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( 810 ) of electrons, unless it be modified by some new hypothesis, would undoubtedly require the existence of such a couple. In order to see this, it will suffice to consider a condenser with aether as dielectricum. It may be shown that in every electrostatic system, moving with a velocity w ## .........(1)Now, if the axis of z is chosen perpendicular to the condenser plates, the velocity u> having any direction we like, and if U is the energy of the condenser, calculated in the ordinary way, the components of © are given') by the following formulae, which are exact up to the first order- Substituting these values in (1), we get for the components of the couple, up to terms of the second order, These expressions show that the axis of the couple lies in the plane of the plates, perpendicular to the translation. If a is the angle between the velocity and the normal to the plates, the moment of the couplc will be; it tends to turn the condenser into such a position that the plates are parallel to (he Earth’s motion. In the apparatus of Trouton and Noble the condenser was fixed to the beam of a torsion-balance, sufficiently delicate to be deflected by a couple of the above order of magnitude. No effect could however be observed. § 2. The experiments of which I have spoken are not the only reason for which a new examination of the problems connected with the motion of the Earlli is desirable. Poincare
| ## (sn >to the existing theory of electric and optical phenomena in moving bodies that, in order to explain Michelson’s negative result, the introduction of a new hypothesis has been required, and that the same necessity may occur each time new facts will be brought to light. Surely, this course of inventing special hypotheses for each new experimental result is somewhat artificial. It would be more satisfactory, if if were possible to show, by means of certain fundamental assumptions, and without neglecting terms of one order of magnitude or another, that many electromagnetic actions are entirely independent of the motion of the system. Some years ago, I have already sought to frame a theory of this kind $3. I shall start from the fundamental equations of the theory of electrons I shall now suppose I hat the system as a whole moves in the direction of x with a constant velocity to, and I shall denote bij h any velocity a point of an electron may have in addition to this, so that If the equations (2) arc at the same time referred to axes moving with the system, they become », = «> + u* i>
2) M. E., § 2. |