Breaking Hypothesis Testing for Failure Rates∗
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Laws of Total Expectation and Total Variance
Laws of Total Expectation and Total Variance Definition of conditional density. Assume and arbitrary random variable X with density fX . Take an event A with P (A) > 0. Then the conditional density fXjA is defined as follows: 8 < f(x) 2 P (A) x A fXjA(x) = : 0 x2 = A Note that the support of fXjA is supported only in A. Definition of conditional expectation conditioned on an event. Z Z 1 E(h(X)jA) = h(x) fXjA(x) dx = h(x) fX (x) dx A P (A) A Example. For the random variable X with density function 8 < 1 3 64 x 0 < x < 4 f(x) = : 0 otherwise calculate E(X2 j X ≥ 1). Solution. Step 1. Z h i 4 1 1 1 x=4 255 P (X ≥ 1) = x3 dx = x4 = 1 64 256 4 x=1 256 Step 2. Z Z ( ) 1 256 4 1 E(X2 j X ≥ 1) = x2 f(x) dx = x2 x3 dx P (X ≥ 1) fx≥1g 255 1 64 Z ( ) ( )( ) h i 256 4 1 256 1 1 x=4 8192 = x5 dx = x6 = 255 1 64 255 64 6 x=1 765 Definition of conditional variance conditioned on an event. Var(XjA) = E(X2jA) − E(XjA)2 1 Example. For the previous example , calculate the conditional variance Var(XjX ≥ 1) Solution. We already calculated E(X2 j X ≥ 1). We only need to calculate E(X j X ≥ 1). Z Z Z ( ) 1 256 4 1 E(X j X ≥ 1) = x f(x) dx = x x3 dx P (X ≥ 1) fx≥1g 255 1 64 Z ( ) ( )( ) h i 256 4 1 256 1 1 x=4 4096 = x4 dx = x5 = 255 1 64 255 64 5 x=1 1275 Finally: ( ) 8192 4096 2 630784 Var(XjX ≥ 1) = E(X2jX ≥ 1) − E(XjX ≥ 1)2 = − = 765 1275 1625625 Definition of conditional expectation conditioned on a random variable. -
Research Participants' Rights to Data Protection in the Era of Open Science
DePaul Law Review Volume 69 Issue 2 Winter 2019 Article 16 Research Participants’ Rights To Data Protection In The Era Of Open Science Tara Sklar Mabel Crescioni Follow this and additional works at: https://via.library.depaul.edu/law-review Part of the Law Commons Recommended Citation Tara Sklar & Mabel Crescioni, Research Participants’ Rights To Data Protection In The Era Of Open Science, 69 DePaul L. Rev. (2020) Available at: https://via.library.depaul.edu/law-review/vol69/iss2/16 This Article is brought to you for free and open access by the College of Law at Via Sapientiae. It has been accepted for inclusion in DePaul Law Review by an authorized editor of Via Sapientiae. For more information, please contact [email protected]. \\jciprod01\productn\D\DPL\69-2\DPL214.txt unknown Seq: 1 21-APR-20 12:15 RESEARCH PARTICIPANTS’ RIGHTS TO DATA PROTECTION IN THE ERA OF OPEN SCIENCE Tara Sklar and Mabel Crescioni* CONTENTS INTRODUCTION ................................................. 700 R I. REAL-WORLD EVIDENCE AND WEARABLES IN CLINICAL TRIALS ....................................... 703 R II. DATA PROTECTION RIGHTS ............................. 708 R A. General Data Protection Regulation ................. 709 R B. California Consumer Privacy Act ................... 710 R C. GDPR and CCPA Influence on State Data Privacy Laws ................................................ 712 R III. RESEARCH EXEMPTION AND RELATED SAFEGUARDS ... 714 R IV. RESEARCH PARTICIPANTS’ DATA AND OPEN SCIENCE . 716 R CONCLUSION ................................................... 718 R Clinical trials are increasingly using sensors embedded in wearable de- vices due to their capabilities to generate real-world data. These devices are able to continuously monitor, record, and store physiological met- rics in response to a given therapy, which is contributing to a redesign of clinical trials around the world. -
Overview of Reliability Engineering
