Supplementary Information. Origin of Chains of Au-PbS Nano-Dumbbells in. Space
|
|
- David Payne
- 5 years ago
- Views:
Transcription
1 Supplementy Infomtion Oigin of Chins of Au-PbS Nno-Dumbbells in Spe Chndn Mondl, Ali Hossin Khn, Bidis Ds, Somobt Ahy* & Sujit Sengupt*, Cente fo Advned Mteils, Indin Assoition fo the Cultivtion of Siene, A & B Rj S.C. Mullik Rod, Jdvpu, Kolkt 000, Indi Tt Institute of Fundmentl Reseh, Cente fo Intedisipliny Sienes, Bundvn Colony, Nsingi, Hydebd 50005, Indi *Coesponding Authos E-mil: ms@is.es.in; sujit@tifh.es.in. These uthos ontibuted eqully to this wok
2 We hve ied out one expeiments on the self-ssembly of PbS nnoods. Diffeent onenttion dependnt TEM expeiments wee ied out, whee TEM gids wee peped fom diffeent onenttion of PbS nnood in toluene solutions. All the TEM obsevtion shows ggegted PbS nnoods nd no odeed ssembly in the fom of hins o y ws obseved in TEM Figue S - S. These ontol expeiments suggest the neessity of the Au tips fo the obseved odeing of dumbbells into hins nd ys. b Figue S. TEM imges of PbS nnoods t thee diffeent onenttions 0- moll-, b 4 0- moll-nd 8 0- moll- espetively. Figue S. A shemti of the lignd TOA moleule in the upight ondition. The geometi length of. nm is lulted ounting the length of the lkyl hins
3 geometilly. b A shemti of dumbbells within the hins long with the lignd TOA moleules dsobed on the sufe of the dumbbells. The ltel distne of.5 nm between the djent dumbbells is lge thn the length of two upight TOA moleules.4 nm suggesting tht the self-ssembly is not medited by the intedigittion of the TOA lkyl tils. Figue S. The seleted e eleton difftion SAED pttens fom Au-PbS ods showing pttens fom the fe-enteed ubi stutues of Au nd ubi ok slt stutue of PbS espetively. The SAED shows 00 PbS, 0 PbS nd PbS difftion ings with the inte-plne distnes of 0.9 nm, 0.0 nm nd 0. nm espetively of bulk ok slt PbS JCPDS The Au shows pominent Au nd 00 Au efletions JCPDS onfiming the HRTEM obsevtions.
4 0. nm b 0. nm 0.4 nm 0. nm 0.4 nm 0.9 nm 0.4 nm 0. nm 0.4 nm 0.4 nm Figue S4. The HRTEM imges of single dumbbells onsisting of nd 00 Au tips t the ends of 00 PbS ods, b, ltente oienttion of Au tips with Au nd 00Au fets long the hins of dumbbells. We hve ied out the sttistil nlysis on ou Au-tipped PbS dumbbells. Fo this pupose, we hve to quie shot fmed HRTEM imges fom the diffeent positions of TEM gid nd diffeent smples to pobe the ltente ystllogphi oienttions of the tips long the length of the hin of dumbbells. We hve monitoed fifty diffeent HRTEM imges fo sttistil nlysis; few of them e pesented in the Figue S5. Genelly, eh HRTEM imge fme ontins 4-5 dumbbells in ode to see the lttie finges of the Au tips nd PbS nnood. Within the sets of HRTEM imges pesented in the Figue S5, we hve monitoed dumbbells out of whih only one dumbbell shows stking fult with epet djent Au lttie plnes t the tips. We hve monitoed 00 of suh dumbbells fo sttistil nlysis in whole. We found tht ~% of the 4
5 dumbbells do not mintin ltente oienttions of 00 Au nd Au plnes with in the ssembled hins. Figue S5. HRTEM imges of Au tips t the ends of Au-PbS dumbbells -d showing ltente oienttion of Au nd 00 Au fets long the hins of dumbbells. 5
6 Summy of DFT lultions The intetion between diffeent fets of PbS nnoods nd Au tips e estimted using DFT studies pefomed on tomi lustes epesenting diffeent fets of Au tip nd PbS nnood. PbS nnood is modelled using two lyes of PbS lttie mimiking 00 PbS fets, whih e pobble sites fo Au deposition. Diffeent fets of Au lustes toms in two lyes e nged s Au, 0 Au nd 00 Au fo intetion with 00 PbS nnoods. Diffeent fets of PbS nd Au lustes e gdully bought lose in steps fom lge distne nd the hnges in totl enegies e lulted. The eletoni stutue studies e done using Density Funtionl Theoy DFT s implemented in Gussin 0 softwe M. J. Fish, Gussin0, Revision C.0, Gussin In.: Wllingfod, CT, 004. The hybid funtionl BLYP is used long with -G** bsis set fo S toms nd LnlDZ bsis set with effetive oe potentil is used fo Au nd Pb toms. To vlidte the esults, we hve lso used PBEPBE funtionl see the Tble below. Tble S. Intetion enegies in kev lulted using diffeent DFT funtionls.
