Reducing the jitter noise power by oversampling in High speed of dm system
|
|
- Christian Perry
- 6 years ago
- Views:
Transcription
1 Itratioa Joura of Egirig Scic Ivtio Voum Iu 3 ǁ arch. 3 Rducig th jittr oi por by ovrampig i High pd of dm ytm B. Vami Kriha, P.Nagarjua, J. SAYANARAYANA 3 (At.Profor, Dpartmt of ECE, IS adaapa, A.P, INDIA) (At.Profor, Dpartmt of ECE, GPREC Kuroo, A.P, INDIA) 3 (At.Profor, Dpartmt of ECE, INELL ENGG COLLEGE,AP, A.P, INDIA ABSRAC: h OFD ytm ha muti ub carrir to d th high pd data. At high data rat thr i b chac of timig jittr i OFD ytm du to mimatch of th ampig coc at th rcivr ith th tramiio pd. h ffct caud by timig jittr i a igificat imitig factor i th prformac of vry high data rat OFD ytm. Ovrampig ca rduc th oi caud by timig jittr. Both fractioa ovrampig achivd by avig om bad-dg OFD ubcarrir uud ad itgra ovrampig ar coidrd. Ovrampig rut i a 3 db rductio i jittr oi por for vry doubig of th ampig rat. Kyord: imig jittr, ovr ampig, jittr oi por, OFD I. INRODUCION Orthogoa frqucy diviio mutipxig(ofd) i bcomig idy appid i ir commuicatio ytm du to it high rat tramiio capabiity ith high badidth fficicy ad it robut ith rgard to muti-path fadig ad day. It ha b ud i digita audio broadcatig (DAB) ytm, digita vido broadcatig (DVB) ytm, digita ubcribr i (DSL) tadard, ad ir LAN. OFD i ud i may ir broadbad commuicatio ytm bcau it i a imp ad caab outio to itr ymbo itrfrc caud by a mutipath cha. Data rat i optica fibr ytm ar typicay much highr tha i RF ir ytm. At th vry high data rat, timig jittr i mrgig a a importat imitatio to th prformac of OFD ytm. A major ourc of jittr i th ampig coc i th vry high pd aaog-to-digita covrtr (ADC) hich ar rquird i th ytm. imig jittr i ao mrgig a a probm i high frqucy bad pa ampig OFD radio. I OFD, fractioa ovrampig ca b achivd by avig om bad-dg ubcarrir uud. Vry high pd ADC typicay u a para pipi architctur ot a PLL for thi mod. II. OVERVIEW OF OFD SYSE A OFD iga i a uprpoitio of N iuoida carrir ith frqucy paratio F N, ach ubcarrir i moduatd by compx ymbo ith priod N qua to th ivr of th frqucy paratio, i.. N =/F N. h moduatd carrir ovrap pctray but, ic thy ar orthogoa ithi a ymbo duratio (th th carrir frqucy i f = f o + F N hr f o i om rfrc frqucy ad < < N ), th iga aociatd ith ach iuoid ca b rcovrd a og a th cha do ot dtroy th orthogoaity. I practic, th amp of th OFD iga ar gratd by taig th ivr dicrt Fourir traform (IDF) of a dicrt-tim iput quc ad paig th traform amp through a pu hapig fitr. At th rcivr dua traformatio ar impmtd. o priodic iga ar orthogoa h th itgra of thir product, ovr o priod, i qua to zro. Dfiitio of Orthogoa: Cotiuou im: co( f t) co( mf t) dt ( m) Dicrtim: N- co N m co N ( m)
2 Rducig th jittr oi por by ovrampig i high pd ofdm ytm h carrir of a OFD ytm ar iuoid that mt thi rquirmt bcau ach o i a mutip of a fudamta frqucy. Each o ha a itgr umbr of cyc i th fudamta priod. III. SYSE ODEL Coidr th high-pd OFD ytm.h OFD ymbo priod, ot icudig th cycic prfix, i. At th tramittr, i ach ymbo priod, up to N compx vau rprtig th cotatio poit ar ud to moduat up to N ubcarrir. imig jittr ca b itroducd at a umbr of poit i a practica OFD ytm but i thi ttr coidr oy jittr itroducd at th ampr boc of th rcivr ADC. Iday th rcivd OFD iga ampd at uiform itrva of /N. h ffct of timig jittr i to cau dviatio τ bt th actua ampig tim ad th uiform ampig itrva. I OFD ytm hi timig jittr dgrad ytm prformac, a cotat tim offt from th ida ampig itat i automaticay corrctd ithout paty by th quaizr i th rcivr. Fig: OFD boc diagram I OFD ytm thr i o chac for itr carrir itrfrc(ici) bcau of th ub carrir ar orthogoa to ach othr. hr a CDA ad GS tchoogi ar ig carrir ytm.at high data rat thr i b chac of timig jittr i OFD ytm du to mimatch of th ampig coc at th rcivr ith th tramiio pd. IV.IING JIER IN OFD: imig jittr i τ oft modd a a id tatioary (WSS) Gauia proc ith zro-ma ad variac. Fig: Dfiitio of timig jittr h ffct of timig jittr ca b dcribd by a timig jittr matrix. h compact matrix form for OFD ytm ith timig jittr i Y = WH +N () hr, Y ad N ar th tramittd, rcivd ad additiv hit Gauia oi (AWGN) vctor rpctivy, H i th cha rpo matrix ad W i th timig jittr matrix. hr Y =[Y N/+. Y Y N/ ] H = diag(h N/+..H. H N/ )
