The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1891 |
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Page 216
... vibrations without collapse ; and even at temperatures at which , when the bottom is clamped , vibrations become impossible through instability , it is always possible , with the top clamped , to get stable vibrations . Thus , to get ...
... vibrations without collapse ; and even at temperatures at which , when the bottom is clamped , vibrations become impossible through instability , it is always possible , with the top clamped , to get stable vibrations . Thus , to get ...
Page 220
... vibrations per second in the horizontal position , I found that ni + n = 2n3 , as should be , to a high degree of accuracy . But there is another check which can always be applied to any set of experiments . The equation ( A ) shows ...
... vibrations per second in the horizontal position , I found that ni + n = 2n3 , as should be , to a high degree of accuracy . But there is another check which can always be applied to any set of experiments . The equation ( A ) shows ...
Page 374
... vibrations differ from two - dimensional vibrations on the one hand ( in which the proportion is zero ) , and from the vibrations of a circular plate on the other hand ( in which the proportion is unity ) . For , according to Mr ...
... vibrations differ from two - dimensional vibrations on the one hand ( in which the proportion is zero ) , and from the vibrations of a circular plate on the other hand ( in which the proportion is unity ) . For , according to Mr ...
Contents
FIFTH SERIES | 1 |
JULY 1891 | 17 |
Dr G Gore on Changes of Voltaic Energy of Alloys during | 27 |
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acid actinometer allotropic atoms axis bismuth body bulb calculated centim centimetres chlorine circuit coil constant copper curve cylinder deflexion density diamagnetism dilute direction discharge dissociation distance effect elastic electricity electrolyte electromotive force electrostatic induction energy equal equation error experimental experiments formula galvanometer give given increase induction intensity ions iron J. J. Thomson kinetic latent heat length liquid load Lupton magnetic force magnetic leakage mathematical mean measured melting-point mercury metal method millim molecular molecules motion negative observed obtained paper pass Phil Pickering plate platinum pole position potential pressure primary produced ratio reflector resistance rigidity solid solitary wave solution strain substance sulphuric sulphuric acid supposed surface Table temperature theory tion Tomlinson torsion tube vector potential velocity vibrations wave wave-length wire Young's modulus zero zinc