Corso di laurea magistrale in Fisica
|
|
- Cory Stafford
- 6 years ago
- Views:
Transcription
1 Coso di laua magisal in Fisica Laboaoio di Fisica I Anonio Sasso Dipaimno di Scinz Fisich Univsià di Napoli Fdico II sasso@na.infn.i i spimno di Millikan con singol micopaicll oicamn inappola
2 spimno di Millikan mx && γ v mg soluzion sazionaia v ρg 9 η 9 η ρ g L v L 0 d soluzion sazionaia γ v S mg q d q 6 πη v L v S di vido da: hp://
3 spimno di Millikan ivisiao con singol micosf inappola oicamn F F op l k Δx q q
4 Singlpaicl Manipulaion Tchniqus Aomic Foc Micoscop Opical Twzs Magnic Twzs las bam objciv F xnal magns F ap F xnal magnic bad focus of opical ap opical ap foc balancs h xnal foc sufac DNA Foc ang : 10pN 10nN 10fN 00 pn 10 nn 100 nn Foc snsiiviy: Spaial soluion: 1pN 0.0pN 0.1pN < nm fw nm fw nm Micopip Aspiaion 0.01 nn 1000 pn Anibodyanign Acinacin Bioinavidin Bioinspavidin 0pN 110pN 160pN 60pN
5 Pion of opical apping: Ahu Ashkin 1969/70: A. Ashkin,.L. Lokhov suggs o mploy adiaion pssu fo manipulaion wih aoms, molculs and micopaicls 1986: A. Ashkin singl bam opical ap Opical wzs 1987: A. Ashkin opical wzs movs wih bacia and viuss wihou hi damag C B
6 Opical Twzs A. Ashkin Op. L. 11, 1986 Opical apping Tapping obsva Opical lviaion Nual dilcic paicls siz: 0nm00μm foc: pn Biological maials: vius, bacia, clls, molcula moos, biological bonds,
7 Mchanical ffcs of ligh Ligh cais: ngy hν Tmpau ha o cu Lina momnum hν p c Focs mov o ap Angula momnum l ±h Toqus oa o wis
8 Bsids ngy ligh cais: lina momnum m m focs Johanns Kpl Gman 1571 sola wind Classical picu M hoy Maxwll 1mW 1pN adiaion pssu Quanum picu phoon momnum angulag momnum oqus p hνν c Wih h advn of lass: Las cooling Bosinsin Condnsaion Opical Twzs
9 Sola adiom by W. Cooks, 1974 P hνν c P hν c
10 Lbdv s xpimn 1901 spcchio fascio luminoso filo di quazo
11 adius of h paicl much small ha h ayligh gim a<<λ adius of h paicl much small ha h apping wavlngh 0 λ a < Inducd dipol m 1 a n m m a n p,, 1 4, 3 0 α ε π n n 1 Sc in f c dissip i p F 1 n n m polaizabiliy Scaing foc dissipaiv T T p sca S m m a k c n S C c n F π m c c 3 Gadin foc consvaiv : im avagd Poyning vco T S Gadin foc consvaiv T x T gad gad m m a n F F 3 0, 1, ε π T, α
12 Sn Glach xpimn
13 Mi gim a>>λ Gomical opics appoximaion Momnum chang Momnum chang in ou Foc ou Δ Δ in Bigh ay Dim ay Laal foc dp F d Axial foc
14 Singl ay soluion F sca fom Fsnl fomula F gad [ ] ] F n P T cosθ cos θ 1 cos θ sca c 1 cos [ sinθ sin ] F n P T sin θ gad c 1 cos θ A. Ashkin, Biophys. J. 61, 199
15 Basic ida: Gadin opical fild a b di appl dal sio hp://ph.coloado.du/
16 3D Opical ap: Gaussian mod Opical axis Wav fon Scaing foc Gadin foc Colloidal paicl Focusd las bam I I zxp[ x y / w z ] I 0 I z b 1 z / b πw 0 λ
17 Basic Schm of Opical Twzs Gaussian High NA objcivs las bam Ovfilling n 1 >n I F gad >F sca 50 μm 3D ap Tapping fficincy: i Q Q foc oc momnum p sc F Pn / c
18 Opical Twzs sup 1μm vino 50μm acqua spac Piano focal olio vino las Gaussian las bam
19 Snso posiion I: Quadan Phoodiod X Q1 Q Q3 Q4 1 Q1 Q Q3 Q4 34 Y Q1 Q3 Q Q4 Q1 Q Q3 Q4 Z Q1 Q Q3 Q4 6 4 z 1 fom h slop h calibaion faco β [nm/vol] is found! Sign nal Sgnal dl foodiodo a quadani Posiion µm 1 yab*x a 0.06±0.03 b ±0.000 /nm β 173 ± Posizion nm 6 nm / Δxβ Lina spons small Dx Typical snsiiviy: 3 nm!! Typicali l bandwidh: khzmhz
20 Polysynbad capu φ1 mm Yas cll Tim shaing aps by galvo mios
21 Scoisch danc is cub
22 Tacking of opically appd paicls QP x y z x Fkx K: ap siffnss Langvin q. ovdampd haminic oscillao m && x γ x& κ x F Fo micomic paicls in wa inial is ngligibl
23 1.quipaiion mhod x man squa displacmn man squa volag 1 k B T 1 κ x 1 κβ x 0 x β
24 .Bolzmann saisics Pobabiliy of finding a small paicl in a ponial x in a volum dx is don by Bolzmann saisics x p x dx C xp k B T 1 x k B T ln p x k B T ln C κ x 1 κβ x offs offs px is don by h hisogam of im cod of sph posiions k is obaind fom h paabolic fi Xaxis Yaxis vn hs mhods nd calibaion of h posiion snso β bu do no nd infomaion abou h sph siz and mdium viscosiy
25 3. Pow Spcal Dnsiy fquncy domain quazion di Langvin m && x γ x& κx F S f γπ k β B T f f c f c κ 1 πγ c loglog lina A.Buosciolo al. Op.Commun
26 4. Auocolaion mhod f B B c c k T k k T k c π 0 k k π d f S f i 1 π d c f S c μs 108 C C This mhod dos no nd calibaion of h posiion snso bu nds infomaion abou sph siz and mdium viscosiy.
