With What Does It Mean the Organic Chemical Phenomena Are Solved?

Size: px
Start display at page:

Download "With What Does It Mean the Organic Chemical Phenomena Are Solved?"

Transcription

1 With What Does It Mean the Oganic Chemical Phenomena Ae Solved? Let me explain the meaning of this title quoting a simple example. Aniline has otho and paa oientation natue and nitobenzene has meta oientation one to an ectophilic substitution eaction (SE). Explanation of the text lev of oganic chemisty, using an aow ecton theoy, comes to show to Fig Resonance of aniline Resonance of nitobenzene Fig.. Oganic chemical expession of esonance in aniline and nitobenzene That is, since the unshaed ecton pai of the atom gathe at otho and paa positions accoding to the aows in aniline and π ecton density of those positions becomes lage, an ectophilic eagent is bought neaby those positions. On the othe hand, in nitobenzene, in ode fo π ectons of otho and paa positions to decease and those positions ae avoided by an ectophilic eagent fo those positions tend to be positivy chaged. Almost all oganic chemists ae satisfied with such explanation. Howeve, does it mean that one undestands these eactions tuly? Let's conside some points bow. () What these aows mean? () If the aows mean the oute to which the ecton movement is expessed, why ae they so? (3) Especially in aniline, why ectons flow into C with low ectonegativity fom with high ectonegativity? (4) What on eath is the cause of deciding atomic ectonegativity, and so on. The aow ecton theoy cannot explain anything of chemical phenomena at all. Owing to the spead of molecula obital calculation pogams, the ecton density in a molecule and the enegy of a eaction pocess can be easily calculated by oganic chemists as wl, and they can show validity of a eaction. Howeve, it is not in chage of the analysis of a phenomenon at all. The poblem is why it bings such a esult. Then, what kind of explanation is the eal explanation of a chemical phenomenon? This is the meaning of the title.

2 See the Fact that a Chemical Phenomenon Bongs to atual Phenomena A chemical phenomenon is egaded as one of the natual phenomena. obody may object this idea. If so, one should also explain a chemical phenomenon fom natual basic pinciples and this may be a natual conclusion. The paticle physics says that thee ae fou sots of foce which goven natue. In ode of stength, they ae stong foce, ectomagnetic foce, weak foce, and gavitational foce. Among them, the foce ated to chemical phenomena is only ectomagnetic foce. The ange which acts although stong foce is vey stong but its action is limited to a nuclea domain (0-5 m). The weak foce commits only at the time of collapse of a nucleus. Gavitational foce is about 0-40 time weak compaed with ectomagnetic foce, and can be disegaded complety. The atual Pinciples that Goven Chemical Phenomena The idea that the ectomagnetic foce is the complete basis to undestand chemical phenomena is not ight. In atoms and molecules, the wave chaacte of ectons plays impotant oles. The wave natue of a substance inevitably accompanies the Pauli uncetainty ation (pinciple). In addition, an ecton has the impotant chaacte: ementay paticles bong to eithe the goup to which only one can exist in one state (femion) o the goup called boson in which many paticles can exist in one state. Hee, a state efes to the stationay enegy state (it does not change in minute time) specified by all the coodinates including intenal ones. Fo example, if it is an ecton, they ae space coodinates and intenal coodinates (the spin, the coodinates of otation in classic undestanding). An ecton bongs to a femion. The question why an ecton is a femion is not a poblem which chemisty asks like the poblem why an ecton has an ectic chage: let's accept these as a fact. The femion chaacte of an ecton appeas concety in chemisty as the Pauli s exclusion pinciple. Afte all, the factos which goven the atomic and molecula wolds will be () the ectomagnetic foce, () the wave chaacte of an ecton (o the pinciple of supepostition), (3) the uncetainty ation, and (4) the Pauli s exclusion pinciple. Although 3 is a facto deived fom, a chemical phenomenon becomes easie to undestand by consideing and 3 sepaaty. The ecton s wave natue seves in undestanding the way of ecton distibution and expansion and shinkage of ecton distibution by obital inteactions. The uncetainty ation is convenient fo qualitative undestanding of the ationship between the ecton's existence ange and its kinetic enegy. How to Undestand Chemical Phenomena on atual Pinciples Using Molecula Obital Theoies Explanation based on the ectomagnetic foce, the wave natue of ectons, the uncetainty ation, and the Pauli s pinciple may be tue undestanding of chemical phenomena. ext, let us

3 conside the concete ways to undestand chemical phenomena fom those basic pinciples. This is compaativy easy. We use molecula obital theoies in ode to explain chemical phenomena. Just use the molecula obital theoies appopiaty. Let me explain using the Hatee-Fock (HF) method as a molecula obital theoy. Although thee ae flows who dislike this method because of not taking the ecton coation, I (tanuki 3) ) think it the exclent molecula obital theoy fo which the viial theoem is mateialized; this is basic equiement as a theoy when it is applied to the mechanical analysis. Besides, the defect that ecton coation is not taken into account is easily emoved by adding vaious ectonic states. Although it is a digession, it should be mentioned that the density functional theoies cannot be used fo the mechanical analyses of chemical phenomena. Although the details of the molecula obital theoy ae omitted, let me point out an impotant fact. The coefficient (c i ) of the expansion function of a molecula obital (ψ) is decided using the vaiation pinciple. E( c, clcilc c n i ) 0 Hee, E is the total ecton enegy. The point is that c is optimized to the total ecton enegy. It is neve optimized to the enegy of atom o between atoms. Although it is a digession, this shows that it is a mistake to divide the enegy of a molecule into those of atoms and between atoms. Moeove, thee is no theoetical guaantee on any kind of patitioning of enegy ad ecton distibution i8nto atoms ad between atoms, such as ecton density population, and bond ode, which have been cuently and taditionally pefomed. Using them also tuns into unsuitable application of a molecula obital theoy. () An Appopiate Enegy Patitioning The Hamiltonian (H ) of a system consists of opeatos of the kinetic enegy of ectons (T) and the potential enegy (V ). V is patitioned into opeatos of -ecton potential enegy (V e ) and -ecton potential enegy (V ee ). The expectation values of these opeatos ae theoetically appopiate. E H T V T V e Ψ V H Ψ T ee Ψ T e ee The fist, second, and thid tems of the ight-hand side of the lowe fomula of Eq.3 espectivy coespond to expectation values of the kinetic enegy of ectons, -ecton potential enegy, and -ecton potential enegy. 3

