Lecture 7: Interchange of integration and limit
|
|
- Tyler Glenn
- 6 years ago
- Views:
Transcription
1 Lecture 7: Interchange of integration an limit Differentiating uner an integral sign To stuy the properties of a chf, we nee some technical result. When can we switch the ifferentiation an integration? If the range of the integral is finite, this switch is usually vali. Theorem (Leibnitz s rule) If f (x,θ), a(θ), an b(θ) are ifferentiable with respect to θ, then θ b(θ) a(θ) f (x,θ)x = f (b(θ),θ)b (θ) f (a(θ),θ)a (θ)+ In particular, if a(θ) = a an b(θ) = b are constants, then θ b a f (x,θ)x = b a f (x,θ) x b(θ) a(θ) If the range of integration is infinite, problems can arise. f (x,θ) x Whether ifferentiation an integration can be switche is the same as whether limit an integration can be interchange. UW-Maison (Statistics) Stat 609 Lecture / 15
2 Interchange of integration an limit Note that f (x,θ) x = lim δ 0 f (x,θ + δ) f (x,θ) x δ Hence, the interchange of ifferentiation an integration means whether this is equal to θ f (x,θ)x = lim δ 0 f (x,θ + δ) f (x,θ) x δ An example of invali interchanging integration an limit Consier { δ 1 0 < x < δ f (x,δ) = 0 otherwise Then, lim δ 0 f (x,δ) = 0 for any x an, hence, 0 = lim δ 0 δ f (x,δ)x lim f (x,δ)x = lim δ 0 δ 0 0 δ 1 x = 1 UW-Maison (Statistics) Stat 609 Lecture / 15
3 We now give some sufficient conitions uner which interchanging integration an limit (or ifferentiation) is vali. The proof of the main result is technical an out of the scope of this course. Theorem (Lebesgue s ominate convergence theorem) Suppose that the function h(x,y) is continuous at y 0 for each x, an there exists a function g(x) satisfying (i) h(x,y) g(x) for all x an y in a neighborhoo of y 0 ; (ii) g(x)x <. Then, lim h(x,y)x = lim h(x,y)x y y 0 y y 0 The key conition in this theorem is the existence of a ominating function g(x) with a finite integral. Applying Theorem to the ifference [f (x,θ + δ) f (x,θ)]/δ, we obtain the next result. UW-Maison (Statistics) Stat 609 Lecture / 15
4 Theorem Suppose that f (x,θ) is ifferentiable at θ = θ 0, i.e., f (x,θ 0 + δ) f (x,θ 0 ) f (x,θ) lim = δ 0 δ θ=θ0 exists for every x, an there exists a function g(x,θ 0 ) an a constant δ 0 > 0 such that (i) f (x,θ 0+δ) f (x,θ 0 ) δ g(x,θ 0 ) for all x an δ δ 0 ; (ii) g(x,θ 0)x <. Then f (x,θ)x f (x,θ) θ = θ=θ0 x θ=θ0 This result is for θ at a particular value, θ 0. Typically f (x,θ) is ifferentiable at all θ, an f (x,θ 0 + δ) f (x,θ 0 ) δ = f (x,θ) θ=θ0 +δ (x) for some δ (x) with δ (x) δ 0, which leas to the next result. UW-Maison (Statistics) Stat 609 Lecture / 15
5 Corollary Suppose that f (x,θ) is ifferentiable in θ an there exists a function g(x,θ) such that (i) f (x,ϑ) ϑ g(x,θ) for all x an ϑ such that ϑ θ δ0 ; (ii) g(x,θ)x < for all θ. Then f (x,θ) f (x,θ)x = x θ Example Let X have the exponential pf f (x) = λ 1 e x/λ, x > 0 where λ > 0 is a constant. We want to prove a recursion relation E(X n+1 ) = λe(x n ) + λ λ E(X n ), n = 1,2,... Note that both E(X n ) an E(X n+1 ) are functions of λ. UW-Maison (Statistics) Stat 609 Lecture / 15
6 If we coul move the ifferentiation insie the integral, we woul have λ E(X n ) = x n ( ) x n λ 0 λ e x/λ x = 0 λ λ e x/λ x x n ( x ) = λ 2 λ 1 e x/λ x = 1 λ 2 E(X n+1 ) 1 λ E(X n ) 0 which is the result we want to show. To justify the interchange of integration an ifferentiation, we take g(x,λ) = x n e x/(λ+δ ( ) 0) x (λ δ 0 ) λ δ 0 Then ( x n ξ ξ e x/ξ ) x n e x/ξ x ξ + 1 g(x,λ), ξ λ δ 0 ξ 2 an we can apply Corollary In the proof of Theorem (ifferentiating mgf to obtain moments), we interchange ifferentiation an integration without justification. We now provie a proof. UW-Maison (Statistics) Stat 609 Lecture / 15
