COMPLEMENTARY IIR FILTER PAIRS WITH AN ADJUSTABLE CROSSOVER FREQUENCY
|
|
- Janis Morgan
- 5 years ago
- Views:
Transcription
1 COPLEENTARY IIR ILTER PAIRS WITH AN ADJUSTABLE CROSSOVER REQUENCY Ljljana lć Tao Saramäk Tamere Internatonal Center for Sgnal Proceng (TICSP) Inttute of Sgnal Proceng, Tamere Unverty of Technology P. O. Box 553, IN-33 Tamere, nl, E-mal: Author ermanent afflaton Unverty of Belgrade, hajlo Pun Inttute, P.O. Box 5, Belgrade, Yugolava, Emal: ABSTRACT Th aer ntroduce three clae of comlementary recurve low-a/hgh-a flter ar wth an adjutable croover frequency n uch a way that the tob attenuaton of both flter reman the ame. or each cla, the flter ar contructed ung two alla ub-flter a buldng block. Baed on the roerte elltc mnmal Q-factor tranfer functon, mle exreon are derved for evaluatng the coeffcent n all-a ecton n order to acheve the dered croover frequency. The degn rocedure are develoed for yntheng comlementary flter ar mlemented a a arallel connecton of two all-a ub-flter for two clae of flter ar contructed a taed cacaded nterconnecton of two dentcal all-a ubflter. The drect arallel connecton ha both the ower-comlementary all-a comlementary roerty. The frt (econd) cla of flter contructed ung everal dentcal coe of the two all-a flter oee the ower-comlementary roerty (both the magntude-comlementary all-a comlementary roerte).. INTRODUCTION Comlementary nfnte-mule reone (IIR) flter ar can be yntheed to generate ower-comlementary, all-a comlementary, or magntudecomlementary flter ar (ee, e.g., [). A very attractve alternatve to generate a ower-comlementary lowa/hgh-a IIR flter ar to ue lattce wave dgtal (LWD) flter (arallel connecton of two all-a flter) [ [4. Uually, the nterecton for a lowa/hgh-a flter ar occur n the mddle of the bae-b, that, the croover frequency located exactly at /4 n term of the normaled frequency. If the tob attenuaton of both flter the ame, then the low-a hgh-a flter are both half-b IIR flter (ee, e.g., [4, [5). Th aer ntroduce a technque to change, by mean of mle formulae, the locaton of the croover frequency of the half-b flter ar to an arbtrary locaton whle tll retanng the attenuaton roerte of the ntal half-b flter. or th uroe, elltc mnmal Q-factor (EQ) tranfer functon ntroduced n [6 [8 rovde drectly the dered oluton. Th due to the fact they are ecal low-a tranfer functon that can be regarded a tranfer functon beng obtanable from half-b IIR flter ung the well known low-a to low-a tranformaton. The attractve roerty of the EQ flter that the actual ynthe can be erformed ung mle equaton, thereby enablng one to develo very mle exlct formulae for generatng a flter ar wth the gven croover frequency. In addton to the drect arallel connecton of two all-a flter, two tructure contructed a taed cacaded nterconnecton of two dentcal all-a flter are condered baed on the ue of the ynthe cheme decrbed n [9 [. The frt (econd) tructure allow one to generate ower-comlementary (magntudecomlementary) flter ar wth an adjutable croover frequency. Comared to the drect mlementaton, the advantage of the frt tructure that electve flter ar can be contructed wth the ad of very low-order all-a flter at the exene of ung addtonal coeffcent for nterconnectng everal dentcal coe of the two all-a ecton. The econd tructure allow one to generate by ung very low-order all-a ecton magntude-comlementary flter ar wth an adjutable croover frequency.. USE O EQ ILTERS OR GENERATING POWER-COPLEENTARY ILTER PAIRS WITH AN ADJUSTABLE CROSSOVER REQUENCY Th ecton how how the roerte of EQ flter [6 [8 can be exloted n a very traghtforward manner for generatng ower-comlementary IIR flter ar wth an adjutable croover frequency uch that the tob attenuaton reman the ame. Due to the fact that EQ flter comre a half-b flter a a ecal cae, we tart wth a half-b flter ar to generate
2 comlementary flter ar whoe croover frequency can be arbtrarly choen. A G.. Proerte of EQ flter for Generatng Power-Comlementary lter Par Comlementary IIR flter ar contructed a a arallel connecton of two all-a ub flter hown n gure. or half-b IIR flter, the comlementary flter ar gven by (ee, e.g., [4, [5 ) G = A ± A ( N ) = 3,5, , ( N ) + = =,4,... + < +. ± () Here, N, the flter order, retrcted to be odd T G ( ) = G G a vector denotng the low-a (wth the lu gn) hgh-a (wth the mnu gn) half-b flter tranfer functon G () G (). The uercrt ued to emhae that the flter under conderaton are halfb flter. One of ole of the above tranfer functon located at the orgn the remanng ole are comlex-conjugate ar beng located on the magnary ax at = jr l for l =,, L, ( N ) /, gvng = ( r ). In Eq. (), the notaton < + ndcate how the ole are hared between the two all-a ecton. Th flter ar when generated by mean of an oddorder elltc flter charactered by the followng attractve roerte. rt, the um of the quaredmagntude reone of the two flter dentcally equal to unty. Hence, the flter ar ha the owercomlementary roerty. Second, the 3-dB croover frequency (the frequency where the quared-magntude reone of both G () G () acheve the value of /) located at f = / 4 n term of the normaled frequency. Thrd, the ab tob edge, denoted by f f n term of the normaled frequency, atfy = / f, that, the dtance of f the edge from the center of the baeb are the ame. ourth, the attenuaton of the low-a hgh-a half-b flter the ame. Snce the um of the tranfer functon G ) () A ( G, the reultng flter ar alo an all-a comlementary flter ar, thereby called a a double comlementary flter ar [. The low-a/hgh-a EQ flter ar generated accordng to the half-b flter ar, a gven by Eq (), a follow: l A G gure. Double-comlementary IIR flter ar contructed a a arallel connecton of two all-a flter. G = [ A ± A = ( N ) + α( + ) + ± =,4,... + α( + ) + ( N ) α + + α( + ) + + α + α + + = 3,5,... ( ) T, < +. where G( ) = G G agan a vector denotng the reultng low-a hgh-a flter tranfer functon G () G () that can be mlemented a hown n gure. The mle formulae for convertng the ure delay the econd-order all-a ecton n Eq. () to the frt-order the econd-order ecton n Eq. () wll be gven later on n th ecton. It hould be onted out that when ung LWD flter for the mlementaton, the adator coeffcent γ = α for the frt-order all-a ecton. or the econd-order all-a ecton, the correondng adator coeffcent are gven by γ = γ = α (ee, e.g., [4). There ext the followng three very attractve roerte of EQ flter guaranteeng that for the reultng EQ flter ar, a hown by Eq (), the croover frequency can be changed whle keeng the attenuaton of the low-a hgh-a flter the ame a for the tart-u half-b flter ar. urthermore, the double comlementary roerty reerved. rt, thee flter are generated ung half-b IIR flter a tart-u oluton [6 [8. Second, ntead of drectly alyng the well known low-a to low-a tranformaton or low-a to hgh-a tranformaton, the flter wth the gven a-b to-b edge are generated ung mle formulae. Thrd, f a low-a or a hgha flter generated frt, then t guaranteed that the flter n the reultng low-a/hgh-a flter ar have exactly the ame attenuaton n the to-b regon. Th due to the fact the tart-u flter an IIR halfb-flter... Degn Procedure () Baed on the roerte of EQ flter, a owercomlementary flter ar wth the gven odd order N, 3- db croover frequency, mnmum to-b A n decbel can be carred out n the fol- attenuaton lowng te: f
3 ) Synthee a ower-comlementary half-b IIR flter ar, a gven by Eq. (), uch that the mnmum attenuaton for both the low-a hgh-a flter tranfer functon G () G () exactly A. Let the correondng normaled cutoff frequence be f f = / f. ) Determne the o-called electvty factor ξ = ( πf ) tan( πf ) tan. 3) Synthee the dered ower-comlementary IIR flter ar, a gven by Eq. (), by determnng t arameter accordng to the formulae gven n Table. Table : Parameter for a ower-comlementary flter ar wth the gven cutoff frequency rt-order Secton Secondorder Secton tan α = + tan α = + f ( πf ) ( πf ) ( tan( πf )) ( tan( πf )) =.3. Proerte of the Reultng lter Par + α α + The above rocedure reult n the owercomlementary flter ar wth the followng roerte: ) The croover frequency beng related to the common contant α n Eq. () or n Table a follow: ( α ) π f co = (3) located exactly at the gven frequency ont. ) The normaled cutoff frequence are gven by f f ( = tan tan( πf ) ξ ) (4a) π ( ξ tan( πf ). = tan ) (4b) π 3) The mnmum to-b attenuaton for both G () on the nterval [ f, G () on the nterval, f exactly. 4) The arameter α the common contant for all the econd-order all-a ecton n Eq. ()..3. Numercal Examle Conder ower-comlementary flter ar of order N = 7 havng A = 6 db. The order of the all-a ecton are thu 4 3. gure (a) how a famly of the reultng low-a flter that are derved from the halfb flter (thck lne). or each new flter only 5 contant value have to be comuted ung the exreon of Table. gure (b) how the reone of the overall bank for ome value of the croover frequency. A Attenuaton Attenuaton Normaled frequency (a) Normaled frequency (b) gure. amly of eventh-order ower-comlementary flter ar for A = 6 db. (a) Low-a flter. (b) Overall flter ar. 3. GENERATING POWER-COPLEENTARY IIR ILTER PAIRS USING A TAPPED CASCADED INTERCONNECTION O TWO IDENTICAL ALL-PASS ILTERS Th ecton how how the ynthe technque decrbed n [9, [ can be ued for generatng owercomlementary IIR flter ar wth an adjutable croover frequency. In th cae, the overall tructure generated a a taed cacaded nterconnecton of two dentcal all-a flter agan the roerte of EQ flter are exloted. 3. Prooed lter Par Effcent Imlementaton In th cae, the low-a hgh-a tranfer functon are gven by H m m = a[ m [ A [ A (5a)