4 If the LCAO expansion is used (Eq. 4), each tem of Eq. 3 ae, in tems of atomic obitals ( χ ) and thei coefficients (c ), expessed as shown in Eqs. 5 to 7. n i i ψ c χ 4 Ψ T Ps χ ( ) () χ s () dτ 5 s e Q Ps χ ( ) χ s () dτ 6 s Q Q ee Ps Ptu ( s / tu) ( t / su) 7 s t u In these fomulas, P s is the bond-ode between atomic obitals χ and χ s while, (s/tu) is, ( s / tu) χ () χ s () χt () χu() dτdτ Z Although epeated, Eq. 5 gives the kinetic enegy of ectons which oiginate fom the uncetainty ation and Eq. 6 does the ectomagnetic (coulombic) enegy of ectons and nuclei. Eq. 7 coesponds to the inteaction enegy between ectons which includes simple coulombic enegy and the effect of avoiding the existence of the same spins by the Pauli s exclusion pinciple. The effect of the Pauli s exclusion pinciple is expessed by ( t / su) in Eq.7. The detail may be efeed to liteatues 5 to 8. Hee, let us make sue of some technical tems. Coulombic inteaction: the inteaction between two chages Electonic inteaction: the inteactions between two ectons including the Pauli s exclusion pinciple. Electon coation: the effect of ectons in which movement of a cetain ecton affects movement of othe ectons. Since ecton has a negative ectic chage, othe ectons move avoiding the ecton. The Hatee-Fock method does not include this effect, since the inteaction between ectons is taken in as the aveage value. As descibed in the "Poposition" of this HP, no infomation is acquied only by looking at the enegy value. By seeing the enegetic changes accompanying with changes of nuclea position, one can know what will paticipate in the chemical phenomenon fom the basic pinciples of natue. () Some Examples of Fundamental Analysis

5 The analyses of the chemical phenomena by such a view have appeaed fo many yeas, although thee ae not many examples. In 96, Ruedenbeg examined the kinetic enegy of ecton and the potential (nucleus inteaction is also included) enegy of the H -- H system as a function of intenuclea distance between H and H. 9) In conclusion, diffusion of the ecton to H fom H atom takes place at fist causing a fall of the kinetic enegy. At the same time a fall of the potential enegy happens in connection with it. This continues until the nuclea-nuclea epling Coulomb enegy and decease of the kinetic and one-ecton potential enegy ae balanced to each the equilibium distance. In this case, since the numbe of the ectons of the system is one, the effect by the Pauli s exclusion pinciple does not ente, but it is claified how the ectonic kinetic enegy which aises accoding to the uncetainty ation, and coulombic enegy ae coated. The poblem of conjugation of the aniline and nitobenzene shown at the beginning has aleady been dealt with. 8) Let me show the conclusion. The method is, as shown in Fig., to analyze the changes of the patitioned enegies when the substituents ae otated along the C- axis. θ X X A B X : H o O Fig.. Rotation of substituents along the C- axis. The conclusion is as follows. In an ecton-donative substituent goup like an amino goup, due to the ief of the kinetic enegy pessue of the unshaed ecton pai of the atom, the ectons flow into the benzene ing, causing a fall of the kinetic enegy. On the othe hand, in the ecton-withdawing substituent goup like nitobenzene, π ectons of the benzene ing move to the atom due to the stong potential of the atom of the nito goup. The authos have advocated that one calls the fome kinetic-enegy oigin and the latte, the potential-enegy oigin. The physical meaning was given to the conventional concept of ecton-donative and ecton-withdawing natues of substituents, and inconsistency of the concept in the chemisty that ectons flow into the small C atom fom the lage atom of ectonegativity in aniline is solved with the concept of ief of kinetic-enegy pessue. Kinetic-enegy pessue is the concept which Reudenbeg intoduced, and since the ecton confined in naow space has a lage kinetic enegy (due to the uncetainty pinciple), ectons have a tendency to spead. Although it is a concept sdom used, since it is moe diect than using the uncetainty ation, the use of kinetic-enegy pessue seems suitable fo an undestanding of chemical phenomena.

6 Poposition Since chemical phenomena bong to the natual phenomena, an undestanding fom the natual basic pinciples tuns into the fundamental undestanding. The factos which sway the wold of atoms and molecules ae () the ectomagnetic foce, () the wave chaacte of ecton (the pinciple of supeposition), (3) the uncetainty ation, and (4) Pauli s exclusion pincicle, and since those quantities ae calculable with molecula obital methods, one can undestand the cause of a chemical phenomenon fom those oles to obtain the tue undestanding. Moeove, the use of the concept of kinetic-enegy pessue is appopiate fo the chaacte in which the ecton tends to spead due to the uncetainty ation.. It is not contained in the text of oganic chemisty although the cause of deciding atomic ectonegativity is wl undestood.. Ration between the uncetainty ation and the wave natue of ecton may be efeed to Why Conjugation Takes Pace in the Poposition of this HP. 3. Takuki is a accoon-like mountain dog who sometime jokes human beings. Be awae! 4. Viial Theoem: the theoem that the atio of kinetic enegy (T) to the potential enegy (V) is - in the system in a stationay state (V/T-). This theoem is an impotant one which is mateialized in both classical and quantum mechanics. If this theoem is not theoetically fulfilled in a molecula obital theoy, such a theoy is not suitable fo the mechanical analysis of a phenomenon. 5. H.Ichikawa and Y. Ebisawa, J. Am. Chem. Soc., 07, 6 (985) 6. H. Ichikawa, Y. Ebisawa, K. Sameshima, Bull. Chem, Soc. Jpn., 6, 659 (988) 7. H. Ichikawa, Y. Ebisawa, A. Shigihaa, J. Phys. Chem., 9, 440 (988) 8. H. Ichikawa, K. Sameshia, J. Phys. Og. Chem., 3, 587 (990) 9. K. Reudenbeg, Rev. Mod. Phys., 34, 36 (96). See also, M.J. Feinbeg, K. Reudenbeg, J. Chem. Phys., 54, 495 (97)

