BOOK 2. THE BATH SCHOOL. N. LEVASHOV'S «SVETL BROOM» IN A. KHATYBOV'S «BATH SCHOOL» AND A LABOUR SPADE

Book 2. The Bath School. Chapter 3. Theory and practice in the description of the Object to be taken to the Bath 138 (**see the lexicon of builders) at a speed less than the speed of light, a dependence is derived for the relativistic generalization of Ohm's law with respect to charge density in the observer's system. 5. The generalized Ohm's law, or Ohm's law for plasma. As follows from modern physics, plasma is the 4th state of matter. (**That is if the conductor is gradually warmed up, it will break up into its component parts, and Ohm's law reduces to a sequential walk around these components). The generalized Ohm's law is a linear dependence for plasma between the current density j and the strength of the effective electric field E eff , which includes volumetric forces of non-electrical origin that cause current. The generalized Ohm's law is written in differential form. For a fully ionized two-component plasma in a magnetic field Н , the basic Ohm's law has the form: , ∥ U ∥ + , U = W − ∇Z [ \$ − ] \ ≡ эфф , Where s çç =e 2 n/m e u ei – longitudinal conductivity of plasma, s =e 2 n/0,51m e u ei – transverse plasma conductivity, m e – electron mass, v ei – frequency of its collisions with an ion, Е ’ = Е – [uH]/c – The electric field in the intrinsic plasma system moving with velocity u<<c . р j – ion pressure, n – plasma concentration, R – thermosil due to the gradient of the plasma temperature Т : = 0,71∇ ∥ + gh ij k i K )\l m [ ∇ ] . (**Thermosil – apparently, the effect of the falling of a hot brick on the head, and the collision of electrons with ions is the collapse of mass, is described in sufficient detail by D. Swift 15 ). In 15 Jonathan Swift- "Gulliver's Travels “