27 volag 1.Spwis gim 0 im q.oscillaoy gim volag im
28 1. Tapping in saic fild volag im
29 Doubl lay lcic fild in h lcoly can b asly calculad fom an quivaln cicui: quivaln cicui quivaln ff q ff C d : Doubllay capacianc d : Doubllay sisanc i : Soluion sisanc d dpnd on: dox acions a lcods lcolys ionic concnaion 0 o 0 d max DL DL d d d d C d DL C d
30 DL d d d o 0 o 0 d 0 max 0 Z o i 0 d o d
31 ff h l h q F F F x x κ γ & ] [ max ff h q F DL 1 max γ γ γ k ff k DL l ff k q k q x DL Z o i 0 1 max OP OP DL x x x DL C d DL DL x k OP γ OP x max x
32 . Tapping in oscillaoy gim γ x& κxκ x F F h F h l q cos π f ff 0 l kbt 1 kbtγ S f δ f 4π γ f f k 3 l c f S f S f f l f C obs al.j. Chm. Phys. 16, f l k BT Psig I p f df γ k q k ff P sig No vy acua dminaion!!
33 Nomalizd auocolaion funcion 1 S f c xp iπ f d π Foc aio c 1 πf ξ c C cos π f l c0 1 ξ 1 ξ ξ q 1 ff F o l kbtk f F l h Thmal conibuio Oscill. m 1 f l 1 1 fc fc ξ <1: hmal nois ξ >1 1 : lcical modulaion
34 cos 1 π ξ π l f f c C c cos π ξ ξ l f c C C 1 ξ ξ 1 ξ c l B ff f f k T k q πγξ k Chag snsiiviy ~!!
35 Wak foc masumns ξ is masud fom ACF k T B f f l c F q πγξ l ff k If h fild is known h chag can b masud o vicvsa SN aio
36 Chag masumns Unifom lcic fild εε η μ 0 ζ ζ 15.7m Q ACF 1. ± C xp Q Z h ζ kbt a λ B 1 κa 10 xp Q Z 1.0 ± C
37 1.lcic fild masumns: Wipla gomy G.Psc al. Labonachip, in pss h150 μm molibdn wi ~ ITO lcod Φ10 μm x y z covslip C x, y, z C x, y, z hoy xp
38 3.lcic fild aound a nanomic ip h35 μm molibdn wi Φ10 μm y x ~ ITO lcod z covslip SM imag y x
39 Thoyxpimn vc xpimn h x
1 Lecture: pp
EE334 - Wavs and Phasos Lcu: pp -35 - -6 This cous aks vyhing ha you hav bn augh in physics, mah and cicuis and uss i. Easy, only nd o know 4 quaions: 4 wks on fou quaions D ρ Gauss's Law B No Monopols
More informationChapter 2 : Fundamental parameters of antennas
Chap : Fundamnal paams of annnas Fom adiaion an adiaion innsiy Bamwidh Diciviy nnna fficincy Gain olaizaion Fom Cicui viwpoin Inpu Impdanc 1 Chap : opics nnna ffciv lngh and ffciv aa Fiis ansmission quaion
More informationStudy of Tyre Damping Ratio and In-Plane Time Domain Simulation with Modal Parameter Tyre Model (MPTM)
Sudy o Ty Damping aio and In-Plan Tim Domain Simulaion wih Modal Paam Ty Modl (MPTM D. Jin Shang, D. Baojang Li, and Po. Dihua Guan Sa Ky Laboaoy o Auomoiv Say and Engy, Tsinghua Univsiy, Bijing, China
More informationDynamics of Bloch Electrons 1
Dynamics of Bloch Elcons 7h Spmb 003 c 003, Michal Mad Dfiniions Dud modl Smiclassical dynamics Bloch oscillaions K P mhod Effciv mass Houson sas Zn unnling Wav pacs Anomalous vlociy Wanni Sa ladds d Haas
More informationWhat is an Antenna? Not an antenna + - Now this is an antenna. Time varying charges cause radiation but NOT everything that radiates is an antenna!