3 Rducig th jittr oi por by ovrampig i high pd ofdm ytm =[ N/+.. N/ ] imig jittr cau a addd oi i compot i th rcivd iga. Y = H + (W I)H +N () hr I i th N N idtity matrix. h firt trm i () i th atd compot hi th cod trm giv th jittr oi.h mt of th timig jittr matrix W ar giv by, N / j j ( ) N N N / hr i th tim idx, i th idx of th tramittd ubcarrir ad i th idx of th rcivd ubcarrir. h timig jittr matrix i giv by (3) (4) V. OVERSAPLING YPES h ffct of both fractioa ad itgra ovrampig i OFD ca b ud to rduc th dgradatio caud by timig jittr. o achiv itgra ovrampig, th rcivd iga i ampd at a rat of N/, hr i a itgr. For fractioa ovrampig om bad-dg ubcarrir ar uud i th tramittd iga. Wh a N ubcarrir ar moduatd, th badidth of th babad OFD iga i N/, o ampig at itrva of /N i Nyquit rat ampig. If itad, oy th ubcarrir ith idic bt N L ad +N U ar o zro, th badidth of th iga i (N L +N U)/. i thi ca ampig at itrva of /N i abov th Nyquit rat. h dgr of ovrampig i giv by (N L + N U)/N. VI. EFFC OF OVERSAPLING ON JIER NOISE POWER: I th gra ca, hr both itgra ad fractioa ovrampig ar appid, th iga amp aftr th ADC i th rcivr ar giv by y y N N N u N H L j N N hr i th ovrampd dicrt tim idx ad η i th AWGN. With itgra ovrampig, th N-poit FF i th rcivr i rpacd by a ovrizd N-poit FF. h output of thi FF i a vctor of gth N ith mt. j N N / Y y (6) N N / hr i th idx at th output of th N poit FF. h modifid ightig cofficit for th ovrampig ca,, N N / N / j j ( ) N By uig th approximatio jθ = +jθ for ma θ, a i(5) ad (7), N / N N / j j( ) / N So for th variac of th ightig cofficit i giv by, p j d N { { (8) N (5) (7)
4 Rducig th jittr oi por by ovrampig i high pd ofdm ytm Whr -p =d. Wh th timig jittr i hit, th {ττ d = for d o, { { N From (9) it ca b that hit timig jittr E{, i ivry proportioa to o icraig th itgr ovrampig factor rduc th itr carrir itrfrc (ICI) du to timig jittr. It i ao that E{, dpd o but ot o, o highr frqucy ubcarrir cau mor ICI, but th ICI affct a ubcarrir quay. AVERAGE JIER NOISE POWER FOR EACH SUBCARRIER Y H NU, I, H N( ) N L hr th cod trm rprt th jittr oi. coidr a fat cha ith,h = ad aum that th tramittd iga por i ditributd quay acro th ud ubcarrir o that for ach ud ubcarrir E{ = σ. h th avrag jittr oi por, Pj () to rcivd iga por of th ubcarrir i giv by (9) () Pj { Nv I,, Nu ( ) N { I,, NL () Rarragig th trm i ()quatio Pj( ) N v N { 3 N () Pj( ) N If thr i o itgra ovrampig or fractioa ovrampig, = ad Nv = N, { (3) 3 N Comparig () ad (3) it ca b that th combiatio of itgra ovrampig ad fractioa ovrampig rduc th jittr oi por by a factor of Nv/N. VII. SIULAION RESULS: By uig mat ab oftar, th imuatio rut ar ho bo. Figur : h graph i dra bt th ovrampig factor ad jittr oi por. Rut: du to ovrampig, hvr icra th ampig Factor by to, thr a th dcra i jittr oi por by 3db.
5 Rducig th jittr oi por by ovrampig i high pd ofdm ytm Figur: h graph i ho bo for th fractioa ovrampig ho to rduc th timig jittr. Rut. h variac of th oi du to jittr a a fuctio of rcivd ubcarrir idx h baddg ubcarrir ar uud. It ho that th por of th jittr oi i ot a fuctio of ubcarrir idx ad that rmovig th bad-dg ubcarrir rduc th oi quay acro a ubcarrir. Avrag jittr oi por a a fuctio of th ovrampig factor. hr i co agrmt bt thory ad imuatio. VIII. CONCLUSIONS It ha b ho both thorticay ad by imuatio that ovrampig ca rduc th dgradatio caud by timig jittr i OFD ytm. o mthod of ovrampig r ud: fractioa ovrampig achivd by avig om of th bad-dg ubcarrir uud, ad itgra ovrampig impmtd by icraig th ampig rat at th rcivr. h jittr variac i ot chagd h ovrampig i appid, o th jittr rprt a argr fractio of th ampig priod for th ovrampd ytm For th ca of hit timig jittr both tchiqu rut i a iar rductio i jittr oi por a a fuctio of ovrampig rat. hu ovrampig giv a 3 db rductio i jittr oi por for vry doubig of ampig rat. Avrag jittr oi por a a fuctio of th ovrampig factor. hr i co agrmt bt thory ad imuatio. It a ao ho that i th prc of timig jittr, high frqucy ubcarrir cau mor ICI tha or frqucy ubcarrir, but that th rutig ICI i prad quay acro a ubcarrir. REFERENCES []. J. Armtrog, OFD for optica commuicatio, J. Lightav cho., vo. 7, o., pp. 89-4, Fb. 9. []. V. Syrjaa ad. Vaama, Jittr mitigatio i high-frqucy bad pa ampig OFD radio, i Proc. WCNC 9, pp. -6. [3]. K. N. aoj ad G. hiagaraja, h ffct of ampig jittr i OFD ytm, i Proc. IEEE It. Cof. Commu., vo. 3, pp. 6-65, ay 3. [4]. U. Ouo, Y. Li, ad A. Sami, Effct of timig jittr o OFD bad UWB ytm, IEEE J. S. Ara Commu., vo. 4, pp ,6. [5]. L. Yag, P. Fitzpatric, ad J. Armtrog, h Effct of timig jittr o high-pd OFD ytm, i Proc. AuCW 9, pp. -6. [6]. L. Suma,. Watari, ad K. A. I. Hao, A -bit -S/ COS para pipi A/D covrtr, IEEE J. Soid-Stat Circuit,vo. 36, pp ,.
