Why Does the Meter Beat the Second?
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Stranger Than Fiction the Tale of the Epic Voyage Made to Establish the Metric System Is an Intriguing and Exciting One
words Stranger than fiction The tale of the epic voyage made to establish the metric system is an intriguing and exciting one. Arago alone to complete the final readings Julyan Cartwright from Majorca. On Majorca, Arago chose ho thinks about science during a S’Eslop, a peak on the northwest coast, as vacation on the Balearic Islands? his viewpoint of Ibiza and Formentera. He WMajorca, Minorca, Ibiza and had a hut built on the summit and settled Formentera are holiday destinations par in with his instruments for the final series excellence, not places where famous scientists of measurements. But events didn’t go of the past lived and worked, or where great according to plan. experiments were carried out. But there was War broke out between France and Spain a moment in history when the Balearic in June 1808, while Arago was on the Islands were crucial for a major scientific summit of S’Eslop. Soon undertaking. Majorcans were com- It was 1806, and the French Bureau des menting that the nightly Longitudes had the task of determining the bonfires were signals Paris meridian — the line of longitude pass- and that Arago must be ing through Paris. At the time there was no a French spy, and a universally agreed prime meridian; it wasn’t detachment of soldiers until 1884 that an international congress was sent up the moun- decided it should be the one that passes tain to capture him. through Greenwich. The reason for deter- Arago got wind of this; Troubled trip: during François mining the meridian with precision wasn’t in his memoirs, he Arago’s year-long journey home map-making but the metric system. -
So, What Is Actually the Distance from the Equator to the Pole? – Overview of the Meridian Distance Approximations
the International Journal Volume 7 on Marine Navigation Number 2 http://www.transnav.eu and Safety of Sea Transportation June 2013 DOI: 10.12716/1001.07.02.14 So, What is Actually the Distance from the Equator to the Pole? – Overview of the Meridian Distance Approximations A. Weintrit Gdynia Maritime University, Gdynia, Poland ABSTRACT: In the paper the author presents overview of the meridian distance approximations. He would like to find the answer for the question what is actually the distance from the equator to the pole ‐ the polar distance. In spite of appearances this is not such a simple question. The problem of determining the polar distance is a great opportunity to demonstrate the multitude of possible solutions in common use. At the beginning of the paper the author discusses some approximations and a few exact expressions (infinite sums) to calculate perimeter and quadrant of an ellipse, he presents convenient measurement units of the distance on the surface of the Earth, existing methods for the solution of the great circle and great elliptic sailing, and in the end he analyses and compares geodetic formulas for the meridian arc length. 1 INTRODUCTION navigational receivers and navigational systems (ECDIS and ECS [Weintrit, 2009]) suggest the Unfortunately, from the early days of the necessity of a thorough examination, modification, development of the basic navigational software built verification and unification of the issue of sailing into satellite navigational receivers and later into calculations for navigational systems and receivers. electronic chart systems, it has been noted that for the The problem of determining the distance from the sake of simplicity and a number of other, often equator to the pole is a great opportunity to incomprehensible reasons, this navigational software demonstrate the multitude of possible solutions in is often based on the simple methods of limited common use. -
The Swinging Spring: Regular and Chaotic Motion