Wha is an Annna? Tim vaying chags caus adiaion bu NOT vyhing ha adias is an annna! No an annna + - Now his is an annna Wha is an Annna? An annna is a dvic ha fficinly ansiions bwn ansmission lin o guidd
More informationLecture 14. Time Harmonic Fields
Lcu 4 Tim amic Filds I his lcu u will la: Cmpl mahmaics f im-hamic filds Mawll s quais f im-hamic filds Cmpl Pig vc C 303 Fall 007 Faha aa Cll Uivsi Tim-amic Filds ad -filds f a pla wav a (fm las lcu:
More informationAakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics
Aakash A UNIQUE PPRTUNITY T HELP YU FULFIL YUR DREAMS Fo Class XII Studying / Passd Studnts Physics, Chmisty & Mathmatics Rgistd ffic: Aakash Tow, 8, Pusa Road, Nw Dlhi-0005. Ph.: (0) 4763456 Fax: (0)
More informationLecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation
Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion
More information3.46 PHOTONIC MATERIALS AND DEVICES Lecture 10: LEDs and Optical Amplifiers
3.46 PHOTONIC MATERIALS AND DEVICES Lctu 0: LEDs and Optical Amplifis Lctu Rfncs:. Salh, M. Tich, Photonics, (John-Wily, Chapts 5-6. This lctu will viw how lctons and hols combin in smiconductos and nat
More informationGRAVITATION 4) R. max. 2 ..(1) ...(2)
GAVITATION PVIOUS AMCT QUSTIONS NGINING. A body is pojctd vtically upwads fom th sufac of th ath with a vlocity qual to half th scap vlocity. If is th adius of th ath, maximum hight attaind by th body
More informationLecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light
Lecue 5 Chape 3 lecomagneic Theo, Phoons, and Ligh Gauss s Gauss s Faada s Ampèe- Mawell s + Loen foce: S C ds ds S C F dl dl q Mawell equaions d d qv A q A J ds ds In mae fields ae defined hough ineacion
More informationWAKEFIELD UNDULATOR RADIATION
WKEFIELD UNDULTOR RDITION. Opanasnko NSC KIPT, UKRINE MECHNISM OF WFU RDITION SPECTRL -NGULR CHRCTERISTICS MODEL OF WF UNDULTOR WKEFIELD DISTRIBUTION HRD X-RY GENERTING POSSIBILITY of EXPERIMENTL STUDY
More informationSuperposition. Section 8.5.3
Supeposition Section 8.5.3 Simple Potential Flows Most complex potential (invicid, iotational) flows can be modeled using a combination of simple potential flows The simple flows used ae: Unifom flows
More informationH is equal to the surface current J S
Chapr 6 Rflcion and Transmission of Wavs 6.1 Boundary Condiions A h boundary of wo diffrn mdium, lcromagnic fild hav o saisfy physical condiion, which is drmind by Maxwll s quaion. This is h boundary condiion
More information8 - GRAVITATION Page 1
8 GAVITATION Pag 1 Intoduction Ptolmy, in scond cntuy, gav gocntic thoy of plantay motion in which th Eath is considd stationay at th cnt of th univs and all th stas and th plants including th Sun volving
More informationQ Q N, V, e, Quantum Statistics for Ideal Gas and Black Body Radiation. The Canonical Ensemble
Quantum Statistics fo Idal Gas and Black Body Radiation Physics 436 Lctu #0 Th Canonical Ensmbl Ei Q Q N V p i 1 Q E i i Bos-Einstin Statistics Paticls with intg valu of spin... qi... q j...... q j...
More informationFourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation
Pof. D. I. Nass Phys57 (T-3) Sptmb 8, 03 Foui_Tansf_phys57_T3 Foui tansfoms (Chapt 5) Foui intgals a gnalizations of Foui sis. Th sis psntation a0 nπx nπx f ( x) = + [ an cos + bn sin ] n = of a function
More informationPhysics C Rotational Motion Name: ANSWER KEY_ AP Review Packet
Linea and angula analogs Linea Rotation x position x displacement v velocity a T tangential acceleation Vectos in otational motion Use the ight hand ule to detemine diection of the vecto! Don t foget centipetal
More informationGRAVITATION. (d) If a spring balance having frequency f is taken on moon (having g = g / 6) it will have a frequency of (a) 6f (b) f / 6
GVITTION 1. Two satllits and o ound a plant P in cicula obits havin adii 4 and spctivly. If th spd of th satllit is V, th spd of th satllit will b 1 V 6 V 4V V. Th scap vlocity on th sufac of th ath is
More informationReinforcement learning
Lecue 3 Reinfocemen leaning Milos Hauskech milos@cs.pi.edu 539 Senno Squae Reinfocemen leaning We wan o lean he conol policy: : X A We see examples of x (bu oupus a ae no given) Insead of a we ge a feedback
More informationMATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH
Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias
More informationDSP-First, 2/e. This Lecture: LECTURE #3 Complex Exponentials & Complex Numbers. Introduce more tools for manipulating complex numbers
DSP-Fis, / LECTURE #3 Compl Eponnials & Compl umbs READIG ASSIGMETS This Lcu: Chap, Scs. -3 o -5 Appndi A: Compl umbs Appndi B: MATLAB Lcu: Compl Eponnials Aug 016 003-016, JH McClllan & RW Schaf 3 LECTURE
More informationEN221 - Fall HW # 7 Solutions
EN221 - Fall2008 - HW # 7 Soluions Pof. Vivek Shenoy 1.) Show ha he fomulae φ v ( φ + φ L)v (1) u v ( u + u L)v (2) can be pu ino he alenaive foms φ φ v v + φv na (3) u u v v + u(v n)a (4) (a) Using v
More informationQuantum Statistical Properties of Resonant Radiation Scattered on Excited Systems
J Mod Phys,,, 63-7 doi:436/m34 Publishd Onlin Augus (h://wwwsciog/ounal/m) Quanum Saisical Pois of sonan adiaion Scad on Excid Sysms Absac Bois A Vklnko Join Insiu fo High Tmau of ussian Acadmy of Scinc,
More informationGMm. 10a-0. Satellite Motion. GMm U (r) - U (r ) how high does it go? Escape velocity. Kepler s 2nd Law ::= Areas Angular Mom. Conservation!!!!
