The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1891 |
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Page 238
... load L2 will necessarily rupture the bar either immediately or in course of time , but simply that for any load greater than Ly the strain is not perfectly elastic . Increasing the load from zero we should reach a load L3 , probably ...
... load L2 will necessarily rupture the bar either immediately or in course of time , but simply that for any load greater than Ly the strain is not perfectly elastic . Increasing the load from zero we should reach a load L3 , probably ...
Page 239
... load instead . The breaking - load for the particular kind of stress the member in question is to be exposed to is divided by some number , e . g . 4 or 5 , called a factor of safety , and the dimensions of the member are calculated so ...
... load instead . The breaking - load for the particular kind of stress the member in question is to be exposed to is divided by some number , e . g . 4 or 5 , called a factor of safety , and the dimensions of the member are calculated so ...
Page 488
varies as the load on the beam ; hence by taking the ordinate at b twice that at a , at e four times , and at d eight times , and so on , the get points on the curve of loading along the normal for the load that gives a difference of ...
varies as the load on the beam ; hence by taking the ordinate at b twice that at a , at e four times , and at d eight times , and so on , the get points on the curve of loading along the normal for the load that gives a difference of ...
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