7.2. Coulomb s Law. The Electric Force

7.2. Coulomb s Law. The Electric Force Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat

More information

On the integration of the equations of hydrodynamics

On the integration of the equations of hydrodynamics Uebe die Integation de hydodynamischen Gleichungen J f eine u angew Math 56 (859) -0 On the integation of the equations of hydodynamics (By A Clebsch at Calsuhe) Tanslated by D H Delphenich In a pevious

More information

Charges, Coulomb s Law, and Electric Fields

Charges, Coulomb s Law, and Electric Fields Q&E -1 Chages, Coulomb s Law, and Electic ields Some expeimental facts: Expeimental fact 1: Electic chage comes in two types, which we call (+) and (). An atom consists of a heavy (+) chaged nucleus suounded

More information

Many Electron Atoms. Electrons can be put into approximate orbitals and the properties of the many electron systems can be catalogued

Many Electron Atoms. Electrons can be put into approximate orbitals and the properties of the many electron systems can be catalogued Many Electon Atoms The many body poblem cannot be solved analytically. We content ouselves with developing appoximate methods that can yield quite accuate esults (but usually equie a compute). The electons

More information

Problem Set 10 Solutions

Problem Set 10 Solutions Chemisty 6 D. Jean M. Standad Poblem Set 0 Solutions. Give the explicit fom of the Hamiltonian opeato (in atomic units) fo the lithium atom. You expession should not include any summations (expand them

More information

Single Particle State AB AB

Single Particle State AB AB LECTURE 3 Maxwell Boltzmann, Femi, and Bose Statistics Suppose we have a gas of N identical point paticles in a box of volume V. When we say gas, we mean that the paticles ae not inteacting with one anothe.

More information

Nuclear and Particle Physics - Lecture 20 The shell model

Nuclear and Particle Physics - Lecture 20 The shell model 1 Intoduction Nuclea and Paticle Physics - Lectue 0 The shell model It is appaent that the semi-empiical mass fomula does a good job of descibing tends but not the non-smooth behaviou of the binding enegy.

More information

PHYSICS 151 Notes for Online Lecture #36

PHYSICS 151 Notes for Online Lecture #36 Electomagnetism PHYSICS 151 Notes fo Online Lectue #36 Thee ae fou fundamental foces in natue: 1) gavity ) weak nuclea 3) electomagnetic 4) stong nuclea The latte two opeate within the nucleus of an atom

More information

5.61 Physical Chemistry Lecture #23 page 1 MANY ELECTRON ATOMS

5.61 Physical Chemistry Lecture #23 page 1 MANY ELECTRON ATOMS 5.6 Physical Chemisty Lectue #3 page MAY ELECTRO ATOMS At this point, we see that quantum mechanics allows us to undestand the helium atom, at least qualitatively. What about atoms with moe than two electons,

More information

Physics 505 Homework No. 9 Solutions S9-1

Physics 505 Homework No. 9 Solutions S9-1 Physics 505 Homewok No 9 s S9-1 1 As pomised, hee is the tick fo summing the matix elements fo the Stak effect fo the gound state of the hydogen atom Recall, we need to calculate the coection to the gound

More information

Appendix B The Relativistic Transformation of Forces

Appendix B The Relativistic Transformation of Forces Appendix B The Relativistic Tansfomation of oces B. The ou-foce We intoduced the idea of foces in Chapte 3 whee we saw that the change in the fou-momentum pe unit time is given by the expession d d w x

More information

A thermodynamic degree of freedom solution to the galaxy cluster problem of MOND. Abstract

A thermodynamic degree of freedom solution to the galaxy cluster problem of MOND. Abstract A themodynamic degee of feedom solution to the galaxy cluste poblem of MOND E.P.J. de Haas (Paul) Nijmegen, The Nethelands (Dated: Octobe 23, 2015) Abstact In this pape I discus the degee of feedom paamete

More information

Chem 453/544 Fall /08/03. Exam #1 Solutions

Chem 453/544 Fall /08/03. Exam #1 Solutions Chem 453/544 Fall 3 /8/3 Exam # Solutions. ( points) Use the genealized compessibility diagam povided on the last page to estimate ove what ange of pessues A at oom tempeatue confoms to the ideal gas law

More information

Introduction to Nuclear Forces

Introduction to Nuclear Forces Intoduction to Nuclea Foces One of the main poblems of nuclea physics is to find out the natue of nuclea foces. Nuclea foces diffe fom all othe known types of foces. They cannot be of electical oigin since

More information

ON THE TWO-BODY PROBLEM IN QUANTUM MECHANICS

ON THE TWO-BODY PROBLEM IN QUANTUM MECHANICS ON THE TWO-BODY PROBLEM IN QUANTUM MECHANICS L. MICU Hoia Hulubei National Institute fo Physics and Nuclea Engineeing, P.O. Box MG-6, RO-0775 Buchaest-Maguele, Romania, E-mail: lmicu@theoy.nipne.o (Received

More information

On a quantity that is analogous to potential and a theorem that relates to it

On a quantity that is analogous to potential and a theorem that relates to it Su une quantité analogue au potential et su un théoème y elatif C R Acad Sci 7 (87) 34-39 On a quantity that is analogous to potential and a theoem that elates to it By R CLAUSIUS Tanslated by D H Delphenich

More information

b Ψ Ψ Principles of Organic Chemistry lecture 22, page 1

b Ψ Ψ Principles of Organic Chemistry lecture 22, page 1 Pinciples of Oganic Chemisty lectue, page. Basis fo LCAO and Hückel MO Theoy.. Souces... Hypephysics online. http://hypephysics.phy-ast.gsu.edu/hbase/quantum/qm.html#c... Zimmeman, H. E., Quantum Mechanics

More information

PROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr.

PROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr. POBLM S # SOLUIONS by obet A. DiStasio J. Q. he Bon-Oppenheime appoximation is the standad way of appoximating the gound state of a molecula system. Wite down the conditions that detemine the tonic and

More information

EXAM NMR (8N090) November , am

EXAM NMR (8N090) November , am EXA NR (8N9) Novembe 5 9, 9. 1. am Remaks: 1. The exam consists of 8 questions, each with 3 pats.. Each question yields the same amount of points. 3. You ae allowed to use the fomula sheet which has been

More information

3.012 Fund of Mat Sci: Bonding Lecture 11. The future of electronics? A pentacene molecule deposited on SiO 2. Image removed for copyright reasons.

3.012 Fund of Mat Sci: Bonding Lecture 11. The future of electronics? A pentacene molecule deposited on SiO 2. Image removed for copyright reasons. 3.012 Fund of Mat Sci: Bonding Lectue 11 BONDING IN MOLECULES The futue of electonics? A pentacene molecule deposited on SiO 2 as a thin film Image emoved fo copyight easons. 3.012 Fundamentals of Mateials

More information

15 Solving the Laplace equation by Fourier method

15 Solving the Laplace equation by Fourier method 5 Solving the Laplace equation by Fouie method I aleady intoduced two o thee dimensional heat equation, when I deived it, ecall that it taes the fom u t = α 2 u + F, (5.) whee u: [0, ) D R, D R is the

More information

Nuclear models: Shell model

Nuclear models: Shell model Lectue 3 Nuclea models: Shell model WS0/3: Intoduction to Nuclea and Paticle Physics,, Pat I Nuclea models Nuclea models Models with stong inteaction between the nucleons Liquid dop model α-paticle model

More information

AP Physics Electric Potential Energy

AP Physics Electric Potential Energy AP Physics lectic Potential negy Review of some vital peviously coveed mateial. The impotance of the ealie concepts will be made clea as we poceed. Wok takes place when a foce acts ove a distance. W F

More information

Circular Orbits. and g =

Circular Orbits. and g = using analyse planetay and satellite motion modelled as unifom cicula motion in a univesal gavitation field, a = v = 4π and g = T GM1 GM and F = 1M SATELLITES IN OBIT A satellite is any object that is

More information

Physics 11 Chapter 20: Electric Fields and Forces

Physics 11 Chapter 20: Electric Fields and Forces Physics Chapte 0: Electic Fields and Foces Yesteday is not ous to ecove, but tomoow is ous to win o lose. Lyndon B. Johnson When I am anxious it is because I am living in the futue. When I am depessed

More information

Determining solar characteristics using planetary data

Determining solar characteristics using planetary data Detemining sola chaacteistics using planetay data Intoduction The Sun is a G-type main sequence sta at the cente of the Sola System aound which the planets, including ou Eath, obit. In this investigation

More information

! E da = 4πkQ enc, has E under the integral sign, so it is not ordinarily an

! E da = 4πkQ enc, has E under the integral sign, so it is not ordinarily an Physics 142 Electostatics 2 Page 1 Electostatics 2 Electicity is just oganized lightning. Geoge Calin A tick that sometimes woks: calculating E fom Gauss s law Gauss s law,! E da = 4πkQ enc, has E unde

More information

A Hartree-Fock Example Using Helium

A Hartree-Fock Example Using Helium Univesity of Connecticut DigitalCommons@UConn Chemisty Education Mateials Depatment of Chemisty June 6 A Hatee-Fock Example Using Helium Cal W. David Univesity of Connecticut, Cal.David@uconn.edu Follow

More information

Projection Gravitation, a Projection Force from 5-dimensional Space-time into 4-dimensional Space-time

Projection Gravitation, a Projection Force from 5-dimensional Space-time into 4-dimensional Space-time Intenational Jounal of Physics, 17, Vol. 5, No. 5, 181-196 Available online at http://pubs.sciepub.com/ijp/5/5/6 Science and ducation Publishing DOI:1.1691/ijp-5-5-6 Pojection Gavitation, a Pojection Foce

More information

763620SS STATISTICAL PHYSICS Solutions 2 Autumn 2012

763620SS STATISTICAL PHYSICS Solutions 2 Autumn 2012 763620SS STATISTICAL PHYSICS Solutions 2 Autumn 2012 1. Continuous Random Walk Conside a continuous one-dimensional andom walk. Let w(s i ds i be the pobability that the length of the i th displacement

More information

Section 11. Timescales Radiation transport in stars

Section 11. Timescales Radiation transport in stars Section 11 Timescales 11.1 Radiation tanspot in stas Deep inside stas the adiation eld is vey close to black body. Fo a black-body distibution the photon numbe density at tempeatue T is given by n = 2

More information

Let us next consider how one can calculate one- electron elements of the long- range nuclear- electron potential:

Let us next consider how one can calculate one- electron elements of the long- range nuclear- electron potential: Hatee- Fock Long Range In the following assume the patition of 1/ into shot ange and long ance components 1 efc( / a) ef ( / a) + Hee a is a paamete detemining the patitioning between shot ange and long

More information

arxiv: v1 [physics.gen-ph] 18 Aug 2018

arxiv: v1 [physics.gen-ph] 18 Aug 2018 Path integal and Sommefeld quantization axiv:1809.04416v1 [physics.gen-ph] 18 Aug 018 Mikoto Matsuda 1, and Takehisa Fujita, 1 Japan Health and Medical technological college, Tokyo, Japan College of Science

More information

From Gravitational Collapse to Black Holes

From Gravitational Collapse to Black Holes Fom Gavitational Collapse to Black Holes T. Nguyen PHY 391 Independent Study Tem Pape Pof. S.G. Rajeev Univesity of Rocheste Decembe 0, 018 1 Intoduction The pupose of this independent study is to familiaize

