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An Analytic Exact Form of the Unit Step Function
Mathematics and Statistics 2(7): 235-237, 2014 http://www.hrpub.org DOI: 10.13189/ms.2014.020702 An Analytic Exact Form of the Unit Step Function J. Venetis Section of Mechanics, Faculty of Applied Mathematics and Physical Sciences, National Technical University of Athens *Corresponding Author: [email protected] Copyright © 2014 Horizon Research Publishing All rights reserved. Abstract In this paper, the author obtains an analytic Meanwhile, there are many smooth analytic exact form of the unit step function, which is also known as approximations to the unit step function as it can be seen in Heaviside function and constitutes a fundamental concept of the literature [4,5,6]. Besides, Sullivan et al [7] obtained a the Operational Calculus. Particularly, this function is linear algebraic approximation to this function by means of a equivalently expressed in a closed form as the summation of linear combination of exponential functions. two inverse trigonometric functions. The novelty of this However, the majority of all these approaches lead to work is that the exact representation which is proposed here closed – form representations consisting of non - elementary is not performed in terms of non – elementary special special functions, e.g. Logistic function, Hyperfunction, or functions, e.g. Dirac delta function or Error function and Error function and also most of its algebraic exact forms are also is neither the limit of a function, nor the limit of a expressed in terms generalized integrals or infinitesimal sequence of functions with point wise or uniform terms, something that complicates the related computational convergence. Therefore it may be much more appropriate in procedures. -
Mathematical Constants and Sequences
Mathematical Constants and Sequences a selection compiled by Stanislav Sýkora, Extra Byte, Castano Primo, Italy. Stan's Library, ISSN 2421-1230, Vol.II. First release March 31, 2008. Permalink via DOI: 10.3247/SL2Math08.001 This page is dedicated to my late math teacher Jaroslav Bayer who, back in 1955-8, kindled my passion for Mathematics. Math BOOKS | SI Units | SI Dimensions PHYSICS Constants (on a separate page) Mathematics LINKS | Stan's Library | Stan's HUB This is a constant-at-a-glance list. You can also download a PDF version for off-line use. But keep coming back, the list is growing! When a value is followed by #t, it should be a proven transcendental number (but I only did my best to find out, which need not suffice). Bold dots after a value are a link to the ••• OEIS ••• database. This website does not use any cookies, nor does it collect any information about its visitors (not even anonymous statistics). However, we decline any legal liability for typos, editing errors, and for the content of linked-to external web pages. Basic math constants Binary sequences Constants of number-theory functions More constants useful in Sciences Derived from the basic ones Combinatorial numbers, including Riemann zeta ζ(s) Planck's radiation law ... from 0 and 1 Binomial coefficients Dirichlet eta η(s) Functions sinc(z) and hsinc(z) ... from i Lah numbers Dedekind eta η(τ) Functions sinc(n,x) ... from 1 and i Stirling numbers Constants related to functions in C Ideal gas statistics ... from π Enumerations on sets Exponential exp Peak functions (spectral) .. -
Survey of Math: Chapter 21: Consumer Finance Savings Page 1
Survey of Math: Chapter 21: Consumer Finance Savings Page 1 Geometric Series Consider the following series: 1 + x + x2 + x3 + ··· + xn−1. We need to figure out a way to write this without the ···. Here’s how: s = 1 + x + x2 + x3 + ··· + xn−1 subtract xs = x + x2 + x3 + ··· + xn−1 + xn s − sx = 1 − 0 − 0 − 0 − · · · − 0 − xn s − sx = 1 − xn Now solve for s: 1 − xn xn − 1 s(1 − x) = 1 − xn ⇒ s = = . 1 − x x − 1 xn − 1 Therefore, a geometric series has the following sum: 1 + x + x2 + x3 + ··· + xn−1 = . x − 1 Exponential and Natural Logarithms As we have seen, some of our equations involve exponents. To effectively deal with exponents, we need to be able to work with exponentials and logarithms. The exponential and natural logarithm functions are inverse functions, and related by the following rules 1 m e = 1 + for m large m e = 2.71828 ... ln(eA) = A where A is a constant eln(A) = A If the base of the exponent is not e, we can use the following rule: ln(bA) = A ln(b) where A and b are constants ln(2A) = A ln(2) ln((1 + r)A) = A ln(1 + r) Note: • The natural logarithm acts on a number, so we read ln(2) as “The natural logarithm of 2”. • We would never write ln(2) = 2 ln, since this loses the fact that the natural logarithm must act on something. It is a functional evaluation, not a multiplication. • This is similar to trigonometric functions, like sin(π). -
Appendix I Integrating Step Functions
