The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1928 - English periodicals |
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Page 124
... infinite depth as far as concerns their effect on the magnetic field of the air - gap . ( ii . ) Effective Width of Slot . By the effective width of the slot is meant a width that can be used for calculation purposes on the basis that ...
... infinite depth as far as concerns their effect on the magnetic field of the air - gap . ( ii . ) Effective Width of Slot . By the effective width of the slot is meant a width that can be used for calculation purposes on the basis that ...
Page 127
... infinite depth it was shown that the gap coefficient could be obtained with sufficient accuracy for practical purposes by taking the effective width of the slot the same as for a single slot with the gap extending to infinity on either ...
... infinite depth it was shown that the gap coefficient could be obtained with sufficient accuracy for practical purposes by taking the effective width of the slot the same as for a single slot with the gap extending to infinity on either ...
Page 128
... infinite depth . enables use to be made of the same primary transformation between the z and planes as employed in the two previous problems . This The result obtained by considering two conductors will also apply with a reasonable ...
... infinite depth . enables use to be made of the same primary transformation between the z and planes as employed in the two previous problems . This The result obtained by considering two conductors will also apply with a reasonable ...
Page 141
... infinite gap due to the grooving . This extra potential is given by the real part of lim 1 ken a { x - Bm ( 2 - d ) } . Flux - Density as Percentage of Mean Flux - Density 140 Fig . 13 . = 07 120 = 0 · 5 p = 0 · 3 100 % = 0 · 1 O 20 T ...
... infinite gap due to the grooving . This extra potential is given by the real part of lim 1 ken a { x - Bm ( 2 - d ) } . Flux - Density as Percentage of Mean Flux - Density 140 Fig . 13 . = 07 120 = 0 · 5 p = 0 · 3 100 % = 0 · 1 O 20 T ...
Page 145
... infinite depth was dealt with in a similar manner , the additional gap - length in this case being given by 1 p lim ( 2 ) = ? { ( 1+ ) log . ( 1+ ; ) # 2π S + ( 1–2 ) log . ( 1–2 ) } . ( 81 ) From fig . 14 , it will be seen that when ...
... infinite depth was dealt with in a similar manner , the additional gap - length in this case being given by 1 p lim ( 2 ) = ? { ( 1+ ) log . ( 1+ ; ) # 2π S + ( 1–2 ) log . ( 1–2 ) } . ( 81 ) From fig . 14 , it will be seen that when ...
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absorption aluminium apparatus approximately atomic number atomic weight axis B₁ Balmer series bands beam calculated calorimeter carbon cathode cent chamber coefficient coil colour corresponding cosh crystal curve d₁ deflexion determined diamagnetic diffusion discharge doublet effect electric electrolytes electrometer electrons electroscope energy equation excited experimental experiments fibre filter finite flux-density forbidden line formula fraction frequency function galvanometer gases given gives glass heat hydrogen increase indicated intensity ionization ionization chamber ions K₁ layer liquid magnetic maximum measurements mercury metal method molecules nitrogen observed obtained oscillator particles Phil photo-electric Phys plane plate potassium potential pressure problem Proc radiation radon ratio reflexion resistance salts satellites Schwarz theorem sensitivity shows sinh slit slot sn² solution spectrum surface Table temperature theory tube values vapour variation velocity viscosity voltage volts wave-length width X-ray y-rays zero