Overview of reliability engineering Eric Marsden <[email protected]> Context ▷ I have a fleet of airline engines and want to anticipate when they mayfail ▷ I am purchasing pumps for my refinery and want to understand the MTBF, lambda etc. provided by the manufacturers ▷ I want to compare different system designs to determine the impact of architecture on availability 2 / 32 Reliability engineering ▷ Reliability engineering is the discipline of ensuring that a system will function as required over a specified time period when operated and maintained in a specified manner. ▷ Reliability engineers address 3 basic questions: • When does something fail? • Why does it fail? • How can the likelihood of failure be reduced? 3 / 32 The termination of the ability of an item to perform a required function. [IEV Failure Failure 191-04-01] ▷ A failure is always related to a required function. The function is often specified together with a performance requirement (eg. “must handleup to 3 tonnes per minute”, “must respond within 0.1 seconds”). ▷ A failure occurs when the function cannot be performed or has a performance that falls outside the performance requirement. 4 / 32 The state of an item characterized by inability to perform a required function Fault Fault [IEV 191-05-01] ▷ While a failure is an event that occurs at a specific point in time, a fault is a state that will last for a shorter or longer period. ▷ When a failure occurs, the item enters the failed state. A failure may occur: • while running • while in standby • due to demand 5 / 32 Discrepancy between a computed, observed, or measured value or condition and Error Error the true, specified, or theoretically correct value or condition. -
Lochner</I> in Cyberspace: the New Economic Orthodoxy Of
Georgetown University Law Center Scholarship @ GEORGETOWN LAW 1998 Lochner in Cyberspace: The New Economic Orthodoxy of "Rights Management" Julie E. Cohen Georgetown University Law Center, [email protected] This paper can be downloaded free of charge from: https://scholarship.law.georgetown.edu/facpub/811 97 Mich. L. Rev. 462-563 (1998) This open-access article is brought to you by the Georgetown Law Library. Posted with permission of the author. Follow this and additional works at: https://scholarship.law.georgetown.edu/facpub Part of the Intellectual Property Law Commons, Internet Law Commons, and the Law and Economics Commons LOCHNER IN CYBERSPACE: THE NEW ECONOMIC ORTHODOXY OF "RIGHTS MANAGEMENT" JULIE E. COHEN * Originally published 97 Mich. L. Rev. 462 (1998). TABLE OF CONTENTS I. THE CONVERGENCE OF ECONOMIC IMPERATIVES AND NATURAL RIGHTS..........6 II. THE NEW CONCEPTUALISM.....................................................18 A. Constructing Consent ......................................................18 B. Manufacturing Scarcity.....................................................32 1. Transaction Costs and Common Resources................................33 2. Incentives and Redistribution..........................................40 III. ON MODELING INFORMATION MARKETS........................................50 A. Bargaining Power and Choice in Information Markets.............................52 1. Contested Exchange and the Power to Switch.............................52 2. Collective Action, "Rent-Seeking," and Public Choice.......................67 -
Understanding Functional Safety FIT Base Failure Rate Estimates Per IEC 62380 and SN 29500
www.ti.com Technical White Paper Understanding Functional Safety FIT Base Failure Rate Estimates per IEC 62380 and SN 29500 Bharat Rajaram, Senior Member, Technical Staff, and Director, Functional Safety, C2000™ Microcontrollers, Texas Instruments ABSTRACT Functional safety standards like International Electrotechnical Commission (IEC) 615081 and International Organization for Standardization (ISO) 262622 require that semiconductor device manufacturers address both systematic and random hardware failures. Systematic failures are managed and mitigated by following rigorous development processes. Random hardware failures must adhere to specified quantitative metrics to meet hardware safety integrity levels (SILs) or automotive SILs (ASILs). Consequently, systematic failures are excluded from the calculation of random hardware failure metrics. Table of Contents 1 Introduction.............................................................................................................................................................................2 2 Types of Faults and Quantitative Random Hardware Failure Metrics .............................................................................. 2 3 Random Failures Over a Product Lifetime and Estimation of BFR ...................................................................................3 4 BFR Estimation Techniques ................................................................................................................................................. 4 5 Siemens SN 29500 FIT model -
