Recursive Implementation of Anisotropic Filters
|
|
- Mark Lindsey
- 5 years ago
- Views:
Transcription
1 Rcursiv Implmtatio of Aisotropic Filtrs Zu Yu Dpartmt of Computr Scic, Uivrsit of Tas at Austi Abstract Gaussia filtr is widl usd for imag smoothig but it is wll kow that this tp of filtrs blur th imag faturs.g., dgs. Two tsios of Gaussia filtrs will b discussd i this surv. O is th aisotropic filtrig bilatral filtrig or PDE-basd aisotropic diffusio for fatur-prsrvig smoothig ad th othr is th rcursiv implmtatio of various filtrs that ca largl rduc th computatioal tim i crtai coditios. W will also discuss th combiatio of aisotropic filtrig ad rcursiv implmtatio for imag smoothig such that th aisotropic smoothig could b do i a fast wa.. Itroductio Nois is commol s i ma tps of imags for ampl, biomdical imags ad rmot ssig imags. It is i a grat dmad to smooth th imags bfor othr tasks could b coductd. Gaussia lowpass filtrig is kow to b a fficit ad simpl wa for imag smoothig. Howvr, it is wll kow that Gaussia filtrig blurs th imag dgs whil smoothig imag ois. Th raso is that Gaussia filtrs ar isotropic i th ss that all surroudig pils affct th ctr pil i a similar fashio rgardlss thir itsit variatios. Hc, th dgs ad th ois ar tratd i th sam wa, which ilds ois rductio as wll as dg blurrig. A ampl of such ffct ca b s from Fig. b. To rmd th problm of traditioal Gaussia filtrig, popl hav proposd lots of mthods, trig to achiv th goal of fatur-prsrvig smoothig. All of ths mthods ar calld aisotropic filtrig ad ca b groupd ito two catgoris. O is calld Bilatral Filtrig [7,, 3], which is a straightforward tsio of Gaussia filtrig. Th othr is a PDE-basd tchiqu, calld aisotropic hat diffusio [4, 8]. W shall s mor dtails o th various tchiqus o ths topics i th followig sctios. I Fig. c,
2 w show a ampl of bilatral filtrig o th sam ois imag. W ca clarl s th diffrc btw th isotropic filtrig ad th aisotropic filtrig. Obviousl th lattr o givs bttr rsults. Aothr importat issu rgardig imag filtrig is th implmtatio of th various filtrs. Gaussia low-pass filtrig ca b implmtd b dirct covolutio, which is furthr acclratd b FFT. Aisotropic filtrs, howvr, ar grall much mor tim-cosumig although som authors studid fast algorithms for bilatral filtrig []. Aothr fast wa for implmtig Gaussia filtrig is b rcursiv schm [5, 6]. Rcursiv implmtatio rquirs a costat ad small umbr of MADDs multiplicatios ad additios rgardlss th siz of th ighborhood big cosidrd. Hc, th tim complit of rcursiv implmtatio of Gaussia filtrig is quit small compard to othr squtial algorithms of Gaussia filtrig [5]. Howvr, th rcursiv schm was origiall dsigd for isotropic Gaussia filtrig ad littl work has b do o combiig th rcursiv schm ad th aisotropic filtrig. I this projct our goal is to plor th possibilit of applig th rcursiv implmtatio tchiqu o th aisotropic filtrig. This surv is orgaizd as follows. W shall bgi i t sctio b rviwig various tchiqus for aisotropic imag smoothig. Th i Sctio 3, w shall giv a brif dscriptio of various rcursiv tchiqus that hav b s i litraturs. I Sctio 4 w will s som prvious work that combis th rcursiv tchiqus ad aisotropic filtrig ad our proposd approach will b brifl dscribd i Sctio 5. Fiall w giv our coclusio i Sctio 6. Origial Nois Imag Isotropic Filtrig Aisotropic Filtrig Figur Eampl of isotropic Gaussia filtrig ad aisotropic filtrig o a mdical imag.
3 . Aisotropic Filtrs Aisotropic filtrig is grall rprstd i two diffrt was. O is b bilatral filtrig [7] ad th othr is b PDE-basd aisotropic hat diffusio [4]. I th followig w will dscrib both was o b o ad latr o th clos rlatioship btw ths approachs will b show. Th bilatral filtrig [7] is a straightforward tsio of Gaussia low-pass filtrig. As w kow, th Gaussia filtrig is dfid b a fuctio as follows: g σ,, πσ whr σ is a giv valu, kow as stadard dviatio. It is obvious that this fuctio is isotropic with rspct to th ctr. Thrfor, a dirct us of this fuctio o th ois imags will rsult i blurrd dgs sic this fuctio ol cosidrs th spatial iformatio without cosidrig th imag iformatio aroud th ctr. Th basic ida of bilatral filtrig is to add a additioal trm to th wightig fuctio i such that th imag iformatio is tak ito accout: g', f, f 0,0 σ d σ c, whr σ d ad σ c ar prst paramtrs. Th ampl i th followig figur, rproducd from [], shows th diffrc btw th Gaussia filtrig show i b ad th bilatral filtrig show i d. a b c d Figur Illustratio of bilatral filtrig []. I a w show a ampl of ois imag ad th spatial krl Gaussia fuctio g, is show i b. Th imag-rlatd wightig fuctio scod trm i g, is show i c. Th combid wightig fuctio g, i d shows a aisotropic proprt.
