Gaussian related distributions

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

Download "Gaussian related distributions"

Transcript

1 Gaussian related distributions Santiago Aja-Fernández June 19, Gaussian related distributions 1. Gaussian: ormal PDF: MGF: Main moments:. Rayleigh: PDF: MGF: Raw moments: Main moments: px = 1 σ π exp x µ σ R = M X t = exp µt + σ t Mean µ Median µ Mode µ Variance σ X 1 + X X i 0, σ px = x σ exp x σ M X t = 1 + σte σ t / π σt erf + 1 µ k = σ k k/ Γ1 + k/ Mean σ π Median σ log 4 Mode σ Variance 4 π σ 1 π µ 1 = σ µ = σ π µ 3 = 3 σ3 µ 4 = 8σ 4 1

2 3. Rician: R = X 1 + X X i A i, σ PDF: where A = A 1 + A. Raw moments: R = X X = A 1, σ + ja, σ p M M A, σ = M M +A σ e σ where L n x = M n, 1, x = 1 F 1 n; 1; x. Main moments: AM I 0 σ µ k = σ k k/ Γ1 + k/l k/ A σ Mean Median Mode Variance π µ 1 = L 1/ π µ 3 = 3 L 3/ σ π L 1/ A σ σ + A πσ L 1/ A σ A σ A σ σ µ = A + σ σ 3 µ 4 = A 4 + 8σ A + 8σ 4 um, 3 π µ 1 = L 1/ x σ µ = σ 1 + x π µ 3 = 3 L 3/ x σ 3 µ 4 = 4σ 4 + 4x + x Var = A 4 + 8σ A + 8σ 4 σ 1 1 4x 1 8x + Ox 3 with x = A σ Series expansion of Hypergeometric Functions: L 1/ x = x 1 + π π x πx + O x 5/ 3/ L 3/ x = 4x3/ 3 π + 3 x 3 + π 8 π x πx + O x 5/. 3/ 4. Central Chi: on-normalized version R = L Xi X i 0, σ

3 PDF: Raw moments: Main moments: R = L Y i Y i = 0, σ + j0, σ px σ, L = 1 L ΓL x L 1 σ L µ k = σ k k/ Γk/ + L ΓL µ 1 = ΓL + 1/ σ ΓL µ = Lσ µ 3 = 3 ΓL + 3/ σ 3 ΓL µ 4 = 4LL + 1σ 4 Γk/ + L Var = σ L ΓL x e σ 4 5. on central Chi: on-normalized version R = L Xi X i A i, σ PDF: with A L = i A i Main moments: µ 1 = µ 3 = 3 R = L Y i Y i = A 1,i, σ + ja,i, σ pm L A L, σ, L = A1 L L σ ML L e M L +A L AL M L σ I L 1 σ um L, 5 ΓL + 1/ 1F 1 1 ΓL, L, A L σ ΓL + 3/ 1F 1 3 ΓL, L, A L σ σ µ = A L + Lσ σ 3 µ 4 = A 4 L + 4L + 1A Lσ + 4LL + 1σ 4 µ 1 = ΓL + 1/ 1F 1 1 ΓL, L, x σ µ = σ L + x µ 3 = 3 ΓL + 3/ 1F 1 3 ΓL, L, x σ 3 µ 4 = 4σ 4 x + L + 1x + LL + 1 ΓL + 1/ Var = σ 1 + x ΓL σ L 3 8L + 4L + 4x 8x + Ox 3 1F 1 1, L, x with x = A σ 3

4 6. Gamma: PDF: MGF: Main moments: k 1 exp x/θ p x x = x Γkθ k ux 6 M X t = 1 θt k for t < 1/θ Mean kθ Median Mode k 1θ Variance kθ k = µ 1 Var θ = Var µ 1 mode = µ 1 Var µ 1 7. K distribution: PDF: x +1 x p x x = K ux 7 aγ + 1 a a In ultrasound we consider the following parameters: a = 1 b = 4α b E{A } = 4α σ = α 1 and then the PDF becomes: General form of the PDF: p x x = b Γα p x x = α xb K α 1 bx ux 8 with p R x/y a Rayleigh distribution Rσ = a y: and p γ y a Gamma distribution γ + 1, 1: Moments: Main moments for ultrasound: E{x k } = p R x/y = x a y e 0 p γ y = p R x/yp γ ydy x a y ux y Γ + 1 e y Γk/ + 1Γ k/ a k Γ + 1 µ 1 = Γ3/Γα + 1/ σ µ = σ αγα µ 3 = σ 3/ Γ5/Γα + 3/ α 3/ Γα [ Var = σ 1 1 α µ 4 = σ α ] Γ3/Γα + 1/ Γα 4

5 Sample Local Variance Gamma Approximation The biased SLV of an image Mx is defined as VarMx = 1 ηx p ηx M p 1 ηx p ηx Mp 9 with ηx a neighborhood centered in x. If = ηx, we define the random variable V = VarMx with moments E{V } = 1 1 µ µ 1 E{V } = 1 3 [ + 1µ µ µ µ µ µ 3 µ 1 ] VarV = 1 [ µ 3 µ µ µ µ + + 1µ µ 4 ] 1 For the main models: 1. Rayleigh E{V } = σn 1 π 4 σn 1 π 4 σ V = σ4 n π π + O 1. Rice E{V } = 1σ n σ4 n 4 + π π 1 1 4x 1 8x + O x 3 for x = A σ. n σv = 4σ4 n with KL = 1σ n σ V = 1σ4 n 1σ4 n 3. Central Chi E{V } = σ n 1 ΓL + 1/ L ΓL L + 8L Γ L + 1/ Γ 4 Γ4 L + 1/ L Γ 4 L L Γ L+1/ Γ L. 1 x x + O x 3 4 ΓL + 1/ΓL + 3/ 1 Γ + O L 5