References The Swinging Spring: Regular and Chaotic Motion Leah Ganis May 30th, 2013 Leah Ganis The Swinging Spring: Regular and Chaotic Motion References Outline of Talk I Introduction to Problem I The Basics: Hamiltonian, Equations of Motion, Fixed Points, Stability I Linear Modes I The Progressing Ellipse and Other Regular Motions I Chaotic Motion I References Leah Ganis The Swinging Spring: Regular and Chaotic Motion References Introduction The swinging spring, or elastic pendulum, is a simple mechanical system in which many different types of motion can occur. The system is comprised of a heavy mass, attached to an essentially massless spring which does not deform. The system moves under the force of gravity and in accordance with Hooke's Law. z y r φ x k m Leah Ganis The Swinging Spring: Regular and Chaotic Motion References The Basics We can write down the equations of motion by finding the Lagrangian of the system and using the Euler-Lagrange equations. The Lagrangian, L is given by L = T − V where T is the kinetic energy of the system and V is the potential energy. Leah Ganis The Swinging Spring: Regular and Chaotic Motion References The Basics In Cartesian coordinates, the kinetic energy is given by the following: 1 T = m(_x2 +y _ 2 +z _2) 2 and the potential is given by the sum of gravitational potential and the spring potential: 1 V = mgz + k(r − l )2 2 0 where m is the mass, g is the gravitational constant, k the spring constant, r the stretched length of the spring (px2 + y 2 + z2), and l0 the unstretched length of the spring. -
Integration Processes of Italian Immigrants in the Republic of Nobles
Odrodzenie i Reformacja w Polsce PL ISSN 0029‑8514 Special Issue Wojciech Tygielski (Warszawa) Together or Apart? Integration Processes of Italian Immigrants in the Republic of Nobles There has been quite a lot written on activities of the Italians in the Polish‑Lithuanian Commonwealth. We have many facts about the lives and achievements of many outstanding figures, especially art‑ ists (architects and builders, musicians, people of theatre) as well as merchants and enterprisers. And despite all that, the phenomenon of Italian immigration to the territory of the Polish‑Lithuanian state seems to have been insufficiently examined – both from the perspective of Italian motivations and extent of fulfilment of their life plans related to Poland, and from the perspective of consequences of the Italian presence for the old Polish society – both in the sphere of culture and politics, and economy. Thus, a relative advancement of studies is accompanied by an ignorance (generally, although not always, being a consequence of scarcity of sources) in fundamental questions – a number of Italian immigrants and chronology of their arrival to Poland, their professional structure, and their territorial settlement, especially outside big cities. There is a need for further studies exploring the goals set by individuals belonging to this very diverse community, and assessing the extent to which they were fulfilled. First and foremost, however, it is the scale of impact those Italian ar‑ rivals had on various factions and communities of the old‑Polish society. The whole picture of this process will be very difficult to reconstruct. Before I attempt to do so, I would like to present a few remarks and doubts about the level of their integration and possible group solidarity that characterised the Italian minority in the Commonwealth. -
Dynamics of the Elastic Pendulum Qisong Xiao; Shenghao Xia ; Corey Zammit; Nirantha Balagopal; Zijun Li Agenda
Dynamics of the Elastic Pendulum Qisong Xiao; Shenghao Xia ; Corey Zammit; Nirantha Balagopal; Zijun Li Agenda • Introduction to the elastic pendulum problem • Derivations of the equations of motion • Real-life examples of an elastic pendulum • Trivial cases & equilibrium states • MATLAB models The Elastic Problem (Simple Harmonic Motion) 푑2푥 푑2푥 푘 • 퐹 = 푚 = −푘푥 = − 푥 푛푒푡 푑푡2 푑푡2 푚 • Solve this differential equation to find 푥 푡 = 푐1 cos 휔푡 + 푐2 sin 휔푡 = 퐴푐표푠(휔푡 − 휑) • With velocity and acceleration 푣 푡 = −퐴휔 sin 휔푡 + 휑 푎 푡 = −퐴휔2cos(휔푡 + 휑) • Total energy of the system 퐸 = 퐾 푡 + 푈 푡 1 1 1 = 푚푣푡2 + 푘푥2 = 푘퐴2 2 2 2 The Pendulum Problem (with some assumptions) • With position vector of point mass 푥 = 푙 푠푖푛휃푖 − 푐표푠휃푗 , define 푟 such that 푥 = 푙푟 and 휃 = 푐표푠휃푖 + 푠푖푛휃푗 • Find the first and second derivatives of the position vector: 푑푥 푑휃 = 푙 휃 푑푡 푑푡 2 푑2푥 푑2휃 푑휃 = 푙 휃 − 푙 푟 푑푡2 푑푡2 푑푡 • From Newton’s Law, (neglecting frictional force) 푑2푥 푚 = 퐹 + 퐹 푑푡2 푔 푡 The Pendulum Problem (with some assumptions) Defining force of gravity as 퐹푔 = −푚푔푗 = 푚푔푐표푠휃푟 − 푚푔푠푖푛휃휃 and tension of the string as 퐹푡 = −푇푟 : 2 푑휃 −푚푙 = 푚푔푐표푠휃 − 푇 푑푡 푑2휃 푚푙 = −푚푔푠푖푛휃 푑푡2 Define 휔0 = 푔/푙 to find the solution: 푑2휃 푔 = − 푠푖푛휃 = −휔2푠푖푛휃 푑푡2 푙 0 Derivation of Equations of Motion • m = pendulum mass • mspring = spring mass • l = unstreatched spring length • k = spring constant • g = acceleration due to gravity • Ft = pre-tension of spring 푚푔−퐹 • r = static spring stretch, 푟 = 푡 s 푠 푘 • rd = dynamic spring stretch • r = total spring stretch 푟푠 + 푟푑 Derivation of Equations of Motion -