7 Completion of the proof of Theorem Assuming that M X (t) exists for t [ h,h], h > 0, we want to show t M X (t) = t It is enough to show (why?) e tx f X (x)x = e tx f X (x)x = t 0 For t ( h/2,h/2) an x > 0, t etx f X (x) = xe tx f X (x) 0 t etx f X (x)x t etx f X (x)x xehx/2 f X (x) = g(x) For sufficiently large x > 0, x e hx/2 an, hence, 0 g(x)x 0 e hx f X (x)x = M X (h) < An application of Corollary proves the result. We now complete the proof of Theorem C1 an establish another useful result for inverting a characteristic function. UW-Maison (Statistics) Stat 609 Lecture / 15
8 Completion of the proof of Theorem C1. We give a proof for the case where X has pf f X (x). If we can exchange the ifferentiation an integration, then r φ X (t) t r = r e ıtx r t r f X (x)x = e ıtx t r f X (x)x = ı r x r e ıtx f X (x)x an the result follows by setting t = 0 at the beginning an en of the above expression. The exchange is justifie by the ominate convergence theorem, since r e ıtx t r f X (x) ı = r x r e ıtx f X (x) x r f X (x) an E X r = x r f X (x)x < Theorem C7. Let φ(t) be a chf satisfying φ(t) t <. Then the corresponing cf F has erivative F (x) = 1 e ıtx φ(t)t 2π UW-Maison (Statistics) Stat 609 Lecture / 15
9 Proof. Let x δ an x + δ be continuity points of F. By Theorem C2, T e ıt(x δ) e ıt(x+δ) F(x + δ) F(x δ) = lim φ(t)t T T 2π ıt T sin(tδ)e ıtx = lim φ(t)t T T πt sin(tδ)e ıtx = φ(t)t πt where the last equality follows from the fact that sin(tδ)e ıtx φ(t) πtδ φ(t) which is integrable. Also, from the previous boun we can apply the ominate convergence theorem to interchange the integration an limit in the following operation to finish the proof: UW-Maison (Statistics) Stat 609 Lecture / 15
10 Example F F(x + δ) F(x δ) (x) = lim δ 0 2δ sin(tδ)e ıtx = lim φ(t)t δ 0 2πtδ sin(tδ)e ıtx = lim φ(t)t δ 0 2πtδ = 1 e ıtx φ(t)t 2π We now apply Theorem C7 to obtain the pf corresponing to the chf φ(t) = e t : F (x) = 1 e ıtx e t t = 1 cos(tx)e t t 2π π 0 Since e at cos(bt)t = e at [acos(bt) + b sin(bt)]/(a 2 + b 2 ), F (x) = 1 e t [ cos(xt) + x sin(xt)] t= 1 π 1 + x 2 = π(1 + x 2 ) t=0 UW-Maison (Statistics) Stat 609 Lecture / 15
11 We now turn to the question of when we can interchange ifferentiation an infinite summation. Theorem Suppose that the series h(θ,x) converges for all θ in an interval (a,b) R an h(θ,x) is continuous in θ for each x; (ii) h(θ,x) converges uniformly on every close boune subinterval of (a, b). Then (i) θ h(θ,x) = h(θ,x) This theorem is from calculus (or mathematical analysis) an is not easy to apply because we nee to show the uniform convergence of an infinite series. It is more convenient to apply the following ominate convergence theorem for infinite sums. UW-Maison (Statistics) Stat 609 Lecture / 15
12 Theorem 2.4.2A (ominate convergence theorem) Suppose that the function h(x,y) is continuous at y 0 for each x, an there exists a function g(x) satisfying (i) h(x,y) g(x) for all x an y in a neighborhoo of y 0 ; (ii) x g(x) <. Then, lim y y 0 h(x,y) = lim h(x,y) y y x x 0 If h(x,θ) is ifferentiable in θ an there is a function g(x,θ) such that g(x,θ) for all x an ϑ such that ϑ θ δ 0 ; (i) h(x,ϑ) ϑ (ii) x g(x,θ) < for all θ. Then θ x Example h(x,θ) h(x,θ) = x Let X be a iscrete ranom variable having pmf f X (x) = P(X = x) = θ(1 θ) x, x = 0,1,2,... where θ (0,1) is a fixe constant. We want to erive E(X). UW-Maison (Statistics) Stat 609 Lecture / 15
13 Note that θ(1 θ) x = 1 If interchange of summation an ifferentiation is justifie, 0 = θ = = 1 θ Thus, E(X) = (1 θ)/θ. θ(1 θ) x = [(1 θ) x θx(1 θ) x 1 ] θ(1 θ) x 1 1 θ = 1 θ 1 1 θ E(X) θ(1 θ)x xθ(1 θ) x To justify the interchange, let h(x,θ) = θ(1 θ) x an then h(θ,x) = (1 θ)x θx(1 θ) x 1 Consier θ [c,] (0,1). UW-Maison (Statistics) Stat 609 Lecture / 15
