem Fall 03-04 Solutions Diections You have 90 minutes to complete the exam. Please do not leave the
More information4/18/2005. Statistical Learning Theory
Statistical Leaning Theoy Statistical Leaning Theoy A model of supevised leaning consists of: a Envionment - Supplying a vecto x with a fixed but unknown pdf F x (x b Teache. It povides a desied esponse
More informationSTAT 430/510 Probability Lecture 7: Random Variable and Expectation
STAT 430/510 Probability Lecture 7: Random Variable and Expectation Pengyuan (Penelope) Wang June 2, 2011 Review Properties of Probability Conditional Probability The Law of Total Probability Bayes Formula
More informationAlternative Tests for the Poisson Distribution
Chiang Mai J Sci 015; 4() : 774-78 http://epgsciencecmuacth/ejounal/ Contibuted Pape Altenative Tests fo the Poisson Distibution Manad Khamkong*[a] and Pachitjianut Siipanich [b] [a] Depatment of Statistics,
More informationGauss s Law Simulation Activities
Gauss s Law Simulation Activities Name: Backgound: The electic field aound a point chage is found by: = kq/ 2 If thee ae multiple chages, the net field at any point is the vecto sum of the fields. Fo a
More information3D-Central Force Problems II
5.73 ectue # - 1 3D-Cental Foce Poblems II ast time: [x,p] vecto commutation ules: genealize fom 1-D to 3-D conugate position and momentum components in Catesian coodinates Coespondence Pinciple Recipe
More informationQuantum Fourier Transform
Chapte 5 Quantum Fouie Tansfom Many poblems in physics and mathematics ae solved by tansfoming a poblem into some othe poblem with a known solution. Some notable examples ae Laplace tansfom, Legende tansfom,
More informationResearch Design - - Topic 17 Multiple Regression & Multiple Correlation: Two Predictors 2009 R.C. Gardner, Ph.D.
Reseach Design - - Topic 7 Multiple Regession & Multiple Coelation: Two Pedictos 009 R.C. Gadne, Ph.D. Geneal Rationale and Basic Aithmetic fo two pedictos Patial and semipatial coelation Regession coefficients
More informationPHYS 301 HOMEWORK #10 (Optional HW)
PHYS 301 HOMEWORK #10 (Optional HW) 1. Conside the Legende diffeential equation : 1 - x 2 y'' - 2xy' + m m + 1 y = 0 Make the substitution x = cos q and show the Legende equation tansfoms into d 2 y 2
More informationLET a random variable x follows the two - parameter
INTERNATIONAL JOURNAL OF MATHEMATICS AND SCIENTIFIC COMPUTING ISSN: 2231-5330, VOL. 5, NO. 1, 2015 19 Shinkage Bayesian Appoach in Item - Failue Gamma Data In Pesence of Pio Point Guess Value Gyan Pakash
More informationK.S.E.E.B., Malleshwaram, Bangalore SSLC Model Question Paper-1 (2015) Mathematics
K.S.E.E.B., Malleshwaam, Bangaloe SSLC Model Question Pape-1 (015) Mathematics Max Maks: 80 No. of Questions: 40 Time: Hous 45 minutes Code No. : 81E Fou altenatives ae given fo the each question. Choose
More informationNuclear Medicine Physics 02 Oct. 2007
Nuclea Medicine Physics Oct. 7 Counting Statistics and Eo Popagation Nuclea Medicine Physics Lectues Imaging Reseach Laboatoy, Radiology Dept. Lay MacDonald 1//7 Statistics (Summaized in One Slide) Type
More informationME 3600 Control Systems Frequency Domain Analysis
ME 3600 Contol Systems Fequency Domain Analysis The fequency esponse of a system is defined as the steady-state esponse of the system to a sinusoidal (hamonic) input. Fo linea systems, the esulting steady-state
More informationPsychometric Methods: Theory into Practice Larry R. Price
ERRATA Psychometic Methods: Theoy into Pactice Lay R. Pice Eos wee made in Equations 3.5a and 3.5b, Figue 3., equations and text on pages 76 80, and Table 9.1. Vesions of the elevant pages that include
More informationOn the Poisson Approximation to the Negative Hypergeometric Distribution
BULLETIN of the Malaysian Mathematical Sciences Society http://mathusmmy/bulletin Bull Malays Math Sci Soc (2) 34(2) (2011), 331 336 On the Poisson Appoximation to the Negative Hypegeometic Distibution
More informationAuchmuty High School Mathematics Department Advanced Higher Notes Teacher Version
The Binomial Theoem Factoials Auchmuty High School Mathematics Depatment The calculations,, 6 etc. often appea in mathematics. They ae called factoials and have been given the notation n!. e.g. 6! 6!!!!!
More informationEncapsulation theory: radial encapsulation. Edmund Kirwan *
Encapsulation theoy: adial encapsulation. Edmund Kiwan * www.edmundkiwan.com Abstact This pape intoduces the concept of adial encapsulation, wheeby dependencies ae constained to act fom subsets towads
More informationDynamic Visualization of Complex Integrals with Cabri II Plus
Dynamic Visualiation of omplex Integals with abi II Plus Sae MIKI Kawai-juu, IES Japan Email: sand_pictue@hotmailcom Abstact: Dynamic visualiation helps us undestand the concepts of mathematics This pape
More informationPhysics: Work & Energy Beyond Earth Guided Inquiry
Physics: Wok & Enegy Beyond Eath Guided Inquiy Elliptical Obits Keple s Fist Law states that all planets move in an elliptical path aound the Sun. This concept can be extended to celestial bodies beyond
More informationNotes on McCall s Model of Job Search. Timothy J. Kehoe March if job offer has been accepted. b if searching
Notes on McCall s Model of Job Seach Timothy J Kehoe Mach Fv ( ) pob( v), [, ] Choice: accept age offe o eceive b and seach again next peiod An unemployed oke solves hee max E t t y t y t if job offe has
More informationSolution to HW 3, Ma 1a Fall 2016
Solution to HW 3, Ma a Fall 206 Section 2. Execise 2: Let C be a subset of the eal numbes consisting of those eal numbes x having the popety that evey digit in the decimal expansion of x is, 3, 5, o 7.
