The Mechanical Theory of HeatMacmillan, 1879 - 376 sider |
Inni boken
Resultat 1-5 av 77
Side 2
... known and easy of measurement . The force usually chosen for this purpose is that of gravity . Gravity acts on a given body as a force always tending downwards , and which for places not too far apart may be taken as absolutely constant ...
... known and easy of measurement . The force usually chosen for this purpose is that of gravity . Gravity acts on a given body as a force always tending downwards , and which for places not too far apart may be taken as absolutely constant ...
Side 8
... known , and given by the co - ordinates x , y , and a1 , y , respec- tively . Then in the first case we can find an expression for the work done by the effective force during the motion , without needing to know the actual path ...
... known , and given by the co - ordinates x , y , and a1 , y , respec- tively . Then in the first case we can find an expression for the work done by the effective force during the motion , without needing to know the actual path ...
Side 11
... known in which the motion takes place , the integration becomes thereby possible . If in this case two points are given as the original and final positions , and various curves are conceived as drawn between these points , along any of ...
... known in which the motion takes place , the integration becomes thereby possible . If in this case two points are given as the original and final positions , and various curves are conceived as drawn between these points , along any of ...
Side 19
... known ( for which it is requisite that we should know the whole course of the motion of all the points ) , then the inte- gration is always possible , and the work done can also be determined as a function of the time . Cases however ...
... known ( for which it is requisite that we should know the whole course of the motion of all the points ) , then the inte- gration is always possible , and the work done can also be determined as a function of the time . Cases however ...
Side 17
... known to be as follows : d2x m dt2 d'y = X , may = Y , m dť d2z dť = Z ............. ( 22 ) . If we multiply these equations respectively by dx dt , dy dt , dz dt , dt dt dt ( dx d'x , dy d3y , dz d3z` m and then add , we obtain dx dt ...
... known to be as follows : d2x m dt2 d'y = X , may = Y , m dť d2z dť = Z ............. ( 22 ) . If we multiply these equations respectively by dx dt , dy dt , dz dt , dt dt dt ( dx d'x , dy d3y , dz d3z` m and then add , we obtain dx dt ...
Innhold
1 | |
2 | |
3 | |
8 | |
9 | |
11 | |
12 | |
13 | |
155 | |
159 | |
169 | |
175 | |
187 | |
189 | |
192 | |
200 | |
17 | |
19 | |
21 | |
22 | |
23 | |
24 | |
25 | |
27 | |
30 | |
32 | |
33 | |
35 | |
42 | |
45 | |
47 | |
48 | |
71 | |
71 | |
76 | |
84 | |
91 | |
97 | |
106 | |
113 | |
116 | |
126 | |
133 | |
142 | |
148 | |
205 | |
212 | |
218 | |
224 | |
235 | |
241 | |
245 | |
250 | |
255 | |
255 | |
257 | |
267 | |
274 | |
281 | |
287 | |
291 | |
292 | |
295 | |
304 | |
307 | |
314 | |
321 | |
323 | |
324 | |
328 | |
334 | |
340 | |
373 | |
Andre utgaver - Vis alle
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
Side 263 - ON THE ALGEBRAICAL AND NUMERICAL THEORY OF ERRORS OF OBSERVATIONS AND THE COMBINATION OF OBSERVATIONS.
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.