The Mechanical Theory of HeatMacmillan, 1879 - 376 sider |
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Side 3
... assume that the motion takes place in a plane in which both the initial direction of motion and the line of force are situated . We will employ rectangular axes of co - ordinates lying in this plane , and will call x and y the co ...
... assume that the motion takes place in a plane in which both the initial direction of motion and the line of force are situated . We will employ rectangular axes of co - ordinates lying in this plane , and will call x and y the co ...
Side 6
... assume any fixed relation to hold between these two quantities , so that one may be expressed as a function of the other , the integration again becomes possible . For if we put ƒ ( xy ) = 0 .. ( 6 ) , in which ƒ expresses any function ...
... assume any fixed relation to hold between these two quantities , so that one may be expressed as a function of the other , the integration again becomes possible . For if we put ƒ ( xy ) = 0 .. ( 6 ) , in which ƒ expresses any function ...
Side 7
... assume some relation between the variables , in order to make inte- gration possible ; and we shall thereby obtain a ... assumed at pleasure , § 4. Geometrical interpretation of the foregoing results , and MATHEMATICAL INTRODUCTION . 7.
... assume some relation between the variables , in order to make inte- gration possible ; and we shall thereby obtain a ... assumed at pleasure , § 4. Geometrical interpretation of the foregoing results , and MATHEMATICAL INTRODUCTION . 7.
Side 8
... assume that the function F ( x , y ) in equation ( A ) is such that it has only a single value for any one point in the plane of co - ordinates . We shall also assume that in the movement of the point p its original and final positions ...
... assume that the function F ( x , y ) in equation ( A ) is such that it has only a single value for any one point in the plane of co - ordinates . We shall also assume that in the movement of the point p its original and final positions ...
Side 28
... assume that the internal forces have an Ergal , which is a quantity fully determined by the existing condition of the body at any time , without its being requisite for us to know how it arrived at that condition . Thus the internal ...
... assume that the internal forces have an Ergal , which is a quantity fully determined by the existing condition of the body at any time , without its being requisite for us to know how it arrived at that condition . Thus the internal ...
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The Mechanical Theory of Heat: With Its Applications to the Steam-engine and ... Rudolf Clausius Uten tilgangsbegrensning - 1867 |
The Mechanical Theory of Heat: With Its Applications to the Steam-engine and ... Rudolf Clausius Uten tilgangsbegrensning - 1867 |
Vanlige uttrykk og setninger
assume boiler C₂ calculated carbonic acid Chapter compression condenser condition corresponding curve cyclical process cylinder denote determine differential coefficient differential equation dp dT dp dv dT dp dt dt dv dp dx dx dx dy dy dx engine equa equal Equation 25 equation becomes Ergal expansion experiments expression external force formula function given gives heat at constant heat Q heat reservoirs Hence indefinitely small independent variables integral isentropic Joule kilogram law of Mariotte liquid magnitudes Mariotte and Gay-Lussac Mechanical Theory motion moving points negative obtain P₁ P₂ Pambour perature perfect gases piston Q₁ quantity of heat Regnault relation reversible saturated steam shews specific heat specific volume steam-engine substitute suppose T₁ T₂ Theory of Heat tion transformations unit of weight unit-weight variable body vessel Vis Viva Viva waste space whence
Populære avsnitt
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Side 265 - HEMMING— AN ELEMENTARY TREATISE ON THE DIFFERENTIAL AND INTEGRAL CALCULUS, for the Use of Colleges and Schools. By GW HEMMING, MA, Fellow of St. John's College, Cambridge. Second Edition, with Corrections and Additions. 8vo.
Side 265 - FR-S., late Fellow and Assistant Tutor of St. Peter's College, Cambridge ; Examiner in the University of London.
Side 274 - Wilson. — A MEMOIR OF GEORGE WILSON, MD, FRSE, Regius Professor of Technology in the University of Edinburgh. By his SISTER. New Edition. Crown 8vo. 6s. "An exquisite and touching portrait of a rare and beautiful spirit.
Side 267 - SOUND : a Series of Simple, Entertaining, and Inexpensive Experiments in the Phenomena of Sound, for the use of Students of every age.
Side 275 - W. ARCHER BUTLER, late Professor of Moral Philosophy in the University of Dublin. Edited from the Author's MSS., with Notes, by WILLIAM HEPWORTH THOMPSON, MA, Master of Trinity College, and Regius Professor of Greek in the University of Cambridge.
Side 274 - WurtZ. — A HISTORY OF CHEMICAL THEORY, from the Age of Lavoisier down to the present time. By AD. WURTZ. Translated by HENRY WATTS, FRS Crown 8vo. 6s. " The treatment of the subject is admirable, and the translator has evidently done his duty most efficiently.
Side 265 - A TREATISE ON THE DIFFERENTIAL CALCULUS. With numerous Examples. New Edition. Crown 8vo. los. 6d. A TREATISE ON THE INTEGRAL CALCULUS AND ITS APPLICATIONS. With numerous Examples. New Edition, revised and enlarged. Crown 8vo.
Side 268 - MUIR— PRACTICAL CHEMISTRY FOR MEDICAL STUDENTS. Specially arranged for the first MB Course.
Side 281 - BOTANY. LESSONS IN ELEMENTARY BOTANY. By D. OLIVER, FRS, FLS, Professor of Botany in University College, London. With nearly Two Hundred Illustrations. New Edition. Fcap.