Golden Ratio Discovered in Quantum World: Hidden Symmetry Observed for the First Time in Solid State Matter:
http://www.sciencedaily.com/releases/2010/01/100107143909.htm

The Great Piramid was designed to comform to Golden Ratio?
http://www.geomancy.org/sacred-geometry/the-great-pyramid/index.php

Электричество_Калашников_2003  http://depositfiles.com/files/ale4lkelo

Hi All,

Pyramid almost ready for paint.  Held together by 6 tie-wraps.  Still have to mount the hanger for the "reactor", a little touch up,
then inside gray and outside "Canary Yellow" paint, just for the heck of it.  It is not sitting on the bottom frame in these pictures,
frame is behind the pyramid.

First picture:  Side view.
Second picture, top and back.
Third picture, inside back right hand corner showing the tie-wraps.

Respectfully
Ben K4ZEP

Ben K4ZEP
good at it
Only the skeleton is better to paint separately from gypsum plasterboard
Ben you say "light at the end tunnel"?
Perhaps this is the beginning, but on the other hand (the beginning of the new features)

SG Kalashnikov
ELECTRICITY
Sixth Edition, stereotyped
Approved by the Ministry of Education
Russian Federation
as a teaching tool
for students of physics specialties
higher education
MOSCOW
FIZMATLIT
2003

TABLE OF CONTENTS
From the Editor
From the preface to the first edition
ELECTRIC FIELD
Chapter I. Electric charges 11
§ 1. Introduction to A1). § 2. The law of interaction of electric-
charges A2). § 3. Absolute electrostatic system of units
A5). § 4. The International System of Units (SI) A6). § 5. Galve-
Galvanic cells A8). § 6. Electrifying as charge separation
A9). § 7. Electrons A9).
Chapter II. The electric field of 21
§ 8. The concept of an electric field, B1). § 9. Tension
electric field B2). § 10. The addition of electric fields
B4). § 11. Volume and surface charge density, B4).
§ 12. The lines of the electric field B5). § 13. Theo-
Theorem Gauss-Ostrogradskii B9). § 14. Poisson equation C6).
§ 15. Dipole in an electric field C8).
Chapter III. The potential difference 40
§ 16. Work in the electrostatic field D0). § 17. The difference in
potentials D1). § 18. Conditions of equilibrium of charges in conductors
D4). § 19. The potential difference and the field D4). § 20.
Equipotential surfaces D6). § 21. Measure the voltage
voltage between the conductors D7). § 22. Normal elements D9).
§ 23. Electric probe E0). § 24. Potential in the simplest elec-
electric fields E1). § 25. Calculation of capacity in a given field
given charge E3). § 26. The general problem of electrostatics E5). § 27.
Conductors in an electric field E7). § 28. Accurate testing for-
Coulomb's law E8). § 29. Tip F0). § 30. Electrostatic re-
generator F1).
Chapter IV. The energy of the electric field 63
§ 31. Capacitance F3). § 32. Capacity simple capacitor
capacitors F4). § 33. The method of images F8). § 34. Energy
charged capacitor F9). § 35. The connection of capacitors


