VYJClair46936972294 2025.04.04 08:27 查看 : 2
Using the identical equation (1) to represent the relation between them, ok, from being a scalar constant, becomes a linear operator ; kE must be thought to be a single image, being E operated upon by okay in a certain method, turning it into a brand new vector kE. This is well proven when not seen to the eye through the use of a microphonic contact; though, by the way, the variability of the contact itself makes it a bad technique. Quantitatively considered, they are all vector magnitudes, having definite instructions as well as strengths, which are reckoned per unit space perpendicular to their instructions in terms of chosen models. E, into the sine of the angle between their directions. We may symbolise E, C, or different physical vector magnitudes by geometrical vectors, strains drawn of the right lengths and in the proper directions. At first sight it'd appear as if three other vector magnitudes associated to the former by these coefficients had been involved; but in reality there are but two, the electric power and the magnetic power, the former being linked with both the conduction present and the displacement. From the conductivity of copper to that of cold glass is such an infinite vary as to check with astronomical ratios, and it speaks properly for electrical science that it may compare definitely such extensively differing magnitudes.
The electric equipment should have mass, in addition to elasticity, by reason of this phenomenon, since there may be motive to believe (from Maxwells principle of mild) that it is not the air, however one thing between the air molecules that's the electromagnetic medium, the air merely modifying the phenomena considerably. Grant that they are propagated in pure ether (space from which all "matter" has been removed) with out loss of vitality in the medium, and it follows that ether is the perfect non-conductor. In a dielectric medium, the power and its displacement are simultaneous, like the pressure and the present in a conductor. From these we may discover the current when the drive acts in any other route than parallel to one of the principal axes. D to E is settled by the values of the principal capacities, and their axes. E act parallel to one of many principal axes, once we might achieve this, with the suitable worth of k for that axis. But two straight traces can not enclose a space, so, in equation (1), C and kE are parallel and equal.
This additionally defines the prefix V earlier than two vectors. indicators, the n vectors kind the n sides of a polygon. Coming subsequent to specific capacity, though there are media, as air, which seem to don't have any conductivity, but, by the continuity of the electric present, they can help present; not regular, but transient, and stopped elastically. Then, the product of its hypothetical density into its velocity is the measure of the present; but, being a mere hypothesis, unless we chose to simply accept it, to talk of the velocity of electricity within the electric current becomes meaningless. In probably the most pure manner attainable, when dynamic electricity came beneath investigation, the static ideas were transferred to the electric current, which grew to become the actual movement of electricity by means of a wire. This had its disadvantages; one can get on sooner if one has ample faithwhich we know moves mountainsto settle for a sure hypothesis unhesitatingly as a fact, and work out its penalties undoubtingly, regardless of the hazard of fixing ones concepts prematurely. This is modified as it progresses by dissipation within the wire, and so gets wiped out.
This is very obscure, little doubt, however is merely to point out that the impressed power is a symmetrical kind of radiation. Let this be D, and let E, as before, be the electric pressure. Within extensive limits ok is independent of the present or the electric drive. Whatever state of magnetic induction and of current there could also be in a perfect conductor is a fixture. But ether cannot be this good conductor consistently with the propagation of magnetic disturbances, for none can be propagated in an ideal conductor. But admitting the ether to propagate gravity instantaneously, it should have fantastic properties, unlike anything we know. Of course, if it comes to numerical comparisons we should have to think about the ratios of units within the strange to what I might name the rational system. Passing to the battery, the complexity of circumstances makes it harder to observe, though the state of electric drive and magnetic power and heat era is reducible to the identical, and could also be made identically the identical as in the wire by correctly selecting its shape, soft round wire electric and many others. But within the battery there's a very remarkable factor going down, specifically, the lack of chemical vitality at a gradual fee; and in the system usually, a still more outstanding factor, an exactly equivalent regular achieve of heat.
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