ANOVA- Analyisis of Variance
ANOVA- Aalii of Variac CS 700 Comparig altrativ Comparig two altrativ u cofidc itrval Comparig mor tha two altrativ ANOVA Aali of Variac Comparig Mor Tha Two Altrativ Naïv approach Compar cofidc itrval
More informationConsider serial transmission. In Proakis notation, we receive
5..3 Dciio-Dirctd Pha Trackig [P 6..4] 5.-1 Trackr commoly work o radom data igal (plu oi), o th kow-igal modl do ot apply. W till kow much about th tructur o th igal, though, ad w ca xploit it. Coidr
More informationECEN 5005 Crystals, Nanocrystals and Device Applications Class 14 Group Theory For Crystals
ECEN 5005 Cryta Naocryta ad Dvic Appicatio Ca 14 Group Thory For Cryta Spi Aguar Motu Quatu Stat of Hydrog-ik Ato Sig Ectro Cryta Fid Thory Fu Rotatio Group 1 Spi Aguar Motu Spi itriic aguar otu of ctro
More informationELG3150 Assignment 3
ELG350 Aigmt 3 Aigmt 3: E5.7; P5.6; P5.6; P5.9; AP5.; DP5.4 E5.7 A cotrol ytm for poitioig th had of a floppy dik driv ha th clodloop trafr fuctio 0.33( + 0.8) T ( ) ( + 0.6)( + 4 + 5) Plot th pol ad zro
More information1985 AP Calculus BC: Section I
985 AP Calculus BC: Sctio I 9 Miuts No Calculator Nots: () I this amiatio, l dots th atural logarithm of (that is, logarithm to th bas ). () Ulss othrwis spcifid, th domai of a fuctio f is assumd to b
More information= (3) family of spreading sequences. The dimension of an Oppermann set with the code length of N is determined by
(EUSIPCO Europa Siga Procssig Cofrc, Gasgow, Aug. 9 Improv Corratio of Graiz DFT with oiar Phas for OFD a CDA Commuicatios Ai. Aasu a Haa Agirma-Tosu w Jrsy Istitut of Tchoogy Dpartmt of Ectrica & Computr
More informationPURE MATHEMATICS A-LEVEL PAPER 1
-AL P MATH PAPER HONG KONG EXAMINATIONS AUTHORITY HONG KONG ADVANCED LEVEL EXAMINATION PURE MATHEMATICS A-LEVEL PAPER 8 am am ( hours) This papr must b aswrd i Eglish This papr cosists of Sctio A ad Sctio
More informationPerformance Analysis of OFDM and CDMA Using Phase Noise and Frequency Error
rformac Aalyi of OFDM a CDMA Uig ha oi a Frqucy rror A. Aou, M. Bbti, M. Djbari, M. Mhi a M. Brali aou@urach.com, m_bbti@hotmail.com, mmhi_m@hotmail.com Abtract- Two multipl acc chm u for high bit rat
More informationDigital Signal Processing, Fall 2006
Digital Sigal Procssig, Fall 6 Lctur 9: Th Discrt Fourir Trasfor Zhg-Hua Ta Dpartt of Elctroic Systs Aalborg Uivrsity, Dar zt@o.aau.d Digital Sigal Procssig, I, Zhg-Hua Ta, 6 Cours at a glac MM Discrt-ti
More informationDiscrete Fourier Transform (DFT)
Discrt Fourir Trasorm DFT Major: All Egirig Majors Authors: Duc guy http://umricalmthods.g.us.du umrical Mthods or STEM udrgraduats 8/3/29 http://umricalmthods.g.us.du Discrt Fourir Trasorm Rcalld th xpotial
More information2. SIMPLE SOIL PROPETIES
2. SIMPLE SOIL PROPETIES 2.1 EIGHT-OLUME RELATIONSHIPS It i oft rquir of th gotchical gir to collct, claify a ivtigat oil ampl. B it for ig of fouatio or i calculatio of arthork volum, trmiatio of oil
More informationSession : Plasmas in Equilibrium
Sssio : Plasmas i Equilibrium Ioizatio ad Coductio i a High-prssur Plasma A ormal gas at T < 3000 K is a good lctrical isulator, bcaus thr ar almost o fr lctros i it. For prssurs > 0.1 atm, collisio amog
More informationFrequency Measurement in Noise
Frqucy Masurmt i ois Porat Sctio 6.5 /4 Frqucy Mas. i ois Problm Wat to o look at th ct o ois o usig th DFT to masur th rqucy o a siusoid. Cosidr sigl complx siusoid cas: j y +, ssum Complx Whit ois Gaussia,
More informationECEN620: Network Theory Broadband Circuit Design Fall 2014
ECE60: work Thory Broadbad Circui Dig Fall 04 Lcur 6: PLL Trai Bhavior Sam Palrmo Aalog & Mixd-Sigal Cr Txa A&M Uivriy Aoucm, Agda, & Rfrc HW i du oday by 5PM PLL Trackig Rpo Pha Dcor Modl PLL Hold Rag
More informationIV Design of Discrete Time Control System by Conventional Methods
IV Dig of Dicrt im Cotrol Sytm by Covtioal Mthod opic to b covrd. Itroductio. Mappig bt th pla ad pla 3. Stability aalyi 4. rait ad tady tat rpo 5. Dig bad o root locu mthod 6. Dig bad o frqucy rpo mthod
More informationDiscrete Fourier Series and Transforms
Lctur 4 Outi: Discrt Fourir Sris ad Trasforms Aoucmts: H 4 postd, du Tus May 8 at 4:3pm. o at Hs as soutios wi b avaiab immdiaty. Midtrm dtais o t pag H 5 wi b postd Fri May, du foowig Fri (as usua) Rviw
More informationECE594I Notes set 6: Thermal Noise
C594I ots, M. odwll, copyrightd C594I Nots st 6: Thrmal Nois Mark odwll Uivrsity of Califoria, ata Barbara rodwll@c.ucsb.du 805-893-344, 805-893-36 fax frcs ad Citatios: C594I ots, M. odwll, copyrightd
More informationAPPENDIX: STATISTICAL TOOLS
I. Nots o radom samplig Why do you d to sampl radomly? APPENDI: STATISTICAL TOOLS I ordr to masur som valu o a populatio of orgaisms, you usually caot masur all orgaisms, so you sampl a subst of th populatio.