7 Dipole moment lultion of PbS nnood Figue S. Shemti fo model PbS nnood nd the top view of the lye t the end of the nnood. The od onsists of 4 of suh lyes. The distne between two lyes is, whih is equl to hlf the lttie pmete of PbS. Thus, the length of the od beomes ~ nm long z-dietion, nd long x nd y-dietions it's dimension is ~.8 nm espetively. Chge of eh Pb tom yellow sphees is e nd tht of eh S tom gey sphee is - e, whee e is hge of n eleton. A ptiul lye in x-y plne n be eithe Pb-ih with 5 Pb toms nd 4 S toms o S-ih with 5 S toms nd 4 Pb toms. The od onsists of 4 of suh lyes. The top nd bottom lye is onstuted to be S-ih due to tthment of Au on PbS nnood. Then thee e S-ih lyes nd 0 Pb-ih lyes.
8 In S-ih lye net hge-e nd in Pb-ih lye net hgee. So, the net hge of the nnood with one ext S-ih lye beomes -e. To neutlize it, two Pb toms e ssumed to be in Pb stte insted of Pb stte. Sine both of these hges e ve, they ty to eside pt fom eh othe. Hene we onside one of them to be situted t the top most lye nd the othe t the bottom most lye. The ight figue shows the topmost lye o the lye t the bottom whee the onge sphee indites the position of the Pb ion. To lulte the dipole moment, we hve onsideed the oigin t the ente of mss of the od. The dipole moment of n ssembly of N numbe of hges is defined s: Hee, fo Pb is e nd fo S is -e, whee e is the hge of one eleton. Hene, whee, ipb is the position of i th Pb tom nd is is the position of i th S tom. With the bove geometil lultions, the z-omponent of net dipole moment n be desibed s follows: The x nd y omponent of net dipole moment i.e x nd y fo eh lye is individully zeo due to symmety exept fo those two lyes onsisting of Pb ions. One suh lye 8
9 is shown in the ight pnel of the bove Figue S. x fo the lye n be 0.0, e-e, e-e, e-e depending on whethe Pb emin on the lines x0, x-x, x-x, x-x espetively. The sme is vlid fo y. Fo two suh lyes, mximum possible vlue of x o y ould be e whih is ~85 Debye. Hene, eh PbS nnood my possess stong dipole moment even in the ubi ystllogphi phse. Now, the dipole-dipole intetion enegy between two dipoles nd septed by distne is given by, Whee is the pemittivity of toluene the solution. whee, nd 0 being the eltive pemittivity nd the pemittivity of fee spe espetively. Fo toluene, ~.8. The intetion enegy between two PbS nnoods with dipole moment of the ode of ~80 Debye nd septed by distne 5 nm in solution phse is lulted to be 0-0 Joule whih is equl to ~k B T t oom tempetue. Moleul Dynmis simultion The intetion potentil between Au tips The intetion between two type- ptiles, is Hmke intetion between two lge sized olloidl ptiles s given below: 9
10 0, ln A A,,,,,, 0,, 800 R A R A <. Whee, A, is the Hmke onstnt nd nd e the dii of the two olloidl ptiles, nd is the utoff. In ou se.0. The intetion between type- ptile nd type-/type- ptile is given by:, /, /, /, / 4 4, /, /, / 0,, A <.. The intetion between two type- ptiles is given below:,,,,,,, 0,, A <...
11 nd two type- ptiles o type- ptile nd type- ptile intets with simple Lennd-JonesLJ intetion: m, n m, n 4Am, n 0, m, n m, n m, n, < m, n..4 Whee, m, n, exept m n. Ou model epesents the min fetues of the luste-luste intetions without the omplexity of n ll-tom ppoh. The fitted vlues of the pmetes e tbulted below. A,.0 A, 40.0 A, 0. A, 0.0 A,.0 A,.0,.0, 0.989,.09,.00,.05,.4,.0, 4.0, 4.0,.0,.0, 4.0 Tble S. Pmetes in the intetion potentil. All quntities e expessed in edued units.
12 Figue S. Phse-digm of D system of dumbbells in -T plne obtined fom MD simultions. The ed dots nd the blk line onneting these iles show the phse boundy of the honeyomb solid phse. The blk ow shows the lowe limit of the honeyomb solid obtined fom elsti onstnt lultions t T0. Blk dshed lines show expeted phse boundies of gsliquid GL, liquidtingul solid LTS, honeyomb solid HStingul solid nd honeyomb solidliquid phses. The system hs liquid phse whih exists t highe density thn the honeyomb solid phse beuse of the pthy intetion. The two phse oexistene egions e shded in gey. A,.0 A, 0.0 A, 8.55 A,.0 A,.0 A, 4.9,.0,.9, 5.48,.0,.0, 4., 0.0, 8.0, 8.05,.5, 5.0, 8.0 Tble S. Pmetes used to lulte the phse-digm shown in Figue S. All quntities e expessed in edued units.