Appendix I Integrating Step Functions In Chapter I, section 1, we were considering step functions of the form (1) where II>"" In were brick functions and AI> ... ,An were real coeffi cients. The integral of I was defined by the formula (2) In case of a single real variable, it is almost obvious that the value JI does not depend on the representation (2). In Chapter I, we admitted formula (2) for several variables, relying on analogy only. There are various methods to prove that formula precisely. In this Appendix we are going to give a proof which uses the concept of Heaviside functions. Since the geometrical intuition, above all in multidimensional case, might be decep tive, all the given arguments will be purely algebraic. 1. Heaviside functions The Heaviside function H(x) on the real line Rl admits the value 1 for x;;;o °and vanishes elsewhere; it thus can be defined on writing H(x) = {I for x ;;;0O, ° for x<O. By a Heaviside function H(x) in the plane R2, where x actually denotes points x = (~I> ~2) of R2, we understand the function which admits the value 1 for x ;;;0 0, i.e., for ~l ~ 0, ~2;;;o 0, and vanishes elsewhere. In symbols, H(x) = {I for x ;;;0O, (1.1) ° for x to. Note that we cannot use here the notation x < °(which would mean ~l <0, ~2<0) instead of x~O, because then H(x) would not be defined in the whole plane R 2 • Similarly, in Euclidean q-dimensional space R'l, the Heaviside function H(x), where x = (~I>' . -
On the Approximation of the Cut and Step Functions by Logistic and Gompertz Functions
www.biomathforum.org/biomath/index.php/biomath ORIGINAL ARTICLE On the Approximation of the Cut and Step Functions by Logistic and Gompertz Functions Anton Iliev∗y, Nikolay Kyurkchievy, Svetoslav Markovy ∗Faculty of Mathematics and Informatics Paisii Hilendarski University of Plovdiv, Plovdiv, Bulgaria Email: [email protected] yInstitute of Mathematics and Informatics Bulgarian Academy of Sciences, Sofia, Bulgaria Emails: [email protected], [email protected] Received: , accepted: , published: will be added later Abstract—We study the uniform approximation practically important classes of sigmoid functions. of the sigmoid cut function by smooth sigmoid Two of them are the cut (or ramp) functions and functions such as the logistic and the Gompertz the step functions. Cut functions are continuous functions. The limiting case of the interval-valued but they are not smooth (differentiable) at the two step function is discussed using Hausdorff metric. endpoints of the interval where they increase. Step Various expressions for the error estimates of the corresponding uniform and Hausdorff approxima- functions can be viewed as limiting case of cut tions are obtained. Numerical examples are pre- functions; they are not continuous but they are sented using CAS MATHEMATICA. Hausdorff continuous (H-continuous) [4], [43]. In some applications smooth sigmoid functions are Keywords-cut function; step function; sigmoid preferred, some authors even require smoothness function; logistic function; Gompertz function; squashing function; Hausdorff approximation. in the definition of sigmoid functions. Two famil- iar classes of smooth sigmoid functions are the logistic and the Gompertz functions. There are I. INTRODUCTION situations when one needs to pass from nonsmooth In this paper we discuss some computational, sigmoid functions (e. -
Lecture 2 ELE 301: Signals and Systems
Lecture 2 ELE 301: Signals and Systems Prof. Paul Cuff Princeton University Fall 2011-12 Cuff (Lecture 2) ELE 301: Signals and Systems Fall 2011-12 1 / 70 Models of Continuous Time Signals Today's topics: Signals I Sinuoidal signals I Exponential signals I Complex exponential signals I Unit step and unit ramp I Impulse functions Systems I Memory I Invertibility I Causality I Stability I Time invariance I Linearity Cuff (Lecture 2) ELE 301: Signals and Systems Fall 2011-12 2 / 70 Sinusoidal Signals A sinusoidal signal is of the form x(t) = cos(!t + θ): where the radian frequency is !, which has the units of radians/s. Also very commonly written as x(t) = A cos(2πft + θ): where f is the frequency in Hertz. We will often refer to ! as the frequency, but it must be kept in mind that it is really the radian frequency, and the frequency is actually f . Cuff (Lecture 2) ELE 301: Signals and Systems Fall 2011-12 3 / 70 The period of the sinuoid is 1 2π T = = f ! with the units of seconds. The phase or phase angle of the signal is θ, given in radians. cos(ωt) cos(ωt θ) − 0 0 -2T -T T 2T t -2T -T T 2T t Cuff (Lecture 2) ELE 301: Signals and Systems Fall 2011-12 4 / 70 Complex Sinusoids The Euler relation defines ejφ = cos φ + j sin φ. A complex sinusoid is Aej(!t+θ) = A cos(!t + θ) + jA sin(!t + θ): e jωt -2T -T 0 T 2T Real sinusoid can be represented as the real part of a complex sinusoid Aej(!t+θ) = A cos(!t + θ) <f g Cuff (Lecture 2) ELE 301: Signals and Systems Fall 2011-12 5 / 70 Exponential Signals An exponential signal is given by x(t) = eσt If σ < 0 this is exponential decay. -
