Electrical field generated by a charged harmonic oscillator at thermodynamic equilibrium

Similar documents
SAFE OPERATION OF TUBULAR (PFR) ADIABATIC REACTORS. FIGURE 1: Temperature as a function of space time in an adiabatic PFR with exothermic reaction.

Ch. 6 Free Electron Fermi Gas

The theory of relativistic spontaneous emission from hydrogen atom in Schwarzschild Black hole

Lecture 14. Time Harmonic Fields

( ) L = D e. e e. Example:

The Real Hydrogen Atom

Light scattering and absorption by atmospheric particulates. Part 2: Scattering and absorption by spherical particles.

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is

Galaxy Photometry. Recalling the relationship between flux and luminosity, Flux = brightness becomes

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom

Magnetic effects and the peculiarity of the electron spin in Atoms


m = Mass flow rate The Lonely Electron Example 0a:

Bohr type models of the atom give a totally incorrect picture of the atom and are of only historical significance.

Axe Wo. Blood Circle Just like with using knives, when we are using an axe we have to keep an area around us clear. Axe Safety Check list:

The Hydrogen Atom. Chapter 7

8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions

VISUALIZATION OF TRIVARIATE NURBS VOLUMES

II.3. DETERMINATION OF THE ELECTRON SPECIFIC CHARGE BY MEANS OF THE MAGNETRON METHOD

GUC (Dr. Hany Hammad)

Helping you learn to save. Pigby s tips and tricks

SOLUTION. The reactor thermal output is related to the maximum heat flux in the hot channel by. Z( z ). The position of maximum heat flux ( z max

PREPARATORY MATHEMATICS FOR ENGINEERS

ENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles

E F. and H v. or A r and F r are dual of each other.

We first write the integrand into partial fractions and then integrate. By EXAMPLE 27 we have the identity

GUC (Dr. Hany Hammad) 4/20/2016

Quantum Mechanics for Scientists and Engineers. David Miller

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation

DISCRETE-TIME RANDOM PROCESSES

Solution: APPM 1360 Final Spring 2013

Eielson Air Force Base PFOS Plume Perflourooctane sulfonate (PFOS), a component of fire-fighting foams Delineation is incomplete 4 known source areas

Helping every little saver

Chapter 6 Perturbation theory

Handout 30. Optical Processes in Solids and the Dielectric Constant

Chapter 4 Derivatives [ ] = ( ) ( )= + ( ) + + = ()= + ()+ Exercise 4.1. Review of Prerequisite Skills. 1. f. 6. d. 4. b. lim. x x. = lim = c.

Chapter Taylor Theorem Revisited

Kinetics. Central Force Motion & Space Mechanics

National Survey of Student Engagement, Spring 2011 The University at Albany, SUNY

physicsandmathstutor.com

6XSSO\ VLGH FRQVWUDLQWV DQG ERWWOHQHFNV

Ballistic Atmospheric Entry

MATH Midterm Examination Victor Matveev October 26, 2016

School of Aerospace Engineering Origins of Quantum Theory. Measurements of emission of light (EM radiation) from (H) atoms found discrete lines

School of Electrical Engineering. Lecture 2: Wire Antennas

ADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS. Ghiocel Groza*, S. M. Ali Khan** 1. Introduction

6.Optical and electronic properties of Low

RMO Sample Paper 1 Solutions :

Curvature singularity

4/20/2017. The Invention of the Modern Atom Early atomic models: Dalton model: Atom as billiard ball. The First Atomic Theorist.

= x. ˆ, eˆ. , eˆ. 5. Curvilinear Coordinates. See figures 2.11 and Cylindrical. Spherical

The tight-binding method

O QP P. Limit Theorems. p and to see if it will be less than a pre-assigned number,. p n

E o and the equilibrium constant, K

( ) ( ) ( ) 2011 HSC Mathematics Solutions ( 6) ( ) ( ) ( ) π π. αβ = = 2. α β αβ. Question 1. (iii) 1 1 β + (a) (4 sig. fig.

TDVDC-345 STA= HT= ELE= PARCEL NO /24/12

= h. Geometrically this quantity represents the slope of the secant line connecting the points

are specified , are linearly independent Otherwise, they are linearly dependent, and one is expressed by a linear combination of the others

The Derivative as a Function

Partition Functions and Ideal Gases

Another Explanation of the Cosmological Redshift. April 6, 2010.

