Mathematical and Physical Papers, Volume 2University Press, 1884 - Mathematics |
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Page 194
... current , make it certain that the phenomena of inversion dis- covered by Cumming could not exist , unless the ... entering on the mathematical details of the theory , or the full application of Carnot's principle , repeat in a few words ...
... current , make it certain that the phenomena of inversion dis- covered by Cumming could not exist , unless the ... entering on the mathematical details of the theory , or the full application of Carnot's principle , repeat in a few words ...
Page 208
... current for six minutes in one direction , after it had been flowing for six ... entering By end next A. TA - TR = D . By end next B. Augmentations of ... current 0 ° .039 , in favour of Vitreous Electricity . Experiment II . November 2nd ...
... current for six minutes in one direction , after it had been flowing for six ... entering By end next A. TA - TR = D . By end next B. Augmentations of ... current 0 ° .039 , in favour of Vitreous Electricity . Experiment II . November 2nd ...
Page 209
... ( Current eight times six minutes in each direction . ) Temperatures and differences of temperature after six minutes of current entering Augmentations of differences from middles to ends of periods . D ' - D . By end next B. TB . TA - TB ...
... ( Current eight times six minutes in each direction . ) Temperatures and differences of temperature after six minutes of current entering Augmentations of differences from middles to ends of periods . D ' - D . By end next B. TB . TA - TB ...
Page 210
... ( Current six times eight minutes in each direction . ) Temperatures and differences of temperature after eight minutes of current entering Augmentations of differences from middles to ends of periods . By end next B. Periods . ΤΑ TB⋅ Тв ...
... ( Current six times eight minutes in each direction . ) Temperatures and differences of temperature after eight minutes of current entering Augmentations of differences from middles to ends of periods . By end next B. Periods . ΤΑ TB⋅ Тв ...
Page 211
... current entering By end next A. Augmentations of differences from middles to ends of periods . D ' – D. By end next B. TB . TB - TA I. 1 ° .80 1 ° .82 0 ° .02 II . * 48.20 51.15 2.95 46.82 49.79 2.97 0.02 VII . 48.31 51.51 3.20 48.06 ...
... current entering By end next A. Augmentations of differences from middles to ends of periods . D ' – D. By end next B. TB . TB - TA I. 1 ° .80 1 ° .82 0 ° .02 II . * 48.20 51.15 2.95 46.82 49.79 2.97 0.02 VII . 48.31 51.51 3.20 48.06 ...
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applied Ave Maria Lane battery brass C. J. CLAY cable Cambridge University Press cells centims circuit CLAY & SONS coil College conductor copper slip copper wire Crown 8vo current entering curves deflection Demy 8vo diminished diminution direction dx² earth Edited electric conductivity electric currents electro-magnetic electrodes entering by end equal equation experiments galvanometer gutta-percha heat inch indicated induction insulated iron wire Joule junctions length magnetizing current magnetizing force magnetometer mechanical value metals meteors miles minute of current motion needle nickel Notes observed periods position potential energy residual magnetism resistance reverse Royal Society slips soft iron soldered specimens square St John's College stress submarine Sun's surface telegraph temperature testing conductor theory thermal thermo thermo-electric effect thermo-electric quality thermometers tion transverse tube University of Cambridge University Press Warehouse velocity weight wire zero zinc
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