Vicious Circle”: Unscrambling A.-C
CORE Metadata, citation and similar papers at core.ac.uk Provided by Elsevier - Publisher Connector HISTORIA MATHEMATICA 15 t 19881, 228-239 Breaking a “Vicious Circle”: Unscrambling A.-C. Clairaut’s Iterative Method of 1743 JOHN L. GREENBERG Centre de Recherches Alexar~dre KoyrC, 12. rue Colherf. 75.002 Puris. FI.N~C.C In this paper 1 show how in 1743 A.-C. Clairaut applied an iterative method to calculate the ellipticity of an infinitesimally flattened, homogeneous ellipsoid of revolution in equilib- rium, taken to represent the earth. Clairaut did not make very clear what he was doing and, as a result, left certain readers in the dark. They could not understand the point of the calculation and erroneously thought that Clairaut was going around in circles. The paper ends with a discussion of Clairaut’s clarification of the calculation, published in 1760 in response to the criticisms of John Muller, and a brief comparison of Clairaut’s iterative method with the “Newton-Raphson Method.” 1 1988.4cademlc Pres\. Inc. Dans cet article je montre la methode d’approximation d’A.-C. Clairaut pour trouver I’ellipticite d’un ellipsoi’de homogene de revolution en equilibre dont l’ellipticitt est infinite- simale et qui reprtsente la terre. Certains lecteurs ont mal compris Clairaut. Ceux-ci ont cru Clairaut pris au piege dans un “cercle vicieux en logique.” Clairaut a repondu a son critique John Muller en 1760, et j’explique cette reponse. Mon article se termine par une breve comparaison de la methode de Clairaut et de celle dite “Newton-Raphson.” Cette com- paraison peut eclairer la cause du malentendu. -
Varying Constants, Gravitation and Cosmology
Varying constants, Gravitation and Cosmology Jean-Philippe Uzan Institut d’Astrophysique de Paris, UMR-7095 du CNRS, Universit´ePierre et Marie Curie, 98 bis bd Arago, 75014 Paris (France) and Department of Mathematics and Applied Mathematics, Cape Town University, Rondebosch 7701 (South Africa) and National Institute for Theoretical Physics (NITheP), Stellenbosch 7600 (South Africa). email: [email protected] http//www2.iap.fr/users/uzan/ September 29, 2010 Abstract Fundamental constants are a cornerstone of our physical laws. Any constant varying in space and/or time would reflect the existence of an almost massless field that couples to mat- ter. This will induce a violation of the universality of free fall. It is thus of utmost importance for our understanding of gravity and of the domain of validity of general relativity to test for their constancy. We thus detail the relations between the constants, the tests of the local posi- tion invariance and of the universality of free fall. We then review the main experimental and observational constraints that have been obtained from atomic clocks, the Oklo phenomenon, Solar system observations, meteorites dating, quasar absorption spectra, stellar physics, pul- sar timing, the cosmic microwave background and big bang nucleosynthesis. At each step we arXiv:1009.5514v1 [astro-ph.CO] 28 Sep 2010 describe the basics of each system, its dependence with respect to the constants, the known systematic effects and the most recent constraints that have been obtained. We then describe the main theoretical frameworks in which the low-energy constants may actually be varying and we focus on the unification mechanisms and the relations between the variation of differ- ent constants. -
From Lacaille to Gill and the Start of the Arc of the 30 Meridian
