Heaviside Electromagnetic Induction and its Propagation Sec i 2 X
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- Johnson Ruyle 작성
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In passing from the battery to the wire via the dielectric the vitality-present is continuous, the state being regular (or the ether machinery frictionless) ; however straight it reaches the conducting matter of the wire dissipation commences and the current begins to fall in power, and on reaching the axis has fallen to nothing. It takes some time to set the electric machinery going steadily. Since on beginning a current the energy reaches the wire from the medium with out, it may be expected that the electric current within the wire is first set up in the outer part, and takes time to penetrate to the middle. Return to our wire from London to Edinburgh with a steady present from the battery in London. The power from the battery neither goes by way of the wire one way nor the other. Many of the vitality is transmitted parallel to the wire practically, with a slight slant in the direction of the wire in the direction of propagation; thus the traces of vitality-present meet the wire very obliquely. Within the state of regular present via a submarine cable, with an iron sheath outside the dielectric, the energy is transmitted wholly by the gutta percha or different appropriate insulator (neglecting the small amount going to earth), thus going practically parallel to the wire, virtually quite parallel, besides as regards the traces near the wire itself, as they all eventually meet the wire.
The traces of energy-current are the intersections of the magnetic and electric equipotential surfaces. On the junctions there is a change of material, the molecules are different, and at their contact some directed high quality is given to the agitations. And there must be a particular quantity of power in transit at a given moment; in the steady state this have to be of fixed quantity, just as the entire rate of transmission is of constant amount. The quantity of power coming into a given length of the conductor is identical wherever that length may be situated. But the theory indicates instantaneous organising of current on the far finish, although not in recognisable quantity. Now, in Maxwells theory there is the potential energy of the displacement produced within the dielectric elements by the electric pressure, and there is the kinetic or magnetic energy of the magnetic induction as a result of magnetic pressure in all elements of the sector, together with the conducting elements. This illustrates the impenetrability of a perfect conductor to magnetic induction (and equally to electric present), utilized by Maxwell to the molecular theory of magnetism. Real transient, and prompt dissipative Magnetic Current. In ether, the electric current and the magnetic present are of equal significance.
Like electric displacement currents, magnetic currents are transient only, i.e., they cannot continue indefinitely in one direction, like an electric conduction present. There isn't any transmission within the sheath lengthwise, although there is dissipation there if it ought to contain, because it does sometimes, part of the return present. That the vitality of the battery passes into heat instantly would require its instantaneous transmission to all parts of the wire, which can't be entertained. There must be an intermediate state or states, after leaving the battery and earlier than becoming heat. Now, heat is the energy of molecular agitation, soft round wire electric and at first sight the only distinction is that the agitation is a little bit extra brisk at one junction than at the opposite. Now, go into the road-wire. Now, one half of the power-current tubes leaving the battery sideways turn spherical to 1 part of the road, the opposite half to the other section.
Some small part of the power leaving the battery may enter it once more, but many of the dissipation in the battery itself is accounted for by the weakening of strength in tubes that are on their manner to depart the battery. Again, the energy-current is a kinetic phenomenon, and because it varies so broadly in numerous elements, we would anticipate completely different elements of the wire itself to be in numerous electrical states, which is exactly what we don't do; for although its potential varies, yet potential shouldn't be a physical state, however a mere scientific idea. There may be an oscillatory phenomenon in the dielectric, a to-and-fro transmission of vitality and strain parallel to the wire all round it with a velocity whose doable maximum is that of undisturbed transmission. The energy is poured out of the battery sideways into the dielectric at a gradual charge. The transmission takes place entirely by way of the dielectric. It's the sink into which the energy is poured from the dielectric and there wasted, passing from the electrical system altogether. Others go between the wire and the earth, however none within the earth itself from London to Edinburgh, or vice versa, though there's a small quantity of power coming into the earth straight downwards, particularly on the earth "plates." If there's an instrument in circuit at Edinburgh, it is labored by energy that has travelled wholly by the dielectric, then finding its way into the instrument, where it enters the coil and is there dissipated, or else used up by the seen motions it results in moving elements of the instrument; which, nonetheless, is a special type of affair from dissipation, as it entails impressed force.
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