Illustrating the space-time coordinates of the events associated with the apparent and the actual position of a light source
Illustting the spe-time oointes of the events ssoite with the ppent n the tul position of light soue Benh Rothenstein ), Stefn Popesu ) n Geoge J. Spi 3) ) Politehni Univesity of Timiso, Physis Deptment,
More informationCHAPTER 7 Applications of Integration
CHAPTER 7 Applitions of Integtion Setion 7. Ae of Region Between Two Cuves.......... Setion 7. Volume: The Disk Method................. Setion 7. Volume: The Shell Method................ Setion 7. A Length
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 3 Due on Sep. 14, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt
More informationThe Area of a Triangle
The e of Tingle tkhlid June 1, 015 1 Intodution In this tile we will e disussing the vious methods used fo detemining the e of tingle. Let [X] denote the e of X. Using se nd Height To stt off, the simplest
More informationPhysics 217 Practice Final Exam: Solutions
Physis 17 Ptie Finl Em: Solutions Fll This ws the Physis 17 finl em in Fll 199 Twenty-thee students took the em The vege soe ws 11 out of 15 (731%), nd the stndd devition 9 The high nd low soes wee 145
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 4 Due on Sep. 1, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt
More informationPhysics 604 Problem Set 1 Due Sept 16, 2010
Physics 64 Polem et 1 Due ept 16 1 1) ) Inside good conducto the electic field is eo (electons in the conducto ecuse they e fee to move move in wy to cncel ny electic field impessed on the conducto inside
More informationAnswers to test yourself questions
Answes to test youself questions opic Descibing fields Gm Gm Gm Gm he net field t is: g ( d / ) ( 4d / ) d d Gm Gm Gm Gm Gm Gm b he net potentil t is: V d / 4d / d 4d d d V e 4 7 9 49 J kg 7 7 Gm d b E
More informationFEATURE-BASED CRYSTAL CONSTRUCTION IN COMPUTER-AIDED NANO- DESIGN
Poeedings of IDET/IE 008 SME 008 Intentionl Design Engineeing Tehnil onfeenes & omputes nd Infomtion in Engineeing onfeene ugust 3-6 008 New Yok ity NY US DET008-49650 FETURE-SED RYSTL ONSTRUTION IN OMPUTER-IDED
More informationEquations from the Millennium Theory of Inertia and Gravity. Copyright 2004 Joseph A. Rybczyk
Equtions fo the illenniu heoy of Ineti nd vity Copyight 004 Joseph A. Rybzyk ollowing is oplete list of ll of the equtions used o deived in the illenniu heoy of Ineti nd vity. o ese of efeene the equtions
More informationClass Summary. be functions and f( D) , we define the composition of f with g, denoted g f by
Clss Summy.5 Eponentil Functions.6 Invese Functions nd Logithms A function f is ule tht ssigns to ech element D ectly one element, clled f( ), in. Fo emple : function not function Given functions f, g:
More informationA NOTE ON THE POCHHAMMER FREQUENCY EQUATION
A note on the Pohhmme feqeny eqtion SCIENCE AND TECHNOLOGY - Reseh Jonl - Volme 6 - Univesity of Mitis Rédit Mitis. A NOTE ON THE POCHHAMMER FREQUENCY EQUATION by F.R. GOLAM HOSSEN Deptment of Mthemtis
More information( ) D x ( s) if r s (3) ( ) (6) ( r) = d dr D x
SIO 22B, Rudnick dpted fom Dvis III. Single vile sttistics The next few lectues e intended s eview of fundmentl sttistics. The gol is to hve us ll speking the sme lnguge s we move to moe dvnced topics.
More informationExperiment 1 Electric field and electric potential
Expeiment 1 Eleti field and eleti potential Pupose Map eleti equipotential lines and eleti field lines fo two-dimensional hage onfiguations. Equipment Thee sheets of ondutive papes with ondutive-ink eletodes,
More informationELECTROSTATICS. 4πε0. E dr. The electric field is along the direction where the potential decreases at the maximum rate. 5. Electric Potential Energy:
LCTROSTATICS. Quntiztion of Chge: Any chged body, big o smll, hs totl chge which is n integl multile of e, i.e. = ± ne, whee n is n intege hving vlues,, etc, e is the chge of electon which is eul to.6
More informationGeneral Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface
Genel Physics II Chpte 3: Guss w We now wnt to quickly discuss one of the moe useful tools fo clculting the electic field, nmely Guss lw. In ode to undestnd Guss s lw, it seems we need to know the concept
More informationNS-IBTS indices calculation procedure
ICES Dt Cente DATRAS 1.1 NS-IBTS indices 2013 DATRAS Pocedue Document NS-IBTS indices clcultion pocedue Contents Genel... 2 I Rw ge dt CA -> Age-length key by RFA fo defined ge nge ALK... 4 II Rw length