6 4. on central Chi E{V } = σ n L 3 8L + 4L + x 8x + O x 3 σ n 1 σv = σ4 n L + O x x σ4 n 1 5. K distribution with E{V } = σ 1 1 K 1 α σ V = σ4 K α + O Γ3/Γα + 1/ K 1 α = 1 1 α Γα K = a + 1 a Γa 4 [ πγa + 1/ Γa a 3πΓa + 1/ Γa π Γa + 1/ 4] On the four cases, the PDF of the SLV may be approximated using a Gamma distribution. The mode of the distribution for each case is: 1. Rayleigh. Rice mode{v } = E{V } σ V E{V } = σn π 1 σn π mode{v } = σ n σ 5π 16π + O1/ π O σ/a 3. Central Chi mode{v } = σ n L Γ L + 1/ 1 Γ + O L KLσ n 4. on central Chi O σ n /A mode{v } = σ n σ n 6

7 5. K distribution mode{v } σ n 4 8K 1 K + 4K1 K 1 1 1/ 3 Combination of Gaussian Variables Let X i A, σ, i = 1,, be a set of Gaussian random variables. 1. Constant added and multiplied: aµ, σ + b aµ + b, a σ. Sum of zero mean Gaussian variables: IID 0, σ1 + 0, σ 0, σ1 + σ 3. Sum of Gaussian variables: IID L L i 0, σi 0, σi µ 1, σ1 + µ, σ µ 1 + µ, σ1 + σ L L L i µ i, σi µ i, 4. Difference of Gaussian variables: IID µ 1, σ1 µ, σ µ 1 µ, σ1 + σ 5. Product of Gaussian variables: IID µ 1, σ1 µ, σ σ i with PDF: px = 1 x K 0 πσ 1 σ σ 1 σ 6. Sum of square zero mean Gaussian variables: IID Xi σ γ/, σ χ σ / with X i σ = 0, σ and χ σ / a chi-square with degrees of freedom. 7. Square root of the sum of square Gaussian variables: IID X1 0, σ + X 0, σ Rσ with Rσ a Rayleigh distribution. X 1 A 1, σ + X A, σ R c A 1 + A ; σ 7

8 with R c A; σ a Rician distribution. L Xi 0, σ χ C L, σ i 1 with χ C L, σ a central Chi distirbution with parameters σ and L. L Xi A i, σ χ A L ; L, σ i 1 with χ A L, L, σ a non central Chi distirbution with parameters σ, L and A L = i A i. 8. Sample variance of Gaussian S = Combination of Rayleigh Variables Let R i σ, i = 1,, be a set of Rayleigh random variables. 1. Sum of square Gaussian variables: with X i σ = 0, σ. Sum of square Rayleigh variables: X i X 1 σ γ, 1 Xi σ γ/, σ Ri σ γ, σ with PDF: p x x = x 1 e x/σ Γσ ux 3. Sample mean of square Rayleigh variables: 1 Ri σ γ, σ χ σ / with PDF: p x x = x 1 Γσ e x/σ ux 4. Sum of Rayleigh variables: R i σ 8

9 with PDF approx: with 5. Sample mean of Rayleigh variables: e x /b p x x = x 1 1 b Γ ux b = σ [ 1!!]1/ ] σ e σ π 4 1 R i σ with PDF approx: p x x = x 1 1 b Γ e x /b ux 6. Square sample mean of Rayleigh variables: 1 R i σ χ b/ γ/, b with PDF approx: p x x = x 1 b Γ e x/b ux 7. Square root of sum of square Rayleigh variables: Ri σ χ, σ with χ, σ a central chi with PDF: p x x = x 1 Γσ e x /σ ux 8. Square root of sample mean of square Rayleigh variables: 1 Ri σ χ, σ / with χ, σ / a central chi with PDF: 9. Local sample variance of Rayleigh variables: p x x = x 1 Γσ e x /σ ux V = 1 Ri σ 1 R i σ 9

10 For x 0 and an even number of degrees of freedom the PDF is p V x = x 1 exp 1 4 α+ x 1 Γσ1 σ 1 ρ γ k=0 with σ1 = σ n, σ σ n π 4 γ = Γ + k Γk + 1Γ k [ σ σ 1 + 4σ 1σ 1 ρ ] 1/ σ 1 σ 1 ρ α + = γ + σ σ 1 σ 1 σ 1 ρ, k γ x and ρ the correlation coefficient, which for large may be approximated as ρ 5 Combination of Rician Variables π 4 16π 4π 0.95 Let R i σ, i = 1,, be a set of Rician random variables. 1. Sum of square Rician variables: Ri A i, σ χ x σ, A σ with χ a noncentral chi square with A = i A i, and PDF px = 1 1/ x σ e x+a xa σ I 1 σ A. Sample mean of square Rician variables: 1 L Ri A i, σ χ with χ a noncentral chi square with PDF px = 1 1/ σ x 1/ e x+a σ A 3. Sum of square Rician variables: approx. L R i A i, σ x σ, A σ with PDF L 1 pt = tl c1 c e t c b c tb 1 I L 1 c b c 1 c with c 1 and c constants, t = x/ LKΩ L and b = K+1, [?]. 4. Square of the sample mean of Rician variables: 1 L R i A i, σ χ xa I 1 σ x c, b c 1 10