Step and Delta Functions 18.031 Haynes Miller and Jeremy Orloff 1
Step and Delta Functions 18.031 Haynes Miller and Jeremy Orloff 1 The unit step function 1.1 Definition Let's start with the definition of the unit step function, u(t): ( 0 for t < 0 u(t) = 1 for t > 0 We do not define u(t) at t = 0. Rather, at t = 0 we think of it as in transition between 0 and 1. It is called the unit step function because it takes a unit step at t = 0. It is sometimes called the Heaviside function. The graph of u(t) is simple. u(t) 1 t We will use u(t) as an idealized model of a natural system that goes from 0 to 1 very quickly. In reality it will make a smooth transition, such as the following. 1 t Figure 1. u(t) is an idealized version of this curve But, if the transition happens on a time scale much smaller than the time scale of the phenomenon we care about then the function u(t) is a good approximation. It is also much easier to deal with mathematically. One of our main uses for u(t) will be as a switch. It is clear that multiplying a function f(t) by u(t) gives ( 0 for t < 0 u(t)f(t) = f(t) for t > 0: We say the effect of multiplying by u(t) is that for t < 0 the function f(t) is switched off and for t > 0 it is switched on. 1 18.031 Step and Delta Functions 2 1.2 Integrals of u0(t) From calculus we know that Z Z b u0(t) dt = u(t) + c and u0(t) dt = u(b) − u(a): a For example: Z 5 u0(t) dt = u(5) − u(−2) = 1; −2 Z 3 u0(t) dt = u(3) − u(1) = 0; 1 Z −3 u0(t) dt = u(−3) − u(−5) = 0: −5 In fact, the following rule for the integral of u0(t) over any interval is obvious ( Z b 1 if 0 is inside the interval (a; b) u0(t) = (1) a 0 if 0 is outside the interval [a; b]. -
Calculating Logs Manually
calculating logs manually File Name: calculating logs manually.pdf Size: 2113 KB Type: PDF, ePub, eBook Category: Book Uploaded: 3 May 2019, 12:21 PM Rating: 4.6/5 from 561 votes. Status: AVAILABLE Last checked: 10 Minutes ago! In order to read or download calculating logs manually ebook, you need to create a FREE account. Download Now! eBook includes PDF, ePub and Kindle version ✔ Register a free 1 month Trial Account. ✔ Download as many books as you like (Personal use) ✔ Cancel the membership at any time if not satisfied. ✔ Join Over 80000 Happy Readers Book Descriptions: We have made it easy for you to find a PDF Ebooks without any digging. And by having access to our ebooks online or by storing it on your computer, you have convenient answers with calculating logs manually . To get started finding calculating logs manually , you are right to find our website which has a comprehensive collection of manuals listed. Our library is the biggest of these that have literally hundreds of thousands of different products represented. Home | Contact | DMCA Book Descriptions: calculating logs manually And let’s start with the logarithm of 2. As a kid I always wanted to know how to calculate log 2 and nobody was able to tell me. Can we guess the logarithm of 19,683.Let’s follow the chain. We are looking for 1225, so to account for the difference let’s round 3.0876 up to 3.088. How to calculate log 11. Here is a way to do this. We can take the geometric mean of 10 and 12. -
1 Introduction
1 Introduction Definition 1. A rational number is a number which can be expressed in the form a/b where a and b are integers with b > 0. Theorem 1. A real number α is a rational number if and only if it can be expressed as a repeating decimal, that is if and only if α = m.d1d2 . dkdk+1dk+2 . dk+r, where m = [α] if α ≥ 0 and m = −[|α|] if α < 0, where k and r are non-negative integers with r ≥ 1, and where the dj are digits. Proof. If α = m.d1d2 . dkdk+1dk+2 . dk+r, then (10k+r − 10k)α ∈ Z and it easily follows that α is rational. If α = a/b with a and b integers and b > 0, then α = m.d1d2 ... for some digits dj. If {x} denotes the fractional part of x, then j {10 |α|} = 0.dj+1dj+2 .... (1) On the other hand, {10j|α|} = {10ja/b} = u/b for some u ∈ {0, 1, . , b − 1}. Hence, by the pigeon-hole principle, there exist non-negative integers k and r with r ≥ 1 and {10k|α|} = {10k+r|α|}. From (1), we deduce that 0.dk+1dk+2 ··· = 0.dk+r+1dk+r+2 ... so that α = m.d1d2 . dkdk+1dk+2 . dk+r, and the result follows. Definition 2. A number is irrational if it is not rational. Theorem 2. A real number α which can be expressed as a non-repeating decimal is irrational. Proof 1. From the argument above, if α = m.d1d2 .. -
Introducing Mathematica