More informationAVS fiziks. Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES
ELECTROMAGNETIC THEORY SOLUTIONS GATE- Q. An insulating sphee of adius a aies a hage density a os ; a. The leading ode tem fo the eleti field at a distane d, fa away fom the hage distibution, is popotional
More informationInfluence of the Magnetic Field in the Solar Interior on the Differential Rotation
Influene of the gneti Fiel in the Sol Inteio on the Diffeentil ottion Lin-Sen Li * Deptment of Physis Nothest Noml Univesity Chnghun Chin * Coesponing utho: Lin-Sen Li Deptment of Physis Nothest Noml Univesity
More informationModule 4: Moral Hazard - Linear Contracts
Module 4: Mol Hzd - Line Contts Infomtion Eonomis (E 55) Geoge Geogidis A pinipl employs n gent. Timing:. The pinipl o es line ontt of the fom w (q) = + q. is the sly, is the bonus te.. The gent hooses
More informationMathematical Reflections, Issue 5, INEQUALITIES ON RATIOS OF RADII OF TANGENT CIRCLES. Y.N. Aliyev
themtil efletions, Issue 5, 015 INEQULITIES ON TIOS OF DII OF TNGENT ILES YN liev stt Some inequlities involving tios of dii of intenll tngent iles whih inteset the given line in fied points e studied
More informationPX3008 Problem Sheet 1
PX38 Poblem Sheet 1 1) A sphee of dius (m) contins chge of unifom density ρ (Cm -3 ). Using Guss' theoem, obtin expessions fo the mgnitude of the electic field (t distnce fom the cente of the sphee) in
More informationPrerna Tower, Road No 2, Contractors Area, Bistupur, Jamshedpur , Tel (0657) ,
R Pen Towe Rod No Conttos Ae Bistupu Jmshedpu 8 Tel (67)89 www.penlsses.om IIT JEE themtis Ppe II PART III ATHEATICS SECTION I (Totl ks : ) (Single Coet Answe Type) This setion ontins 8 multiple hoie questions.
More informationDEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3
DEPATMENT OF CIVIL AND ENVIONMENTAL ENGINEEING FLID MECHANICS III Solutions to Poblem Sheet 3 1. An tmospheic vote is moelle s combintion of viscous coe otting s soli boy with ngul velocity Ω n n iottionl
More informationarxiv: v2 [gr-qc] 22 Sep 2010
PERFECT FLUID DARK MATTER F. Rhmn Deptment of Mthemtis, Jdvpu Univesity, Kolkt 700 032, West Bengl, Indi K. K. Nndi Deptment of Mthemtis, Noth Bengl Univesity, Siligui - 73403, West Bengl, Indi A. Bhd
More informationChapter 28 Sources of Magnetic Field
Chpte 8 Souces of Mgnetic Field - Mgnetic Field of Moving Chge - Mgnetic Field of Cuent Element - Mgnetic Field of Stight Cuent-Cying Conducto - Foce Between Pllel Conductos - Mgnetic Field of Cicul Cuent
More informationMATH34032: Green s Functions, Integral Equations and the Calculus of Variations 1. 1 [(y ) 2 + yy + y 2 ] dx,
MATH3403: Green s Funtions, Integrl Equtions nd the Clulus of Vritions 1 Exmples 5 Qu.1 Show tht the extreml funtion of the funtionl I[y] = 1 0 [(y ) + yy + y ] dx, where y(0) = 0 nd y(1) = 1, is y(x)
More informationFriedmannien equations
..6 Fiedmnnien equtions FLRW metic is : ds c The metic intevl is: dt ( t) d ( ) hee f ( ) is function which detemines globl geometic l popety of D spce. f d sin d One cn put it in the Einstein equtions
More informationOptimization. x = 22 corresponds to local maximum by second derivative test
Optimiztion Lectue 17 discussed the exteme vlues of functions. This lectue will pply the lesson fom Lectue 17 to wod poblems. In this section, it is impotnt to emembe we e in Clculus I nd e deling one-vible
More informationFluids & Bernoulli s Equation. Group Problems 9
Goup Poblems 9 Fluids & Benoulli s Eqution Nme This is moe tutoil-like thn poblem nd leds you though conceptul development of Benoulli s eqution using the ides of Newton s 2 nd lw nd enegy. You e going
More informationSolutions to Midterm Physics 201
Solutions to Midtem Physics. We cn conside this sitution s supeposition of unifomly chged sphee of chge density ρ nd dius R, nd second unifomly chged sphee of chge density ρ nd dius R t the position of
More information(A) 6.32 (B) 9.49 (C) (D) (E) 18.97
Univesity of Bhin Physics 10 Finl Exm Key Fll 004 Deptment of Physics 13/1/005 8:30 10:30 e =1.610 19 C, m e =9.1110 31 Kg, m p =1.6710 7 Kg k=910 9 Nm /C, ε 0 =8.8410 1 C /Nm, µ 0 =4π10 7 T.m/A Pt : 10
More informationElectric Potential. and Equipotentials
Electic Potentil nd Euipotentils U Electicl Potentil Review: W wok done y foce in going fom to long pth. l d E dl F W dl F θ Δ l d E W U U U Δ Δ l d E W U U U U potentil enegy electic potentil Potentil
More informationApril 8, 2017 Math 9. Geometry. Solving vector problems. Problem. Prove that if vectors and satisfy, then.
