Mathematics of Distances and Applications
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Glossary Physics (I-Introduction)
1 Glossary Physics (I-introduction) - Efficiency: The percent of the work put into a machine that is converted into useful work output; = work done / energy used [-]. = eta In machines: The work output of any machine cannot exceed the work input (<=100%); in an ideal machine, where no energy is transformed into heat: work(input) = work(output), =100%. Energy: The property of a system that enables it to do work. Conservation o. E.: Energy cannot be created or destroyed; it may be transformed from one form into another, but the total amount of energy never changes. Equilibrium: The state of an object when not acted upon by a net force or net torque; an object in equilibrium may be at rest or moving at uniform velocity - not accelerating. Mechanical E.: The state of an object or system of objects for which any impressed forces cancels to zero and no acceleration occurs. Dynamic E.: Object is moving without experiencing acceleration. Static E.: Object is at rest.F Force: The influence that can cause an object to be accelerated or retarded; is always in the direction of the net force, hence a vector quantity; the four elementary forces are: Electromagnetic F.: Is an attraction or repulsion G, gravit. const.6.672E-11[Nm2/kg2] between electric charges: d, distance [m] 2 2 2 2 F = 1/(40) (q1q2/d ) [(CC/m )(Nm /C )] = [N] m,M, mass [kg] Gravitational F.: Is a mutual attraction between all masses: q, charge [As] [C] 2 2 2 2 F = GmM/d [Nm /kg kg 1/m ] = [N] 0, dielectric constant Strong F.: (nuclear force) Acts within the nuclei of atoms: 8.854E-12 [C2/Nm2] [F/m] 2 2 2 2 2 F = 1/(40) (e /d ) [(CC/m )(Nm /C )] = [N] , 3.14 [-] Weak F.: Manifests itself in special reactions among elementary e, 1.60210 E-19 [As] [C] particles, such as the reaction that occur in radioactive decay. -
Forces Different Types of Forces
Forces and motion are a part of your everyday life for example pushing a trolley, a horse pulling a rope, speed and acceleration. Force and motion causes objects to move but also to stay still. Motion is simply a movement but needs a force to move. There are 2 types of forces, contact forces and act at a distance force. Forces Every day you are using forces. Force is basically push and pull. When you push and pull you are applying a force to an object. If you are Appling force to an object you are changing the objects motion. For an example when a ball is coming your way and then you push it away. The motion of the ball is changed because you applied a force. Different Types of Forces There are more forces than push or pull. Scientists group all these forces into two groups. The first group is contact forces, contact forces are forces when 2 objects are physically interacting with each other by touching. The second group is act at a distance force, act at a distance force is when 2 objects that are interacting with each other but not physically touching. Contact Forces There are different types of contact forces like normal Force, spring force, applied force and tension force. Normal force is when nothing is happening like a book lying on a table because gravity is pulling it down. Another contact force is spring force, spring force is created by a compressed or stretched spring that could push or pull. Applied force is when someone is applying a force to an object, for example a horse pulling a rope or a boy throwing a snow ball. -
Maurice Pouzet References
Maurice Pouzet References [1] M. Kabil, M. Pouzet, I.G. Rosenberg, Free monoids and metric spaces, To the memory of Michel Deza, Europ. J. of Combinatorics, Online publi- cation complete: April 2, 2018, https://doi.org/10.1016/j.ejc.2018.02.008. arXiv: 1705.09750v1, 27 May 2017. [2] I.Chakir, M.Pouzet, A characterization of well-founded algebraic lattices, Contribution to Discrete Math. Vol 13, (1) (2018) 35-50. [3] K.Adaricheva, M.Pouzet, On scattered convex geometries, Order, (2017) 34:523{550. [4] C.Delhomm´e,M.Pouzet, Length of an intersection, Mathematical Logic Quarterly 63 (2017) no.3-4, 243-255. [5] C.DELHOMME,´ M.MIYAKAWA, M.POUZET, I.G.ROSENBERG, H.TATSUMI, Semirigid systems of three equivalence relations, J. Mult.-Valued Logic Soft Comput. 28 (2017), no. 4-5, 511-535. [6] C.Laflamme, M.Pouzet, R.Woodrow, Equimorphy- the case of chains, Archive for Mathematical Logic, 56 (2017), no. 7-8, 811{829. [7] C.Laflamme, M.Pouzet, N.Sauer, Invariant subsets of scattered trees. An application to the tree alternative property of Bonato and Tardif, Ab- handlungen aus dem Mathematischen Seminar der Universitt Hamburg (Abh. Math. Sem. Univ. Hamburg) October 2017, Volume 87, Issue 2, pp 369-408. [8] D.Oudrar, M.Pouzet, Profile and hereditary classes of relational struc- tures, J. of MVLSC Volume 27, Number 5-6 (2016), pp. 475-500. [9] M.Pouzet, H.Si-Kaddour, Isomorphy up to complementation, Journal of Combinatorics, Vol. 7, No. 2 (2016), pp. 285-305. [10] C.Laflamme, M.Pouzet, N.Sauer, I.Zaguia, Orthogonal countable ordinals, Discrete Math. -
LINEAR ALGEBRA METHODS in COMBINATORICS László Babai