4 H m m m = ( ) a[ m [ A [ A, (5b) where an odd nteger A () A () are the alla flter n Eq. () or (), that, G = [ A + A a low-a flter of an odd order N. The above ower-comlementary flter ar can be mlemented ung the lattce tructure hown n g. 3. The detal on how to convert the a[ m to the k can be found, e.g., n [. 3. Degn Procedure Gven the mnmum tob attenuaton, the frt te n the overall ynthe to fnd the + coeffcent a m the Nth-order low-a half-b flter [ A A ( ) G ( ) = +, a gven by Eq. (), uch that the followng condton are met: Condton : The mnmum attenuaton for both the lowa hgh-a flter tranfer functon H () H () exactly A. Condton : The normaled cutoff frequence are related va f = / f f f maxmed. a[ m A f The dered coeffcent can be found a follow: A ) Determne =. ) Otme the a m to maxme f uch that the amltude reone of wthn the lmt m a[ m = tay n the normaled a-b regon [, f the maxmum amltude value [ f, Note that. n the normaled to-b regon the tranfer functon of a mnmumhae fnte-mule reone (IR) flter. The above rocedure can be accomlhed by lghtly modfyng the degn cheme decrbed n [9. What left to degn the ower-comlementary half-b flter ar, a gven by Eq. (), uch that the above-mentoned two condton are met, then, to tranfer the croover frequency f to the dered frequency accordng to the dcuon of Subecton.. Th can be accomlhed by ung the degn rocedure decrbed n Subecton.. The man dfference that now, due to the ue of everal coe of the two dentcal all-a ecton, the mnmum to-b attenuaton, In th cae, the all-a ecton n g. 3 are A A. A A [ A () k k3 k [ A ( ) k 3 [ A () [ A ( ) H k k H gure 3. Lattce tructure for the rooed owercomlementary flter ar. Attenuaton Attenuaton Normaled frequency (a) Normaled frequency (b) gure 4. A famly of ower-comlementary flter ar contructed ung 5 dentcal coe of econdorder frt-order all-a ecton for A = 6 db. (a) Low-a flter. (b) Overall flter ar. ntead of the orgnal detal): A A 3.3 Numercal Examle, gven a follow (ee [9 for ( ( f = log π )). (6) Conder ower-comlementary flter ar that are contructed ung = 5 dentcal coe of two all-a flter of order, that, N = 3. The dered attenuaton A = 6 db. gure 4(a) llutrate a famly of the reultng low-a flter. The thck lne ued for the ntal half-b flter. or each new flter only 3 contant value have to be comuted. The value of the ad-
5 dtonal ta coeffcent tay unchanged. The requred attenuaton of the arallel connecton of the frt-order econd-order all-a flter only 9.37 db. The reone of the overall bank for ome value of the croover frequency are dected n gure 4(b). 4. GENERATING APLITUDE-COPLE- ENTARY IIR ILTER PAIRS USING A TAPPED CASCADED INTERCONNECTION O TWO IDENTICAL ALL-PASS ILTERS Th ecton how how the ynthe technque decrbed n [9 can be ued for generatng amltudecomlementary IIR flter ar wth an adjutable croover frequency. A n the revou ecton, the overall tructure generated a a taed cacaded nterconnecton of two dentcal all-a flter the roerte of EQ flter are exloted. 4.. Prooed lter Par Effcent Imlementaton [ [ A ( ) [ A ( ) A A A A [ A ( ) a [ a[ a[ a A [ A ( ) H H gure 5. Structure for the rooed magntudecomlementary (all-a comlementary) flter ar. 8 A In th cae, the low-a hgh-a tranfer functon leadng to the effcent mlementaton are gven by Attenuaton 6 4 H H m a[ m [ A [ A = m m b[ m [ A [ A, = m (7a) (7b) Normaled frequency (a) where an nteger that two tme an odd nteger, a [ m = a[ m, b [ m = b[ m, b[ m = a[ m for m =,, L, ( ) /. urthermore, a [ = b[ = a [ m = b[ m = for the remanng odd value of m. An effcent mlementaton for the above magntude-comlementary flter ar hown n g. 5. The um of the above two tranfer functon [ A [ A o that they form alo an all-a comlementary flter ar. 4.. Degn Procedure In th cae, the dered coeffcent a follow: A ) Determne =. a[ m can be found ) Otme the a m to maxme f uch that the ero-hae frequency reone of = a [ m m tay wthn the lmt ( ) n the normaled a-b regon [, f wthn the lmt n the normaled tob regon [ f,. Attenuaton Normaled frequency (b) gure 6. A famly of magntude-comlementary (all-a comlementary) flter ar contructed ung 6 dentcal coe of econd-order frt-order all-a ecton. (a) A =6dB. (b) A =db. ( ) Note that the tranfer functon of a lnear-hae IR half-b flter. The above rocedure can be accomlhed by lghtly modfyng the degn cheme decrbed n [. Otherwe, the overall ynthe the ame a n the revou ecton.
