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The Philosophy of Physics
The Philosophy of Physics ROBERTO TORRETTI University of Chile PUBLISHED BY THE PRESS SYNDICATE OF THE UNIVERSITY OF CAMBRIDGE The Pitt Building, Trumpington Street, Cambridge, United Kingdom CAMBRIDGE UNIVERSITY PRESS The Edinburgh Building, Cambridge CB2 2RU, UK www.cup.cam.ac.uk 40 West 20th Street, New York, NY 10011-4211, USA www.cup.org 10 Stamford Road, Oakleigh, Melbourne 3166, Australia Ruiz de Alarcón 13, 28014, Madrid, Spain © Roberto Torretti 1999 This book is in copyright. Subject to statutory exception and to the provisions of relevant collective licensing agreements, no reproduction of any part may take place without the written permission of Cambridge University Press. First published 1999 Printed in the United States of America Typeface Sabon 10.25/13 pt. System QuarkXPress [BTS] A catalog record for this book is available from the British Library. Library of Congress Cataloging-in-Publication Data is available. 0 521 56259 7 hardback 0 521 56571 5 paperback Contents Preface xiii 1 The Transformation of Natural Philosophy in the Seventeenth Century 1 1.1 Mathematics and Experiment 2 1.2 Aristotelian Principles 8 1.3 Modern Matter 13 1.4 Galileo on Motion 20 1.5 Modeling and Measuring 30 1.5.1 Huygens and the Laws of Collision 30 1.5.2 Leibniz and the Conservation of “Force” 33 1.5.3 Rømer and the Speed of Light 36 2 Newton 41 2.1 Mass and Force 42 2.2 Space and Time 50 2.3 Universal Gravitation 57 2.4 Rules of Philosophy 69 2.5 Newtonian Science 75 2.5.1 The Cause of Gravity 75 2.5.2 Central Forces 80 2.5.3 Analytical -
Dark Energy and Dark Matter As Inertial Effects Introduction
Dark Energy and Dark Matter as Inertial Effects Serkan Zorba Department of Physics and Astronomy, Whittier College 13406 Philadelphia Street, Whittier, CA 90608 [email protected] ABSTRACT A disk-shaped universe (encompassing the observable universe) rotating globally with an angular speed equal to the Hubble constant is postulated. It is shown that dark energy and dark matter are cosmic inertial effects resulting from such a cosmic rotation, corresponding to centrifugal (dark energy), and a combination of centrifugal and the Coriolis forces (dark matter), respectively. The physics and the cosmological and galactic parameters obtained from the model closely match those attributed to dark energy and dark matter in the standard Λ-CDM model. 20 Oct 2012 Oct 20 ph] - PACS: 95.36.+x, 95.35.+d, 98.80.-k, 04.20.Cv [physics.gen Introduction The two most outstanding unsolved problems of modern cosmology today are the problems of dark energy and dark matter. Together these two problems imply that about a whopping 96% of the energy content of the universe is simply unaccounted for within the reigning paradigm of modern cosmology. arXiv:1210.3021 The dark energy problem has been around only for about two decades, while the dark matter problem has gone unsolved for about 90 years. Various ideas have been put forward, including some fantastic ones such as the presence of ghostly fields and particles. Some ideas even suggest the breakdown of the standard Newton-Einstein gravity for the relevant scales. Although some progress has been made, particularly in the area of dark matter with the nonstandard gravity theories, the problems still stand unresolved. -
Foundations of Newtonian Dynamics: an Axiomatic Approach For
Foundations of Newtonian Dynamics: 1 An Axiomatic Approach for the Thinking Student C. J. Papachristou 2 Department of Physical Sciences, Hellenic Naval Academy, Piraeus 18539, Greece Abstract. Despite its apparent simplicity, Newtonian mechanics contains conceptual subtleties that may cause some confusion to the deep-thinking student. These subtle- ties concern fundamental issues such as, e.g., the number of independent laws needed to formulate the theory, or, the distinction between genuine physical laws and deriva- tive theorems. This article attempts to clarify these issues for the benefit of the stu- dent by revisiting the foundations of Newtonian dynamics and by proposing a rigor- ous axiomatic approach to the subject. This theoretical scheme is built upon two fun- damental postulates, namely, conservation of momentum and superposition property for interactions. Newton’s laws, as well as all familiar theorems of mechanics, are shown to follow from these basic principles. 