4 Rctl a fast implmtatio of bilatral filtrig was proposd b Durad t al []. Th acclratd th bilatral filtrig b usig a picwis-liar approimatio i th itsit domai ad appropriat subsamplig. Elad [3] discussd th bilatral filtrig from a liar algbra poit of viw ad poitd out som possibl was to improv it. Aothr commol s tchiqu to raliz aisotropic filtrig is dfid b hat diffusio quatios. Th first modl about th aisotropic diffusio is wll kow as Proa-Malik modl as s i [4]. Proa- Malik modl is dfid b a o-liar PDE hat diffusio as follows [4]: u t div g u u 3 whr g. is a positiv o-icrasig fuctio which supprsss diffusio aroud imag dgs whr th orm of th gradit is high. A commo choic for g. is giv b g s K s 4 whr K is a prst costat. Strictl spakig, howvr, Proa-Malik modl is ot a aisotropic diffusio modl sic th wightig fuctio g. is just a scalar fuctio, which dos ot idicat th aisotropic diffusio aroud a poit. A tru aisotropic diffusio modl was discussd b J. Wickrt [8], who dfid th diffusio PDE as follows: u t div D u u 5 whr D. is dfid as a tsor of u. This matri givs a dirctio whr th diffusio is prfrrd ad aothr dirctio whr th diffusio is supprssd. Similar to th rlatioship btw Gaussia filtrig ad liar hat diffusio, thr is also a clos rlatioship btw bilatral filtrig ad PDE-basd aisotropic hat diffusio as discussd i []. Both bilatral filtrig ad aisotropic hat diffusio ar quit tim-cosumig to implmt. I th followig sctios w will s o of th stratgis to rduc th computatioal tim of both tps of filtrs b usig rcursiv implmtatio.
5 3. Rcursiv Implmtatio Th rcursiv implmtatio of svral tps of filtrs had b discussd i litraturs. I [,, 3], Drich studid th rcursiv implmtatio of svral tps of filtrs with potial wightig fuctios. I [3], Th author discussd two tps of filtrs. O is calld scod ordr rcursiv filtr dfid b:, 6 k S whr is a prst costat ad k is chos as k 7 such that. S Assum th iput sigal ad output sigal ar ad, rspctivl. Th th rcursiv ralizatio of th filtrig with covolutio mask dfid b 6 is drivd b th followig causal ad ati-causal squcs:, 8 k k It is clar that th abov rcursiv implmtatio of such filtr rquirs 8 multiplicatios ad 7 additios pr output pil. This fact idicats th computatioal advatag of rcursiv implmtatio of filtrs. I [3], th authors also discussd th rcursiv ralizatios of th first ordr filtr ad th drivativs of both first ordr ad scod ordr filtrs. Th claimd that thir rcursiv implmtatio of filtrs is much computatioall fastr tha th o-rcursiv implmtatio if o paralllism is cosidrd. Howvr, as poitd out i [5], all th rcursiv implmtatios s i [,, 3] ar basd o o- Gaussia filtrig, that is, th ar all basd o filtrs dfid b potiall wightig fuctios. Thrfor, th do ot hav th imprssiv proprtis that Gaussia filtrs hav. For ampl, th
6 potiall dfid filtrs ar ot isotropic i D, ot circularl smmtric. I [5], th authors proposd a rcursiv implmtatio of th Gaussia filtr. Thir approach is basd o a ratioal approimatio of th Gaussia fuctio giv b: t / g t 4 π a a t a t a t ε t 9 whr a , a , a ad a Th rror ε t is provd to b limitd to ε t < Accordig to th ratioal approimatio of th Gaussia fuctio, o ca driv th followig rcursiv implmtatio of Gaussia filtrig: forward : backward w B B w bw b b w b b b 0 0 b w 3 b whr B b b b b ad b, b b ar costats drivd from th stadard dviatio σ of th 3 / 0, 3 Gaussia filtr. It was claimd i [5] that th abov rcursiv implmtatio of th Gaussia filtr ol rquirs 6 MADDs multiplicatios ad additios pr output pil. It is fastr tha th rcursiv schm s i Eq. 8 ad furthrmor, it givs a mor isotropic circularl smmtric impuls rspos [5]. Now w giv a short summar o th tim complit of som of th abov algorithms. Assum th siz of th imag big cosidrd is N N ad th siz of th mask widow is M M. Algorithms Tim Complit Gaussia low-pass filtrig dirct covolutio O N M Bilatral filtrig [7] O N M Proa-Malik modl [4] O N K, whr K is umbr of itratios Rcursiv implmtatio of potial filtr [3] Rcursiv implmtatio of Gaussia filtr [5] 8 MADDs multiplicatios ad additios pr pil 6 MADDs multiplicatios ad additios pr pil Not: Accordig to [5], th rcursiv implmtatio s i 0 is fastr tha FFT-basd Gaussia lowpass filtrig.
