## Philosophical MagazineTaylor & Francis., 1898 - Physics |

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Page 57

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**deflection**in the case of the**deflection**formula , then Ta = − $ tW { xy− ‡ + ( u2 + * + 28 + 8 ) 60 To = { tW { xy − 2− ( u2 + $ + u3 + 3 ) w + { To = ‡ sW { ś ( x − y ) + ( x2 + i + w + 8 ) w - 2u ́ ( 1 — u ) 3 } , ⋅ ( 35 ) 2u ...Page 64

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**deflection**( 40 ) . Write & for the**deflection**( 41 ) , 8 + 8 ' for the**deflection**( 40 ) , and 81 , 8 ' for the greatest values of d and . First add a uniform loading 222W , this by the 8 ' . Bernoulli - Euler theory will give the boom ...Page 65

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**deflection**agreeing with 8+ at the centre and very nearly equal to it elsewhere . Now 42k is a small fraction , squares of which cannot be worth keeping , so the reduction in**deflection**under loading W , due to the bottom boom being ...### Contents

CONTENTS OF VOL XLV | 1 |

F Brush on the Transmission of Radiant Heat | 31 |

Mr W H Macaulay on the Stresses and Deflection | 42 |

38 other sections not shown

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accuracy acid adjusted æther alternating currents aluminium amperes angle apparatus axis bars bulb calculated cathodic rays cell centim centre charge circuit cloud coil condenser constant cooling copper corresponding curve cylinder deflection deflexion determined disk distance effect electric electrification electrodes electrodynamometer electrolyte electrometer electromotive force equal equation error experiments film gases girder give given glass heat Hence hydrogen inductor integral intensity isomorphisms J. J. Thomson light lines Lord Kelvin Lord Rayleigh magnetic force means measured mercury metal method millimetre minute motion mutual inductances nearly negative observed obtained oxygen particle Phil plane plate platinum position potential pressure radius reflector resistance scale self-induction simple isomorphisms solution sphere spherometer subgroup substitutions surface temperature tensions thermometer thickness tube variation velocity verre dur vertical waves wire x-rays zero zinc