1. Introduction Teaching introductory mechanics can be a major challenge, especially in a class of students that are not willing to take anything for granted! The problem is that, even some of the most prestigious textbooks on the subject may leave the student with some degree of confusion, which manifests itself in questions like the following: • Is the law of inertia (Newton’s first law) a law of motion (of free bodies) or is it a statement of existence (of inertial reference frames)? • Are the first two of Newton’s laws independent of each other? It appears that -
Dark Matter and the Early Universe: a Review Arxiv:2104.11488V1 [Hep-Ph
Dark matter and the early Universe: a review A. Arbey and F. Mahmoudi Univ Lyon, Univ Claude Bernard Lyon 1, CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, UMR 5822, 69622 Villeurbanne, France Theoretical Physics Department, CERN, CH-1211 Geneva 23, Switzerland Institut Universitaire de France, 103 boulevard Saint-Michel, 75005 Paris, France Abstract Dark matter represents currently an outstanding problem in both cosmology and particle physics. In this review we discuss the possible explanations for dark matter and the experimental observables which can eventually lead to the discovery of dark matter and its nature, and demonstrate the close interplay between the cosmological properties of the early Universe and the observables used to constrain dark matter models in the context of new physics beyond the Standard Model. arXiv:2104.11488v1 [hep-ph] 23 Apr 2021 1 Contents 1 Introduction 3 2 Standard Cosmological Model 3 2.1 Friedmann-Lema^ıtre-Robertson-Walker model . 4 2.2 A quick story of the Universe . 5 2.3 Big-Bang nucleosynthesis . 8 3 Dark matter(s) 9 3.1 Observational evidences . 9 3.1.1 Galaxies . 9 3.1.2 Galaxy clusters . 10 3.1.3 Large and cosmological scales . 12 3.2 Generic types of dark matter . 14 4 Beyond the standard cosmological model 16 4.1 Dark energy . 17 4.2 Inflation and reheating . 19 4.3 Other models . 20 4.4 Phase transitions . 21 5 Dark matter in particle physics 21 5.1 Dark matter and new physics . 22 5.1.1 Thermal relics . 22 5.1.2 Non-thermal relics . -
On the Origin of the Inertia: the Modified Newtonian Dynamics Theory
CORE Metadata, citation and similar papers at core.ac.uk Provided by Repositori Obert UdL ON THE ORIGIN OF THE INERTIA: THE MODIFIED NEWTONIAN DYNAMICS THEORY JAUME GINE¶ Abstract. The sameness between the inertial mass and the grav- itational mass is an assumption and not a consequence of the equiv- alent principle is shown. In the context of the Sciama's inertia theory, the sameness between the inertial mass and the gravita- tional mass is discussed and a certain condition which must be experimentally satis¯ed is given. The inertial force proposed by Sciama, in a simple case, is derived from the Assis' inertia the- ory based in the introduction of a Weber type force. The origin of the inertial force is totally justi¯ed taking into account that the Weber force is, in fact, an approximation of a simple retarded potential, see [18, 19]. The way how the inertial forces are also derived from some solutions of the general relativistic equations is presented. We wonder if the theory of inertia of Assis is included in the framework of the General Relativity. In the context of the inertia developed in the present paper we establish the relation between the constant acceleration a0, that appears in the classical Modi¯ed Newtonian Dynamics (M0ND) theory, with the Hubble constant H0, i.e. a0 ¼ cH0. 1. Inertial mass and gravitational mass The gravitational mass mg is the responsible of the gravitational force. This fact implies that two bodies are mutually attracted and, hence mg appears in the Newton's universal gravitation law m M F = G g g r: r3 According to Newton, inertia is an inherent property of matter which is independent of any other thing in the universe. -