F Satllt Moton 10a-0 U () - U ( ) 0 f ow g dos t go? scap locty Kpl s nd Law ::= Aas Angula Mo. Consaton!!!! Nwton s Unsal Law of Gaty 10a-1 M F F 1) F acts along t ln connctng t cnts of objcts Cntal Foc
More informationCollaborative ASSIGNMENT Assignment 3: Sources of magnetic fields Solution
Electicity and Magnetism: PHY-04. 11 Novembe, 014 Collaboative ASSIGNMENT Assignment 3: Souces of magnetic fields Solution 1. a A conducto in the shape of a squae loop of edge length l m caies a cuent
More informationBethe-Salpeter Equation Green s Function and the Bethe-Salpeter Equation for Effective Interaction in the Ladder Approximation
Bh-Salp Equaon n s Funcon and h Bh-Salp Equaon fo Effcv Inacon n h Ladd Appoxmaon Csa A. Z. Vasconcllos Insuo d Físca-UFRS - upo: Físca d Hadons Sngl-Pacl Popagao. Dagam xpanson of popagao. W consd as
More informationCONDITION OF DAMPING OF ANOMALOUS RADIAL TRANSPORT, DETERMINED BY ORDERED CONVECTIVE ELECTRON DYNAMICS
CONDITION OF DAMPING OF ANOMALOUS RADIAL TRANSPORT DETERMINED BY ORDERED CONVECTIVE ELECTRON DYNAMICS VIMaslv SVBachuk VILapshin YuVMlnsv* EDVlkv NSC Khakv Insiu f Physics and Tchnlgy Khakv 608 Ukain *Kaain
More informationA moving charged particle creates a magnetic field vector at every point in space except at its position.
1 Pat 3: Magnetic Foce 3.1: Magnetic Foce & Field A. Chaged Paticles A moving chaged paticle ceates a magnetic field vecto at evey point in space ecept at its position. Symbol fo Magnetic Field mks units
More informationLecture 2: Current in RC circuit D.K.Pandey
Lcur 2: urrn in circui harging of apacior hrough Rsisr L us considr a capacior of capacianc is conncd o a D sourc of.m.f. E hrough a rsisr of rsisanc R and a ky K in sris. Whn h ky K is swichd on, h charging
More informationToday - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations
Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy
More information[Griffiths Ch.1-3] 2008/11/18, 10:10am 12:00am, 1. (6%, 7%, 7%) Suppose the potential at the surface of a hollow hemisphere is specified, as shown
[Giffiths Ch.-] 8//8, :am :am, Useful fomulas V ˆ ˆ V V V = + θ+ φ ˆ and v = ( v ) + (sin θvθ ) + v θ sinθ φ sinθ θ sinθ φ φ. (6%, 7%, 7%) Suppose the potential at the suface of a hollow hemisphee is specified,
More informationAlmost power law : Tempered power-law models (T-FADE)
Almos powr law : Tmprd powr-law modls T-FADE Yong Zhang Dsr Rsarch Insiu Novmbr 4, 29 Acknowldgmns Boris Baumr Mark Mrschar Donald Rvs Oulin Par Spac T-FADE modl. Inroducion 2. Numrical soluion 3. Momn
More informationEXTENDED CHARGE ELECTRO-OSMOSIS AND ELECTRO-CONVECTIVE INSTABILITY. Isaak Rubinstein. Boris Zaltzman Ben-Gurion University of the Negev Israel
EXTENDED CHARGE ELECTRO-OSMOSS AND ELECTRO-CONECTE NSTABLTY saak Rubinsin Bois Zalman Bn-Guion Unisi of h Ng sal Conduion fom an lol ino a hag-sli solid ion hang mmban o mal lod Eli doubl la -- - ψ C C
More information4038/02 October/November 2009
Additional Mathematics (408/0) version 1.1 ADDITIONAL MATHEMATIS Paper Suggested Solutions 1. Topic: Further Trigonometric Identities sin(a B) sin A cos B cos A sin B 8 5 8 cos A sin B 8 8 408/0 October/November
More informationLecture 17: Kinetics of Phase Growth in a Two-component System:
Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien
More informationMagnetic Dipoles Challenge Problem Solutions
Magnetic Dipoles Challenge Poblem Solutions Poblem 1: Cicle the coect answe. Conside a tiangula loop of wie with sides a and b. The loop caies a cuent I in the diection shown, and is placed in a unifom
More informationDynamics of Rotational Motion
Dynamics of Rotational Motion Toque: the otational analogue of foce Toque = foce x moment am τ = l moment am = pependicula distance though which the foce acts a.k.a. leve am l l l l τ = l = sin φ = tan
