Philosophical MagazineTaylor & Francis., 1898 - Physics |
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Page 71
I may say , however , that it is sometimes possible , as in method 12 for instance , to choose a method in which the error does not exist . However , with the very best method , much rests with the experimenter , as errors from ...
I may say , however , that it is sometimes possible , as in method 12 for instance , to choose a method in which the error does not exist . However , with the very best method , much rests with the experimenter , as errors from ...
Page 153
Were it possible to measure conductivity with sufficient exactness , however , it would be possible to solve them by a partially graphical process . For This purpose , reducing equations ( ) , ( c ) , and ( e ) to two , we should have ...
Were it possible to measure conductivity with sufficient exactness , however , it would be possible to solve them by a partially graphical process . For This purpose , reducing equations ( ) , ( c ) , and ( e ) to two , we should have ...
Page 239
We shall see in the next section that it is not generally possible to obtain all the transforms of a given isomorphism of a general substitution - group in this manner . . - § 3. Simple Isomorphisms of G to itself . Let 81 , 82 , 83 , .
We shall see in the next section that it is not generally possible to obtain all the transforms of a given isomorphism of a general substitution - group in this manner . . - § 3. Simple Isomorphisms of G to itself . Let 81 , 82 , 83 , .
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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