Effective Description of Dark Matter As a Viscous Fluid
Motivation Framework Perturbation theory Effective viscosity Results FRG improvement Conclusions Effective Description of Dark Matter as a Viscous Fluid Nikolaos Tetradis University of Athens Work with: D. Blas, S. Floerchinger, M. Garny, U. Wiedemann . N. Tetradis University of Athens Effective Description of Dark Matter as a Viscous Fluid Motivation Framework Perturbation theory Effective viscosity Results FRG improvement Conclusions Distribution of dark and baryonic matter in the Universe Figure: 2MASS Galaxy Catalog (more than 1.5 million galaxies). N. Tetradis University of Athens Effective Description of Dark Matter as a Viscous Fluid Motivation Framework Perturbation theory Effective viscosity Results FRG improvement Conclusions Inhomogeneities Inhomogeneities are treated as perturbations on top of an expanding homogeneous background. Under gravitational attraction, the matter overdensities grow and produce the observed large-scale structure. The distribution of matter at various redshifts reflects the detailed structure of the cosmological model. Define the density field δ = δρ/ρ0 and its spectrum hδ(k)δ(q)i ≡ δD(k + q)P(k): . N. Tetradis University of Athens Effective Description of Dark Matter as a Viscous Fluid 31 timation method in its entirety, but it should be equally valid. 7.3. Comparison to other results Figure 35 compares our results from Table 3 (modeling approach) with other measurements from galaxy surveys, but must be interpreted with care. The UZC points may contain excess large-scale power due to selection function effects (Padmanabhan et al. 2000; THX02), and the an- gular SDSS points measured from the early data release sample are difficult to interpret because of their extremely broad window functions. -
Newtonian Particles
Newtonian Particles Steve Rotenberg CSE291: Physics Simulation UCSD Spring 2019 CSE291: Physics Simulation • Instructor: Steve Rotenberg ([email protected]) • Lecture: EBU3 4140 (TTh 5:00 – 6:20pm) • Office: EBU3 2210 (TTh 3:50– 4:50pm) • TA: Mridul Kavidayal ([email protected]) • Web page: https://cseweb.ucsd.edu/classes/sp19/cse291-d/index.html CSE291: Physics Simulation • Focus will be on physics of motion (dynamics) • Main subjects: – Solid mechanics (deformable bodies & fracture) – Fluid dynamics – Rigid body dynamics • Additional topics: – Vehicle dynamics – Galactic dynamics – Molecular modeling Programming Project • There will a single programming project over the quarter • You can choose one of the following options – Fracture modeling – Particle based fluids – Rigid body dynamics • Or you can suggest your own idea, but talk to me first • The project will involve implementing the physics, some level of collision detection and optimization, some level of visualization, and some level of user interaction • You can work on your own or in a group of two • You also have to do a presentation for the final and demo it live or show some rendered video • I will provide more details on the web page Grading • There will be two pop quizzes, each worth 5% of the total grade • For the project, you will have to demonstrate your current progress at two different times in the quarter (roughly 1/3 and 2/3 through). These will each be worth 10% of the total grade • The final presentation is worth 10% • The remaining 60% is for the content of the project itself Course Outline 1. Newtonian Particles 10.Poisson Equations 2. -
Classical Particle Trajectories‡
