A Walk Through Time
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Floating and Platform Balances an Introduction
Floating and Platform Balances An introduction ©Darrah Artzner 3/2018 Floating and Platform Balances • Introduce main types • Discuss each in some detail including part identification and function • Testing and Inspecting • Cleaning tips • Lubrication • Performing repairs Balance Assembly Type Floating Platform Floating Balance Frame Spring stud Helicoid spring Hollow Tube Mounting Post Regulator Balance wheel Floating Balance cont. Jewel Roller Pin Paired weight Hollow Tube Safety Roller Pivot Wire Floating Balance cont. Example Retaining Hermle screws Safety Roller Note: moving fork Jewel cover Floating Balance cont. Inspecting and Testing (Balance assembly is removed from movement) • Inspect pivot (suspension) wire for distortion, corrosion, breakage. • Balance should appear to float between frame. Top and bottom distance. • Balance spring should be proportional and not distorted in any way. • Inspect jewels for cracks and or breakage. • Roller pin should be centered when viewed from front. (beat) • Rotate balance wheel three quarters of a turn (270°) and release. It should rotate smoothly with no distortion and should oscillate for several (3) minutes. Otherwise it needs attention. Floating Balance cont. Cleaning • Make sure the main spring has been let down before working on movement. • Use non-aqueous watch cleaner and/or rinse. • Agitate in cleaner/rinse by hand or briefly in ultrasonic. • Rinse twice and final in naphtha, Coleman fuel (or similar) or alcohol. • Allow to dry. (heat can be used with caution – ask me how I would do it.) Lubrication • There are two opinions. To lube or not to lube. • Place a vary small amount of watch oil on to the upper and lower jewel where the pivot wire passed through the jewel holes. -
Pendulum Time" Lesson Explores How the Pendulum Has Been a Reliable Way to Keep Time for Centuries
IEEE Lesson Plan: P endulum Time Explore other TryEngineering lessons at www.tryengineering.org L e s s o n F o c u s Lesson focuses on how pendulums have been used to measure time and how mechanical mechanism pendulum clocks operate. Students work in teams to develop a pendulum out of everyday objects that can reliably measure time and operate at two different speeds. They will determine the materials, the optimal length of swing or size of weight to adjust speed, and then develop their designs on paper. Next, they will build and test their mechanism, compare their results with other student teams, and share observations with their class. Lesson Synopsis The "Pendulum Time" lesson explores how the pendulum has been a reliable way to keep time for centuries. Students work in teams to build their own working clock using a pendulum out of every day materials. They will need to be able to speed up and slow down the motion of the pendulum clock. They sketch their plans, consider what materials they will need, build the clock, test it, reflect on the assignment, and present to their class. A g e L e v e l s 8-18. Objectives Learn about timekeeping and engineering. Learn about engineering design and redesign. Learn how engineering can help solve society's challenges. Learn about teamwork and problem solving. Anticipated Learner Outcomes As a result of this activity, students should develop an understanding of: timekeeping engineering design teamwork Pendulum Time Provided by IEEE as part of TryEngineering www.tryengineering.org © 2018 IEEE – All rights reserved. -
Coordinates and Proper Time
Coordinates and Proper Time Edmund Bertschinger, [email protected] January 31, 2003 Now it came to me: . the independence of the gravitational acceleration from the na- ture of the falling substance, may be expressed as follows: In a gravitational ¯eld (of small spatial extension) things behave as they do in a space free of gravitation. This happened in 1908. Why were another seven years required for the construction of the general theory of relativity? The main reason lies in the fact that it is not so easy to free oneself from the idea that coordinates must have an immediate metrical meaning. | A. Einstein (quoted in Albert Einstein: Philosopher-Scientist, ed. P.A. Schilpp, 1949). 1. Introduction These notes supplement Chapter 1 of EBH (Exploring Black Holes by Taylor and Wheeler). They elaborate on the discussion of bookkeeper coordinates and how coordinates are related to actual physical distances and times. Also, a brief discussion of the classic Twin Paradox of special relativity is presented in order to illustrate the principal of maximal (or extremal) aging. Before going to details, let us review some jargon whose precise meaning will be important in what follows. You should be familiar with these words and their meaning. Spacetime is the four- dimensional playing ¯eld for motion. An event is a point in spacetime that is uniquely speci¯ed by giving its four coordinates (e.g. t; x; y; z). Sometimes we will ignore two of the spatial dimensions, reducing spacetime to two dimensions that can be graphed on a sheet of paper, resulting in a Minkowski diagram. -
Collectable POCKET Watches 1750-1920
