IFT 6085 - Lecture 2 Basics of Convex Analysis and Gradient Descent
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
4. Convex Optimization Problems
Convex Optimization — Boyd & Vandenberghe 4. Convex optimization problems optimization problem in standard form • convex optimization problems • quasiconvex optimization • linear optimization • quadratic optimization • geometric programming • generalized inequality constraints • semidefinite programming • vector optimization • 4–1 Optimization problem in standard form minimize f0(x) subject to f (x) 0, i =1,...,m i ≤ hi(x)=0, i =1,...,p x Rn is the optimization variable • ∈ f : Rn R is the objective or cost function • 0 → f : Rn R, i =1,...,m, are the inequality constraint functions • i → h : Rn R are the equality constraint functions • i → optimal value: p⋆ = inf f (x) f (x) 0, i =1,...,m, h (x)=0, i =1,...,p { 0 | i ≤ i } p⋆ = if problem is infeasible (no x satisfies the constraints) • ∞ p⋆ = if problem is unbounded below • −∞ Convex optimization problems 4–2 Optimal and locally optimal points x is feasible if x dom f and it satisfies the constraints ∈ 0 ⋆ a feasible x is optimal if f0(x)= p ; Xopt is the set of optimal points x is locally optimal if there is an R> 0 such that x is optimal for minimize (over z) f0(z) subject to fi(z) 0, i =1,...,m, hi(z)=0, i =1,...,p z x≤ R k − k2 ≤ examples (with n =1, m = p =0) f (x)=1/x, dom f = R : p⋆ =0, no optimal point • 0 0 ++ f (x)= log x, dom f = R : p⋆ = • 0 − 0 ++ −∞ f (x)= x log x, dom f = R : p⋆ = 1/e, x =1/e is optimal • 0 0 ++ − f (x)= x3 3x, p⋆ = , local optimum at x =1 • 0 − −∞ Convex optimization problems 4–3 Implicit constraints the standard form optimization problem has an implicit -
Section 8.8: Improper Integrals
Section 8.8: Improper Integrals One of the main applications of integrals is to compute the areas under curves, as you know. A geometric question. But there are some geometric questions which we do not yet know how to do by calculus, even though they appear to have the same form. Consider the curve y = 1=x2. We can ask, what is the area of the region under the curve and right of the line x = 1? We have no reason to believe this area is finite, but let's ask. Now no integral will compute this{we have to integrate over a bounded interval. Nonetheless, we don't want to throw up our hands. So note that b 2 b Z (1=x )dx = ( 1=x) 1 = 1 1=b: 1 − j − In other words, as b gets larger and larger, the area under the curve and above [1; b] gets larger and larger; but note that it gets closer and closer to 1. Thus, our intuition tells us that the area of the region we're interested in is exactly 1. More formally: lim 1 1=b = 1: b − !1 We can rewrite that as b 2 lim Z (1=x )dx: b !1 1 Indeed, in general, if we want to compute the area under y = f(x) and right of the line x = a, we are computing b lim Z f(x)dx: b !1 a ASK: Does this limit always exist? Give some situations where it does not exist. They'll give something that blows up. -
Convex Optimisation Matlab Toolbox
UNLOCBOX: USER’S GUIDE MATLAB CONVEX OPTIMIZATION TOOLBOX Lausanne - February 2014 PERRAUDIN Nathanaël, KALOFOLIAS Vassilis LTS2 - EPFL Abstract Nowadays the trend to solve optimization problems is to use specific algorithms rather than very gen- eral ones. The UNLocBoX provides a general framework allowing the user to design his own algorithms. To do so, the framework try to stay as close from the mathematical problem as possible. More precisely, the UNLocBoX is a Matlab toolbox designed to solve convex optimization problem of the form K min ∑ fn(x); x2C n=1 using proximal splitting techniques. It is mainly composed of solvers, proximal operators and demonstra- tion files allowing the user to quickly implement a problem. Contents 1 Introduction 1 2 Literature 2 3 Installation and initialization2 3.1 Dependencies.........................................2 3.2 GPU computation.......................................2 4 Structure of the UNLocBoX2 5 Problems of interest4 6 Solvers 4 6.1 Defining functions......................................5 6.2 Selecting a