7 4. Rcursiv Implmtatio of Aisotropic Filtrs Rcursiv implmtatio of aisotropic filtrs is th mai goal of this projct. As far as I kow, thr hav b svral paprs dalig with this issu. Th first papr is th o b Alvarz t al. [9, 0], who discussd th rcursiv ralizatio of th oliar vrsio of th potial filtrs as s i Eq. 6. Th ida is that, istad of usig costat paramtr, w ca cosidr a varig paramtr o th orm of th drivativ of th iput sigal., which dpds h t, t whr h. is a o-dcrasig fuctio with h 0 ε > 0. For simplicit, th authors i [9, 0] chos h. as a liar fuctio: h s ε M s, whr M is a positiv costat. W ow show som simulatio rsults that ar rproducd from [9]. I Fig. 3, w show th rsults b th approach s i [9, 0]. W ca s that as M gos smallr ad smallr, th smoothd imags bcom mor ad mor blurrd. I Fig. 4, w show th simulatio rsults b Proa-Malik modl [4]. From all ths imags, w ca s that th rcursiv implmtatio ca grat rsults as good as thos w s i Proa- Malik modl but th rcursiv implmtatio clarl rquirs much lss computatioal tim. I [5, 6], th authors discussd th rcursiv implmtatio of th act Gaussia filtr. Th D Gaussia fuctio th cosidrd could b aisotropic i th ss that th pricipal ais of th Gaussia fuctio could b i a oritatio ad th associatd dviatios σ u ad σ v could hav a aspct Iput imag M 0.5 M 0. M 0.05 Figur 3 Th simulatio rsults b th approach s i [9, 0]. Rproducd from [9]
8 Iput imag K 0 K 0 K 50 Figur 4 Th simulatio rsults b th Proa-Malik approach s i [4]. Rproducd from [9] ratio. Howvr, th assumd th Gaussia fuctio to b uiforml applid i vrwhr of th imag. Thrfor, thir mthod ca ol b usd to smooth or dtct th lis with a spcific oritatio. This assumptio is crtail ivalid for imag smoothig with arbitraril oritd faturs. 5. Proposd Approach W hav s th two tsios of Gaussia filtrig. O is aisotropic filtrig for highr smoothig qualit ad th othr is rcursiv implmtatio of filtrs for lss computatioal tim. Th goal of this projct is to combi ths two tsios togthr such that a fast implmtatio of aisotropic filtrs could b possibl. Although w hav s som prvious work o this issu, it is still itrstig to go furthr i this dirctio. Our ida is to dsig a aisotropic vrsio of th rcursiv filtrs as discussd i [5, 6]. Our mthod will b quit similar to th o usd i [9, 0] ad th ida is also b rplacig th costat propagatio paramtrs with varig paramtrs. Howvr, sic th filtrs that w ar goig to work o ar diffrt from that s i [9, 0], th dtaild approach is pctd to b diffrt ad th rsultig impuls rspos as wll as th primtal rsults should also b diffrt. 6. Coclusio I this rport w rviwd som prvious work o two tsios of th classic Gaussia filtrs. O is th aisotropic filtrig ad th othr is rcursiv implmtatio of filtrs. W also saw som work that combid ths two tsios togthr, ildig a rcursiv implmtatio of aisotropic filtrs. W
9 propos a approach that is rlatd to th rcursiv implmtatio of th Gaussia filtr [5, 6] ad th rcursiv implmtatio of aisotropic potial filtr [9, 0]. Mor dtails will b availabl soo. Rfrcs [] R. Drich, Optimal dg dtctio usig rcursiv filtrig, Procdig of st Itratioal Cofrc o Computr Visio, Lodo, Ju 8-, 987. [] R. Drich, Usig Ca's critria to driv a rcursivl implmtd optimal dg dtctor, Itratioal Joural of Computr Visio, vol., o., pp , Ma 987. [3] R. Drich, Fast algorithms for low-lvl visio, IEEE Tras. Pattr Aalsis ad Machi Itlligc, vol., o., pp 78-87, 990. [4] P. Proa, J. Malik, Scal-spac ad dg dtctio usig aisotropic diffusio, IEEE Tras. o Pattr Aalsis ad Machi Itlligc, vol., o. 7, pp , 990. [5] I.T. Youg, L.J. Vlit, Rcursiv implmtatio of th Gaussia filtr, Sigal Procssig, vol. 44, pp. 39-5, 995. [6] L.J. Vlit, I.T. Youg ad P.W. Vrbk, Rcursiv Gaussia drivativ filtrs, Procdigs of th 4th Itratioal Cofrc o Pattr Rcogitio, vol., pp , Brisba, Australia, 6-0 August 998. [7] C. Tomasi ad R. Maduchi, Bilatral filtrig for gra ad color imags, I Proc. IEEE It. Cof. o Computr Visio, pp , 