14 (1 θ) x θx(1 θ) x 1 (1 c) x + x(1 c) x 1 = g(x) Since [(1 c) x + x(1 c) x 1 ] < the exchange of sum an ifferentiation is justifie. Monotone convergence theorem In some cases, the following result is more convenient to apply. Suppose that functions g n (x), n = 1,2,..., x R, satisfying that 0 g n (x) g n+1 (x) for all n an x an lim n g n (x) = g(x) for all x. Then lim g n (x)x = lim g n(x)x = g(x)x n n which hols even if g(x) is not integrable (i.e., both sies are infinity). The same result hols when is replace by for iscrete x. Proof. We prove the continuous case, since the iscrete case is similar. If g(x)x <, then this result is a irect consequence of the ominate convergence theorem. UW-Maison (Statistics) Stat 609 Lecture / 15
15 Suppose now that g(x)x =. Then g(x)i { x M,g(x) M} x = lim M where I A is the inicator function of A. For each M > 0, g(x)i { x M,g(x) M} x 2M 2 < an g n (x)i { x M,g(x) M} is monotone an converges to g(x)i { x M,g(x) M}. Then, for every M. lim n g n (x)x lim = Since the right sie goes to, n lim n g n (x)i { x M,g(x) M} x g(x)i { x M,g(x) M} x g n (x)x = UW-Maison (Statistics) Stat 609 Lecture / 15
MA 2232 Lecture 08 - Review of Log and Exponential Functions and Exponential Growth
MA 2232 Lecture 08 - Review of Log an Exponential Functions an Exponential Growth Friay, February 2, 2018. Objectives: Review log an exponential functions, their erivative an integration formulas. Exponential
More informationMake graph of g by adding c to the y-values. on the graph of f by c. multiplying the y-values. even-degree polynomial. graph goes up on both sides
Reference 1: Transformations of Graphs an En Behavior of Polynomial Graphs Transformations of graphs aitive constant constant on the outsie g(x) = + c Make graph of g by aing c to the y-values on the graph
More informationTopic 7: Convergence of Random Variables
Topic 7: Convergence of Ranom Variables Course 003, 2016 Page 0 The Inference Problem So far, our starting point has been a given probability space (S, F, P). We now look at how to generate information
More informationFinal Exam Study Guide and Practice Problems Solutions
Final Exam Stuy Guie an Practice Problems Solutions Note: These problems are just some of the types of problems that might appear on the exam. However, to fully prepare for the exam, in aition to making
More informationSolutions to Math 41 Second Exam November 4, 2010
Solutions to Math 41 Secon Exam November 4, 2010 1. (13 points) Differentiate, using the metho of your choice. (a) p(t) = ln(sec t + tan t) + log 2 (2 + t) (4 points) Using the rule for the erivative of
More informationLagrangian and Hamiltonian Mechanics
Lagrangian an Hamiltonian Mechanics.G. Simpson, Ph.. epartment of Physical Sciences an Engineering Prince George s Community College ecember 5, 007 Introuction In this course we have been stuying classical
More informationMath 342 Partial Differential Equations «Viktor Grigoryan
Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite
More information1 Lecture 13: The derivative as a function.
1 Lecture 13: Te erivative as a function. 1.1 Outline Definition of te erivative as a function. efinitions of ifferentiability. Power rule, erivative te exponential function Derivative of a sum an a multiple
More informationConvergence of Random Walks
Chapter 16 Convergence of Ranom Walks This lecture examines the convergence of ranom walks to the Wiener process. This is very important both physically an statistically, an illustrates the utility of
More informationNOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy,
NOTES ON EULER-BOOLE SUMMATION JONATHAN M BORWEIN, NEIL J CALKIN, AND DANTE MANNA Abstract We stuy a connection between Euler-MacLaurin Summation an Boole Summation suggeste in an AMM note from 196, which
More informationYou should also review L Hôpital s Rule, section 3.6; follow the homework link above for exercises.
