The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1928 - English periodicals |
From inside the book
Results 1-5 of 84
Page iii
... Mass Action , being a Function of the Volume and Masses of the Constituents , as well as of the Temperature and Catalytic Action . - I . ..... 192 195 Dr. Y. Rocard on the Theory of Light - scattering in Liquids Mr. J. A. Tomkins : A ...
... Mass Action , being a Function of the Volume and Masses of the Constituents , as well as of the Temperature and Catalytic Action . - I . ..... 192 195 Dr. Y. Rocard on the Theory of Light - scattering in Liquids Mr. J. A. Tomkins : A ...
Page vi
... Mass Action being a Function of the Volume and Masses of the Constituents as well as of the Temperature , and Catalytic Action . - II . .... Mr. H. F. Biggs on Covalency , the Paramagnetism of Oxygen and Stereochemistry Mr. C. D. Niven ...
... Mass Action being a Function of the Volume and Masses of the Constituents as well as of the Temperature , and Catalytic Action . - II . .... Mr. H. F. Biggs on Covalency , the Paramagnetism of Oxygen and Stereochemistry Mr. C. D. Niven ...
Page 44
... mass m is properly included in 9. Then for the potential energy we have V = 2π2vo2q2 . Schrödinger's equation then becomes , as he has shown . ( Wellenmechanik ' ) , p . 514 , d2P ST ? dq2 + ( E。- 2π2vo2 q2 ) P = 0. . h2 · ( 49 ) If ...
... mass m is properly included in 9. Then for the potential energy we have V = 2π2vo2q2 . Schrödinger's equation then becomes , as he has shown . ( Wellenmechanik ' ) , p . 514 , d2P ST ? dq2 + ( E。- 2π2vo2 q2 ) P = 0. . h2 · ( 49 ) If ...
Page 70
... mass absorption coefficients as a function of wave - length , that μ P λκ at a wave - length λg ' , approximately where AK is the " 2 wave - length of the K absorption discontinuity , the coefficient k in the well - known empirical ...
... mass absorption coefficients as a function of wave - length , that μ P λκ at a wave - length λg ' , approximately where AK is the " 2 wave - length of the K absorption discontinuity , the coefficient k in the well - known empirical ...
Page 86
... mass absorption- coefficient in this region , the ratio Io / I of the incident to the transmitted radiation at each wave - length λ in the region 0.27 < x < 0.33 is given by the line 2 of fig . 6 . Multiplying each ordinate of the ...
... mass absorption- coefficient in this region , the ratio Io / I of the incident to the transmitted radiation at each wave - length λ in the region 0.27 < x < 0.33 is given by the line 2 of fig . 6 . Multiplying each ordinate of the ...
Contents
1 | |
17 | |
25 | |
33 | |
50 | |
64 | |
88 | |
98 | |
678 | |
685 | |
695 | |
712 | |
729 | |
743 | |
745 | |
763 | |
146 | |
175 | |
192 | |
204 | |
210 | |
217 | |
223 | |
229 | |
239 | |
241 | |
259 | |
271 | |
280 | |
289 | |
307 | |
318 | |
324 | |
335 | |
352 | |
369 | |
385 | |
401 | |
422 | |
433 | |
447 | |
458 | |
466 | |
479 | |
510 | |
526 | |
547 | |
558 | |
567 | |
593 | |
601 | |
631 | |
633 | |
648 | |
661 | |
672 | |
775 | |
788 | |
795 | |
801 | |
807 | |
817 | |
828 | |
839 | |
842 | |
854 | |
878 | |
889 | |
910 | |
920 | |
939 | |
945 | |
965 | |
977 | |
992 | |
1008 | |
1019 | |
1044 | |
1055 | |
1073 | |
1090 | |
1104 | |
1117 | |
1123 | |
1132 | |
1140 | |
1154 | |
1167 | |
1168 | |
1191 | |
1210 | |
1216 | |
1231 | |
1254 | |
1282 | |
1288 | |
Other editions - View all
Common terms and phrases
absorption aluminium apparatus approximately atomic number atomic weight axis B₁ Balmer series bands beam calculated calorimeter carbon cathode cent chamber coefficient coil colour corresponding cosh crystal curve d₁ deflexion determined diamagnetic diffusion discharge doublet effect electric electrolytes electrometer electrons electroscope energy equation excited experimental experiments fibre filter finite flux-density forbidden line formula fraction frequency function galvanometer gases given gives glass heat hydrogen increase indicated intensity ionization ionization chamber ions K₁ layer liquid magnetic maximum measurements mercury metal method molecules nitrogen observed obtained oscillator particles Phil photo-electric Phys plane plate potassium potential pressure problem Proc radiation radon ratio reflexion resistance salts satellites Schwarz theorem sensitivity shows sinh slit slot sn² solution spectrum surface Table temperature theory tube values vapour variation velocity viscosity voltage volts wave-length width X-ray y-rays zero