Molecular Orbitals in Inorganic Chemistry

Size: px
Start display at page:

Download "Molecular Orbitals in Inorganic Chemistry"

Transcription

1 Outlin olcular Orbitals in Inorganic Chmistry Dr. P. Hunt Rm 167 (Chmistry) octahdral complxs forming th O diagram for Oh colour, slction ruls Δoct, spctrochmical sris forming th O diagram for C4v 1 Octahdral Complxs vry larg and important class of transition mtal complxs T complxs act as catalysts to control and improv catalysts w nd to undrstand th undrlying lctronic structur magntic proprtis, colour! Rmovd du Imag from p16 of tal igand Bonding by R. Jans and E. oor RSC, Cambridg, work through for an octahdral molcul 2 O chcklist Stps to construct a O diagram dtrmin th molcular shap and idntify th point group of th molcul dfin th axial systm and find all of th symmtry oprations on th molcul idntify th chmical fragmnts, and put thm along th bottom of th diagram dtrmin th nrgy lvls and symmtry labls of th fragmnt orbitals (us H1s as a rfrnc) combin fragmnt orbitals of th sam symmtry, stimat th splitting nrgy and draw in th O nrgy lvls and Os (in pncil!) dtrmin th numbr of lctrons in ach fragmnt and hnc th cntral O rgion, add thm to th diagram idntify if any O mixing occurs, dtrmin th mixd orbitals and rdraw th O diagram with shiftd nrgy lvls and th mixd Os annotat your diagram us th O diagram to undrstand th structur, bonding and chmistry of th molcul 3 4 6_Slids_wb.ky - 1 Dcmbr 2017

2 Stps 1-2: Point Group dtrmin molcular shap: octahdral dtrmin th point group of th molcul find Oh in your charactr tabls dfin th axial systm find all of th symmtry oprations covrd last lctur Fig. 3 C 3 σ d C 4 Fig. 1 E 8C 3 6C 3σ 2 6C 4 3 i 6S 4 8S 6 h 6σ d A 1g A 2g Eg T 1g T 2g A 1u A 2u Eu T 1u T 2u y z x (x 2 +y 2 +z 2 ) (2z 2 -x 2 -y 2, x 2 -y 2 ) (xy, xz, yz) (T x, T y,t x) Fig. 2 Stps 3-4: Fragmnt Orbitals dtrmin th fragmnts cntral mtal and th symmtry adaptd fragmnt orbitals for 6 dtrmin th nrgy lvls and symmtry labls of th fragmnts covrd last lctur => tricks to hlp rmmbr Fig. 4 ligands C 4,C 4 σ v = σ h, C 4 mtal,c 4,C 4, C 4, C 4 Fig.5 Fig St up O Diagram St up O Diagram draw th fragmnts and chmical structur us plac holdrs! add th fragmnt orbitals mtal is lctropositiv daos ar highr in nrgy ligand orbitals ar bonding FOs li dpr in nrgy Fig 7 Pag 3 colour th plac holdrs in on your nots! 7 8 6_Slids_wb.ky - 1 Dcmbr 2017

3 Enrgy Diagram Combin Orbitals combin orbitals of th sam symmtry stimat th xtnt of nrgy splitting g ar s-σ =>strong splitting nrgy g ar far apart in nrgy =>rducs splitting stimat th xtnt of nrgy splitting t1u intraction is p-σ => mdium t1u nrgy diffrnc is vry larg => dcrass splitting siz mattrs! siz mattrs! antibonding =>larg bonding =>larg Fig.8 Fig Combin Orbitals Combin Orbitals stimat th xtnt of nrgy splitting g intraction is d-σ => small g clos in nrgy => incrass splitting stimat th xtnt of nrgy splitting mtal rmain non-bonding as thr ar no ligand orbitals of this symmtry siz mattrs! Fig _Slids_wb.ky - 1 Dcmbr 2017

4 Stps: 6-8 lctronic configuration six 2 donor ligands =12 numbr d lctrons dpnds on th mtal and oxidation stat I v usd six hr Enrgy Diagram Th full O diagram! dtrmin if thr is mixing no mixing occurs us O diagram chcklist! Fig.9 y z x Stp 9: Analysis Stp 9: Analysis thr lowst nrgy sts of orbitals ar ligand basd thr lowst nrgy sts of orbitals ar ligand basd highr nrgy Os ar mtal basd tal basd Os Fig.8 for xampl th Os igand basd Os Fig.8 for xampl th Os _Slids_wb.ky - 1 Dcmbr 2017

5 Not! lav off som of th lins for th mtal dominatd (s & p FOs) and th ligand dominatd (low nrgy) FOs kp all th lins for th daos! lav off som of th lins! paramtr Δoct nrgy span of th dao dominatd Os σ-ligands is non-bonding g is antibonding! Δoct dpnds on strngth of intraction: Δε nrgy btwn and FOs Sij strngth/dnsity of ovrlap of FOs Hij which is hard to stimat! total charg on complx oxidation stat of th (charg on ) 17 paramtr 18 Colour and d-d Transitions highr in nrgy th ligand FOs th bttr th intraction larg small g colour molcul absorbs light lctron is xcitd d-d transition right wavlngth for colour [Ti(OH2)6] 3+ absorbs in yllow/ grn and appars rd/violt Rmovd du rmindr Fig.10 => largr intraction => highr orbital => a largr Δoct Rmovd du Fig.11 Coordination Chmistry imi Hi ( ) Fig _Slids_wb.ky - 1 Dcmbr 2017