solver.......................................5 6.3 Optional parameters......................................6 6.4 Plug-ins: how to tune your algorithm.............................6 6.5 Returned arguments......................................8 7 Proximal operators9 7.1 Constraints..........................................9 8 Example 10 References 16 LTS2 - EPFL 1 Introduction During your research, you have most likely faced the situation where you need to solve a convex optimiza- tion problem. Maybe you were trying to find an optimal combination of parameters, you were transforming some process into something automatic or, even more simply, your algorithm was equivalent to solving convex problem. In this situation, you usually face a dilemma: you need a specific algorithm to solve your problem, but you do not want to spend hours writing it. -
Notes on Calculus II Integral Calculus Miguel A. Lerma
Notes on Calculus II Integral Calculus Miguel A. Lerma November 22, 2002 Contents Introduction 5 Chapter 1. Integrals 6 1.1. Areas and Distances. The Definite Integral 6 1.2. The Evaluation Theorem 11 1.3. The Fundamental Theorem of Calculus 14 1.4. The Substitution Rule 16 1.5. Integration by Parts 21 1.6. Trigonometric Integrals and Trigonometric Substitutions 26 1.7. Partial Fractions 32 1.8. Integration using Tables and CAS 39 1.9. Numerical Integration 41 1.10. Improper Integrals 46 Chapter 2. Applications of Integration 50 2.1. More about Areas 50 2.2. Volumes 52 2.3. Arc Length, Parametric Curves 57 2.4. Average Value of a Function (Mean Value Theorem) 61 2.5. Applications to Physics and Engineering 63 2.6. Probability 69 Chapter 3. Differential Equations 74 3.1. Differential Equations and Separable Equations 74 3.2. Directional Fields and Euler’s Method 78 3.3. Exponential Growth and Decay 80 Chapter 4. Infinite Sequences and Series 83 4.1. Sequences 83 4.2. Series 88 4.3. The Integral and Comparison Tests 92 4.4. Other Convergence Tests 96 4.5. Power Series 98 4.6. Representation of Functions as Power Series 100 4.7. Taylor and MacLaurin Series 103 3 CONTENTS 4 4.8. Applications of Taylor Polynomials 109 Appendix A. Hyperbolic Functions 113 A.1. Hyperbolic Functions 113 Appendix B. Various Formulas 118 B.1. Summation Formulas 118 Appendix C. Table of Integrals 119 Introduction These notes are intended to be a summary of the main ideas in course MATH 214-2: Integral Calculus. -
Conditional Gradient Sliding for Convex Optimization ∗
CONDITIONAL GRADIENT SLIDING FOR CONVEX OPTIMIZATION ∗ GUANGHUI LAN y AND YI ZHOU z Abstract. In this paper, we present a new conditional gradient type method for convex optimization by calling a linear optimization (LO) oracle to minimize a series of linear functions over the feasible set. Different from the classic conditional gradient method, the conditional gradient sliding (CGS) algorithm developed herein can skip the computation of gradients from time to time, and as a result, can achieve the optimal complexity bounds in terms of not only the number of callsp to the LO oracle, but also the number of gradient evaluations. More specifically, we show that the CGS method requires O(1= ) and O(log(1/)) gradient evaluations, respectively, for solving smooth and strongly convex problems, while still maintaining the optimal O(1/) bound on the number of calls to LO oracle. We also develop variants of the CGS method which can achieve the optimal complexity bounds for solving stochastic optimization problems and an important class of saddle point optimization problems. To the best of our knowledge, this is the first time that these types of projection-free optimal first-order methods have been developed in the literature. Some preliminary numerical results have also been provided to demonstrate the advantages of the CGS method. Keywords: convex programming, complexity, conditional gradient method, Frank-Wolfe method, Nesterov's method AMS 2000 subject classification: 90C25, 90C06, 90C22, 49M37 1. Introduction. The conditional gradient (CndG) method, which was initially developed by Frank and Wolfe in 1956 [13] (see also [11, 12]), has been considered one of the earliest first-order methods for solving general convex programming (CP) problems. -