cOLLECTABLE POCKET watches 1750-1920 Ian Beilby Clocks Magazine Beginner’s Guide Series No 5 cOLLECTABLE POCKET watches 1750-1920 Ian Beilby Clocks Magazine Beginner’s Guide Series No 5 Published by Splat Publishing Ltd. 141b Lower Granton Road Edinburgh EH5 1EX United Kingdom www.clocksmagazine.com © 2017 Ian Beilby World copyright reserved ISBN: 978-0-9562732-4-6 The right of Ian Beilby to be identified as author of this work has been asserted in accordance with the Copyright, Designs and Patents Act 1988. All rights reserved. No part of this publication may be reproduced, stored in a retrieval system, or transmitted in any form or by any means electronic, mechanical, photocopying, recording or otherwise, without the prior permission of the publisher. 2 4 6 8 10 9 7 5 3 1 Printed by CBF Cheltenham Business Forms Ltd, 67 Hatherley Road, Cheltenham GL51 6EG CONTENTS Introduction 7 Chapter 1. The eighteenth century verge watch 13 Chapter 2. The nineteenth century verge watch 22 Chapter 3. The English cylinder and rack lever watch 36 Chapter 4. The English lever watch 42 Chapter 5. The Swiss lever watch 54 Chapter 6. The American lever watch 62 Chapter 7. The Swiss cylinder ladies’ fob watch 72 Chapter 8. Advice on collecting and maintenance 77 Appendix 1. Glossary 82 Appendix 2. Further reading 86 CLOCKS MAGAZINE BEGINNER’S GUIDE SERIES No. 1. Clock Repair, A Beginner’s Guide No. 2. Beginner’s Guide to Pocket Watches No. 3. American Clocks, An Introduction No. 4. What’s it Worth, Price Guide to Clocks 2014 No. -
On the Isochronism of Galilei's Horologium
IFToMM Workshop on History of MMS – Palermo 2013 On the isochronism of Galilei's horologium Francesco Sorge, Marco Cammalleri, Giuseppe Genchi DICGIM, Università di Palermo, [email protected], [email protected], [email protected] Abstract − Measuring the passage of time has always fascinated the humankind throughout the centuries. It is amazing how the general architecture of clocks has remained almost unchanged in practice to date from the Middle Ages. However, the foremost mechanical developments in clock-making date from the seventeenth century, when the discovery of the isochronism laws of pendular motion by Galilei and Huygens permitted a higher degree of accuracy in the time measure. Keywords: Time Measure, Pendulum, Isochronism Brief Survey on the Art of Clock-Making The first elements of temporal and spatial cognition among the primitive societies were associated with the course of natural events. In practice, the starry heaven played the role of the first huge clock of mankind. According to the philosopher Macrobius (4 th century), even the Latin term hora derives, through the Greek word ‘ώρα , from an Egyptian hieroglyph to be pronounced Heru or Horu , which was Latinized into Horus and was the name of the Egyptian deity of the sun and the sky, who was the son of Osiris and was often represented as a hawk, prince of the sky. Later on, the measure of time began to assume a rudimentary technical connotation and to benefit from the use of more or less ingenious devices. Various kinds of clocks developed to relatively high levels of accuracy through the Egyptian, Assyrian, Greek and Roman civilizations. -
Physics 2305 Lab 11: Torsion Pendulum
Name___________________ ID number_________________________ Date____________________ Lab partner_________________________ Lab CRN________________ Lab instructor_______________________ Physics 2305 Lab 11: Torsion Pendulum Objective 1. To demonstrate that the motion of the torsion pendulum satisfies the simple harmonic form in equation (3) 2. To show that the period (or angular frequency) of the simple harmonic motion of the torsion pendulum is independent of the amplitude of the motion 3. To make measurements to demonstrate the validity of equation (6), which relates the angular frequency of motion to the torsion constant and the moment of inertia of the torsion pendulum Useful background reading Young and Freedman, section 13.1, 13.2, 13.4 (the “angular SHM” section, specifically) Introduction A torsion pendulum is shown schematically to the right. A disk with moment of inertia I0 is fastened near the center of a long straight wire stretched between two fixed mounts. If the disk is rotated through an angle θ and released, the twist in the wire rotates the disk back toward equilibrium. It overshoots and I 0 oscillates back and forth like a pendulum, hence the name. Torsion pendulums are used for the timing element in some θ clocks. The most common variety is a decorative polished brass mechanism under a glass dome. You may have seen one. The balance wheel in an old fashioned mechanical watch is a kind of torsion pendulum, though the restoring force is provided by a flat coiled spring rather than a long twisted wire. Torsion pendulums can be made very accurate and have been used in numerous precision experiments in 1 physics. -
The Book of Common Prayer
The Book of Common Prayer and Administration of the Sacraments and Other Rites and Ceremonies of the Church Together with The Psalter or Psalms of David According to the use of The Episcopal Church Church Publishing Incorporated, New York Certificate I certify that this edition of The Book of Common Prayer has been compared with a certified copy of the Standard Book, as the Canon directs, and that it conforms thereto. Gregory Michael Howe Custodian of the Standard Book of Common Prayer January, 2007 Table of Contents The Ratification of the Book of Common Prayer 8 The Preface 9 Concerning the Service of the Church 13 The Calendar of the Church Year 15 The Daily Office Daily Morning Prayer: Rite One 37 Daily Evening Prayer: Rite One 61 Daily Morning Prayer: Rite Two 75 Noonday Prayer 103 Order of Worship for the Evening 108 Daily Evening Prayer: Rite Two 115 Compline 127 Daily Devotions for Individuals and Families 137 Table of Suggested Canticles 144 The Great Litany 148 The Collects: Traditional Seasons of the Year 159 Holy Days 185 Common of Saints 195 Various Occasions 199 The Collects: Contemporary Seasons of the Year 211 Holy Days 237 Common of Saints 246 Various Occasions 251 Proper Liturgies for Special Days Ash Wednesday 264 Palm Sunday 270 Maundy Thursday 274 Good Friday 276 Holy Saturday 283 The Great Vigil of Easter 285 Holy Baptism 299 The Holy Eucharist An Exhortation 316 A Penitential Order: Rite One 319 The Holy Eucharist: Rite One 323 A Penitential Order: Rite Two 351 The Holy Eucharist: Rite Two 355 Prayers of the People -