Probability Cheatsheet V2.0 Thinking Conditionally Law of Total Probability (LOTP)
Probability Cheatsheet v2.0 Thinking Conditionally Law of Total Probability (LOTP) Let B1;B2;B3; :::Bn be a partition of the sample space (i.e., they are Compiled by William Chen (http://wzchen.com) and Joe Blitzstein, Independence disjoint and their union is the entire sample space). with contributions from Sebastian Chiu, Yuan Jiang, Yuqi Hou, and Independent Events A and B are independent if knowing whether P (A) = P (AjB )P (B ) + P (AjB )P (B ) + ··· + P (AjB )P (B ) Jessy Hwang. Material based on Joe Blitzstein's (@stat110) lectures 1 1 2 2 n n A occurred gives no information about whether B occurred. More (http://stat110.net) and Blitzstein/Hwang's Introduction to P (A) = P (A \ B1) + P (A \ B2) + ··· + P (A \ Bn) formally, A and B (which have nonzero probability) are independent if Probability textbook (http://bit.ly/introprobability). Licensed and only if one of the following equivalent statements holds: For LOTP with extra conditioning, just add in another event C! under CC BY-NC-SA 4.0. Please share comments, suggestions, and errors at http://github.com/wzchen/probability_cheatsheet. P (A \ B) = P (A)P (B) P (AjC) = P (AjB1;C)P (B1jC) + ··· + P (AjBn;C)P (BnjC) P (AjB) = P (A) P (AjC) = P (A \ B1jC) + P (A \ B2jC) + ··· + P (A \ BnjC) P (BjA) = P (B) Last Updated September 4, 2015 Special case of LOTP with B and Bc as partition: Conditional Independence A and B are conditionally independent P (A) = P (AjB)P (B) + P (AjBc)P (Bc) given C if P (A \ BjC) = P (AjC)P (BjC). -
Probability Cheatsheet
Probability Cheatsheet v1.1.1 Simpson's Paradox Expected Value, Linearity, and Symmetry P (A j B; C) < P (A j Bc;C) and P (A j B; Cc) < P (A j Bc;Cc) Expected Value (aka mean, expectation, or average) can be thought Compiled by William Chen (http://wzchen.com) with contributions yet still, P (A j B) > P (A j Bc) of as the \weighted average" of the possible outcomes of our random from Sebastian Chiu, Yuan Jiang, Yuqi Hou, and Jessy Hwang. variable. Mathematically, if x1; x2; x3;::: are all of the possible values Material based off of Joe Blitzstein's (@stat110) lectures Bayes' Rule and Law of Total Probability that X can take, the expected value of X can be calculated as follows: P (http://stat110.net) and Blitzstein/Hwang's Intro to Probability E(X) = xiP (X = xi) textbook (http://bit.ly/introprobability). Licensed under CC i Law of Total Probability with partitioning set B1; B2; B3; :::Bn and BY-NC-SA 4.0. Please share comments, suggestions, and errors at with extra conditioning (just add C!) Note that for any X and Y , a and b scaling coefficients and c is our http://github.com/wzchen/probability_cheatsheet. constant, the following property of Linearity of Expectation holds: P (A) = P (AjB1)P (B1) + P (AjB2)P (B2) + :::P (AjBn)P (Bn) Last Updated March 20, 2015 P (A) = P (A \ B1) + P (A \ B2) + :::P (A \ Bn) E(aX + bY + c) = aE(X) + bE(Y ) + c P (AjC) = P (AjB1; C)P (B1jC) + :::P (AjBn; C)P (BnjC) If two Random Variables have the same distribution, even when they are dependent by the property of Symmetry their expected values P (AjC) = P (A \ B jC) + P (A \ B jC) + :::P (A \ B jC) Counting 1 2 n are equal. -
Probability Analysis in Determining the Behaviour of Variable Amplitude Strain Signal Based on Extraction Segments