pril 8, 2017 Mth 9 Geometry Solving vetor prolems Prolem Prove tht if vetors nd stisfy, then Solution 1 onsider the vetor ddition prllelogrm shown in the Figure Sine its digonls hve equl length,, the prllelogrm
More informationAnalysis of Variance for Multiple Factors
Multiple Fto ANOVA Notes Pge wo Fto Anlsis Anlsis of Vine fo Multiple Ftos Conside two ftos (tetments) A nd B with A done t levels nd B done t levels. Within given tetment omintion of A nd B levels, leled
More information1 Fundamental Solutions to the Wave Equation
1 Fundamental Solutions to the Wave Equation Physial insight in the sound geneation mehanism an be gained by onsideing simple analytial solutions to the wave equation. One example is to onside aousti adiation
More information4.2 Boussinesq s Theory. Contents
00477 Pvement Stuctue 4. Stesses in Flexible vement Contents 4. Intoductions to concet of stess nd stin in continuum mechnics 4. Boussinesq s Theoy 4. Bumiste s Theoy 4.4 Thee Lye System Weekset Sung Chte
More informationThe Formulas of Vector Calculus John Cullinan
The Fomuls of Vecto lculus John ullinn Anlytic Geomety A vecto v is n n-tuple of el numbes: v = (v 1,..., v n ). Given two vectos v, w n, ddition nd multipliction with scl t e defined by Hee is bief list
More informationSAMPLE LABORATORY SESSION FOR JAVA MODULE B. Calculations for Sample Cross-Section 2
SAMPLE LABORATORY SESSION FOR JAVA MODULE B Calulations fo Sample Coss-Setion. Use Input. Setion Popeties The popeties of Sample Coss-Setion ae shown in Figue and ae summaized below. Figue : Popeties of
More informationRELATIVE KINEMATICS. q 2 R 12. u 1 O 2 S 2 S 1. r 1 O 1. Figure 1
RELAIVE KINEMAICS he equtions of motion fo point P will be nlyzed in two diffeent efeence systems. One efeence system is inetil, fixed to the gound, the second system is moving in the physicl spce nd the
More informationElectricity & Magnetism Lecture 6: Electric Potential
Electicity & Mgnetism Lectue 6: Electic Potentil Tody s Concept: Electic Potenl (Defined in tems of Pth Integl of Electic Field) Electicity & Mgnesm Lectue 6, Slide Stuff you sked bout:! Explin moe why
More informationELECTRO - MAGNETIC INDUCTION
NTRODUCTON LCTRO - MAGNTC NDUCTON Whenee mgnetic flu linked with cicuit chnges, n e.m.f. is induced in the cicuit. f the cicuit is closed, cuent is lso induced in it. The e.m.f. nd cuent poduced lsts s
More informationRadial geodesics in Schwarzschild spacetime
Rdil geodesics in Schwzschild spcetime Spheiclly symmetic solutions to the Einstein eqution tke the fom ds dt d dθ sin θdϕ whee is constnt. We lso hve the connection components, which now tke the fom using
More informationCOMPUTER AIDED ANALYSIS OF KINEMATICS AND KINETOSTATICS OF SIX-BAR LINKAGE MECHANISM THROUGH THE CONTOUR METHOD
SINTIFI PROINGS XIV INTRNTIONL ONGRSS "MHINS. THNOLОGIS. MTRILS." 17 - SUMMR SSSION W ISSN 55-X PRINT ISSN 55-1 OMPUTR I NLYSIS OF KINMTIS N KINTOSTTIS OF SIX-R LINKG MHNISM THROUGH TH ONTOUR MTHO Pof.so..
More informationPhysics 2A Chapter 10 - Moment of Inertia Fall 2018
Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.