Two Fundamental Theorems About the Definite Integral
Two Fundamental Theorems about the Definite Integral These lecture notes develop the theorem Stewart calls The Fundamental Theorem of Calculus in section 5.3. The approach I use is slightly different than that used by Stewart, but is based on the same fundamental ideas. 1 The definite integral Recall that the expression b f(x) dx ∫a is called the definite integral of f(x) over the interval [a,b] and stands for the area underneath the curve y = f(x) over the interval [a,b] (with the understanding that areas above the x-axis are considered positive and the areas beneath the axis are considered negative). In today's lecture I am going to prove an important connection between the definite integral and the derivative and use that connection to compute the definite integral. The result that I am eventually going to prove sits at the end of a chain of earlier definitions and intermediate results. 2 Some important facts about continuous functions The first intermediate result we are going to have to prove along the way depends on some definitions and theorems concerning continuous functions. Here are those definitions and theorems. The definition of continuity A function f(x) is continuous at a point x = a if the following hold 1. f(a) exists 2. lim f(x) exists xœa 3. lim f(x) = f(a) xœa 1 A function f(x) is continuous in an interval [a,b] if it is continuous at every point in that interval. The extreme value theorem Let f(x) be a continuous function in an interval [a,b]. -
Lecture 13 Gradient Methods for Constrained Optimization
Lecture 13 Gradient Methods for Constrained Optimization October 16, 2008 Lecture 13 Outline • Gradient Projection Algorithm • Convergence Rate Convex Optimization 1 Lecture 13 Constrained Minimization minimize f(x) subject x ∈ X • Assumption 1: • The function f is convex and continuously differentiable over Rn • The set X is closed and convex ∗ • The optimal value f = infx∈Rn f(x) is finite • Gradient projection algorithm xk+1 = PX[xk − αk∇f(xk)] starting with x0 ∈ X. Convex Optimization 2 Lecture 13 Bounded Gradients Theorem 1 Let Assumption 1 hold, and suppose that the gradients are uniformly bounded over the set X. Then, the projection gradient method generates the sequence {xk} ⊂ X such that • When the constant stepsize αk ≡ α is used, we have 2 ∗ αL lim inf f(xk) ≤ f + k→∞ 2 P • When diminishing stepsize is used with k αk = +∞, we have ∗ lim inf f(xk) = f . k→∞ Proof: We use projection properties and the line of analysis similar to that of unconstrained method. HWK 6 Convex Optimization 3 Lecture 13 Lipschitz Gradients • Lipschitz Gradient Lemma For a differentiable convex function f with Lipschitz gradients, we have for all x, y ∈ Rn, 1 k∇f(x) − ∇f(y)k2 ≤ (∇f(x) − ∇f(y))T (x − y), L where L is a Lipschitz constant. • Theorem 2 Let Assumption 1 hold, and assume that the gradients of f are Lipschitz continuous over X. Suppose that the optimal solution ∗ set X is not empty. Then, for a constant stepsize αk ≡ α with 0 2 < α < L converges to an optimal point, i.e., ∗ ∗ ∗ lim kxk − x k = 0 for some x ∈ X . -
Calculus Terminology
AP Calculus BC Calculus Terminology Absolute Convergence Asymptote Continued Sum Absolute Maximum Average Rate of Change Continuous Function Absolute Minimum Average Value of a Function Continuously Differentiable Function Absolutely Convergent Axis of Rotation Converge Acceleration Boundary Value Problem Converge Absolutely Alternating Series Bounded Function Converge Conditionally Alternating Series Remainder Bounded Sequence Convergence Tests Alternating Series Test Bounds of Integration Convergent Sequence Analytic Methods Calculus Convergent Series Annulus Cartesian Form Critical Number Antiderivative of a Function Cavalieri’s Principle Critical Point Approximation by Differentials Center of Mass Formula Critical Value Arc Length of a Curve Centroid Curly d Area below a Curve Chain Rule Curve Area