998. [8] J. Wickrt, Aisotropic Diffusio I Imag Procssig, ECMI Sris, Tubr, Stuttgart, ISBN , 998. [9] L. Alvarz, R. Drich ad F. Sataa, "Rcursivit ad PDE's i Imag Procssig", Uivrsidad d Las Palmas d G.C. Tchical Rport availabl oli at: Octobr 999. [0] L. Alvarz, R. Drich ad F. Sataa, Rcursivit ad PDE's i imag procssig, Proc. Itratioal Cofrc o Pattr Rcogitio, vol., pp. 4-48, Barcloa, Spai, Sptmbr, 000. [] D. Barash, A fudamtal rlatioship btw bilatral filtrig, adaptiv smoothig ad th oliar diffusio quatio, IEEE Tras. Pattr Aalsis ad Machi Itlligc, vol. 4, o. 6, pp , Ju 00. [] F. Durad ad J. Dors, Fast bilatral filtrig for th displa of high-damic-rag imags, I Proc. ACM Cofrc o Computr Graphics SIGGRAPH, pp , 00. [3] M. Elad, O th bilatral filtr ad was to improv it, IEEE Trasactios O Imag Procssig, vol., o. 0, pp. 4-5, Octobr 00. [4] I.T. Youg, L.J.va Vlit ad M.va Gikl, Rcursiv Gabor filtrig, IEEE Tras. Sigal Procssig, vol. 50, No., Novmbr 00. [5] J.M. Gusbrok, A.W.M. Smuldrs, ad J. va d Wijr. Fast aisotropic Gauss filtrig. Proc. 7th Europa Cofrc o Computr Visio A. Hd, G. Sparr, M. Nils, ad P. Johas, ditors, volum, pags 99-. Sprigr Vrlag LNCS 350, Cophag, Dmark, 00. [6] J.M. Gusbrok, A.W.M. Smuldrs, ad J. va d Wijr. Fast aisotropic Gauss filtrig. IEEE Tras. Imag Procssig, accptd, 003.
Discrete 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 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 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 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 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 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 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 informationChapter Taylor Theorem Revisited
Captr 0.07 Taylor Torm Rvisitd Atr radig tis captr, you sould b abl to. udrstad t basics o Taylor s torm,. writ trascdtal ad trigoomtric uctios as Taylor s polyomial,. us Taylor s torm to id t valus o
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 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 informationA Novel Approach to Recovering Depth from Defocus
Ssors & Trasducrs 03 by IFSA http://www.ssorsportal.com A Novl Approach to Rcovrig Dpth from Dfocus H Zhipa Liu Zhzhog Wu Qiufg ad Fu Lifag Collg of Egirig Northast Agricultural Uivrsity 50030 Harbi Chia
More informationStatistics 3858 : Likelihood Ratio for Exponential Distribution
Statistics 3858 : Liklihood Ratio for Expotial Distributio I ths two xampl th rjctio rjctio rgio is of th form {x : 2 log (Λ(x)) > c} for a appropriat costat c. For a siz α tst, usig Thorm 9.5A w obtai
More informationUNIT 2: MATHEMATICAL ENVIRONMENT
UNIT : MATHEMATICAL ENVIRONMENT. Itroductio This uit itroducs som basic mathmatical cocpts ad rlats thm to th otatio usd i th cours. Wh ou hav workd through this uit ou should: apprciat that a mathmatical
More information3 Error Equations for Blind Equalization Schemes
3 Error Equatios or Blid Equalizatio Schms I this sctio dirt rror quatios or blid qualizatio will b aalzd. Basd o this aalsis a suitabl rror quatio will b suggstd aimd at providig bttr prormac. Th modl
More informationChapter (8) Estimation and Confedence Intervals Examples
Chaptr (8) Estimatio ad Cofdc Itrvals Exampls Typs of stimatio: i. Poit stimatio: Exampl (1): Cosidr th sampl obsrvatios, 17,3,5,1,18,6,16,10 8 X i i1 17 3 5 118 6 16 10 116 X 14.5 8 8 8 14.5 is a poit
More informationThe Interplay between l-max, l-min, p-max and p-min Stable Distributions
DOI: 0.545/mjis.05.4006 Th Itrplay btw lma lmi pma ad pmi Stabl Distributios S Ravi ad TS Mavitha Dpartmt of Studis i Statistics Uivrsity of Mysor Maasagagotri Mysuru 570006 Idia. Email:ravi@statistics.uimysor.ac.i
More informationPage 1. Before-After Control-Impact (BACI) Power Analysis For Several Related Populations (Variance Known) Richard A. Hinrichsen. September 24, 2010