More informationCHAPTER 25 ELECTRIC POTENTIAL
CHPTE 5 ELECTIC POTENTIL Potential Diffeence and Electic Potential Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic foce on the paticle given by F=E. When
More informationChem Homework 11 due Monday, Apr. 28, 2014, 2 PM
Chem 44 - Homework due ondy, pr. 8, 4, P.. . Put this in eq 8.4 terms: E m = m h /m e L for L=d The degenery in the ring system nd the inresed sping per level (4x bigger) mkes the sping between the HOO
More information3.1 Magnetic Fields. Oersted and Ampere
3.1 Mgnetic Fields Oested nd Ampee The definition of mgnetic induction, B Fields of smll loop (dipole) Mgnetic fields in mtte: ) feomgnetism ) mgnetiztion, (M ) c) mgnetic susceptiility, m d) mgnetic field,
More informationU>, and is negative. Electric Potential Energy
Electic Potentil Enegy Think of gvittionl potentil enegy. When the lock is moved veticlly up ginst gvity, the gvittionl foce does negtive wok (you do positive wok), nd the potentil enegy (U) inceses. When
More information17.1 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 informationHomework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is:
. Homewok 3 MAE 8C Poblems, 5, 7, 0, 4, 5, 8, 3, 30, 3 fom Chpte 5, msh & Btt Point souces emit nuetons/sec t points,,, n 3 fin the flux cuent hlf wy between one sie of the tingle (blck ot). The flux fo
More informationCHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD
ollege Physics Student s Mnul hpte 8 HAPTR 8: LTRI HARG AD LTRI ILD 8. STATI LTRIITY AD HARG: OSRVATIO O HARG. ommon sttic electicity involves chges nging fom nnocoulombs to micocoulombs. () How mny electons
More informationMark Scheme (Results) January 2008
Mk Scheme (Results) Jnuy 00 GCE GCE Mthemtics (6679/0) Edecel Limited. Registeed in Englnd nd Wles No. 4496750 Registeed Office: One90 High Holbon, London WCV 7BH Jnuy 00 6679 Mechnics M Mk Scheme Question
More informationPreviously. Extensions to backstepping controller designs. Tracking using backstepping Suppose we consider the general system
436-459 Advnced contol nd utomtion Extensions to bckstepping contolle designs Tcking Obseves (nonline dmping) Peviously Lst lectue we looked t designing nonline contolles using the bckstepping technique
More informationMichael Rotkowitz 1,2
Novembe 23, 2006 edited Line Contolles e Unifomly Optiml fo the Witsenhusen Counteexmple Michel Rotkowitz 1,2 IEEE Confeence on Decision nd Contol, 2006 Abstct In 1968, Witsenhusen intoduced his celebted
More informationπ,π is the angle FROM a! TO b
Mth 151: 1.2 The Dot Poduct We hve scled vectos (o, multiplied vectos y el nume clled scl) nd dded vectos (in ectngul component fom). Cn we multiply vectos togethe? The nswe is YES! In fct, thee e two
More informationPhotographing a time interval
Potogaping a time inteval Benad Rotenstein and Ioan Damian Politennia Univesity of imisoaa Depatment of Pysis imisoaa Romania benad_otenstein@yaoo.om ijdamian@yaoo.om Abstat A metod of measuing time intevals
More informationElectrostatics (Electric Charges and Field) #2 2010
Electic Field: The concept of electic field explains the action at a distance foce between two chaged paticles. Evey chage poduces a field aound it so that any othe chaged paticle expeiences a foce when
More informationChapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s:
Chpte 7 Kleene s Theoem 7.1 Kleene s Theoem The following theoem is the most impotnt nd fundmentl esult in the theoy of FA s: Theoem 6 Any lnguge tht cn e defined y eithe egul expession, o finite utomt,
More informationChapter Direct Method of Interpolation More Examples Mechanical Engineering
Chpte 5 iect Method o Intepoltion Moe Exmples Mechnicl Engineeing Exmple Fo the pupose o shinking tunnion into hub, the eduction o dimete o tunnion sht by cooling it though tempetue chnge o is given by
More informationAlgebra Based Physics. Gravitational Force. PSI Honors universal gravitation presentation Update Fall 2016.notebookNovember 10, 2016
Newton's Lw of Univesl Gvittion Gvittionl Foce lick on the topic to go to tht section Gvittionl Field lgeb sed Physics Newton's Lw of Univesl Gvittion Sufce Gvity Gvittionl Field in Spce Keple's Thid Lw
More informationMAT 403 NOTES 4. f + f =
MAT 403 NOTES 4 1. Fundmentl Theorem o Clulus We will proo more generl version o the FTC thn the textook. But just like the textook, we strt with the ollowing proposition. Let R[, ] e the set o Riemnn
More informationCHAPTER 2 ELECTROSTATIC POTENTIAL
1 CHAPTER ELECTROSTATIC POTENTIAL 1 Intoduction Imgine tht some egion of spce, such s the oom you e sitting in, is pemeted by n electic field (Pehps thee e ll sots of electiclly chged bodies outside the
More informationr r E x w, y w, z w, (1) Where c is the speed of light in vacuum.
