The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1904 - English periodicals |
From inside the book
Results 1-5 of 98
Page iv
... Charges transported by Cathode and Canal Rays to the Exciting Current Prof. Karl Pearson on a Novel Instrument for Drawing Parabolas . ( Plate XV . ) Profs . E. Rutherford and H. T. Barnes on the Heating Effect of the Radium Emanation ...
... Charges transported by Cathode and Canal Rays to the Exciting Current Prof. Karl Pearson on a Novel Instrument for Drawing Parabolas . ( Plate XV . ) Profs . E. Rutherford and H. T. Barnes on the Heating Effect of the Radium Emanation ...
Page 84
... charge up at a rate pro- portional to the number of ions produced in the gas per second . The rate at which this electrode charges up will therefore be a measure of the amount of ionization produced in the given volume of gas per second ...
... charge up at a rate pro- portional to the number of ions produced in the gas per second . The rate at which this electrode charges up will therefore be a measure of the amount of ionization produced in the given volume of gas per second ...
Page 92
... charge up for exactly the same time , and under the influence of the same cone of rays . The reading of the electrometer corresponding to the charge on E was observed , and then the quadrants of the electrometer were discharged and ...
... charge up for exactly the same time , and under the influence of the same cone of rays . The reading of the electrometer corresponding to the charge on E was observed , and then the quadrants of the electrometer were discharged and ...
Page 106
... charge through mercury vapour . In absence of air no striations could be obtained * . The arc is at the first moment rather dim , and reaches its full brilliancy only after about 10 to 15 seconds ( if the tube was cold to begin with ) ...
... charge through mercury vapour . In absence of air no striations could be obtained * . The arc is at the first moment rather dim , and reaches its full brilliancy only after about 10 to 15 seconds ( if the tube was cold to begin with ) ...
Page 112
... charged , and move back toward the cathode , must be left undecided . It was , however , in- teresting to see what ... charges at the anode , will diffuse and condense in the condensing - chamber C , which , being outside of the arc , is ...
... charged , and move back toward the cathode , must be left undecided . It was , however , in- teresting to see what ... charges at the anode , will diffuse and condense in the condensing - chamber C , which , being outside of the arc , is ...
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Common terms and phrases
absorption æther aggregate Aleph alternating current ampere angle anode antenna apparatus arrangement atom basalt calculated canal rays cardinal number cathode rays cell cent charge colours conductivity connexion constant corpuscles corresponding curve cylinder Dattenberg deflexion density diameter direct current direction distance doublet electric electrodes electrometer emanation emission energy equal equation excited activity experiments galvanometer gases given glass heating effect hydrogen increase ionization ions isostacy J. J. Thomson length light liquid magnetic maximum means measured mercury mercury vapour metal method molecules negative number of corpuscles observed obtained ordinal oscillations paper particles Phil plane plate platinum polarization position potential pressure produced Prof radiation radioactivity radium radium bromide reflecting-power resistance ring rotation selenide selenium shown surface temperature theory thickness tube velocity vibration volts wave-length waves wire