Electronic Energies in Delta Doped AlGaAs/GaAs Heterostuctures

Size: px
Start display at page:

Download "Electronic Energies in Delta Doped AlGaAs/GaAs Heterostuctures"

Transcription

1 Amcn Jounl of Appld Scncs 5 (4: 45-49, 8 ISS Scnc Publctons Elctonc Engs n Dlt Dopd AlGAs/GAs Htostuctus A. Mfth, H. Ajln, A. Mouk, R. Chtouou nd M. Ouslt Fculty of Scncs of Tuns, Unvsty cmpus, 9 El Mn, Tuns tonl Insttut of Scntfc nd Tchncl Rsch Abstct: Th bnd bndng of th potntl t th AlGAs/GAs ntfc ncss wth th lctons concntton n th GAs chnnl. Ths bnd bndng s oftn gnod n th thotcl clculton of th lctonc ngs nd ln potntl ppoxmton ws usd. Ths ld to mpcs ngy vlus nd occupd subbnd confgutons. W hv tkn ccount of th bnd bndng n th subbnd ngs clculton. Th potntl xpsson ws consdd s sum of ln nd qudtc tms. Th qudtc tm ws consdd s tm ndpndnt ptubton nd th lctonc ngs w coctd to th fst od. W hv clcultd th Fm ngy fo dffnt lctonc concnttons. Th lton btwn th Fm ngy nd th lctonc concntton t th ntfc lds to th dsd confguton of th occupd subbnds. Whn th fundmntl subbnd s only occupd, th chctstcs of thos htostuctus bst nhncd. Th cospondng lctonc concntton ws clcultd. Th thotcl sults w usd fo th dtmnton of th ctv lcton concntton n two AlGAs/GAs htostuctus. Kywods: AlGAs/GAs ntfc, lctonc ngs. ITRODUCTIO In AlGAs/GAs htostuctus, two dmnsonl lcton gs (DEG s fomd n th GAs chnnl n th AlGAs/GAs ntfc []. In th pln of th DEG, lctons hv hgh moblty nd hgh concntton chng cm []. Thos lcton chctstcs usd n th fbcton of hgh spd optolctonc dvcs. Mo sophstclly dvc ngnng qus n ccut knowldg of subbnds stuctu nd Fm s lvl loclston. In AlGAs/GAs htostuctus, lctonc stuctus oftn numclly clcultd usng slf consstnt soluton of Schödng nd Posson qutons [-8] o usng SILVACO Mcuy softw. In thotcl bnd stuctu clculton, th GAs conducton bnd bndng n th AlGAs/GAs ntfc s oftn gnod, nd tngul potntl s consdd [9]. Schubt nd ll hv ppoxmtd th GAs bnd dg by polygonl cuv [] nd th lcton ngy s clcultd by mtchng th lcton D Bogl wv lght nd th wdth of th tngul wll. In ths pp, w show tht th tngul potntl ntoducd n th cunt dnsty quton gvs s to sptl dpndnc of th lctonc concntton whch cn b ppoxmtd by ln functon ntfc. Th soluton of th Posson quton gvs s to n ppoxmtd potntl V ( b. Th ln tm s fst consdd n th Schödng quton nd th lctonc ngs nd wv functons clcultd n th bsc of th ffctv mss ppoxmton. Th qudtc tm s ttd s tm ndpndnt ptubton nd th lctonc ngs coctd to th fst od. Th confgutons of occupd subbnds ltd to th Fm ngy. Ths ngy s clcultd fo dffnt concntton of th two dmnsonl lcton gs. Elctcl fld nd potntl xpssons n th AlGAs/GAs ntfc: th AlGAs/GAs ntfc, ln potntl V ( s oftn consdd. By wtng th cunt-dnsty nd th Posson qutons, w wll cy th lctcl fld nd potntl xpssons. Th cunt-dnsty quton fo lctons n th GAs chnnl s: n DEG E µ D ndeg E s th lctcl fld. n DEG,, µ nd D lcton concntton, chg, moblty nd dft coffcnt spctvly. Th soluton of quton gvs: dpndng of th dstnc to th AlGAs/GAs Cospondng Autho: Abdl MEFTAH, Fculty of Scncs of Tuns, Unvsty cmpus, 9 El Mn, Tuns 45

2 Am. J. Appld Sc., 5 (4: 45-49, 8 µ D n DEG ( ndeg ( Fo wk vlu of, on cn wt: n DEG ( α ( µ Wh ndeg ( D α nd s th D µ flt bnd bgnnng bscs. In th two dmnsonl lcton gs ppoxmton, ll lctons supposd to b n th ntfc pln wh th lcton concntton s n DEG. W cn wt: n DEG n DEG ( d n Ths gvs: α DEG Th soluton of th Posson quton gvs: α E( ( α nd V ( ( 6 Wh s th GAs dlctc-pmttvty constnt To th fst od ppoxmton w hv n V α ( DEG, thn ndeg. To th scond od ppoxmton, th potntl s: V ( b V ( s constnt fo, thn b Subbnd ngs n th tngul potntl: In th bsc of th ffctv mss ppoxmton, th Schödng quton n th GAs chnnl s: P ( // m// P m GAs E g ( E ( ψ ( ψ ( P //, m // nd P, m lcton momntum nd ffctv mss n th dctons plll nd GAs ppndcul to th ntfc spctvly. E g s th GAs bnd gp. In lttu, no dffnc btwn th ffctv msss m // nd m w potd, w thn wt: m // m m Th clculus of th wv functons nd ngs gvn n th ppndx. Th wv functon s ψ k // S // ϕ(, wh k // nd // ( th wv nd poston vctos plll to th ntfc spctvly. m ϕ ( s th Ay functon (( A ( h GAs h k// nd th ngy s E Eg wth m π h ndeg ( ( (.75 ( m Wh,,,... Fo m.67 * m nd *8.85* SI s gvn by:, th ngy ( mv 6 ( mv.997 * ndeg (.75 (4 Wh n DEG s xpssd n cm W msmtch th subbnd ngs clcultd by th xpsson (4 nd thos found n lttu, fo th DEG concntton n DEG 5. cm. Th ngs nd of th fundmntl nd th fst xctd lvls spctvly gvn n tbl. Engy cocton: Th fst od cocton of th ngy s: 46

3 Am. J. Appld Sc., 5 (4: 45-49, 8 Tbl : Engs nd of th fundmntl nd fst xctd lvls n th tngul potntl of th AlGAs/GAs htostuctu. Th fst ow shows ngs gvn by ths wok. Th oth ows show ngs found n lttu. Rfncs Engs Ths wok [] [9] [] [] [,] [4] ( mv ( mv Tbl : α nd β vlus, nd fundmntl nd 5 fst xctd lvls ngs bfo nd ft coctons fo n DEG 5* cm nd 5. Α 4 5 α β (mv ( ( mv ϕ b ϕ (5 ϕ ϕ m Wh ( Z ( h { n DEG α n DEG { h β ( m } h α ( m I I Wh α, β, I A I I dz, ZA ( Z dz nd I I, ltd to I t, I Z A dz I clcultd by comput. n DEG nd by: s β.77* n } DEG, n DEG nd xpssd n mv spctvly. Fo n DEG 5* cm nd 5 Α Α, cm nd th α nd β coffcnts nd th coctd ngs fo th fundmntl nd th fv fst xctd lvls gvn n tbl. Th volutons wth n DEG of th ngs nd fo, nd psntd n fgu. Fo ch lvl, th ngy cocton s ngtv, ts bsolut vlu ncss wth ncsng n DEG. 47