More information

AST 121S: The origin and evolution of the Universe. Introduction to Mathematical Handout 1

AST 121S: The origin and evolution of the Universe. Introduction to Mathematical Handout 1 Please ead this fist... AST S: The oigin and evolution of the Univese Intoduction to Mathematical Handout This is an unusually long hand-out and one which uses in places mathematics that you may not be

More information

The Substring Search Problem

The Substring Search Problem The Substing Seach Poblem One algoithm which is used in a vaiety of applications is the family of substing seach algoithms. These algoithms allow a use to detemine if, given two chaacte stings, one is

More information

PES 3950/PHYS 6950: Homework Assignment 6

PES 3950/PHYS 6950: Homework Assignment 6 PES 3950/PHYS 6950: Homewok Assignment 6 Handed out: Monday Apil 7 Due in: Wednesday May 6, at the stat of class at 3:05 pm shap Show all woking and easoning to eceive full points. Question 1 [5 points]

More information

The Millikan Experiment: Determining the Elementary Charge

The Millikan Experiment: Determining the Elementary Charge LAB EXERCISE 7.5.1 7.5 The Elementay Chage (p. 374) Can you think of a method that could be used to suggest that an elementay chage exists? Figue 1 Robet Millikan (1868 1953) m + q V b The Millikan Expeiment:

More information

Pulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects

Pulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects Pulse Neuton Neuton (PNN) tool logging fo poosity Some theoetical aspects Intoduction Pehaps the most citicism of Pulse Neuton Neuon (PNN) logging methods has been chage that PNN is to sensitive to the

More information

Chapter 2: Basic Physics and Math Supplements

Chapter 2: Basic Physics and Math Supplements Chapte 2: Basic Physics and Math Supplements Decembe 1, 215 1 Supplement 2.1: Centipetal Acceleation This supplement expands on a topic addessed on page 19 of the textbook. Ou task hee is to calculate

More information

Quantum Mechanics II

Quantum Mechanics II Quantum Mechanics II Pof. Bois Altshule Apil 25, 2 Lectue 25 We have been dicussing the analytic popeties of the S-matix element. Remembe the adial wave function was u kl () = R kl () e ik iπl/2 S l (k)e

More information

Doublet structure of Alkali spectra:

Doublet structure of Alkali spectra: Doublet stuctue of : Caeful examination of the specta of alkali metals shows that each membe of some of the seies ae closed doublets. Fo example, sodium yellow line, coesponding to 3p 3s tansition, is

More information

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below. Fall 2007 Qualifie Pat II 12 minute questions 11) A thin, unifom od of mass M is suppoted by two vetical stings, as shown below. Find the tension in the emaining sting immediately afte one of the stings

More information

Mechanics Physics 151

Mechanics Physics 151 Mechanics Physics 151 Lectue 5 Cental Foce Poblem (Chapte 3) What We Did Last Time Intoduced Hamilton s Pinciple Action integal is stationay fo the actual path Deived Lagange s Equations Used calculus

More information

Lecture 7: Angular Momentum, Hydrogen Atom

Lecture 7: Angular Momentum, Hydrogen Atom Lectue 7: Angula Momentum, Hydogen Atom Vecto Quantization of Angula Momentum and Nomalization of 3D Rigid Roto wavefunctions Conside l, so L 2 2 2. Thus, we have L 2. Thee ae thee possibilities fo L z

More information

The law of universal attraction with momentum exchange between objects and microparticles

The law of universal attraction with momentum exchange between objects and microparticles Vol. 8(40), pp. 1968-197, 5 Octobe, 013 DOI 10.5897/SRE013.5631 ISSN 199-48 013 Academic Jounals http://www.academicjounals.og/sre Scientific Reseach and Essays Review The law of univesal attaction with

More information

OSCILLATIONS AND GRAVITATION

OSCILLATIONS AND GRAVITATION 1. SIMPLE HARMONIC MOTION Simple hamonic motion is any motion that is equivalent to a single component of unifom cicula motion. In this situation the velocity is always geatest in the middle of the motion,

More information

Entropy and Free Energy: Predicting the direction of spontaneous change The approach to Chemical equilibrium

Entropy and Free Energy: Predicting the direction of spontaneous change The approach to Chemical equilibrium Lectue 8-9 Entopy and Fee Enegy: Pedicting the diection of spontaneous change The appoach to Chemical equilibium Absolute entopy and the thid law of themodynamics To define the entopy of a compound in

More information

Preliminary Exam: Quantum Physics 1/14/2011, 9:00-3:00

Preliminary Exam: Quantum Physics 1/14/2011, 9:00-3:00 Peliminay Exam: Quantum Physics /4/ 9:-: Answe a total of SIX questions of which at least TWO ae fom section A and at least THREE ae fom section B Fo you answes you can use eithe the blue books o individual

More information

Scattering in Three Dimensions

Scattering in Three Dimensions Scatteing in Thee Dimensions Scatteing expeiments ae an impotant souce of infomation about quantum systems, anging in enegy fom vey low enegy chemical eactions to the highest possible enegies at the LHC.

More information

Chapter 5 Force and Motion

Chapter 5 Force and Motion Chapte 5 Foce and Motion In Chaptes 2 and 4 we have studied kinematics, i.e., we descibed the motion of objects using paametes such as the position vecto, velocity, and acceleation without any insights

More information

Physics 235 Chapter 5. Chapter 5 Gravitation

Physics 235 Chapter 5. Chapter 5 Gravitation Chapte 5 Gavitation In this Chapte we will eview the popeties of the gavitational foce. The gavitational foce has been discussed in geat detail in you intoductoy physics couses, and we will pimaily focus

More information

Chapter 5 Force and Motion

Chapter 5 Force and Motion Chapte 5 Foce and Motion In chaptes 2 and 4 we have studied kinematics i.e. descibed the motion of objects using paametes such as the position vecto, velocity and acceleation without any insights as to

More information

Stanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012

Stanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012 Stanfod Univesity CS59Q: Quantum Computing Handout 8 Luca Tevisan Octobe 8, 0 Lectue 8 In which we use the quantum Fouie tansfom to solve the peiod-finding poblem. The Peiod Finding Poblem Let f : {0,...,

