The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1901 - English periodicals |
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Page 4
... distances from the atom . At a distance of twenty diameters it differs exceedingly little from uniformity . § 6. But it is only when the velocity of the atom is very small in comparison with the velocity of light , that the disturbance ...
... distances from the atom . At a distance of twenty diameters it differs exceedingly little from uniformity . § 6. But it is only when the velocity of the atom is very small in comparison with the velocity of light , that the disturbance ...
Page 9
... distance . None of the demonstrations , unsuccessful or successful , to which I have referred would be essentially ... distance , according to any law for distances less Dynamical Theory of Heat and Light . 9.
... distance . None of the demonstrations , unsuccessful or successful , to which I have referred would be essentially ... distance , according to any law for distances less Dynamical Theory of Heat and Light . 9.
Page 10
diminishing distance , according to any law for distances less than the sum of the radii , subject only to the condition that it would be infinite before the distance became zero . In fact the impact , oblique or direct , between two ...
diminishing distance , according to any law for distances less than the sum of the radii , subject only to the condition that it would be infinite before the distance became zero . In fact the impact , oblique or direct , between two ...
Page 12
... distance between their centres is greater than a + a ' or a + a " . We need not perplex our minds with the inconceivable idea of " virtue , " whether for force or for inertia , residing in a mathematical point the centre of the atom ...
... distance between their centres is greater than a + a ' or a + a " . We need not perplex our minds with the inconceivable idea of " virtue , " whether for force or for inertia , residing in a mathematical point the centre of the atom ...
Page 15
... 1 = 4 = 2222 . Example 3. - Let i = 2 ; let there be stable equilibrium , with the centres C , C ' of the two atoms at a finite distance a asunder , and let the atoms be always very nearly Dynamical Theory of Heat and Light . 15.
... 1 = 4 = 2222 . Example 3. - Let i = 2 ; let there be stable equilibrium , with the centres C , C ' of the two atoms at a finite distance a asunder , and let the atoms be always very nearly Dynamical Theory of Heat and Light . 15.
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æther apparatus atom bismuth calculated carbon cathode centim centre charge coil component condenser condensing-plates constant corresponding Crémieu crystal Crystallographic Axis curve cyanogen deflexion density diameter dielectric direction discharge disk distance effect electric electrodes electrometer electromotive force element equal equation equilibrium experiments field force formula frequency function galvanometer gases given gives harmonic heat Hence hydrogen increase ionization ions J. J. Thomson kilometres per second kinetic energy length light lines liquid magnetic mean measured metal method millimetres molecules motion needle negative ions observed obtained paper particles period Phil phosphorus plane plate positive potential pressure produced quaternions radiation radius ratio resistance reversed rotation sectors space spectra spectrum spheres suppose surface TABLE temperature theory tube vary velocity vibrations volts volume Voss machine wave-length waves wire zero