6 4.3. Numercal Examle Conder magntude-comlementary flter ar that are contructed ung = 6 dentcal coe of two all-a flter of order, that, N = 3. gure 6(a) how two bank wth the tob attenuaton of 6 db llutratng the flter charactertc for ome value of the croover frequency. gure 6(b) dect two flter bank for the tob attenuaton of db. The thck lne are ued for the ntal half-b flter. The requred attenuaton for the arallel connecton of the frt-order econd-order all-a flter are only 4.53 db 4.39 db for the flter of gure 6(a) 6(b), reectvely. 5. CONCLUSION Three clae of comlementary IIR low-a/hgh-a flter ar wth an adjutable croover frequency have been ntroduced. or the frt cla, the tart-u comlementary flter are low-a/hgh-a half-b flter ar contructed a arallel connecton of two all-a flter ecton (lattce wave dgtal flter). It ha been hown how thee flter ar can be ealy redegned to have an arbtrary croover frequency n uch a manner that the tob attenuaton for both the low-a hgh-a flter the ame ndeendent of the croover frequency. Th goal ha been acheved by exlotng the attractve roerte of elltc mnmal Q- factor tranfer functon. The ue of the charactertc of thee tranfer functon ha leaded to mle formulae for drectly changng the coeffcent value of the two all-a ecton to acheve the dered croover frequency. Th allow one to mlement rogrammable comlementary flter bank wth an adjutable croover frequency n a very mle traghtforward manner. The flter ar belongng to the frt cla both ower comlementary all-a comlementary. The comlementary flter ar belongng to the remanng two clae have been contructed a taed cacaded nterconnecton of two dentcal all-a ubflter. The man beneft of thee flter ar le n the fact that the all-a ub-flter are of very low order, thereby makng the adjutment of the croover frequency gnfcantly eaer. The rce to be ad for th fact that there a need for addtonal contant coeffcent for nterconnectng the all-a ub-flter. lter ar belongng to the econd (thrd) cla are ower comlementary (both magntude comlementary alla comlementary). ACKNOWLEDGEENTS Th work wa uorted by the academy of nl, roject No (nnh Centre of Excellence Program ( 5). Author greatly arecate the nrng dcuon wth Prof. arkku Renfor, Tamere Unverty of Technology. REERENCES [ S. K. tra, Dgtal Sgnal Proceng: A Comuter- Baed Aroach. cgraw-hll,. [ R. Nouta, The Jaumann tructure n wave-dgtal flter, Int. J. Crcut Theory Alcat., vol., , June 974. [3 A. ettwe H. Levn A. Sedlmeyer, Wave dgtal lattce flter, Int. J. Crcut Theory Alcat., vol.,. 3, June 974. [4 L. Ga, Exlct formula for lattce wave dgtal flter, IEEE Tran. Crcut Syt., vol. CAS-3,. 3, Jan [5. Renfor T. Saramäk, Recurve Nth-b dgtal flter Part I: Degn roerte, Part II: Degn of multtage decmator nterolator," IEEE Tran. Crcut Syt., vol. CAS-34,. 4 5, Jan [6. D. Lutovac, D. V. Tošć, B. L. Evan, lter Degn for Sgnal Proceng Ung ATLAB athematca. Uerde Rver, New Jerey: Prentce Hall,. [7. D. Lutovac Lj. D. lć, "Degn of comutatonally effcent elltc IIR flter wth a reduced number of hft--add oeraton n multler," IEEE Tran. Sgnal Proceng, vol. 45, no.,. 4 43, Oct.997. [8 Lj. D. lć. D. Lutovac, "Degn of multlerle elltc IIR flter wth a mall quantaton error," IEEE Tran. Sgnal Proceng, Vol.47, No., , eb [9 T. Saramäk. Renfor, A novel aroach for the degn IIR flter a a taed cacaded nterconnecton of dentcal alla ubflter, n Proc. 987 IEEE Int. Sym. Crcut Syt. (Phladelha, Pennylvana), ay 987, vol., [ H. Johanon T. Saramäk, A cla of comlementary IIR flter, n Proc. 999 IEEE Int. Sym. Crcut Syt. (Orlo, lorda), July 999, vol. 3, [ H. Johanon L. Wanhammar, Hgh-eed recurve flter tructure comoed of dentcal all-a ubflter for nterolaton, decmaton, Q bank wth erfect magntude recontructon, IEEE Tran. Crcut Sytem-II: Analog Dgtal Sgnal Proceng, vol. 46, no.,. 6 8, January 999.