LINEAR ALGEBRA METHODS IN COMBINATORICS L´aszl´oBabai and P´eterFrankl Version 2.1∗ March 2020 ||||| ∗ Slight update of Version 2, 1992. ||||||||||||||||||||||| 1 c L´aszl´oBabai and P´eterFrankl. 1988, 1992, 2020. Preface Due perhaps to a recognition of the wide applicability of their elementary concepts and techniques, both combinatorics and linear algebra have gained increased representation in college mathematics curricula in recent decades. The combinatorial nature of the determinant expansion (and the related difficulty in teaching it) may hint at the plausibility of some link between the two areas. A more profound connection, the use of determinants in combinatorial enumeration goes back at least to the work of Kirchhoff in the middle of the 19th century on counting spanning trees in an electrical network. It is much less known, however, that quite apart from the theory of determinants, the elements of the theory of linear spaces has found striking applications to the theory of families of finite sets. With a mere knowledge of the concept of linear independence, unexpected connections can be made between algebra and combinatorics, thus greatly enhancing the impact of each subject on the student's perception of beauty and sense of coherence in mathematics. If these adjectives seem inflated, the reader is kindly invited to open the first chapter of the book, read the first page to the point where the first result is stated (\No more than 32 clubs can be formed in Oddtown"), and try to prove it before reading on. (The effect would, of course, be magnified if the title of this volume did not give away where to look for clues.) What we have said so far may suggest that the best place to present this material is a mathematics enhancement program for motivated high school students. -
Geodesic Distance Descriptors
Geodesic Distance Descriptors Gil Shamai and Ron Kimmel Technion - Israel Institute of Technologies [email protected] [email protected] Abstract efficiency of state of the art shape matching procedures. The Gromov-Hausdorff (GH) distance is traditionally used for measuring distances between metric spaces. It 1. Introduction was adapted for non-rigid shape comparison and match- One line of thought in shape analysis considers an ob- ing of isometric surfaces, and is defined as the minimal ject as a metric space, and object matching, classification, distortion of embedding one surface into the other, while and comparison as the operation of measuring the discrep- the optimal correspondence can be described as the map ancies and similarities between such metric spaces, see, for that minimizes this distortion. Solving such a minimiza- example, [13, 33, 27, 23, 8, 3, 24]. tion is a hard combinatorial problem that requires pre- Although theoretically appealing, the computation of computation and storing of all pairwise geodesic distances distances between metric spaces poses complexity chal- for the matched surfaces. A popular way for compact repre- lenges as far as direct computation and memory require- sentation of functions on surfaces is by projecting them into ments are involved. As a remedy, alternative representa- the leading eigenfunctions of the Laplace-Beltrami Opera- tion spaces were proposed [26, 22, 15, 10, 31, 30, 19, 20]. tor (LBO). When truncated, the basis of the LBO is known The question of which representation to use in order to best to be the optimal for representing functions with bounded represent the metric space that define each form we deal gradient in a min-max sense. -
Robust Topological Inference: Distance to a Measure and Kernel Distance
Journal of Machine Learning Research 18 (2018) 1-40 Submitted 9/15; Revised 2/17; Published 4/18 Robust Topological Inference: Distance To a Measure and Kernel Distance Fr´ed´ericChazal [email protected] Inria Saclay - Ile-de-France Alan Turing Bldg, Office 2043 1 rue Honor´ed'Estienne d'Orves 91120 Palaiseau, FRANCE Brittany Fasy [email protected] Computer Science Department Montana State University 357 EPS Building Montana State University Bozeman, MT 59717 Fabrizio Lecci [email protected] New York, NY Bertrand Michel [email protected] Ecole Centrale de Nantes Laboratoire de math´ematiquesJean Leray 1 Rue de La Noe 44300 Nantes FRANCE Alessandro Rinaldo [email protected] Department of Statistics Carnegie Mellon University Pittsburgh, PA 15213 Larry Wasserman [email protected] Department of Statistics Carnegie Mellon University Pittsburgh, PA 15213 Editor: Mikhail Belkin Abstract Let P be a distribution with support S. The salient features of S can be quantified with persistent homology, which summarizes topological features of the sublevel sets of the dis- tance function (the distance of any point x to S). Given a sample from P we can infer the persistent homology using an empirical version of the distance function. However, the empirical distance function is highly non-robust to noise and outliers. Even one outlier is deadly. The distance-to-a-measure (DTM), introduced by Chazal et al. (2011), and the ker- nel distance, introduced by Phillips et al. (2014), are smooth functions that provide useful topological information but are robust to noise and outliers. Chazal et al. (2015) derived concentration bounds for DTM. -
