Zero Vectors Combinatorial Code Family for Spectral Amplitude Coding (SAC-OCDMA)

Size: px
Start display at page:

Download "Zero Vectors Combinatorial Code Family for Spectral Amplitude Coding (SAC-OCDMA)"

Transcription

1 0 IJCSNS Intrnational Journal of Computr Scinc and Ntwork Scurity, VOL.8 No.3, March 008 Zro Vctors Combinatorial Cod Family for Spctral Amplitud Coding (SAC-OCDMA) Hassan Yousif Ahmd, Ibrahima Fay, and N.M.Saad, Elctrical & Elctronic Enginring Dpartmnt, Univrsiti Tknologi PETRONAS, Bandar Sri Iskandar, Tronoh, Prak, MALAYSIA Summary Although multipl accss intrfrnc (MAI) problms xisting in optical cod division multipl accss (OCDMA) systms can b solvd by lctrical subtraction, phas inducd intnsity nois (PIIN) rsulting from th phas incohrnt of ovrlapping still rmains and compltly dtriorats th systm prformanc. It is thrfor dsirabl to allviat MAI and PIIN ffcts in dsigning OCDMA systm. W propos a nw mthod to construct cods with zro in-phas cross corrlation namly Zro Vctor Combinatorial Cod (ZVCC) basd on combination of spcific vctors with combinatorial thoris. Simplicity of cod construction, flxibility of choosing th numbr of usrs and wights, mak our proposd systm strong candidat for futur ntworks. In addition, transmittr sid and rcivr sid ar proposd. Dtaild xampls ar givn on how to pick th bst cod among diffrnt options basd on spcific paramtrs. Th rsults show that th proposd cod is ffctiv to rduc th MAI, PIIN and cost, whil maintaining a good signal to nois ratio and bit rror probability. A comparison study btwn th proposd cod and th xisting cods such as Hadamard and MDW has bn carrid out. Ky words: Optical Cod Division Multipl Accss (OCDMA), Multipl Accss Intrfrnc (MAI), Zro Vctor Combinatorial Cod (ZVCC), Optical Communication, Dirct Rcovry Schm (DRS) 1. Introduction A major challng in dvising optical communication systms is to fully xploit th vast bandwidth providd by optical fibr channls. Th succssful of long-span fibr optic communication systms has shiftd th focus of optical ntwork to shortr-span mtropolitan and local ara domains [1]. Thr is not much diffrnc btwn multipl accss and multiplxing tchniqus. Multipl accss allows communication mdia to b shard btwn diffrnt usrs. It rprsnts on of th most ssntial functions of accss ntworks, whil multiplxing is combination of signals into singl transmission signal. Th thr basic multipl accss tchniqus ar Wav Division Multipl Accss (WDMA), Tim Division Multipl Accss (TDMA) and Cod Division Multipl Accss (CDMA). TDMA is a tchnology that allows multipl usrs to accss a channl by allocating tim slots to ach usr within ach channl. WDMA is a tchnology allowing multipl usrs to accss a channl by allocating wavlngth or frquncy to ach usr within ach channl.tdma and WDMA hav a limitd bandwidth for vry usr. Optical Cod Division Multipl Accsss (OCDMA) [1-4] has gaind mor attntion in rcnt yars du to its succss in wirlss communication systms. This is bcaus it allows multipl usrs to accss th channl simultanously with low latncy through assignmnt of uniqu cod squnc [3]. An OCDMA systm suffrs from diffrnt noiss such as shot nois, thrmal nois, dark currnt and multipl accss intrfrnc (MAI) from othr usrs. Among ths noiss, MAI is considrd as th dominat sourc. Thrfor, intllignt dsign of cod squnc is important to rduc th contribution of MAI to th total rcivd powr [4]. Although MAI can b canclld by balanc dtction schm, a phas inducd intnsity nois (PIIN) arising from spontanous mission of broad band sourc, inhrntly rmains. It is thn important to dsign codword such that th ffct of MAI and PIIN of th total rcivd powr is rducd. In OCDMA systms, minimization of cross corrlation to a vry small valu is an advantag. Systms using Cods with zro cross corrlation hav lss nois, which rsults in rducing th hardwar complxity. In this work, Zro Vctor Combinatorial cods (ZVCC) is proposd. This papr is organizd as it follows. In sction II, optical spctral cod division multipl accss is rviwd. In sction III, cods construction and dvlopmnt of all thortical studis is prsntd. Th advantags of ZVCC compard to othr OSCDMA cods, is rportd in sction IV. In sction V, th prformanc analysis of th nw proposd systm is don, and finally, conclusions ar givn in sction VI

2 IJCSNS Intrnational Journal of Computr Scinc and Ntwork Scurity, VOL.8 No.3, March Optical Spctrum Cod Division Multipl Accss (OSCDMA) Optical CDMA systms can b dividd into major catgoris. Th first is cohrnt systms, whr knowldg of th phas and amplitud is ndd in ordr to achiv succssful dtction. Th scond is incohrnt systms, whr th prformanc of th systm dpnds mainly on th amplitud. OSCDMA is an incohrnt broadband light sourc which contains N usr with optical transmittrs and rcivrs as shown in Fig. 1 [5][6]. OSCDMA systm contains ncodrs and dcodrs which can b dsignd by using any kind of optical filtring tchnology. Spctral Amplitud Coding (SAC) was introducd to liminat th MAI xisting in convntional OCDMA systms. SAC systms us complmntary dtction tchniqu to rcovr th original signals. This balanc rcivr is usd as a part of rcivr which filtrs th incoming signals. For unmatchd transmittrs half of transmittr spctral componnts will match th dirct filtr and th othr half will match th complmntary filtr. Th output of th balanc rcivr rprsnts th diffrnc btwn th two parts, with unmatchd channls bing canclld, whil th matchd channl is dmodulatd. It is possibl to dsign cods with th full orthogonality in th incohrnt spctral intnsity OCDMA systm, sinc thr is a subtraction btwn two photo dtctors. In this systm, th signatur squnc is sprad across diffrnt wavlngth with ach chip occupying diffrnt wavlngth [5][6].Th advantag of OSCDMA is it dos not nd synchronization as th chip sprads in frquncy and not in tim. 3. CODE CONSTRUCTION Lt V b a vctor spac of dimnsion n. Th st {v 1, v,.., v n } is a basis of V if th st spans {v i } whr i=1,.., n ar linarly indpndnt and if any lmnt of V can b writtn as a combination of th v i, i= 1,,,n Lt R dnots th fild of ral numbrs. Th spac of all n-tupls of ral numbrs forms an n-dimnsional vctor spac ovr R dnotd by R n. An lmnt x of R n can b writtn as a column vctor: x1 x x = (1) M xn Lt i dnot th lmnt of R n having 0 at all lins xcpt th i th lin. {,,, } n 1 K is a basis of R n calld th standard basis. For n = =, = () 0 1 x1 Lt x = an lmnt of R x x1 x1 0 x= = + (3) x 0 x Thrfor, w hav x1 1 x1 0 x = + x 0 x 1 = x 1 1 +x (4) For n= = 0, = 1, 3 = 0 (5) Whr { 1,, 3} is a basis of R 3. Fig. 1: OCDMA Ntwork