11 6 Combination of K Variables Let K i σ, α, i = 1,, be a set of K-distributed random variables. 1. Transformation of K-variables: If then p S x = with T = fr i and R i Rayleigh variables.. Sum of square K variables: with PDF: 3. Sum of K variables: with PDF approximation p S x = p S x = fk i 0 p T x/yp γ ydy M Ki σ, α M+α x ΓMΓαa α+m x M+α 1 M K i σ, α x 1 K α M a M+α a K3M M+α ΓMΓα K α M ux x a K 3 M ux with K 3 M = M 1!! 1/M 7 Logarithmic transformation of RV 7.1 The lograyleigh distribution Let Rσ be a Rayleigh RV with σ parameter, the transformation, la transformacin lrσ = a logrσ + b is a log-rayleigh withpdf with σ a = σ e b a. Main moments p lr x = 1 x aσa e x a e e a σa E{x} = a [ logσ a γ ] where γ is the Euler s constant. E{x } = a 4 [ logσa + b ] a γ + π 6 11

12 MGF: Varx = π a 4 Φ lr ω = σ a jω a Γ j a ω Operation over log-rayleigh 1. Sum of lograyleigh lr i σ then the MGF is Φ P lrω = σa jω a Γ j a ω + 1 The mean is. Sum of two lograyleigh with PDF E{x} = a [ logσ a γ ] lr 1 σ + lr σ p t = 1 e aσa 4 e t/a t/a K 0 σa 7.3 The LogRician distribution If we define the variable Lrx = log Mx = log A + nr σn + n i σn this variable follows a LogRician distribution with PDF p L x = ex σn e e x +A σ Ae x n I 0 σn with x, +. The moments of this distribution are E{x} = 1 Γl 0, A σn + loga 1 E{x } = 1 4 log σn 1 + log σn [ ] Γ 0, l A A σn + log σn + 1 A 4Ñ1 σn 13 σx = 1 ] A Ñ 1 4 σn + [Γ 0, l A A σn + log σn 14 1 A A Ñ 1 log 15 4 σ n σ n with Γ l a, b the lower incomplete Gamma function and Ñ k x = e x i=0 x i [ ] ψi + k + ψ 1 i + k. Γi + 1 1

13 ψx is the polygamma function and ψ 1 x is its first derivative. It is easy to see that 1 σx A σn. The same solution for the variance may be obtained using a Series expansion on eq. 10 Lrx loga + n 1 A + n A n 1 A +... loga + n 1 A σ L r = σ A 7.4 The Log-on Central Chi distribution For parallel acquisitions, if we define the variable Lcx = log M L x = 1 L log Clr x + C li x 16 this variable follows a Log-on central Chi distribution with PDF p Lc x = A1 L L σn e x+1 e e x +A L AL e x σn I L 1 σn with x, +. The moments of this distribution are E{x} = 1 log σn 1 + E{x } = 1 [ log σn 4 ] A L +ÑL σ x = σ n [ Ñ L A L σ n ψl + l=1 A L Lσn F 1, 1 :, 1 + L; A L σn + log σ n ψl + A L Lσn Lσ n ψl 18 F 1, 1 :, 1 + ; A L σ n log σn A L Lσn F 1, 1 :, 1 + ; A L σn ] A L F 1, 1 :, 1 + ; A L [ ] A Ñ L A L σn log L σn 8 About the Coefficient of variation 8.1 CV of a Rayleigh distribution The square coeffiecient of variation CV of a random variable x is defined to be σ n C x = Varx E {x} = E{x } E {x} E = E{x } {x} E {x} 1 If x is a random variable that follows a Rayleigh distribution, then C x = 4 π σ n = 4 π π σ n π 13

14 So, the CV of a Rayleigh distribution does not depend on the value of σ n. In the paper, the value of the sample CV is used to tune the filter. 8. Sample CV of Rayleigh Let R i σn, i = {1,, } be a set of random variables with Rayleigh distribution. Then, if X = 1 Ri 1 Y = R i the sample CV may be defined as Z = X Y Y = X Y 1 3 Both X and Y are Chi-Square random variables. σ X χ n b Y χ The PDF of U = X Z assuming that X and Y are independent i i f U u = Γ σ Γ n b u 1 bu + σn 4 and making b σ n π 4 As Z = U 1 then with mode f U u = Γ π u 1 Γ 4 πu/ f Z z = Γ π z Γ 4 πz + 1/ f Z z Γ 4 z Γ z π/4 mode{f Z z} = 1 4 π 4 π + 1 π π 8.3 CV in a Rician distribution The square CV is Cx = E{x } E {x} 1 = = A [ σ π 4σ n e n 1 + A σn A [ π σ e n 1 + A σn σn + A I 0 + A/σ n I 0 A 4σ n A 4σ n + A σ n + A σ n I 1 A 4σn I 1 A 4σn ] 1 ] 1 14

15 If R = A σ n we can write C = 1 + R π e R [ 1 + R I 0 R + RI1 R ] 1 15

Solution Series 9. i=1 x i and i=1 x i.