TABLE OF CONTENTS
G0). § 36. Complex capacitors G2). § 37. The energy of the electric
electric field G4).
Chapter V. Dielectrics 77
§ 38. Polarization of dielectrics G7). § 39. Polarity (80).
§ 40. The electric field inside the dielectric
(83). § 41. Electric displacement in a dielectric (85). § 42. Iso-
Isotropic and anisotropic dielectrics (88). § 43. Refraction is-
bias lines and the field strength (89). § 44. The laws of electric
electric field in the insulators (90). § 45. Mechanical forces on in-
the presence of insulators (93). § 46. Electron theory of polarization
insulators (94). § 47. The dielectric constant of non-polar
non-polar dielectrics (96). § 48. The dielectric constant in
polar dielectrics (98). § 49. Determination of the dipole moments
molecules (99). § 50. Ferroelectrics A01). § 51. Piezoelectric
The piezoelectric effect A04). § 52. Inverse piezoelectric effect
(PO).
Chapter VI. Constant electric current 115
§ 53. The characteristics of electric current A15). § 54. Equation
continuity of the A17). § 55. Electric current A18).
§ 56. Ballistic galvanometer A21). § 57. Ohm's Law A23).
§ 58. Resistance Measurement A24). § 59. Resistance to conduction
wires A26). § 60. Dependence of resistance on temperature A27).
§ 61. Ohm's law in differential form, A28). § 62. Elec-
The electrolytic bath A32). § 63 - Grounding in communication lines A33).
Chapter VII. Electromotive Force 136
§ 64. Current sources A36). § 65. Work and power of the permanent
current. Joule-Lenz A36). § 66. Energy released in
galvanic cell A38). § 67. Electromotive force of galvanic
galvanic cell A38). § 68. Terminal voltage sources
current source A41). § 69. Electromotive force and a source of job
Current A43). § 70. Branched chain. Kirchhoff's rules A46).
§ 71. Power in the external circuit and the efficiency of action
of the current source A52). § 72. The energy conservation law for
electric field A54). § 73. Quasistationary currents A57).
§ 74. Capacitor in the circuit with a resistance of A59).
MAGNETIC FIELD
Chapter VIII. The magnetic field of currents in the vacuum of 162
§ 75. The magnetic interaction of currents A62). § 76. The magnetic in-
induction of A64). § 77. The absolute electromagnetic unit system,
Units A68). § 78. Magnetic constant A70). § 79. Tension
magnetic field A71). § 80. The lines of magnetic induction
A73). § 81. Vortex nature of the magnetic field A74). § 82. Mag-
The magnetic moment of the current A79). § 83. Two parallel conductors with


TABLE OF CONTENTS
current A81). § 84. Mechanical work in a magnetic field. Mag-
The magnetic flux A82). § 85. Circuit with a current in a magnetic field A85).
§ 86. The magnetic field of a moving charge A88). § 87. Experiments Ro-
Uhland and Eichenwald A89). § 88. Lorentz force A91).
Chapter IX. Electromagnetic induction 192
§ 89. Electromagnetic induction A92). § 90. Law Lenz A94).
§ 91. The basic law of electromagnetic induction, A95). § 92. Because
Measurement of the voltage B00). § 93. Inductance B01).
§ 94. The magnetic permeability material B05). § 95. Disappearance
and the establishment of the current B06).
Chapter X. The energy of the magnetic field 208
§ 96. The self-energy current B08). § 97. The energy of the magnetic
Field B10). § 98. Mutual induction of B12). § 99. Mutual energy
two currents B14). § 100. The law of conservation of energy in the presence of
magnetic field B15). § 101. Kia mechanical strength in the magnetic field
B18). § 102. Pressure and tension of the Faraday-Maxwell B21).
Chapter XI. 222 magnets
§ 103. Magnetization environments B22). § 104. The intensity of the magnetic
magnetic field inside the magnet B24). § 105. Magnetic induction in
magnet B25). § 106. The laws of magnetic fields in magnetic materials B27).
§ 107. The influence of body shape on the magnetization of B30). § 108. Pre-
Refraction of the magnetic field lines, B32). § 109. Mag-
The magnetic properties of substances. Diamagnetism and paramagnetism B36).
§ Software. Ferromagnetism B38). § 111. Jobs in magnetization
B42). § 112. Magnetic materials. Ferrites B45). § 113. Magnetic
Magnetic charges. The formal theory of magnetism B47). § 114. Influence
environment on the magnetic interaction of B53). § 115. The nature of the molecule
molecular currents B55). § 116. Magnetomechanical and mehanomag-
nitnos phenomenon B57). § 117. Magnetic and mechanical moments
electron B59). § 118. Explanation of para-and diamagnetism B61).
§ 119. Explanation of ferromagnetism B65).
Chapter XII. Technical use of magnetic flux.
Generators and motors 271
§ 120. Magnetic circuit B71). § 121. Electromagnets B74).
§ 122. Branching of the magnetic flux B76). § 123. Generators
AC B78). § 124. DC generators B80).
§ 125. DC motor B82). § 126. Synchronous
Engines B83). § 127. Biphasic current B84). § 128. Three-phase
current B86). § 129. Vector diagram of B90). § 130. Rotating
magnetic field B93).
Chapter XIII. Interconversions of electric and magnetic fields
magnetic fields. Maxwell's theory 296
§ 131. Rotational electric Nole B97). § 132. Eddy currents
B99). § 133. Transformer C01). § 134. Displacement variable