3 IJCSNS Intrnational Journal of Computr Scinc and Ntwork Scurity, VOL.8 No.3, March 008 Lt x1 x = x an lmnt of R 3 x3 Thrfor, w obtain x x x = x 1 1 +x + x 3 3 (6) Lt N b th numbr of usrs and L th cod lngth. W can writ th cod in a matrix form corrsponding to th cod word of N usrs. W obtain N L matrix with two dimnsions as shown in Fig.. Start Entr th wight W and numbr of usr N Comput th lngth L Matrix (N usrs L lngth) Usr1# Usr# Cod pattrns possibilitis UsrN# Fig.: Matrix of ZVCC Th construction of ZVCC is basd on th following mntiond: to hav (shortst) Zro Cross Corrlation (ZCC), w hav to hav on 1 in ach column. This mans for ZCC any column is an lmnt of th standard basis of R n. Givn N and th wight W, w can gnrat all possibilitis of ZVCC having lngth L=N W by gtting all th prmutations of th vctors 1,,, n with rptitions of ach vctor W-tims Any rdundant No All possibilitis Ys Elimination rdundant pattrns of A. Elimination of rdundant pattrns Prmutation has bn don for th first vctor to produc pattrns of ths vctors. Symmtric pattrns appard for th sam wight and numbr of usrs i.., swapping btwn th locations of usrs, th first usr bcom scond usr or th last usr and so on, whil for asymmtric no such duplicat, so w hav to find way to rmov th symmtric pattrns. Fig. 3 shows th flowchart stp to construct cod pattrn for both cass. End Fig.3: Flow chart of cod construction Th cod lngth L for numbr of usrs N with wight W is givn by: L = N W (7) To calculat th cod possibilitis (Cpos) of givn N and W by quation appar blow as prmutation opration

4 IJCSNS Intrnational Journal of Computr Scinc and Ntwork Scurity, VOL.8 No.3, March Cpos = ( W N )! ( W! W!) whr W rprsnt th invrt of W (i.., th numbr of zro). By applying this quation, it is clar that it dpnds on th wight to gt bttr Signal to Nois Ratio (SNR), nvrthlss, its dcras th numbr of possibilitis and th lngth rmain th sam. Lt us invstigat th following xampl. N= W= L= N W= = 4. W = L-W= 4-= Thrfor ( ) ( ) W N!! Cpos = ( W! W!) = (!! ) = 6 W obtain th cods pattrns possibilitis as shown in (9), (10), (11), (1), (13), and (14). Hz 1 = Hz = Hz 3 = Hz 4 = Hz 5 = Hz 6 = (8) (9) (10) (11) (1) (13) (14) From th abov cods pattrns possibilitis, w obsrv that thr is a symmtric btwn (9) and (1), (10) and (14), (11) and (13). Combination of any two symmtric quations produc on pattrn, hnc, whn w swap th position of usr1# and usr#, to rduc th numbrs of symmtric pattrns w us th following quation: ( W N )! Nc = N!( W!) N (15) Whr Nc is numbr of pattrns aftr modification. For th xampl of (N=, W=) aftr applying Eq. (15) w obtain: ( W N )! Nc = N! W! ( ) N = ( )!!(!) = 3 Cpos bcam 3 instad of 6 aftr applying th nw quation, hnc, w obtain Hz 1, Hz, and Hz COMPARSION AND EVALUATION In rcnt yar, many cods hav bn proposd such as modifid doubl wight (MDW) cod [5], modifid frquncy hopping (MFH) [10] and zro cross corrlation (ZCC) [11]. All ths cods suffr from various limitations on way or anothr, th cod construction is complicatd (.g., MFH and ZCC) or th cross corrlation is not idal. Howvr, th cod construction not only dpnds on a cross corrlation proprtis, th lngth plays an important rol w hav to considr as wll. Long lngth is a disadvantag sinc th cod is subjct to ithr vry wid band sourc or narrow filtr bandwidths ar rquird. ZVCC has long lngth and this is considrd as disadvantag, w hav to mak a tradoff btwn th lngth and multipl accss intrfrnc (MAI), bcaus a MAI is a dominant sourc of th noiss. In MFH cod, although th cod lngth is shortr compard to ZVCC, th cross corrlation always qual to unity and this contributs to phas induc intnsity nois (PIIN), whil in ZVCC always th cross corrlation quals to zro which liminats th ffct of PIIN. In tabl.i ZVCC shows flxibility in trms of choosing th numbr of usrs and th wight du to th us of a novl mthod in cod construction which gnrats many possibilitis from a givn numbr of usrs and wights. Tabl 1: SAC-OCDMA cods comparaison cod xistnc wigh Cross Cod lngth t corrlatio n MFH K=Q Q+1 λ=1 N= Q +Q MDW K=n Evn λ=1 N=3n+8/3[sin ( Nii/3)] ZCC K= m m -1 λ=0 C= m Hadamar K= M -1 M-1 λ= M- N= M d M ZVCC Any numbr option λ=0 L=W N