Solution Series 9. i=1 x i and i=1 x i. Lecturer: Prof. Dr. Mete SONER Coordinator: Yilin WANG Solution Series 9 Q1. Let α, β >, the p.d.f. of a beta distribution with parameters α and β is { Γ(α+β) Γ(α)Γ(β) f(x α, β) xα 1 (1 x) β 1 for < x

Διαβάστε περισσότερα

Statistics 104: Quantitative Methods for Economics Formula and Theorem Review

Statistics 104: Quantitative Methods for Economics Formula and Theorem Review Harvard College Statistics 104: Quantitative Methods for Economics Formula and Theorem Review Tommy MacWilliam, 13 tmacwilliam@college.harvard.edu March 10, 2011 Contents 1 Introduction to Data 5 1.1 Sample

Διαβάστε περισσότερα

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr T t N n) Pr max X 1,..., X N ) t N n) Pr max

Διαβάστε περισσότερα

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013 Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering

Διαβάστε περισσότερα

Bayesian statistics. DS GA 1002 Probability and Statistics for Data Science.

Bayesian statistics. DS GA 1002 Probability and Statistics for Data Science. Bayesian statistics DS GA 1002 Probability and Statistics for Data Science http://www.cims.nyu.edu/~cfgranda/pages/dsga1002_fall17 Carlos Fernandez-Granda Frequentist vs Bayesian statistics In frequentist

Διαβάστε περισσότερα

ST5224: Advanced Statistical Theory II

ST5224: Advanced Statistical Theory II ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known

Διαβάστε περισσότερα

An Inventory of Continuous Distributions

An Inventory of Continuous Distributions Appendi A An Inventory of Continuous Distributions A.1 Introduction The incomplete gamma function is given by Also, define Γ(α; ) = 1 with = G(α; ) = Z 0 Z 0 Z t α 1 e t dt, α > 0, >0 t α 1 e t dt, α >

Διαβάστε περισσότερα

Other Test Constructions: Likelihood Ratio & Bayes Tests

Other Test Constructions: Likelihood Ratio & Bayes Tests Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :

Διαβάστε περισσότερα

Probability and Random Processes (Part II)

Probability and Random Processes (Part II) Probability and Random Processes (Part II) 1. If the variance σ x of d(n) = x(n) x(n 1) is one-tenth the variance σ x of a stationary zero-mean discrete-time signal x(n), then the normalized autocorrelation

Διαβάστε περισσότερα

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr (T t N n) Pr (max (X 1,..., X N ) t N n) Pr (max

Διαβάστε περισσότερα

4.6 Autoregressive Moving Average Model ARMA(1,1)

4.6 Autoregressive Moving Average Model ARMA(1,1) 84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this

Διαβάστε περισσότερα

Solutions to Exercise Sheet 5

Solutions to Exercise Sheet 5 Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X

Διαβάστε περισσότερα

Statistical Inference I Locally most powerful tests

Statistical Inference I Locally most powerful tests Statistical Inference I Locally most powerful tests Shirsendu Mukherjee Department of Statistics, Asutosh College, Kolkata, India. shirsendu st@yahoo.co.in So far we have treated the testing of one-sided

Διαβάστε περισσότερα

FORMULAS FOR STATISTICS 1

FORMULAS FOR STATISTICS 1 FORMULAS FOR STATISTICS 1 X = 1 n Sample statistics X i or x = 1 n x i (sample mean) S 2 = 1 n 1 s 2 = 1 n 1 (X i X) 2 = 1 n 1 (x i x) 2 = 1 n 1 Xi 2 n n 1 X 2 x 2 i n n 1 x 2 or (sample variance) E(X)

Διαβάστε περισσότερα

6.3 Forecasting ARMA processes

6.3 Forecasting ARMA processes 122 CHAPTER 6. ARMA MODELS 6.3 Forecasting ARMA processes The purpose of forecasting is to predict future values of a TS based on the data collected to the present. In this section we will discuss a linear

Διαβάστε περισσότερα

6. MAXIMUM LIKELIHOOD ESTIMATION

6. MAXIMUM LIKELIHOOD ESTIMATION 6 MAXIMUM LIKELIHOOD ESIMAION [1] Maximum Likelihood Estimator (1) Cases in which θ (unknown parameter) is scalar Notational Clarification: From now on, we denote the true value of θ as θ o hen, view θ

Διαβάστε περισσότερα

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R + Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b

Διαβάστε περισσότερα

Homework 3 Solutions

Homework 3 Solutions Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For

Διαβάστε περισσότερα

Homework for 1/27 Due 2/5

Homework for 1/27 Due 2/5 Name: ID: Homework for /7 Due /5. [ 8-3] I Example D of Sectio 8.4, the pdf of the populatio distributio is + αx x f(x α) =, α, otherwise ad the method of momets estimate was foud to be ˆα = 3X (where

Διαβάστε περισσότερα

Aquinas College. Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET

Aquinas College. Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET Aquinas College Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET Pearson Edexcel Level 3 Advanced Subsidiary and Advanced GCE in Mathematics and Further Mathematics Mathematical

Διαβάστε περισσότερα

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0. DESIGN OF MACHINERY SOLUTION MANUAL -7-1! PROBLEM -7 Statement: Design a double-dwell cam to move a follower from to 25 6, dwell for 12, fall 25 and dwell for the remader The total cycle must take 4 sec

Διαβάστε περισσότερα

Second Order Partial Differential Equations

Second Order Partial Differential Equations Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y

Διαβάστε περισσότερα

2 Composition. Invertible Mappings

2 Composition. Invertible Mappings Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,

Διαβάστε περισσότερα

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch: HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying

Διαβάστε περισσότερα

w o = R 1 p. (1) R = p =. = 1

w o = R 1 p. (1) R = p =. = 1 Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 205 ιδάσκων : Α. Μουχτάρης Τριτη Σειρά Ασκήσεων Λύσεις Ασκηση 3. 5.2 (a) From the Wiener-Hopf equation we have:

Διαβάστε περισσότερα

The Simply Typed Lambda Calculus

The Simply Typed Lambda Calculus Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and

Διαβάστε περισσότερα

Example Sheet 3 Solutions

Example Sheet 3 Solutions Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note

Διαβάστε περισσότερα

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8  questions or comments to Dan Fetter 1 Eon : Fall 8 Suggested Solutions to Problem Set 8 Email questions or omments to Dan Fetter Problem. Let X be a salar with density f(x, θ) (θx + θ) [ x ] with θ. (a) Find the most powerful level α test

Διαβάστε περισσότερα

APPENDICES APPENDIX A. STATISTICAL TABLES AND CHARTS 651 APPENDIX B. BIBLIOGRAPHY 677 APPENDIX C. ANSWERS TO SELECTED EXERCISES 679

APPENDICES APPENDIX A. STATISTICAL TABLES AND CHARTS 651 APPENDIX B. BIBLIOGRAPHY 677 APPENDIX C. ANSWERS TO SELECTED EXERCISES 679 APPENDICES APPENDIX A. STATISTICAL TABLES AND CHARTS 1 Table I Summary of Common Probability Distributions 2 Table II Cumulative Standard Normal Distribution Table III Percentage Points, 2 of the Chi-Squared

Διαβάστε περισσότερα

Partial Differential Equations in Biology The boundary element method. March 26, 2013

Partial Differential Equations in Biology The boundary element method. March 26, 2013 The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet

Διαβάστε περισσότερα

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits. EAMCET-. THEORY OF EQUATIONS PREVIOUS EAMCET Bits. Each of the roots of the equation x 6x + 6x 5= are increased by k so that the new transformed equation does not contain term. Then k =... - 4. - Sol.

Διαβάστε περισσότερα

Problem Set 3: Solutions

Problem Set 3: Solutions CMPSCI 69GG Applied Information Theory Fall 006 Problem Set 3: Solutions. [Cover and Thomas 7.] a Define the following notation, C I p xx; Y max X; Y C I p xx; Ỹ max I X; Ỹ We would like to show that C

Διαβάστε περισσότερα

Areas and Lengths in Polar Coordinates

Areas and Lengths in Polar Coordinates Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the

Διαβάστε περισσότερα

D Alembert s Solution to the Wave Equation

D Alembert s Solution to the Wave Equation D Alembert s Solution to the Wave Equation MATH 467 Partial Differential Equations J. Robert Buchanan Department of Mathematics Fall 2018 Objectives In this lesson we will learn: a change of variable technique

Διαβάστε περισσότερα

5.4 The Poisson Distribution.

5.4 The Poisson Distribution. The worst thing you can do about a situation is nothing. Sr. O Shea Jackson 5.4 The Poisson Distribution. Description of the Poisson Distribution Discrete probability distribution. The random variable

Διαβάστε περισσότερα

DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C

DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C By Tom Irvine Email: tomirvine@aol.com August 6, 8 Introduction The obective is to derive a Miles equation which gives the overall response

Διαβάστε περισσότερα

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics Fourier Series MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Introduction Not all functions can be represented by Taylor series. f (k) (c) A Taylor series f (x) = (x c)

Διαβάστε περισσότερα

Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3

Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 1 State vector space and the dual space Space of wavefunctions The space of wavefunctions is the set of all

Διαβάστε περισσότερα

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- ----------------- Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin

Διαβάστε περισσότερα

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

Chapter 6: Systems of Linear Differential. be continuous functions on the interval Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations

Διαβάστε περισσότερα

Approximation of distance between locations on earth given by latitude and longitude

Approximation of distance between locations on earth given by latitude and longitude Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth

Διαβάστε περισσότερα

6.1. Dirac Equation. Hamiltonian. Dirac Eq.

6.1. Dirac Equation. Hamiltonian. Dirac Eq. 6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2

Διαβάστε περισσότερα

( ) 2 and compare to M.

( ) 2 and compare to M. Problems and Solutions for Section 4.2 4.9 through 4.33) 4.9 Calculate the square root of the matrix 3!0 M!0 8 Hint: Let M / 2 a!b ; calculate M / 2!b c ) 2 and compare to M. Solution: Given: 3!0 M!0 8

Διαβάστε περισσότερα

Every set of first-order formulas is equivalent to an independent set

Every set of first-order formulas is equivalent to an independent set Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent

Διαβάστε περισσότερα

ΣΤΟΧΑΣΤΙΚΑ ΣΥΣΤΗΜΑΤΑ & ΕΠΙΚΟΙΝΩΝΙΕΣ 1o Τμήμα (Α - Κ): Αμφιθέατρο 4, Νέα Κτίρια ΣΗΜΜΥ Θεωρία Πιθανοτήτων & Στοχαστικές Ανελίξεις - 2

ΣΤΟΧΑΣΤΙΚΑ ΣΥΣΤΗΜΑΤΑ & ΕΠΙΚΟΙΝΩΝΙΕΣ 1o Τμήμα (Α - Κ): Αμφιθέατρο 4, Νέα Κτίρια ΣΗΜΜΥ Θεωρία Πιθανοτήτων & Στοχαστικές Ανελίξεις - 2 ΣΤΟΧΑΣΤΙΚΑ ΣΥΣΤΗΜΑΤΑ & ΕΠΙΚΟΙΝΩΝΙΕΣ 1o Τμήμα (Α - Κ): Αμφιθέατρο 4, Νέα Κτίρια ΣΗΜΜΥ Θεωρία Πιθανοτήτων & Στοχαστικές Ανελίξεις - 5.4: Στατιστικοί Μέσοι Όροι 5.5 Στοχαστικές Ανελίξεις (Stochastic Processes)