6 Colour and d-d Transitions Colour and d-d Transitions Slction Ruls d-d transitions ar forbiddn aport slction rul : only ±1 for angular quantum numbr s->p or p->d NOT d->d anothr form rul : must hav a chang of parity u->g or g->u NOT g->g (d->d transition involvs ->g) spin slction rul : cannot chang spin stat d->d transitions rmindr rul is brokn! wak transitions du to vibronic coupling vibrations and lctronic structur coupl low intnsity broad du to vibrations (mov nrgy lvls slightly) dx 2 -y 2 basd O Fig.12 Stats or configurations dz 2 basd O dxy dyz dxz start d 2 ground stat 21 Colour and d-d Transitions 22 Colour and d-d Transitions Stats or configurations ach stat has slightly diffrnt nrgy diffrnt lctron distribution diffrnt Coulomb intractions diffrnt lctron corrlation dx 2 -y 2 basd O dz 2 basd O multipl stats = multipl paks in spctra Trm symbols: dfin symmtry, multiplicity, total angular momntum of th stat nxt trm! dxy dyz dxz any initial and final stats! important for lcturs nxt yar! Rmovd du Fig.12 Absorption spctrum of [n(h2o)6] 2+, downloadd from Tanab Sugano_diagram, Dc [n(h 2O) 6] 2+ Fig _Slids_wb.ky - 1 Dcmbr 2017

7 Spctrochmical Sris Spctrochmical Sris uv-vis xprimntally masurs Δoct ordr ligands according to siz Δoct rmindr strong fild ligand larg Δoct for xampl CO wak fild ligand small Δoct for xampl Clwak fild Spctrochmical sris I- <Br- <Cl- <F- < OH- <O 2- <H 2O < py < NR 3 <NH 3 < n < NO 2 - < CH 3 - < C 6H 5 - < CN- < CO < NO + strong fild 25 xampl! rplac Ni6 ligands from strongr fild to wakr fild chang Δoct and th colour [Ni(H2O)6] 2+ has low nrgy, small Δoct absorbs in th rd and is grn Fig.14 Colour of various Ni(II) complxs in aquous solution. Rmovd du [Ni(NH 3) 6] 2+, [Ni(n) 3] 2+, [NiCl 4] 2-, [Ni(H 2O) 6] Spctrochmical sris I- <Br- <Cl- <F- <OH- <O 2 - <H 2O <NH 3 < n < NO 2 - <CH 3 - <C 6H 5 - <CN- <CO Rmovd du Imag from Inorganic_Chmistry/Crystal_Fild_Thory/ Colors_of_Coordination_Complxs, downloadd 1 Dc 2014 Imag from Nickl(II)_chlorid, Hch, downloadd 1 Dc 2014 Fig.15 T-Colour! Info-graphics from Rmovd du Rmovd du Othr Factors not only th ligands ffct th siz of Δoct ovrall charg on th th complx oxidation stat mtal charg on th mtal / ligands dnsity of ovrlapping orbitals radius of mtal (row) stric congstion ligands rmindr high charg on draws ligands in incrass ovrlap incrass intraction incrass Δoct Rmovd du Rmovd du Rmovd du larg ligand cannot approach mtal poor ovrlap rducd intraction dcrass Δoct Fig.16 Coordination Chmistry imi Hi ( ) _Slids_wb.ky - 1 Dcmbr 2017

8 Rduc th Symmtry rplac 1 ligand with a diffrnt σ-ligand loss of symmtry Oh -> C4v C 4 σ ' σ σ v σ σ σ σ σ d σ σ σ σ dtrmin nw symmtry labls for mtal AOs dtrmin th nw symmtry labls for th ligand FOs VERY Fig.19 dz 2, dx 2 -y 2 dxy, dyz, dxz dgnrat lvls rmain dgnrat, I v split thm for as of intrprtation σ σ procss simpl: Os rmain th sam just nd to work out rducd symmtry labls! watch for dgnracy braking Fig.18 us short-cuts and your charactr tabl for Fig dtrmin nw symmtry labls for mtal AOs dtrmin th nw symmtry labls for th ligand FOs VERY dz 2, dx 2 -y 2 dxy, dyz, dxz rad off charactr tabl for Fig.19 b1 b2 dtrmin nw symmtry labls for mtal AOs dtrmin th nw symmtry labls for th ligand FOs VERY dz 2, dx 2 -y 2 dxy, dyz, dxz Fig.19 b1 b2 Fig.20 Fig.20 totally symmtric _Slids_wb.ky - 1 Dcmbr 2017

9 dtrmin nw symmtry labls for mtal AOs dtrmin th nw symmtry labls for th ligand FOs VERY dz 2, dx 2 -y 2 dxy, dyz, dxz Fig.19 b1 b2 dtrmin nw symmtry labls for mtal AOs dtrmin th nw symmtry labls for th ligand FOs VERY dz 2, dx 2 -y 2 dxy, dyz, dxz Fig.19 b1 b2 b1 lik dz 2 and dx 2 -y 2 lik paos -> T x,t y,t z Fig.20 Fig now combin th T daos and th ligand FO to form th nrgy lvl diagram for a C4v T complx now combin th T daos and th ligand FO to form th nrgy lvl diagram for a C4v T complx hint 1 add th fragmnt orbital nrgy lvls ' σ ' σ σ σ σ σ σ σ σ σ Fig.21 σ σ _Slids_wb.ky - 1 Dcmbr 2017