BEFORE You Begin Calculus II If it has been awhile since you ha Calculus, I strongly suggest that you refresh both your ifferentiation an integration skills. I woul also like to remin you that in Calculus,
More information3.6. Let s write out the sample space for this random experiment:
STAT 5 3 Let s write out the sample space for this ranom experiment: S = {(, 2), (, 3), (, 4), (, 5), (2, 3), (2, 4), (2, 5), (3, 4), (3, 5), (4, 5)} This sample space assumes the orering of the balls
More informationExistence of equilibria in articulated bearings in presence of cavity
J. Math. Anal. Appl. 335 2007) 841 859 www.elsevier.com/locate/jmaa Existence of equilibria in articulate bearings in presence of cavity G. Buscaglia a, I. Ciuperca b, I. Hafii c,m.jai c, a Centro Atómico
More informationMath Chapter 2 Essentials of Calculus by James Stewart Prepared by Jason Gaddis
Math 231 - Chapter 2 Essentials of Calculus by James Stewart Prepare by Jason Gais Chapter 2 - Derivatives 21 - Derivatives an Rates of Change Definition A tangent to a curve is a line that intersects
More information12.11 Laplace s Equation in Cylindrical and
SEC. 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential 593 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential One of the most important PDEs in physics an engineering
More informationExam 2 Review Solutions
Exam Review Solutions 1. True or False, an explain: (a) There exists a function f with continuous secon partial erivatives such that f x (x, y) = x + y f y = x y False. If the function has continuous secon
More informationLecture 5: Moment generating functions
Lecture 5: Moment generating functions Definition 2.3.6. The moment generating function (mgf) of a random variable X is { x e tx f M X (t) = E(e tx X (x) if X has a pmf ) = etx f X (x)dx if X has a pdf
More information1 Heisenberg Representation
1 Heisenberg Representation What we have been ealing with so far is calle the Schröinger representation. In this representation, operators are constants an all the time epenence is carrie by the states.
More informationFall 2016: Calculus I Final
Answer the questions in the spaces provie on the question sheets. If you run out of room for an answer, continue on the back of the page. NO calculators or other electronic evices, books or notes are allowe
More informationStep 1. Analytic Properties of the Riemann zeta function [2 lectures]
Step. Analytic Properties of the Riemann zeta function [2 lectures] The Riemann zeta function is the infinite sum of terms /, n. For each n, the / is a continuous function of s, i.e. lim s s 0 n = s n,
More informationCHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold
CHAPTER 1 : DIFFERENTIABLE MANIFOLDS 1.1 The efinition of a ifferentiable manifol Let M be a topological space. This means that we have a family Ω of open sets efine on M. These satisfy (1), M Ω (2) the
More information1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7.
Lectures Nine an Ten The WKB Approximation The WKB metho is a powerful tool to obtain solutions for many physical problems It is generally applicable to problems of wave propagation in which the frequency
More informationarxiv:math/ v1 [math.pr] 19 Apr 2001
Conitional Expectation as Quantile Derivative arxiv:math/00490v math.pr 9 Apr 200 Dirk Tasche November 3, 2000 Abstract For a linear combination u j X j of ranom variables, we are intereste in the partial
More informationJUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson
JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises
More informationEuler equations for multiple integrals
Euler equations for multiple integrals January 22, 2013 Contents 1 Reminer of multivariable calculus 2 1.1 Vector ifferentiation......................... 2 1.2 Matrix ifferentiation........................
More informationQF101: Quantitative Finance September 5, Week 3: Derivatives. Facilitator: Christopher Ting AY 2017/2018. f ( x + ) f(x) f(x) = lim
QF101: Quantitative Finance September 5, 2017 Week 3: Derivatives Facilitator: Christopher Ting AY 2017/2018 I recoil with ismay an horror at this lamentable plague of functions which o not have erivatives.
More informationConsistency and asymptotic normality
Consistency an asymtotic normality Class notes for Econ 842 Robert e Jong March 2006 1 Stochastic convergence The asymtotic theory of minimization estimators relies on various theorems from mathematical
More informationLectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs
Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent
More informationELEC3114 Control Systems 1
ELEC34 Control Systems Linear Systems - Moelling - Some Issues Session 2, 2007 Introuction Linear systems may be represente in a number of ifferent ways. Figure shows the relationship between various representations.
More informationCalculus in the AP Physics C Course The Derivative
Limits an Derivatives Calculus in the AP Physics C Course The Derivative In physics, the ieas of the rate change of a quantity (along with the slope of a tangent line) an the area uner a curve are essential.