More informationProblem Value Score Earned No/Wrong Rec -3 Total
GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL of ELECTRICAL & COMPUTER ENGINEERING ECE6 Fall Quiz # Writt Eam Novmr, NAME: Solutio Kys GT Usram: LAST FIRST.g., gtiit Rcitatio Sctio: Circl t dat & tim w your Rcitatio
More informationLECTURE 13 Filling the bands. Occupancy of Available Energy Levels
LUR 3 illig th bads Occupacy o Availabl rgy Lvls W hav dtrmid ad a dsity o stats. W also d a way o dtrmiig i a stat is illd or ot at a giv tmpratur. h distributio o th rgis o a larg umbr o particls ad
More informationz 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z
Sris Expasio of Rciprocal of Gamma Fuctio. Fuctios with Itgrs as Roots Fuctio f with gativ itgrs as roots ca b dscribd as follows. f() Howvr, this ifiit product divrgs. That is, such a fuctio caot xist
More information07 - SEQUENCES AND SERIES Page 1 ( Answers at he end of all questions ) b, z = n
07 - SEQUENCES AND SERIES Pag ( Aswrs at h d of all qustios ) ( ) If = a, y = b, z = c, whr a, b, c ar i A.P. ad = 0 = 0 = 0 l a l
More informationOrdinary Differential Equations
Ordiary Diffrtial Equatio Aftr radig thi chaptr, you hould b abl to:. dfi a ordiary diffrtial quatio,. diffrtiat btw a ordiary ad partial diffrtial quatio, ad. Solv liar ordiary diffrtial quatio with fid
More informationPower Spectrum Estimation of Stochastic Stationary Signals
ag of 6 or Spctru stato of Stochastc Statoary Sgas Lt s cosr a obsrvato of a stochastc procss (). Ay obsrvato s a ft rcor of th ra procss. Thrfor, ca say:
More informationUNIT I FOURIER SERIES T
UNIT I FOURIER SERIES PROBLEM : Th urig mom T o h crkh o m gi i giv or ri o vu o h crk g dgr 6 9 5 8 T 5 897 785 599 66 Epd T i ri o i. Souio: L T = i + i + i +, Sic h ir d vu o T r rpd gc o T T i T i
More informationThey must have different numbers of electrons orbiting their nuclei. They must have the same number of neutrons in their nuclei.
37 1 How may utros ar i a uclus of th uclid l? 20 37 54 2 crtai lmt has svral isotops. Which statmt about ths isotops is corrct? Thy must hav diffrt umbrs of lctros orbitig thir ucli. Thy must hav th sam
More informationDiscrete Fourier Transform. Nuno Vasconcelos UCSD
Discrt Fourir Trasform uo Vascoclos UCSD Liar Shift Ivariat (LSI) systms o of th most importat cocpts i liar systms thory is that of a LSI systm Dfiitio: a systm T that maps [ ito y[ is LSI if ad oly if
More informationHow many neutrino species?
ow may utrio scis? Two mthods for dtrmii it lium abudac i uivrs At a collidr umbr of utrio scis Exasio of th uivrs is ovrd by th Fridma quatio R R 8G tot Kc R Whr: :ubblcostat G :Gravitatioal costat 6.
More information(1) Then we could wave our hands over this and it would become:
MAT* K285 Spring 28 Anthony Bnoit 4/17/28 Wk 12: Laplac Tranform Rading: Kohlr & Johnon, Chaptr 5 to p. 35 HW: 5.1: 3, 7, 1*, 19 5.2: 1, 5*, 13*, 19, 45* 5.3: 1, 11*, 19 * Pla writ-up th problm natly and
More informationProbability & Statistics,
Probability & Statistics, BITS Pilai K K Birla Goa Campus Dr. Jajati Kshari Sahoo Dpartmt of Mathmatics BITS Pilai, K K Birla Goa Campus Poisso Distributio Poisso Distributio: A radom variabl X is said
More informationChapter 3 Fourier Series Representation of Periodic Signals
Chptr Fourir Sris Rprsttio of Priodic Sigls If ritrry sigl x(t or x[] is xprssd s lir comitio of som sic sigls th rspos of LI systm coms th sum of th idividul rsposs of thos sic sigls Such sic sigl must:
More informationMM1. Introduction to State-Space Method
MM Itroductio to Stt-Spc Mthod Wht tt-pc thod? How to gt th tt-pc dcriptio? 3 Proprty Alyi Bd o SS Modl Rdig Mtril: FC: p469-49 C: p- /4/8 Modr Cotrol Wht th SttS tt-spc Mthod? I th tt-pc thod th dyic
More informationMONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx
MONTGOMERY COLLEGE Dpartmt of Mathmatics Rockvill Campus MATH 8 - REVIEW PROBLEMS. Stat whthr ach of th followig ca b itgratd by partial fractios (PF), itgratio by parts (PI), u-substitutio (U), or o of
More informationEngineering Differential Equations Practice Final Exam Solutions Fall 2011
9.6 Enginring Diffrntial Equation Practic Final Exam Solution Fall 0 Problm. (0 pt.) Solv th following initial valu problm: x y = xy, y() = 4. Thi i a linar d.. bcau y and y appar only to th firt powr.