10 Diagram now combin th T daos and th ligand FO to form th nrgy lvl diagram for a C4v T complx hint 1 add th fragmnt orbital nrgy lvls dgnrat sprad out to illustrat diffrnt symmtris compltd! hint 2 combin lvls of th sam symmtry ' σ ' σ ' σ ' σ σ σ σ σ σ σ σ σ σ σ σ σ σ σ σ σ Fig.21 σ σ Fig.22 σ σ Diagram Diagram compltd! compltd! was dgnracy is brokn was dgnracy is rducd ' σ ' σ ' σ ' σ σ σ σ σ σ σ σ σ σ σ σ σ σ σ σ σ Fig.22 σ σ Fig.22 σ σ _Slids_wb.ky - 1 Dcmbr 2017

11 Diagram T Diagram compltd! ligand Os T daobasd Os primary ffct of th rduction in symmtry => split th g nrgy lvls ordring of and b1 will dpnd on th ligands Δoct is splitting of dao manifold (group of orbitals!) bonding ligand-basd Os dx 2 -y 2 and dz 2 antibonding mtal-basd Os non-bonding mtal-basd Os dxy, dxz and dyz ' σ ' σ Fig.22 σ σ σ σ σ σ σ σ σ σ Fig Ky Points b abl to draw nrgy lvl diagrams for octahdral T complxs with σ b abl to draw and dscrib th important Os b abl to discuss ky faturs of th diagrams, spcially faturs rlating to th charactr of th Os b abl to dfin th octahdral splitting paramtr and b abl to discuss ky proprtis that impact on or ffct Δoct b abl to draw th nrgy diagram for a lowr symmtry T complx with σ-bonding ligands, including squar planar S my wb-sit 42 Finally nots AND slids link to panopto whn it bcoms availabl optional background support for bginnrs optional matrial to tak you a littl furthr links to intrsting popl and wb-sits links to rlvant rsarch paprs on Os modl answrs!! _Slids_wb.ky - 1 Dcmbr 2017

Molecular Orbital Diagrams for TM Complexes with

Molecular Orbital Diagrams for TM Complexes with olcular Orbital Diagrams for T Complxs with p-intracting igands CO and othr iso-lctronic p-accptor s CO s ar vry usful for charactrising th amount of back donation in othr s o th vibrational IR spctrum

More information

Chapter 8: Electron Configurations and Periodicity

Chapter 8: Electron Configurations and Periodicity Elctron Spin & th Pauli Exclusion Principl Chaptr 8: Elctron Configurations and Priodicity 3 quantum numbrs (n, l, ml) dfin th nrgy, siz, shap, and spatial orintation of ach atomic orbital. To xplain how

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

Title: Vibrational structure of electronic transition

Title: Vibrational structure of electronic transition Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum

More information

Classical Magnetic Dipole

Classical Magnetic Dipole Lctur 18 1 Classical Magntic Dipol In gnral, a particl of mass m and charg q (not ncssarily a point charg), w hav q g L m whr g is calld th gyromagntic ratio, which accounts for th ffcts of non-point charg

More information

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals. Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby

More information

Hydrogen Atom and One Electron Ions

Hydrogen Atom and One Electron Ions Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

Coupled Pendulums. Two normal modes.

Coupled Pendulums. Two normal modes. Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron

More information

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic

More information

September 23, Honors Chem Atomic structure.notebook. Atomic Structure

September 23, Honors Chem Atomic structure.notebook. Atomic Structure Atomic Structur Topics covrd Atomic structur Subatomic particls Atomic numbr Mass numbr Charg Cations Anions Isotops Avrag atomic mass Practic qustions atomic structur Sp 27 8:16 PM 1 Powr Standards/ Larning

More information

Determination of Vibrational and Electronic Parameters From an Electronic Spectrum of I 2 and a Birge-Sponer Plot

Determination of Vibrational and Electronic Parameters From an Electronic Spectrum of I 2 and a Birge-Sponer Plot 5 J. Phys. Chm G Dtrmination of Vibrational and Elctronic Paramtrs From an Elctronic Spctrum of I 2 and a Birg-Sponr Plot 1 15 2 25 3 35 4 45 Dpartmnt of Chmistry, Gustavus Adolphus Collg. 8 Wst Collg

More information

The pn junction: 2 Current vs Voltage (IV) characteristics

The pn junction: 2 Current vs Voltage (IV) characteristics Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n

More information

2. Laser physics - basics

2. Laser physics - basics . Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"

More information

Give the letter that represents an atom (6) (b) Atoms of A and D combine to form a compound containing covalent bonds.

Give the letter that represents an atom (6) (b) Atoms of A and D combine to form a compound containing covalent bonds. 1 Th diagram shows th lctronic configurations of six diffrnt atoms. A B C D E F (a) You may us th Priodic Tabl on pag 2 to hlp you answr this qustion. Answr ach part by writing on of th lttrs A, B, C,

More information

6. The Interaction of Light and Matter

6. The Interaction of Light and Matter 6. Th Intraction of Light and Mattr - Th intraction of light and mattr is what maks lif intrsting. - Light causs mattr to vibrat. Mattr in turn mits light, which intrfrs with th original light. - Excitd

More information

Exam 2 Thursday (7:30-9pm) It will cover material through HW 7, but no material that was on the 1 st exam.