Design of Recursive Digital Filters IIR
Degn of Recurve Dgtal Flter IIR The outut from a recurve dgtal flter deend on one or more revou outut value, a well a on nut t nvolve feedbac. A recurve flter ha an nfnte mule reone (IIR). The mulve reone
More informationImprovements on Waring s Problem
Imrovement on Warng Problem L An-Png Bejng 85, PR Chna al@nacom Abtract By a new recurve algorthm for the auxlary equaton, n th aer, we wll gve ome mrovement for Warng roblem Keyword: Warng Problem, Hardy-Lttlewood
More informationAdditional File 1 - Detailed explanation of the expression level CPD
Addtonal Fle - Detaled explanaton of the expreon level CPD A mentoned n the man text, the man CPD for the uterng model cont of two ndvdual factor: P( level gen P( level gen P ( level gen 2 (.).. CPD factor
More informationSmall signal analysis
Small gnal analy. ntroducton Let u conder the crcut hown n Fg., where the nonlnear retor decrbed by the equaton g v havng graphcal repreentaton hown n Fg.. ( G (t G v(t v Fg. Fg. a D current ource wherea
More informationA Novel Approach for Testing Stability of 1-D Recursive Digital Filters Based on Lagrange Multipliers
Amercan Journal of Appled Scence 5 (5: 49-495, 8 ISSN 546-939 8 Scence Publcaton A Novel Approach for Tetng Stablty of -D Recurve Dgtal Flter Baed on Lagrange ultpler KRSanth, NGangatharan and Ponnavakko
More informationChapter 11. Supplemental Text Material. The method of steepest ascent can be derived as follows. Suppose that we have fit a firstorder
S-. The Method of Steepet cent Chapter. Supplemental Text Materal The method of teepet acent can be derved a follow. Suppoe that we have ft a frtorder model y = β + β x and we wh to ue th model to determne
More informationRoot Locus Techniques
Root Locu Technque ELEC 32 Cloed-Loop Control The control nput u t ynthezed baed on the a pror knowledge of the ytem plant, the reference nput r t, and the error gnal, e t The control ytem meaure the output,
More informationHarmonic oscillator approximation
armonc ocllator approxmaton armonc ocllator approxmaton Euaton to be olved We are fndng a mnmum of the functon under the retrcton where W P, P,..., P, Q, Q,..., Q P, P,..., P, Q, Q,..., Q lnwgner functon
More informationPythagorean triples. Leen Noordzij.
Pythagorean trple. Leen Noordz Dr.l.noordz@leennoordz.nl www.leennoordz.me Content A Roadmap for generatng Pythagorean Trple.... Pythagorean Trple.... 3 Dcuon Concluon.... 5 A Roadmap for generatng Pythagorean
More informationImprovements on Waring s Problem
Improvement on Warng Problem L An-Png Bejng, PR Chna apl@nacom Abtract By a new recurve algorthm for the auxlary equaton, n th paper, we wll gve ome mprovement for Warng problem Keyword: Warng Problem,
More informationScattering of two identical particles in the center-of. of-mass frame. (b)
Lecture # November 5 Scatterng of two dentcal partcle Relatvtc Quantum Mechanc: The Klen-Gordon equaton Interpretaton of the Klen-Gordon equaton The Drac equaton Drac repreentaton for the matrce α and
More informationDesign of Two-Channel Low-Delay FIR Filter Banks Using Constrained Optimization
contrained otimization, CIT Journal of Comuting and Information Technology, vol. 8, no 4,. 34 348, 2. Deign of Two-Channel Low-Delay FIR Filter Bank Uing Contrained Otimization Abtract Robert Bregović
More informationChapter 5: Root Locus
Chater 5: Root Locu ey condton for Plottng Root Locu g n G Gven oen-loo tranfer functon G Charactertc equaton n g,,.., n Magntude Condton and Arguent Condton 5-3 Rule for Plottng Root Locu 5.3. Rule Rule
More informationVariable Structure Control ~ Basics
Varable Structure Control ~ Bac Harry G. Kwatny Department of Mechancal Engneerng & Mechanc Drexel Unverty Outlne A prelmnary example VS ytem, ldng mode, reachng Bac of dcontnuou ytem Example: underea
More informationa new crytoytem baed on the dea of Shmuley and roved t rovably ecure baed on ntractablty of factorng [Mc88] After that n 999 El Bham, Dan Boneh and Om
Weak Comote Dffe-Hellman not Weaker than Factorng Koohar Azman, azman@ceharfedu Javad Mohajer mohajer@harfedu Mahmoud Salmazadeh alma@harfedu Electronc Reearch Centre, Sharf Unverty of Technology Deartment
More informationComputer Control Systems
Computer Control ytem In th chapter we preent the element and the bac concept of computercontrolled ytem. The dcretaton and choce of amplng frequency wll be frt examned, followed by a tudy of dcrete-tme
More informationDigital PI Controller Equations