Introducing Mathematica John H. Lowenstein Preface This informal introduction to Mathematica®(a product of Wolfram Research, Inc.) is offered as a downloadable resource for users of the textbook Essentials of Hamiltonian Dynamics (Cambridge University Press, 2012). The aim is to familiarize the student with the core concepts and functions of Mathematica programming, so that he or she can very quickly become comfortable with computational methods in dealing with the illustrative examples and exercises in the textbook. The scope of Mathematica obviously greatly exceeds what can be covered in these few pages, and so it is highly recommended that the student take full advantage of the excellent documentation which is included with the software (accessible via the Help menu). 1. Getting started Mathematica conducts a dialogue with the user: you type in a mathematical expression, press Enter , and Mathemat- ica evaluates the expression according to rules which are either built-in or have been prescribed by you, displaying the result as output. The input/output alternation continues until you quit the session, with all steps recorded in the cells of your notebook. The simplest expressions involve ordinary numbers (e.g. 1, 2, 3, . , 1/2, 2/3, . , 3.14159), and the familiar operations and relations of arithmetic and logic. Elementary numerical operations: + (plus), - (minus), * (times), / (divided by), ^ (to the power) Elementary numerical relations: == (is equal to), != (is not equal to), < (is less than), > (is greater than), <= (is less than or equal to), >= (is greater than or equal to) Elementary logical relations: || (or), && (and), ! (not) For example, 2+2 evaluates to 4 , 1<2 evaluates to True , and !(2>1) evaluates to False . -
Twisting Algorithm for Controlling F-16 Aircraft
TWISTING ALGORITHM FOR CONTROLLING F-16 AIRCRAFT WITH PERFORMANCE MARGINS IDENTIFICATION by AKSHAY KULKARNI A THESIS Submitted in partial fulfillment of the requirements For the degree of Master of Science in Engineering In The Department of Electrical and Computer Engineering To The School of Graduate Studies Of The University of Alabama in Huntsville HUNTSVILLE, ALABAMA 2014 In presenting this thesis in partial fulfillment of the requirements for a master's degree from The University of Alabama in Huntsville, I agree that the Library of this University shall make it freely available for inspection. I further agree that permission for extensive copying for scholarly purposes may be granted by my advisor or, in his absence, by the Chair of the Department or the Dean of the School of Graduate Studies. It is also understood that due recognition shall be given to me and to The University of Alabama in Huntsville in any scholarly use which may be made of any material in this thesis. ____________________________ ___________ (Student signature) (Date) ii THESIS APPROVAL FORM Submitted by Akshay Kulkarni in partial fulfillment of the requirements for the degree of Master of Science in Engineering and accepted on behalf of the Faculty of the School of Graduate Studies by the thesis committee. We, the undersigned members of the Graduate Faculty of The University of Alabama in Huntsville, certify that we have advised and/or supervised the candidate on the work described in this thesis. We further certify that we have reviewed the thesis manuscript and approve it in partial fulfillment of the requirements for the degree of Master of Science in Engineering. -
Piecewise-Defined Functions and Periodic Functions
28 Piecewise-Defined Functions and Periodic Functions At the start of our study of the Laplace transform, it was claimed that the Laplace transform is “particularly useful when dealing with nonhomogeneous equations in which the forcing func- tions are not continuous”. Thus far, however, we’ve done precious little with any discontinuous functions other than step functions. Let us now rectify the situation by looking at the sort of discontinuous functions (and, more generally, “piecewise-defined” functions) that often arise in applications, and develop tools and skills for dealing with these functions. We willalsotakea brieflookat transformsof periodicfunctions other than sines and cosines. As you will see, many of these functions are, themselves, piecewise defined. And finally, we will use some of the material we’ve recently developed to re-examine the issue of resonance in mass/spring systems. 28.1 Piecewise-Defined Functions Piecewise-Defined Functions, Defined When we talk about a “discontinuous function f ” in the context of Laplace transforms, we usually mean f is a piecewise continuous function that is not continuous on the interval (0, ) . ∞ Such a functionwill have jump discontinuitiesat isolatedpoints in this interval. Computationally, however, the real issue is often not so much whether there is a nonzero jump in the graph of f at a point t0 , but whether the formula for computing f (t) is the same on either side of t0 . So we really should be looking at the more general class of “piecewise-defined” functions that, at worst, have jump discontinuities. Just what is a piecewise-defined function? It is any function given by different formulas on different intervals.