More informationEXACT SOLUTION OF DISCRETE HEDGING EQUATION FOR EUROPEAN OPTION
EXACT SOLUTION OF DISCRETE HEDGING EQUATION FOR EUROPEAN OPTION Yaovlv D.E., Zhabi D. N. Dartmt of Highr athmatic ad athmatical Phyic Tom Polytchic Uivrity, Tom, Lia avu 3, 6344, Ruia Th aroach that allow
More informationPhysics of the Interstellar and Intergalactic Medium
PYA0 Sior Sophistr Physics of th Itrstllar ad Itrgalactic Mdium Lctur 7: II gios Dr Graham M. arpr School of Physics, TCD Follow-up radig for this ad t lctur Chaptr 5: Dyso ad Williams (lss dtaild) Chaptr
More informationWorksheet: Taylor Series, Lagrange Error Bound ilearnmath.net
Taylor s Thorm & Lagrag Error Bouds Actual Error This is th ral amout o rror, ot th rror boud (worst cas scario). It is th dirc btw th actual () ad th polyomial. Stps:. Plug -valu ito () to gt a valu.
More information15/03/1439. Lectures on Signals & systems Engineering
Lcturs o Sigals & syms Egirig Dsigd ad Prd by Dr. Ayma Elshawy Elsfy Dpt. of Syms & Computr Eg. Al-Azhar Uivrsity Email : aymalshawy@yahoo.com A sigal ca b rprd as a liar combiatio of basic sigals. Th
More informationOption 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges.
Optio Chaptr Ercis. Covrgs to Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Divrgs 8 Divrgs Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Covrgs to Covrgs to 8 Proof Covrgs to π l 8 l a b Divrgt π Divrgt
More informationZero Point Energy: Thermodynamic Equilibrium and Planck Radiation Law
Gaug Institut Journa Vo. No 4, Novmbr 005, Zro Point Enrgy: Thrmodynamic Equiibrium and Panck Radiation Law Novmbr, 005 vick@adnc.com Abstract: In a rcnt papr, w provd that Panck s radiation aw with zro
More informationExam 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 informationTime : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120
Tim : hr. Tst Papr 8 D 4//5 Bch - R Marks : SINGLE CORRECT CHOICE TYPE [4, ]. If th compl umbr z sisfis th coditio z 3, th th last valu of z is qual to : z (A) 5/3 (B) 8/3 (C) /3 (D) o of ths 5 4. Th itgral,
More informationINTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS
adjoint...6 block diagram...4 clod loop ytm... 5, 0 E()...6 (t)...6 rror tady tat tracking...6 tracking...6...6 gloary... 0 impul function...3 input...5 invr Laplac tranform, INTRODUCTION TO AUTOMATIC
More informationOn the approximation of the constant of Napier
Stud. Uiv. Babş-Bolyai Math. 560, No., 609 64 O th approximatio of th costat of Napir Adri Vrscu Abstract. Startig from som oldr idas of [] ad [6], w show w facts cocrig th approximatio of th costat of
More informationNote 6 Frequency Response
No 6 Frqucy Rpo Dparm of Mchaical Egirig, Uivriy Of Sakachwa, 57 Campu Driv, Sakaoo, S S7N 59, Caada Dparm of Mchaical Egirig, Uivriy Of Sakachwa, 57 Campu Driv, Sakaoo, S S7N 59, Caada. alyical Exprio
More informationDPSK signal carrier synchronization module implemented on the FPGA
06 Sixth Itratioal Cofrc o Itrumtatio & Maurmt, Computr, Commuicatio ad Cotrol DPSK igal carrir ychroiatio modul implmtd o th FPGA Yufi Yag, Zhuomig i, Ricai Tia, Xiaoli Zhag 3 School of Elctroic ad Iformatio
More informationSolution to 1223 The Evil Warden.