More informationFinal Exam: Sat 12 Dec 2009, 09:00-12:00
MATH 1013 SECTIONS A: Professor Szeptycki APPLIED CALCULUS I, FALL 009 B: Professor Toms C: Professor Szeto NAME: STUDENT #: SECTION: No ai (e.g. calculator, written notes) is allowe. Final Exam: Sat 1
More informationMath 1271 Solutions for Fall 2005 Final Exam
Math 7 Solutions for Fall 5 Final Eam ) Since the equation + y = e y cannot be rearrange algebraically in orer to write y as an eplicit function of, we must instea ifferentiate this relation implicitly
More informationFebruary 21 Math 1190 sec. 63 Spring 2017
February 21 Math 1190 sec. 63 Spring 2017 Chapter 2: Derivatives Let s recall the efinitions an erivative rules we have so far: Let s assume that y = f (x) is a function with c in it s omain. The erivative
More informationRules of Differentiation. Lecture 12. Product and Quotient Rules.
Rules of Differentiation. Lecture 12. Prouct an Quotient Rules. We warne earlier that we can not calculate the erivative of a prouct as the prouct of the erivatives. It is easy to see that this is so.
More informationPartial Differential Equations
Chapter Partial Differential Equations. Introuction Have solve orinary ifferential equations, i.e. ones where there is one inepenent an one epenent variable. Only orinary ifferentiation is therefore involve.
More informationSeparation of Variables
Physics 342 Lecture 1 Separation of Variables Lecture 1 Physics 342 Quantum Mechanics I Monay, January 25th, 2010 There are three basic mathematical tools we nee, an then we can begin working on the physical
More informationNotes on Lie Groups, Lie algebras, and the Exponentiation Map Mitchell Faulk
Notes on Lie Groups, Lie algebras, an the Exponentiation Map Mitchell Faulk 1. Preliminaries. In these notes, we concern ourselves with special objects calle matrix Lie groups an their corresponing Lie
More informationMath 190 Chapter 3 Lecture Notes. Professor Miguel Ornelas
Math 190 Chapter 3 Lecture Notes Professor Miguel Ornelas 1 M. Ornelas Math 190 Lecture Notes Section 3.1 Section 3.1 Derivatives of Polynomials an Exponential Functions Derivative of a Constant Function
More information1 Math 285 Homework Problem List for S2016
1 Math 85 Homework Problem List for S016 Note: solutions to Lawler Problems will appear after all of the Lecture Note Solutions. 1.1 Homework 1. Due Friay, April 8, 016 Look at from lecture note exercises:
More informationx = c of N if the limit of f (x) = L and the right-handed limit lim f ( x)
Limit We say the limit of f () as approaches c equals L an write, lim L. One-Sie Limits (Left an Right-Hane Limits) Suppose a function f is efine near but not necessarily at We say that f has a left-hane
More informationThe Exact Form and General Integrating Factors
7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily
More informationExtreme Values by Resnick
1 Extreme Values by Resnick 1 Preliminaries 1.1 Uniform Convergence We will evelop the iea of something calle continuous convergence which will be useful to us later on. Denition 1. Let X an Y be metric
More informationSchrödinger s equation.
Physics 342 Lecture 5 Schröinger s Equation Lecture 5 Physics 342 Quantum Mechanics I Wenesay, February 3r, 2010 Toay we iscuss Schröinger s equation an show that it supports the basic interpretation of
More informationClosed and Open Loop Optimal Control of Buffer and Energy of a Wireless Device
Close an Open Loop Optimal Control of Buffer an Energy of a Wireless Device V. S. Borkar School of Technology an Computer Science TIFR, umbai, Inia. borkar@tifr.res.in A. A. Kherani B. J. Prabhu INRIA
More informationMath 115 Section 018 Course Note
Course Note 1 General Functions Definition 1.1. A function is a rule that takes certain numbers as inputs an assigns to each a efinite output number. The set of all input numbers is calle the omain of
More informationLimits at Infinity. Horizontal Asymptotes. Definition (Limits at Infinity) Horizontal Asymptotes
Limits at Infinity If a function f has a domain that is unbounded, that is, one of the endpoints of its domain is ±, we can determine the long term behavior of the function using a it at infinity. Definition
More informationLower Bounds for the Smoothed Number of Pareto optimal Solutions
Lower Bouns for the Smoothe Number of Pareto optimal Solutions Tobias Brunsch an Heiko Röglin Department of Computer Science, University of Bonn, Germany brunsch@cs.uni-bonn.e, heiko@roeglin.org Abstract.
