Philosophical MagazineTaylor & Francis., 1898 - Physics |
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Page 151
ments on conductivity alluded to in Section 13 , will be ready for publication in the near future . In conclusion , I desire to express my thanks to Professor Thomson for the valuable assistance his suggestions have afforded . XIV .
ments on conductivity alluded to in Section 13 , will be ready for publication in the near future . In conclusion , I desire to express my thanks to Professor Thomson for the valuable assistance his suggestions have afforded . XIV .
Page 154
These volumes being mixed , we have a complex solution in which the a's and N's are known , the conductivity of which is therefore calculable by the dissociation theory . A series of observations and calculations of the conductivity of ...
These volumes being mixed , we have a complex solution in which the a's and N's are known , the conductivity of which is therefore calculable by the dissociation theory . A series of observations and calculations of the conductivity of ...
Page 478
Hence in this case the loss of conductivity due to the carriers attracting themselves up to the sides is small compared with the loss of conductivity due to diffusion . 7. When there is an excess of carriers charged with electricity of ...
Hence in this case the loss of conductivity due to the carriers attracting themselves up to the sides is small compared with the loss of conductivity due to diffusion . 7. When there is an excess of carriers charged with electricity of ...
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Contents
m FIFTH SERIES | 1 |
Mr W Sutherland on the Relative Motion of the Earth | 23 |
F Brush on the Transmission of Radiant Heat | 31 |
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adjusted apparatus appear apply approximately bars becomes bulb calculated cell centre charge circuit coil compared conductivity considerable constant containing cooling copper correction corresponding curve described determined direction distance effect electric equal equation error experiments expression field force gases give given glass greater heat Hence hydrogen increase inductances integral intensity length less light lines liquid magnetic means measured mercury metal method minutes motion nature nearly negative object observed obtained ordinary passing Phil placed plane plate positive possible potential practically present pressure produced range rays represented resistance respectively scale seen shown side similar simple solution standard substitutions suppose surface taken temperature theory thermometer thickness tube variation vary vertical volume waves wire zero zinc