Pag for-aftr Cotrol-Impact (ACI) Powr Aalysis For Svral Rlatd Populatios (Variac Kow) Richard A. Hirichs Sptmbr 4, Cavat: This primtal dsig tool is a idalizd powr aalysis built upo svral simplifyig assumptios
More information6. Comparison of NLMS-OCF with Existing Algorithms
6. Compariso of NLMS-OCF with Eistig Algorithms I Chaptrs 5 w drivd th NLMS-OCF algorithm, aalyzd th covrgc ad trackig bhavior of NLMS-OCF, ad dvlopd a fast vrsio of th NLMS-OCF algorithm. W also mtiod
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 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 informationINTRODUCTION TO SAMPLING DISTRIBUTIONS
http://wiki.stat.ucla.du/socr/id.php/socr_courss_2008_thomso_econ261 INTRODUCTION TO SAMPLING DISTRIBUTIONS By Grac Thomso INTRODUCTION TO SAMPLING DISTRIBUTIONS Itro to Samplig 2 I this chaptr w will
More informationBipolar Junction Transistors
ipolar Juctio Trasistors ipolar juctio trasistors (JT) ar activ 3-trmial dvics with aras of applicatios: amplifirs, switch tc. high-powr circuits high-spd logic circuits for high-spd computrs. JT structur:
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 informationInternational Journal of Advanced and Applied Sciences
Itratioal Joural of Advacd ad Applid Scics x(x) xxxx Pags: xx xx Cotts lists availabl at Scic Gat Itratioal Joural of Advacd ad Applid Scics Joural hompag: http://wwwscic gatcom/ijaashtml Symmtric Fuctios
More informationAn Introduction to Asymptotic Expansions
A Itroductio to Asmptotic Expasios R. Shaar Subramaia Dpartmt o Chmical ad Biomolcular Egirig Clarso Uivrsit Asmptotic xpasios ar usd i aalsis to dscrib th bhavior o a uctio i a limitig situatio. Wh a
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 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 informationEmpirical Study in Finite Correlation Coefficient in Two Phase Estimation
M. Khoshvisa Griffith Uivrsity Griffith Busiss School Australia F. Kaymarm Massachustts Istitut of Tchology Dpartmt of Mchaical girig USA H. P. Sigh R. Sigh Vikram Uivrsity Dpartmt of Mathmatics ad Statistics
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 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 informationCDS 101: Lecture 5.1 Reachability and State Space Feedback
CDS, Lctur 5. CDS : Lctur 5. Rachability ad Stat Spac Fdback Richard M. Murray 7 Octobr 3 Goals: Di rachability o a cotrol systm Giv tsts or rachability o liar systms ad apply to ampls Dscrib th dsig o
More informationJournal of Modern Applied Statistical Methods
Joural of Modr Applid Statistical Mthods Volum Issu Articl 6 --03 O Som Proprtis of a Htrogous Trasfr Fuctio Ivolvig Symmtric Saturatd Liar (SATLINS) with Hyprbolic Tagt (TANH) Trasfr Fuctios Christophr
More informationNEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES
Digst Joural of Naomatrials ad Biostructurs Vol 4, No, March 009, p 67-76 NEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES A IRANMANESH a*, O KHORMALI b, I NAJAFI KHALILSARAEE c, B SOLEIMANI
More informationCDS 101: Lecture 5.1 Reachability and State Space Feedback
CDS, Lctur 5. CDS : Lctur 5. Rachability ad Stat Spac Fdback Richard M. Murray ad Hido Mabuchi 5 Octobr 4 Goals: Di rachability o a cotrol systm Giv tsts or rachability o liar systms ad apply to ampls
More informationComparison of Simple Indicator Kriging, DMPE, Full MV Approach for Categorical Random Variable Simulation
Papr 17, CCG Aual Rport 11, 29 ( 29) Compariso of Simpl Idicator rigig, DMPE, Full MV Approach for Catgorical Radom Variabl Simulatio Yupg Li ad Clayto V. Dutsch Ifrc of coditioal probabilitis at usampld
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 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 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 informationPage 1 BACI. Before-After-Control-Impact Power Analysis For Several Related Populations (Variance Known) October 10, Richard A.
