Elementary Treatise on Electricity and MagnetismLongmans, Green, and Company, 1896 - 576 páginas |
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Página ix
... density . 13. Gold - leaf electroscope - Proof plane . 14. The charge of a conductor in electrical equilibrium is purely super- ficial . 15 , 16. Faraday's ice - pail experiment . 17. Determination of the electric density at different ...
... density . 13. Gold - leaf electroscope - Proof plane . 14. The charge of a conductor in electrical equilibrium is purely super- ficial . 15 , 16. Faraday's ice - pail experiment . 17. Determination of the electric density at different ...
Página 15
... , there can be no doubt that any satisfactory explanation of these phenomena must take account of the functions of non - conductors as well as of conductors . CHAPTER II . DISTRIBUTION OF ELECTRICITY . 12. Electric Density.
... , there can be no doubt that any satisfactory explanation of these phenomena must take account of the functions of non - conductors as well as of conductors . CHAPTER II . DISTRIBUTION OF ELECTRICITY . 12. Electric Density.
Página 16
... density , of the space . If the space is very small , the density at any point within it cannot differ appre- ciably from the mean density . Hence we may define the electric density at a given point as being that to which the value of ...
... density , of the space . If the space is very small , the density at any point within it cannot differ appre- ciably from the mean density . Hence we may define the electric density at a given point as being that to which the value of ...
Página 17
... the gold - leaf electroscope . A proof - ball may be used instead of a proof - plane , but the relation between the charge received by a ball when put in contact with a B conductor is related to the surface - density at the.
... the gold - leaf electroscope . A proof - ball may be used instead of a proof - plane , but the relation between the charge received by a ball when put in contact with a B conductor is related to the surface - density at the.
Página 18
... density . 14. The Charge of a Conductor in Electrical Equilibrium is purely Superficial in other words , An Electric Field does not penetrate the Surfaces of the Conductors which form its Boundaries . The following are some of the most ...
... density . 14. The Charge of a Conductor in Electrical Equilibrium is purely Superficial in other words , An Electric Field does not penetrate the Surfaces of the Conductors which form its Boundaries . The following are some of the most ...
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Otras ediciones - Ver todas
Elementary Treatise on Electricity and Magnetism George Carey Foster,Alfred William Porter Vista completa - 1909 |
Elementary Treatise on Electricity and Magnetism George Carey Foster,Edmund Atkinson Vista completa - 1896 |
Términos y frases comunes
acid action amperes angle armature axis battery capacity cell centimetre charge chemical circuit coefficient coil condenser conductor connected constant copper corresponding coulomb curve cylinder deflection density dielectric difference of potentials discharge distance effect electric field electric force electrode electromagnetic electromotive force electroscope electrostatic ends energy equal equation equilibrium equipotential surfaces equivalent experiment expressed flux formula galvanometer given gives glass gramme increase induction insulated Joule's law joules junction length Leyden jar lines of force machine magnetic force magnetisation measured mercury metal needle negative electrode Ohm's law opposite direction oxygen parallel passes Peltier effect perpendicular placed plane plate platinum polarisation pole positive electricity produced proportional quantity of electricity quantity of heat represents resistance result rotation self-induction soft iron spark sphere strength sulphate suppose temperature terminals thermo-electric tion traversed tube uniform unit V₁ velocity volts wire zero zinc