More information1 Definition of the derivative
Math 20A - Calculus by Jon Rogawski Chapter 3 - Differentiation Prepare by Jason Gais Definition of the erivative Remark.. Recall our iscussion of tangent lines from way back. We now rephrase this in terms
More informationConvergence of random variables, and the Borel-Cantelli lemmas
Stat 205A Setember, 12, 2002 Convergence of ranom variables, an the Borel-Cantelli lemmas Lecturer: James W. Pitman Scribes: Jin Kim (jin@eecs) 1 Convergence of ranom variables Recall that, given a sequence
More informationProof of SPNs as Mixture of Trees
A Proof of SPNs as Mixture of Trees Theorem 1. If T is an inuce SPN from a complete an ecomposable SPN S, then T is a tree that is complete an ecomposable. Proof. Argue by contraiction that T is not a
More informationLaplace s Equation in Cylindrical Coordinates and Bessel s Equation (II)
Laplace s Equation in Cylinrical Coorinates an Bessel s Equation (II Qualitative properties of Bessel functions of first an secon kin In the last lecture we foun the expression for the general solution
More informationPDE Notes, Lecture #11
PDE Notes, Lecture # from Professor Jalal Shatah s Lectures Febuary 9th, 2009 Sobolev Spaces Recall that for u L loc we can efine the weak erivative Du by Du, φ := udφ φ C0 If v L loc such that Du, φ =
More informationJointly continuous distributions and the multivariate Normal
Jointly continuous istributions an the multivariate Normal Márton alázs an álint Tóth October 3, 04 This little write-up is part of important founations of probability that were left out of the unit Probability
More informationThe derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)
Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)
More informationStudents need encouragement. So if a student gets an answer right, tell them it was a lucky guess. That way, they develop a good, lucky feeling.
Chapter 8 Analytic Functions Stuents nee encouragement. So if a stuent gets an answer right, tell them it was a lucky guess. That way, they evelop a goo, lucky feeling. 1 8.1 Complex Derivatives -Jack
More informationImplicit Differentiation. Lecture 16.
Implicit Differentiation. Lecture 16. We are use to working only with functions that are efine explicitly. That is, ones like f(x) = 5x 3 + 7x x 2 + 1 or s(t) = e t5 3, in which the function is escribe
More informationMATH 1300 Lecture Notes Wednesday, September 25, 2013
MATH 300 Lecture Notes Wenesay, September 25, 203. Section 3. of HH - Powers an Polynomials In this section 3., you are given several ifferentiation rules that, taken altogether, allow you to quickly an
More informationSwitching Time Optimization in Discretized Hybrid Dynamical Systems
Switching Time Optimization in Discretize Hybri Dynamical Systems Kathrin Flaßkamp, To Murphey, an Sina Ober-Blöbaum Abstract Switching time optimization (STO) arises in systems that have a finite set
More informationIEOR 3106: Introduction to Operations Research: Stochastic Models. Fall 2011, Professor Whitt. Class Lecture Notes: Thursday, September 15.
IEOR 3106: Introduction to Operations Research: Stochastic Models Fall 2011, Professor Whitt Class Lecture Notes: Thursday, September 15. Random Variables, Conditional Expectation and Transforms 1. Random
More informationIPA Derivatives for Make-to-Stock Production-Inventory Systems With Backorders Under the (R,r) Policy
IPA Derivatives for Make-to-Stock Prouction-Inventory Systems With Backorers Uner the (Rr) Policy Yihong Fan a Benamin Melame b Yao Zhao c Yorai Wari Abstract This paper aresses Infinitesimal Perturbation
More information3.7 Implicit Differentiation -- A Brief Introduction -- Student Notes
Fin these erivatives of these functions: y.7 Implicit Differentiation -- A Brief Introuction -- Stuent Notes tan y sin tan = sin y e = e = Write the inverses of these functions: y tan y sin How woul we
More information13.1: Vector-Valued Functions and Motion in Space, 14.1: Functions of Several Variables, and 14.2: Limits and Continuity in Higher Dimensions
13.1: Vector-Value Functions an Motion in Space, 14.1: Functions of Several Variables, an 14.2: Limits an Continuity in Higher Dimensions TA: Sam Fleischer November 3 Section 13.1: Vector-Value Functions
More information1 Lecture 18: The chain rule
1 Lecture 18: The chain rule 1.1 Outline Comparing the graphs of sin(x) an sin(2x). The chain rule. The erivative of a x. Some examples. 1.2 Comparing the graphs of sin(x) an sin(2x) We graph f(x) = sin(x)
More informationP(x) = 1 + x n. (20.11) n n φ n(x) = exp(x) = lim φ (x) (20.8) Our first task for the chain rule is to find the derivative of the exponential
20. Derivatives of compositions: the chain rule At the en of the last lecture we iscovere a nee for the erivative of a composition. In this lecture we show how to calculate it. Accoringly, let P have omain
More informationSOME LYAPUNOV TYPE POSITIVE OPERATORS ON ORDERED BANACH SPACES
Ann. Aca. Rom. Sci. Ser. Math. Appl. ISSN 2066-6594 Vol. 5, No. 1-2 / 2013 SOME LYAPUNOV TYPE POSITIVE OPERATORS ON ORDERED BANACH SPACES Vasile Dragan Toaer Morozan Viorica Ungureanu Abstract In this
More information0.1 The Chain Rule. db dt = db
0. The Chain Rule A basic illustration of the chain rules comes in thinking about runners in a race. Suppose two brothers, Mark an Brian, hol an annual race to see who is the fastest. Last year Mark won
More information0.1 Differentiation Rules
0.1 Differentiation Rules From our previous work we ve seen tat it can be quite a task to calculate te erivative of an arbitrary function. Just working wit a secon-orer polynomial tings get pretty complicate
More informationLinear First-Order Equations
5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)
More informationAdvanced Partial Differential Equations with Applications
MIT OpenCourseWare http://ocw.mit.eu 18.306 Avance Partial Differential Equations with Applications Fall 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.eu/terms.