More information

20-9 ELECTRIC FIELD LINES 20-9 ELECTRIC POTENTIAL. Answers to the Conceptual Questions. Chapter 20 Electricity 241

20-9 ELECTRIC FIELD LINES 20-9 ELECTRIC POTENTIAL. Answers to the Conceptual Questions. Chapter 20 Electricity 241 Chapte 0 Electicity 41 0-9 ELECTRIC IELD LINES Goals Illustate the concept of electic field lines. Content The electic field can be symbolized by lines of foce thoughout space. The electic field is stonge

More information

Electromagnetism Physics 15b

Electromagnetism Physics 15b lectomagnetism Physics 15b Lectue #20 Dielectics lectic Dipoles Pucell 10.1 10.6 What We Did Last Time Plane wave solutions of Maxwell s equations = 0 sin(k ωt) B = B 0 sin(k ωt) ω = kc, 0 = B, 0 ˆk =

More information

Chapter Sixteen: Electric Charge and Electric Fields

Chapter Sixteen: Electric Charge and Electric Fields Chapte Sixteen: Electic Chage and Electic Fields Key Tems Chage Conducto The fundamental electical popety to which the mutual attactions o epulsions between electons and potons ae attibuted. Any mateial

More information

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations MATH 415, WEEK 3: Paamete-Dependence and Bifucations 1 A Note on Paamete Dependence We should pause to make a bief note about the ole played in the study of dynamical systems by the system s paametes.

More information

Exploration of the three-person duel

Exploration of the three-person duel Exploation of the thee-peson duel Andy Paish 15 August 2006 1 The duel Pictue a duel: two shootes facing one anothe, taking tuns fiing at one anothe, each with a fixed pobability of hitting his opponent.

More information

Diffusion and Transport. 10. Friction and the Langevin Equation. Langevin Equation. f d. f ext. f () t f () t. Then Newton s second law is ma f f f t.

Diffusion and Transport. 10. Friction and the Langevin Equation. Langevin Equation. f d. f ext. f () t f () t. Then Newton s second law is ma f f f t. Diffusion and Tanspot 10. Fiction and the Langevin Equation Now let s elate the phenomena of ownian motion and diffusion to the concept of fiction, i.e., the esistance to movement that the paticle in the

More information

20th Century Atomic Theory - Hydrogen Atom

20th Century Atomic Theory - Hydrogen Atom 0th Centuy Atomic Theoy - Hydogen Atom Ruthefod s scatteing expeiments (Section.5, pp. 53-55) in 1910 led to a nuclea model of the atom whee all the positive chage and most of the mass wee concentated

More information

Chapter 13 Gravitation

Chapter 13 Gravitation Chapte 13 Gavitation In this chapte we will exploe the following topics: -Newton s law of gavitation, which descibes the attactive foce between two point masses and its application to extended objects

More information

A new approach in classical electrodynamics to protect principle of causality

A new approach in classical electrodynamics to protect principle of causality A new appoach in classical electodynamics to potect pinciple of causality Biswaanjan Dikshit * Lase and Plasma Technology Division Bhabha Atomic Reseach Cente, Mumbai-400085 INDIA * Coesponding autho E-mail:

More information

The evolution of the phase space density of particle beams in external fields

The evolution of the phase space density of particle beams in external fields The evolution of the phase space density of paticle beams in extenal fields E.G.Bessonov Lebedev Phys. Inst. RAS, Moscow, Russia, COOL 09 Wokshop on Beam Cooling and Related Topics August 31 Septembe 4,

More information

5.111 Lecture Summary #6 Monday, September 15, 2014

5.111 Lecture Summary #6 Monday, September 15, 2014 5.111 Lectue Summay #6 Monday, Septembe 15, 014 Readings fo today: Section 1.9 Atomic Obitals. Section 1.10 Electon Spin, Section 1.11 The Electonic Stuctue of Hydogen. (Same sections in 4 th ed.) Read

More information

Supporting information

Supporting information Electonic Supplementay Mateial (ESI) fo Physical Chemisty Chemical Physics. This jounal is the Owne Societies 18 Suppoting infomation Nonstoichiometic oxides as a continuous homologous seies: linea fee-enegy

More information

A Relativistic Electron in a Coulomb Potential

A Relativistic Electron in a Coulomb Potential A Relativistic Electon in a Coulomb Potential Alfed Whitehead Physics 518, Fall 009 The Poblem Solve the Diac Equation fo an electon in a Coulomb potential. Identify the conseved quantum numbes. Specify

More information

calculation the Hartree -Fock energy of 1s shell for some ions

calculation the Hartree -Fock energy of 1s shell for some ions JOURNAL OF KUFA PHYSICS Vol.6/ No. (4) calculation the Hatee -Fock enegy of s shell fo some ions Depatment of Physics, College of Science, Kufa Univesity E-mail : shaimanuclea@yahoo.com Abstact: In this

More information

Radial Inflow Experiment:GFD III

Radial Inflow Experiment:GFD III Radial Inflow Expeiment:GFD III John Mashall Febuay 6, 003 Abstact We otate a cylinde about its vetical axis: the cylinde has a cicula dain hole in the cente of its bottom. Wate entes at a constant ate

More information

Teachers notes. Beyond the Thrills excursions. Worksheets in this book. Completing the worksheets

Teachers notes. Beyond the Thrills excursions. Worksheets in this book. Completing the worksheets Beyond the Thills excusions Teaches notes Physics is the science of how the wold (and Univese) woks. Luna Pak Sydney is a lage hands-on physics laboatoy full of fee falling objects, otating systems and

More information

Interatomic Forces. Overview

Interatomic Forces. Overview Inteatomic Foces Oveview an de Walls (shot ange ~1/ 6, weak ~0.010.1 e) Ionic (long ange, ~1/, stong ~510 e) Metallic (no simple dependence, ~0.1e) Covalent (no simple dependence, diectional,~3 e) Hydogen

