Experimental Researches On the Identity of the Various Modifications of the ...
Experimental Researches On the Identity of the Various Modifications of the ...
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Goodman/ IS towards and attracted by the positive terminating ball, some* times as near as possible^ but contact was purposely prevented; Thid was invariably the case during a dozen or more repetitions of the experiment. Upon applying excited sealing wax the pith ball was attracted strongly^ shewing ^e same to be positively electrified. In all these experiments the ball wa^first attracted to the positive pole — it then receded a little until the residuum was discharged^ after which a permanent ...attraction was the result. The most rational method of accounting for the alter- nately opposite electrical condition of each pole is by supposing the charge to pass in a globular volume. Thus :— Fig.l, p-p. jj^ n n-p Fig. 2, p-p- n P Pp By the Franklinian bypotilwsis.
During the passage of the charge at the termination of the positive pole p. the opposing end of the negative pole n. would be negatived by the polarizing influence of p. But the moment the charge arrives at n (represented by p.
What to read after Experimental Researches On the Identity of the Various Modifications of the ...?
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To quickly assess the difficulty of the text, read a short excerpt:
Goodman/ IS towards and attracted by the positive terminating ball, some* times as near as possible^ but contact was purposely prevented; Thid was invariably the case during a dozen or more repetitions of the experiment. Upon applying excited sealing wax the pith ball was attracted strongly^ shewing ^e same to be positively electrified. In all these experiments the ball wa^first attracted to the positive pole — it then receded a little until the residuum was discharged^ after which a permanent ...attraction was the result. The most rational method of accounting for the alter- nately opposite electrical condition of each pole is by supposing the charge to pass in a globular volume. Thus :— Fig.l, p-p. jj^ n n-p Fig. 2, p-p- n P Pp By the Franklinian bypotilwsis.
During the passage of the charge at the termination of the positive pole p. the opposing end of the negative pole n. would be negatived by the polarizing influence of p. But the moment the charge arrives at n (represented by p.
What to read after Experimental Researches On the Identity of the Various Modifications of the ...?
You can find similar books in the "Read Also" column, or choose other free books by John Goodman to read onlineMoreLess
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