4 Am. J. Appld Sc., 5 (4: 45-49, 8 Engy (mv F,E 4,E 6,E 8,E n DEG Fg. : Evoluton wth n DEG of th fundmntl, two fst xctd nd Fm lvls ngs bfo nd ft th cocton. Th volutons wth th wll wdth of th ngy cocton fo th th lvls psntd n fgu. Fo wk vlu, th bnd bndng s mo ponouncd n th AlGAs/GAs ntfc, th ln potntl ppoxmton s nsuffcnt nd th ngy cocton fo ch lvl s mpotnt. Fo lg vlu, th potntl s goously ln n th AlGAs/GAs ntfc nd th ngy cocton s wk. Engy (mv (b (c ( F m n ( DEG Log (6 Wh T nd K tmptu nd Boltmn constnt. n DEG could b wttn: n DEG F m Log( ( m LogA π (7 Wh A ( F (...( Wth nd s th ngy of th upp confnd lvl Th condton > s oftn stsfd, thus s wk nd w cn ppoxmt A to th scond od n nd wt: A (... W put: α j nd (8 β ( (9 j j Th qutons (8 nd (9 gv: ndeg m α β A Th soluton of gvs: Z (Angstom Fg. : Evoluton wth th potntl-wll wdth of th ngy coctons of th fundmntl (, th fst (b nd scond (c xctd lvls Th Fm ngy: Th ov ll lcton concntton n th two dmnsonl lcton gs s gvn by [5] : 48 n j DEG m ( 4( ( j j F Log j ( j j Th Fm ngy F s clcultd by comput. Th voluton of F wth n DEG s shown n fgu. Th fundmntl lvl s popultd fo

5 Am. J. Appld Sc., 5 (4: 45-49, 8 n DEG > 6.* cm. Th fst xctd lvl s popultd fo n DEG > 4.8* cm. Th n DEG cn b ltd to th dopng concntton, whch choc lds to th dsd confguton of th occupd subbnds. COCLUSIO In GAs chnnl nd n th AlGAs/GAs ntfc, th potntl s ppoxmtd by th xpsson V ( b. Th qudtc tm s wk compd to th ln on. To fst ppoxmton th potntl s tngul. Th subbnd ngs nd wv functons xctly clcultd n th bsc of th ffctv mss ppoxmton. Th qudtc tm s consdd s tm ndpndnt ptubton, nd ngs coctd to th fst od. Th clcultd subbnd ngs g wll wth tht found n lttu. Th Fm ngy s clcultd fo dffnt concnttons n DEG of th two dmnsonl lcton gs. Th concntton n DEG cn b ltd to dopng concntton, thus th dsd confguton of th occupd subbnds wll b obtnd by th choc of th dopng concntton. REFERECES. Stöm, L. H., R. Dngl, A. C. Gossd, W. Wgmn nd M. D. Stug, 98. TWO DIMESIOA L ELECTRO GAS AT SEMICODUCTOR-SEMICODUCTOR ITERFACE. Sold. Stt. Com., 9: Shubt, E. F., J. E. Cunnghm nd W. T. Tsng, 987. Elcton-Moblty Enhncmnt nd Elcton concntton Enhncmnt n δ-dopd n- GAs t K. Sold. Stt. Com., 6: Stn, F.nd S. Ds Sm, 984. Elcton ngy lvls n GAs-G -x Al x As htojunctons. Phys. Rv. B, : Tn, I. H., G. L Snd, L. D. Chng, nd E. L Hu, 99. A slf-consstnt soluton of Schödng- Posson qutons usng nonunfom msh. J. App. Phys., 68 (8: Boun, L., L. Sfx, H. Sgh.nd H. Mf, 999., Impovmnt of th lcton dnsty n th chnnl of n AlGAs/GAs htojuncton by ntoducng S dopng n th quntum wll. J. Appl. Phys., 85 : Aloulou, S., H. Ajln, A. Mfth, M. Ouslt, L. Sfx nd H. Mf,. Elcton confnmnt n pln dopd htostuctu G - xal x As:S/GAs. Mtl Scncs nd ngnng B, 96: Sngh, R., C. M. Snowd, 999. A chg contol HEMT modl ncopotng dp lvl ffcts,.sold. Stt.. Elctoncs, 4: Ajln, H., A. Mfth, R. Chtouou, M. Ouslt nd H. Mf, 6. Photolumnscnc studs of confnd stts n AlGAs/GAs symmtc quntum wll. Physc E, : Ando, T., A. B. Fowl nd F. Stn, 98. Elctonc popts of two-dmnsonl systms. Rv. Mod. Phys., 54 (: Schubt, E. F., 985. Elcton Subbnd Stuctu n Slctvly Dopd n-al x G -x As/GAs Htostuctus. IEEE Tns. Elcton Dvcs ED-, 9: Ando, T., 98. Slf-Consstnt Rsults fo GAs/Al x G -x As Htojuncton Subbnd Stuctu nd Lght-Scttng Spct. J. Phys. Soc. Jpn, 5: Stn, F., 98. Dopng consdton fo htojunctons. Appl. Phys. Ltt., 4: Dlgbuduf, D. nd. T. Lhn, 98. Mtl- (n AlGAs-GAs two-dmnsonl lcton gs FET. IEEE Tns. Elcton Dvc, ED-9: Mthu, H., 998. Physqu ds smconductus t ds composnts élctonqus. Edton MASSO, Ps, Qutèm édton, pp:5. 49

3. Anomalous magnetic moment

3. Anomalous magnetic moment 3. Anolos gntc ont 3.1 Mgntc ont of th lcton: Dc qton wth lcton colng to lcto-gntc t fld: D A A D ψ 0 cnoncl ont Anstz fo th solton s fo f tcl: t t Χ Φ Φ Χ 0 A 0 A Χ Φ 0 Χ Φ χ ϕ x x 4 Non-ltvstc lt: E,

More information

Chapter 5. Atomic structure

Chapter 5. Atomic structure Cpt 5. Atomc tuctu I. Hydognc tom H, H, L nuclu ngl - pct of ydogn tom Wvnumb: ~ ν ν cm - λ c ν: fquncy -, Hz λ: wvlngt nm c: pd of lgt 3. 8 m/ Rydbg fomul: ~ ν RH R H 9677 cm - Rydbg contnt n n n, n >

More information

CIVL 7/ D Boundary Value Problems - Axisymmetric Elements 1/8

CIVL 7/ D Boundary Value Problems - Axisymmetric Elements 1/8 CIVL 7/8 -D Bounday Valu Poblms - xsymmtc Elmnts /8 xsymmtc poblms a somtms fd to as adally symmtc poblms. hy a gomtcally th-dmnsonal but mathmatcally only two-dmnsonal n th physcs of th poblm. In oth

More information

Mathematical model of Unemployment- an analysis with delay

Mathematical model of Unemployment- an analysis with delay Globl Jounl of Mthmtcl Scncs: Thoy nd Pctcl. ISSN 97- Volum 9 Numb 7 pp. 5-7 Intntonl Rsch Publcton Hous http://www.phous.com Mthmtcl modl of Unmploymnt- n nlyss wth dly Gulbnu Pthn P.H.Bhthwl Sttstcl