More informationMath 1B, lecture 8: Integration by parts
Math B, lecture 8: Integration by parts Nathan Pflueger 23 September 2 Introuction Integration by parts, similarly to integration by substitution, reverses a well-known technique of ifferentiation an explores
More informationARAB ACADEMY FOR SCIENCE TECHNOLOGY AND MARITIME TRANSPORT
ARAB ACADEMY FOR SCIENCE TECHNOLOGY AND MARITIME TRANSPORT Course: Math For Engineering Winter 8 Lecture Notes By Dr. Mostafa Elogail Page Lecture [ Functions / Graphs of Rational Functions] Functions
More informationImplicit Differentiation
Implicit Differentiation Implicit Differentiation Using the Chain Rule In the previous section we focuse on the erivatives of composites an saw that THEOREM 20 (Chain Rule) Suppose that u = g(x) is ifferentiable
More informationUnit #6 - Families of Functions, Taylor Polynomials, l Hopital s Rule
Unit # - Families of Functions, Taylor Polynomials, l Hopital s Rule Some problems an solutions selecte or aapte from Hughes-Hallett Calculus. Critical Points. Consier the function f) = 54 +. b) a) Fin
More informationd dx [xn ] = nx n 1. (1) dy dx = 4x4 1 = 4x 3. Theorem 1.3 (Derivative of a constant function). If f(x) = k and k is a constant, then f (x) = 0.
Calculus refresher Disclaimer: I claim no original content on this ocument, which is mostly a summary-rewrite of what any stanar college calculus book offers. (Here I ve use Calculus by Dennis Zill.) I
More information2.20 Marine Hydrodynamics Lecture 3
2.20 Marine Hyroynamics, Fall 2018 Lecture 3 Copyright c 2018 MIT - Department of Mechanical Engineering, All rights reserve. 1.7 Stress Tensor 2.20 Marine Hyroynamics Lecture 3 1.7.1 Stress Tensor τ ij
More informationALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS
ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS MARK SCHACHNER Abstract. When consiere as an algebraic space, the set of arithmetic functions equippe with the operations of pointwise aition an
More informationQuantum Mechanics in Three Dimensions
Physics 342 Lecture 20 Quantum Mechanics in Three Dimensions Lecture 20 Physics 342 Quantum Mechanics I Monay, March 24th, 2008 We begin our spherical solutions with the simplest possible case zero potential.