More information

COLLISIONLESS PLASMA PHYSICS TAKE-HOME EXAM

COLLISIONLESS PLASMA PHYSICS TAKE-HOME EXAM Honou School of Mathematical and Theoetical Physics Pat C Maste of Science in Mathematical and Theoetical Physics COLLISIONLESS PLASMA PHYSICS TAKE-HOME EXAM HILARY TERM 18 TUESDAY, 13TH MARCH 18, 1noon

More information

Physics 111. Ch 12: Gravity. Newton s Universal Gravity. R - hat. the equation. = Gm 1 m 2. F g 2 1. ˆr 2 1. Gravity G =

Physics 111. Ch 12: Gravity. Newton s Universal Gravity. R - hat. the equation. = Gm 1 m 2. F g 2 1. ˆr 2 1. Gravity G = ics Announcements day, embe 9, 004 Ch 1: Gavity Univesal Law Potential Enegy Keple s Laws Ch 15: Fluids density hydostatic equilibium Pascal s Pinciple This week s lab will be anothe physics wokshop -

More information

EQUATIONS OF MOTION LUCA GUIDO MOLINARI

EQUATIONS OF MOTION LUCA GUIDO MOLINARI EQUATIONS OF MOTION LUCA GUIDO MOLINARI 1. Equation of motion of destuction opeatos Conside a system of bosons o femions descibed by a Hamiltonian H = H 1 + H 2, whee H 1 and H 2 ae espectively the one

More information

2 x 8 2 x 2 SKILLS Determine whether the given value is a solution of the. equation. (a) x 2 (b) x 4. (a) x 2 (b) x 4 (a) x 4 (b) x 8

2 x 8 2 x 2 SKILLS Determine whether the given value is a solution of the. equation. (a) x 2 (b) x 4. (a) x 2 (b) x 4 (a) x 4 (b) x 8 5 CHAPTER Fundamentals When solving equations that involve absolute values, we usually take cases. EXAMPLE An Absolute Value Equation Solve the equation 0 x 5 0 3. SOLUTION By the definition of absolute

More information

Quantum Mechanics and General Relativity: Creation Creativity. Youssef Al-Youssef, 2 Rama Khoulandi. University of Aleppo, Aleppo, Syria

Quantum Mechanics and General Relativity: Creation Creativity. Youssef Al-Youssef, 2 Rama Khoulandi. University of Aleppo, Aleppo, Syria Quantum Mechanics and Geneal Relativity: Ceation Ceativity Youssef Al-Youssef, Rama Khoulandi Univesity of Aleppo, Aleppo, Syia Abstact This aticle is concened with a new concept of quantum mechanics theoy

More information

New problems in universal algebraic geometry illustrated by boolean equations

New problems in universal algebraic geometry illustrated by boolean equations New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic

More information

221B Lecture Notes Scattering Theory I

221B Lecture Notes Scattering Theory I Why Scatteing? B Lectue Notes Scatteing Theoy I Scatteing of paticles off taget has been one of the most impotant applications of quantum mechanics. It is pobably the most effective way to study the stuctue

More information

Homework 7 Solutions

Homework 7 Solutions Homewok 7 olutions Phys 4 Octobe 3, 208. Let s talk about a space monkey. As the space monkey is oiginally obiting in a cicula obit and is massive, its tajectoy satisfies m mon 2 G m mon + L 2 2m mon 2

More information

HOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS?

HOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS? 6th INTERNATIONAL MULTIDISCIPLINARY CONFERENCE HOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS? Cecília Sitkuné Göömbei College of Nyíegyháza Hungay Abstact: The

More information

( n x ( ) Last Time Exam 3 results. Question. 3-D particle in box: summary. Modified Bohr model. 3-D Hydrogen atom. r n. = n 2 a o

( n x ( ) Last Time Exam 3 results. Question. 3-D particle in box: summary. Modified Bohr model. 3-D Hydrogen atom. r n. = n 2 a o Last Time Exam 3 esults Quantum tunneling 3-dimensional wave functions Deceasing paticle size Quantum dots paticle in box) This week s honos lectue: Pof. ad histian, Positon Emission Tomogaphy Tue. Dec.

More information

Chapter 3: Theory of Modular Arithmetic 38

Chapter 3: Theory of Modular Arithmetic 38 Chapte 3: Theoy of Modula Aithmetic 38 Section D Chinese Remainde Theoem By the end of this section you will be able to pove the Chinese Remainde Theoem apply this theoem to solve simultaneous linea conguences

More information

Inseting this into the left hand side of the equation of motion above gives the most commonly used algoithm in classical molecula dynamics simulations

Inseting this into the left hand side of the equation of motion above gives the most commonly used algoithm in classical molecula dynamics simulations Chem465 in 2000 Univesity of Washington Lectue notes Hannes Jonsson Classical dynamics When we ae dealing with heavy atoms and high enough enegy o tempeatue, it is often suciently accuate to neglect quantum

More information

QUALITATIVE AND QUANTITATIVE ANALYSIS OF MUSCLE POWER

QUALITATIVE AND QUANTITATIVE ANALYSIS OF MUSCLE POWER QUALITATIVE AND QUANTITATIVE ANALYSIS OF MUSCLE POWER Jey N. Baham Anand B. Shetty Mechanical Kinesiology Laboatoy Depatment of Kinesiology Univesity of Nothen Coloado Geeley, Coloado Muscle powe is one

More information

AP Physics - Coulomb's Law

AP Physics - Coulomb's Law AP Physics - oulomb's Law We ve leaned that electons have a minus one chage and potons have a positive one chage. This plus and minus one business doesn t wok vey well when we go in and ty to do the old

More information

= e2. = 2e2. = 3e2. V = Ze2. where Z is the atomic numnber. Thus, we take as the Hamiltonian for a hydrogenic. H = p2 r. (19.4)