Exam 2 Thursday (7:30-9pm) It will cover material through HW 7, but no material that was on the 1 st exam. Exam 2 Thursday (7:30-9pm) It will covr matrial through HW 7, but no matrial that was on th 1 st xam. What happns if w bash atoms with lctrons? In atomic discharg lamps, lots of lctrons ar givn kintic

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration

More information

Lecture 28 Title: Diatomic Molecule : Vibrational and Rotational spectra

Lecture 28 Title: Diatomic Molecule : Vibrational and Rotational spectra Lctur 8 Titl: Diatomic Molcul : Vibrational and otational spctra Pag- In this lctur w will undrstand th molcular vibrational and rotational spctra of diatomic molcul W will start with th Hamiltonian for

More information

Why is a E&M nature of light not sufficient to explain experiments?

Why is a E&M nature of light not sufficient to explain experiments? 1 Th wird world of photons Why is a E&M natur of light not sufficint to xplain xprimnts? Do photons xist? Som quantum proprtis of photons 2 Black body radiation Stfan s law: Enrgy/ ara/ tim = Win s displacmnt

More information

ph People Grade Level: basic Duration: minutes Setting: classroom or field site

ph People Grade Level: basic Duration: minutes Setting: classroom or field site ph Popl Adaptd from: Whr Ar th Frogs? in Projct WET: Curriculum & Activity Guid. Bozman: Th Watrcours and th Council for Environmntal Education, 1995. ph Grad Lvl: basic Duration: 10 15 minuts Stting:

More information

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the Lctur 22-1 Byond Bohr Modl Unfortunatly, th classical visualization of th orbiting lctron turns out to b wrong vn though it still givs us a simpl way to think of th atom. Quantum Mchanics is ndd to truly

More information

Figure 1 M-O interaction modes. triple bond p x p y. resonance structures. double bond and lone pair. M d 0 -O 2- p z. σ-donor interaction

Figure 1 M-O interaction modes. triple bond p x p y. resonance structures. double bond and lone pair. M d 0 -O 2- p z. σ-donor interaction Slf-Stud Problms / Eam Prparation In what situations is th valu of Δ oct difficult to idntif? o whn thr ar multipl lctronic transitions which giv ris to multipl paks in th uv-vis spctrum, for ampl [n(h

More information

Contemporary, atomic, nuclear, and particle physics

Contemporary, atomic, nuclear, and particle physics Contmporary, atomic, nuclar, and particl physics 1 Blackbody radiation as a thrmal quilibrium condition (in vacuum this is th only hat loss) Exampl-1 black plan surfac at a constant high tmpratur T h is

More information

Electrochemistry L E O

Electrochemistry L E O Rmmbr from CHM151 A rdox raction in on in which lctrons ar transfrrd lctrochmistry L O Rduction os lctrons xidation G R ain lctrons duction W can dtrmin which lmnt is oxidizd or rducd by assigning oxidation

More information

Statistical Thermodynamics: Sublimation of Solid Iodine

Statistical Thermodynamics: Sublimation of Solid Iodine c:374-7-ivap-statmch.docx mar7 Statistical Thrmodynamics: Sublimation of Solid Iodin Chm 374 For March 3, 7 Prof. Patrik Callis Purpos:. To rviw basic fundamntals idas of Statistical Mchanics as applid

More information

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian Drivation of Elctron-Elctron Intraction Trms in th Multi-Elctron Hamiltonian Erica Smith Octobr 1, 010 1 Introduction Th Hamiltonian for a multi-lctron atom with n lctrons is drivd by Itoh (1965) by accounting

More information

PH300 Modern Physics SP11 Final Essay. Up Next: Periodic Table Molecular Bonding

PH300 Modern Physics SP11 Final Essay. Up Next: Periodic Table Molecular Bonding PH Modrn Physics SP11 Final Essay Thr will b an ssay portion on th xam, but you don t nd to answr thos qustions if you submit a final ssay by th day of th final: Sat. 5/7 It dosnʼt mattr how smart you

More information

Brief Introduction to Statistical Mechanics

Brief Introduction to Statistical Mechanics Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.

More information

A Propagating Wave Packet Group Velocity Dispersion

A Propagating Wave Packet Group Velocity Dispersion Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to

More information

Phys 402: Nonlinear Spectroscopy: SHG and Raman Scattering

Phys 402: Nonlinear Spectroscopy: SHG and Raman Scattering Rquirmnts: Polariation of Elctromagntic Wavs Phys : Nonlinar Spctroscopy: SHG and Scattring Gnral considration of polariation How Polarirs work Rprsntation of Polariation: Jons Formalism Polariation of

More information

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding... Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg

More information

5.80 Small-Molecule Spectroscopy and Dynamics

5.80 Small-Molecule Spectroscopy and Dynamics MIT OpnCoursWar http://ocw.mit.du 5.80 Small-Molcul Spctroscopy and Dynamics Fall 008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. Lctur # 3 Supplmnt Contnts

More information

On the Hamiltonian of a Multi-Electron Atom

On the Hamiltonian of a Multi-Electron Atom On th Hamiltonian of a Multi-Elctron Atom Austn Gronr Drxl Univrsity Philadlphia, PA Octobr 29, 2010 1 Introduction In this papr, w will xhibit th procss of achiving th Hamiltonian for an lctron gas. Making

More information

High Energy Physics. Lecture 5 The Passage of Particles through Matter

High Energy Physics. Lecture 5 The Passage of Particles through Matter High Enrgy Physics Lctur 5 Th Passag of Particls through Mattr 1 Introduction In prvious lcturs w hav sn xampls of tracks lft by chargd particls in passing through mattr. Such tracks provid som of th most

More information

Davisson Germer experiment

Davisson Germer experiment Announcmnts: Davisson Grmr xprimnt Homwork st 5 is today. Homwork st 6 will b postd latr today. Mad a good guss about th Nobl Priz for 2013 Clinton Davisson and Lstr Grmr. Davisson won Nobl Priz in 1937.