More informationArturo R. Samana* in collaboration with Carlos Bertulani*, & FranjoKrmpotic(UNLP-Argentina) *Department of Physics Texas A&M University -Commerce 07/
Comparison of RPA-lik modls in Nurino-Nuclus Nuclus Procsss Aruro R. Samana* in collaboraion wih Carlos Brulani* & FranjoKrmpoicUNLP-Argnina *Dparmn of Physics Txas A&M Univrsiy -Commrc 07/ 0/008 Aomic
More informationELECTROMAGNETIC FIELDS
Pf. ng. an Macháč Dc. lcmagnic Filds LCTROMAGNTC FLD yllabus f Lcus Pf. ng. an Macháč Dc. - - Pf. ng. an Macháč Dc. lcmagnic Filds nducin nvinmn: hmgnus - nnhmgnus ispic - anispic lina - nnlina nndispsiv
More informationQuiz 6--Work, Gravitation, Circular Motion, Torque. (60 pts available, 50 points possible)
Name: Class: Date: ID: A Quiz 6--Wok, Gavitation, Cicula Motion, Toque. (60 pts available, 50 points possible) Multiple Choice, 2 point each Identify the choice that best completes the statement o answes
More informationPhys Nov. 3, 2017 Today s Topics. Continue Chapter 2: Electromagnetic Theory, Photons, and Light Reading for Next Time
Phys 31. No. 3, 17 Today s Topcs Cou Chap : lcomagc Thoy, Phoos, ad Lgh Radg fo Nx Tm 1 By Wdsday: Radg hs Wk Fsh Fowls Ch. (.3.11 Polazao Thoy, Jos Macs, Fsl uaos ad Bws s Agl Homwok hs Wk Chap Homwok
More informationE F. and H v. or A r and F r are dual of each other.
A Duality Thom: Consid th following quations as an xampl = A = F μ ε H A E A = jωa j ωμε A + β A = μ J μ A x y, z = J, y, z 4π E F ( A = jω F j ( F j β H F ωμε F + β F = ε M jβ ε F x, y, z = M, y, z 4π
More informationAcoustics and electroacoustics
coustics and lctoacoustics Chapt : Sound soucs and adiation ELEN78 - Chapt - 3 Quantitis units and smbols: f Hz : fqunc of an acoustical wav pu ton T s : piod = /f m : wavlngth= c/f Sound pssu a : pzt
More informationMicro-bunching: Longitudinal Bunch Profile Measurements at TTF
Shot Pulses in Rings Mico-bunching: Longitudinal Bunch Pofile Measuements at TTF ) The time vaying fields in a tansvese mode cavity kick the font of a bunch up, and the back of the bunch don. ) A betaton
More information5.61 Fall 2007 Lecture #2 page 1. The DEMISE of CLASSICAL PHYSICS
5.61 Fall 2007 Lctu #2 pag 1 Th DEMISE of CLASSICAL PHYSICS (a) Discovy of th Elcton In 1897 J.J. Thomson discovs th lcton and masus ( m ) (and inadvtntly invnts th cathod ay (TV) tub) Faaday (1860 s 1870
More informationSTATISTICAL MECHANICS OF DIATOMIC GASES
Pof. D. I. ass Phys54 7 -Ma-8 Diatomic_Gas (Ashly H. Cat chapt 5) SAISICAL MECHAICS OF DIAOMIC GASES - Fo monatomic gas whos molculs hav th dgs of fdom of tanslatoy motion th intnal u 3 ngy and th spcific
More informationRectilinea Motion. A foce P is applied to the initially stationay cat. Detemine the velocity and displacement at time t=5 s fo each of the foce histoi
Rectilinea Motion 1. Small objects ae deliveed to the m inclined chute by a conveyo belt A which moves at a speed v 1 =0.4 m/s. If the conveyo belt B has a speed v =0.9 m/s and the objects ae deliveed
More informationPHYS 2135 Exam I February 13, 2018
Exam Total /200 PHYS 2135 Exam I Febuay 13, 2018 Name: Recitation Section: Five multiple choice questions, 8 points each Choose the best o most nealy coect answe Fo questions 6-9, solutions must begin
More informationMon. Tues. 6.2 Field of a Magnetized Object 6.3, 6.4 Auxiliary Field & Linear Media HW9
Fi. on. Tus. 6. Fild of a agntid Ojct 6.3, 6.4 uxiliay Fild & Lina dia HW9 Dipol t fo a loop Osvation location x y agntic Dipol ont Ia... ) ( 4 o I I... ) ( 4 I o... sin 4 I o Sa diction as cunt B 3 3
More informationC From Faraday's Law, the induced voltage is, C The effect of electromagnetic induction in the coil itself is called selfinduction.