MAT3700. Tutorial Letter 201/2/2016. Mathematics III (Engineering) Semester 2. Department of Mathematical sciences MAT3700/201/2/2016

Analysis of a Finite Quantum Well

physicsandmathstutor.com

Exponential Functions

PD12 21 The Highlands East Sign Package

ATTACHMENT 1. MOUNTAIN PARK LAND Page 2 of 5

Handout 32. Electronic Energy Transport and Thermoelectric Effects

r ADD. TEMP. WORKSPACE

Control Systems. Controllability and Observability (Chapter 6)

Central County Fire & Rescue - Station #5

Proc. of the 23rd Intl. Conf. on Parallel Processing, St. Charles, Illinois, August 1994, vol. 3, pp. 227{ Hanan Samet

Einstein Equations for Tetrad Fields

Digital Signal Processing, Fall 2006

ENGO 431 Analytical Photogrammetry

Trade Patterns, Production networks, and Trade and employment in the Asia-US region

Zeroth moment of the Boltzmann Equation The Equation of Continuity (Particle conservation)

Collisionless Hall-MHD Modeling Near a Magnetic Null. D. J. Strozzi J. J. Ramos MIT Plasma Science and Fusion Center

Surface x(u, v) and curve α(t) on it given by u(t) & v(t). Math 4140/5530: Differential Geometry

Homework 1: Solutions

SUPPLEMENTARY INFORMATION

physicsandmathstutor.com

Notes on Planetary Motion

Free carriers in materials

Practice Problem Solutions: Exam 1

UGC POINT LEADING INSTITUE FOR CSIR-JRF/NET, GATE & JAM. are the polar coordinates of P, then. 2 sec sec tan. m 2a m m r. f r.

ANSWER KEY WITH SOLUTION PAPER - 2 MATHEMATICS SECTION A 1. B 2. B 3. D 4. C 5. B 6. C 7. C 8. B 9. B 10. D 11. C 12. C 13. A 14. B 15.

Chapter 4 Rigid Models and Angular Momentum Eigenstates Homework Solutions

Entire Solution of a Singular Semilinear Elliptic Problem

Lecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e

Problem Value Score Earned No/Wrong Rec -3 Total

Numerical Analysis MTH603. dy dt = = (0) , y n+1. We obtain yn. Therefore. and. Copyright Virtual University of Pakistan 1

GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL

35H MPa Hydraulic Cylinder 3.5 MPa Hydraulic Cylinder 35H-3

Continuous-Time Fourier Transform. Transform. Transform. Transform. Transform. Transform. Definition The CTFT of a continuoustime

Non-Relativistic Limit of Neutron Beta-Decay Cross-Section in the Presence of Strong Magnetic Field

Problem Set 4 Solutions Distributed: February 26, 2016 Due: March 4, 2016

PhysicsAndMathsTutor.com

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

MIL-HDBK OCTOBER 1984 MAINTAINABILITY ANALYSIS

Transcription:

lctical fild gatd by a cagd aic scillat at tdyaic uilibiu STFANO GIODANO Dpatt f Bipysical ad lctic giig Uivsity f Ga Via Opa Pia A 65 Gva ITALY Abstact: - I tis pap w aalys t lctagtic fild gatd by a cagd paticl i Bwia ti. Tis ti is dscibd as kw by t Lagvi uatis []. t fllwig ctibuts a tak it accut: a ficti fc a additiv wit gaussia is fc ad a dtiistic csvativ fc divd by a gic pttial. T Fkk-Plack [] uati is usful t dscib t ti vluti f t pbability dsity i t pas spac. it t pbability dsity w ca fid t avag valu f t distibuti cag ad t dsity cut du t t paticl ti. Tf w dti t a lctagtic fild by as f t tadd pttials. T tal cuplig wit t bat lads t syst t t uilibiu situati: t Fkk-Plack uati adits t Bltza distibuti as asypttic sluti. cput t lctical fild i tis situati f tal uilibiu. I paticula w csid a aic scillat cupld t t tal bat at tdyaic uilibiu. Tis calculati is ad wit classical ad uatu caics: i bt cas w btai sults wic galis t Culb law. I t liit f lw tpatu t classical fula f t lctical pttial bc bviusly cicidt wit t Culb law: t uatal sults i tis liit giv paticula latis wic a itisically dpdig t uatu caics. Oly w t Plack cstat is csidd gligibl t uatal sults bca siila t t classical. Ky-ds: -Pbabilistic tds Stcastic pcsss lctagtics Quatu caics. Itducti T classical ti f a paticl i a tal bat ud t acti f a csvativ fc fild is dscibd by t wll kw Lagvi uatis []. T ffcts f t bat a dlld wit a ficti t ad a is t. T cspdig Fkk-Plack uati [] dscibs t ti vluti f t pbability dsity i t pas spac ad at uilibiu it lads t t Bltza distibuti law. If t paticl i ti is cagd it gats a lctagtic fild wic assus t caact f stcastic pcss. csid a paticl f ass [Kg] ad cag [Cb] dscibd by psiti [] ad vlcity v [.sc - ]. If t fc fild is du t pttial gy U() [J] t Lagvi dyaic syst f uatis is t fllwig: d v dt dv dt U β v D () β [z] is t Lagvi s cllisi fucy ficti cfficit; D[ sc - ] is t diffusi cfficit ad ccs t ffct f t additiv wit gaussia is [sc -/ ]. I t fllwig w always us gaussia is wit a clati T fucti ( ( τ ) I δ t τ ad a a valu ( { } (T as taspsiti as avag valu I is t idtity ati f d t δ ( is t Diac dlta fucti). T