ISSN: 77-754 ISO 900:008 Cetified Intentionl Jonl of Engineeing nd Innovtive Tehnology (IJEIT) olme, Isse 0, Apil 04 The Replement of the Potentils s Conseene of the Limittions Set by the Lw of the Self
More informationWork, Potential Energy, Conservation of Energy. the electric forces are conservative: ur r
Wok, Potentil Enegy, Consevtion of Enegy the electic foces e consevtive: u Fd = Wok, Potentil Enegy, Consevtion of Enegy b b W = u b b Fdl = F()[ d + $ $ dl ] = F() d u Fdl = the electic foces e consevtive
More informationLecture 11: Potential Gradient and Capacitor Review:
Lectue 11: Potentil Gdient nd Cpcito Review: Two wys to find t ny point in spce: Sum o Integte ove chges: q 1 1 q 2 2 3 P i 1 q i i dq q 3 P 1 dq xmple of integting ove distiution: line of chge ing of
More informationAn Analysis of the LRE-Algorithm using Sojourn Times
An Anlysis of the LRE-Algoithm using Sooun Times Nobet Th. Mülle Abteilung Infomtik Univesität Tie D-5486 Tie, Gemny E-mil: muelle@uni-tie.de Tel: ++49-65-0-845 Fx: ++49-65-0-3805 KEYWORDS Disete event
More informationExample 2: ( ) 2. $ s ' 9.11" 10 *31 kg ( )( 1" 10 *10 m) ( e)
Emple 1: Two point chge e locted on the i, q 1 = e t = 0 nd q 2 = e t =.. Find the wok tht mut be done b n etenl foce to bing thid point chge q 3 = e fom infinit to = 2. b. Find the totl potentil eneg
More informationMolecular Energy Changes During a Reaction
Reation Kinetis Moleula Enegy Changes Duing a Reation Chemial Enegy of Speies E xn E* +BP E* P+B Moleules above this enegy level (defined somewhat abitaily) ae alled ativated omplexes Poduts Reatants Pogession
More informationElectromagnetism Notes, NYU Spring 2018
Eletromgnetism Notes, NYU Spring 208 April 2, 208 Ation formultion of EM. Free field desription Let us first onsider the free EM field, i.e. in the bsene of ny hrges or urrents. To tret this s mehnil system
More informationFlux. Area Vector. Flux of Electric Field. Gauss s Law
Gauss s Law Flux Flux in Physics is used to two distinct ways. The fist meaning is the ate of flow, such as the amount of wate flowing in a ive, i.e. volume pe unit aea pe unit time. O, fo light, it is
More informationEELE 3331 Electromagnetic I Chapter 4. Electrostatic fields. Islamic University of Gaza Electrical Engineering Department Dr.
EELE 3331 Electomagnetic I Chapte 4 Electostatic fields Islamic Univesity of Gaza Electical Engineeing Depatment D. Talal Skaik 212 1 Electic Potential The Gavitational Analogy Moving an object upwad against
More information8 THREE PHASE A.C. CIRCUITS
8 THREE PHSE.. IRUITS The signls in hpter 7 were sinusoidl lternting voltges nd urrents of the so-lled single se type. n emf of suh type n e esily generted y rotting single loop of ondutor (or single winding),
More information9.4 The response of equilibrium to temperature (continued)
9.4 The esponse of equilibium to tempetue (continued) In the lst lectue, we studied how the chemicl equilibium esponds to the vition of pessue nd tempetue. At the end, we deived the vn t off eqution: d
More informationContinuous Charge Distributions
Continuous Chge Distibutions Review Wht if we hve distibution of chge? ˆ Q chge of distibution. Q dq element of chge. d contibution to due to dq. Cn wite dq = ρ dv; ρ is the chge density. = 1 4πε 0 qi
More informationThe geometric construction of Ewald sphere and Bragg condition:
The geometic constuction of Ewald sphee and Bagg condition: The constuction of Ewald sphee must be done such that the Bagg condition is satisfied. This can be done as follows: i) Daw a wave vecto k in
More information(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information
m m m00 kg dult, m0 kg bby. he seesw stts fom est. Which diection will it ottes? ( Counte-Clockwise (b Clockwise ( (c o ottion ti (d ot enough infomtion Effect of Constnt et oque.3 A constnt non-zeo toque
More informationChapter 25 Electric Potential
Chpte 5 lectic Potentil consevtive foces -> potentil enegy - Wht is consevtive foce? lectic potentil = U / : the potentil enegy U pe unit chge is function of the position in spce Gol:. estblish the eltionship
More informationCourse Updates. Reminders: 1) Assignment #8 available. 2) Chapter 28 this week.
Couse Updtes http://www.phys.hwii.edu/~vne/phys7-sp1/physics7.html Remindes: 1) Assignment #8 vilble ) Chpte 8 this week Lectue 3 iot-svt s Lw (Continued) θ d θ P R R θ R d θ d Mgnetic Fields fom long
More informationElectric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin
1 1 Electic Field + + q F Q R oigin E 0 0 F E ˆ E 4 4 R q Q R Q - - Electic field intensity depends on the medium! Electic Flux Density We intoduce new vecto field D independent of medium. D E So, electic
More informationPhysics 2B Chapter 22 Notes - Magnetic Field Spring 2018
Physics B Chapte Notes - Magnetic Field Sping 018 Magnetic Field fom a Long Staight Cuent-Caying Wie In Chapte 11 we looked at Isaac Newton s Law of Gavitation, which established that a gavitational field
More informationPhysics 505 Fall 2005 Midterm Solutions. This midterm is a two hour open book, open notes exam. Do all three problems.
Physics 55 Fll 5 Midtem Solutions This midtem is two hou open ook, open notes exm. Do ll thee polems. [35 pts] 1. A ectngul ox hs sides of lengths, nd c z x c [1] ) Fo the Diichlet polem in the inteio
More information10 Statistical Distributions Solutions
Communictions Engineeing MSc - Peliminy Reding 1 Sttisticl Distiutions Solutions 1) Pove tht the vince of unifom distiution with minimum vlue nd mximum vlue ( is ) 1. The vince is the men of the sques
More information20 b The prime numbers are 2,3,5,7,11,13,17,19.