Inducors and Inducanc C For inducors, v() is proporional o h ra of chang of i(). Inducanc (con d) C Th proporionaliy consan is h inducanc, L, wih unis of Hnris. 1 Hnry = 1 Wb / A or 1 V sc / A. C L dpnds
More informationSchool of Electrical Engineering. Lecture 2: Wire Antennas
School of lctical ngining Lctu : Wi Antnnas Wi antnna It is an antnna which mak us of mtallic wis to poduc a adiation. KT School of lctical ngining www..kth.s Dipol λ/ Th most common adiato: λ Dipol 3λ/
More informationThe Global Trade and Environment Model: GTEM
The Global Tade and Envionmen Model: A pojecion of non-seady sae daa using Ineempoal GTEM Hom Pan, Vivek Tulpulé and Bian S. Fishe Ausalian Bueau of Agiculual and Resouce Economics OBJECTIVES Deive an
More informationDIELECTRICS MICROSCOPIC VIEW
HYS22 M_ DILCTRICS MICROSCOIC VIW DILCTRIC MATRIALS Th tm dilctic coms fom th Gk dia lctic, wh dia mans though, thus dilctic matials a thos in which a stady lctic fild can st up without causing an appcial
More informationExercise 4: Adimensional form and Rankine vortex. Example 1: adimensional form of governing equations
Fluid Mechanics, SG4, HT9 Septembe, 9 Execise 4: Adimensional fom and Rankine votex Example : adimensional fom of govening equations Calculating the two-dimensional flow aound a cylinde (adius a, located
More informationChapter 5 Transmission Lines
ap 5 ao 5- aacc of ao ao l: a o cou ca cu o uppo a M av c M o qua-m o. Fo M o a H M H a M a µ M. cu a M av av ff caacc. A M av popaa o ff lcc a paal flco a paal ao ll occu. A ob follo ul. ll la: p a β
More informationOptimal design of full disks with respect to mixed creep rupture time
Compu Aidd Opimum Dsign in Engining XII 83 Opimal dsign of full disks wih spc o mixd cp upu im K. Szuwalski & A. Uszycka Cacow Univsiy of Tchnology, Poland Absac Th mixd upu hoy o h opimizaion poblm fo
More informationand in each case give the range of values of x for which the expansion is valid.
α β γ δ ε ζ η θ ι κ λ µ ν ξ ο π ρ σ τ υ ϕ χ ψ ω Mathematics is indeed dangerous in that it absorbs students to such a degree that it dulls their senses to everything else P Kraft Further Maths A (MFPD)
More informationUniversity of Toledo REU Program Summer 2002
Univiy of Toldo REU Pogam Summ 2002 Th Effc of Shadowing in 2-D Polycyallin Gowh Jff Du Advio: D. Jacqu Ama Dpamn of Phyic, Univiy of Toldo, Toldo, Ohio Abac Th ffc of hadowing in 2-D hin film gowh w udid
More informationSolid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch
Solid stat physics Lctu 3: chmical bonding Pof. D. U. Pitsch Elcton chag dnsity distibution fom -ay diffaction data F kp ik dk h k l i Fi H p H; H hkl V a h k l Elctonic chag dnsity of silicon Valnc chag
More information( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba
THE INTEACTION OF ADIATION AND MATTE: SEMICLASSICAL THEOY PAGE 26 III. EVIEW OF BASIC QUANTUM MECHANICS : TWO -LEVEL QUANTUM SYSTEMS : The lieaue of quanum opics and lase specoscop abounds wih discussions
More informationThe Production of Polarization
Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview
More informationPhysics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas
Physics 111 Lctu 38 (Walk: 17.4-5) Phas Chang May 6, 2009 Lctu 38 1/26 Th Th Basic Phass of Matt Solid Liquid Gas Squnc of incasing molcul motion (and ngy) Lctu 38 2/26 If a liquid is put into a sald contain
More informationm H = ± 0.24GeV
m H = 125.09 ± 0.24GeV Y B n B s =(8.59 ± 0.11) 10 11 n B = n b n b( b) : n b s : W = g 2 2/4 (s) B ( W T ) 4 =0.1 1.0 (b) B T 4 e E sph/t E sph : v(t ) v v C T T C v C T C V e (T ) T>T C T = T C T
More informationω = θ θ o = θ θ = s r v = rω
Unifom Cicula Motion Unifom cicula motion is the motion of an object taveling at a constant(unifom) speed in a cicula path. Fist we must define the angula displacement and angula velocity The angula displacement
More informationPartial Fraction Expansion
Paial Facion Expanion Whn ying o find h inv Laplac anfom o inv z anfom i i hlpfl o b abl o bak a complicad aio of wo polynomial ino fom ha a on h Laplac Tanfom o z anfom abl. W will illa h ing Laplac anfom.