Pag BACI Bfor-Aftr-Cotrol-Impact Powr Aalysis For Svral Rlatd Populatios (Variac Kow) Octobr, 3 Richard A. Hirichs Cavat: This study dsig tool is for a idalizd powr aalysis built upo svral simplifyig assumptios
More informationChapter 6: DFT/FFT Transforms and Applications 6.1 DFT and its Inverse
6. Chaptr 6: DFT/FFT Trasforms ad Applicatios 6. DFT ad its Ivrs DFT: It is a trasformatio that maps a -poit Discrt-tim DT) sigal ] ito a fuctio of th compl discrt harmoics. That is, giv,,,, ]; L, a -poit
More informationFolding of Hyperbolic Manifolds
It. J. Cotmp. Math. Scics, Vol. 7, 0, o. 6, 79-799 Foldig of Hyprbolic Maifolds H. I. Attiya Basic Scic Dpartmt, Collg of Idustrial Educatio BANE - SUEF Uivrsity, Egypt hala_attiya005@yahoo.com Abstract
More informationLearning objectives. Three models of aggregate supply. 1. The sticky-wage model 2. The imperfect-information model 3. The sticky-price model
Larig objctivs thr modls of aggrgat supply i which output dpds positivly o th pric lvl i th short ru th short-ru tradoff btw iflatio ad umploymt kow as th Phillips curv Aggrgat Supply slid 1 Thr modls
More information2617 Mark Scheme June 2005 Mark Scheme 2617 June 2005
Mark Schm 67 Ju 5 GENERAL INSTRUCTIONS Marks i th mark schm ar plicitly dsigatd as M, A, B, E or G. M marks ("mthod" ar for a attmpt to us a corrct mthod (ot mrly for statig th mthod. A marks ("accuracy"
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 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 informationEuler s Method for Solving Initial Value Problems in Ordinary Differential Equations.
Eulr s Mthod for Solvig Iitial Valu Problms i Ordiar Diffrtial Equatios. Suda Fadugba, M.Sc. * ; Bosd Ogurid, Ph.D. ; ad Tao Okulola, M.Sc. 3 Dpartmt of Mathmatical ad Phsical Scics, Af Babalola Uivrsit,
More informationSearch 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 informationmacro Road map to this lecture Objectives Aggregate Supply and the Phillips Curve Three models of aggregate supply W = ω P The sticky-wage model
Road map to this lctur macro Aggrgat Supply ad th Phillips Curv W rlax th assumptio that th aggrgat supply curv is vrtical A vrsio of th aggrgat supply i trms of iflatio (rathr tha th pric lvl is calld
More informationSTIRLING'S 1 FORMULA AND ITS APPLICATION
MAT-KOL (Baja Luka) XXIV ()(08) 57-64 http://wwwimviblorg/dmbl/dmblhtm DOI: 075/МК80057A ISSN 0354-6969 (o) ISSN 986-588 (o) STIRLING'S FORMULA AND ITS APPLICATION Šfkt Arslaagić Sarajvo B&H Abstract:
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 informationOn a problem of J. de Graaf connected with algebras of unbounded operators de Bruijn, N.G.
O a problm of J. d Graaf coctd with algbras of uboudd oprators d Bruij, N.G. Publishd: 01/01/1984 Documt Vrsio Publishr s PDF, also kow as Vrsio of Rcord (icluds fial pag, issu ad volum umbrs) Plas chck
More informationGlobal Chaos Synchronization of the Hyperchaotic Qi Systems by Sliding Mode Control
Dr. V. Sudarapadia t al. / Itratioal Joural o Computr Scic ad Egirig (IJCSE) Global Chaos Sychroizatio of th Hyprchaotic Qi Systms by Slidig Mod Cotrol Dr. V. Sudarapadia Profssor, Rsarch ad Dvlopmt Ctr
More informationEinstein 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 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 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 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 informationTechnical Support Document Bias of the Minimum Statistic
Tchical Support Documt Bias o th Miimum Stattic Itroductio Th papr pla how to driv th bias o th miimum stattic i a radom sampl o siz rom dtributios with a shit paramtr (also kow as thrshold paramtr. Ths
More informationNew Sixteenth-Order Derivative-Free Methods for Solving Nonlinear Equations
Amrica Joural o Computatioal ad Applid Mathmatics 0 (: -8 DOI: 0.59/j.ajcam.000.08 Nw Sixtth-Ordr Drivativ-Fr Mthods or Solvig Noliar Equatios R. Thukral Padé Rsarch Ctr 9 Daswood Hill Lds Wst Yorkshir
More informationTraveling Salesperson Problem and Neural Networks. A Complete Algorithm in Matrix Form
Procdigs of th th WSEAS Itratioal Cofrc o COMPUTERS, Agios Nikolaos, Crt Islad, Grc, July 6-8, 7 47 Travlig Salsprso Problm ad Nural Ntworks A Complt Algorithm i Matrix Form NICOLAE POPOVICIU Faculty of
More informationNET/JRF, GATE, IIT JAM, JEST, TIFR
Istitut for NET/JRF, GATE, IIT JAM, JEST, TIFR ad GRE i PHYSICAL SCIENCES Mathmatical Physics JEST-6 Q. Giv th coditio φ, th solutio of th quatio ψ φ φ is giv by k. kφ kφ lφ kφ lφ (a) ψ (b) ψ kφ (c) ψ
More information2.29 Numerical Fluid Mechanics Spring 2015 Lecture 12
REVIEW Lctur 11: Numrical Fluid Mchaics Sprig 2015 Lctur 12 Fiit Diffrcs basd Polyomial approximatios Obtai polyomial (i gral u-qually spacd), th diffrtiat as dd Nwto s itrpolatig polyomial formulas Triagular
More informationTriple Play: From De Morgan to Stirling To Euler to Maclaurin to Stirling
Tripl Play: From D Morga to Stirlig To Eulr to Maclauri to Stirlig Augustus D Morga (186-1871) was a sigificat Victoria Mathmaticia who mad cotributios to Mathmatics History, Mathmatical Rcratios, Mathmatical
More informationOrdinary Differential Equations
Basi Nomlatur MAE 0 all 005 Egirig Aalsis Ltur Nots o: Ordiar Diffrtial Equatios Author: Profssor Albrt Y. Tog Tpist: Sakurako Takahashi Cosidr a gral O. D. E. with t as th idpdt variabl, ad th dpdt variabl.