between Curves Comparison Test Curve Sketching Area of an Ellipse Concave Cusp Area of a Parabolic Segment Concave Down Cylindrical Shell Method Area under a Curve Concave Up Decreasing Function Area Using Parametric Equations Conditional Convergence Definite Integral Area Using Polar Coordinates Constant Term Definite Integral Rules Degenerate Divergent Series Function Operations Del Operator e Fundamental Theorem of Calculus Deleted Neighborhood Ellipsoid GLB Derivative End Behavior Global Maximum Derivative of a Power Series Essential Discontinuity Global Minimum Derivative Rules Explicit Differentiation Golden Spiral Difference Quotient Explicit Function Graphic Methods Differentiable Exponential Decay Greatest Lower Bound Differential -
The Infinite and Contradiction: a History of Mathematical Physics By
The infinite and contradiction: A history of mathematical physics by dialectical approach Ichiro Ueki January 18, 2021 Abstract The following hypothesis is proposed: \In mathematics, the contradiction involved in the de- velopment of human knowledge is included in the form of the infinite.” To prove this hypothesis, the author tries to find what sorts of the infinite in mathematics were used to represent the con- tradictions involved in some revolutions in mathematical physics, and concludes \the contradiction involved in mathematical description of motion was represented with the infinite within recursive (computable) set level by early Newtonian mechanics; and then the contradiction to describe discon- tinuous phenomena with continuous functions and contradictions about \ether" were represented with the infinite higher than the recursive set level, namely of arithmetical set level in second or- der arithmetic (ordinary mathematics), by mechanics of continuous bodies and field theory; and subsequently the contradiction appeared in macroscopic physics applied to microscopic phenomena were represented with the further higher infinite in third or higher order arithmetic (set-theoretic mathematics), by quantum mechanics". 1 Introduction Contradictions found in set theory from the end of the 19th century to the beginning of the 20th, gave a shock called \a crisis of mathematics" to the world of mathematicians. One of the contradictions was reported by B. Russel: \Let w be the class [set]1 of all classes which are not members of themselves. Then whatever class x may be, 'x is a w' is equivalent to 'x is not an x'. Hence, giving to x the value w, 'w is a w' is equivalent to 'w is not a w'."[52] Russel described the crisis in 1959: I was led to this contradiction by Cantor's proof that there is no greatest cardinal number. -
Additional Exercises for Convex Optimization
Additional Exercises for Convex Optimization Stephen Boyd Lieven Vandenberghe January 4, 2020 This is a collection of additional exercises, meant to supplement those found in the book Convex Optimization, by Stephen Boyd and Lieven Vandenberghe. These exercises were used in several courses on convex optimization, EE364a (Stanford), EE236b (UCLA), or 6.975 (MIT), usually for homework, but sometimes as exam questions. Some of the exercises were originally written for the book, but were removed at some point. Many of them include a computational component using one of the software packages for convex optimization: CVX (Matlab), CVXPY (Python), or Convex.jl (Julia). We refer to these collectively as CVX*. (Some problems have not yet been updated for all three languages.) The files required for these exercises can be found at the book web site www.stanford.edu/~boyd/cvxbook/. You are free to use these exercises any way you like (for example in a course you teach), provided you acknowledge the source. In turn, we gratefully acknowledge the teaching assistants (and in some cases, students) who have helped us develop and debug these exercises. Pablo Parrilo helped develop some of the exercises that were originally used in MIT 6.975, Sanjay Lall developed some other problems when he taught EE364a, and the instructors of EE364a during summer quarters developed others. We’ll update this document as new exercises become available, so the exercise numbers and sections will occasionally change. We have categorized the exercises into sections that follow the book chapters, as well as various additional application areas. Some exercises fit into more than one section, or don’t fit well into any section, so we have just arbitrarily assigned these. -