Daisy Cubes and Distance Cube Polynomial
Daisy cubes and distance cube polynomial Sandi Klavˇzar a,b,c Michel Mollard d July 21, 2017 a Faculty of Mathematics and Physics, University of Ljubljana, Slovenia [email protected] b Faculty of Natural Sciences and Mathematics, University of Maribor, Slovenia c Institute of Mathematics, Physics and Mechanics, Ljubljana, Slovenia d Institut Fourier, CNRS Universit´eGrenoble Alpes, France [email protected] Dedicated to the memory of our friend Michel Deza Abstract n Let X ⊆ {0, 1} . The daisy cube Qn(X) is introduced as the subgraph of n Qn induced by the union of the intervals I(x, 0 ) over all x ∈ X. Daisy cubes are partial cubes that include Fibonacci cubes, Lucas cubes, and bipartite wheels. If u is a vertex of a graph G, then the distance cube polynomial DG,u(x,y) is introduced as the bivariate polynomial that counts the number of induced subgraphs isomorphic to Qk at a given distance from the vertex u. It is proved that if G is a daisy cube, then DG,0n (x,y)= CG(x + y − 1), where CG(x) is the previously investigated cube polynomial of G. It is also proved that if G is a daisy cube, then DG,u(x, −x) = 1 holds for every vertex u in G. Keywords: daisy cube; partial cube; cube polynomial; distance cube polynomial; Fibonacci cube; Lucas cube AMS Subj. Class. (2010): 05C31, 05C75, 05A15 1 Introduction In this paper we introduce a class of graphs, the members of which will be called daisy cubes. -
Hydraulics Manual Glossary G - 3
Glossary G - 1 GLOSSARY OF HIGHWAY-RELATED DRAINAGE TERMS (Reprinted from the 1999 edition of the American Association of State Highway and Transportation Officials Model Drainage Manual) G.1 Introduction This Glossary is divided into three parts: · Introduction, · Glossary, and · References. It is not intended that all the terms in this Glossary be rigorously accurate or complete. Realistically, this is impossible. Depending on the circumstance, a particular term may have several meanings; this can never change. The primary purpose of this Glossary is to define the terms found in the Highway Drainage Guidelines and Model Drainage Manual in a manner that makes them easier to interpret and understand. A lesser purpose is to provide a compendium of terms that will be useful for both the novice as well as the more experienced hydraulics engineer. This Glossary may also help those who are unfamiliar with highway drainage design to become more understanding and appreciative of this complex science as well as facilitate communication between the highway hydraulics engineer and others. Where readily available, the source of a definition has been referenced. For clarity or format purposes, cited definitions may have some additional verbiage contained in double brackets [ ]. Conversely, three “dots” (...) are used to indicate where some parts of a cited definition were eliminated. Also, as might be expected, different sources were found to use different hyphenation and terminology practices for the same words. Insignificant changes in this regard were made to some cited references and elsewhere to gain uniformity for the terms contained in this Glossary: as an example, “groundwater” vice “ground-water” or “ground water,” and “cross section area” vice “cross-sectional area.” Cited definitions were taken primarily from two sources: W.B. -
European Journal of Combinatorics Preface
European Journal of Combinatorics 31 (2010) 419–422 Contents lists available at ScienceDirect European Journal of Combinatorics journal homepage: www.elsevier.com/locate/ejc Preface We are pleased to dedicate this special issue of the European Journal of Combinatorics to Michel Deza on the occasion of his 70th birthday, celebrated on April 27, 2009. This issue includes research articles by a selected group of authors – some of his students, colleagues, collaborators and friends. M. Deza is a distinguished figure in contemporary discrete mathematics. He graduated in 1961 from Moscow University where he learned to love mathematics by following lectures from professors such as P.S. Alexandrov, B.N. Delone, A.A. Markov and A.N. Kolmogorov. Then he took a position as researcher in the Academy of Sciences of USSR until his emigration in 1972 to France. From 1973 until his retirement in 2005, he served as a researcher at CNRS (Centre National de la Recheche Scientifique) in Paris. Michel Deza's most important research contributions are in discrete, combinatorial and applied geometry, but his mathematical interests are much more broader and include areas where discrete geometry meets algebra, classical combinatorics, graph theory, number theory, optimization, analysis and applications. Many of his works have had impacts in other various scientific domains, especially organic chemistry (on fullerenes and symmetry) and crystallography (Frank–Kasper phases, alloys, and viruses). M. Deza has a strong impact on the development of all of these domains for well over forty years. From very early on, he was distinguished for his combinatorial geometry intuition and problem solving skills. -
Topology Distance: a Topology-Based Approach for Evaluating Generative Adversarial Networks
