By James Clerk Maxwell
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Additional info for An Elementary Treatise on Electricity
Take a metal electrify it ball at the end of an ebonite rod, by means of the electrophorus, and by the rod as a handle let it down into carrying it the metal vessel without touching the sides. As the electrified ball approaches the vessel the indications of the electroscope continually increase, but when the ball Fig. 9. when is fairly within the vessel, that depth below the opening of the vessel becomes considerable compared with the diameter is its of the opening, the indications of the electroscope no longer increase, but remain unchanged in whatever way the ball is moved about within the is vessel.
Is new branches commonly of called the 23 ELECTRIC POTENTIAL. ] GENERAL STATEMENT OF THE CONSERVATION OF ENERGY. ] The total energy which can neither be increased nor diminished by any mutual action of those bodies, though it may be transformed into any of the forms of which energy is susceptible. If, by the action of some external agent, the configuration of the system is changed, then, if the forces of the system are such as to resist this change of configuration, the external agent In work on the system.
Let the charge of the conductor at any instant be represented by a horizontal line OC, drawn from the point 0, which is called the origin of the diagram, and let the potential of the conductor at the same instant be represented by a vertical line CA, drawn from the extremity of the first line, then the position of the extremity of the second line will indicate the electric state of the conductor, both with respect to its charge, and also with respect to its potential. If during any electrical operation this point moves along the line AFGHB, we know not only that the charge has been increased from the value OC to the value 02), and that the potential has been increased from potential at any CA to that the charge and the of the DB, but instant, corresponding, say, to the point F by Ox and xF.