From LaCaille to Gill and the start of the Arc of the 30th Meridian Jim R. SMITH, United Kingdom Key words: LaCaille. Maclear. Gill. Meridian Arcs. 30th Arc. SUMMARY If one looks at a map of European arcs of meridian and parallel at the beginning of the 20th century there will be seen to be a plethora them. Turning to Africa there was the complete opposite. Other than the arcs of Eratosthenes (c 300 BC) and the short arcs by LaCaille (1752) and Maclear (1841-48) the continent was empty. It was in 1879 that David Gill had the idea for a Cape to Cairo meridian arc but 1954 before it was completed. This presentation summaries the work of LaCaille and Maclear and then concentrates on a description of the 30th Meridian Arc in East Africa. The only other comparable arcs at the time were that through the centre of India by Lambton and Everest observed between 1800 and 1843; the Struve arc of 1816 to 1852 and the various arcs in France during the 18th century. The usefulness of such arcs was highlighted in 2005 with the inscription by UNESCO of the Struve Geodetic Arc on the World Heritage Monument list. A practical extension to the Struve Arc Monument is the 30th Meridian Arc since there is a connection between the two. At an ICA Symposium in Cape Town, 2003, Lindsay Braun gave a presentation that detailed the political machinations of the history of the 30th Arc; here it is hoped to fill in other aspects of this work including some facts and figures since that is what surveyors thrive upon. -
Significance of Beating Observed in Earthquake Responses of Buildings
SIGNIFICANCE OF BEATING OBSERVED IN EARTHQUAKE RESPONSES OF BUILDINGS Mehmet Çelebi1, S. Farid Ghahari2, and Ertuğrul Taciroǧlu2 U.S. Geological Survey1 and University of California, Los Angeles2 Menlo Park, California, USA1 and Los Angeles, California, USA2 Abstract The beating phenomenon observed in the recorded responses of a tall building in Japan and another in the U.S. are examined in this paper. Beating is a periodic vibrational behavior caused by distinctive coupling between translational and torsional modes that typically have close frequencies. Beating is prominent in the prolonged resonant responses of lightly damped structures. Resonances caused by site effects also contribute to accentuating the beating effect. Spectral analyses and system identification techniques are used herein to quantify the periods and amplitudes of the beating effects from the strong motion recordings of the two buildings. Quantification of beating effects is a first step towards determining remedial actions to improve resilient building performance to strong earthquake induced shaking. Introduction In a cursory survey of several textbooks on structural dynamics, it can be seen that beating effects have not been included in their scopes. On the other hand, as more earthquake response records from instrumented buildings became available, it also became evident that the beating phenomenon is common. As modern digital equipment routinely provide recordings of prolonged responses of structures, we were prompted to visit the subject of beating, since such response characteristics may impact the instantaneous and long-term shaking performances of buildings during large or small earthquakes. The main purpose in deploying seismic instruments in buildings (and other structures) is to record their responses during seismic events to facilitate studies understanding and assessing their behavior and performances during and future strong shaking events. -
Geodesy Methods Over Time
Geodesy methods over time GISC3325 - Lecture 4 Astronomic Latitude/Longitude • Given knowledge of the positions of an astronomic body e.g. Sun or Polaris and our time we can determine our location in terms of astronomic latitude and longitude. US Meridian Triangulation This map shows the first project undertaken by the founding Superintendent of the Survey of the Coast Ferdinand Hassler. Triangulation • Method of indirect measurement. • Angles measured at all nodes. • Scaled provided by one or more precisely measured base lines. • First attributed to Gemma Frisius in the 16th century in the Netherlands. Early surveying instruments Left is a Quadrant for angle measurements, below is how baseline lengths were measured. A non-spherical Earth • Willebrod Snell van Royen (Snellius) did the first triangulation project for the purpose of determining the radius of the earth from measurement of a meridian arc. • Snellius was also credited