Topology Distance: A Topology-Based Approach For Evaluating Generative Adversarial Networks Danijela Horak 1 Simiao Yu 1 Gholamreza Salimi-Khorshidi 1 Abstract resemble real images Xr, while D discriminates between Xg Automatic evaluation of the goodness of Gener- and Xr. G and D are trained by playing a two-player mini- ative Adversarial Networks (GANs) has been a max game in a competing manner. Such novel adversarial challenge for the field of machine learning. In training process is a key factor in GANs’ success: It im- this work, we propose a distance complementary plicitly defines a learnable objective that is flexibly adaptive to existing measures: Topology Distance (TD), to various complicated image-generation tasks, in which it the main idea behind which is to compare the would be difficult or impossible to explicitly define such an geometric and topological features of the latent objective. manifold of real data with those of generated data. One of the biggest challenges in the field of generative More specifically, we build Vietoris-Rips com- models – including for GANs – is the automatic evaluation plex on image features, and define TD based on of the goodness of such models (e.g., whether or not the the differences in persistent-homology groups of data generated by such models are similar to the data they the two manifolds. We compare TD with the were trained on). Unlike supervised learning, where the most commonly-used and relevant measures in goodness of the models can be assessed by comparing their the field, including Inception Score (IS), Frechet´ predictions with the actual labels, or in some other deep- Inception Distance (FID), Kernel Inception Dis- learning models where the goodness of the model can be tance (KID) and Geometry Score (GS), in a range assessed using the likelihood of the validation data under the of experiments on various datasets. -
Lesson 3 – Understanding Distance in Space (Optional)
Lesson 3 – Understanding Distance in Space (optional) Background The distance between objects in space is vast and very difficult for most children to grasp. The values for these distances are cumbersome for astronomers and scientists to manipulate. Therefore, scientists use a unit of measurement called an astronomical unit. An astronomical unit is the average distance between the Earth and the Sun – 150 million kilometers. Using a scale model to portray the distances of the planets will help the students begin to understand the vastness of space. Astronomers soon found that even the astronomical unit was not large enough to measure the distance of objects outside of our solar system. For these distances, the parsec is used. A parsec is a unit of light-years. A parsec equals approximately 3.3 light-years. (Keep in mind that a light-year is the distance light travels in one year – 9.5 trillion km – and that light travels 300,000 km per second!) Teacher Notes and Hints Prior to lesson • Discuss and review measuring length or distance. How far is one meter? • Discuss the use of prefixes that add or subtract to “basic” units of length. Example: meter is the basic metric unit for length “kilo” means 1000 – kilometer is 1000 meters “centi” means 1/100 – centimeter is 1/100 of a meter Adapt the discussion for grade level. For example, fifth graders can learn the metric prefixes for more “lengths” and may add to decimal work in math class: Kilo – 1000 Hecto – 100 Deka – 10 Deci – 1/10 (0.1) Centi – 1/100 (0.01) Milli – 1/1000 (0.001) • When discussing kilometers, it is helpful to know the number of km’s to local places (for example, kilometers to the Mall). -
Lecture 24 Angular Momentum
LECTURE 24 ANGULAR MOMENTUM Instructor: Kazumi Tolich Lecture 24 2 ¨ Reading chapter 11-6 ¤ Angular momentum n Angular momentum about an axis n Newton’s 2nd law for rotational motion Angular momentum of an rotating object 3 ¨ An object with a moment of inertia of � about an axis rotates with an angular speed of � about the same axis has an angular momentum, �, given by � = �� ¤ This is analogous to linear momentum: � = �� Angular momentum in general 4 ¨ Angular momentum of a point particle about an axis is defined by � � = �� sin � = ��� sin � = �-� = ��. � �- ¤ �⃗: position vector for the particle from the axis. ¤ �: linear momentum of the particle: � = �� �⃗ ¤ � is moment arm, or sometimes called “perpendicular . Axis distance.” �. Quiz: 1 5 ¨ A particle is traveling in straight line path as shown in Case A and Case B. In which case(s) does the blue particle have non-zero angular momentum about the axis indicated by the red cross? A. Only Case A Case A B. Only Case B C. Neither D. Both Case B Quiz: 24-1 answer 6 ¨ Only Case A ¨ For a particle to have angular momentum about an axis, it does not have to be Case A moving in a circle. ¨ The particle can be moving in a straight path. Case B ¨ For it to have a non-zero angular momentum, its line of path is displaced from the axis about which the angular momentum is calculated. ¨ An object moving in a straight line that does not go through the axis of rotation has an angular position that changes with time. So, this object has an angular momentum.