TABLE OF CONTENTS
current (skin effect) C04). § 135. Induction accelerator C06).
§ 136. Bias current C08). § 137. Maxwell's Equations C11).
§ 138. Maxwell's equations in differential form C13).
§ 139. The value of the Maxwell theory C16). § 140. Electromagnetic
Electromagnetic field in moving tolah C17). § 141. For electromagnetic
phenomena important to the relative motion of C20). § 142. Electro-
Electromagnetic induction in moving conductors C23). §] 43. Trans-
Lorentz transformation of C25).
Electronic and Ionic Phenomena
Chapter XIV. The nature of the electric current in metals and in-
semiconductors 329
§ 144. Measurement of the electron charge C29). § 145. The nature of carrier
charge carriers in metals C32). § 146. The reason electric co-
resistance to C34). § 147. Classical theory of electron-ME
Metal C36). § 148. Superconductivity C40). § 149. Limits
applicability of the classical electron theory of metals C44).
§ 150. Concentration and mobility of electrons in metals, C46).
§ 151. Semiconductors and dielectrics C48). § 152. Own
conductivity of semiconductors C50). § 153. Extrinsic conductivity
conductivity of semiconductors C52). § 154. The concept of energy
zones C54). § 155. Distribution of momentum and energy in electricity
electrons C59).
Chapter XV. Electric currents in vacuum 363
§ 156. Electron emission C63). § 157. The current-voltage char-
characteristic of a vacuum diode C64). § 158. Dependence of the current saturation
saturation temperature of C67). § 159. Tube-like you
rectifier C69). § 160. Three-electrode vacuum tube (three
(Triode) C70). § 161. Amplification of electrical signals C74). § 162.
Electrical fluctuations in C77). § 163. Secondary electron
emission of C79). § 164. Multigrid lamp C81). § 165. Avtoelek-
Field emission C82).
Chapter XVI. Discharges in gases 383
§ 166. Ionization of gases C83). § 167. Ionization by electron impact
strikes C85). § 168. The movement of ions in gases C86). § 169. Non-self-
Combining self-discharge and C88). § 170. The occurrence of
The emergence of self-discharge C90). § 171. Glow discharge
C94). § 172. Corona discharge C97). § 173. Spark D00).
§ 174. Lightning D02). § 175. Arc D03). § 176. Stable
The stability of electrical discharges D06). § 177. Plasma D10).
The head XVII. The motion of charged particles in electric
and magnetic fields 412
§ 178. The motion of charged particles in a uniform electric
field D12). § 179. The motion of charged particles in a homogeneous


TABLE OF CONTENTS
magnetic field D13). § 280. Cyclotron D16). § 181. Definition
Determining the specific charge of electrons by magnetic-focusing
Focus D18). § 182. Magnegron D19). § 183. Determination of specific
charge / 3-particles D22). § 184. The measurement results for the share-
electron charge D24). § 185. Cyclotron (diamagnetic) resonance
resonance D25). § 186. The effective mass of D27). § 187. Reflection and
refraction of electron beams. Electron and ion optics
D29). § 188. Electronic Oscilloscope D33).
Chapter XVIII. Electrical current in electrolytes 435
§ 189. The laws of electrolysis Faraday D35). § 190. Electrolytic
Electrolytic dissociation of D38). § 191. The movement of ions in electrolytes
D41). § 192. The conductivity of electrolytes D43). § 193. The number of re-
transfer. Mobility of ions in electrolytes D44). § 194. Electrode
Electrode potentials D47). § 195. Chemical sources of current D51).
§ 196. Decomposition voltage of the electrolyte D55). § 197. Accumulates,
Batteries D57).
Chapter XIX. Electrical phenomena in contacts of 459
§ 198. Contact potential difference D59). § 199. Thermo-
Thermo-D63). § 200. Peltier D67). § 201. Ef-
Effect Thomson D70). § 202. Thermoelectric applications D72).
§ 203. Electron-hole transitions in semiconductors, D73).
§ 204. Semiconductor diodes D78). § 205. Nonequilibrium electron
electrons and holes in semiconductors, D79). § 206. Semiconductor
Semiconductor amplifiers D82).
ELECTROMAGNETIC OSCILLATIONS AND WAVES
Chapter XX. Proper electrical fluctuations 485
§ 207. Proper electrical signal D85). § 208. Damping
Damping of the oscillations D88). § 209. The equation of its own electrical
oscillations. Fluctuations in the absence of damping, D90). § 210. Vi-
Fluctuations in the presence of damping D93). § 211. Maintenance of oscillations
oscillations. Spark circuit D96). § 212. Self-oscillatory systems
D97). § 213. The use of negative resistances D98).
§ 214. Tube generators. Feedback E00). § 215. Condition
self E03). § 216. Relaxation oscillations E05).
Chapter XXI. Forced electric vibrations. Re-
Alternating current 506
§ 217. Resistance in AC circuits, E07). § 218. Em-
Capacity in AC circuits, E08). § 219. Inductance in the circuit
AC E11). § 220. Ohm's law for alternating currents
E14). § 221. Resonance voltage E16). § 222. The establishment of co-
fluctuations E20). § 223. Work and power AC E22)