More informationA New Method of Estimation of Size-Biased Generalized Logarithmic Series Distribution
The Open Statistics and Pobability Jounal, 9,, - A New Method of Estimation of Size-Bied Genealized Logaithmic Seies Distibution Open Access Khushid Ahmad Mi * Depatment of Statistics, Govt Degee College
More informationProbabilistic Systems Analysis Spring 2018 Lecture 6. Random Variables: Probability Mass Function and Expectation
EE 178 Probabilistic Systems Analysis Spring 2018 Lecture 6 Random Variables: Probability Mass Function and Expectation Probability Mass Function When we introduce the basic probability model in Note 1,
More informationFractional Zero Forcing via Three-color Forcing Games
Factional Zeo Focing via Thee-colo Focing Games Leslie Hogben Kevin F. Palmowski David E. Robeson Michael Young May 13, 2015 Abstact An -fold analogue of the positive semidefinite zeo focing pocess that
More informationBetween any two masses, there exists a mutual attractive force.
YEAR 12 PHYSICS: GRAVITATION PAST EXAM QUESTIONS Name: QUESTION 1 (1995 EXAM) (a) State Newton s Univesal Law of Gavitation in wods Between any two masses, thee exists a mutual attactive foce. This foce
More informationExperiment I Voltage Variation and Control
ELE303 Electicity Netwoks Expeiment I oltage aiation and ontol Objective To demonstate that the voltage diffeence between the sending end of a tansmission line and the load o eceiving end depends mainly
More informationEXAM NMR (8N090) November , am
EXA NR (8N9) Novembe 5 9, 9. 1. am Remaks: 1. The exam consists of 8 questions, each with 3 pats.. Each question yields the same amount of points. 3. You ae allowed to use the fomula sheet which has been
More informationPhysics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism
Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up
More informationMEASURES OF BLOCK DESIGN EFFICIENCY RECOVERING INTERBLOCK INFORMATION
MEASURES OF BLOCK DESIGN EFFICIENCY RECOVERING INTERBLOCK INFORMATION Walte T. Fedee 337 Waen Hall, Biometics Unit Conell Univesity Ithaca, NY 4853 and Tey P. Speed Division of Mathematics & Statistics,
More informationNuclear and Particle Physics - Lecture 20 The shell model
1 Intoduction Nuclea and Paticle Physics - Lectue 0 The shell model It is appaent that the semi-empiical mass fomula does a good job of descibing tends but not the non-smooth behaviou of the binding enegy.
More informationof the contestants play as Falco, and 1 6
JHMT 05 Algeba Test Solutions 4 Febuay 05. In a Supe Smash Bothes tounament, of the contestants play as Fox, 3 of the contestants play as Falco, and 6 of the contestants play as Peach. Given that thee
More informationLecture 8 - Gauss s Law
Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.
More information221B Lecture Notes Scattering Theory I
Why Scatteing? B Lectue Notes Scatteing Theoy I Scatteing of paticles off taget has been one of the most impotant applications of quantum mechanics. It is pobably the most effective way to study the stuctue
More informationControl Chart Analysis of E k /M/1 Queueing Model
Intenational OPEN ACCESS Jounal Of Moden Engineeing Reseach (IJMER Contol Chat Analysis of E /M/1 Queueing Model T.Poongodi 1, D. (Ms. S. Muthulashmi 1, (Assistant Pofesso, Faculty of Engineeing, Pofesso,
More informationMONTE CARLO SIMULATION OF FLUID FLOW
MONTE CARLO SIMULATION OF FLUID FLOW M. Ragheb 3/7/3 INTRODUCTION We conside the situation of Fee Molecula Collisionless and Reflective Flow. Collisionless flows occu in the field of aefied gas dynamics.
More informationarxiv: v1 [math.co] 1 Apr 2011
Weight enumeation of codes fom finite spaces Relinde Juius Octobe 23, 2018 axiv:1104.0172v1 [math.co] 1 Ap 2011 Abstact We study the genealized and extended weight enumeato of the - ay Simplex code and
More informationMultiple Criteria Secretary Problem: A New Approach
J. Stat. Appl. Po. 3, o., 9-38 (04 9 Jounal of Statistics Applications & Pobability An Intenational Jounal http://dx.doi.og/0.785/jsap/0303 Multiple Citeia Secetay Poblem: A ew Appoach Alaka Padhye, and
More informationTemporal-Difference Learning
.997 Decision-Making in Lage-Scale Systems Mach 17 MIT, Sping 004 Handout #17 Lectue Note 13 1 Tempoal-Diffeence Leaning We now conside the poblem of computing an appopiate paamete, so that, given an appoximation
More informationMATH 415, WEEK 3: Parameter-Dependence and Bifurcations
MATH 415, WEEK 3: Paamete-Dependence and Bifucations 1 A Note on Paamete Dependence We should pause to make a bief note about the ole played in the study of dynamical systems by the system s paametes.
More informationProblem 1. Part b. Part a. Wayne Witzke ProblemSet #1 PHY 361. Calculate x, the expected value of x, defined by
Poblem Pat a The nomal distibution Gaussian distibution o bell cuve has the fom f Ce µ Calculate the nomalization facto C by equiing the distibution to be nomalized f Substituting in f, defined above,
More informationRigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018
Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining
More information