More information

5- Scattering Stationary States

5- Scattering Stationary States Lctu 19 Pyscs Dpatmnt Yamou Unvsty 1163 Ibd Jodan Pys. 441: Nucla Pyscs 1 Pobablty Cunts D. Ndal Esadat ttp://ctaps.yu.du.jo/pyscs/couss/pys641/lc5-3 5- Scattng Statonay Stats Rfnc: Paagaps B and C Quantum

More information

Lecture on Thursday, March 22, 2007 Instructor Dr. Marina Y. Koledintseva ELECTROMAGNETIC THEOREMS

Lecture on Thursday, March 22, 2007 Instructor Dr. Marina Y. Koledintseva ELECTROMAGNETIC THEOREMS Lctu on Thusdy, Mch, 7 Instucto D Mn Y Koldntsv ELECTROMAGNETIC THEOREM Intoducton Th fundntl thos of thtcl physcs ppld to clsscl lctognts pncpl of dulty; g pncpl; sufc uvlnc tho (Lov/chlkunoff s foulton);

More information

C-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0)

C-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0) An ltntiv to th us of hypolic dclin cuvs Ppd y: Sfim Ltd S E R A F I M info@sfimltd.com P. +44 (02890 4206 www.sfimltd.com Contnts Contnts... i Intoduction... Initil ssumptions... Solving fo cumultiv...

More information

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find BSE SMLE ER SOLUTONS LSS-X MTHS SET- BSE SETON Gv tht d W d to fd 7 7 Hc, 7 7 7 Lt, W ow tht Thus, osd th vcto quto of th pl z - + z = - + z = Thus th ts quto of th pl s - + z = Lt d th dstc tw th pot,,

More information

Handout 7. Properties of Bloch States and Electron Statistics in Energy Bands

Handout 7. Properties of Bloch States and Electron Statistics in Energy Bands Hdout 7 Popts of Bloch Stts d Elcto Sttstcs Eg Bds I ths lctu ou wll l: Popts of Bloch fuctos Podc boud codtos fo Bloch fuctos Dst of stts -spc Elcto occupto sttstcs g bds ECE 407 Spg 009 Fh R Coll Uvst

More information

Massachusetts Institute of Technology Introduction to Plasma Physics

Massachusetts Institute of Technology Introduction to Plasma Physics Massachustts Insttut of Tchnology Intoducton to Plasma Physcs NAME 6.65J,8.63J,.6J R. Pak Dcmb 5 Fnal Eam :3-4:3 PM NOTES: Th a 8 pags to th am, plus on fomula sht. Mak su that you copy s complt. Each

More information

Hetero- and low-dimensional structures. Impact of semiconductor quantum dots bandgap on reabsorption in luminescent concentrator

Hetero- and low-dimensional structures. Impact of semiconductor quantum dots bandgap on reabsorption in luminescent concentrator Smconducto Pyscs, Quntum lctoncs & Optolctoncs, 8. V., N. P.58-64. Hto- nd low-dmnsonl stuctus Impct of smconducto quntum dots ndgp on sopton n lumnscnt concntto A.I. Skt, A.V. Scnko, I.O. Sokolovsky,

More information

CBSE , ˆj. cos CBSE_2015_SET-1. SECTION A 1. Given that a 2iˆ ˆj. We need to find. 3. Consider the vector equation of the plane.

CBSE , ˆj. cos CBSE_2015_SET-1. SECTION A 1. Given that a 2iˆ ˆj. We need to find. 3. Consider the vector equation of the plane. CBSE CBSE SET- SECTION. Gv tht d W d to fd 7 7 Hc, 7 7 7. Lt,. W ow tht.. Thus,. Cosd th vcto quto of th pl.. z. - + z = - + z = Thus th Cts quto of th pl s - + z = Lt d th dstc tw th pot,, - to th pl.

More information

Chapter 2 Reciprocal Lattice. An important concept for analyzing periodic structures

Chapter 2 Reciprocal Lattice. An important concept for analyzing periodic structures Chpt Rcpocl Lttc A mpott cocpt o lyzg podc stuctus Rsos o toducg cpocl lttc Thoy o cystl dcto o x-ys, utos, d lctos. Wh th dcto mxmum? Wht s th tsty? Abstct study o uctos wth th podcty o Bvs lttc Fou tsomto.

More information

Chapter-10. Ab initio methods I (Hartree-Fock Methods)

Chapter-10. Ab initio methods I (Hartree-Fock Methods) Chapt- Ab nto mthods I (Hat-Fock Mthods) Ky wods: Ab nto mthods, quantum chmsty, Schodng quaton, atomc obtals, wll bhavd functons, poduct wavfunctons, dtmnantal wavfunctons, Hat mthod, Hat Fock Mthod,

More information

(A) the function is an eigenfunction with eigenvalue Physical Chemistry (I) First Quiz

(A) the function is an eigenfunction with eigenvalue Physical Chemistry (I) First Quiz 96- Physcl Chmstry (I) Frst Quz lctron rst mss m 9.9 - klogrm, Plnck constnt h 6.66-4 oul scon Sp of lght c. 8 m/s, lctron volt V.6-9 oul. Th functon F() C[cos()+sn()] s n gnfuncton of /. Th gnvlu s (A)

More information

Homework: Due

Homework: Due hw-.nb: //::9:5: omwok: Du -- Ths st (#7) s du on Wdnsday, //. Th soluton fom Poblm fom th xam s found n th mdtm solutons. ü Sakua Chap : 7,,,, 5. Mbach.. BJ 6. ü Mbach. Th bass stats of angula momntum

More information

Electromagnetics: The Smith Chart (9-6)

Electromagnetics: The Smith Chart (9-6) Elctomagntcs: Th Smth Chat (9-6 Yoonchan Jong School of Elctcal Engnng, Soul Natonal Unvsty Tl: 8 (0 880 63, Fax: 8 (0 873 9953 Emal: yoonchan@snu.ac.k A Confomal Mappng ( Mappng btwn complx-valud vaabls:

More information

Rate of Molecular Exchange Through the Membranes of Ionic Liquid Filled. Polymersomes Dispersed in Water

Rate of Molecular Exchange Through the Membranes of Ionic Liquid Filled. Polymersomes Dispersed in Water Supportng Informton for: Rt of Molculr Exchng hrough th Mmrns of Ionc Lqud Flld olymrsoms Dsprsd n Wtr Soonyong So nd mothy. Lodg *,, Dprtmnt of Chmcl Engnrng & Mtrls Scnc nd Dprtmnt of Chmstry, Unvrsty

More information

DESIGNING OF GENERALIZED TWO-PLAN SYSTEM WITH REFERENCE SAMPLING PLAN. Department of Statistics, Bharathiar University, Coimbatore,Tamilnadu,India.

DESIGNING OF GENERALIZED TWO-PLAN SYSTEM WITH REFERENCE SAMPLING PLAN. Department of Statistics, Bharathiar University, Coimbatore,Tamilnadu,India. DESIGNING OF GENERALIZED TWO-PLAN SYSTEM WITH REFERENCE SAMPLING PLAN 1 K. K. Sush nd K. Vnth Xv 2 1 Pofsso nd Hd of th Dptmnt Dptmnt of Sttstcs, Bhth Unvsty, Combto,Tmlndu,Ind. 2 Rsch Schol, Dptmnt of

More information

Statics. Consider the free body diagram of link i, which is connected to link i-1 and link i+1 by joint i and joint i-1, respectively. = r r r.