5 4 IJCSNS Intrnational Journal of Computr Scinc and Ntwork Scurity, VOL.8 No.3, March 008 Fig.4: Dirct rcovry schm (ncodr and dcodr using ZVCC) 5. DIRECT RECOVERY SCHEME In OCDMA systm, intllignt cod dsign is dsird to rduc th MAI contribution. Thrfor, a rcivr sid which plays an important rol should b addrssd as wll. In convntional SAC-OCDMA, balanc dtction schm is us to diffrntiat btwn th wantd and th unwantd cod squncs. Hnc, in Dirct Rcovry Schm (DRS), no subtractors ar ndd. At th rcivr sid, dirct filtrs ar using and this significantly liminat th ffct of MAI sinc only th wantd signal will b filtrd out. DRS hav bn proposd as structur of transmittr and rcivr for ZVCC cod family. Fig. 4, shows th procdur of ncoding th signal in transmittr sid thn coupld to th fibr mdia, at th rcivr sid, th rcivr signals ar splitting into qually part followd by filtr and photodiod, finally th signals ar rcovrd by th intndd usrs. Du to all ths, phas induc intnsity nois (PIIN) could b liminatd which provids a possibl way of achiving gratr prformanc. Fig.5: Ey diagram of ZVCC at 10 km 6. CODE SELECTION FROM Cpos Sinc w hav larg numbrs of Cpos in cod construction, in ordr to diffrntiat btwn ths possibilitis, simulation rsults ar acquird by using a softwar tool namd VPI transmission makr. For Hz 1, Hz, Hz 3, Hz 4, Hz 5, and Hz 6, th numbr of usrs is, th wight is, th lngth is 4 and Cpos is 6. Aftr liminats th symmtric pattrns bcam 3. To choos on family among six familis, a simulation work has bn don rspctivly for ach family startd from Hz 1 up to Hz 6 using dirct rcovry schm (transmittr part and rcivr part) to rproduc th signal for intndd usr and th rsults can b show as follows: Fig.6: Ey diagram of ZVCC at 50 km

6 IJCSNS Intrnational Journal of Computr Scinc and Ntwork Scurity, VOL.8 No.3, March SNR BER= P = rfc ( ) (17) 8 Whr L is th cod lngth, W is th cod wight, N th of usrs, R is photodiod rsponsivly, P sr is th ffctiv powr of a broad-band sourc at th rcivr, is an lctronic charg, B is th lctrical quivalnt nois band-width of th rcivr, K B is th Boltizmann s constant, Tr th absolut tmpratur of rcivr nois, R L th load rsistanc and ΔV th optical sourc bandwidth. rfc is a complmntary rror function xprss as follows Fig.7: Ey diagram of ZVCC at 70 km In Fig.5, Fig.6, and Fig.7, a diffrnt fibr lngth has bn chosn to obsrv th incrasing lngth in systm prformanc in trms of y diagram pattrns. In Figs 5, and Fig.6, ZVCC is adoptd with th following paramtrs: lngth of fibr varis from 10 up 50 and data rat is.5gbps. It is shown that, th systm improvs and th ffct of MAI is liminatd whil in Fig 7 th ffct of disprsion in optical fibr is unavoidabl bcaus th distanc is quit long. Th simulation rsults obtaind from Hz and Hz 3 is similar as compard to Hz 1 whn using th sam paramtrs, thrfor, w can tak any cod randomly from Cpos. Furthr improvmnt could b achivd by incrasing th data rat up to 10Gbps. 7. SYSTEM PERFORMANCE In communication systm maximum Signal to Nois Ratio (SNR) yilds bttr Bit Error Rat (BER), ths two compltly affct th systm prformanc. In SAC- OCDMA systm good dsign of th cod plays an important rol by kping up th valu of intrfrnc from simultanous usrs as small as possibl. In ZVCC, in ordr to comput th SNR, w usd th sam mthod dscribd in [7]. Sinc th valu of cross corrlation is zro w compnsat this valu in th SNR [7], th SNR of ZVCC can b xprssd as follows SNR= P sr BR L (16) R P sr W L P [ ] sr BR N 4 ( N 1) + W + [( N 1) + W ] + L ΔV L K b T n B R rfc ( x) = π x u du (18) In litratur rviws, thr hav bn many cods proposd for SAC-OCDMA such as Hadamard [8] and modifid doubl wight (MDW) cod [9] and zro cross corrlation (ZCC) [11]. Howvr, our proposd cod familis hav mor flxibility of gnrating trmndous option of cod pattrns. In this work, th cod prformanc has bn don, th systm paramtrs ar: ΔV=3.75 THz; B=80 MHz; Tr = 300; R L = 1030 Ω ; bitrat 155 Mb/s; photodiod fficincy 0.6 and cntral wavlngth 1550 nm. In Fig.8 and Fig.9, a diffrnt wight valus hav bn chosn to obsrv th incras of th wight on th prformanc. It is shown that, th prformanc of th systm improvs whn th wight incrass which incrass th SNR. In Fig 8, th paramtr takn: w=4, w obsrv th numbr of usrs supportd by ZVCC ar quit much du to non-ovrlapping compar with MDW and larg compard with Hadamard, whil in Fig.9 th wight takn is W=6. It is clar that, th ffct of MAI and PIIN is rducd whn th wight incrass rgardlss for th numbr of usrs. Bit rror rat (BER) MDW (W=4) Hadamard ZVCC (W=4) Numbr of simultanous usrs Fig.8. BER vrsus th numbr of simultanous usrs