Solutio to 1 Th Evil Ward. This is o of thos vry rar PoWs (I caot thik of aothr cas) that o o solvd. About 10 of you submittd th basic approach, which givs a probability of 47%. I was shockd wh I foud
More informationMixed Mode Oscillations as a Mechanism for Pseudo-Plateau Bursting
Mixd Mod Oscillatios as a Mchaism for Psudo-Platau Burstig Richard Brtram Dpartmt of Mathmatics Florida Stat Uivrsity Tallahass, FL Collaborators ad Support Thodor Vo Marti Wchslbrgr Joël Tabak Uivrsity
More informationDTFT Properties. Example - Determine the DTFT Y ( e ) of n. Let. We can therefore write. From Table 3.1, the DTFT of x[n] is given by 1
DTFT Proprtis Exampl - Dtrmi th DTFT Y of y α µ, α < Lt x α µ, α < W ca thrfor writ y x x From Tabl 3., th DTFT of x is giv by ω X ω α ω Copyright, S. K. Mitra Copyright, S. K. Mitra DTFT Proprtis DTFT
More informationAn Introduction to Asymptotic Expansions
A Itroductio to Asmptotic Expasios R. Shaar Subramaia Asmptotic xpasios ar usd i aalsis to dscrib th bhavior of a fuctio i a limitig situatio. Wh a fuctio ( x, dpds o a small paramtr, ad th solutio of
More informationASSERTION AND REASON
ASSERTION AND REASON Som qustios (Assrtio Rso typ) r giv low. Ech qustio cotis Sttmt (Assrtio) d Sttmt (Rso). Ech qustio hs choics (A), (B), (C) d (D) out of which ONLY ONE is corrct. So slct th corrct
More informationSuperfluid Liquid Helium
Surfluid Liquid Hlium:Bo liquid ad urfluidity Ladau thory: two fluid modl Bo-iti Codatio ad urfluid ODLRO, otaou ymmtry brakig, macrocoic wafuctio Gro-Pitakii GP quatio Fyma ictur Rfrc: Thory of quatum
More informationVtusolution.in FOURIER SERIES. Dr.A.T.Eswara Professor and Head Department of Mathematics P.E.S.College of Engineering Mandya
LECTURE NOTES OF ENGINEERING MATHEMATICS III Su Cod: MAT) Vtusoutio.i COURSE CONTENT ) Numric Aysis ) Fourir Sris ) Fourir Trsforms & Z-trsforms ) Prti Diffrti Equtios 5) Lir Agr 6) Ccuus of Vritios Tt
More informationln x = n e = 20 (nearest integer)
H JC Prlim Solutios 6 a + b y a + b / / dy a b 3/ d dy a b at, d Giv quatio of ormal at is y dy ad y wh. d a b () (,) is o th curv a+ b () y.9958 Qustio Solvig () ad (), w hav a, b. Qustio d.77 d d d.77
More informationKISS: A Bit Too Simple. Greg Rose
KI: A Bit Too impl Grg Ros ggr@qualcomm.com Outli KI radom umbr grator ubgrators Efficit attack N KI ad attack oclusio PAGE 2 O approach to PRNG scurity "A radom umbr grator is lik sx: Wh it's good, its
More information[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then
SYSTEM PERFORMANCE Lctur 0: Stady-tat Error Stady-tat Error Lctur 0: Stady-tat Error Dr.alyana Vluvolu Stady-tat rror can b found by applying th final valu thorm and i givn by lim ( t) lim E ( ) t 0 providd
More informationAsymptotic Behaviors for Critical Branching Processes with Immigration
Acta Mathmatica Siica, Eglih Sri Apr., 9, Vol. 35, No. 4, pp. 537 549 Publihd oli: March 5, 9 http://doi.org/.7/4-9-744-6 http://www.actamath.com Acta Mathmatica Siica, Eglih Sri Sprigr-Vrlag GmbH Grmay
More informationESCI 341 Atmospheric Thermodynamics Lesson 14 Curved Droplets and Solutions Dr. DeCaria
ESCI 41 Atmophric hrmodynamic Lon 14 Curd Dropt and Soution Dr. DCaria Rfrnc: hrmodynamic and an Introduction to hrmotatitic, Can Phyica Chmitry, Lin A hort Cour in Coud Phyic, Rogr and Yau hrmodynamic
More informationω (argument or phase)
Imagiary uit: i ( i Complx umbr: z x+ i y Cartsia coordiats: x (ral part y (imagiary part Complx cougat: z x i y Absolut valu: r z x + y Polar coordiats: r (absolut valu or modulus ω (argumt or phas x
More informationResearch of Routing Protocol for Support Pressure Monitor in Mine Base on WSN Zhang Wei 1,a,Zhao Liang 12,b
Appid Mchanic and Matria Submittd: 214-6-25 ISSN: 1662-7482, Vo. 614, pp 535-538 Accptd: 214-6-25 doi:1.428/www.cintific.nt/amm.614.535 Onin: 214-9-26 214 Tran Tch Pubication, Switzrand Rarch of Routing
More informationQuasi-Supercontinuum Interband Lasing Characteristics of Quantum Dot Nanostructures
USOD 008 ottiha UK Quasi-Suprcotiuu Itrbad Lasi Charactristics of Quatu Dot aostructurs C. L. a Y. Wa H. S. Di B. S. Ooi Ctr for Optica choois ad Dpartt of ctrica ad Coputr iri Lhih Uivrsity Bthh Psyvaia
More informationA 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 informationDISCRETE TIME FOURIER TRANSFORM (DTFT)
DISCRETE TIME FOURIER TRANSFORM (DTFT) Th dicrt-tim Fourir Tranform x x n xn n n Th Invr dicrt-tim Fourir Tranform (IDTFT) x n Not: ( ) i a complx valud continuou function = π f [rad/c] f i th digital
More informationEEO 401 Digital Signal Processing Prof. Mark Fowler
EEO 401 Digital Signal Procssing Prof. Mark Fowlr Dtails of th ot St #19 Rading Assignmnt: Sct. 7.1.2, 7.1.3, & 7.2 of Proakis & Manolakis Dfinition of th So Givn signal data points x[n] for n = 0,, -1
More informationChapter 11.00C Physical Problem for Fast Fourier Transform Civil Engineering
haptr. Physical Problm for Fast Fourir Trasform ivil Egirig Itroductio I this chaptr, applicatios of FFT algorithms [-5] for solvig ral-lif problms such as computig th dyamical (displacmt rspos [6-7] of
More informationWEEK 3 Effective Stress and Pore Water Pressure Changes
WEEK 3 Effctiv Str and Por Watr Prur Chang 5. Effctiv tr ath undr undraind condition 5-1. Dfinition of ffctiv tr: A rvi A you mut hav larnt that th ffctiv tr, σ, in oil i dfind a σ σ u Whr σ i th total
More informationPhase Rotation for the 80 MHz ac Mixed Mode Packet
Phas Rotation for th 80 MHz 802.11ac Mixd Mod Packt Dat: 2010-07-12 Authors: Nam Affiliations Addrss Phon mail Lonardo Lanant Jr. Kyushu Inst. of Tchnology Kawazu 680-, Iizuka, JAPAN Yuhi Nagao Kyushu
More informationExact and Approximate Detection Probability Formulas in Fundamentals of Radar Signal Processing
Exact and Approximat tction robabiity Formuas in Fundamntas of Radar Signa rocssing Mark A. Richards Sptmbr 8 Introduction Tab 6. in th txt Fundamntas of Radar Signa rocssing, nd d. [], is rproducd bow.