Διαβάστε περισσότερα

MATHEMATICS. 1. If A and B are square matrices of order 3 such that A = -1, B =3, then 3AB = 1) -9 2) -27 3) -81 4) 81

MATHEMATICS. 1. If A and B are square matrices of order 3 such that A = -1, B =3, then 3AB = 1) -9 2) -27 3) -81 4) 81 1. If A and B are square matrices of order 3 such that A = -1, B =3, then 3AB = 1) -9 2) -27 3) -81 4) 81 We know that KA = A If A is n th Order 3AB =3 3 A. B = 27 1 3 = 81 3 2. If A= 2 1 0 0 2 1 then

Διαβάστε περισσότερα

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)

Διαβάστε περισσότερα

Section 8.3 Trigonometric Equations

Section 8.3 Trigonometric Equations 99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.

Διαβάστε περισσότερα

Concrete Mathematics Exercises from 30 September 2016

Concrete Mathematics Exercises from 30 September 2016 Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)

Διαβάστε περισσότερα

forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with

forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with Week 03: C lassification of S econd- Order L inear Equations In last week s lectures we have illustrated how to obtain the general solutions of first order PDEs using the method of characteristics. We

Διαβάστε περισσότερα

Areas and Lengths in Polar Coordinates

Areas and Lengths in Polar Coordinates Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the

Διαβάστε περισσότερα

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

Chapter 6: Systems of Linear Differential. be continuous functions on the interval Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations

Διαβάστε περισσότερα

Lecture 12: Pseudo likelihood approach

Lecture 12: Pseudo likelihood approach Lecture 12: Pseudo likelihood approach Pseudo MLE Let X 1,...,X n be a random sample from a pdf in a family indexed by two parameters θ and π with likelihood l(θ,π). The method of pseudo MLE may be viewed

Διαβάστε περισσότερα

EE512: Error Control Coding

EE512: Error Control Coding EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3

Διαβάστε περισσότερα

Notes on the Open Economy

Notes on the Open Economy Notes on the Open Econom Ben J. Heijdra Universit of Groningen April 24 Introduction In this note we stud the two-countr model of Table.4 in more detail. restated here for convenience. The model is Table.4.

Διαβάστε περισσότερα

HW 3 Solutions 1. a) I use the auto.arima R function to search over models using AIC and decide on an ARMA(3,1)

HW 3 Solutions 1. a) I use the auto.arima R function to search over models using AIC and decide on an ARMA(3,1) HW 3 Solutions a) I use the autoarima R function to search over models using AIC and decide on an ARMA3,) b) I compare the ARMA3,) to ARMA,0) ARMA3,) does better in all three criteria c) The plot of the

Διαβάστε περισσότερα

Web-based supplementary materials for Bayesian Quantile Regression for Ordinal Longitudinal Data

Web-based supplementary materials for Bayesian Quantile Regression for Ordinal Longitudinal Data Web-based supplementary materials for Bayesian Quantile Regression for Ordinal Longitudinal Data Rahim Alhamzawi, Haithem Taha Mohammad Ali Department of Statistics, College of Administration and Economics,

Διαβάστε περισσότερα

Quadratic Expressions

Quadratic Expressions Quadratic Expressions. The standard form of a quadratic equation is ax + bx + c = 0 where a, b, c R and a 0. The roots of ax + bx + c = 0 are b ± b a 4ac. 3. For the equation ax +bx+c = 0, sum of the roots

Διαβάστε περισσότερα

Reminders: linear functions

Reminders: linear functions Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U

Διαβάστε περισσότερα

Tutorial on Multinomial Logistic Regression

Tutorial on Multinomial Logistic Regression Tutorial on Multinomial Logistic Regression Javier R Movellan June 19, 2013 1 1 General Model The inputs are n-dimensional vectors the outputs are c-dimensional vectors The training sample consist of m

Διαβάστε περισσότερα

Lecture 34 Bootstrap confidence intervals

Lecture 34 Bootstrap confidence intervals Lecture 34 Bootstrap confidence intervals Confidence Intervals θ: an unknown parameter of interest We want to find limits θ and θ such that Gt = P nˆθ θ t If G 1 1 α is known, then P θ θ = P θ θ = 1 α

Διαβάστε περισσότερα

Exercises to Statistics of Material Fatigue No. 5

Exercises to Statistics of Material Fatigue No. 5 Prof. Dr. Christine Müller Dipl.-Math. Christoph Kustosz Eercises to Statistics of Material Fatigue No. 5 E. 9 (5 a Show, that a Fisher information matri for a two dimensional parameter θ (θ,θ 2 R 2, can

Διαβάστε περισσότερα

Introduction to the ML Estimation of ARMA processes

Introduction to the ML Estimation of ARMA processes Introduction to the ML Estimation of ARMA processes Eduardo Rossi University of Pavia October 2013 Rossi ARMA Estimation Financial Econometrics - 2013 1 / 1 We consider the AR(p) model: Y t = c + φ 1 Y

Διαβάστε περισσότερα

Matrices and Determinants

Matrices and Determinants Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z

Διαβάστε περισσότερα

Theorem 8 Let φ be the most powerful size α test of H

Theorem 8 Let φ be the most powerful size α test of H Testing composite hypotheses Θ = Θ 0 Θ c 0 H 0 : θ Θ 0 H 1 : θ Θ c 0 Definition 16 A test φ is a uniformly most powerful (UMP) level α test for H 0 vs. H 1 if φ has level α and for any other level α test

