William Rowan Hamilton
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Vector Calculus and Multiple Integrals Rob Fender, HT 2018
Vector Calculus and Multiple Integrals Rob Fender, HT 2018 COURSE SYNOPSIS, RECOMMENDED BOOKS Course syllabus (on which exams are based): Double integrals and their evaluation by repeated integration in Cartesian, plane polar and other specified coordinate systems. Jacobians. Line, surface and volume integrals, evaluation by change of variables (Cartesian, plane polar, spherical polar coordinates and cylindrical coordinates only unless the transformation to be used is specified). Integrals around closed curves and exact differentials. Scalar and vector fields. The operations of grad, div and curl and understanding and use of identities involving these. The statements of the theorems of Gauss and Stokes with simple applications. Conservative fields. Recommended Books: Mathematical Methods for Physics and Engineering (Riley, Hobson and Bence) This book is lazily referred to as “Riley” throughout these notes (sorry, Drs H and B) You will all have this book, and it covers all of the maths of this course. However it is rather terse at times and you will benefit from looking at one or both of these: Introduction to Electrodynamics (Griffiths) You will buy this next year if you haven’t already, and the chapter on vector calculus is very clear Div grad curl and all that (Schey) A nice discussion of the subject, although topics are ordered differently to most courses NB: the latest version of this book uses the opposite convention to polar coordinates to this course (and indeed most of physics), but older versions can often be found in libraries 1 Week One A review of vectors, rotation of coordinate systems, vector vs scalar fields, integrals in more than one variable, first steps in vector differentiation, the Frenet-Serret coordinate system Lecture 1 Vectors A vector has direction and magnitude and is written in these notes in bold e.g. -
Blanchardstown Urban Structure Plan Development Strategy and Implementation
BLANCHARDSTOWN DEVELOPMENT STRATEGY URBAN STRUCTURE PLAN AND IMPLEMENTATION VISION, DEVELOPMENT THEMES AND OPPORTUNITIES PLANNING DEPARTMENT SPRING 2007 BLANCHARDSTOWN URBAN STRUCTURE PLAN DEVELOPMENT STRATEGY AND IMPLEMENTATION VISION, DEVELOPMENT THEMES AND OPPORTUNITIES PLANNING DEPARTMENT • SPRING 2007 David O’Connor, County Manager Gilbert Power, Director of Planning Joan Caffrey, Senior Planner BLANCHARDSTOWN URBAN STRUCTURE PLAN E DEVELOPMENT STRATEGY AND IMPLEMENTATION G A 01 SPRING 2007 P Contents Page INTRODUCTION . 2 SECTION 1: OBJECTIVES OF THE BLANCHARDSTOWN URBAN STRUCTURE PLAN – DEVELOPMENT STRATEGY 3 BACKGROUND PLANNING TO DATE . 3 VISION STATEMENT AND KEY ISSUES . 5 SECTION 2: DEVELOPMENT THEMES 6 INTRODUCTION . 6 THEME: COMMERCE RETAIL AND SERVICES . 6 THEME: SCIENCE & TECHNOLOGY . 8 THEME: TRANSPORT . 9 THEME: LEISURE, RECREATION & AMENITY . 11 THEME: CULTURE . 12 THEME: FAMILY AND COMMUNITY . 13 SECTION 3: DEVELOPMENT OPPORTUNITIES – ESSENTIAL INFRASTRUCTURAL IMPROVEMENTS 14 SECTION 4: DEVELOPMENT OPPORTUNITY AREAS 15 Area 1: Blanchardstown Town Centre . 16 Area 2: Blanchardstown Village . 19 Area 3: New District Centre at Coolmine, Porterstown, Clonsilla . 21 Area 4: Blanchardstown Institute of Technology and Environs . 24 Area 5: Connolly Memorial Hospital and Environs . 25 Area 6: International Sports Campus at Abbotstown. (O.P.W.) . 26 Area 7: Existing and Proposed District & Neighbourhood Centres . 27 Area 8: Tyrrellstown & Environs Future Mixed Use Development . 28 Area 9: Hansfield SDZ Residential and Mixed Use Development . 29 Area 10: North Blanchardstown . 30 Area 11: Dunsink Lands . 31 SECTION 5: RECOMMENDATIONS & CONCLUSIONS 32 BLANCHARDSTOWN URBAN STRUCTURE PLAN E G DEVELOPMENT STRATEGY AND IMPLEMENTATION A 02 P SPRING 2007 Introduction Section 1 details the key issues and need for an Urban Structure Plan – Development Strategy as the planning vision for the future of Blanchardstown. -
A2241: Clusters with Head-Tails at X-Rays L. Norci