Statics. Consider the free body diagram of link i, which is connected to link i-1 and link i+1 by joint i and joint i-1, respectively. = r r r. Statcs Th cotact btw a mapulato ad ts vomt sults tactv ocs ad momts at th mapulato/vomt tac. Statcs ams at aalyzg th latoshp btw th actuato dv tous ad th sultat oc ad momt appld at th mapulato dpot wh

More information

Transient Thermal Stress Problem of a Functionally Graded Magneto-Electro-Thermoelastic Hollow Sphere

Transient Thermal Stress Problem of a Functionally Graded Magneto-Electro-Thermoelastic Hollow Sphere Mtls 6-5; o:.9/m6 Atcl OPE AESS mtls ISS 996-9 www.mp.com/ounl/mtls Tnsnt Thml Stss Polm of Functonlly G Mnto-Elcto-Thmolstc Hollow Sph Yoshho Ooto * n Msyuk Ishh Dptmnt of Mchncl Ennn Gut School of Ennn

More information

CHARACTERISTICS OF MAGNETICALLY ENHANCED CAPACITIVELY COUPLED DISCHARGES*

CHARACTERISTICS OF MAGNETICALLY ENHANCED CAPACITIVELY COUPLED DISCHARGES* CHARACTERISTICS OF MAGNETICALLY ENHANCED CAPACITIVELY COUPLED DISCHARGES* Alx V. Vasnkov and Mak J. Kushn Unvsty of Illnos 1406 W. Gn St. Ubana, IL 61801 vasnkov@uuc.du k@uuc.du http://uglz.c.uuc.du Octob

More information

A general N-dimensional vector consists of N values. They can be arranged as a column or a row and can be real or complex.

A general N-dimensional vector consists of N values. They can be arranged as a column or a row and can be real or complex. Lnr lgr Vctors gnrl -dmnsonl ctor conssts of lus h cn rrngd s column or row nd cn rl or compl Rcll -dmnsonl ctor cn rprsnt poston, loct, or cclrton Lt & k,, unt ctors long,, & rspctl nd lt k h th componnts

More information

Degenerate Clifford Algebras and Their Reperesentations

Degenerate Clifford Algebras and Their Reperesentations BAÜ Fn Bl. Enst. Dgs t 8-8 Dgnt ffod Algbs nd Th Rsnttons Şny BULUT * Andolu Unvsty Fculty of Scnc Dtmnt of Mthmtcs Yunum Cmus Eskşh. Abstct In ths study w gv n mbddng thom fo dgnt ffod lgb nto nondgnt

More information

Path (space curve) Osculating plane

Path (space curve) Osculating plane Fo th cuilin motion of pticl in spc th fomuls did fo pln cuilin motion still lid. But th my b n infinit numb of nomls fo tngnt dwn to spc cu. Whn th t nd t ' unit ctos mod to sm oigin by kping thi ointtions

More information

( V ) 0 in the above equation, but retained to keep the complete vector identity for V in equation.

( V ) 0 in the above equation, but retained to keep the complete vector identity for V in equation. Cuvlna Coodnats Outln:. Otogonal cuvlna coodnat systms. Dffntal opatos n otogonal cuvlna coodnat systms. Dvatvs of t unt vctos n otogonal cuvlna coodnat systms 4. Incompssbl N-S quatons n otogonal cuvlna

More information

The Random Phase Approximation:

The Random Phase Approximation: Th Random Phas Appoxmaton: Elctolyts, Polym Solutons and Polylctolyts I. Why chagd systms a so mpotant: thy a wat solubl. A. bology B. nvonmntally-fndly polym pocssng II. Elctolyt solutons standad dvaton

More information

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

E 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 information

D. Bertsekas and R. Gallager, "Data networks." Q: What are the labels for the x-axis and y-axis of Fig. 4.2?

D. Bertsekas and R. Gallager, Data networks. Q: What are the labels for the x-axis and y-axis of Fig. 4.2? pd by J. Succ ECE 543 Octob 22 2002 Outl Slottd Aloh Dft Stblzd Slottd Aloh Uslottd Aloh Splttg Algoths Rfc D. Btsks d R. llg "Dt twoks." Rvw (Slottd Aloh): : Wht th lbls fo th x-xs d y-xs of Fg. 4.2?

More information

A New Generalization of Quadratic Hazard Rate Distribution

A New Generalization of Quadratic Hazard Rate Distribution A Nw Gnlzton of Qudtc Hzd Rt Dstuton Ihm Eltl Insttut of Sttstcl Studs nd Rsch Dptmnt of Mthmtcl Sttstcs, Co Unvsty _ltl@stff.cu.du.g Ndm Shfqu Butt COMSATS Insttut of Infomton Tchnology, Lho ndmshfqu@ctlho.du.pk

More information

Preview. Graph. Graph. Graph. Graph Representation. Graph Representation 12/3/2018. Graph Graph Representation Graph Search Algorithms

Preview. Graph. Graph. Graph. Graph Representation. Graph Representation 12/3/2018. Graph Graph Representation Graph Search Algorithms /3/0 Prvw Grph Grph Rprsntton Grph Srch Algorthms Brdth Frst Srch Corrctnss of BFS Dpth Frst Srch Mnmum Spnnng Tr Kruskl s lgorthm Grph Drctd grph (or dgrph) G = (V, E) V: St of vrt (nod) E: St of dgs

More information

Convergence tests for the cluster DFT calculations

Convergence tests for the cluster DFT calculations Covgc ss o h clus DF clculos. Covgc wh spc o bss s. s clculos o bss s covgc hv b po usg h PBE ucol o 7 os gg h-b. A s o h Guss bss ss wh csg s usss hs b us clug h -G -G** - ++G(p). A l sc o. Å h c bw h

More information

Grand Canonical Ensemble

Grand Canonical Ensemble Th nsmbl of systms mmrsd n a partcl-hat rsrvor at constant tmpratur T, prssur P, and chmcal potntal. Consdr an nsmbl of M dntcal systms (M =,, 3,...M).. Thy ar mutually sharng th total numbr of partcls

More information

Load Equations. So let s look at a single machine connected to an infinite bus, as illustrated in Fig. 1 below.