Ver. 4, 9 th March 7 Dgtal PI Controller Equatons Probably the most common tye of controller n ndustral ower electroncs s the PI (Proortonal - Integral) controller. In feld orented motor control, PI controllers
More informationCircuit Theorems. Introduction
//5 Crcut eorem ntroducton nearty Property uperpoton ource Tranformaton eenn eorem orton eorem Maxmum Power Tranfer ummary ntroducton To deelop analy technque applcable to lnear crcut. To mplfy crcut analy
More informationThe Decibel and its Usage
The Decbel and ts Usage Consder a two-stage amlfer system, as shown n Fg.. Each amlfer rodes an ncrease of the sgnal ower. Ths effect s referred to as the ower gan,, of the amlfer. Ths means that the sgnal
More informationChapter 6 The Effect of the GPS Systematic Errors on Deformation Parameters
Chapter 6 The Effect of the GPS Sytematc Error on Deformaton Parameter 6.. General Beutler et al., (988) dd the frt comprehenve tudy on the GPS ytematc error. Baed on a geometrc approach and aumng a unform
More informationDigital Signal Processing
Dgtal Sgnal Processng Dscrete-tme System Analyss Manar Mohasen Offce: F8 Emal: manar.subh@ut.ac.r School of IT Engneerng Revew of Precedent Class Contnuous Sgnal The value of the sgnal s avalable over
More informationLesson 16: Basic Control Modes
0/8/05 Lesson 6: Basc Control Modes ET 438a Automatc Control Systems Technology lesson6et438a.tx Learnng Objectves Ater ths resentaton you wll be able to: Descrbe the common control modes used n analog
More informationElectrical Circuits II (ECE233b)
Electrcal Crcut II (ECE33b) Applcaton of Laplace Tranform to Crcut Analy Anet Dounav The Unverty of Wetern Ontaro Faculty of Engneerng Scence Crcut Element Retance Tme Doman (t) v(t) R v(t) = R(t) Frequency
More informationSpecification -- Assumptions of the Simple Classical Linear Regression Model (CLRM) 1. Introduction
ECONOMICS 35* -- NOTE ECON 35* -- NOTE Specfcaton -- Aumpton of the Smple Clacal Lnear Regreon Model (CLRM). Introducton CLRM tand for the Clacal Lnear Regreon Model. The CLRM alo known a the tandard lnear
More informationTranslational Equations of Motion for A Body Translational equations of motion (centroidal) for a body are m r = f.
Lesson 12: Equatons o Moton Newton s Laws Frst Law: A artcle remans at rest or contnues to move n a straght lne wth constant seed there s no orce actng on t Second Law: The acceleraton o a artcle s roortonal
More informationProperty-based Integration for Sustainable Development
Proerty-baed Integraton for Sutanable Develoment V. Kazantz, D. Harell, F. Gabrel, Qn X., and M.M. El-Halwag * Deartment of Chemcal Engneerng Texa A&M Unverty, College Staton, TX 77843-3122, USA Abtract
More informationModule 5. Cables and Arches. Version 2 CE IIT, Kharagpur
odule 5 Cable and Arche Veron CE IIT, Kharagpur Leon 33 Two-nged Arch Veron CE IIT, Kharagpur Intructonal Objectve: After readng th chapter the tudent wll be able to 1. Compute horzontal reacton n two-hnged
More informationIterative Methods for Searching Optimal Classifier Combination Function
htt://www.cub.buffalo.edu Iteratve Method for Searchng Otmal Clafer Combnaton Functon Sergey Tulyakov Chaohong Wu Venu Govndaraju Unverty at Buffalo Identfcaton ytem: Alce Bob htt://www.cub.buffalo.edu
More informationCHAPTER 9 LINEAR MOMENTUM, IMPULSE AND COLLISIONS
CHAPTER 9 LINEAR MOMENTUM, IMPULSE AND COLLISIONS 103 Phy 1 9.1 Lnear Momentum The prncple o energy conervaton can be ued to olve problem that are harder to olve jut ung Newton law. It ued to decrbe moton
More informationEECE 301 Signals & Systems Prof. Mark Fowler
-T Sytem: Ung Bode Plot EEE 30 Sgnal & Sytem Pro. Mark Fowler Note Set #37 /3 Bode Plot Idea an Help Vualze What rcut Do Lowpa Flter Break Pont = / H ( ) j /3 Hghpa Flter c = / L Bandpa Flter n nn ( a)
More informationChapter 8: Fast Convolution. Keshab K. Parhi
Cater 8: Fat Convoluton Keab K. Par Cater 8 Fat Convoluton Introducton Cook-Too Algort and Modfed Cook-Too Algort Wnograd Algort and Modfed Wnograd Algort Iterated Convoluton Cyclc Convoluton Degn of Fat
More informationand decompose in cycles of length two
Permutaton of Proceedng of the Natona Conference On Undergraduate Reearch (NCUR) 006 Domncan Unverty of Caforna San Rafae, Caforna Apr - 4, 007 that are gven by bnoma and decompoe n cyce of ength two Yeena
More informationChapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems
Numercal Analyss by Dr. Anta Pal Assstant Professor Department of Mathematcs Natonal Insttute of Technology Durgapur Durgapur-713209 emal: anta.bue@gmal.com 1 . Chapter 5 Soluton of System of Lnear Equatons
More informationLet s start from a first-order low pass filter we already discussed.