A2241: CLUSTERS WITH HEAD-TAILS AT X-RAYS L. NORCI Dunsink Observatory Castleknock, Dublin 15, Ireland L. FERETTI Istituto di Radio Astronomia Via Gobetti 101, 1-40129 Bologna, Italy AND E.J.A. MEURS Dunsink Observatory Castleknock, Dublin 15, Ireland Abstract. A ROSAT Ρ SPC image of the galaxy cluster Abell 2241 has been obtained, showing X-ray emission from the intracluster medium and from individual objects. The brightness distribution of the cluster gas is used to assess the physical conditions at the location of two tailed radio galaxies (in A2241E and A2241W, at different redshifts). Together with radio and X-ray information on the two galaxies themselves the results are of relevance to the question of energy equipartition in radio sources. 1. Background A cluster intergalactic medium plays an important role in determining the morphology and evolution of radio sources. The external gas can interact with a radio source in different ways: confining the source, modifying the source morphology via ram-pressure and possibly feeding the active nucleus. We have obtained ROSAT X-ray data of the region of the cluster Abell 2241, which was previously studied by Bijleveld & Valentijn (1982). A2241 was originally classified as an irregular galaxy cluster, until redshift mea- surements showed it to consist of two separate clusters projected onto each other: A2241W and A2241E, located at redshifts of 0.0635 and 0.1021, respectively. 361 R. Ekers et al. (eds.), Extragalactic Radio Sources, 361-362. © 1996 IAU. Printed in the Netherlands. Downloaded from https://www.cambridge.org/core. IP address: 170.106.33.14, on 29 Sep 2021 at 08:43:38, subject to the Cambridge Core terms of use, available at https://www.cambridge.org/core/terms. -
Generated on 2012-08-23 18:24 GMT
1SS5 mtt TEGfiNIG. OLD SERIES, NO. II. NEW SERIES, NO. 8. University of Michigan Engineering Society. ALEX. M. HAUBRICH, HEMAN BURR LEONARD, Managing Editor. Business Manager. THOMAS DURAND McCOLL, HOMER WILSON WYCKOFF, CHARLES HENRY SPENCER. THE DETROIT OBSERVATORY OF THE UNIVERSITY OF MICHIGAN. ASAPH HALL, JR., PH.D. This Observatory was built about 1854 through the efforts of Presi- dent Tappan, money for the purpose being raised in Detroit. Mr. Henry N. Walker of Detroit was especially interested in the project and gave funds for the purchase of a meridian circle. The Observatory building is of the usual old-fashioned type, a cen- tral part on the top of which is the dome for the equatorial, and eaBt and west wings, the meridian circle being in the east wing and the library in the west. All the walls are of heavy masonry. About 1853 Dr. Tappan visited Europe and consulted Encke, direc- tor of the Berlin Observatory and Professor of Astronomy in the Uni- versity of Berlin, with regard to the Ann Arbor Observatory. By his advice a meridian circle was ordered of Pistor and Martins and a clock of Tiede. At this time Francis Brunnow was first assistant in the Berlin Obser- vatory. Probably it was through Encke that Brunnow came, in 1854, to- the University of Michigan as the first Professor of Astronomy and. Generated on 2012-08-23 18:24 GMT / http://hdl.handle.net/2027/mdp.39015071371267 Open Access, Google-digitized / http://www.hathitrust.org/access_use#oa-google 10 Thk Technic. Director of the Observatory. 1 think it likely that the 12} inch Fitz equatorial was ordered before his coming; but it was not delivered till after he was on the ground. -
PDF < Theory of Screws: a Study in the Dynamics of a Rigid Body (1876
Theory of Screws: A Study in the Dynamics of a Rigid Body... ~ PDF ^ ILWU0YQOFY Theory of Screws: A Study in the Dynamics of a Rigid Body (1876) by Robert Stawe By Robert Stawell Ball Createspace Independent Publishing Platform, United States, 2016. Paperback. Book Condition: New. 229 x 152 mm. Language: English . Brand New Book ***** Print on Demand *****.Sir Robert Stawell Ball FRS (1 July 1840 - 25 November 1913) was an Irish astronomerwho founded the screw theory He was the son of naturalist Robert Ball[2] and Amelia Gresley Hellicar. He was born in Dublin. Ball worked for Lord Rosse from 1865 to 1867. In 1867 he became Professor of Applied Mathematics at the Royal College of Science in Dublin. There he lectured on mechanics and published an elementary account of the science. In 1874 Ball was appointed Royal Astronomer of Ireland and Andrews Professor of Astronomy in the University of Dublin at Dunsink Observatory. Ball contributed to the