More informationElectric field generated by an electric dipole
Electic field geneated by an electic dipole ( x) 2 (22-7) We will detemine the electic field E geneated by the electic dipole shown in the figue using the pinciple of supeposition. The positive chage geneates
More informationCentral Force Motion
Cental Foce Motion Cental Foce Poblem Find the motion of two bodies inteacting via a cental foce. Examples: Gavitational foce (Keple poblem): m1m F 1, ( ) =! G ˆ Linea estoing foce: F 1, ( ) =! k ˆ Two
More informationChapter 1 Electric Circuit Variables
Chaper 1 Elecric Circui Variables Exercises Exercise 1.2-1 Find he charge ha has enered an elemen by ime when i = 8 2 4 A, 0. Assume q() = 0 for < 0. 8 3 2 Answer: q () = 2 C 3 () 2 i = 8 4 A 2 8 3 2 8
More informationF = net force on the system (newton) F,F and F. = different forces working. E = Electric field strength (volt / meter)
All the Impotant Fomulae that a student should know fom. XII Physics Unit : CHAPTER - ELECTRIC CHARGES AND FIELD CHAPTER ELECTROSTATIC POTENTIAL AND CAPACITANCE S. Fomula No.. Quantization of chage Q =
More informationModule 05: Gauss s s Law a
Module 05: Gauss s s Law a 1 Gauss s Law The fist Maxwell Equation! And a vey useful computational technique to find the electic field E when the souce has enough symmety. 2 Gauss s Law The Idea The total
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More information3. ANALYTICAL KINEMATICS
In planar mechanisms, kinematic analysis can be performed either analytically or graphically In this course we first discuss analytical kinematic analysis nalytical kinematics is based on projecting the
More information4.4 Linear Dielectrics F
4.4 Lina Dilctics F stal F stal θ magntic dipol imag dipol supconducto 4.4.1 Suscptiility, mitivility, Dilctic Constant I is not too stong, th polaization is popotional to th ild. χ (sinc D, D is lctic
More informationWORK POWER AND ENERGY Consevaive foce a) A foce is said o be consevaive if he wok done by i is independen of pah followed by he body b) Wok done by a consevaive foce fo a closed pah is zeo c) Wok done
More information! 94
! 94 4 : - : : / : : : : ( :) : : : - : / : / : : - 4 : -4 : : : : : -5 () ( ) : -6 : - - : : : () : : : :4 : -7. : : -8. (. : ( : -9 : ( ( ( (5 (4 4 : -0! : ( : ( :. : (. (. (. (4. ( ( ( : ( 4 : - : :
More informationCHM 424 EXAM 2 - COVER PAGE FALL
CHM 44 EXAM - COVER PAGE FALL 006 There are seven numbered pages with five questions. Answer the questions on the exam. Exams done in ink are eligible for regrade, those done in pencil will not be regraded.
More informationWireless Networking Guide
ilss woking Guid Ging h bs fom you wilss nwok wih h ZTE H98 ou w A n B Rs B A w ilss shligh.co.uk wok Guid; ZTE H98 ous Las amndd: 08000/0/0 768 Cns. Cncing o a wilss nwok. Toublshooing a wilss cnci. Oh
More information3.012 Fund of Mat Sci: Bonding Lecture 1 bis. Photo courtesy of Malene Thyssen,
3.012 Fund of Ma Sci: Bonding Lecue 1 bis WAVE MECHANICS Phoo couesy of Malene Thyssen, www.mfoo.dk/malene/ 3.012 Fundamenals of Maeials Science: Bonding - Nicola Mazai (MIT, Fall 2005) Las Time 1. Playes:
More informationRAO IIT ACADEMY / NSEP Physics / Code : P 152 / Solutions NATIONAL STANDARD EXAMINATION IN PHYSICS SOLUTIONS
RAO ACADEMY / NSEP Physics / Code : P 5 / Solutions NAONAL SANDARD EXAMNAON N PHYSCS - 5 SOLUONS RAO ACADEMY / NSEP Physics / Code : P 5 / Solutions NSEP SOLUONS (PHYSCS) CODE - P 5 ANSWER KEY & SOLUONS.