2141 Probability Analysis in Determining the Behaviour of Variable Amplitude Strain Signal Based on Extraction Segments Abstract M. F. M. Yunoh a This paper focuses on analysis in determining the behaviour of vari- S. Abdullah b, * able amplitude strain signals based on extraction of segments. The M. H. M. Saad c constant Amplitude loading (CAL), that was used in the laboratory d Z. M. Nopiah tests, was designed according to the variable amplitude loading e (VAL) from Society of Automotive Engineers (SAE). The SAE strain M. Z. Nuawi signal was then edited to obtain those segments that cause fatigue a damage to components. The segments were then sorted according to Department of Mechanical and Materials their amplitude and were used as a reference in the design of the Engineering, Faculty of Engineering & CAL loading for the laboratory tests. The strain signals that were Built Enviroment, Universiti Kebangsaan obtained from the laboratory tests were then analysed using fatigue Malaysia, 43600 UKM Bangi, Selangor, life prediction approach and statistics, i.e. Weibull distribution anal- Malaysia. [email protected] b ysis. Based on the plots of the Probability Density Function (PDF), [email protected] c Cumulative Distribution Function (CDF) and the probability of fail- [email protected]; d ure in the Weibull distribution analysis, it was shown that more than [email protected]; e 70% failure occurred when the number of cycles approached 1.0 x [email protected] 1011. Therefore, the Weibull distribution analysis can be used as an alternative to predict the failure probability. * Corresponding author: S. -
(Introduction to Probability at an Advanced Level) - All Lecture Notes
Fall 2018 Statistics 201A (Introduction to Probability at an advanced level) - All Lecture Notes Aditya Guntuboyina August 15, 2020 Contents 0.1 Sample spaces, Events, Probability.................................5 0.2 Conditional Probability and Independence.............................6 0.3 Random Variables..........................................7 1 Random Variables, Expectation and Variance8 1.1 Expectations of Random Variables.................................9 1.2 Variance................................................ 10 2 Independence of Random Variables 11 3 Common Distributions 11 3.1 Ber(p) Distribution......................................... 11 3.2 Bin(n; p) Distribution........................................ 11 3.3 Poisson Distribution......................................... 12 4 Covariance, Correlation and Regression 14 5 Correlation and Regression 16 6 Back to Common Distributions 16 6.1 Geometric Distribution........................................ 16 6.2 Negative Binomial Distribution................................... 17 7 Continuous Distributions 17 7.1 Normal or Gaussian Distribution.................................. 17 1 7.2 Uniform Distribution......................................... 18 7.3 The Exponential Density...................................... 18 7.4 The Gamma Density......................................... 18 8 Variable Transformations 19 9 Distribution Functions and the Quantile Transform 20 10 Joint Densities 22 11 Joint Densities under Transformations 23 11.1 Detour to Convolutions...................................... -
Individual Failure Rate Modelling and Exploratory Failure Data Analysis for Power System Components
INDIVIDUAL FAILURE RATE MODELLING AND EXPLORATORY FAILURE DATA ANALYSIS FOR POWER SYSTEM COMPONENTS REPORT 2018:549 RISK- OCH TILLFÖRLITLIGHETSANALYS Individual Failure Rate Modelling and Exploratory Failure Data Analysis for Power System Components JAN HENNING JÜRGENSEN ISBN 978-91-7673-549-7 | © Energiforsk December 2018 Energiforsk AB | Phone: 08-677 25 30 | E-mail: [email protected] | www.energiforsk.se INDIVIDUAL FAILURE RATE MODELLING AND EXPLORATORY FAILURE DATA ANALYSIS FOR POWER SYSTEM COMPONENTS Foreword Detta projekt är en fortsättning på ett doktorandprojekt från tidigare programperiod. Etappen Riskanalys III hanterade projektet från licentiat till doktorsavhandling genom att stötta en slutrapportering. Projektet studerade om felfrekvensnoggrannheten på en enskild komponentnivå kan öka trots att det tillgängliga historiska feldatat är begränsat. Resultatet var att effekterna av riskfaktorer på felfrekvens med regressionsmodeller kvantifierades, samt en ökad förståelse av riskfaktorer och högre noggrannhet av felfrekvensen. Statistisk data-underbyggda metoder används fortfarande sällan i kraftsystemen samtidigt som metoder behövs för att förbättra felfrekvensnoggrannheten trots begränsade tillgängliga data. Metoden beräknar individuella felfrekvenser. Jan Henning Jürgensen från Kungliga Tekniska Högskolan, har varit projektledare för projektet. Han har arbetat under handledning av docent Patrik Hilber och professor Lars Nordström, bägge på KTH. Stort tack till följande programstyrelse för all hjälp och vägledning: • Jenny -