1 Variational approach to a theory of CLASSICAL PARTICLE TRAJECTORIES ‡ Introduction. The problem central to the classical mechanics of a particle is usually construed to be to discover the function x(t) that describes—relative to an inertial Cartesian reference frame—the positions assumed by the particle at successive times t. This is the problem addressed by Newton, according to whom our analytical task is to discover the solution of the differential equation d2x(t) m = F (x(t)) dt2 that conforms to prescribed initial data x(0) = x0, x˙ (0) = v0. Here I explore an alternative approach to the same physical problem, which we cleave into two parts: we look first for the trajectory traced by the particle, and then—as a separate exercise—for its rate of progress along that trajectory. The discussion will cast new light on (among other things) an important but frequently misinterpreted variational principle, and upon a curious relationship between the “motion of particles” and the “motion of photons”—the one being, when you think about it, hardly more abstract than the other. ‡ The following material is based upon notes from a Reed College Physics Seminar “Geometrical Mechanics: Remarks commemorative of Heinrich Hertz” that was presented February . 2 Classical trajectories 1. “Transit time” in 1-dimensional mechanics. To describe (relative to an inertial frame) the 1-dimensional motion of a mass point m we were taught by Newton to write mx¨ = F (x) − d If F (x) is “conservative” F (x)= dx U(x) (which in the 1-dimensional case is automatic) then, by a familiar line of argument, ≡ 1 2 ˙ E 2 mx˙ + U(x) is conserved: E =0 Therefore the speed of the particle when at x can be described 2 − v(x)= m E U(x) (1) and is determined (see the Figure 1) by the “local depth E − U(x) of the potential lake.” Several useful conclusions are immediate. -
Thomas Aquinas on the Separability of Accidents and Dietrich of Freiberg’S Critique
Thomas Aquinas on the Separability of Accidents and Dietrich of Freiberg’s Critique David Roderick McPike Thesis submitted to the Faculty of Graduate and Postdoctoral Studies in partial fulfillment of the requirements for the Doctorate in Philosophy degree in Philosophy Department of Philosophy Faculty of Arts University of Ottawa © David Roderick McPike, Ottawa, Canada, 2015 Abstract The opening chapter briefly introduces the Catholic doctrine of the Eucharist and the history of its appropriation into the systematic rational discourse of philosophy, as culminating in Thomas Aquinas’ account of transubstantiation with its metaphysical elaboration of the separability of accidents from their subject (a substance), so as to exist (supernaturally) without a subject. Chapter Two expounds St. Thomas’ account of the separability of accidents from their subject. It shows that Thomas presents a consistent rational articulation of his position throughout his works on the subject. Chapter Three expounds Dietrich of Freiberg’s rejection of Thomas’ view, examining in detail his treatise De accidentibus, which is expressly dedicated to demonstrating the utter impossibility of separate accidents. Especially in light of Kurt Flasch’s influential analysis of this work, which praises Dietrich for his superior level of ‘methodological consciousness,’ this chapter aims to be painstaking in its exposition and to comprehensively present Dietrich’s own views just as we find them, before taking up the task of critically assessing Dietrich’s position. Chapter Four critically analyses the competing doctrinal positions expounded in the preceding two chapters. It analyses the various elements of Dietrich’s case against Thomas and attempts to pinpoint wherein Thomas and Dietrich agree and wherein they part ways. -
Axion Dark Matter from Higgs Inflation with an Intermediate H∗
Axion dark matter from Higgs inflation with an intermediate H∗ Tommi Tenkanena and Luca Visinellib;c;d aDepartment of Physics and Astronomy, Johns Hopkins University, 3400 N. Charles Street, Baltimore, MD 21218, USA bDepartment of Physics and Astronomy, Uppsala University, L¨agerhyddsv¨agen1, 75120 Uppsala, Sweden cNordita, KTH Royal Institute of Technology and Stockholm University, Roslagstullsbacken 23, 10691 Stockholm, Sweden dGravitation Astroparticle Physics Amsterdam (GRAPPA), Institute for Theoretical Physics Amsterdam and Delta Institute for Theoretical Physics, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands E-mail: [email protected], [email protected], [email protected] Abstract. In order to accommodate the QCD axion as the dark matter (DM) in a model in which the Peccei-Quinn (PQ) symmetry is broken before the end of inflation, a relatively low scale of inflation has to be invoked in order to avoid bounds from DM isocurvature 9 fluctuations, H∗ . O(10 ) GeV. We construct a simple model in which the Standard Model Higgs field is non-minimally coupled to Palatini gravity and acts as the inflaton, leading to a 8 scale of inflation H∗ ∼ 10 GeV. When the energy scale at which the PQ symmetry breaks is much larger than the scale of inflation, we find that in this scenario the required axion mass for which the axion constitutes all DM is m0 . 