More information

PRINCIPLES OF PLASMA PROCESSING Course Notes: Prof. J. P. Chang Part B3: ATOMIC COLLISIONS AND SPECTRA

PRINCIPLES OF PLASMA PROCESSING Course Notes: Prof. J. P. Chang Part B3: ATOMIC COLLISIONS AND SPECTRA Atomic Collisions and Spctra 125 PRINCIPLES OF PLASMA PROCESSING Cours Nots: Prof. J. P. Chang Part B3: ATOMIC COLLISIONS AND SPECTRA I. ATOMIC ENERGY LEVELS Atoms and molculs mit lctromagntic radiation

More information

Constants and Conversions:

Constants and Conversions: EXAM INFORMATION Radial Distribution Function: P 2 ( r) RDF( r) Br R( r ) 2, B is th normalization constant. Ordr of Orbital Enrgis: Homonuclar Diatomic Molculs * * * * g1s u1s g 2s u 2s u 2 p g 2 p g

More information

CE 530 Molecular Simulation

CE 530 Molecular Simulation CE 53 Molcular Simulation Lctur 8 Fr-nrgy calculations David A. Kofk Dpartmnt of Chmical Enginring SUNY Buffalo kofk@ng.buffalo.du 2 Fr-Enrgy Calculations Uss of fr nrgy Phas quilibria Raction quilibria

More information

Davisson Germer experiment Announcements:

Davisson Germer experiment Announcements: Davisson Grmr xprimnt Announcmnts: Homwork st 7 is du Wdnsday. Problm solving sssions M3-5, T3-5. Th 2 nd midtrm will b April 7 in MUEN E0046 at 7:30pm. BFFs: Davisson and Grmr. Today w will go ovr th

More information

REGISTER!!! The Farmer and the Seeds (a parable of scientific reasoning) Class Updates. The Farmer and the Seeds. The Farmer and the Seeds

REGISTER!!! The Farmer and the Seeds (a parable of scientific reasoning) Class Updates. The Farmer and the Seeds. The Farmer and the Seeds How dos light intract with mattr? And what dos (this say about) mattr? REGISTER!!! If Schrödingr s Cat walks into a forst, and no on is around to obsrv it, is h rally in th forst? sourc unknown Phys 1010

More information

Brief Notes on the Fermi-Dirac and Bose-Einstein Distributions, Bose-Einstein Condensates and Degenerate Fermi Gases Last Update: 28 th December 2008

Brief Notes on the Fermi-Dirac and Bose-Einstein Distributions, Bose-Einstein Condensates and Degenerate Fermi Gases Last Update: 28 th December 2008 Brif ots on th Frmi-Dirac and Bos-Einstin Distributions, Bos-Einstin Condnsats and Dgnrat Frmi Gass Last Updat: 8 th Dcmbr 8 (A)Basics of Statistical Thrmodynamics Th Gibbs Factor A systm is assumd to

More information

de/dx Effectively all charged particles except electrons

de/dx Effectively all charged particles except electrons de/dx Lt s nxt turn our attntion to how chargd particls los nrgy in mattr To start with w ll considr only havy chargd particls lik muons, pions, protons, alphas, havy ions, Effctivly all chargd particls

More information

How can I control light? (and rule the world?)

How can I control light? (and rule the world?) How can I control light? (and rul th world?) "You know, I hav on simpl rqust. And that is to hav sharks with frickin' lasr bams attachd to thir hads! - Dr. Evil Phys 230, Day 35 Qustions? Spctra (colors

More information

The following information relates to Questions 1 to 4:

The following information relates to Questions 1 to 4: Th following information rlats to Qustions 1 to 4: QUESTIN 1 Th lctrolyt usd in this ful cll is D watr carbonat ions hydrogn ions hydroxid ions QUESTIN 2 Th product formd in th ful cll is D hydrogn gas

More information

University of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination

University of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination Univrsity of Illinois at Chicago Dpartmnt of hysics hrmodynamics & tatistical Mchanics Qualifying Eamination January 9, 009 9.00 am 1:00 pm Full crdit can b achivd from compltly corrct answrs to 4 qustions.

More information

A central nucleus. Protons have a positive charge Electrons have a negative charge

A central nucleus. Protons have a positive charge Electrons have a negative charge Atomic Structur Lss than ninty yars ago scintists blivd that atoms wr tiny solid sphrs lik minut snookr balls. Sinc thn it has bn discovrd that atoms ar not compltly solid but hav innr and outr parts.

