Lecture 7: Interchange of integration and limit

Size: px
Start display at page:

Download "Lecture 7: Interchange of integration and limit"

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 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 information

Make 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

Make 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 information

Topic 7: Convergence of Random Variables

Topic 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 information

Final Exam Study Guide and Practice Problems Solutions

Final 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 information

Solutions to Math 41 Second Exam November 4, 2010

Solutions 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 information

Lagrangian and Hamiltonian Mechanics

Lagrangian 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 information

Math 342 Partial Differential Equations «Viktor Grigoryan

Math 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 information

1 Lecture 13: The derivative as a function.

1 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 information

Convergence of Random Walks

Convergence 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 information

NOTES 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 (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 information

You should also review L Hôpital s Rule, section 3.6; follow the homework link above for exercises.

You 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 information

3.6. Let s write out the sample space for this random experiment:

3.6. 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 information

Existence of equilibria in articulated bearings in presence of cavity

Existence 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 information

Math Chapter 2 Essentials of Calculus by James Stewart Prepared by Jason Gaddis

Math 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 information

12.11 Laplace s Equation in Cylindrical and

12.11 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 information

Exam 2 Review Solutions

Exam 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 information

Lecture 5: Moment generating functions

Lecture 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 information

1 Heisenberg Representation

1 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 information

Fall 2016: Calculus I Final

Fall 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 information

Step 1. Analytic Properties of the Riemann zeta function [2 lectures]

Step 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 information

CHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold

CHAPTER 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 information

1 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.

1 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 information

arxiv:math/ v1 [math.pr] 19 Apr 2001

arxiv: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 information

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson

JUST 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 information

Euler equations for multiple integrals

Euler 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 information

QF101: 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, 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 information

Consistency and asymptotic normality

Consistency 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 information

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs

Lectures - 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 information

ELEC3114 Control Systems 1

ELEC3114 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 information

Calculus in the AP Physics C Course The Derivative

Calculus 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 information

Final Exam: Sat 12 Dec 2009, 09:00-12:00

Final 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 information

Math 1271 Solutions for Fall 2005 Final Exam

Math 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 information

February 21 Math 1190 sec. 63 Spring 2017

February 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 information

Rules of Differentiation. Lecture 12. Product and Quotient Rules.

Rules 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 information

Partial Differential Equations

Partial 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 information

Separation of Variables

Separation 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 information

Notes on Lie Groups, Lie algebras, and the Exponentiation Map Mitchell Faulk

Notes 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 information

Math 190 Chapter 3 Lecture Notes. Professor Miguel Ornelas

Math 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 information

1 Math 285 Homework Problem List for S2016

1 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 information

x = c of N if the limit of f (x) = L and the right-handed limit lim f ( x)

x = 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 information

The Exact Form and General Integrating Factors

The 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 information

Extreme Values by Resnick

Extreme 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 information

Schrödinger s equation.

Schrödinger 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 information

Closed and Open Loop Optimal Control of Buffer and Energy of a Wireless Device

Closed 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 information

Math 115 Section 018 Course Note

Math 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 information

Limits at Infinity. Horizontal Asymptotes. Definition (Limits at Infinity) Horizontal Asymptotes

Limits 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 information

Lower Bounds for the Smoothed Number of Pareto optimal Solutions

Lower 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 information

1 Definition of the derivative

1 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 information

Convergence of random variables, and the Borel-Cantelli lemmas

Convergence 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 information

Proof of SPNs as Mixture of Trees

Proof 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 information

Laplace s Equation in Cylindrical Coordinates and Bessel s Equation (II)

Laplace 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 information

PDE Notes, Lecture #11

PDE 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 information

Jointly continuous distributions and the multivariate Normal

Jointly 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 information

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)

The 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 information

Students 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.

Students 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 information

Implicit Differentiation. Lecture 16.

Implicit 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 information

MATH 1300 Lecture Notes Wednesday, September 25, 2013

MATH 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 information

Switching Time Optimization in Discretized Hybrid Dynamical Systems

Switching 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 information

IEOR 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. 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 information

IPA Derivatives for Make-to-Stock Production-Inventory Systems With Backorders Under the (R,r) Policy

IPA 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 information

3.7 Implicit Differentiation -- A Brief Introduction -- Student Notes

3.7 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 information

13.1: 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-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 information

1 Lecture 18: The chain rule

1 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 information

P(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

P(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 information

SOME LYAPUNOV TYPE POSITIVE OPERATORS ON ORDERED BANACH SPACES

SOME 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 information

0.1 The Chain Rule. db dt = db

0.1 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 information

0.1 Differentiation Rules

0.1 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 information

Linear First-Order Equations

Linear 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 information

Advanced Partial Differential Equations with Applications

Advanced 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 information

Math 1B, lecture 8: Integration by parts

Math 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 information

ARAB ACADEMY FOR SCIENCE TECHNOLOGY AND MARITIME TRANSPORT

ARAB 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 information

Implicit Differentiation

Implicit 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 information

Unit #6 - Families of Functions, Taylor Polynomials, l Hopital s Rule

Unit #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 information

d 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.

d 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 information

2.20 Marine Hydrodynamics Lecture 3

2.20 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 information

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS

ALGEBRAIC 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 information

Quantum Mechanics in Three Dimensions

Quantum 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 information

Some Examples. Uniform motion. Poisson processes on the real line

Some 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 information

UC Berkeley Department of Electrical Engineering and Computer Science Department of Statistics

UC 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 information

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions

Computing 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 information

By 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)

By 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 information

Lecture 2 Lagrangian formulation of classical mechanics Mechanics

Lecture 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 information

SYDE 112, LECTURE 1: Review & Antidifferentiation

SYDE 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 information

Dynamics of the synchronous machine

Dynamics 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 information

Implicit Differentiation

Implicit 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 information

Chapter 4. Continuous Random Variables 4.1 PDF

Chapter 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 information

1.2 - Stress Tensor Marine Hydrodynamics Lecture 3

1.2 - 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 information

Introduction to the Vlasov-Poisson system

Introduction 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 information

Lie symmetry and Mei conservation law of continuum system

Lie 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 information

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012

Lecture 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 information

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations

Lecture 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 information

Monte Carlo Methods with Reduced Error

Monte 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 information

the convolution of f and g) given by

the 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 information

COUPLING REQUIREMENTS FOR WELL POSED AND STABLE MULTI-PHYSICS PROBLEMS

COUPLING 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 information

Some functions and their derivatives

Some 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 information

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments

Time-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 information

6 General properties of an autonomous system of two first order ODE

6 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 information

4. Important theorems in quantum mechanics

4. 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 information

YORK 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 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