The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1894 - English periodicals |
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Results 1-5 of 55
Page vi
... Energy of the Amperian Molecule 473 .. Mr. F. L. O. Wadsworth on a New Method of Magnetizing and Astaticizing Galvanometer - Needles . ( Plate XIII . ) 482 Mr. J. B. Henderson on the Effects of Magnetic Fields on the Electric ...
... Energy of the Amperian Molecule 473 .. Mr. F. L. O. Wadsworth on a New Method of Magnetizing and Astaticizing Galvanometer - Needles . ( Plate XIII . ) 482 Mr. J. B. Henderson on the Effects of Magnetic Fields on the Electric ...
Page vii
... Energy of the Amperian Molecule , by Prof. A. P. Chattock 577 Index On the Propagation of Electromagnetic Waves in Ice , and on the Dielectric Power of this Substance , by M. Blondlot . 578 580 PLATES . I.-IV. Illustrative of Mr. W. B. ...
... Energy of the Amperian Molecule , by Prof. A. P. Chattock 577 Index On the Propagation of Electromagnetic Waves in Ice , and on the Dielectric Power of this Substance , by M. Blondlot . 578 580 PLATES . I.-IV. Illustrative of Mr. W. B. ...
Page 8
... energy of two molecules in contact , and V2 is the mean square of the relative velocity . So for unlike molecules of masses m1 and m , and radii a1 and a2 , with potential energy m1m2f ( 1 / α1 + a2 ) at contact and mean relative ...
... energy of two molecules in contact , and V2 is the mean square of the relative velocity . So for unlike molecules of masses m1 and m , and radii a1 and a2 , with potential energy m1m2f ( 1 / α1 + a2 ) at contact and mean relative ...
Page 9
... energy of molecules 1 and 2 in contact . Loschmidt was the first to measure diffusion - coefficients at one , or at different temperatures , but as von Obermayer's results are later and more elaborately determined it will suffice to use ...
... energy of molecules 1 and 2 in contact . Loschmidt was the first to measure diffusion - coefficients at one , or at different temperatures , but as von Obermayer's results are later and more elaborately determined it will suffice to use ...
Page 10
the law of energy is that of the inverse cube , then m1m2ƒ ( 1 / a1 + a » ) = m1m2 1A2 / ( α1 + ɑ2 ) 3 , 25 and if we know relative values of a1 and a2 , then C1 ( α , + α2 ) 3 will give relative values of 1Am1m . There are two sources ...
the law of energy is that of the inverse cube , then m1m2ƒ ( 1 / a1 + a » ) = m1m2 1A2 / ( α1 + ɑ2 ) 3 , 25 and if we know relative values of a1 and a2 , then C1 ( α , + α2 ) 3 will give relative values of 1Am1m . There are two sources ...
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acid ampere amplitude angle apparatus axis Boyle's law calculated capillary carbon dioxide carbonic acid cell centim centimetre circuit Clark cell coefficient coil condensation constant copper corresponding curve cylinder deflexion density determined diameter dielectric discharge disk displacement distance effect electrical electrodes electromotive force energy equal equation experiments gabbro galvanometer gases gauge give given glass gutta-percha heat hydrogen increase induction iron J. J. Thomson layer length liquid magnetic maximum McLeod gauge means measured megohms mercury metal method metre millim mirror molecular molecules motion nitrogen observed obtained ohms oscillations oxygen paper particles Phil phosphorescence phosphorus plane plate poles position potential pressure prism Prof quantity quaternion radius ratio rays readings resistance rotation solution spectrum sun-heat surface surface-tension telephone temperature theory tion tube vapour velocity vibration volts volts volts volume wave-length waves wire zero