Lecture Notes 17: Proper Time, Proper Velocity, the Energy-Momentum 4-Vector, Relativistic Kinematics, Elastic/Inelastic
UIUC Physics 436 EM Fields & Sources II Fall Semester, 2015 Lect. Notes 17 Prof. Steven Errede LECTURE NOTES 17 Proper Time and Proper Velocity As you progress along your world line {moving with “ordinary” velocity u in lab frame IRF(S)} on the ct vs. x Minkowski/space-time diagram, your watch runs slow {in your rest frame IRF(S')} in comparison to clocks on the wall in the lab frame IRF(S). The clocks on the wall in the lab frame IRF(S) tick off a time interval dt, whereas in your 2 rest frame IRF( S ) the time interval is: dt dtuu1 dt n.b. this is the exact same time dilation formula that we obtained earlier, with: 2 2 uu11uc 11 and: u uc We use uurelative speed of an object as observed in an inertial reference frame {here, u = speed of you, as observed in the lab IRF(S)}. We will henceforth use vvrelative speed between two inertial systems – e.g. IRF( S ) relative to IRF(S): Because the time interval dt occurs in your rest frame IRF( S ), we give it a special name: ddt = proper time interval (in your rest frame), and: t = proper time (in your rest frame). The name “proper” is due to a mis-translation of the French word “propre”, meaning “own”. Proper time is different than “ordinary” time, t. Proper time is a Lorentz-invariant quantity, whereas “ordinary” time t depends on the choice of IRF - i.e. “ordinary” time is not a Lorentz-invariant quantity. 222222 The Lorentz-invariant interval: dI dx dx dx dx ds c dt dx dy dz Proper time interval: d dI c2222222 ds c dt dx dy dz cdtdt22 = 0 in rest frame IRF(S) 22t Proper time: ddtttt 21 t 21 11 Because d and are Lorentz-invariant quantities: dd and: {i.e. -
Class 3: Time Dilation, Lorentz Contraction, Relativistic Velocity Transformations
Class 3: Time dilation, Lorentz contraction, relativistic velocity transformations Transformation of time intervals Suppose two events are recorded in a laboratory (frame S), e.g. by a cosmic ray detector. Event A is recorded at location xa and time ta, and event B is recorded at location xb and time tb. We want to know the time interval between these events in an inertial frame, S ′, moving with relative to the laboratory at speed u. Using the Lorentz transform, ux x′=−γ() xut,,, yyzzt ′′′ = = =− γ t , (3.1) c2 we see, from the last equation, that the time interval in S ′ is u ttba′−= ′ γ() tt ba −− γ () xx ba − , (3.2) c2 i.e., the time interval in S ′ depends not only on the time interval in the laboratory but also in the separation. If the two events are at the same location in S, the time interval (tb− t a ) measured by a clock located at the events is called the proper time interval . We also see that, because γ >1 for all frames moving relative to S, the proper time interval is the shortest time interval that can be measured between the two events. The events in the laboratory frame are not simultaneous. Is there a frame, S ″ in which the separated events are simultaneous? Since tb′′− t a′′ must be zero, we see that velocity of S ″ relative to S must be such that u c( tb− t a ) β = = , (3.3) c xb− x a i.e., the speed of S ″ relative to S is the fraction of the speed of light equal to the time interval between the events divided by the light travel time between the events. -
SETTING up and MOVING a PENDULUM CLOCK by Brian Loomes, UK
SETTING UP AND MOVING A PENDULUM CLOCK by Brian Loomes, UK oving a pendulum This problem may face clock with anchor the novice in two different Mescapement can ways. Firstly as a clock be difficult unless you have that runs well in its present a little guidance. Of all position but that you need these the longcase clock to move. Or as a clock is trickiest because the that is new to you and that long pendulum calls for you need to assemble greater care at setting it in and set going for the very balance, usually known as first time—such as one you have just inherited or bought at auction. If it is the first of these then you can attempt to ignore my notes about levelling. But floors in different rooms or different houses seldom agree Figure 1. When moving an on levels, and you may eight-day longcase clock you eventually have to follow need to hold the weight lines through the whole process in place by taping round the of setting the clock level accessible part of the barrel. In and in beat. a complicated musical clock, Sometimes you can such as this by Thomas Lister of persuade a clock to run by Halifax, it is vital. having it at a silly angle, or by pushing old pennies or wooden wedges under the seatboard. But this is hardly ideal and next time you move the clock you start with the same performance all over again. setting it ‘in beat’. These My suggestion is that you notes deal principally with bite the bullet right away longcase clocks. -
Time for a Change?