7 6 IJCSNS Intrnational Journal of Computr Scinc and Ntwork Scurity, VOL.8 No.3, March 008 Bit rror rat (BER) (w=4) MDW (w=6) Hadamard ZVCC (w=6) Numbr of Simultanous Usrs Fig.8. BER vrsus th numbr of simultanous usrs (w=6) 8. CONLUSTION In this work, construction mthods for nw cod familis with zro cross corrlation for SAC-OCDMA systm, ZVCC has bn proposd. Th proprtis and thortical dvlopmnt of nw family hav bn provd. Nw dsign for transmittr sid and rcivr sid using dirct filtrs to rcovry and rproduc th original data namly dirct rcovry schm (DRS) has bn xamind. Th nw transmittr has bn analyzd using ZVCC taking into considration th ffct of noiss such as thrmal nois and shot nois. Th study showd that, compard with a formr cod such as Hadamard and MDW bttr prformanc du to limination of th ffct of phas induc intnsity nois. Morovr, th way of constructing ZVCC is vry flxibly in choosing th numbr of usrs and th wight. It has shown that, a lot of possibilitis for cod gnration can b obtaind and no diffrnc btwn thm in trms of systm prformanc. provisioning, IEEE Ntwork, vol. 14, no. 6, pp. 4 46, Nov [5] S.A.Aljunid,,M.Ismail, A.R.Ramli, Borhanuddin M Ali, and Mohamad Khazani Abdullah, A NwFamily of Optical Cod Squncs for Spctral-Amplitud-Coding Optical CDMA Systms IEEE Photonics Tchnology Lttrs, Vol. 16, No. 10, Octobr 004 [6] Syd Alw Aljunid, Zuraidah Zan, Siti Barirah Ahmad Anas and Mohd. Khazani Abdullah "A Nw Cod for Optical Cod Division Multipl Accss Systms," Malaysian Journal of Computr Scinc, Vol. 17 No., Dcmbr 004, pp [7] Ivan B. Djordjvic and Ban Vasic, Combinatorial Constructions of Optical Orthogonal Cods for OCDMA Systms. IEEE Communications Lttrs, Vol. 8, No. 6, Jun 004. [8] M. Kavhrad, and D. Zaccarh, "Optical Cod-Division- Multiplxd Systms Basd on Spctral Encoding of Noncohrnt Sourcs," Journal oflightwav Tchnology, Vol. 13, No. 3, March 1995 [9] Syd Alw Aljunid, Zuraidah Zan, Siti Barirah Ahmad Anas and Mohd. Khazani Abdullah "A Nw Cod for Optical Cod Division Multipl Accss Systms," Malaysian Journal of Computr Scinc, Vol. 17 No., Dcmbr 004, pp [10] Zou Wi, H. Ghafouri-Shiraz, "Cods for Spctral-Amplitud- Coding Optical CDMA Systms," Journal of Lightwav Tchnology, Vol. 50, August 00, pp [11] S. Anuar, S.A. Aljunid, A.Mohammd, E.I.Babkir and N.M.Saad, Dvlopmnt of Zro Cross-Corrlation cod for Spctral-Amplitud Coding Optical cod Division Multipl Accss (OCDMA. Hassan Yousif Ahmd rcivd th B.Eng. in Computr Enginring (Ntwork) and M.Sc in Computr Sinc and Information from Gzira Univrsity, Sudan in 00 and 007 rspctivly. His rsarch intrsts ar on Computr Ntwork, wirlss communications ntworks, optical communications, and h is currntly working toward Ph.D dgr in optical communications, working at Univrsity Tcknolgi PETRONAS dpartmnt of Elctrical and Elctronic, Malaysia I. REFERENCES [1] J. A. Salhi, Cod division multipl accss tchniqus in optical fibr ntwork Par I: Fundamntal principls, IEEE Trans. Commun., vol.37, pp , [] J. A. Salhi and C. A. Bracktt, Cod division multipl accss tchniqus in optical fibr ntwork Part II: Systm prformanc analysis, IEEE Trans. Commun., vol. 37, pp , [3] P. R. Prucnal, M. A. Santoro, and T. R. Fan, Sprad-spctrum fibr-optic local ara ntwork using optical procssing, J. Lightwav Tchnol., vol. LT-4, pp , May [4] A. Stok and E. H. Sargnt, Lighting th local ntwork: Optical cod division multipl accss and quality of srvic

INTERNATIONAL JOURNAL OF COMPUTERS AND COMMUNICATIONS Issue 1, Volume 7, Theoretical Analysis of BER Performance of Optical ZCZ-CDMA System

INTERNATIONAL JOURNAL OF COMPUTERS AND COMMUNICATIONS Issue 1, Volume 7, Theoretical Analysis of BER Performance of Optical ZCZ-CDMA System ITERATIOAL JOURAL OF COMPUTERS AD COMMUICATIOS Issu, Volum 7, 3 Thortical Analysis of BER Prformanc of Optical ZCZ-CDMA Systm Takahiro MATSUMOTO, Hidyuki TORII and Shinya MATSUFUJI Abstract In this papr,

More information

Code Cross-Correlation Effects on the Performance of Optical CDMA Systems in the Presence of Receiver Noises

Code Cross-Correlation Effects on the Performance of Optical CDMA Systems in the Presence of Receiver Noises 0 8th Intrnational Confrnc on Tlcommunications Cod Cross-Corrlation Effcts on th Prformanc of Optical CDMA Systms in th Prsnc of Rcivr Noiss S. M. Zabihi-Maddah M. Molavi Kakhki Faculty of Enginring, Frdowsi

More information

Construction of asymmetric orthogonal arrays of strength three via a replacement method

Construction of asymmetric orthogonal arrays of strength three via a replacement method isid/ms/26/2 Fbruary, 26 http://www.isid.ac.in/ statmath/indx.php?modul=prprint Construction of asymmtric orthogonal arrays of strngth thr via a rplacmnt mthod Tian-fang Zhang, Qiaoling Dng and Alok Dy

More information

(Upside-Down o Direct Rotation) β - Numbers

(Upside-Down o Direct Rotation) β - Numbers Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg

More information

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical

More information

A Propagating Wave Packet Group Velocity Dispersion

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

More information

Procdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is

Procdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is Procdings of IC-IDC0 EFFECTS OF STOCHASTIC PHASE SPECTRUM DIFFERECES O PHASE-OLY CORRELATIO FUCTIOS PART I: STATISTICALLY COSTAT PHASE SPECTRUM DIFFERECES FOR FREQUECY IDICES Shunsu Yamai, Jun Odagiri,

More information

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

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

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

More information

Computing and Communications -- Network Coding

Computing 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 information

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim. MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function

More information

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

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

More information

Function Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0

Function Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0 unction Spacs Prrquisit: Sction 4.7, Coordinatization n this sction, w apply th tchniqus of Chaptr 4 to vctor spacs whos lmnts ar functions. Th vctor spacs P n and P ar familiar xampls of such spacs. Othr

More information

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013 18.782 Introduction to Arithmtic Gomtry Fall 2013 Lctur #20 11/14/2013 20.1 Dgr thorm for morphisms of curvs Lt us rstat th thorm givn at th nd of th last lctur, which w will now prov. Thorm 20.1. Lt φ:

More information

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient Full Wavform Invrsion Using an Enrgy-Basd Objctiv Function with Efficint Calculation of th Gradint Itm yp Confrnc Papr Authors Choi, Yun Sok; Alkhalifah, ariq Ali Citation Choi Y, Alkhalifah (217) Full

More information

Koch Fractal Boundary Single feed Circularly Polarized Microstrip Antenna

Koch Fractal Boundary Single feed Circularly Polarized Microstrip Antenna 1 Journal of Microwavs, Optolctronics and Elctromagntic Applications, Vol. 6, No. 2, Dcmbr 2007 406 Koch Fractal Boundary Singl fd Circularly Polarizd Microstrip Antnna P. Nagswara Rao and N. V. S.N Sarma

More information

Design Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance

Design Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance TECHNICAL NTE 30 Dsign Guidlins for Quartz Crystal scillators Introduction A CMS Pirc oscillator circuit is wll known and is widly usd for its xcllnt frquncy stability and th wid rang of frquncis ovr which

More information

Search sequence databases 3 10/25/2016

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

More information

PHASE-ONLY CORRELATION IN FINGERPRINT DATABASE REGISTRATION AND MATCHING

PHASE-ONLY CORRELATION IN FINGERPRINT DATABASE REGISTRATION AND MATCHING Anall Univrsităţii d Vst din Timişoara Vol. LII, 2008 Sria Fizică PHASE-OLY CORRELATIO I FIGERPRIT DATABASE REGISTRATIO AD ATCHIG Alin C. Tusda, 2 Gianina Gabor Univrsity of Orada, Environmntal Faculty,

More information

The Matrix Exponential

The 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 information

Higher order derivatives

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

More information

Sliding Mode Flow Rate Observer Design

Sliding Mode Flow Rate Observer Design Sliding Mod Flow Rat Obsrvr Dsign Song Liu and Bin Yao School of Mchanical Enginring, Purdu Univrsity, Wst Lafaytt, IN797, USA liu(byao)@purdudu Abstract Dynamic flow rat information is ndd in a lot of

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 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 information

MEASURING HEAT FLUX FROM A COMPONENT ON A PCB

MEASURING HEAT FLUX FROM A COMPONENT ON A PCB MEASURING HEAT FLUX FROM A COMPONENT ON A PCB INTRODUCTION Elctronic circuit boards consist of componnts which gnrats substantial amounts of hat during thir opration. A clar knowldg of th lvl of hat dissipation

More information

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM Elctronic Journal of Diffrntial Equations, Vol. 2003(2003), No. 92, pp. 1 6. ISSN: 1072-6691. URL: http://jd.math.swt.du or http://jd.math.unt.du ftp jd.math.swt.du (login: ftp) LINEAR DELAY DIFFERENTIAL

More information

CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS

CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS Stig Holst ABB Automation Products Swdn Bapuji S Palki ABB Utilitis India This papr rports

More information

1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by:

1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by: Elctromagntic Induction. Lorntz forc on moving charg Point charg moving at vlocity v, F qv B () For a sction of lctric currnt I in a thin wir dl is Idl, th forc is df Idl B () Elctromotiv forc f s any

More information

Quasi-Classical States of the Simple Harmonic Oscillator

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

More information

Two Products Manufacturer s Production Decisions with Carbon Constraint

Two Products Manufacturer s Production Decisions with Carbon Constraint Managmnt Scinc and Enginring Vol 7 No 3 pp 3-34 DOI:3968/jms9335X374 ISSN 93-34 [Print] ISSN 93-35X [Onlin] wwwcscanadant wwwcscanadaorg Two Products Manufacturr s Production Dcisions with Carbon Constraint

More information

Mutually Independent Hamiltonian Cycles of Pancake Networks

Mutually Independent Hamiltonian Cycles of Pancake Networks Mutually Indpndnt Hamiltonian Cycls of Pancak Ntworks Chng-Kuan Lin Dpartmnt of Mathmatics National Cntral Univrsity, Chung-Li, Taiwan 00, R O C discipl@ms0urlcomtw Hua-Min Huang Dpartmnt of Mathmatics

More information

Random Access Techniques: ALOHA (cont.)

Random Access Techniques: ALOHA (cont.) Random Accss Tchniqus: ALOHA (cont.) 1 Exampl [ Aloha avoiding collision ] A pur ALOHA ntwork transmits a 200-bit fram on a shard channl Of 200 kbps at tim. What is th rquirmnt to mak this fram collision

More information

On the irreducibility of some polynomials in two variables

On the irreducibility of some polynomials in two variables ACTA ARITHMETICA LXXXII.3 (1997) On th irrducibility of som polynomials in two variabls by B. Brindza and Á. Pintér (Dbrcn) To th mmory of Paul Erdős Lt f(x) and g(y ) b polynomials with intgral cofficints

More information

Direct Approach for Discrete Systems One-Dimensional Elements

Direct Approach for Discrete Systems One-Dimensional Elements CONTINUUM & FINITE ELEMENT METHOD Dirct Approach or Discrt Systms On-Dimnsional Elmnts Pro. Song Jin Par Mchanical Enginring, POSTECH Dirct Approach or Discrt Systms Dirct approach has th ollowing aturs:

More information

VII. Quantum Entanglement

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

More information

Learning Spherical Convolution for Fast Features from 360 Imagery

Learning Spherical Convolution for Fast Features from 360 Imagery Larning Sphrical Convolution for Fast Faturs from 36 Imagry Anonymous Author(s) 3 4 5 6 7 8 9 3 4 5 6 7 8 9 3 4 5 6 7 8 9 3 3 3 33 34 35 In this fil w provid additional dtails to supplmnt th main papr

More information

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals

More information

SER/BER in a Fading Channel

SER/BER in a Fading Channel SER/BER in a Fading Channl Major points for a fading channl: * SNR is a R.V. or R.P. * SER(BER) dpnds on th SNR conditional SER(BER). * Two prformanc masurs: outag probability and avrag SER(BER). * Ovrall,

More information

Outline. Why speech processing? Speech signal processing. Advanced Multimedia Signal Processing #5:Speech Signal Processing 2 -Processing-

Outline. Why speech processing? Speech signal processing. Advanced Multimedia Signal Processing #5:Speech Signal Processing 2 -Processing- Outlin Advancd Multimdia Signal Procssing #5:Spch Signal Procssing -Procssing- Intllignt Elctronic Systms Group Dpt. of Elctronic Enginring, UEC Basis of Spch Procssing Nois Rmoval Spctral Subtraction

More information

Einstein Equations for Tetrad Fields

Einstein Equations for Tetrad Fields Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for

More information

Problem Set #2 Due: Friday April 20, 2018 at 5 PM.

Problem 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 information

Evaluating Reliability Systems by Using Weibull & New Weibull Extension Distributions Mushtak A.K. Shiker

Evaluating Reliability Systems by Using Weibull & New Weibull Extension Distributions Mushtak A.K. Shiker Evaluating Rliability Systms by Using Wibull & Nw Wibull Extnsion Distributions Mushtak A.K. Shikr مشتاق عبذ الغني شخير Univrsity of Babylon, Collg of Education (Ibn Hayan), Dpt. of Mathmatics Abstract

More information

Analysis and Optimization for Weighted Sum Rate in Energy Harvesting Cooperative NOMA Systems

Analysis and Optimization for Weighted Sum Rate in Energy Harvesting Cooperative NOMA Systems Analysis and Optimization for Wightd Sum Rat in Enrgy Harvsting Cooprativ NOMA Systms Binh Van Nguyn, Quang-Doanh Vu, and Kison Kim arxiv:86.264v [cs.it] 6 Jun 28 Abstract W considr a cooprativ non-orthogonal

More information

4.2 Design of Sections for Flexure

4.2 Design of Sections for Flexure 4. Dsign of Sctions for Flxur This sction covrs th following topics Prliminary Dsign Final Dsign for Typ 1 Mmbrs Spcial Cas Calculation of Momnt Dmand For simply supportd prstrssd bams, th maximum momnt

More information

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

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

More information

Elements of Statistical Thermodynamics

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

More information

Inter-Packet Symbol Approach To Reed-Solomon FEC Codes For RTP-Multimedia Stream Protection

Inter-Packet Symbol Approach To Reed-Solomon FEC Codes For RTP-Multimedia Stream Protection Intr-Packt Symbol Approach To Rd-Solomon FEC Cods For RTP-Multimdia Stram Protction Filippo Casu, Julián Cabrra, Frnando Jaurguizar, Narciso García Grupo d Trataminto d Imágns Univrsidad Politécnica d

More information

Section 11.6: Directional Derivatives and the Gradient Vector

Section 11.6: Directional Derivatives and the Gradient Vector Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th

More information

Discrete Hilbert Transform. Numeric Algorithms

Discrete Hilbert Transform. Numeric Algorithms Volum 49, umbr 4, 8 485 Discrt Hilbrt Transform. umric Algorithms Ghorgh TODORA, Rodica HOLOEC and Ciprian IAKAB Abstract - Th Hilbrt and Fourir transforms ar tools usd for signal analysis in th tim/frquncy

More information

Week 3: Connected Subgraphs

Week 3: Connected Subgraphs Wk 3: Connctd Subgraphs Sptmbr 19, 2016 1 Connctd Graphs Path, Distanc: A path from a vrtx x to a vrtx y in a graph G is rfrrd to an xy-path. Lt X, Y V (G). An (X, Y )-path is an xy-path with x X and y

More information

Problem Set 6 Solutions

Problem Set 6 Solutions 6.04/18.06J Mathmatics for Computr Scinc March 15, 005 Srini Dvadas and Eric Lhman Problm St 6 Solutions Du: Monday, March 8 at 9 PM in Room 3-044 Problm 1. Sammy th Shark is a financial srvic providr

More information

Coupled Pendulums. Two normal modes.

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

More information

On spanning trees and cycles of multicolored point sets with few intersections

On spanning trees and cycles of multicolored point sets with few intersections On spanning trs and cycls of multicolord point sts with fw intrsctions M. Kano, C. Mrino, and J. Urrutia April, 00 Abstract Lt P 1,..., P k b a collction of disjoint point sts in R in gnral position. W

More information

STATISTICAL PROPERTIES ANALYSIS OF Er 3+ -DOPED Ti:LiNbO 3 M -MODE STRAIGHT WAVEGUIDE AMPLIFIERS

STATISTICAL PROPERTIES ANALYSIS OF Er 3+ -DOPED Ti:LiNbO 3 M -MODE STRAIGHT WAVEGUIDE AMPLIFIERS Journal of Optolctronics and Advancd Matrials Vol. 6 No. March 4 p. 63-69 STATISTICAL PROPERTIES ANALYSIS OF Er 3+ -DOPED Ti:LiNbO 3 M -MODE STRAIGHT WAVEGUIDE AMPLIFIERS N. N. Puscas * Physics Dpartmnt