with the law of refraction and incidence in optics. • He also devised the solution of the resection problem. At point P observations are made to known points A, B and C. We solve for P. Jean Picard’s Meridian Arc • Measured meridian arc through Paris between Malvoisine and Amiens using triangulation network. • First to use a telescope with cross hairs as part of the quadrant. • Value obtained used by Newton to verify his law of gravitation. Ellipsoid Earth Model • On an expedition J.D. Cassini discovered that a one-second pendulum regulated at Paris needed to be shortened to regain a one-second oscillation. • Pendulum measurements are effected by gravity! Newton • Newton used measurements of Picard and Halley and the laws of gravitation to postulate a rotational ellipsoid as the equilibrium figure for a homogeneous, fluid, rotating Earth. -
OF Versailles
THE CHÂTEAU DE VErSAILLES PrESENTS science & CUrIOSITIES AT THE COUrT OF versailles AN EXHIBITION FrOM 26 OCTOBEr 2010 TO 27 FEBrUArY 2011 3 Science and Curiosities at the Court of Versailles CONTENTS IT HAPPENED AT VErSAILLES... 5 FOrEWOrD BY JEAN-JACqUES AILLAGON 7 FOrEWOrD BY BÉATrIX SAULE 9 PrESS rELEASE 11 PArT I 1 THE EXHIBITION - Floor plan 3 - Th e exhibition route by Béatrix Saule 5 - Th e exhibition’s design 21 - Multimedia in the exhibition 22 PArT II 1 ArOUND THE EXHIBITION - Online: an Internet site, and TV web, a teachers’ blog platform 3 - Publications 4 - Educational activities 10 - Symposium 12 PArT III 1 THE EXHIBITION’S PArTNErS - Sponsors 3 - Th e royal foundations’ institutional heirs 7 - Partners 14 APPENDICES 1 USEFUL INFOrMATION 3 ILLUSTrATIONS AND AUDIOVISUAL rESOUrCES 5 5 Science and Curiosities at the Court of Versailles IT HAPPENED AT VErSAILLES... DISSECTION OF AN Since then he has had a glass globe made that ELEPHANT WITH LOUIS XIV is moved by a big heated wheel warmed by holding IN ATTENDANCE the said globe in his hand... He performed several experiments, all of which were successful, before Th e dissection took place at Versailles in January conducting one in the big gallery here... it was 1681 aft er the death of an elephant from highly successful and very easy to feel... we held the Congo that the king of Portugal had given hands on the parquet fl oor, just having to make Louis XIV as a gift : “Th e Academy was ordered sure our clothes did not touch each other.” to dissect an elephant from the Versailles Mémoires du duc de Luynes Menagerie that had died; Mr. -
Redalyc.The International Pendulum Project
Revista Electrónica de Investigación en Educación en Ciencias E-ISSN: 1850-6666 [email protected] Universidad Nacional del Centro de la Provincia de Buenos Aires Argentina Matthews, Michael R. The International Pendulum Project Revista Electrónica de Investigación en Educación en Ciencias, vol. 1, núm. 1, octubre, 2006, pp. 1-5 Universidad Nacional del Centro de la Provincia de Buenos Aires Buenos Aires, Argentina Available in: http://www.redalyc.org/articulo.oa?id=273320433002 How to cite Complete issue Scientific Information System More information about this article Network of Scientific Journals from Latin America, the Caribbean, Spain and Portugal Journal's homepage in redalyc.org Non-profit academic project, developed under the open access initiative Año 1 – Número 1 – Octubre de 2006 ISSN: en trámite The International Pendulum Project Michael R. Matthews [email protected] School of Education, University of New South Wales, Sydney 2052, Australia The Pendulum in Modern Science Galileo in his final great work, The Two New Sciences , written during the period of house arrest after the trial that, for many, marked the beginning of the Modern Age, wrote: We come now to the other questions, relating to pendulums, a subject which may appear to many exceedingly arid, especially to those philosophers who are continually occupied with the more profound questions of nature. Nevertheless, the problem is one which I do not scorn. I am encouraged by the example of Aristotle whom I admire especially because he did not fail to discuss every subject which he thought in any degree worthy of consideration. (Galileo 1638/1954, pp.94-95) This was the pendulum’s low-key introduction to the stage of modern science and modern society.