More informationSome Examples. Uniform motion. Poisson processes on the real line
Some Examples Our immeiate goal is to see some examples of Lévy processes, an/or infinitely-ivisible laws on. Uniform motion Choose an fix a nonranom an efine X := for all (1) Then, {X } is a [nonranom]
More informationUC Berkeley Department of Electrical Engineering and Computer Science Department of Statistics
UC Berkeley Department of Electrical Engineering an Computer Science Department of Statistics EECS 8B / STAT 4B Avance Topics in Statistical Learning Theory Solutions 3 Spring 9 Solution 3. For parti,
More informationComputing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions
Working Paper 2013:5 Department of Statistics Computing Exact Confience Coefficients of Simultaneous Confience Intervals for Multinomial Proportions an their Functions Shaobo Jin Working Paper 2013:5
More informationBy writing (1) as y (x 5 1). (x 5 1), we can find the derivative using the Product Rule: y (x 5 1) 2. we know this from (2)
3.5 Chain Rule 149 3.5 Chain Rule Introuction As iscusse in Section 3.2, the Power Rule is vali for all real number exponents n. In this section we see that a similar rule hols for the erivative of a power
More informationLecture 2 Lagrangian formulation of classical mechanics Mechanics
Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,
More informationSYDE 112, LECTURE 1: Review & Antidifferentiation
SYDE 112, LECTURE 1: Review & Antiifferentiation 1 Course Information For a etaile breakown of the course content an available resources, see the Course Outline. Other relevant information for this section
More informationDynamics of the synchronous machine
ELEC0047 - Power system ynamics, control an stability Dynamics of the synchronous machine Thierry Van Cutsem t.vancutsem@ulg.ac.be www.montefiore.ulg.ac.be/~vct These slies follow those presente in course
More informationImplicit Differentiation
Implicit Differentiation Thus far, the functions we have been concerne with have been efine explicitly. A function is efine explicitly if the output is given irectly in terms of the input. For instance,
More informationChapter 4. Continuous Random Variables 4.1 PDF
Chapter 4 Continuous Random Variables In this chapter we study continuous random variables. The linkage between continuous and discrete random variables is the cumulative distribution (CDF) which we will
More information1.2 - Stress Tensor Marine Hydrodynamics Lecture 3
13.021 Marine Hyroynamics, Fall 2004 Lecture 3 Copyright c 2004 MIT - Department of Ocean Engineering, All rights reserve. 1.2 - Stress Tensor 13.021 Marine Hyroynamics Lecture 3 Stress Tensor τ ij:. The
More informationIntroduction to the Vlasov-Poisson system
Introuction to the Vlasov-Poisson system Simone Calogero 1 The Vlasov equation Consier a particle with mass m > 0. Let x(t) R 3 enote the position of the particle at time t R an v(t) = ẋ(t) = x(t)/t its
More informationLie symmetry and Mei conservation law of continuum system
Chin. Phys. B Vol. 20, No. 2 20 020 Lie symmetry an Mei conservation law of continuum system Shi Shen-Yang an Fu Jing-Li Department of Physics, Zhejiang Sci-Tech University, Hangzhou 3008, China Receive
More informationLecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012
CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration
More informationLecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations
Lecture XII Abstract We introuce the Laplace equation in spherical coorinates an apply the metho of separation of variables to solve it. This will generate three linear orinary secon orer ifferential equations:
More informationMonte Carlo Methods with Reduced Error
Monte Carlo Methos with Reuce Error As has been shown, the probable error in Monte Carlo algorithms when no information about the smoothness of the function is use is Dξ r N = c N. It is important for
More informationthe convolution of f and g) given by
09:53 /5/2000 TOPIC Characteristic functions, cont d This lecture develops an inversion formula for recovering the density of a smooth random variable X from its characteristic function, and uses that
More informationCOUPLING REQUIREMENTS FOR WELL POSED AND STABLE MULTI-PHYSICS PROBLEMS
VI International Conference on Computational Methos for Couple Problems in Science an Engineering COUPLED PROBLEMS 15 B. Schrefler, E. Oñate an M. Paparakakis(Es) COUPLING REQUIREMENTS FOR WELL POSED AND
More informationSome functions and their derivatives
Chapter Some functions an their erivatives. Derivative of x n for integer n Recall, from eqn (.6), for y = f (x), Also recall that, for integer n, Hence, if y = x n then y x = lim δx 0 (a + b) n = a n
More informationTime-of-Arrival Estimation in Non-Line-Of-Sight Environments
2 Conference on Information Sciences an Systems, The Johns Hopkins University, March 2, 2 Time-of-Arrival Estimation in Non-Line-Of-Sight Environments Sinan Gezici, Hisashi Kobayashi an H. Vincent Poor
More information6 General properties of an autonomous system of two first order ODE
6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x
More information4. Important theorems in quantum mechanics
TFY4215 Kjemisk fysikk og kvantemekanikk - Tillegg 4 1 TILLEGG 4 4. Important theorems in quantum mechanics Before attacking three-imensional potentials in the next chapter, we shall in chapter 4 of this
More informationYORK UNIVERSITY. Faculty of Science Department of Mathematics and Statistics. MATH A Test #2. June 25, 2014 SOLUTIONS
YORK UNIVERSITY Faculty of Science Department of Mathematics an Statistics MATH 505 6.00 A Test # June 5, 04 SOLUTIONS Family Name (print): Given Name: Stuent No: Signature: INSTRUCTIONS:. Please write
More information