Διαβάστε περισσότερα

Second Order RLC Filters

Second Order RLC Filters ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor

Διαβάστε περισσότερα

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Αν κάπου κάνετε κάποιες υποθέσεις να αναφερθούν στη σχετική ερώτηση. Όλα τα αρχεία που αναφέρονται στα προβλήματα βρίσκονται στον ίδιο φάκελο με το εκτελέσιμο

Διαβάστε περισσότερα

EE101: Resonance in RLC circuits

EE101: Resonance in RLC circuits EE11: Resonance in RLC circuits M. B. Patil mbatil@ee.iitb.ac.in www.ee.iitb.ac.in/~sequel Deartment of Electrical Engineering Indian Institute of Technology Bombay I V R V L V C I = I m = R + jωl + 1/jωC

Διαβάστε περισσότερα

Μηχανική Μάθηση Hypothesis Testing

Μηχανική Μάθηση Hypothesis Testing ΕΛΛΗΝΙΚΗ ΔΗΜΟΚΡΑΤΙΑ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ Μηχανική Μάθηση Hypothesis Testing Γιώργος Μπορμπουδάκης Τμήμα Επιστήμης Υπολογιστών Procedure 1. Form the null (H 0 ) and alternative (H 1 ) hypothesis 2. Consider

Διαβάστε περισσότερα

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β 3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle

Διαβάστε περισσότερα

Differential equations

Differential equations Differential equations Differential equations: An equation inoling one dependent ariable and its deriaties w. r. t one or more independent ariables is called a differential equation. Order of differential

Διαβάστε περισσότερα

HOMEWORK#1. t E(x) = 1 λ = (b) Find the median lifetime of a randomly selected light bulb. Answer:

HOMEWORK#1. t E(x) = 1 λ = (b) Find the median lifetime of a randomly selected light bulb. Answer: HOMEWORK# 52258 李亞晟 Eercise 2. The lifetime of light bulbs follows an eponential distribution with a hazard rate of. failures per hour of use (a) Find the mean lifetime of a randomly selected light bulb.

Διαβάστε περισσότερα

ECE598: Information-theoretic methods in high-dimensional statistics Spring 2016

ECE598: Information-theoretic methods in high-dimensional statistics Spring 2016 ECE598: Information-theoretic methods in high-dimensional statistics Spring 06 Lecture 7: Information bound Lecturer: Yihong Wu Scribe: Shiyu Liang, Feb 6, 06 [Ed. Mar 9] Recall the Chi-squared divergence

Διαβάστε περισσότερα

5. Choice under Uncertainty

5. Choice under Uncertainty 5. Choice under Uncertainty Daisuke Oyama Microeconomics I May 23, 2018 Formulations von Neumann-Morgenstern (1944/1947) X: Set of prizes Π: Set of probability distributions on X : Preference relation

Διαβάστε περισσότερα

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ. Chemistry 362 Dr Jean M Standard Problem Set 9 Solutions The ˆ L 2 operator is defined as Verify that the angular wavefunction Y θ,φ) Also verify that the eigenvalue is given by 2! 2 & L ˆ 2! 2 2 θ 2 +

Διαβάστε περισσότερα

derivation of the Laplacian from rectangular to spherical coordinates

derivation of the Laplacian from rectangular to spherical coordinates derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used

Διαβάστε περισσότερα

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =

Διαβάστε περισσότερα

BarChart y 1, y 2, makes a bar chart with bar lengths y 1, y 2,.

BarChart y 1, y 2, makes a bar chart with bar lengths y 1, y 2,. In[]:= In[]:= In[3]:= In[4]:= In[5]:= Out[5]= r : Random ri : Random Integer rdice : Random Integer,, 6 disp : Export "t.ps",, "EPS" & list Table rdice, 0 5,, 4, 6,, 3,, 3, 4,, 6, 4, 6,,, 6, 6,, 3, In[6]:=

Διαβάστε περισσότερα

Local Approximation with Kernels

Local Approximation with Kernels Local Approximation with Kernels Thomas Hangelbroek University of Hawaii at Manoa 5th International Conference Approximation Theory, 26 work supported by: NSF DMS-43726 A cubic spline example Consider

Διαβάστε περισσότερα

Math221: HW# 1 solutions

Math221: HW# 1 solutions Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin

Διαβάστε περισσότερα

( y) Partial Differential Equations

( y) Partial Differential Equations Partial Dierential Equations Linear P.D.Es. contains no owers roducts o the deendent variables / an o its derivatives can occasionall be solved. Consider eamle ( ) a (sometimes written as a ) we can integrate

Διαβάστε περισσότερα

These derivations are not part of the official forthcoming version of Vasilaky and Leonard

These derivations are not part of the official forthcoming version of Vasilaky and Leonard Target Input Model with Learning, Derivations Kathryn N Vasilaky These derivations are not part of the official forthcoming version of Vasilaky and Leonard 06 in Economic Development and Cultural Change.