More informationMonte Carlo Radiation Transfer I
Monte Carlo Radiation Transfer I Monte Carlo Photons and interactions Sampling from probability distributions Optical depths, isotropic emission, scattering Monte Carlo Basics Emit energy packet, hereafter
More informationAperture Antennas 1 Introduction
1 Introduction Very often, we have antennas in aperture forms, for example, the antennas shown below: Pyramidal horn antenna Conical horn antenna 1 Paraboloidal antenna Slot antenna Analysis Method for.1
More informationLecture 2: Bayesian inference - Discrete probability models
cu : Baysian infnc - Disc obabiliy modls Many hings abou Baysian infnc fo disc obabiliy modls a simila o fqunis infnc Disc obabiliy modls: Binomial samling Samling a fix numb of ials fom a Bnoulli ocss
More informationIntroduction to Accelerator Physics
Intoduction to Acceleato Physics Pat 3 Pedo Casto / Acceleato Physics Goup (MPY) Intoduction to Acceleato Physics DSY, 5th July 017 acceleating devices vacuum chambe injecto acceleating device staight
More informationCHAPTER 5 CIRCULAR MOTION
CHAPTER 5 CIRCULAR MOTION and GRAVITATION 5.1 CENTRIPETAL FORCE It is known that if a paticl mos with constant spd in a cicula path of adius, it acquis a cntiptal acclation du to th chang in th diction
More informationCollective Focusing of a Neutralized Intense Ion Beam Propagating Along a Weak Solenodial Magnetic Field
Havy Ion Fusion Scinc Vitual National Laoatoy Collctiv Focusing of a Nutalizd Intns Ion Bam Popagating Along a Wak Solnodial Magntic Fild M. Dof (LLNL) In collaoation with I. Kaganovich, E. Statsv, and
More informationGUIDE FOR SUPERVISORS 1. This event runs most efficiently with two to four extra volunteers to help proctor students and grade the student
GUIDE FOR SUPERVISORS 1. This vn uns mos fficinly wih wo o fou xa voluns o hlp poco sudns and gad h sudn scoshs. 2. EVENT PARAMETERS: Th vn supviso will povid scoshs. You will nd o bing a im, pns and pncils
More informationScanning Force Microscopy
Scanning Force Microscopy Roland Bennewitz Rutherford Physics Building 405 Phone 398-3058 roland.bennewitz@mcgill.ca Scanning Probe is moved along scan lines over a sample surface 1 Force Microscopy Data
More informationA2 Assignment lambda Cover Sheet. Ready. Done BP. Question. Aa C4 Integration 1 1. C4 Integration 3
A Assignment lambda Cover Sheet Name: Question Done BP Ready Topic Comment Drill Mock Exam Aa C4 Integration sin x+ x+ c 4 Ab C4 Integration e x + c Ac C4 Integration ln x 5 + c Ba C Show root change of
More information6.Optical and electronic properties of Low
6.Optical and lctonic poptis of Low dinsional atials (I). Concpt of Engy Band. Bonding foation in H Molculs Lina cobination of atoic obital (LCAO) Schoding quation:(- i VionV) E find a,a s.t. E is in a
More informationAP Calculus BC - Parametric equations and vectors Chapter 9- AP Exam Problems solutions
AP Calculus BC - Parameric equaions and vecors Chaper 9- AP Exam Problems soluions. A 5 and 5. B A, 4 + 8. C A, 4 + 4 8 ; he poin a is (,). y + ( x ) x + 4 4. e + e D A, slope.5 6 e e e 5. A d hus d d
More informationPhysics 201 Lecture 18
Phsics 0 ectue 8 ectue 8 Goals: Define and anale toque ntoduce the coss poduct Relate otational dnamics to toque Discuss wok and wok eneg theoem with espect to otational motion Specif olling motion (cente
More informationEE 529 Remote Sensing Techniques. Review
59 Rmo Snsing Tchniqus Rviw Oulin Annna array Annna paramrs RCS Polariaion Signals CFT DFT Array Annna Shor Dipol l λ r, R[ r ω ] r H φ ηk Ilsin 4πr η µ - Prmiiviy ε - Prmabiliy
More informationCircular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.
1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule
More information9.4 Absorption and Dispersion
9.4 Absoon and Dsson 9.4. loagn Wavs n Conduos un dnsy n a onduo ollowng Oh s law: J Th Maxwll s uaons n a onduo lna da should b: ρ B B B J To sly h suaon w agu ha h hag dsaas uly n a aoso od. Fo h onnuy
More informationLecture 20. Transmission Lines: The Basics
Lcu 0 Tansmissin Lins: Th Basics n his lcu u will lan: Tansmissin lins Diffn ps f ansmissin lin sucus Tansmissin lin quains Pw flw in ansmissin lins Appndi C 303 Fall 006 Fahan Rana Cnll Univsi Guidd Wavs
More informationInvariant and Conditionally Invariant Solutions of Magnetohydrodynamic Equations in (3 + 1) Dimensions
Proceedings of Institute of Mathematics of NAS of Ukraine 2004, Vol. 50, Part 1, 118 124 Invariant and Conditionally Invariant Solutions of Magnetohydrodynamic Equations in 3 + 1) Dimensions A.M. GRUNDLAND
More informationRepresenting Knowledge. CS 188: Artificial Intelligence Fall Properties of BNs. Independence? Reachability (the Bayes Ball) Example
C 188: Aificial Inelligence Fall 2007 epesening Knowledge ecue 17: ayes Nes III 10/25/2007 an Klein UC ekeley Popeies of Ns Independence? ayes nes: pecify complex join disibuions using simple local condiional
More informationPhysics NYB problem set 5 solution
Physics NY poblem set 5 solutions 1 Physics NY poblem set 5 solution Hello eveybody, this is ED. Hi ED! ED is useful fo dawing the ight hand ule when you don t know how to daw. When you have a coss poduct
More informationObserving Fast Molecular Dynamics with a Coherent Raman Oscillator
FRISNO 13 - March 19, 2015 Observing Fas Molecular Dynamics wih a Coheren Raman Oscillaor Igal Aharonovich, Avi Pe er Physics Dep. and BINA cener for nanoechnology, Bar Ilan Universiy ISF Unlocking he
More information