Fluctuation-Electromagnetic Interaction of Rotating Neutral Particle with the Surface: Relativistic Theory

Similar documents
V A. V-A ansatz for fundamental fermions

EE243 Advanced Electromagnetic Theory Lec # 10: Poynting s Theorem, Time- Harmonic EM Fields

American International Journal of Research in Science, Technology, Engineering & Mathematics

( ) ( ) ( ) 0. Conservation of Energy & Poynting Theorem. From Maxwell s equations we have. M t. From above it can be shown (HW)

Supplementary Figure 1. Experiment and simulation with finite qudit. anharmonicity. (a), Experimental data taken after a 60 ns three-tone pulse.

t the propensity to consume the resource good. Maximizing U t in (9) subject to the budget constraint (8) yields

Priority Search Trees - Part I

9.4 Absorption and Dispersion

Wave Phenomena Physics 15c

Integrated Optical Waveguides

EE"232"Lightwave"Devices Lecture"16:"p7i7n"Photodiodes"and" Photoconductors"

Generalized Den Hartog tuned mass damper system for control of vibrations in structures

The Electrodynamic Origin of the Force of Inertia (F = m i a) Part 2

1. Quark mixing and CKM matrix

Chapter 7 Stead St y- ate Errors

New perspectives on the classical theory of motion, interaction and geometry of space-time

Introduction to Inertial Dynamics

FOR MORE PAPERS LOGON TO

A L A BA M A L A W R E V IE W

Chapter 7. Now, for 2) 1. 1, if z = 1, Thus, Eq. (7.20) holds

Workshop Neckarzimmern. Symmetries Standard Model Langrangian Higgs Coupling to Quarks and Mass Generation CKM Matrix Unitarity Triangles Mixing

Exponential Stability Analysis of a System Comprised of a Robot and its Associated Safety Mechanism

Frequency Response. Response of an LTI System to Eigenfunction

INTRODUCTION TO HEAT EXCHANGERS

EE 232 Lightwave Devices. Photodiodes

Article Nonlinear Theory of Elementary Particles: VI. Electrodynamic Sense of the Quantum Forms of Dirac Electron Theory. Alexander G.

Canonical Quantizing of Spinor Fields: Anti-Commutation Relations

Advanced Queueing Theory. M/G/1 Queueing Systems

CATAVASII LA NAȘTEREA DOMNULUI DUMNEZEU ȘI MÂNTUITORULUI NOSTRU, IISUS HRISTOS. CÂNTAREA I-A. Ήχος Πα. to os se e e na aș te e e slă ă ă vi i i i i

EE 247B/ME 218: Introduction to MEMS Design Lecture 27m2: Gyros, Noise & MDS CTN 5/1/14. Copyright 2014 Regents of the University of California

Fractal diffusion retrospective problems

Version 1.0 VLADIMIR V. KOROSTELEV. A Primer in Quantum Mechanics for NMR Students

Consider a system of 2 simultaneous first order linear equations

P a g e 5 1 of R e p o r t P B 4 / 0 9

r 3 > o m > o > z m Z -< Z il r H O O H H i-» 00 a o x3 X M > I- > 1 n 0) l' 1

T h e C S E T I P r o j e c t

SYMMETRICAL COMPONENTS

Summary: Solving a Homogeneous System of Two Linear First Order Equations in Two Unknowns

Convergence of Quintic Spline Interpolation

Mathematics. Exercise 9.3. (Chapter 9) (Sequences and Series) Question 1: Find the 20 th and n th terms of the G.P. Answer 1:

INF5820 MT 26 OCT 2012

ECE 422 Power System Operations & Planning 2 Synchronous Machine Modeling

Chapter 13 Laplace Transform Analysis

Nikon i-line Glass Series

Dynamic Safety Margin in Fault-Tolerant Predictive Controller

Subrings and Ideals 2.1 INTRODUCTION 2.2 SUBRING

t=0 t>0: + vr - i dvc Continuation

Multiple-Choice Test Runge-Kutta 4 th Order Method Ordinary Differential Equations COMPLETE SOLUTION SET

(heat loss divided by total enthalpy flux) is of the order of 8-16 times

S.Y. B.Sc. (IT) : Sem. III. Applied Mathematics. Q.1 Attempt the following (any THREE) [15]

Phys463.nb Conductivity. Another equivalent definition of the Fermi velocity is

- Prefixes 'mono', 'uni', 'bi' and 'du' - Why are there no asprins in the jungle? Because the parrots ate them all.

Lecture 12: HEMT AC Properties

Multi-fluid magnetohydrodynamics in the solar atmosphere

Chapter 8 Theories of Systems

ECE 522 Power Systems Analysis II 2 Power System Modeling

Improved Ratio Estimators for Population Mean Based on Median Using Linear Combination of Population Mean and Median of an Auxiliary Variable

FL/VAL ~RA1::1. Professor INTERVI of. Professor It Fr recru. sor Social,, first of all, was. Sys SDC? Yes, as a. was a. assumee.

THIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.

SAN JOSE CITY COLLEGE PHYSICAL EDUCATION BUILDING AND RENOVATED LAB BUILDING SYMBOL LIST & GENERAL NOTES - MECHANICAL

The Variance-Covariance Matrix

176 5 t h Fl oo r. 337 P o ly me r Ma te ri al s

FREE VIBRATION ANALYSIS OF FUNCTIONALLY GRADED BEAMS

Numerical solution of compressible fluid flow in porous media with boundary element method

Emigration The movement of individuals out of an area The population decreases

The Mathematics of Harmonic Oscillators

ELECTROMAGNETISM, NUCLEAR STRUCTURES & GRAVITATION

Electromagnetic waves in vacuum.

EQUATION SHEETS FOR ELEC

elnpol^l SSJU (tl = N) gnot

Scripture quotations marked cev are from the Contemporary English Version, Copyright 1991, 1992, 1995 by American Bible Society. Used by permission.

Response of MDOF systems

EE105 Fall 2015 Microelectronic Devices and Circuits. LTI: Linear Time-Invariant System

10.5 Linear Viscoelasticity and the Laplace Transform

Reliability Mathematics Analysis on Traction Substation Operation

Theory of the non-linear quantized electromagnetic waves, adequate of Standard Model theory

CHAPTER-2. S.No Name of the Sub-Title No. 2.5 Use of Modified Heffron Phillip's model in Multi- Machine Systems 32

Root behavior in fall and spring planted roses...

THEORETICAL AUTOCORRELATIONS. ) if often denoted by γ. Note that

Two-Dimensional Quantum Harmonic Oscillator

Homework 4 Solutions

Handout on. Crystal Symmetries and Energy Bands

OUTLINE FOR Chapter 2-2. Basic Laws

c. What is the average rate of change of f on the interval [, ]? Answer: d. What is a local minimum value of f? Answer: 5 e. On what interval(s) is f

J = 1 J = 1 0 J J =1 J = Bout. Bin (1) Ey = 4E0 cos(kz (2) (2) (3) (4) (5) (3) cos(kz (1) ωt +pπ/2) (2) (6) (4) (3) iωt (3) (5) ωt = π E(1) E = [E e

Exercises for lectures 23 Discrete systems

C241 Homework Assignment 9

" W I T H M A L I C E T O W A - P t D N O I S T E A - I S T D O H A n i T Y F O R. A L L. " A TENDERFOOT. an awful storm." At this juncture,

n r t d n :4 T P bl D n, l d t z d th tr t. r pd l

The non-linear wave theory, adequate of Standard Model

4" 4" BM 7 SPIKE IN POWER POLE ELEV= " CP 15 8" 4" 10" 4" 6" 4" 6" 8" 8" 8" 12" 12" 16" 8" 4" 10" 6"

Theoretical Seismology

Motivation. Loop-suppressed B meson decays can serve as sensitive probes for New Physics:

Exhibit 2-9/30/15 Invoice Filing Page 1841 of Page 3660 Docket No

On the Existence and uniqueness for solution of system Fractional Differential Equations

Anouncements. Conjugate Gradients. Steepest Descent. Outline. Steepest Descent. Steepest Descent

P. We make the following assumptions

dy 1. If fx ( ) is continuous at x = 3, then 13. If y x ) for x 0, then f (g(x)) = g (f (x)) when x = a. ½ b. ½ c. 1 b. 4x a. 3 b. 3 c.

ENGR 7181 LECTURE NOTES WEEK 3 Dr. Amir G. Aghdam Concordia University

APPH 4200 Physics of Fluids

Transcription:

Fluuaon-lroagn Inraon of Roang Nural Parl w Surfa: Rlavs or A.A. Kasov an G.V. Dov as on fluuaon-lroagn or w av alula rar for of araon fronal on an ang ra of a nural parl roang nar a polarabl surfa. parl an surfa ar arar b arbrar aral proprs an praurs. surfa s assu o b n ral ulbru w vauu nvronn. PACS: 4.5.W; 78.7.-g. Inrouon Roaon of a bo along w unfor oon affs s ouplng w fluuaon lroagn fl of or bos. s rsuls n ang of van r Waals Casr fors arav an sspav an raav vauu a ang [ 3]. In a srs of our paprs [45] w av an pa of roaon [4] an a obn ff of roaon an unfor oon [5] on fluuaon lroagn nraon n ffrn onfguraons of nrang subsss. oban ngral prssons pn on ron of roaon wl subsss ar arar b arbrar lr an agn proprs an ffrn praurs. a of s papr s o onsr pa of roaon on fluuaon lroagn nraon bwn a sall polalabl parl an surfa oognous alf-a w allowan for raraon ffs. orronng nonrar l was onsr n [3] an all bas forulas n [3] follow fro our gnral rar forulas n s wor as a paral as.. or Consr a sall ral parl of raus R w lr an agn polarabls an praur roang w angular vlo Ω Ω an loa a san apar fro surfa Fg. Surfa aras vauu alf-a > fro alf-a < fll b a onnuous u w lr an agn prvs ε µ an praur. Assung onons R << { Ω } R << n