science of kinematics by delineating the screw displacement: When Ball and the screw theorists speak of screws they no longer mean actual cylindrical objects with helical threads cut into them but the possible motion of any body whatsoever, including that of the screw independently of the nut. READ ONLINE [ 5.33 MB ] Reviews I actually began looking over this pdf. This can be for all those who statte there was not a worthy of reading through. I am easily can get a enjoyment of reading through a written publication. -- Rafael Feeney Jr. Great electronic book and useful one. Better then never, though i am quite late in start reading this one. -
Course Material
SREENIVASA INSTITUTE of TECHNOLOGY and MANAGEMENT STUDIES (autonomous) (ENGINEERING MATHEMATICS-III) Course Material II- B.TECH / I - SEMESTER regulation: r18 Course Code: 18SAH211 Compiled by Department OF MATHEMATICS Unit-I: Numerical Integration Source:https://www.intmath.com/integration/integration-intro.php Numerical Integration: Simpson’s 1/3- Rule Note: While applying the Simpson’s 1/3 rule, the number of sub-intervals (n) should be taken as multiple of 2. Simpson’s 3/8- Rule Note: While applying the Simpson’s 3/8 rule, the number of sub-intervals (n) should be taken as multiple of 3. Numerical solution of ordinary differential equations Taylor’s Series Method Picard’s Method Euler’s Method Runge-Kutta Formula UNIT-II Multiple Integrals 1. Double Integration Evaluation of Double Integration Triple Integration UNIT-III Partial Differential Equations Partial differential equations are those equations which contain partial differential coefficients, independent variables and dependent variables. The independent variables are denoted by x and y and dependent variable by z. the partial differential coefficients are denoted as follows The order of the partial differential equation is the same as that of the order of the highest differential coefficient in it. UNIT-IV Vector Differentiation Elementary Vector Analysis Definition (Scalar and vector): Scalar is a quantity that has magnitude but not direction. For instance mass, volume, distance Vector is a directed quantity, one with both magnitude and direction. For instance acceleration, velocity, force Basic Vector System Magnitude of vectors: Let P = (x, y, z). Vector OP P is defined by OP p x i + y j + z k []x, y, z with magnitude (length) OP p x2 + y 2 + z2 Calculation of Vectors Vector Equation Two vectors are equal if and only if the corresponding components are equals Let a a1i + a2 j + a3 k and b b1i + b2 j + b3 k. -
Vector Calculus MA3VC 2016-17
Vector calculus MA3VC 2016–17: Assignment 1 SOLUTIONS AND FEEDBACK (Exercise 1) Prove that if f is a (smooth) scalar field and G~ is an irrotational vector field, then (∇~ f × G~ )f is solenoidal. Hint: do not expand in coordinates and partial derivatives. Use instead the vector differential identities of §1.4 and the properties of the vector product from §1.1.2 (recall in particular Exercise 1.15). (Version 1) We compute the divergence of the vector field (∇~ f × G~ )f using the product rules (29) and (30) for the divergence: (29) ∇~ · (∇~ f × G~ )f = ∇~ f · (∇~ f × G~ )+ f∇~ · (∇~ f × G~ ) (30) = ∇~ f · (∇~ f × G~ )+ f(∇×~ ∇~ f) · G~ − f∇~ f · (∇×~ G~ ). The first term in this expression vanishes1 because of the identities u~ ·(~u×w~ )= w~ ·(~u×~u) (by Exercise 1.15) and ~u × u~ = ~0 (by the anticommutativity of the vector product (3)), which hold for all u~ , w~ ∈ R3. Applying these formulas with ~u = ∇~ f and w~ = G~ we get ∇~ f · (∇~ f × G~ )= G~ · (∇~ f × ∇~ f)= G~ · ~0 = 0. The second term vanishes because of the “curl-grad identity” (26): ∇×~ ∇~ f = ~0. The last term vanishes because G~ is irrotational: ∇×~ G~ = ~0. So we conclude that the field (∇~ f × G~ )f is solenoidal because its divergence vanishes: ∇~ · (∇~ f × G~ )f = G~ · (∇~ f × ∇~ f)+ f(∇×~ ∇~ f) · G~ − f∇~ f · (∇×~ G~ )=0. =~0 =~0 =~0 | {z } | {z } | {z } (Version 2) Alternatively, one could expand the field in coordinates. This solution is of course much more complicated and prone to errors than the previous one. We first write the product rule for products of three scalar fields, which is proved by applying twice the usual product rule for partial derivatives (8): ∂ ∂ (8) ∂(fg) ∂h (8) ∂f ∂g ∂h ∂f ∂g ∂h (fgh)= (fg)h = h + fg = g + f h + fg = gh + f h + fg . -