More informationI M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o
I M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o u l d a l w a y s b e t a k e n, i n c l u d f o l
More informationSystems in Transform Domain Frequency Response Transfer Function Introduction to Filters
LTI Discrt-Tim Systms i Trasform Domai Frqucy Rspos Trasfr Fuctio Itroductio to Filtrs Taia Stathai 811b t.stathai@imprial.ac.u Frqucy Rspos of a LTI Discrt-Tim Systm Th wll ow covolutio sum dscriptio
More informationIntroduction to Quantum Information Processing. Overview. A classical randomised algorithm. q 3,3 00 0,0. p 0,0. Lecture 10.
Itroductio to Quatum Iformatio Procssig Lctur Michl Mosca Ovrviw! Classical Radomizd vs. Quatum Computig! Dutsch-Jozsa ad Brsti- Vazirai algorithms! Th quatum Fourir trasform ad phas stimatio A classical
More informationPart B: Transform Methods. Professor E. Ambikairajah UNSW, Australia
Part B: Trasform Mthods Chaptr 3: Discrt-Tim Fourir Trasform (DTFT) 3. Discrt Tim Fourir Trasform (DTFT) 3. Proprtis of DTFT 3.3 Discrt Fourir Trasform (DFT) 3.4 Paddig with Zros ad frqucy Rsolutio 3.5
More informationIdeal crystal : Regulary ordered point masses connected via harmonic springs
Statistical thrmodyamics of crystals Mooatomic crystal Idal crystal : Rgulary ordrd poit masss coctd via harmoic sprigs Itratomic itractios Rprstd by th lattic forc-costat quivalt atom positios miima o
More information+ x. x 2x. 12. dx. 24. dx + 1)
INTEGRATION of FUNCTION of ONE VARIABLE INDEFINITE INTEGRAL Fidig th idfiit itgrals Rductio to basic itgrals, usig th rul f ( ) f ( ) d =... ( ). ( )d. d. d ( ). d. d. d 7. d 8. d 9. d. d. d. d 9. d 9.
More informationNARAYANA I I T / P M T A C A D E M Y. C o m m o n P r a c t i c e T e s t 1 6 XII STD BATCHES [CF] Date: PHYSIS HEMISTRY MTHEMTIS
. (D). (A). (D). (D) 5. (B) 6. (A) 7. (A) 8. (A) 9. (B). (A). (D). (B). (B). (C) 5. (D) NARAYANA I I T / P M T A C A D E M Y C o m m o n P r a c t i c T s t 6 XII STD BATCHES [CF] Dat: 8.8.6 ANSWER PHYSIS
More informationChapter 4 - The Fourier Series
M. J. Robrts - 8/8/4 Chaptr 4 - Th Fourir Sris Slctd Solutios (I this solutio maual, th symbol,, is usd for priodic covolutio bcaus th prfrrd symbol which appars i th txt is ot i th fot slctio of th word
More informationMultiple Short Term Infusion Homework # 5 PHA 5127
Multipl Short rm Infusion Homwork # 5 PHA 527 A rug is aministr as a short trm infusion. h avrag pharmacokintic paramtrs for this rug ar: k 0.40 hr - V 28 L his rug follows a on-compartmnt boy mol. A 300
More informationComputing and Communications -- Network Coding
89 90 98 00 Computing and Communications -- Ntwork Coding Dr. Zhiyong Chn Institut of Wirlss Communications Tchnology Shanghai Jiao Tong Univrsity China Lctur 5- Nov. 05 0 Classical Information Thory Sourc
More informationSolid State Device Fundamentals
8 Biasd - Juctio Solid Stat Dvic Fudamtals 8. Biasd - Juctio ENS 345 Lctur Cours by Aladr M. Zaitsv aladr.zaitsv@csi.cuy.du Tl: 718 98 81 4N101b Dartmt of Egirig Scic ad Physics Biasig uiolar smicoductor
More informationQ.28 Q.29 Q.30. Q.31 Evaluate: ( log x ) Q.32 Evaluate: ( ) Q.33. Q.34 Evaluate: Q.35 Q.36 Q.37 Q.38 Q.39 Q.40 Q.41 Q.42. Q.43 Evaluate : ( x 2) Q.