Load Equations. So let s look at a single machine connected to an infinite bus, as illustrated in Fig. 1 below. oa Euatons Thoughout all of chapt 4, ou focus s on th machn tslf, thfo w wll only pfom a y smpl tatmnt of th ntwok n o to s a complt mol. W o that h, but alz that w wll tun to ths ssu n Chapt 9. So lt

More information

Appendix A2 - Derivation of the Neutron-Proton Capture Cross- Sections In This Universe

Appendix A2 - Derivation of the Neutron-Proton Capture Cross- Sections In This Universe Rc s Cosmology Tutol: Andx A - Dvton of th Nuton-Poton Ctu Coss-Sctons In Ths Unvs Andx A - Dvton of th Nuton-Poton Ctu Coss- Sctons In Ths Unvs. Intoducton In ths Andx w dv th coss-scton fo nuton ctu

More information

IFYFM002 Further Maths Appendix C Formula Booklet

IFYFM002 Further Maths Appendix C Formula Booklet Ittol Foudto Y (IFY) IFYFM00 Futh Mths Appd C Fomul Booklt Rltd Documts: IFY Futh Mthmtcs Syllbus 07/8 Cotts Mthmtcs Fomul L Equtos d Mtcs... Qudtc Equtos d Rmd Thom... Boml Epsos, Squcs d Ss... Idcs,

More information

A Velocity Extraction Method in Molecular Dynamic Simulation of Low Speed Nanoscale Flows

A Velocity Extraction Method in Molecular Dynamic Simulation of Low Speed Nanoscale Flows Int. J. Mol. Sc. 006, 7, 405-416 Intnatonal Jounal of Molcula Scncs ISSN 14-0067 006 by MDPI www.mdp.og/ms/ A Vlocty Extacton Mthod n Molcula Dynamc Smulaton of Low Spd Nanoscal Flows Wnf Zhang School

More information

Minimum Spanning Trees

Minimum Spanning Trees Mnmum Spnnng Trs Spnnng Tr A tr (.., connctd, cyclc grph) whch contns ll th vrtcs of th grph Mnmum Spnnng Tr Spnnng tr wth th mnmum sum of wghts 1 1 Spnnng forst If grph s not connctd, thn thr s spnnng

More information

Convergence Theorems for Two Iterative Methods. A stationary iterative method for solving the linear system: (1.1)

Convergence Theorems for Two Iterative Methods. A stationary iterative method for solving the linear system: (1.1) Conrgnc Thors for Two Itrt Mthods A sttonry trt thod for solng th lnr syst: Ax = b (.) ploys n trton trx B nd constnt ctor c so tht for gn strtng stt x of x for = 2... x Bx c + = +. (.2) For such n trton

More information

Special Random Variables: Part 1

Special Random Variables: Part 1 Spcl Rndom Vrbls: Prt Dscrt Rndom Vrbls Brnoull Rndom Vrbl (wth prmtr p) Th rndom vrbl x dnots th succss from trl. Th probblty mss functon of th rndom vrbl X s gvn by p X () p X () p p ( E[X ]p Th momnt

More information

Role of NMDA conductance in average firing rate shifts caused by external periodic forcing. Nikita Novikov 1 and Boris Gutkin 1,2 1 ABSTRACT

Role of NMDA conductance in average firing rate shifts caused by external periodic forcing. Nikita Novikov 1 and Boris Gutkin 1,2 1 ABSTRACT Rol of conductnc n vg fng t shfts cusd by xtnl podc focng Nkt Novkov 1 nd Bos Gutkn 1,2 1 Cnt fo Cognton nd Dcson Mkng, Ntonl Rsch Unvsty Hgh School of Economcs, Moscow, Ru, 101000 2 Goup fo Nul Thoy,

More information

CERTAIN RESULTS ON TIGHTENED-NORMAL-TIGHTENED REPETITIVE DEFERRED SAMPLING SCHEME (TNTRDSS) INDEXED THROUGH BASIC QUALITY LEVELS

CERTAIN RESULTS ON TIGHTENED-NORMAL-TIGHTENED REPETITIVE DEFERRED SAMPLING SCHEME (TNTRDSS) INDEXED THROUGH BASIC QUALITY LEVELS Intnatonal Rsach Jounal of Engnng and Tchnology (IRJET) -ISSN: 2395-0056 Volum: 03 Issu: 02 Fb-2016 www.jt.nt p-issn: 2395-0072 CERTAIN RESULTS ON TIGHTENED-NORMAL-TIGHTENED REPETITIVE DEFERRED SAMPLING

More information

Lecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9

Lecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9 Lctur contnts Bloch thorm -vctor Brillouin zon Almost fr-lctron modl Bnds ffctiv mss Hols Trnsltionl symmtry: Bloch thorm On-lctron Schrödingr qution ch stt cn ccommo up to lctrons: If Vr is priodic function:

More information

DMC Based on Weighting Correction of Predictive Model Errors

DMC Based on Weighting Correction of Predictive Model Errors ELKOIK Vol o 4 l 9 ~ -ISS: 87-78X 9 DC Bsd on Wgtng Cocton of dctv odl Eos L n* Sn ong X Fngng Wng o Scool of Elctcl Engnng & Infoton otst tol nvst Dqng Olfld Con Dvlont Stt 99#Go xn Dstct 68 *Cosondng

More information

SAMPLE LITANY OF THE SAINTS E/G. Dadd9/F. Aadd9. cy. Christ, have. Lord, have mer cy. Christ, have A/E. Dadd9. Aadd9/C Bm E. 1. Ma ry and. mer cy.

SAMPLE LITANY OF THE SAINTS E/G. Dadd9/F. Aadd9. cy. Christ, have. Lord, have mer cy. Christ, have A/E. Dadd9. Aadd9/C Bm E. 1. Ma ry and. mer cy. LTNY OF TH SNTS Cntrs Gnt flwng ( = c. 100) /G Ddd9/F ll Kybrd / hv Ddd9 hv hv Txt 1973, CL. ll rghts rsrvd. Usd wth prmssn. Musc: D. Bckr, b. 1953, 1987, D. Bckr. Publshd by OCP. ll rghts rsrvd. SMPL

More information

Ch 1.2: Solutions of Some Differential Equations

Ch 1.2: Solutions of Some Differential Equations Ch 1.2: Solutions of Som Diffrntil Equtions Rcll th fr fll nd owl/mic diffrntil qutions: v 9.8.2v, p.5 p 45 Ths qutions hv th gnrl form y' = y - b W cn us mthods of clculus to solv diffrntil qutions of

More information

b.) v d =? Example 2 l = 50 m, D = 1.0 mm, E = 6 V, " = 1.72 #10 $8 % & m, and r = 0.5 % a.) R =? c.) V ab =? a.) R eq =?

b.) v d =? Example 2 l = 50 m, D = 1.0 mm, E = 6 V,  = 1.72 #10 $8 % & m, and r = 0.5 % a.) R =? c.) V ab =? a.) R eq =? xmpl : An 8-gug oppr wr hs nomnl mtr o. mm. Ths wr rrs onstnt urrnt o.67 A to W lmp. Th nsty o r ltrons s 8.5 x 8 ltrons pr u mtr. Fn th mgntu o. th urrnt nsty. th rt vloty xmpl D. mm,.67 A, n N 8.5" 8

More information

Part II, Measures Other Than Conversion I. Apr/ Spring 1

Part II, Measures Other Than Conversion I. Apr/ Spring 1 Pt II, Msus Oth hn onvsion I p/7 11 Sping 1 Pt II, Msus Oth hn onvsion II p/7 11 Sping . pplictions/exmpls of th RE lgoithm I Gs Phs Elmnty Rction dditionl Infomtion Only fd P = 8. tm = 5 K =. mol/dm 3

More information

Laboratory of Physics and Material Chemistry, Physics Department, Sciences Faculty, University of M'sila-M sila Algeria * a

Laboratory of Physics and Material Chemistry, Physics Department, Sciences Faculty, University of M'sila-M sila Algeria * a Intnatonal Font Scnc Ltts Submttd: 7--5 ISSN: 49-4484, Vol., pp 9-44 Accptd: 7--4 do:.85/www.scpss.com/ifsl..9 Onln: 7--8 7 ScPss Ltd., Swtzl Invstgatons on th Rlatvstc Intactons n On-lcton Atoms wth Modfd