More information

5.62 Physical Chemistry II Spring 2008

5.62 Physical Chemistry II Spring 2008 MIT OpnCoursWar http://ocw.mit.du 5.62 Physical Chmistry II Spring 2008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. 5.62 Lctur #7: Translational Part of

More information

Lecture 2: Rotational and Vibrational Spectra

Lecture 2: Rotational and Vibrational Spectra Lctur : Rotational and Vibrational Spctra 1. Light-mattr intraction. Rigid-rotor modl for diatomic molcul 3. Non-rigid rotation 4. Vibration-rotation for diatomics H O 1. Light-mattr intraction Possibilitis

More information

Numerical Problem Set for Atomic and Molecular Spectroscopy. Yr 2 HT SRM

Numerical Problem Set for Atomic and Molecular Spectroscopy. Yr 2 HT SRM Numrical Problm St for Atomic and Molcular Spctroscopy Yr HT SRM Sction 1: Atomic Spctra 1. For ach of th atomic trm symbols 1 S, P, 3 P, 3 D, 4 D, writ down: a) Th associatd valus of th total spin and

More information

the electrons. Expanding the exponential and neglecting the constant term Ze 2 λ, we have

the electrons. Expanding the exponential and neglecting the constant term Ze 2 λ, we have LECTURE.8 Prof.R.Parthasarathy Atomic Structur - Elmntary Tratmnt Th ground stat of hydrogn atom has bn solvd xactly in th nonrlativistic tratmnt. Th ground stat of hlium atom has bn handld in variational

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th

More information

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17)

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17) MCB37: Physical Biology of th Cll Spring 207 Homwork 6: Ligand binding and th MWC modl of allostry (Du 3/23/7) Hrnan G. Garcia March 2, 207 Simpl rprssion In class, w drivd a mathmatical modl of how simpl

More information

The failure of the classical mechanics

The failure of the classical mechanics h failur of th classical mchanics W rviw som xprimntal vidncs showing that svral concpts of classical mchanics cannot b applid. - h blac-body radiation. - Atomic and molcular spctra. - h particl-li charactr

More information

CHAPTER 16 HW: CONJUGATED SYSTEMS

CHAPTER 16 HW: CONJUGATED SYSTEMS APTER 6 W: JUGATED SYSTEMS NAMING PLYENES. Giv th IUPA nam for ach compound, including cis/trans or E/Z dsignations whr ndd. ompound no E/Z trans or E 2 3 4 3 Nam trans-2-mthyl-2,4-hxadin 2-mthoxy-,3-cyclohptadin

More information

A=P=E M-A=N Alpha particle Beta Particle. Periodic table

A=P=E M-A=N Alpha particle Beta Particle. Periodic table Nam Pr. Atomic Structur/Nuclar Chmistry (Ch. 3 & 21) OTHS Acadmic Chmistry Objctivs: Undrstand th xprimntal dsign and conclusions usd in th dvlopmnt of modrn atomic thory, including Dalton's Postulats,

More information

Elements of Statistical Thermodynamics

Elements of Statistical Thermodynamics 24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,

More information

Schrodinger Equation in 3-d

Schrodinger Equation in 3-d Schrodingr Equation in 3-d ψ( xyz,, ) ψ( xyz,, ) ψ( xyz,, ) + + + Vxyz (,, ) ψ( xyz,, ) = Eψ( xyz,, ) m x y z p p p x y + + z m m m + V = E p m + V = E E + k V = E Infinit Wll in 3-d V = x > L, y > L,

More information

Principles of Humidity Dalton s law

Principles of Humidity Dalton s law Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid

More information

Modern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom

Modern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom Mdrn Physics Unit 5: Schrödingr s Equatin and th Hydrgn Atm Lctur 5.6: Enrgy Eignvalus f Schrödingr s Equatin fr th Hydrgn Atm Rn Rifnbrgr Prfssr f Physics Purdu Univrsity 1 Th allwd nrgis E cm frm th

More information

Assessment Schedule 2013 Chemistry: Demonstrate understanding of the properties of selected organic compounds (91165)

Assessment Schedule 2013 Chemistry: Demonstrate understanding of the properties of selected organic compounds (91165) NCEA Lvl 2 Chmistry (91165) 2013 pag 1 of 5 Assssmnt Schdul 2013 Chmistry: Dmonstrat undrstanding of th proprtis of slctd organic compounds (91165) Assssmnt Critria Achivmnt Achivmnt with Mrit Achivmnt

More information

Forces. Quantum ElectroDynamics. α = = We have now:

Forces. Quantum ElectroDynamics. α = = We have now: W hav now: Forcs Considrd th gnral proprtis of forcs mdiatd by xchang (Yukawa potntial); Examind consrvation laws which ar obyd by (som) forcs. W will nxt look at thr forcs in mor dtail: Elctromagntic

More information

Solid State Theory Physics 545 Band Theory III

Solid State Theory Physics 545 Band Theory III Solid Stat Thory Physics 545 Band Thory III ach atomic orbital lads to a band of allowd stats in th solid Band of allowd stats Gap: no allowd stats Band of allowd stats Gap: no allowd stats Band of allowd

More information

Sara Godoy del Olmo Calculation of contaminated soil volumes : Geostatistics applied to a hydrocarbons spill Lac Megantic Case

Sara Godoy del Olmo Calculation of contaminated soil volumes : Geostatistics applied to a hydrocarbons spill Lac Megantic Case wwwnvisol-canadaca Sara Godoy dl Olmo Calculation of contaminatd soil volums : Gostatistics applid to a hydrocarbons spill Lac Mgantic Cas Gostatistics: study of a PH contamination CONTEXT OF THE STUDY

More information

What makes laser light special? Lasers. Lasers. Laser history. Lasers are everywhere! Review of atom discharge lamps. So how do we make laser light?

