Elements of Natural Philosophy, Part 1 |
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Page 4
... Hence , when P moves through any space in the direction of the cord , the pulley B moves in the same direction , through half the space . ( 2 ) If there be two cords and two pulleys , the ends AA ' being fixed , and the other end of AB ...
... Hence , when P moves through any space in the direction of the cord , the pulley B moves in the same direction , through half the space . ( 2 ) If there be two cords and two pulleys , the ends AA ' being fixed , and the other end of AB ...
Page 8
... Hence the resultant of any two velocities as OA , AC , in the figure , is a velocity represented by the third side , OC , of the triangle OAC . Hence if a point have , at the same time , velocities represented by OA , AC , and CO , the ...
... Hence the resultant of any two velocities as OA , AC , in the figure , is a velocity represented by the third side , OC , of the triangle OAC . Hence if a point have , at the same time , velocities represented by OA , AC , and CO , the ...
Page 9
... Hence if v be the change in the velocity during the interval t , v = at , or a = ข 33. Acceleration is variable when the point's velocity does not receive equal increments in successive equal periods of time . It is then measured by the ...
... Hence if v be the change in the velocity during the interval t , v = at , or a = ข 33. Acceleration is variable when the point's velocity does not receive equal increments in successive equal periods of time . It is then measured by the ...
Page 10
... Hence the velocity of P is to and is therefore equal to that of A as OP to CA , i . e . as V to R ; Ꮴ V3 • V or R R " and this ( § 35 ) is the amount of the acceleration in the circular path ABD . 37. The whole acceleration in any ...
... Hence the velocity of P is to and is therefore equal to that of A as OP to CA , i . e . as V to R ; Ꮴ V3 • V or R R " and this ( § 35 ) is the amount of the acceleration in the circular path ABD . 37. The whole acceleration in any ...
Page 12
... Hence , if AP be the direction of motion at A , AB the direction of acceleration , and Q the position of the point at time t ; draw QP parallel to BA , meeting AP in P : then C P AP = Vt , PQ = at . A B Hence AP = 212 a · PQ . This is a ...
... Hence , if AP be the direction of motion at A , AB the direction of acceleration , and Q the position of the point at time t ; draw QP parallel to BA , meeting AP in P : then C P AP = Vt , PQ = at . A B Hence AP = 212 a · PQ . This is a ...
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Common terms and phrases
acceleration according acting action amount angle angular applied attraction axes axis body called centre centre of inertia circle component condition consider constant corresponding couple course curvature curve denote density described determined direction displacement distance divided effect elastic elements energy equal equations equilibrium evidently expression figure fixed fluid force give given gravity harmonic Hence important increase infinitely small instant internal kinetic length less mass matter mean measured method motion moving natural normal observation opposite parallel particle passing path period perpendicular plane portion position potential practical pressure principle produce projection proportional quantity radius reference relative remain remarkable respectively rest resultant right angles rigid rotation round sides simple solid space spherical square straight strain stress suppose surface theory turned uniform unit velocity weight whole wire
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Page 2 - NALOPAKHYANAM, OR, THE TALE OF NALA ; containing the Sanskrit Text in Roman Characters, followed by a Vocabulary in which each word is placed under its root, with references to derived words in Cognate Languages, and a sketch of Sanskrit Grammar. By the Rev. THOMAS JARRETT, MA Trinity College, Regius Professor of Hebrew, late Professor of Arabic, and formerly Fellow of St Catharine's College, Cambridge. Demy 8vo.
Page 167 - that every particle of matter in the universe attracts every other particle, with a force whose direction is that of the line joining the two, and whose magnitude is directly as the product of their masses, and inversely as the square of their distances from each other.
Page 292 - The Missing Fragment of the Latin Translation of the Fourth Book of Ezra, discovered, and edited with an Introduction and Notes, and a facsimile of the MS., by ROBERT L. BENSLY, MA, Sub-Librarian of the University Library, and Reader in Hebrew, Gonville and Caius College, Cambridge.
Page 295 - Wilson's Illustration of the Method of explaining the New Testament, by the early opinions of Jews and Christians concerning Christ.
Page 293 - M. Minucii Felicis Octavius. The text newly revised from the original MS. with an English Commentary, Analysis, Introduction, and Copious Indices. Edited by HA HOLDEN, LL.D.. Head Master of Ipswich School, late Fellow of Trinity College, Cambridge, Classical Examiner to the University of London. Crown Octavo. 7^. 6d. Theophili Episcopi Antiochensis Libri Tres ad Autolycum. Edidit, Prolegomenis Versione Notulis Indicibus instruxit GuLIELMUs GILsON HUMPHRY, STB Collegii Sanctiss.
Page 4 - A Synopsis of the Classification of the British Palaeozoic Rocks, by the Rev. ADAM SEDGWICK, MA, FRS, with a systematic description of the British Palaeozoic Fossils in the Geological Museum of the University of Cambridge, by FREDERICK M°CoY, FGS One vol., Royal Quarto, cloth, Plates, £i.
Page 293 - THEOLOGY— (ENGLISH). Works of Isaac Barrow, compared with the original MSS., enlarged with Materials hitherto unpublished. A new Edition, by A. NAPIER, MA of Trinity College, Vicar of Holkham, Norfolk.
Page 294 - Wheatly on the Common Prayer, edited by GE CORRIE, DD Master of Jesus College, Examining Chaplain to the late Lord Bishop of Ely. Demy Octavo. 7*. dd. The Homilies, with Various Readings, and the Quotations from the Fathers given at length in the Original Languages.
Page 4 - A Catalogue of the Collection of Cambrian and Silurian Fossils contained in the Geological Museum of the University of Cambridge, by JW SALTER, FGS With a Preface by the Rev.