Efficient Convex Quadratic Optimization Solver for Embedded MPC Applications
DEGREE PROJECT IN ELECTRICAL ENGINEERING, SECOND CYCLE, 30 CREDITS STOCKHOLM, SWEDEN 2018 Efficient Convex Quadratic Optimization Solver for Embedded MPC Applications ALBERTO DÍAZ DORADO KTH ROYAL INSTITUTE OF TECHNOLOGY SCHOOL OF ELECTRICAL ENGINEERING AND COMPUTER SCIENCE Efficient Convex Quadratic Optimization Solver for Embedded MPC Applications ALBERTO DÍAZ DORADO Master in Electrical Engineering Date: October 2, 2018 Supervisor: Arda Aytekin , Martin Biel Examiner: Mikael Johansson Swedish title: Effektiv Konvex Kvadratisk Optimeringslösare för Inbäddade MPC-applikationer School of Electrical Engineering and Computer Science iii Abstract Model predictive control (MPC) is an advanced control technique that requires solving an optimization problem at each sampling instant. Sev- eral emerging applications require the use of short sampling times to cope with the fast dynamics of the underlying process. In many cases, these applications also need to be implemented on embedded hard- ware with limited resources. As a result, the use of model predictive controllers in these application domains remains challenging. This work deals with the implementation of an interior point algo- rithm for use in embedded MPC applications. We propose a modular software design that allows for high solver customization, while still producing compact and fast code. Our interior point method includes an efficient implementation of a novel approach to constraint softening, which has only been tested in high-level languages before. We show that a well conceived low-level implementation of integrated constraint softening adds no significant overhead to the solution time, and hence, constitutes an attractive alternative in embedded MPC solvers. iv Sammanfattning Modell prediktiv reglering (MPC) är en avancerad regler-teknik som involverar att lösa ett optimeringsproblem vid varje sampeltillfälle. -
1 Linear Programming
ORF 523 Lecture 9 Princeton University Instructor: A.A. Ahmadi Scribe: G. Hall Any typos should be emailed to a a [email protected]. In this lecture, we see some of the most well-known classes of convex optimization problems and some of their applications. These include: • Linear Programming (LP) • (Convex) Quadratic Programming (QP) • (Convex) Quadratically Constrained Quadratic Programming (QCQP) • Second Order Cone Programming (SOCP) • Semidefinite Programming (SDP) 1 Linear Programming Definition 1. A linear program (LP) is the problem of optimizing a linear function over a polyhedron: min cT x T s.t. ai x ≤ bi; i = 1; : : : ; m; or written more compactly as min cT x s.t. Ax ≤ b; for some A 2 Rm×n; b 2 Rm: We'll be very brief on our discussion of LPs since this is the central topic of ORF 522. It suffices to say that LPs probably still take the top spot in terms of ubiquity of applications. Here are a few examples: • A variety of problems in production planning and scheduling 1 • Exact formulation of several important combinatorial optimization problems (e.g., min-cut, shortest path, bipartite matching) • Relaxations for all 0/1 combinatorial programs • Subroutines of branch-and-bound algorithms for integer programming • Relaxations for cardinality constrained (compressed sensing type) optimization prob- lems • Computing Nash equilibria in zero-sum games • ::: 2 Quadratic Programming Definition 2. A quadratic program (QP) is an optimization problem with a quadratic ob- jective and linear constraints min xT Qx + qT x + c x s.t. Ax ≤ b: Here, we have Q 2 Sn×n, q 2 Rn; c 2 R;A 2 Rm×n; b 2 Rm: The difficulty of this problem changes drastically depending on whether Q is positive semidef- inite (psd) or not.