flanges, and rendered water-tight by an intervening collar of leather.
In the centre of the hollow sphere thus formed, a ball of amalgamated
zinc was suspended by a well-varnished copper wire, connected with
one of the cups of a galvanometer, and was contained in a membranous bag holding the acid solution; the whole being introduced
through a short tube in the top of the upper hemisphere, and the
remaining space being filled with a saturated solution of sulphate of
copper. The galvanic circuit was completed by wires establishing
connexions between either hemisphere and the other cup of the galvaFor measuring the forces developed, sometimes the ordinometer.
nary magnetic, but in the greater number of instances the calorific
galvanometer of De la Rive was employed; the indications given by
these instruments were noted, on the completion of the circuit, in
various ways; and the deposition of copper in the hemispheres was
examined after the apparatus had been in action for a certain number
of hours.
The following are the conclusions which the author deduced from a series of experiments thus conducted:
1st. The force emanating from the active zinc centre diffuses itself over every part of the upper hemisphere, from which there is a good conducting passage for its circulation
2nd. The same amount of force is maintained by either hemisphere indifferently; but when both conducting hemispheres are in metallic communication there is no increase of force
3rd. Although the force is not increased, it spreads itself equally over the whole sphere.
4th. When one hemisphere is connected with the zinc centre by a short wire capable of affording circulation to the whole force, and the other hemisphere is connected by a long wire, through the galvanometer, with the same centre, the equal diffusion of the force over the whole sphere is maintained
5th. There is no greater accumulation of precipitated copper about the point with which the conducting wires are brought into contact, and towards which the force diffused over the whole sphere must converge, than at any other point: proving that the force must diverge from the centre equally through the electrolyte, and can only have drawn towards the conducting wires in the conducting sphere itself. Other experiments showed that the force is but slightly increased by a great increase of the generating surface.
The author's attention was next directed to ascertaining the nature of the law according to which the force emanates from the zinc centre to the surrounding conducting sphere. With this view, a variety of experiments were made with the zinc in different positions in the interior of the sphere; and from these it appeared that, whatever may be its position, the whole force is the same. From these results it is inferred, that the force emanating from the zinc ball diffuses itself over the surrounding conducting sphere in obedience to the well known law of radiant forces being in the inverse duplicate ratio of the distance.
Experiments of the same kind were likewise made with the pre-