What makes laser light special? Lasers. Lasers. Laser history. Lasers are everywhere! Review of atom discharge lamps. So how do we make laser light? Lasrs Lasrs What is diffrnt/spcial about lasr light. How dos a lasr work. - rviw atomic discharg lamps. - how light intracts with atoms - how ths idas ar usd to mak lasr. "You know, I hav on simpl rqust.

More information

K

K Alicyclic Chmistry. Lctur 3 Th ovrall strain in cycloalkns can b masurd by th magnitud of th complxation constants with Ag +. Th gratr th angl strain th mor it is rlivd in th π-complx which rducs th π-charactr

More information

Today. Wave-Matter Duality. Quantum Non-Locality. What is waving for matter waves?

Today. Wave-Matter Duality. Quantum Non-Locality. What is waving for matter waves? Today Wav-Mattr Duality HW 7 and Exam 2 du Thurs. 8pm 0 min rcap from last lctur on QM Finish QM odds and nds from ch.4 Th Standard Modl 4 forcs of Natur Fundamntal particls of Natur Fynman diagrams EM

More information

Atomic and Laser Spectroscopy

Atomic and Laser Spectroscopy L-E B, OL, MOV 83 Atomic and Lasr Spctroscopy Th aim of this xrcis is to giv an ovrviw of th fild of lasr spctroscopy and to show modrn spctroscopic mthods usd in atomic, molcular and chmical physics.

More information

Outline. Thanks to Ian Blockland and Randy Sobie for these slides Lifetimes of Decaying Particles Scattering Cross Sections Fermi s Golden Rule

Outline. Thanks to Ian Blockland and Randy Sobie for these slides Lifetimes of Decaying Particles Scattering Cross Sections Fermi s Golden Rule Outlin Thanks to Ian Blockland and andy obi for ths slids Liftims of Dcaying Particls cattring Cross ctions Frmi s Goldn ul Physics 424 Lctur 12 Pag 1 Obsrvabls want to rlat xprimntal masurmnts to thortical

More information

Optics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007

Optics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007 Optics and Non-Linar Optics I - 007 Non-linar Optics Tutorial Sht Novmbr 007 1. An altrnativ xponntial notion somtims usd in NLO is to writ Acos (") # 1 ( Ai" + A * $i" ). By using this notation and substituting

More information

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME 43 Introduction to Finit Elmnt Analysis Chaptr 3 Computr Implmntation of D FEM Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt

More information

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in Surfac plasmon rsonanc is snsitiv mchanism for obsrving slight changs nar th surfac of a dilctric-mtal intrfac. It is commonl usd toda for discovring th was in which protins intract with thir nvironmnt,

More information

Chapter 1 Late 1800 s Several failures of classical (Newtonian) physics discovered

Chapter 1 Late 1800 s Several failures of classical (Newtonian) physics discovered Chaptr 1 Lat 1800 s Svral failurs of classical (Nwtonian) physics discovrd 1905 195 Dvlopmnt of QM rsolvd discrpancis btwn xpt. and classical thory QM Essntial for undrstanding many phnomna in Chmistry,

More information

Molecular Orbital Theory (MOT)

Molecular Orbital Theory (MOT) Molecular Orbital Theory (MOT) In this section, There are another approach to the bonding in metal complexes: the use of molecular orbital theory (MOT). In contrast to crystal field theory, the molecular

More information

Physical Chemistry Spring 2018 TR 5:00-6:15 pm, 207 BrL Quiz #1

Physical Chemistry Spring 2018 TR 5:00-6:15 pm, 207 BrL Quiz #1 Physical Chmistry 444-0 Spring 08 TR 5:00-6:5 pm, 07 BrL Quiz # Nam KEY Problm (3 points). Ammonia gas is vry hygroscopic (asily racts with watr), so it is packagd for shipping in a small dry gas cylindr

More information

Utilizing exact and Monte Carlo methods to investigate properties of the Blume Capel Model applied to a nine site lattice.

Utilizing exact and Monte Carlo methods to investigate properties of the Blume Capel Model applied to a nine site lattice. Utilizing xat and Mont Carlo mthods to invstigat proprtis of th Blum Capl Modl applid to a nin sit latti Nik Franios Writing various xat and Mont Carlo omputr algorithms in C languag, I usd th Blum Capl

More information

Precise Masses of particles

Precise Masses of particles /1/15 Physics 1 April 1, 15 Ovrviw of topic Th constitunts and structur of nucli Radioactivity Half-lif and Radioactiv dating Nuclar Binding Enrgy Nuclar Fission Nuclar Fusion Practical Applications of

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 07 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat

More information

Higher order derivatives

Higher order derivatives Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of

More information

Alpha and beta decay equation practice

Alpha and beta decay equation practice Alpha and bta dcay quation practic Introduction Alpha and bta particls may b rprsntd in quations in svral diffrnt ways. Diffrnt xam boards hav thir own prfrnc. For xampl: Alpha Bta α β alpha bta Dspit

More information

MA 262, Spring 2018, Final exam Version 01 (Green)

MA 262, Spring 2018, Final exam Version 01 (Green) MA 262, Spring 218, Final xam Vrsion 1 (Grn) INSTRUCTIONS 1. Switch off your phon upon ntring th xam room. 2. Do not opn th xam booklt until you ar instructd to do so. 3. Bfor you opn th booklt, fill in

More information

Collisions between electrons and ions

Collisions between electrons and ions DRAFT 1 Collisions btwn lctrons and ions Flix I. Parra Rudolf Pirls Cntr for Thortical Physics, Unirsity of Oxford, Oxford OX1 NP, UK This rsion is of 8 May 217 1. Introduction Th Fokkr-Planck collision

More information

Machine Detector Interface Workshop: ILC-SLAC, January 6-8, 2005.