LASS XII Q Evlut : Q sc Evlut c Q Evlut: ( ) Q Evlut: Q5 α Evlut: α Q Evlut: Q7 Evlut: { t (t sc )} / Q8 Evlut : ( )( ) Q9 Evlut: Q0 Evlut: Q Evlut : ( ) ( ) Q Evlut : / ( ) Q Evlut: / ( ) Q Evlut : )
More informationDFT: Discrete Fourier Transform
: Discrt Fourir Trasform Cogruc (Itgr modulo m) I this sctio, all lttrs stad for itgrs. gcd m, = th gratst commo divisor of ad m Lt d = gcd(,m) All th liar combiatios r s m of ad m ar multils of d. a b
More informationElements 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 informationChapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series
Chatr Ifiit Sris Pag of Sctio F Itgral Tst Chatr : Ifiit Sris By th d of this sctio you will b abl to valuat imror itgrals tst a sris for covrgc by alyig th itgral tst aly th itgral tst to rov th -sris
More informationFigure 2-18 Thevenin Equivalent Circuit of a Noisy Resistor
.8 NOISE.8. Th Nyquist Nois Thorm W ow wat to tur our atttio to ois. W will start with th basic dfiitio of ois as usd i radar thory ad th discuss ois figur. Th typ of ois of itrst i radar thory is trmd
More informationHow many neutrons does this aluminium atom contain? A 13 B 14 C 27 D 40
alumiium atom has a uclo umbr of 7 ad a roto umbr of 3. How may utros dos this alumiium atom cotai? 3 4 7 40 atom of lmt Q cotais 9 lctros, 9 rotos ad 0 utros. What is Q? calcium otassium strotium yttrium
More informationA Simple Proof that e is Irrational
Two of th most bautiful ad sigificat umbrs i mathmatics ar π ad. π (approximatly qual to 3.459) rprsts th ratio of th circumfrc of a circl to its diamtr. (approximatly qual to.788) is th bas of th atural
More informationChapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1
Chatr Fiv Mor Dimsios 51 Th Sac R W ar ow rard to mov o to sacs of dimsio gratr tha thr Ths sacs ar a straightforward gralizatio of our Euclida sac of thr dimsios Lt b a ositiv itgr Th -dimsioal Euclida
More informationH2 Mathematics Arithmetic & Geometric Series ( )
H Mathmatics Arithmtic & Gomtric Sris (08 09) Basic Mastry Qustios Arithmtic Progrssio ad Sris. Th rth trm of a squc is 4r 7. (i) Stat th first four trms ad th 0th trm. (ii) Show that th squc is a arithmtic
More informationLectures 9 IIR Systems: First Order System
EE3054 Sigals ad Systms Lcturs 9 IIR Systms: First Ordr Systm Yao Wag Polytchic Uivrsity Som slids icludd ar xtractd from lctur prstatios prpard by McCllla ad Schafr Lics Ifo for SPFirst Slids This work
More informationLecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e
8/7/018 Cours Instructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 3 Skin Dpth & Powr Flow Skin Dpth Ths & Powr nots Flow may contain
More informationProblem Set #2 Due: Friday April 20, 2018 at 5 PM.
1 EE102B Spring 2018 Signal Procssing and Linar Systms II Goldsmith Problm St #2 Du: Friday April 20, 2018 at 5 PM. 1. Non-idal sampling and rcovry of idal sampls by discrt-tim filtring 30 pts) Considr
More informationPart B: Transform Methods. Professor E. Ambikairajah UNSW, Australia
Par B: rasform Mhods Profssor E. Ambikairaah UNSW, Ausralia Chapr : Fourir Rprsaio of Sigal. Fourir Sris. Fourir rasform.3 Ivrs Fourir rasform.4 Propris.4. Frqucy Shif.4. im Shif.4.3 Scalig.4.4 Diffriaio
More informationEstimating the Variance in a Simulation Study of Balanced Two Stage Predictors of Realized Random Cluster Means Ed Stanek
Etatg th Varac a Sulato Study of Balacd Two Stag Prdctor of Ralzd Rado Clutr Ma Ed Stak Itroducto W dcrb a pla to tat th varac copot a ulato tudy N ( µ µ W df th varac of th clutr paratr a ug th N ulatd
More informationThe Matrix Exponential
Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!
More informationSolution to Volterra Singular Integral Equations and Non Homogenous Time Fractional PDEs
G. Math. Not Vol. No. Jauary 3 pp. 6- ISSN 9-78; Copyright ICSRS Publicatio 3 www.i-cr.org Availabl fr oli at http://www.gma.i Solutio to Voltrra Sigular Itgral Equatio ad No Homogou Tim Fractioal PDE
More informationNetwork Congestion Games
Ntwork Congstion Gams Assistant Profssor Tas A&M Univrsity Collg Station, TX TX Dallas Collg Station Austin Houston Bst rout dpnds on othrs Ntwork Congstion Gams Travl tim incrass with congstion Highway
More informationReview Exercises. 1. Evaluate using the definition of the definite integral as a Riemann Sum. Does the answer represent an area? 2
MATHEMATIS --RE Itgral alculus Marti Huard Witr 9 Rviw Erciss. Evaluat usig th dfiitio of th dfiit itgral as a Rima Sum. Dos th aswr rprst a ara? a ( d b ( d c ( ( d d ( d. Fid f ( usig th Fudamtal Thorm
More informationFrequency Response & Digital Filters
Frquy Rspos & Digital Filtrs S Wogsa Dpt. of Cotrol Systms ad Istrumtatio Egirig, KUTT Today s goals Frquy rspos aalysis of digital filtrs LTI Digital Filtrs Digital filtr rprstatios ad struturs Idal filtrs
More informationAdvanced Engineering Mathematics, K.A. Stroud, Dexter J. Booth Engineering Mathematics, H.K. Dass Higher Engineering Mathematics, Dr. B.S.
Rfrc: (i) (ii) (iii) Advcd Egirig Mhmic, K.A. Sroud, Dxr J. Booh Egirig Mhmic, H.K. D Highr Egirig Mhmic, Dr. B.S. Grwl Th mhod of m Thi coi of h followig xm wih h giv coribuio o h ol. () Mid-rm xm : 3%
More information5.1 The Nuclear Atom
Sav My Exams! Th Hom of Rvisio For mor awsom GSE ad lvl rsourcs, visit us at www.savmyxams.co.uk/ 5.1 Th Nuclar tom Qustio Papr Lvl IGSE Subjct Physics (0625) Exam oard Topic Sub Topic ooklt ambridg Itratioal
More information