Culture Night Event Schedule
SWORDS CASTLE For information & any booking queries contact: CULTURE NIGHT Bridge St, Swords, Co. Dublin 16th SEPTEMBER 2016 5PM-11PM Come and meet Fingal County Council’s Erin Lynch Heritage and Conservation team and find Fingal County Council out more about the history of Swords p: (01) 890 5733 VARIOUS LOCATIONS IN FINGAL Castle, the ongoing conservation works e: [email protected] and the recent community archaeology project Swords Castle: Digging History. A www.fingalarts.ie NORTH COUNTY DUBLIN ARDGILLAN CASTLE series of 45 minute talks will take place at 5.00pm, 5.45pm, 6.30pm and 7.15pm. Time: 5.00pm – 8.00pm ALL EVENTS FREE OF CHARGE Genre: Heritage, Talk, Tour Phone: 01 8905600 Website: www.fingal.ie ARDGILLAN CASTLE DIAS - DUNSINK OBSERVATORY DRAÍOCHT BLANCHARDSTOWN EMMAUS RETREAT CENTRE MALAHIDE CASTLE & GARDENS Balbriggan, Co Dublin Dunsink Ln, Castleknock, D15 The Blanchardstown Centre, D15 Ennis Lane, Lissenhall, Swords, Co. Malahide, Co Dublin Ardgillan Castle will be holding a Visit Dublin’s historical observatory and Enjoy a taste of Youth Theatre Culture Dublin Come and visit Malahide Castle & traditional music night in the castle for the home of Ireland’s greatest (7pm – 8pm workshop for ages 14-18), Emmaus is a centre of spirituality and Gardens, an international and award culture night with local Skerries group mathematician and scientist, William an Open Studio with artist Katie O’Neill relaxation that offers an oasis for people winning visitor attraction. Once owned by Inis Rua performing in the stunning Rowan Hamilton. See the magnificent and a film screening of ‘Wild’ starring to come away and rest a while and really the Talbot Family since the 12th Century, drawing room. -
Twenty Years of the Hamilton Walk Fiacre O´ Cairbre
Irish Math. Soc. Bulletin 65 (2010), 33{49 33 Twenty Years of the Hamilton Walk Fiacre O´ Cairbre 1. Introduction It all started on a bright Monday morning on October 16, 1843. The famous event was later described in a letter from Hamilton to his son, as follows: Although your mother talked with me now and then, yet an undercur- rent of thought was going on in my mind, which gave at last a result, whereof it is not too much to say that I felt at once an importance. An electric current seemed to close; and a spark flashed forth, the herald (as I foresaw, immediately) of many long years to come of def- initely directed thought and work .... Nor could I resist the impulse { unphilosophical as it may have been { to cut with a knife on a stone of Brougham Bridge as we passed it, the fundamental formula... The above piece describes Hamilton's famous creation of a strange new system of four{dimensional numbers called Quaternions, which are his most celebrated contribution to mathematics. \Number cou- ples" (or complex numbers) had been important in mathematics and science for working in two{dimensional geometry and Hamilton was trying to extend his theory of number couples to a theory of \Num- ber triples" (or triplets). He hoped these triplets would provide a natural mathematical structure and a new way for describing our three{dimensional world, in the same way that the number couples played a significant role in two{dimensional geometry. He was hav- ing a difficult time defining the multiplication operation in his quest for a suitable theory of triplets. -
Of 146 RAY VELOCITY DERIVATIVES in ANISOTROPIC ELASTIC MEDIA
RAY VELOCITY DERIVATIVES IN ANISOTROPIC ELASTIC MEDIA. PART II – POLAR ANISOTROPY Igor Ravve (corresponding author) and Zvi Koren, Emerson [email protected] , [email protected] ABSTRACT In Part I of this study, we obtained the ray (group) velocity gradients and Hessians with respect to the ray locations, directions and the anisotropic model parameters, at nodal points along ray trajectories, considering general anisotropic (triclinic) media and both, quasi-compressional and quasi-shear waves. Ray velocity derivatives for anisotropic media with higher symmetries were considered particular cases of general anisotropy. In this part, Part II, we follow the computational workflow presented in Part I, formulating the ray velocity derivatives directly for polar