More information

THE IMPACT OF A PRIORI INFORMATION ON THE MAP EQUALIZER PERFORMANCE WITH M-PSK MODULATION

THE IMPACT OF A PRIORI INFORMATION ON THE MAP EQUALIZER PERFORMANCE WITH M-PSK MODULATION 5th Europan Signal Procssing Confrnc (EUSIPCO 007), Poznan, Poland, Sptmbr 3-7, 007, copyright by EURASIP THE IMPACT OF A PRIORI INFORMATION ON THE MAP EQUALIZER PERFORMANCE WITH M-PSK MODULATION Chaabouni

More information

Principles of Humidity Dalton s law

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

More information

Chapter 6. The Discrete Fourier Transform and The Fast Fourier Transform

Chapter 6. The Discrete Fourier Transform and The Fast Fourier Transform Pusan ational Univrsity Chaptr 6. Th Discrt Fourir Transform and Th Fast Fourir Transform 6. Introduction Frquncy rsponss of discrt linar tim invariant systms ar rprsntd by Fourir transform or z-transforms.

More information

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

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

More information

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS It is not possibl to find flu through biggr loop dirctly So w will find cofficint of mutual inductanc btwn two loops and thn find th flu through biggr loop Also rmmbr M = M ( ) ( ) EDT- (JEE) SOLUTIONS

More information

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a 204 Intrnational Confrnc on Computr Scinc and Elctronic Tchnology (ICCSET 204) Rotor Stationary Control Analysis Basd on Coupling KdV Equation Finit Stady Analysis Liu Dalong,a, Xu Lijuan2,a Dpartmnt of

More information

Symmetric centrosymmetric matrix vector multiplication

Symmetric centrosymmetric matrix vector multiplication Linar Algbra and its Applications 320 (2000) 193 198 www.lsvir.com/locat/laa Symmtric cntrosymmtric matrix vctor multiplication A. Mlman 1 Dpartmnt of Mathmatics, Univrsity of San Francisco, San Francisco,

More information

by wavelength modulation of a distributed-feedback laser

by wavelength modulation of a distributed-feedback laser Prformanc analysis of a timdivision-multiplxd fibr-optic gas-snsor array by wavlngth modulation of a distributd-fdback lasr Wi Jin Th rsults of an invstigation of th prformanc of a tim-division-addrssd

More information

Title: Vibrational structure of electronic transition

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

More information

A New Optical Waveguide for Implementation of Multi-wavelengths Narrowband Filters for DWDM Systems

A New Optical Waveguide for Implementation of Multi-wavelengths Narrowband Filters for DWDM Systems IJCSNS Intrnational Journal of Computr Scinc and Ntwork Scurity, VOL.6 No.8B, August 6 39 A Nw Optical Wavguid for Implmntation of Multi-wavlngths Narrowband Filtrs for DWDM Systms A. Rostami [a, b] a)-

More information

Addition of angular momentum

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

More information

Communication Technologies

Communication Technologies Communication Tchnologis. Principls of Digital Transmission. Structur of Data Transmission.2 Spctrum of a Data Signal 2. Digital Modulation 2. Linar Modulation Mthods 2.2 Nonlinar Modulations (CPM-Signals)

More information

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula 7. Intgration by Parts Each drivativ formula givs ris to a corrsponding intgral formula, as w v sn many tims. Th drivativ product rul yilds a vry usful intgration tchniqu calld intgration by parts. Starting

More information

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

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

More information

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002 3.4 Forc Analysis of Linkas An undrstandin of forc analysis of linkas is rquird to: Dtrmin th raction forcs on pins, tc. as a consqunc of a spcifid motion (don t undrstimat th sinificanc of dynamic or

More information

2. Background Material

2. Background Material S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds

More information

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation. Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform

More information

2.3 Matrix Formulation

2.3 Matrix Formulation 23 Matrix Formulation 43 A mor complicatd xampl ariss for a nonlinar systm of diffrntial quations Considr th following xampl Exampl 23 x y + x( x 2 y 2 y x + y( x 2 y 2 (233 Transforming to polar coordinats,

More information

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH.

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH. C:\Dallas\0_Courss\03A_OpSci_67\0 Cgh_Book\0_athmaticalPrliminaris\0_0 Combath.doc of 8 COPUTER GENERATED HOLOGRAS Optical Scincs 67 W.J. Dallas (onday, April 04, 005, 8:35 A) PART I: CHAPTER TWO COB ATH

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

The Equitable Dominating Graph

The Equitable Dominating Graph Intrnational Journal of Enginring Rsarch and Tchnology. ISSN 0974-3154 Volum 8, Numbr 1 (015), pp. 35-4 Intrnational Rsarch Publication Hous http://www.irphous.com Th Equitabl Dominating Graph P.N. Vinay

More information

Note If the candidate believes that e x = 0 solves to x = 0 or gives an extra solution of x = 0, then withhold the final accuracy mark.

Note If the candidate believes that e x = 0 solves to x = 0 or gives an extra solution of x = 0, then withhold the final accuracy mark. . (a) Eithr y = or ( 0, ) (b) Whn =, y = ( 0 + ) = 0 = 0 ( + ) = 0 ( )( ) = 0 Eithr = (for possibly abov) or = A 3. Not If th candidat blivs that = 0 solvs to = 0 or givs an tra solution of = 0, thn withhold

More information

Dynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA *

Dynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA * 17 nd Intrnational Confrnc on Mchanical Control and Automation (ICMCA 17) ISBN: 978-1-6595-46-8 Dynamic Modlling of Hoisting Stl Wir Rop Da-zhi CAO, Wn-zhng DU, Bao-zhu MA * and Su-bing LIU Xi an High

More information

Davisson Germer experiment

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

More information

Phase Rotation for the 80 MHz ac Mixed Mode Packet

Phase 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 information

10. The Discrete-Time Fourier Transform (DTFT)

10. The Discrete-Time Fourier Transform (DTFT) Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w

More information

DIFFERENTIAL EQUATION

DIFFERENTIAL EQUATION MD DIFFERENTIAL EQUATION Sllabus : Ordinar diffrntial quations, thir ordr and dgr. Formation of diffrntial quations. Solution of diffrntial quations b th mthod of sparation of variabls, solution of homognous