Διαβάστε περισσότερα

( )( ) ( ) ( )( ) ( )( ) β = Chapter 5 Exercise Problems EX α So 49 β 199 EX EX EX5.4 EX5.5. (a)

( )( ) ( ) ( )( ) ( )( ) β = Chapter 5 Exercise Problems EX α So 49 β 199 EX EX EX5.4 EX5.5. (a) hapter 5 xercise Problems X5. α β α 0.980 For α 0.980, β 49 0.980 0.995 For α 0.995, β 99 0.995 So 49 β 99 X5. O 00 O or n 3 O 40.5 β 0 X5.3 6.5 μ A 00 β ( 0)( 6.5 μa) 8 ma 5 ( 8)( 4 ) or.88 P on + 0.0065

Διαβάστε περισσότερα

Fractional Colorings and Zykov Products of graphs

Fractional Colorings and Zykov Products of graphs Fractional Colorings and Zykov Products of graphs Who? Nichole Schimanski When? July 27, 2011 Graphs A graph, G, consists of a vertex set, V (G), and an edge set, E(G). V (G) is any finite set E(G) is

Διαβάστε περισσότερα

Estimation for ARMA Processes with Stable Noise. Matt Calder & Richard A. Davis Colorado State University

Estimation for ARMA Processes with Stable Noise. Matt Calder & Richard A. Davis Colorado State University Estimation for ARMA Processes with Stable Noise Matt Calder & Richard A. Davis Colorado State University rdavis@stat.colostate.edu 1 ARMA processes with stable noise Review of M-estimation Examples of

Διαβάστε περισσότερα

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ting Zhang Stanford May 11, 2001 Stanford, 5/11/2001 1 Outline Ordinal Classification Ordinal Addition Ordinal Multiplication Ordinal

Διαβάστε περισσότερα

Multi-dimensional Central Limit Theorem

Multi-dimensional Central Limit Theorem Mult-dmensonal Central Lmt heorem Outlne () () () t as () + () + + () () () Consder a sequence of ndependent random proceses t, t, dentcal to some ( t). Assume t 0. Defne the sum process t t t t () t tme

Διαβάστε περισσότερα

Homework 8 Model Solution Section

Homework 8 Model Solution Section MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx

Διαβάστε περισσότερα

Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων. Εξάμηνο 7 ο

Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων. Εξάμηνο 7 ο Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων Εξάμηνο 7 ο Procedures and Functions Stored procedures and functions are named blocks of code that enable you to group and organize a series of SQL and PL/SQL

Διαβάστε περισσότερα

Additional Results for the Pareto/NBD Model

Additional Results for the Pareto/NBD Model Additional Results for the Pareto/NBD Model Peter S. Fader www.petefader.com Bruce G. S. Hardie www.brucehardie.com January 24 Abstract This note derives expressions for i) the raw moments of the posterior

Διαβάστε περισσότερα

SPECIAL FUNCTIONS and POLYNOMIALS

SPECIAL FUNCTIONS and POLYNOMIALS SPECIAL FUNCTIONS and POLYNOMIALS Gerard t Hooft Stefan Nobbenhuis Institute for Theoretical Physics Utrecht University, Leuvenlaan 4 3584 CC Utrecht, the Netherlands and Spinoza Institute Postbox 8.195

Διαβάστε περισσότερα

Section 9.2 Polar Equations and Graphs

Section 9.2 Polar Equations and Graphs 180 Section 9. Polar Equations and Graphs In this section, we will be graphing polar equations on a polar grid. In the first few examples, we will write the polar equation in rectangular form to help identify

Διαβάστε περισσότερα

The Relationship Between Flux Density and Brightness Temperature

The Relationship Between Flux Density and Brightness Temperature The Relationship Between Flux Density and Brightness Temperature Jeff Mangum (NRAO) June 3, 015 Contents 1 The Answer 1 Introduction 1 3 Elliptical Gaussian Source 3 Uniform Disk Source 5 1 The Answer

Διαβάστε περισσότερα

Overview. Transition Semantics. Configurations and the transition relation. Executions and computation

Overview. Transition Semantics. Configurations and the transition relation. Executions and computation Overview Transition Semantics Configurations and the transition relation Executions and computation Inference rules for small-step structural operational semantics for the simple imperative language Transition

Διαβάστε περισσότερα

Biostatistics for Health Sciences Review Sheet

Biostatistics for Health Sciences Review Sheet Biostatistics for Health Sciences Review Sheet http://mathvault.ca June 1, 2017 Contents 1 Descriptive Statistics 2 1.1 Variables.............................................. 2 1.1.1 Qualitative........................................

Διαβάστε περισσότερα

SCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018

SCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018 Journal of rogressive Research in Mathematics(JRM) ISSN: 2395-028 SCITECH Volume 3, Issue 2 RESEARCH ORGANISATION ublished online: March 29, 208 Journal of rogressive Research in Mathematics www.scitecresearch.com/journals

Διαβάστε περισσότερα

Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in

Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in : tail in X, head in A nowhere-zero Γ-flow is a Γ-circulation such that

Διαβάστε περισσότερα

Module 5. February 14, h 0min

Module 5. February 14, h 0min Module 5 Stationary Time Series Models Part 2 AR and ARMA Models and Their Properties Class notes for Statistics 451: Applied Time Series Iowa State University Copyright 2015 W. Q. Meeker. February 14,

Διαβάστε περισσότερα

On the Galois Group of Linear Difference-Differential Equations

On the Galois Group of Linear Difference-Differential Equations On the Galois Group of Linear Difference-Differential Equations Ruyong Feng KLMM, Chinese Academy of Sciences, China Ruyong Feng (KLMM, CAS) Galois Group 1 / 19 Contents 1 Basic Notations and Concepts

Διαβάστε περισσότερα

C.S. 430 Assignment 6, Sample Solutions

C.S. 430 Assignment 6, Sample Solutions C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order

Διαβάστε περισσότερα