More informationNormal Form for Systems with Linear Part N 3(n)
Applid Mathmatics 64-647 http://dxdoiorg/46/am7 Publishd Oli ovmbr (http://wwwscirporg/joural/am) ormal Form or Systms with Liar Part () Grac Gachigua * David Maloza Johaa Sigy Dpartmt o Mathmatics Collg
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 informationModule 5: IIR and FIR Filter Design Prof. Eliathamby Ambikairajah Dr. Tharmarajah Thiruvaran School of Electrical Engineering & Telecommunications
Modul 5: IIR ad FIR Filtr Dsig Prof. Eliathamby Ambiairaah Dr. Tharmaraah Thiruvara School of Elctrical Egirig & Tlcommuicatios Th Uivrsity of w South Wals Australia IIR filtrs Evry rcursiv digital filtr
More informationHomotopy 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 informationA NEW CURRENT TRANSFORMER SATURATION DETECTION ALGORITHM
A NEW CURRENT TRANSFORMER SATURATION DETECTION ALGORITHM CHAPTER 5 I uit protctio schms, whr CTs ar diffrtially coctd, th xcitatio charactristics of all CTs should b wll matchd. Th primary currt flow o
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 informationA Note on Quantile Coupling Inequalities and Their Applications
A Not o Quatil Couplig Iqualitis ad Thir Applicatios Harriso H. Zhou Dpartmt of Statistics, Yal Uivrsity, Nw Hav, CT 06520, USA. E-mail:huibi.zhou@yal.du Ju 2, 2006 Abstract A rlatioship btw th larg dviatio
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 informationA Strain-based Non-linear Elastic Model for Geomaterials
A Strai-basd No-liar Elastic Modl for Gomatrials ANDREW HEATH Dpartmt of Architctur ad Civil Egirig Uivrsity of Bath Bath, BA2 7AY UNITED KINGDOM A.Hath@bath.ac.uk http://www.bath.ac.uk/ac Abstract: -
More informationRestricted Factorial And A Remark On The Reduced Residue Classes
Applid Mathmatics E-Nots, 162016, 244-250 c ISSN 1607-2510 Availabl fr at mirror sits of http://www.math.thu.du.tw/ am/ Rstrictd Factorial Ad A Rmark O Th Rducd Rsidu Classs Mhdi Hassai Rcivd 26 March
More informationNumerical Simulation for the 2-D Heat Equation with Derivative Boundary Conditions
IOSR Joural of Applid Chmisr IOSR-JAC -ISSN: 78-576.Volum 9 Issu 8 Vr. I Aug. 6 PP 4-8 www.iosrjourals.org Numrical Simulaio for h - Ha Equaio wih rivaiv Boudar Codiios Ima. I. Gorial parm of Mahmaics
More informationIterative Methods of Order Four for Solving Nonlinear Equations
Itrativ Mods of Ordr Four for Solvig Noliar Equatios V.B. Kumar,Vatti, Shouri Domii ad Mouia,V Dpartmt of Egirig Mamatis, Formr Studt of Chmial Egirig Adhra Uivrsity Collg of Egirig A, Adhra Uivrsity Visakhapatam
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 information10. Joint Moments and Joint Characteristic Functions
0 Joit Momts ad Joit Charactristic Fctios Followig sctio 6 i this sctio w shall itrodc varios paramtrs to compactly rprst th iformatio cotaid i th joit pdf of two rvs Giv two rvs ad ad a fctio g x y dfi
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 informationClass #24 Monday, April 16, φ φ φ
lass #4 Moday, April 6, 08 haptr 3: Partial Diffrtial Equatios (PDE s First of all, this sctio is vry, vry difficult. But it s also supr cool. PDE s thr is mor tha o idpdt variabl. Exampl: φ φ φ φ = 0
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 informationHigher 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 informationAn Efficient Classification System for Medical Diagnosis using SVM
A Efficit Classificatio Systm for Mical Diaosis usig SVM G. Ravi Kumar 1, Dr. G.A Ramachadra 2 ad K.Nagamai 3 1. Rsarch Scholar, Dpartmt of Computr Scic & Tchology, Sri Krishadvaraya Uivrsity, Aapur-515