Machine Detector Interface Workshop: ILC-SLAC, January 6-8, 2005. Intrnational Linar Collidr Machin Dtctor Intrfac Workshop: ILCSLAC, January 68, 2005. Prsntd by Brtt Parkr, BNLSMD Mssag: Tools ar now availabl to optimiz IR layout with compact suprconducting quadrupols

More information

Extraction of Doping Density Distributions from C-V Curves

Extraction of Doping Density Distributions from C-V Curves Extraction of Doping Dnsity Distributions from C-V Curvs Hartmut F.-W. Sadrozinski SCIPP, Univ. California Santa Cruz, Santa Cruz, CA 9564 USA 1. Connction btwn C, N, V Start with Poisson quation d V =

More information

Part 7: Capacitance And Capacitors

Part 7: Capacitance And Capacitors Part 7: apacitanc And apacitors 7. Elctric harg And Elctric Filds onsidr a pair of flat, conducting plats, arrangd paralll to ach othr (as in figur 7.) and sparatd by an insulator, which may simply b air.

More information

DIELECTRIC AND MAGNETIC PROPERTIES OF MATERIALS

DIELECTRIC AND MAGNETIC PROPERTIES OF MATERIALS DILCTRIC AD MAGTIC PROPRTIS OF MATRIALS Dilctric Proprtis: Dilctric matrial Dilctric constant Polarization of dilctric matrials, Typs of Polarization (Polarizability). quation of intrnal filds in liquid

More information

Properties of Quarks ( ) Isospin. π = 1, 1

Properties of Quarks ( ) Isospin. π = 1, 1 Proprtis of Quarks Isospin So far, w hav discussd thr familis of lptons but principally concntratd on on doublt of quarks, th u and d. W will now introduc othr typs of quarks, along with th nw quantum

More information

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

More information

1 Isoparametric Concept

1 Isoparametric Concept UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric

More information

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017 Th following qustions ar to b answrd individually. Usful information such as tabls with dtctor charactristics and graphs with th proprtis of matrials ar availabl in th cours wb sit: http://www.lip.pt/~patricia/fisicadaradiacao.

More information

Quasi-Classical States of the Simple Harmonic Oscillator

Quasi-Classical States of the Simple Harmonic Oscillator Quasi-Classical Stats of th Simpl Harmonic Oscillator (Draft Vrsion) Introduction: Why Look for Eignstats of th Annihilation Oprator? Excpt for th ground stat, th corrspondnc btwn th quantum nrgy ignstats

More information

Search sequence databases 3 10/25/2016

Search sequence databases 3 10/25/2016 Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an

More information

Neutrino Mass and Forbidden Beta Decays

Neutrino Mass and Forbidden Beta Decays NUCLEAR THEORY Vol. 35 016) ds. M. Gaidarov N. Minkov Hron Prss Sofia Nutrino Mass and Forbiddn Bta Dcays R. Dvornický 1 D. Štfánik F. Šimkovic 3 1 Dzhlpov Laboratory of Nuclar Problms JINR 141980 Dubna

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator. Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r

More information

BETA DECAY VISUAL PHYSICS ONLINE

BETA DECAY VISUAL PHYSICS ONLINE VISUAL PHYSICS ONLINE BETA DECAY Suppos now that a nuclus xists which has ithr too many or too fw nutrons rlativ to th numbr of protons prsnt for stability. Stability can b achivd by th convrsion insid

More information

Physics 2D Lecture Slides. Oct 21. UCSD Physics. Vivek Sharma

Physics 2D Lecture Slides. Oct 21. UCSD Physics. Vivek Sharma Physics D Lctur Slids Oct 1 Vivk Sharma UCSD Physics Modrn Viw of Photolctric Effct E = hf = KE+ ϕ Is h sam in Photolctric Effct as in BBQ Radiation? Slop h = 6.66 x 10-34 JS Einstin Nobl Priz! No mattr

More information

Pion condensation with neutrinos

Pion condensation with neutrinos Pion condnsation with nutrinos Or how dos QCD bhav undr high dnsitis of lctron/muon nutrinos Harmn Warringa, Goth Univrsität, Frankfurt Basd on work don with Hiroaki Abuki and Tomas Braunr arxiv:0901.2477

More information

Electrochemical Energy Systems Spring 2014 MIT, M. Z. Bazant. Midterm Exam

Electrochemical Energy Systems Spring 2014 MIT, M. Z. Bazant. Midterm Exam 10.66 Elctrochmical Enrgy Systms Spring 014 MIT, M. Z. Bazant Midtrm Exam Instructions. This is a tak-hom, opn-book xam du in Lctur. Lat xams will not b accptd. You may consult any books, handouts, or

More information

VII. Quantum Entanglement

VII. Quantum Entanglement VII. Quantum Entanglmnt Quantum ntanglmnt is a uniqu stat of quantum suprposition. It has bn studid mainly from a scintific intrst as an vidnc of quantum mchanics. Rcntly, it is also bing studid as a basic

More information

Math 34A. Final Review

Math 34A. Final Review Math A Final Rviw 1) Us th graph of y10 to find approimat valus: a) 50 0. b) y (0.65) solution for part a) first writ an quation: 50 0. now tak th logarithm of both sids: log() log(50 0. ) pand th right

More information