A Treatise on the Mathematical Theory of the Motion of FluidsThe University Press, 1879 - 258 pagina's |
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Pagina ix
... Plane waves 201 167 , 168 . Spherical waves 203 169 , 170 . General equations of sound waves . Integration 206 171 , 172 . Solutions of the exact equations of motion of plane waves 208 Methods of Earnshaw and Riemann , Change of type ...
... Plane waves 201 167 , 168 . Spherical waves 203 169 , 170 . General equations of sound waves . Integration 206 171 , 172 . Solutions of the exact equations of motion of plane waves 208 Methods of Earnshaw and Riemann , Change of type ...
Pagina x
... planes . Stresses in terms of rates of strain Coefficient of viscosity . 179 . Dissipation - function 180 , 181 . Equations of motion PA GE 215 · 216 . 218 220 221 223 Boundary - conditions . 182-185 . Examples : Flux through a straight ...
... planes . Stresses in terms of rates of strain Coefficient of viscosity . 179 . Dissipation - function 180 , 181 . Equations of motion PA GE 215 · 216 . 218 220 221 223 Boundary - conditions . 182-185 . Examples : Flux through a straight ...
Pagina 2
... plane area situated at a point P of the fluid be wholly normal , its intensity ( per unit area ) is the same for all aspects of the plane . The following proof of B C P A this theorem is given here for purposes of reference . Through ...
... plane area situated at a point P of the fluid be wholly normal , its intensity ( per unit area ) is the same for all aspects of the plane . The following proof of B C P A this theorem is given here for purposes of reference . Through ...
Pagina 10
... d ' 0 & c . , where F. denotes the value of the function Fat P ( x , y , z ) . The rate of flow of matter into the space included between the three planes meeting in P , and the surface F = 10 [ CHAP . I. THE EQUATIONS OF MOΤΙΟΝ .
... d ' 0 & c . , where F. denotes the value of the function Fat P ( x , y , z ) . The rate of flow of matter into the space included between the three planes meeting in P , and the surface F = 10 [ CHAP . I. THE EQUATIONS OF MOΤΙΟΝ .
Pagina 11
Sir Horace Lamb. planes meeting in P , and the surface F = 0 , is ultimately ἐρ ( κβγ + υγα + υαβ ) ; and the rate of increase of the mass included in this space is ultim- d ately I ( έραβγ ) . Equating these expressions , substituting ...
Sir Horace Lamb. planes meeting in P , and the surface F = 0 , is ultimately ἐρ ( κβγ + υγα + υαβ ) ; and the rate of increase of the mass included in this space is ultim- d ately I ( έραβγ ) . Equating these expressions , substituting ...
Overige edities - Alles bekijken
A Treatise on the Mathematical Theory of the Motion of Fluids Sir Horace Lamb Volledige weergave - 1879 |
A Treatise on the Mathematical Theory of the Motion of Fluids Sir Horace Lamb Volledige weergave - 1879 |
A Treatise on the Mathematical Theory of the Motion of Fluids Sir Horace Lamb Volledige weergave - 1879 |
Veelvoorkomende woorden en zinsdelen
angle angular velocity Ave Maria Lane axes axis Book boundary C. J. CLAY Cambridge University Press centre Christ's College circle circuit CLAY & SONS co-ordinates coefficients const constant corresponding Crown 8vo curves Demy 8vo denote direction dx dy dz Edited element English equation of continuity equations of motion external Fellow finite fluid forces formulę given Green's theorem Hence impulse infinity integration Introduction irrotational irrotational motion J. E. SANDYS liquid LL.D mass moving Notes obtain orifice origin P. G. TAIT p₁ parallel particle plane portion pressure Professor radius region RENDEL HARRIS rotation satisfied shews simply-connected solid sphere St John's College stream-lines surface theorem Thomson Trans Trinity College University of Cambridge University Press Warehouse velocity-potential vertical vortex waves zero
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