Philosophical Transactions of the Royal Society of London, Volume 125W. Bowyer and J. Nichols for Lockyer Davis, printer to the Royal Society, 1835 |
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Pagina 95
... disturbed configuration of a system by the rules of undisturbed motion , if only the initial components of veloci- ties be changed in a suitable manner . Another manner of extending rigorously to disturbed motion the rules of ...
... disturbed configuration of a system by the rules of undisturbed motion , if only the initial components of veloci- ties be changed in a suitable manner . Another manner of extending rigorously to disturbed motion the rules of ...
Pagina 96
... disturbed and disturbing masses may be expressed by the coefficients of one disturbing function . Transformations of the Differential Equations of Motion of an Attracting or Repelling System . 1. It is well known to mathematicians ...
... disturbed and disturbing masses may be expressed by the coefficients of one disturbing function . Transformations of the Differential Equations of Motion of an Attracting or Repelling System . 1. It is well known to mathematicians ...
Pagina 103
... disturbed motion of that system ; and to pass from the one to the other , may be called a Pro- blem of Perturbation . 9. To accomplish this passage , let us observe that the differential equations of un- disturbed motion ( H. ) , being ...
... disturbed motion of that system ; and to pass from the one to the other , may be called a Pro- blem of Perturbation . 9. To accomplish this passage , let us observe that the differential equations of un- disturbed motion ( H. ) , being ...
Pagina 104
... disturbed motion may be put under the following forms , & S2 ni = 0 ; ( t , l1 , C2 , . · C3 n ' P1 + без de P2 + & S2 δεξ · Pзn +852 ) . S , z n ni ( L. ) We may therefore calculate rigorously the disturbed variables 7 by the rules of ...
... disturbed motion may be put under the following forms , & S2 ni = 0 ; ( t , l1 , C2 , . · C3 n ' P1 + без de P2 + & S2 δεξ · Pзn +852 ) . S , z n ni ( L. ) We may therefore calculate rigorously the disturbed variables 7 by the rules of ...
Pagina 105
... disturbed coordi- nates 7 , only as they enter into the coefficients of this small disturbing function S2 , it is evidently permitted to substitute for these coordinates , at first , their undisturbed values , and then to correct the ...
... disturbed coordi- nates 7 , only as they enter into the coefficients of this small disturbing function S2 , it is evidently permitted to substitute for these coordinates , at first , their undisturbed values , and then to correct the ...
Overige edities - Alles bekijken
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Philosophical Transactions of the Royal Society of London, Volume 103 Royal Society (Great Britain) Volledige weergave - 1813 |
Philosophical Transactions of the Royal Society of London, Volume 126 Royal Society (Great Britain) Volledige weergave - 1836 |
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9 a² animal Apparent Solar appears April attached Baltic Barom barometer blood Bombay bottom carbonic acid clouds coast coefficients colour columns coordinates copper Crab Crustacea cubic foot Decapod dewing-point differential equations disturbing function diurnal Docks Dukhun electricity electromotor expression FAHR fall feet Fine-light function Gefle genus gneiss ground-gru h m h m h m H₁ H₂ Height of High helix High Water hygrometer inches integrals Interval January June maximum MDCCCXXXV moist monsoon months Moon's Transit needle observations obtained P₁ P₂ pairs plates Poona quantity R₁ R₂ rain range rigorous rise rocks Royal Medals S₁ S₂ shells Solna spark species sunrise surface Table Ther Therm thermometer tide tion trough Uddevalla undisturbed motion varying elements venous whilst wind wire zinc Zoea δε δη δκ