More information

Boyce/DiPrima 9 th ed, Ch 7.6: Complex Eigenvalues

Boyce/DiPrima 9 th ed, Ch 7.6: Complex Eigenvalues BocDPm 9 h d Ch 7.6: Compl Egvlus Elm Dffl Equos d Boud Vlu Poblms 9 h do b Wllm E. Boc d Rchd C. DPm 9 b Joh Wl & Sos Ic. W cosd g homogous ssm of fs od l quos wh cos l coffcs d hus h ssm c b w s ' A

More information

Verification of a Complete Pore Network Simulator of Drainage and Imbibition

Verification of a Complete Pore Network Simulator of Drainage and Imbibition Vfcton of Complt Po Ntwok Smulto of Dng nd Imbbton Td W. Ptzk, SPE, U. of Clfon, Bkly Summy Rltv-pmblty nd cplly-pssu functons dfn how much ol cn b covd nd t wht t. Ths functons, n tun, dpnd ctclly on

More information

glo beau bid point full man branch last ior s all for ap Sav tree tree God length per down ev the fect your er Cm7 a a our

glo beau bid point full man branch last ior s all for ap Sav tree tree God length per down ev the fect your er Cm7 a a our SING, MY TONGU, TH SAVIOR S GLORY mj7 Mlod Kbd fr nd S would tm flsh s D nd d tn s drw t crd S, Fth t So Th L lss m ful wn dd t, Fs4 F wd; v, snr, t; ngh, t: lod; t; tgu, now Chrst, h O d t bnd Sv God

More information

Winnie flies again. Winnie s Song. hat. A big tall hat Ten long toes A black magic wand A long red nose. nose. She s Winnie Winnie the Witch.

Winnie flies again. Winnie s Song. hat. A big tall hat Ten long toes A black magic wand A long red nose. nose. She s Winnie Winnie the Witch. Wnn f gn ht Wnn Song A g t ht Tn ong to A k g wnd A ong d no. no Sh Wnn Wnn th Wth. y t d to A ong k t Bg gn y H go wth Wnn Whn h f. wnd ootk H Wu Wu th t. Ptu Dtony oo hopt oon okt hng gd ho y ktod nh

More information

Analysis of a M/G/1/K Queue with Vacations Systems with Exhaustive Service, Multiple or Single Vacations

Analysis of a M/G/1/K Queue with Vacations Systems with Exhaustive Service, Multiple or Single Vacations Analyss of a M/G// uu wth aatons Systms wth Ehaustv Sv, Multpl o Sngl aatons W onsd h th fnt apaty M/G// uu wth th vaaton that th sv gos fo vaatons whn t s dl. Ths sv modl s fd to as on povdng haustv sv,

More information

( ) + is the distance from the point of interest to the location of the charge q i

( ) + is the distance from the point of interest to the location of the charge q i Elctcal Engy and apactanc 57. Bcaus lctc ocs a consvatv, th kntc ngy gand s qual to th dcas n lctcal potntal ngy, o + + 4 4 KE PE q( ).. so th coct choc s (a).. Fom consvaton o ngy, KE + PE KE + PE, o

More information

1 Vectors & Tensors tensor

1 Vectors & Tensors tensor Vctos & nsos h mthmtcl modln of th physcl wold qs nowld of qt fw dffnt mthmtcs sbcts sch s Clcls Dffntl Eqtons nd Ln lb. hs topcs slly ncontd n fndmntl mthmtcs coss. How n mo thooh nd n-dpth ttmnt of mchncs

More information

External Equivalent. EE 521 Analysis of Power Systems. Chen-Ching Liu, Boeing Distinguished Professor Washington State University

External Equivalent. EE 521 Analysis of Power Systems. Chen-Ching Liu, Boeing Distinguished Professor Washington State University xtrnal quvalnt 5 Analyss of Powr Systms Chn-Chng Lu, ong Dstngushd Profssor Washngton Stat Unvrsty XTRNAL UALNT ach powr systm (ara) s part of an ntrconnctd systm. Montorng dvcs ar nstalld and data ar

More information

8. Linear Contracts under Risk Neutrality

8. Linear Contracts under Risk Neutrality 8. Lnr Contrcts undr Rsk Nutrlty Lnr contrcts r th smplst form of contrcts nd thy r vry populr n pplctons. Thy offr smpl ncntv mchnsm. Exmpls of lnr contrcts r mny: contrctul jont vnturs, quty jont vnturs,

More information

Radial Cataphoresis in Hg-Ar Fluorescent Lamp Discharges at High Power Density

Radial Cataphoresis in Hg-Ar Fluorescent Lamp Discharges at High Power Density [NWP.19] Radal Cataphorss n Hg-Ar Fluorscnt Lamp schargs at Hgh Powr nsty Y. Aura, G. A. Bonvallt, J. E. Lawlr Unv. of Wsconsn-Madson, Physcs pt. ABSTRACT Radal cataphorss s a procss n whch th lowr onzaton

More information

Integration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals

Integration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals Intgrtion Continud Intgrtion y Prts Solving Dinit Intgrls: Ar Undr Curv Impropr Intgrls Intgrtion y Prts Prticulrly usul whn you r trying to tk th intgrl o som unction tht is th product o n lgric prssion

More information

TOPIC 5: INTEGRATION

TOPIC 5: INTEGRATION TOPIC 5: INTEGRATION. Th indfinit intgrl In mny rspcts, th oprtion of intgrtion tht w r studying hr is th invrs oprtion of drivtion. Dfinition.. Th function F is n ntidrivtiv (or primitiv) of th function

More information

Filter Design Techniques

Filter Design Techniques Fltr Dsgn chnqus Fltr Fltr s systm tht psss crtn frquncy componnts n totlly rcts ll othrs Stgs of th sgn fltr Spcfcton of th sr proprts of th systm ppromton of th spcfcton usng cusl scrt-tm systm Rlzton

More information

OPTICAL DESIGN. FIES fibre assemblies B and C. of the. LENS-TECH AB Bo Lindberg Document name: Optical_documentation_FIES_fiber_BC_2

OPTICAL DESIGN. FIES fibre assemblies B and C. of the. LENS-TECH AB Bo Lindberg Document name: Optical_documentation_FIES_fiber_BC_2 OPTICAL DESIGN f h FIES fb ssmbs B d C LENS-TECH AB B Ldbg 2-4-3 Dcm m: Opc_dcm_FIES_fb_BC_2 Idc Ths p s dcm f h pc dsg f h FIES fb ssmbs B d C Th mchc dsg s shw I s shw h ssmb dwg md b Ahs Uvs Fb c Th

More information

8-node quadrilateral element. Numerical integration

8-node quadrilateral element. Numerical integration Fnt Elmnt Mthod lctur nots _nod quadrlatral lmnt Pag of 0 -nod quadrlatral lmnt. Numrcal ntgraton h tchnqu usd for th formulaton of th lnar trangl can b formall tndd to construct quadrlatral lmnts as wll

More information

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals Hydogn atom Engy lvls and wav functions Obital momntum, lcton spin and nucla spin Fin and hypfin intaction Hydogn obitals Hydogn atom A finmnt of th Rydbg constant: R ~ 109 737.3156841 cm -1 A hydogn mas