The Effects of Autocorrelation in the Estimation of Process Capability Indices." (1998)
Louisiana State University LSU Digital Commons LSU Historical Dissertations and Theses Graduate School 1998 The ffecE ts of Autocorrelation in the Estimation of Process Capability Indices. Lawrence Lee Magee Louisiana State University and Agricultural & Mechanical College Follow this and additional works at: https://digitalcommons.lsu.edu/gradschool_disstheses Recommended Citation Magee, Lawrence Lee, "The Effects of Autocorrelation in the Estimation of Process Capability Indices." (1998). LSU Historical Dissertations and Theses. 6847. https://digitalcommons.lsu.edu/gradschool_disstheses/6847 This Dissertation is brought to you for free and open access by the Graduate School at LSU Digital Commons. It has been accepted for inclusion in LSU Historical Dissertations and Theses by an authorized administrator of LSU Digital Commons. For more information, please contact [email protected]. INFORMATION TO USERS This manuscript has been reproduced from the microfilm master. U M I films the text directly from die original or copy submitted. Thus, some thesis and dissertation copies are in typewriter face, while others may be from any type o f computer printer. The quality o f this reproduction is dependent upon the quality o f the copy submitted. Broken or indistinct print, colored or poor quality illustrations and photographs, print bleedthrough, substandard margins, and improper alignment can adversely affect reproduction. hi the unlikely event that the author did not send UMI a complete manuscript and there are missing pages, these will be noted. Also, if unauthorized copyright material had to be removed, a note w ill indicate the deletion. Oversize materials (e.g., maps, drawings, charts) are reproduced by sectioning the original, beginning at the upper left-hand corner and continuing from left to right in equal sections with small overlaps. -
Chapter 2 Failure Models Part 1: Introduction
Chapter 2 Failure Models Part 1: Introduction Marvin Rausand Department of Production and Quality Engineering Norwegian University of Science and Technology [email protected] Marvin Rausand, March 14, 2006 System Reliability Theory (2nd ed), Wiley, 2004 – 1 / 31 Introduction Rel. measures Life distributions State variable Time to failure Distr. function Probability density Distribution of T Reliability funct. Failure rate Introduction Bathtub curve Some formulas MTTF Example 2.1 Median Mode MRL Example 2.2 Discrete distributions Life distributions Marvin Rausand, March 14, 2006 System Reliability Theory (2nd ed), Wiley, 2004 – 2 / 31 Reliability measures Introduction In this chapter we introduce the following measures: Rel. measures Life distributions State variable Time to failure ■ Distr. function The reliability (survivor) function R(t) Probability density ■ The failure rate function z(t) Distribution of T ■ Reliability funct. The mean time to failure (MTTF) Failure rate ■ The mean residual life (MRL) Bathtub curve Some formulas MTTF Example 2.1 of a single item that is not repaired when it fails. Median Mode MRL Example 2.2 Discrete distributions Life distributions Marvin Rausand, March 14, 2006 System Reliability Theory (2nd ed), Wiley, 2004 – 3 / 31 Life distributions Introduction The following life distributions are discussed: Rel. measures Life distributions State variable ■ The exponential distribution Time to failure ■ Distr. function The gamma distribution Probability density ■ The Weibull distribution Distribution of