TIME FOR A CHANGE? Raymond H.V. Gallucci, PhD., P.E.; Frederick, Maryland, USA [email protected] ABSTRACT This work was inspired by Hughes’ book The Binary Universe, which proposes a unique theory about the nature of time and its dominance over phenomena since as gravity and electromagnetic radiation. While Hughes treats time as variable and time dilation as a real phenomenon, I divert while retaining much of Hughes’ proposals to speculate that time is immutable and equivalent to change, albeit progressing at a fixed rate analogous to the fastest proposed by Hughes – the Planck time interval. Keywords: Time (dilation), Planck time, absolute zero, zero point energy, kinetic energy, Bohr hydrogen atom 1. INTRODUCTION In his book The Binary Universe, Hughes strives “to provide a more accurate, simpler and realistic view of relativity and to encourage QM [Quantum Mechanics] physicists to review and re-assess the relationship between QM and the Special and General [Relativity] theories. The book focuses firstly on the macro universe and takes a logical, deductive approach to investigating the nature of space-time and gravity … [W]e focus down to the quantum scale and an in-depth analysis of the nature of time itself is presented … I offer here an alternative theory for gravitation … Finally, … I present the inevitable conclusions about the nature of time and of the universe itself from the Planck scale upwards …” [1] I find much with which to agree in Hughes’ theories, in particular, the following: Time is independent of the physical void since there is no known cause or effect, or suggested mechanism that links the two … Quantum Mechanical Theory recognizes that there is more to the vacuum than simply empty void … Space, the void (or volume), or anything within the void, cannot “exist” without the passage of time. -
Relativity and Clocks
RELATIVITY AND CLOCKS Carroll 0. Alley Universityof Maryland CollegePark, Maryland Sumnary be mentioned. In this centennial year of the birth of Albert The internationaltimekeeping communityshould Einstein, it is fittingto review the revolutionary takegreat pride in the fact that the great stabil- andfundamental insights about time whichhe gave ity of cont-mporaryatomic clocks requires the us inthe Restricted Theory of Relativity (1905) first practical applications g Einstein's General and in the conseqences of the Principle of Equiv- Theory of Relativity.This circumstance can be ex- alence (l'. .The happiest thought of my life.. .") pected to produce a better understanding among whichhe developed (1907-1915) into histheory of physicists andengineers of the physical basis of gravityas curved space-time, the General Theory of gravity as curvedspace-time. For slow motions and Relativity. weak gravitational fields, such as we normally ex- perience on the earth, the primary curvature is It is of particularsignificance that the ex- thatof &, notspace. A body falls,according traordinary stability ofmodern atomicclocks has to Einstein's view, not because of the Newtonian recentlyallowed the experimental Study and accur- forcepulling it tothe earth, but because of the ate measurement of these basic effects of motion properties of time: clocksrun slower when moving and gravitationalpotential on time. Experiments andrun faster or slower, the higher or lower re- with aircraft flights and laser pulseremote time spectively they are in the earth's gravity field. comparison(Alley, Cutler, Reisse, Williams, et al, 1975)and an experiment with a rocketprobe (Vessot,Levine, et al, 1976) are brieflydes- Some Eventsin Einstein's cribed. Intellectual Development Properunderstanding and allowance for these Figure 1 shows Einstein in his study in Berlin remarkableeffects is now necessary for accurate several years after he hadbrought the General global time synchronization using ultrastable Theoryof Relativity to its complete form in 1915.