cspdig Fkk-Plack uati f t v t is: dsity ( v t U v β ( v ) D () v v p T cag distibuti ad cut dsity f t paticl accdig t stadad us f t Diac t-disial dlta fucti a: J δ ( ( ) v( δ ( ( ) () ca cput t avag valu f t cag distibuti ad cut dsity usig t pbability dsity i t pas spac: J δ ( ~ ) ( ~ ~ v ~ v ~ v ( δ ( ~ ) ( ~ ~ v ~ v dv ~ v~ dv~ ddv ~ ~ () d~ dv~ T avag f t lctagtic pttials ca b calculatd by as f t tadd pttials btaiig: A ( µ v t v v t c c dvd (5) dvd Tus t a filds a divd by t pttials: B A A t (6) Tf t pbability dsity sluti f t Fkk-Plack uati dscibig t ti f a cagd paticl is t fudatal tl t aalys t avagd lctagtic fild gatd by t paticl itslf. I paticula w aalys t fild gatd by a paticl i tdyaic uilibiu wit a tal bat. It is t difficult t vify tat t fllwig Bltza distibuti is t asypttic sluti ( t vyw) f t Fkk-Plack uati (): vv U (7) ( v ) w is t classical patiti fucti: vv p dv U p d U p d ad w av dfid t tpatu T [ K] by as f t isti lati D β ; K is t Bltza cstat. Tis is t asypttic cct sluti ly if t ipp itgal is cvgt. I t fllwig w always f by yptsis t pttial gis wit cvgt patiti fucti. c at uilibiu t lctagtic pttials bc: ( A U p d U p d (8)

ad t w av a uivalt lctstatic situati wit cag distibuti giv by: U p (9) U p d Q F f p () giv t fial pssi f t a lctical fild gatd by a classical aic scillat at tdyaic uilibiu: Classical aic scillat F w w csid t pttial gy f t stadad aic scillat: U () Tf t cag distibuti at uilibiu is: () p T uivalt lctstatic pbl as spical syty ad t w ca us t Gauss law i stadad f: Q ds S w S is a spical sufac f adius ad Q is t ttal cag ctaid. T siplify t calculati w lt : F ad () t w cput t ttal cag Q usig spical cdiats: f p () T cspdig lctical pttial is t fllwig as ca asily vify: f (5) b tat t a valu f t agtic fild is z. Fut w t tat t pssis () ad (5) duc t t Culb law w t tpatu is at abslut z. Idd t a valu f t gy f t classical scillat is ad if T w fid. O ca fid t alizd gapics f t lctical pttial ad fild i Fig. ad w: w ad y w..8.6. Q Fp siϑ d dϑ d. 5 5 aft s aipulati w btai itgatig by pats: Fig.. lctical pttial.

Fig.. lctical fild. As a csuc f t pssis () ad (5) as t fllwig sults f : d d A plig cag is attactd by t scillat if <. If is cls ug t t f gais a fucy Ω f scillati giv by: Ω Quatu aic scillat csid a disial uatu aic scillat; t gy igvalus ad igfuctis a t fllwig: wit! At uilibiu t dsity ati fllws t Bltza distibuti: w δ T dsity pat agig ad is asily btaid by: * ' ' Lttig w calculat t pbability dsity f t psiti at tal uilibiu: f Tis sis ca b cputd [5]btaiig: w f ct If w csid a istpic t-disial aic scillat t t cdiats a statistically idpdt ad t t avag f t cag distibuti is giv by t latisip: tg tg p (6) Lik i t classical cas w lt: tg F ct t fula () is agai cct givig f t a fild:

f tg tg p tg T lctical pttial is: (7) d tg f tg (8) T fucy f scillati f a plig cag wit ass a t t scillatig cag is: If is gligibl t fulas (7) ad (8) bc t classical latis () ad (5). b t a valu f t gy f a istpic t disial aic scillat i tdyaic uilibiu at a tpatu T : at abslut z t gy bcs stis calld z pit gy ad t scillat is i t gud stat. F T w btai t pttial ad fild: f p (9) tg fcs: [] G..Ulbck L.S.Osti"O t ty f t Bwia ti" Pys.v.6()8-8 (9). [] Mig C ag G..Ulbck"O t ty f Bwia ti II" v.md.pys.7(&)-(95). [] S.Cadaska"Stcastic pbls i Pysics ad Asty" v.md.pys.5()-89( 9). [].isk T Fkk-Plack uati (Spig-VlagBli989). [5] L.Ladau Quatu Mcaics( MI Mscw 976). f () I tis cas w ls t aalgy wit t Culb law bcaus t z pit gy is difft t z. As i t classical cas w pt t pptis at : 5