TABLE OF CONTENTS
§ 224. Branching alternating currents E25). § 225. Resonance currents
E27). § 226. Parametric resonance E30). § 227. Complex
value of E32). § 228. Complete resistance to E36).
Chapter XXII. Electromagnetic waves along wires. . . 541
§ 229. Distributed Systems E41). § 230 - Electromagnetic
pulse along the wires E42). § 231. Electromagnetic waves
E45). § 232. Standing electromagnetic waves E47). § 233. Sob-
Natural oscillations of a two-wire line E51). § 234. Experi-
Experimental study of standing electromagnetic waves E53).
§ 235. Open vibrator E55). § 236. Standing waves in coils
E56).
Chapter XXIII. Free electromagnetic waves 557
§ 237. The formation of free electromagnetic waves E57).
§ 238. The wave equation E58). § 239. Plane electromagnetic
electromagnetic waves E60). § 240. Properties of electromagnetic waves, E62).
§ 241. Experimental study of electromagnetic waves
E63). § 242, energy of electromagnetic waves E67). § 243. Ele-
Elementary dipole E71). § 244. The pressure of electromagnetic waves
E74). § 245. Momentum and mass of the electromagnetic field E75).
§ 246. Electromagnetic mass of the moving charge E79).
Chapter XXIV-application of electromagnetic waves for
communication 582
§ 247. The principle of radio E82). § 248. Modulation oscillations
E83). § 249. Transmitter E86). § 250. Demodulation oscillations
oscillations. Radio E88). § 251. Heterodyne reception E91).
§ 252. Superheterodyne E91). § 253. Semi-free
electromagnetic waves E93).
Adding 595
1. The theory of the experiments of Cavendish and Maxwell (§ 28) 595
2. The orientation of polar molecules in an electric field (§ 48). 598
3. Lilies of voltage and current (§ 61) 599
4. The method of loop currents (§ 70) 600
5. Maxwell relaxation time (§ 73) 601
6. Mutual energy of two currents (arbitrary contours) (§ 90). 602
7. Larmor's theorem (§ 115), 603
8. Law Boguslavsky Langmuir-604
9. The stability of electrical discharges (§ 176, 213) 605
10. An explanation of the cyclotron resonance (§ 185), 608
11. The electromagnetic field of a dipole (§ 243) 610
12. The pressure of electromagnetic waves (§ 244) 612
13. Gaussian system of units 6] 4
14. Table of electrical and magnetic units 619
Index 621