anisotropic (transverse isotropy with tilted axis of symmetry, TTI) media for the coupled qP and qSV waves and for SH waves. The acoustic approximation for qP waves is considered a special case. The medium properties, normally specified at regular three-dimensional fine grid points, are the five material parameters: the axial compressional and shear velocities and the three Thomsen parameters, and two geometric parameters: the polar angles defining the local direction of the medium symmetry axis. All the parameters are assumed spatially (smoothly) varying, where their gradients and Hessians can be reliably computed. Two case examples are considered; the first represents compacted shale/sand rocks (with positive anellipticity) and the second, unconsolidated sand rocks with strong -
Students' Difficulties with Vector Calculus in Electrodynamics
PHYSICAL REVIEW SPECIAL TOPICS—PHYSICS EDUCATION RESEARCH 11, 020129 (2015) Students’ difficulties with vector calculus in electrodynamics † ‡ Laurens Bollen,1,* Paul van Kampen,2, and Mieke De Cock1, 1Department of Physics and Astronomy & LESEC, KU Leuven, Celestijnenlaan 200c, 3001 Leuven, Belgium 2Centre for the Advancement of Science and Mathematics Teaching and Learning & School of Physical Sciences, Dublin City University, Glasnevin, Dublin 9, Ireland (Received 27 January 2015; published 2 November 2015) Understanding Maxwell’s equations in differential form is of great importance when studying the electrodynamic phenomena discussed in advanced electromagnetism courses. It is therefore necessary that students master the use of vector calculus in physical situations. In this light we investigated the difficulties second year students at KU Leuven encounter with the divergence and curl of a vector field in mathematical and physical contexts. We have found that they are quite skilled at doing calculations, but struggle with interpreting graphical representations of vector fields and applying vector calculus to physical situations. We have found strong indications that traditional instruction is not sufficient for our students to fully understand the meaning and power of Maxwell’s equations in electrodynamics. DOI: 10.1103/PhysRevSTPER.11.020129 PACS numbers: 01.40.Fk, 01.40.gb, 01.40.Di I. INTRODUCTION Maxwell’s equations can be formulated in differential It is difficult to overestimate the importance of or in integral form. In differential form, the four laws are Maxwell’s equations in the study of electricity and magnet- written in the language of vector calculus that includes ism. Together with the Lorentz force law, these equations the differential operators divergence and curl. -
Awz8x (Free and Download) Edmond Halley: Great Astronomers Online
awz8x (Free and download) Edmond Halley: Great Astronomers Online [awz8x.ebook] Edmond Halley: Great Astronomers Pdf Free Robert Stawell Ball *Download PDF | ePub | DOC | audiobook | ebooks Download Now Free Download Here Download eBook #1885752 in Books 2017-03-24Original language:English 8.00 x .23 x 5.25l, #File Name: 1988357489102 pages | File size: 48.Mb Robert Stawell Ball : Edmond Halley: Great Astronomers before purchasing it in order to gage whether or not it would be worth my time, and all praised Edmond Halley: Great Astronomers: 0 of 0 people found the following review helpful. Not a lot to be told about Halley. The ...By Dimitrios MarkakisNot a lot to be told about Halley. The name speaks by itself. I bought it for a kid to be read after 10 years from now.0 of 0 people found the following review helpful. This is the best version of "Edmond Halley: Great Astronomers" on By BookWormThis is the best version of "Edmond Halley: Great Astronomers" on - period. It has all the original illustrations. Interior of the book has been laid out very well with proper readable font size, well organized interior along with the author Robert Stawell Balls's brief biography at the end. On top of it, there is a nice "Gift Certificate" page, so that if we wish to give this book as a gift to someone, this would be amazing. I would say, this is the best copy or edition of GREAT ASTRONOMERS ever, with complete original illustrations. I highly recommend you buy a copy of this book, published by "DIAMOND BOOKS / DIAMOND PUBLISHERS".