More information

Scalability of Network-Failure Resilience

Scalability of Network-Failure Resilience Scllty of Ntwo-Flu Rslnc Gungl Lu nd Chuny J, Sno Mm Astct In ths wo w quntfy scllty of ntwo slnc upon flus. W chctz slnc s th pcntg of lost tffc upon flus [5] nd dfn scllty s th gowth t of th pcntg of

More information

CHAPTER TWO MULTIPLE INTEGRAL

CHAPTER TWO MULTIPLE INTEGRAL CHAPTE TWO MULTIPLE INTEGAL Aft complting ths tutoils, stunts shoul b bl to: vlut th oubl intgl ov th givn ctngul gion fin th volum of th soli boun b th plns fin th of th gion boun b th cuvs ug oubl intgl

More information

Applications of Lagrange Equations

Applications of Lagrange Equations Applcaton of agang Euaton Ca Stuy : Elctc Ccut ng th agang uaton of oton, vlop th athatcal ol fo th ccut hown n Fgu.Sulat th ult by SIMI. Th ccuty paat a: 0.0 H, 0.00 H, 0.00 H, C 0.0 F, C 0. F, 0 Ω, Ω

More information

Theory of Spatial Problems

Theory of Spatial Problems Chpt 7 ho of Sptil Polms 7. Diffntil tions of iliim (-D) Z Y X Inol si nknon stss componnts:. 7- 7. Stt of Stss t Point t n sfc ith otd noml N th sfc componnts ltd to (dtmind ) th 6 stss componnts X N

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 301 Signls & Systms Pf. Mk Fwl Discussin #1 Cmplx Numbs nd Cmplx-Vlud Functins Rding Assignmnt: Appndix A f Kmn nd Hck Cmplx Numbs Cmplx numbs is s ts f plynmils. Dfinitin f imginy # j nd sm sulting

More information

Realistic model for radiation-matter interaction

Realistic model for radiation-matter interaction Ralstc modl fo adaton-m ntacton Rchad A. Pakula Scnc Applcatons Intnatonal Copoaton (SAIC) 41 Noth Fafax D. Sut 45 Alngton VA 3 ABSTRACT Ths pap psnts a alstc modl that dscbs adaton-m ntactons. Ths s achvd

More information

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 2: Derivation of Ideal MHD Equation

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 2: Derivation of Ideal MHD Equation .65, MHD Thory of Fuson Systms Prof. Frdbrg Lctur : Drvton of Idl MHD Equton Rvw of th Drvton of th Momnt Equton. Strtng Pont: Boltzmnn Equton for lctrons, ons nd Mxwll Equtons. Momnts of Boltzmnn Equton:

More information

Uniform Circular Motion

Uniform Circular Motion Unfom Ccul Moton Unfom ccul Moton An object mong t constnt sped n ccle The ntude of the eloct emns constnt The decton of the eloct chnges contnuousl!!!! Snce cceleton s te of chnge of eloct:!! Δ Δt The

More information

ADORO TE DEVOTE (Godhead Here in Hiding) te, stus bat mas, la te. in so non mor Je nunc. la in. tis. ne, su a. tum. tas: tur: tas: or: ni, ne, o:

ADORO TE DEVOTE (Godhead Here in Hiding) te, stus bat mas, la te. in so non mor Je nunc. la in. tis. ne, su a. tum. tas: tur: tas: or: ni, ne, o: R TE EVTE (dhd H Hdg) L / Mld Kbrd gú s v l m sl c m qu gs v nns V n P P rs l mul m d lud 7 súb Fí cón ví f f dó, cru gs,, j l f c r s m l qum t pr qud ct, us: ns,,,, cs, cut r l sns m / m fí hó sn sí

More information

Dynamic Modelling and Simulation of Five Phase Induction Motor

Dynamic Modelling and Simulation of Five Phase Induction Motor ISSN (Pnt : 30 3765 ISSN (Onln: 78 8875 Intnatonal Jounal of Advancd Rsach n Elctcal, Elctoncs and Instuntaton Engnng (An ISO 397: 007 Ctfd Oganzaton ol. 4, Issu 4, Apl 05 Dynac Modllng and Sulaton of

More information

International Journal of Scientific & Engineering Research, Volume 4, Issue 9, September ISSN

International Journal of Scientific & Engineering Research, Volume 4, Issue 9, September ISSN Intntinl Junl f Scintific & Engining Rsch, Vlum, Issu 9, Sptmb- bstct: Jcbin intgl nd Stbility f th quilibium psitin f th cnt f mss f n xtnsibl cbl cnnctd stllits systm in th lliptic bit. Vijy Kum ssistnt

More information

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari snbrg Modl Sad Mohammad Mahd Sadrnhaad Survsor: Prof. bdollah Langar bstract: n ths rsarch w tr to calculat analtcall gnvalus and gnvctors of fnt chan wth ½-sn artcls snbrg modl. W drov gnfuctons for closd

More information

PLANAR KNOTTING MECHANISMS FOR TURKISH HAND WOVEN CARPET

PLANAR KNOTTING MECHANISMS FOR TURKISH HAND WOVEN CARPET PLANAR KNOTTIN ECHANISS OR TURKISH HAND WOVEN CARPET E THEORY O ACHINES INSTRUCTOR:POR.DR.TECH.SCI.RASI ALIZADE ASISTANT:RES.ASST.OZUN SELVI :ROUUP EBER NAES: AHET APAK 7 SERKAN CİLARA DENİZ ÖZÜN 6 LEVENT

More information

Solid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch

Solid 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

Current Status of Orbit Determination methods in PMO

Current Status of Orbit Determination methods in PMO unt ttus of Obit Dtintion thods in PMO Dong Wi, hngyin ZHO, Xin Wng Pu Mountin Obsvtoy, HINEE DEMY OF IENE bstct tit obit dtintion OD thods hv vovd ot ov th st 5 ys in Pu Mountin Obsvtoy. This tic ovids

More information

Solution of Tutorial 5 Drive dynamics & control

Solution of Tutorial 5 Drive dynamics & control ELEC463 Unversty of New South Wles School of Electrcl Engneerng & elecommunctons ELEC463 Electrc Drve Systems Queston Motor Soluton of utorl 5 Drve dynmcs & control 500 rev/mn = 5.3 rd/s 750 rted 4.3 Nm

More information

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28 Chapt 10 Phys 3 Lctu 8 Dffacton Dffacton: gnal Fsnl vs. Faunhof dffacton Sval cohnt oscllatos Sngl-slt dffacton Dffacton Gmald, 1600s: dffacto, dvaton of lght fom lna popagaton Dffacton s a consqunc of

More information

ELEC 351 Notes Set #18

ELEC 351 Notes Set #18 Assignmnt #8 Poblm 9. Poblm 9.7 Poblm 9. Poblm 9.3 Poblm 9.4 LC 35 Nots St #8 Antnns gin nd fficincy Antnns dipol ntnn Hlf wv dipol Fiis tnsmission qution Fiis tnsmission qution Do this ssignmnt by Novmb

More information

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

A L A BA M A L A W R E V IE W A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N

More information

6.6 The Marquardt Algorithm

6.6 The Marquardt Algorithm 6.6 The Mqudt Algothm lmttons of the gdent nd Tylo expnson methods ecstng the Tylo expnson n tems of ch-sque devtves ecstng the gdent sech nto n tetve mtx fomlsm Mqudt's lgothm utomtclly combnes the gdent