More informationCalculus & analytic geometry
Calculus & aalytic gomtry B Sc MATHEMATICS Admissio owards IV SEMESTER CORE COURSE UNIVERSITY OF CALICUT SCHOOL OF DISTANCE EDUCATION CALICUT UNIVERSITYPO, MALAPPURAM, KERALA, INDIA 67 65 5 School of Distac
More informationFusion of Retrieval Models at CLEF 2008 Ad-Hoc Persian Track
Fusio of Rtrival Modls at CLEF 008 Ad-Hoc Prsia rack Zahra Aghazad*, Nazai Dhghai* Lili Farzivash* Razih Rahimi* Abolfazl AlAhmad* Hadi Amiri Farhad Oroumchia** * Dpartmt of ECE, Uivrsity of hra {z.aghazadh,.dhghay,
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 informationFirst derivative analysis
Robrto s Nots on Dirntial Calculus Chaptr 8: Graphical analysis Sction First drivativ analysis What you nd to know alrady: How to us drivativs to idntiy th critical valus o a unction and its trm points
More informationEC1305 SIGNALS & SYSTEMS
EC35 SIGNALS & SYSTES DEPT/ YEAR/ SE: IT/ III/ V PREPARED BY: s. S. TENOZI/ Lcturr/ECE SYLLABUS UNIT I CLASSIFICATION OF SIGNALS AND SYSTES Cotiuous Tim Sigals (CT Sigals Discrt Tim Sigals (DT Sigals Stp
More informationTwo 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 informationDiscrete Fourier Transform. Discrete Fourier Transform. Discrete Fourier Transform. Discrete Fourier Transform. Discrete Fourier Transform
Discrt Fourir Trasform Dfiitio - T simplst rlatio btw a lt- squc x dfid for ω ad its DTFT X ( ) is ω obtaid by uiformly sampli X ( ) o t ω-axis btw ω < at ω From t dfiitio of t DTFT w tus av X X( ω ) ω
More informationBlackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted?
All bodis at a tmpratur T mit ad absorb thrmal lctromagtic radiatio Blackbody radiatio I thrmal quilibrium, th powr mittd quals th powr absorbd How is blackbody radiatio absorbd ad mittd? 1 2 A blackbody
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 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 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 informationImage Filtering: Noise Removal, Sharpening, Deblurring. Yao Wang Polytechnic University, Brooklyn, NY11201
Imag Filtring: Nois Rmoval, Sharpning, Dblurring Yao Wang Polytchnic Univrsity, Brooklyn, NY http://wb.poly.du/~yao Outlin Nois rmoval by avraging iltr Nois rmoval by mdian iltr Sharpning Edg nhancmnt
More informationNumerov-Cooley Method : 1-D Schr. Eq. Last time: Rydberg, Klein, Rees Method and Long-Range Model G(v), B(v) rotation-vibration constants.
Numrov-Cooly Mthod : 1-D Schr. Eq. Last tim: Rydbrg, Kli, Rs Mthod ad Log-Rag Modl G(v), B(v) rotatio-vibratio costats 9-1 V J (x) pottial rgy curv x = R R Ev,J, v,j, all cocivabl xprimts wp( x, t) = ai
More information4037 ADDITIONAL MATHEMATICS
CAMBRIDGE INTERNATIONAL EXAMINATIONS GCE Ordinary Lvl MARK SCHEME for th Octobr/Novmbr 0 sris 40 ADDITIONAL MATHEMATICS 40/ Papr, maimum raw mark 80 This mark schm is publishd as an aid to tachrs and candidats,
More informationECE 599/692 Deep Learning
ECE 599/69 Dp Lari Lctur Autocors Hairo Qi Goal Family Profssor Elctrical Eiri a Computr Scic Uivrsity of ss Kovill http://www.cs.ut.u/faculty/qi Email: hqi@ut.u A loo ac i tim INPU 33 C: fatur maps 6@88
More informationHadamard Exponential Hankel Matrix, Its Eigenvalues and Some Norms
Math Sci Ltt Vol No 8-87 (0) adamard Exotial al Matrix, Its Eigvalus ad Som Norms İ ad M bula Mathmatical Scics Lttrs Itratioal Joural @ 0 NSP Natural Scics Publishig Cor Dartmt of Mathmatics, aculty of
More information