0:05 µeV for a quartic Higgs self-coupling 14 λφ = 0:1, which correspond to the PQ breaking scale vσ & 10 GeV and tensor-to-scalar ratio r ∼ 10−12. Future experiments sensitive to the relevant QCD axion mass scale can therefore shed light on the physics of the Universe before the end of inflation. -
Modified Newtonian Dynamics, an Introductory Review
Modified Newtonian Dynamics, an Introductory Review Riccardo Scarpa European Southern Observatory, Chile E-mail [email protected] Abstract. By the time, in 1937, the Swiss astronomer Zwicky measured the velocity dispersion of the Coma cluster of galaxies, astronomers somehow got acquainted with the idea that the universe is filled by some kind of dark matter. After almost a century of investigations, we have learned two things about dark matter, (i) it has to be non-baryonic -- that is, made of something new that interact with normal matter only by gravitation-- and, (ii) that its effects are observed in -8 -2 stellar systems when and only when their internal acceleration of gravity falls below a fix value a0=1.2×10 cm s . Being completely decoupled dark and normal matter can mix in any ratio to form the objects we see in the universe, and indeed observations show the relative content of dark matter to vary dramatically from object to object. This is in open contrast with point (ii). In fact, there is no reason why normal and dark matter should conspire to mix in just the right way for the mass discrepancy to appear always below a fixed acceleration. This systematic, more than anything else, tells us we might be facing a failure of the law of gravity in the weak field limit rather then the effects of dark matter. Thus, in an attempt to avoid the need for dark matter many modifications of the law of gravity have been proposed in the past decades. The most successful – and the only one that survived observational tests -- is the Modified Newtonian Dynamics. -
Modified Newtonian Dynamics
Faculty of Mathematics and Natural Sciences Bachelor Thesis University of Groningen Modified Newtonian Dynamics (MOND) and a Possible Microscopic Description Author: Supervisor: L.M. Mooiweer prof. dr. E. Pallante Abstract Nowadays, the mass discrepancy in the universe is often interpreted within the paradigm of Cold Dark Matter (CDM) while other possibilities are not excluded. The main idea of this thesis is to develop a better theoretical understanding of the hidden mass problem within the paradigm of Modified Newtonian Dynamics (MOND). Several phenomenological aspects of MOND will be discussed and we will consider a possible microscopic description based on quantum statistics on the holographic screen which can reproduce the MOND phenomenology. July 10, 2015 Contents 1 Introduction 3 1.1 The Problem of the Hidden Mass . .3 2 Modified Newtonian Dynamics6 2.1 The Acceleration Constant a0 .................................7 2.2 MOND Phenomenology . .8 2.2.1 The Tully-Fischer and Jackson-Faber relation . .9 2.2.2 The external field effect . 10 2.3 The Non-Relativistic Field Formulation . 11 2.3.1 Conservation of energy . 11 2.3.2 A quadratic Lagrangian formalism (AQUAL) . 12 2.4 The Relativistic Field Formulation . 13 2.5 MOND Difficulties . 13 3 A Possible Microscopic Description of MOND 16 3.1 The Holographic Principle . 16 3.2 Emergent Gravity as an Entropic Force . 16 3.2.1 The connection between the bulk and the surface . 18 3.3 Quantum Statistical Description on the Holographic Screen . 19 3.3.1 Two dimensional quantum gases . 19 3.3.2 The connection with the deep MOND limit .