EEE0 Netrk Analy II Dr. harle Km Nte09: Actve Flter ---Part. gher-order Actve Flter The rt-rder lter d nt harply dvde the pa band and the tp band. One apprach t btan a harper trantn beteen the pa band
More informationMethod Of Fundamental Solutions For Modeling Electromagnetic Wave Scattering Problems
Internatonal Workhop on MehFree Method 003 1 Method Of Fundamental Soluton For Modelng lectromagnetc Wave Scatterng Problem Der-Lang Young (1) and Jhh-We Ruan (1) Abtract: In th paper we attempt to contruct
More informationA total variation approach
Denosng n dgtal radograhy: A total varaton aroach I. Froso M. Lucchese. A. Borghese htt://as-lab.ds.unm.t / 46 I. Froso, M. Lucchese,. A. Borghese Images are corruted by nose ) When measurement of some
More informationModel Reference Adaptive Control for Perforated Mill. Xiu-Chun Zhao, Guo-Kai Xu, TaoZhang and Ping-Shu Ge
nd Internatonal Conference on Electronc & Mechancal Engneerng and Inforaton Technology (EMEIT-) Model Reference Adatve Control for Perforated Mll Xu-Chun Zhao, Guo-Ka Xu, TaoZhang and Png-Shu Ge Deartent
More informationThe optimal delay of the second test is therefore approximately 210 hours earlier than =2.
THE IEC 61508 FORMULAS 223 The optmal delay of the second test s therefore approxmately 210 hours earler than =2. 8.4 The IEC 61508 Formulas IEC 61508-6 provdes approxmaton formulas for the PF for smple
More informationIntroduction to Interfacial Segregation. Xiaozhe Zhang 10/02/2015
Introducton to Interfacal Segregaton Xaozhe Zhang 10/02/2015 Interfacal egregaton Segregaton n materal refer to the enrchment of a materal conttuent at a free urface or an nternal nterface of a materal.
More informationTwo Approaches to Proving. Goldbach s Conjecture
Two Approache to Provng Goldbach Conecture By Bernard Farley Adved By Charle Parry May 3 rd 5 A Bref Introducton to Goldbach Conecture In 74 Goldbach made h mot famou contrbuton n mathematc wth the conecture
More informationFingerprint Verification Using Genetic Algorithms
Fngerrnt Verfcaton Ung Genetc Algorthm Xuejun Tan and Br Bhanu Center for Reearch n Intellgent Sytem, Unverty of Calforna, Rverde, CA 92521 {xtan, bhanu}@cr.ucr.edu Abtract Fngerrnt matchng tll a challengng
More informationEE 508 Lecture 7. Degrees of Freedom The Approximation Problem
EE 508 Lecture 7 Degrees of Freedom The Approxmaton Problem vew from Last Tme Desgn Strategy Theorem: A crcut wth transfer functon T(s) can be obtaned from a crcut wth normalzed transfer functon T n (s
More informationNECESSARY AND SUFFICIENT CONDITIONS FOR ALMOST REGULARITY OF UNIFORM BIRKHOFF INTERPOLATION SCHEMES. by Nicolae Crainic
NECESSARY AND SUFFICIENT CONDITIONS FOR ALMOST REGULARITY OF UNIFORM BIRKHOFF INTERPOLATION SCHEMES by Ncolae Cranc Abstract: In ths artcle usng a combnaton of the necessary and suffcent condtons for the
More informationAn Upper Bound on SINR Threshold for Call Admission Control in Multiple-Class CDMA Systems with Imperfect Power-Control
An Upper Bound on SINR Threshold for Call Admsson Control n Multple-Class CDMA Systems wth Imperfect ower-control Mahmoud El-Sayes MacDonald, Dettwler and Assocates td. (MDA) Toronto, Canada melsayes@hotmal.com
More informationPhysics 111. CQ1: springs. con t. Aristocrat at a fixed angle. Wednesday, 8-9 pm in NSC 118/119 Sunday, 6:30-8 pm in CCLIR 468.