Topi : Probbility Short nswer tehnology- free The following my be of use in this test:! 0 0 Two rows of Psl s tringle re: ontiner holds irulr piees eh of the sme size. Written on eh is different number,
More informationRed Shift and Blue Shift: A realistic approach
Red Shift and Blue Shift: A ealisti appoah Benhad Rothenstein Politehnia Uniesity of Timisoaa, Physis Dept., Timisoaa, Romania E-mail: benhad_othenstein@yahoo.om Coina Nafonita Politehnia Uniesity of Timisoaa,
More informationOn the Eötvös effect
On the Eötvös effect Mugu B. Răuţ The im of this ppe is to popose new theoy bout the Eötvös effect. We develop mthemticl model which loud us bette undestnding of this effect. Fom the eqution of motion
More informationNon-equilibrium Green function method: theory and application in simulation of nanometer electronic devices
Advnes in Ntul Sienes: Nnosiene nd Nnotehnology REVIEW OPEN ACCESS Non-equilibium een funtion method: theoy nd pplition in simultion of nnomete eletoni devies To ite this tile: Vn-Nm Do 4 Adv. Nt. Si:
More informationMathematical formulation of the F 0 motor model
negy Tnsduction in TP Synthse: Supplement Mthemticl fomultion of the F 0 moto model. Mkov chin model fo the evolution of the oto stte The fou possible potontion sttes of the two oto sp61 sites t the otostto
More informationSPA7010U/SPA7010P: THE GALAXY. Solutions for Coursework 1. Questions distributed on: 25 January 2018.
SPA7U/SPA7P: THE GALAXY Solutions fo Cousewok Questions distibuted on: 25 Jnuy 28. Solution. Assessed question] We e told tht this is fint glxy, so essentilly we hve to ty to clssify it bsed on its spectl
More information1 This question is about mean bond enthalpies and their use in the calculation of enthalpy changes.
1 This question is out men ond enthlpies nd their use in the lultion of enthlpy hnges. Define men ond enthlpy s pplied to hlorine. Explin why the enthlpy of tomistion of hlorine is extly hlf the men ond
More information1 Fundamental Solutions to the Wave Equation
1 Fundamental Solutions to the Wave Equation Physial insight in the sound geneation mehanism an be gained by onsideing simple analytial solutions to the wave equation One example is to onside aousti adiation
More information1 This diagram represents the energy change that occurs when a d electron in a transition metal ion is excited by visible light.
1 This igrm represents the energy hnge tht ours when eletron in trnsition metl ion is exite y visile light. Give the eqution tht reltes the energy hnge ΔE to the Plnk onstnt, h, n the frequeny, v, of the
More informationPart 4. Integration (with Proofs)
Prt 4. Integrtion (with Proofs) 4.1 Definition Definition A prtition P of [, b] is finite set of points {x 0, x 1,..., x n } with = x 0 < x 1
More information2 E. on each of these two surfaces. r r r r. Q E E ε. 2 2 Qencl encl right left 0
Ch : 4, 9,, 9,,, 4, 9,, 4, 8 4 (a) Fom the diagam in the textbook, we see that the flux outwad though the hemispheical suface is the same as the flux inwad though the cicula suface base of the hemisphee
More informationPolymer A should have the medium T g. It has a larger sidechain than polymer B, and may also have hydrogen bonding, due the -COOH group.
MATERIALS 0 INTRODUTION TO STRUTURE AND PROPERTIES WINTER 202 Poblem Set 2 Due: Tuesdy, Jnuy 3, :00 AM. Glss Tnsition Tempetue ) The glss tnsition tempetue, T g, is stongly govened by the bility of the
More informationMultiple-input multiple-output (MIMO) communication systems. Advanced Modulation and Coding : MIMO Communication Systems 1
Multiple-input multiple-output (MIMO) communiction systems Advnced Modultion nd Coding : MIMO Communiction Systems System model # # #n #m eceive tnsmitte infobits infobits #N #N N tnsmit ntenns N (k) M
More informationData Structures. Element Uniqueness Problem. Hash Tables. Example. Hash Tables. Dana Shapira. 19 x 1. ) h(x 4. ) h(x 2. ) h(x 3. h(x 1. x 4. x 2.
Element Uniqueness Poblem Dt Stuctues Let x,..., xn < m Detemine whethe thee exist i j such tht x i =x j Sot Algoithm Bucket Sot Dn Shpi Hsh Tbles fo (i=;i
More information(conservation of momentum)
Dynamis of Binay Collisions Assumptions fo elasti ollisions: a) Eletially neutal moleules fo whih the foe between moleules depends only on the distane between thei entes. b) No intehange between tanslational
More informationUnit II Crystal Structure and X-ray diffraction Engineering Physics
Unit II Cyst Stutue nd X-y difftion Engineeing Pysis Intodution It is we nown ft tt mtte onsists of toms nd moeues. Te popeties of mtte depend on te ngement of toms inside mtte wi depends on te emi onding
More information6. Gravitation. 6.1 Newton's law of Gravitation
Gvittion / 1 6.1 Newton's lw of Gvittion 6. Gvittion Newton's lw of gvittion sttes tht evey body in this univese ttcts evey othe body with foce, which is diectly popotionl to the poduct of thei msses nd
More information