= e2. = 2e2. = 3e2. V = Ze2. where Z is the atomic numnber. Thus, we take as the Hamiltonian for a hydrogenic. H = p2 r. (19.4) Chapte 9 Hydogen Atom I What is H int? That depends on the physical system and the accuacy with which it is descibed. A natual stating point is the fom H int = p + V, (9.) µ which descibes a two-paticle

More information

12.1 INTRODUCTION: STATES OF MANY-PARTICLE SYSTEMS

12.1 INTRODUCTION: STATES OF MANY-PARTICLE SYSTEMS Chapte 1 2 : Many- Paticle Systems Chapte 12: Many-Paticle Systems...186 12.1 Intoduction: States of Many-Paticle Systems...186 12.2 Systems Divisible into Independent Subsystems...188 12.2.1 Distinguishable

More information

TheWaveandHelmholtzEquations

TheWaveandHelmholtzEquations TheWaveandHelmholtzEquations Ramani Duaiswami The Univesity of Mayland, College Pak Febuay 3, 2006 Abstact CMSC828D notes (adapted fom mateial witten with Nail Gumeov). Wok in pogess 1 Acoustic Waves 1.1

More information

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other Electic Potential Enegy, PE Units: Joules Electic Potential, Units: olts 17.1 Electic Potential Enegy Electic foce is a consevative foce and so we can assign an electic potential enegy (PE) to the system

More information

Why Professor Richard Feynman was upset solving the Laplace equation for spherical waves? Anzor A. Khelashvili a)

Why Professor Richard Feynman was upset solving the Laplace equation for spherical waves? Anzor A. Khelashvili a) Why Pofesso Richad Feynman was upset solving the Laplace equation fo spheical waves? Anzo A. Khelashvili a) Institute of High Enegy Physics, Iv. Javakhishvili Tbilisi State Univesity, Univesity St. 9,

More information

Structure of Hadrons. quarks d (down) s (strange) c (charm)

Structure of Hadrons. quarks d (down) s (strange) c (charm) quaks Flavo A t t 0 S B T Q(e) Mc 2 (GeV) u (up) 1 3 1 2-1 2 0 0 0 0 2 3 0.002-0.008 d (down) 1 3 1 2 1 2 0 0 0 0-1 3 0.005-0.015 s (stange) 1 3 0 0-1 0 0 0-1 3 0.1-0.3 c (cham) 1 3 0 0 0 1 0 0 2 3 1.0-1.6

More information

arxiv:hep-th/ v11 4 Feb 2016

arxiv:hep-th/ v11 4 Feb 2016 A Fundamental Modification of Standad Cosmological Metic ChiYi Chen a a chenchiyi@hznu.edu.cn Hangzhou Nomal Univesity, Hangzhou 310036, China axiv:hep-th/0411047v11 4 Feb 016 In this pape a novel physical

More information

HW Solutions # MIT - Prof. Please study example 12.5 "from the earth to the moon". 2GmA v esc

HW Solutions # MIT - Prof. Please study example 12.5 from the earth to the moon. 2GmA v esc HW Solutions # 11-8.01 MIT - Pof. Kowalski Univesal Gavity. 1) 12.23 Escaping Fom Asteoid Please study example 12.5 "fom the eath to the moon". a) The escape velocity deived in the example (fom enegy consevation)

More information

Errors in Nobel Prize for Physics (3) Conservation of Energy Leads to Probability Conservation of Parity, Momentum and so on

Errors in Nobel Prize for Physics (3) Conservation of Energy Leads to Probability Conservation of Parity, Momentum and so on Eos in Nobel ize fo hysics (3) Conseation of Enegy Leads to obability Conseation of aity, Momentum and so on Fu Yuhua (CNOOC Reseach Institute, E-mail:fuyh945@sina.com) Abstact: One of the easons fo 957

More information

? this lecture. ? next lecture. What we have learned so far. a Q E F = q E a. F = q v B a. a Q in motion B. db/dt E. de/dt B.

? this lecture. ? next lecture. What we have learned so far. a Q E F = q E a. F = q v B a. a Q in motion B. db/dt E. de/dt B. PHY 249 Lectue Notes Chapte 32: Page 1 of 12 What we have leaned so fa a a F q a a in motion F q v a a d/ Ae thee othe "static" chages that can make -field? this lectue d/? next lectue da dl Cuve Cuve

More information

2 Lecture 2: The Bohr atom (1913) and the Schrödinger equation (1925)

2 Lecture 2: The Bohr atom (1913) and the Schrödinger equation (1925) 1 Lectue 1: The beginnings of quantum physics 1. The Sten-Gelach expeiment. Atomic clocks 3. Planck 1900, blackbody adiation, and E ω 4. Photoelectic effect 5. Electon diffaction though cystals, de Boglie

More information

( ) [ ] [ ] [ ] δf φ = F φ+δφ F. xdx.

( ) [ ] [ ] [ ] δf φ = F φ+δφ F. xdx. 9. LAGRANGIAN OF THE ELECTROMAGNETIC FIELD In the pevious section the Lagangian and Hamiltonian of an ensemble of point paticles was developed. This appoach is based on a qt. This discete fomulation can

More information

Physics 121 Hour Exam #5 Solution

Physics 121 Hour Exam #5 Solution Physics 2 Hou xam # Solution This exam consists of a five poblems on five pages. Point values ae given with each poblem. They add up to 99 points; you will get fee point to make a total of. In any given

More information

Hypothesis of dark matter and dark energy with minus mass

Hypothesis of dark matter and dark energy with minus mass Hypothesis of dak matte and dak enegy with minus mass Hyoyoung Choi In 1998 yea, obsevation by The High-z Supenova Seach team, if the cosmological constant is 0, Ω M = 0.38(±0.). The quantity of the matte

More information

arxiv: v1 [physics.pop-ph] 3 Jun 2013

arxiv: v1 [physics.pop-ph] 3 Jun 2013 A note on the electostatic enegy of two point chages axiv:1306.0401v1 [physics.pop-ph] 3 Jun 013 A C Tot Instituto de Física Univesidade Fedeal do io de Janeio Caixa Postal 68.58; CEP 1941-97 io de Janeio,

More information