o b fulfll on an onsr roang parl as a pon-l fluuang lr an agn pol. In aon u o rlavs probl san valu of as no uppr rsrons. Aorng o wll-ap o of alulaon for a rvw s [6] w allowan for onanous an nu fluuaons alulang for of araon o surfa Q& an fronal on M av for n ss Σ nal prssons for F ra of ang oolng of parl F n n n n n n n n Q& & & & & M n n n n [ ] [ ] [ ] [ ] 3 wr an uppr pons abov Q no rvavs. In wa follows soul b an no onsraon a n as of roaon aroun as fluuaon-sspaon rlaons for onanous fluuang lr an agn ons of parl n ss Σ of surfa a for δ o 4 o o δ 5 o δ o 6 δ o 7

o o δ 8 o o δ 9 wr Ω ± ±. In aon rlaons bwn nu pol an agn ons of roang parl an onanous fluuang lroagn fl of surfa n rfrn fra Σ ar gvn b p 3 n p 3 n p 3 n p 3 n 3 p 3 n 4 p 3 n 5 I s wor nong a all Fourr-ransfors ar an a pon. 3. Rsuls

As a rsul of followng sanar alulaons w allowan for 5 w oban on- an oubl-pr uans no ral an agnar oponns of funons o I p o p R o p I o p R 4 F 6 o o p I o o p I 4 Q & 7 o o p I M 8 wr µ ε

µ µ ε ε. Morovr bra rs n s. 6 8 ar gvn b pll wrn rs w rplans. 4. Roaon as paralll o surfa as wr roaon as s paralll o surfa s u slar o as Ω II. Obvousl onfguraons Ω Ω Ω Ω Ω an Ω Ω Ω Ω Ω orronng o Ω II an Ω II. ar uvaln. Fluuaon-sspaon rlaons 4-9 an s. 5 soul b rwrn usng a l pruaon. n n as Ω II uaons analogous o 6 8 a for o p I o p R o p I o p R 4 F 9 o o p I o o p I 4 Q &

M p I o o In as Ω II s. 9 ar sa w rplans. Morovr s as o vrf a a Ω s. 6 9 an s. 7 ar ransfor no on anor an srb sa Casr-Polr for an parl-surfa raav a ang wn surfa s n ral ulbru w vauu nvronn bu ou of ulbru w parl [6]. On or an wn nglng raraon ffs n l [34]. s.6 ru o orronng nonrar rsuls oban n 5. Iall onung surfa an parl L us onsr spls as assung nrang subsss o b all onung. In s as w us a o R sgn Ω 3 R 3 o sgn Subsung no 6 an arrng ou ngraons ls wll-nown rsul [67] 3 9 R F 3 4 5 orronng o an all onung ovabl parl an all onung alf-a. sa rsul s oban unr onons of fn onuv n lng as of srong raraon wr parl-surfa san s u grar an arars wav-lng n r absorpon ra [8]. ffrn n nural offns n [67] an [8] s u o la of ff of agn polaraon n [8].

rfor wn ap assupons roaon of parl os no alr Casr- Polr for. s rsul an also b forula as follows: prov a agnar pars of parl polarabls ar ual o ro r s no ouplng bwn parl roaon an ro osllaons of surfa lroagn fl. Morovr a for all onung parl an surfa fronal on an ang ra of parl sappar. Conrar o a ff of roaon wll b apprabl n as of ral aral proprs of parl surfa or bo of as wll as n as of ffrn praurs. 6. Conlusons For frs w av gnral rnl oban oral prssons for fluuaon lroagn araon for fronal on an ra of raav a ang bwn a roang parl an surfa w allowan for ff of raraon. arlr forulas n vansn-fl l follow fro gnral rsuls as a paral as. W av sown a n as of all onung parl an surfa angular roaon of parl os no nflun Casr-Polr for a ro praur of ss wl fronal on an ang ra a ar ual o ro. Rfrns [] A. Manjavaas F. Gara Abajo Ps. Rv. L. 5 36. [] R. Zao A. Manjavaas F Gara Abajo an J.. Pnr Ps. Rv. L. 9 364. [3] G.V. Dov A.A. Kasov urops. L. 99 63. [4] A.A. Kasov G.V. Dov arv: 8.63; 9.46; 9.488;.6957. [5] G.V. Dov A.A. Kasov arxv: 3.76; 3.67. [6] G.V. Dov A.A. Kasov Ps. Sol. Sa 593; Nanosruurs. Ma. Ps. & Molng 95. [7]. Daa L.H. For Ps. L. A839834. [8] L.D. Lanau.M. Lfs Cours of oral Pss Vol. 9: Sasal Pss Par urwor-hnann Ofor 998.

Fg. Goral onfguraon an oorna sss us.