More information

Addition of angular momentum

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

More information

Rational Approximation for the one-dimensional Bratu Equation

Rational Approximation for the one-dimensional Bratu Equation Intrnational Journal of Enginring & Tchnology IJET-IJES Vol:3 o:05 5 Rational Approximation for th on-dimnsional Bratu Equation Moustafa Aly Soliman Chmical Enginring Dpartmnt, Th British Univrsity in

More information

Recursive Estimation of Dynamic Time-Varying Demand Models

Recursive Estimation of Dynamic Time-Varying Demand Models Intrnational Confrnc on Computr Systms and chnologis - CompSysch 06 Rcursiv Estimation of Dynamic im-varying Dmand Modls Alxandr Efrmov Abstract: h papr prsnts an implmntation of a st of rcursiv algorithms

More information

u 3 = u 3 (x 1, x 2, x 3 )

u 3 = u 3 (x 1, x 2, x 3 ) Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.

More information

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon.

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon. PART I TRUE/FALSE/UNCERTAIN (5 points ach) 1. Lik xpansionary montary policy, xpansionary fiscal policy rturns output in th mdium run to its natural lvl, and incrass prics. Thrfor, fiscal policy is also

More information

Basic Polyhedral theory

Basic Polyhedral theory Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist

More information

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN Intrnational Journal of Scintific & Enginring Rsarch, Volum 6, Issu 7, July-25 64 ISSN 2229-558 HARATERISTIS OF EDGE UTSET MATRIX OF PETERSON GRAPH WITH ALGEBRAI GRAPH THEORY Dr. G. Nirmala M. Murugan

More information

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming CPSC 665 : An Algorithmist s Toolkit Lctur 4 : 21 Jan 2015 Lcturr: Sushant Sachdva Linar Programming Scrib: Rasmus Kyng 1. Introduction An optimization problm rquirs us to find th minimum or maximum) of

More information

5.80 Small-Molecule Spectroscopy and Dynamics

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

More information

1 Minimum Cut Problem

1 Minimum Cut Problem CS 6 Lctur 6 Min Cut and argr s Algorithm Scribs: Png Hui How (05), Virginia Dat: May 4, 06 Minimum Cut Problm Today, w introduc th minimum cut problm. This problm has many motivations, on of which coms

More information

Topology Optimization of Suction Muffler for Noise Attenuation

Topology Optimization of Suction Muffler for Noise Attenuation Purdu Univrsity Purdu -Pubs Intrnational Comprssor Enginring Confrnc School of Mchanical Enginring 2012 Topology Optimization of Suction Mufflr for Nois Attnuation Jin Woo L jinwool@ajou.ac.kr Dong Wook

More information

Improvement of Rotation Matrix Based Differential Limited Feedback with DFT Codebook and Its Application in CoMP Environment

Improvement of Rotation Matrix Based Differential Limited Feedback with DFT Codebook and Its Application in CoMP Environment Improvmnt of Rotation Matrix Basd Diffrntial Limitd Fdback with DFT Codbook and Its Application in CoMP Environmnt Yin Zhu, Yushng Ji, Ping Wang, and Fuqiang Liu Broadband Wirlss Communications and Multimdia

More information

The influence of electron trap on photoelectron decay behavior in silver halide

The influence of electron trap on photoelectron decay behavior in silver halide Th influnc of lctron trap on photolctron dcay bhavior in silvr halid Rongjuan Liu, Xiaowi Li 1, Xiaodong Tian, Shaopng Yang and Guangshng Fu Collg of Physics Scinc and Tchnology, Hbi Univrsity, Baoding,

More information

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

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

More information

Bit-Loading Algorithms for OFDM with Adaptive Cyclic Prefix Length in PLC Channels

Bit-Loading Algorithms for OFDM with Adaptive Cyclic Prefix Length in PLC Channels Bit-Loading Algorithms for OFD with Adaptiv Cyclic Prfix Lngth in PLC Channls Salvator D Alssandro (), Andra. Tonllo (), and Lutz Lamp (3) (,) DIEG - Univrsità di Udin, Udin, Italy, -mail: salvator.dalssandro@uniud.it,

More information

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation Diffrnc -Analytical Mthod of Th On-Dimnsional Convction-Diffusion Equation Dalabav Umurdin Dpartmnt mathmatic modlling, Univrsity of orld Economy and Diplomacy, Uzbistan Abstract. An analytical diffrncing

More information

Robust surface-consistent residual statics and phase correction part 2

Robust surface-consistent residual statics and phase correction part 2 Robust surfac-consistnt rsidual statics and phas corrction part 2 Ptr Cary*, Nirupama Nagarajappa Arcis Sismic Solutions, A TGS Company, Calgary, Albrta, Canada. Summary In land AVO procssing, nar-surfac

More information

Numerical considerations regarding the simulation of an aircraft in the approaching phase for landing

Numerical considerations regarding the simulation of an aircraft in the approaching phase for landing INCAS BULLETIN, Volum, Numbr 1/ 1 Numrical considrations rgarding th simulation of an aircraft in th approaching phas for landing Ionl Cristinl IORGA ionliorga@yahoo.com Univrsity of Craiova, Alxandru

More information

EE140 Introduction to Communication Systems Lecture 2

EE140 Introduction to Communication Systems Lecture 2 EE40 Introduction to Communication Systms Lctur 2 Instructor: Prof. Xiliang Luo ShanghaiTch Univrsity, Spring 208 Architctur of a Digital Communication Systm Transmittr Sourc A/D convrtr Sourc ncodr Channl

More information

Square of Hamilton cycle in a random graph

Square of Hamilton cycle in a random graph Squar of Hamilton cycl in a random graph Andrzj Dudk Alan Friz Jun 28, 2016 Abstract W show that p = n is a sharp thrshold for th random graph G n,p to contain th squar of a Hamilton cycl. This improvs

More information