FROM THE EDITOR
This book of Professor
SG Kalashnikov "Electricity" is written on the basis of lectures
lectures which the author read in a number of years on the physical
Faculty of Moscow State University. Leck
Lectures SG Kalashnikov at the rate of General Physics, and he created
course on semiconductor physics has always distinguished by their depth
the content, accuracy and clarity of exposition transparent
and invariably the current level. This feature lectures
attracted to them not only to students in which they had previously
all been calculated, but also graduate students, faculty and
researchers of all ranks.
The book was first published in 1956, quickly gained
widely accepted and has become a major educational ben-
benefits for students in physics disciplines of higher education
institutions. In preparing the reprint author constantly-Sauveur
improved the course, supplementing it with new material and expanding
content. A few days before his death, following-
followed April 23, 1984, Sergei G. Kalashnikov over-
completed the main text of this, the fifth, because of
edition of "Electricity", not written by you only pre-
Preface.
As in previous editions, the author has made into a book some-
some changes and improvements, while retaining the general idea,
course structure and style of presentation. For example, expanded and recycling-
revised § 113 (a magnetic charge. The formal theory of magnetism
Magnetism), § 117 (Magnetic and mechanical moments of the electron),
§ 246 (Electromagnetic Mass of the moving charge). Addendum
Added important information about isotropic and anisotropic dielectric
dielectrics (§ 42), forward and reverse piezoelectric effects
(§ 42, 51), the energy of a charged capacitor (§ 34) and energy
magnetic field (§ 47), as well as thermoelectricity (§ 199).
Included a question about the orientation of polar molecules in electric
electric field (Appendix 2). In addition, done a considerable
smaller number of insertions and substitutions in other places of the book.
In the process of editing and finalization of py-
manuscript for publication held clarification of terminology, notation
denote the physical units are given in accordance
GOST 8.417-81 with the current (ST SEV 1052-78).

Any thing look interesting? let me know the pages, Ill run it through the translator

Hi Tektron, zhak, all,

Sure wish there was a English translation ............

Somehow sent this twice.......arrrrrrrr.  Wont let me delete it, only modify..........
Respectfully
Ben K4ZEP

Have an idea to make a removable panel.
What do you think such an option may damage the operation of TPP?
â–¼
â–¼
â–¼

Hi Tektron, zhak, all,

Sure wish there was a English translation of the total book.  Downloaded the PDF, working with translation software.
Thanks for the heads up!  Especially interested in the piezo discussion in the book. 

Unable to work on Pyramid today, family coming, things to do.....back on it tomorrow.

Respectfully
Ben K4ZEP

This wont make any sense without the equations and the background instruction leading up to this chapter. SORRY

§ 51 The piezoelectric effect 109
Consequently, the piezoelectric effect of quartz is described by the
equations
Pi - / 3llUl - / 3uU2 + / 3uli4,
Py =-Rii-gillie, E1.3)
Pz = 0.
As a result of polarization changes during deformation and
electric displacement D within the crystal. In this case, in general, deter-
determining the displacement of D1.2) under P is necessary to understand the amount of Fe + P ", where Fe
caused by an electric field, E, - deformation:
D = e0E + PB + P «. E1.4)
Here polarization of Pu is generally determined by the relations
E1.1). If the polarity of the electric field does not depend on the Fe-on
direction of E, we can introduce a scalar dielectric constant
e (§ 42) and write eoE + Fe = eeoE. Then
D =?? OE + PU. E1.5)
We now estimate the magnitude of piezoelectric effect on
sample of quartz. For this we consider plate cut perpendicular to the
perpendicular to the electrical axis X (si. Fig. 71), and assume that it subjected-
subjected to unilateral stretching along the axis.
Let the tensile stress is equal to si = 105 Pa. The resulting
strain is, and \ = si / C, where C - the elastic modulus (modulus of Yun-
Jung), depending on the direction of stretching and on the fixed side
edge of the plate or free (depending on boundary conditions for deformation
strain). We assume the side faces of the plate free. Then for
stretching along the X axis for quartz C = 7,8 • YU10 Pa. Then the deformation
is
Ad si YU5,, 1P-a
U October 13
Arising as a result of this deformation polarization, according to
the first equation E1.3), is
Px \ =? N "1 = 0,23 | 10 6 Kl/m2.
We now find the electric field caused by this
polarization. It can be determined from the expression for the electric displacement of
bias. In quartz, e depends weakly on the direction and we can use
by E1.5).
Since the volume charge density p inside the plate is zero,
then, according to the Poisson equation A4.1), divD = 0, and consequently, D =
= Const which means that the appearance of any section of the plate
X = const polarization P "will be accompanied by the appearance in the same
section of the electric field E in the opposite direction and a ve-
magnitude to the changes of both terms on the right side of E1 5)
compensate each other. Therefore found higher polarity
| Pxi = j3nui cause the electric field
Bxi = - ^ ui. E1.6)
? 0
Substituting for quartz e = 4.5 and using the above values
values ​​of /? and q «1, we find that \ E \ = 5900 V / m = 59 V / cm. When the thickness of the plate,
say, d = 0,5 cm voltage between the plates will be U = Ed, and 30 V.