More information

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28 Chapt 10 Phys 3 Lctu 8 Dffacton Dffacton: gnal Fsnl vs. Faunhof dffacton Sval cohnt oscllatos Sngl-slt dffacton Dffacton Gmald, 1600s: dffacto, dvaton of lght fom lna popagaton Dffacton s a consqunc of

More information

Chapter 10 DIELECTRICS. Dielectrics

Chapter 10 DIELECTRICS. Dielectrics 86 Dlctcs Chat DILCTRICS Dlctcs : Dlctcs a fct nsulatos. In dlctcs lctons a vy tghtly bound to th atoms so that at odnay tmatus thy do not conduct any lctc cunt. xamls: Solds: glass, ocln; gass: H, N ;

More information

MODELING AND SIMULATION OF THE VECTORIAL CONTROL SYSTEM WHICH CONTAIN AN EXTENDED GOPINATH OBSERVER

MODELING AND SIMULATION OF THE VECTORIAL CONTROL SYSTEM WHICH CONTAIN AN EXTENDED GOPINATH OBSERVER MODEING AND SIMUAION OF HE VECOIA CONO SYSEM WHICH CONAIN AN EXENDED GOPINAH OBSEVE Conlu Mndcu, PhD Aoc, Pof, Unvt of Pton Olpu Stocut, PhD ctu, Unvt of Pton Nd Stocut, PhD At, Unvt of Pton ABSAC: h pp

More information

h Summary Chapter 7.

h Summary Chapter 7. Summry Chptr 7. In Chptr 7 w dscussd byond th fr lctron modl of chptr 6. In prtculrly w focusd on th nflunc of th prodc potntl of th on cors on th nrgy lvl dgrm of th outr lctrons of th toms. It wll hlp

More information

Analysis of Effects of Rebounds and Aerodynamics for Trajectory of Table Tennis Ball

Analysis of Effects of Rebounds and Aerodynamics for Trajectory of Table Tennis Ball Al f Effc f Ru Ac f Tjc f Tl T Bll Juk Nu Mchcl Scc Egg, Gu Schl f Egg, Ng Uv, Fu-ch, Chku-ku, Ng, J Ak Nkh Mchcl Scc Egg, Gu Schl f Egg, Ng Uv, Fu-ch, Chku-ku, Ng, J Yhku Hkw Mchcl Scc Egg, Gu Schl f

More information

STABILITY ANALYSIS IN A FALLING FILM REACTOR Dr. Mohammad F. Abid Chemical Engineering Department- University of Technology

STABILITY ANALYSIS IN A FALLING FILM REACTOR Dr. Mohammad F. Abid Chemical Engineering Department- University of Technology kt Jounl of ng. Scncs/ol.5/No./Mch 8, -6 ASRA SAIIY ANAYSIS IN A FAING FIM RAOR. Mohmmd F. Ad hmcl ngnng ptmnt- Unvst of chnolog An ndustl scl fllng flm cto FFR usng gsous SO3/ lqud Alklnzn s optng sstm-

More information

Theoretical Electron Impact Ionization, Recombination, and Photon Emissivity Coefficient for Tungsten Ions

Theoretical Electron Impact Ionization, Recombination, and Photon Emissivity Coefficient for Tungsten Ions TM on Unctanty ssssmnt and Bnchmak Expmnts fo &M Data fo Fuson pplcatons Thotcal Elcton Impact Ionzaton, Rcombnaton, and Photon Emssvty Coffcnt fo Tungstn Ions D.-H. Kwon, Koa tomc Engy Rsach Insttut 2016.

More information

5.61 Fall 2007 Lecture #2 page 1. The DEMISE of CLASSICAL PHYSICS

5.61 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 information

Outline. Motivation. Motivation. Theoretical method. Main results. Summary. Motivation. Theoretical method. Main results. Summary.

Outline. Motivation. Motivation. Theoretical method. Main results. Summary. Motivation. Theoretical method. Main results. Summary. Outln Thotcal Study on Elcton Impact Exctaton and Dlctonc Rcombnaton of Hghly Chagd Tungstn Ions Thotcal mthod, Zhongwn Wu, and Chnzhong Dong Ky Lab of Atomc and Molcula Physcs & Functonal Matals of Gansu,

More information

1- Summary of Kinetic Theory of Gases

1- Summary of Kinetic Theory of Gases Dr. Kasra Etmad Octobr 5, 011 1- Summary of Kntc Thory of Gass - Radaton 3- E4 4- Plasma Proprts f(v f ( v m 4 ( kt 3/ v xp( mv kt V v v m v 1 rms V kt v m ( m 1/ v 8kT m 3kT v rms ( m 1/ E3: Prcntag of

More information

Stabilizing gain design for PFC (Predictive Functional Control) with estimated disturbance feed-forward

Stabilizing gain design for PFC (Predictive Functional Control) with estimated disturbance feed-forward Stblzg g sg o PFC Pctv Fctol Cotol wth stt stbc -ow. Zbt R. Hb. och Dtt o Pocss Egg Plt Dsg Lboto o Pocss Atoto Colog Uvst o Al Scc D-5679 öl Btzo St. -l: hl.zbt@sl.h-ol. {obt.hb l.och}@ h-ol. Abstct:

More information

Section 5.1/5.2: Areas and Distances the Definite Integral

Section 5.1/5.2: Areas and Distances the Definite Integral Scto./.: Ars d Dstcs th Dt Itgrl Sgm Notto Prctc HW rom Stwrt Ttook ot to hd p. #,, 9 p. 6 #,, 9- odd, - odd Th sum o trms,,, s wrtt s, whr th d o summto Empl : Fd th sum. Soluto: Th Dt Itgrl Suppos w

More information

DISCUSSION ON THE COMPOSITION AND TRANSPORT COEFFICIENTS CALCULATION MADE IN PLASMA OUT OF EQUILIBRIUM

DISCUSSION ON THE COMPOSITION AND TRANSPORT COEFFICIENTS CALCULATION MADE IN PLASMA OUT OF EQUILIBRIUM DISCUSSI THE CMPSITI AD TRASPRT CEFFICIETS CALCULATI MADE I PLASMA UT F EQUILIBRIUM Pascal Andé, Jacqus Aubton, Mao Da Slva, Mchl Dudck, Ma-Fanços Elchng, Buno Lopz To ct ths vson: Pascal Andé, Jacqus

More information

Study of Dynamic Aperture for PETRA III Ring K. Balewski, W. Brefeld, W. Decking, Y. Li DESY

Study of Dynamic Aperture for PETRA III Ring K. Balewski, W. Brefeld, W. Decking, Y. Li DESY Stud of Dnamc Aprtur for PETRA III Rng K. Balws, W. Brfld, W. Dcng, Y. L DESY FLS6 Hamburg PETRA III Yong-Jun L t al. Ovrvw Introducton Dnamcs of dampng wgglrs hoc of machn tuns, and optmzaton of stupol

More information

4D SIMPLICIAL QUANTUM GRAVITY

4D SIMPLICIAL QUANTUM GRAVITY T.YUKAWA and S.HORATA Soknda/KEK D SIMPLICIAL QUATUM GRAITY Plan of th talk Rvw of th D slcal quantu gravty Rvw of nurcal thods urcal rsult and dscusson Whr dos th slcal quantu gravty stand? In short dstanc

More information