c Announcement day, ober 8, 004 Ch 8: Ch 10: Work done by orce at an angle Power Rotatonal Knematc angular dplacement angular velocty angular acceleraton Wedneday, 8-9 pm n NSC 118/119 Sunday, 6:30-8 pm
More informationNon-Ideality Through Fugacity and Activity
Non-Idealty Through Fugacty and Actvty S. Patel Deartment of Chemstry and Bochemstry, Unversty of Delaware, Newark, Delaware 19716, USA Corresondng author. E-mal: saatel@udel.edu 1 I. FUGACITY In ths dscusson,
More informationDepartment of Electrical & Electronic Engineeing Imperial College London. E4.20 Digital IC Design. Median Filter Project Specification
Desgn Project Specfcaton Medan Flter Department of Electrcal & Electronc Engneeng Imperal College London E4.20 Dgtal IC Desgn Medan Flter Project Specfcaton A medan flter s used to remove nose from a sampled
More informationProblem #1. Known: All required parameters. Schematic: Find: Depth of freezing as function of time. Strategy:
BEE 3500 013 Prelm Soluton Problem #1 Known: All requred parameter. Schematc: Fnd: Depth of freezng a functon of tme. Strategy: In thee mplfed analy for freezng tme, a wa done n cla for a lab geometry,
More informationChapter 6. Operational Amplifier. inputs can be defined as the average of the sum of the two signals.
6 Operatonal mpler Chapter 6 Operatonal mpler CC Symbol: nput nput Output EE () Non-nvertng termnal, () nvertng termnal nput mpedance : Few mega (ery hgh), Output mpedance : Less than (ery low) Derental
More informationAlgorithms for factoring
CSA E0 235: Crytograhy Arl 9,2015 Instructor: Arta Patra Algorthms for factorng Submtted by: Jay Oza, Nranjan Sngh Introducton Factorsaton of large ntegers has been a wdely studed toc manly because of
More informationOne-sided finite-difference approximations suitable for use with Richardson extrapolation
Journal of Computatonal Physcs 219 (2006) 13 20 Short note One-sded fnte-dfference approxmatons sutable for use wth Rchardson extrapolaton Kumar Rahul, S.N. Bhattacharyya * Department of Mechancal Engneerng,
More information728. Mechanical and electrical elements in reduction of vibrations
78. Mechancal and electrcal element n reducton of vbraton Katarzyna BIAŁAS The Slean Unverty of Technology, Faculty of Mechancal Engneerng Inttute of Engneerng Procee Automaton and Integrated Manufacturng
More informationAP Statistics Ch 3 Examining Relationships
Introducton To tud relatonhp between varable, we mut meaure the varable on the ame group of ndvdual. If we thnk a varable ma eplan or even caue change n another varable, then the eplanator varable and
More informationELG3336: Op Amp-based Active Filters
ELG6: Op Amp-baed Actve Flter Advantage: educed ze and weght, and thereore paratc. Increaed relablty and mproved perormance. Smpler degn than or pave lter and can realze a wder range o uncton a well a
More informationANSWERS. Problem 1. and the moment generating function (mgf) by. defined for any real t. Use this to show that E( U) var( U)
Econ 413 Exam 13 H ANSWERS Settet er nndelt 9 deloppgaver, A,B,C, som alle anbefales å telle lkt for å gøre det ltt lettere å stå. Svar er gtt . Unfortunately, there s a prntng error n the hnt of
More informationSUBTRACTION METHOD FOR REMOVING POWERLINE INTERFERENCE
SUBTRACTION METHOD OR REMOVING POWERLINE INTERERENCE ROM ECG IN CASE O REQUENCY DEVIATION Georgy Slavtchev Mhov, Ratcho Marnov Ivanov, Chavdar Lev Levkov aculty of Electronc Engneerng and Technologe (ETT),
More informationImproved Adaptive Time Delay Estimation Algorithm Based on Fourth-order Cumulants
Available online www.jocr.com Journal of hemical and Pharmaceutical Reearch, 016, 8(5):889-894 Reearch Article ISSN : 0975-784 ODEN(USA) : JPR5 Imroved Adative Time Delay Etimation Algorithm Baed on Fourth-order
More information% & 5.3 PRACTICAL APPLICATIONS. Given system, (49) , determine the Boolean Function, , in such a way that we always have expression: " Y1 = Y2
5.3 PRACTICAL APPLICATIONS st EXAMPLE: Gven system, (49) & K K Y XvX 3 ( 2 & X ), determne the Boolean Functon, Y2 X2 & X 3 v X " X3 (X2,X)", n such a way that we always have expresson: " Y Y2 " (50).
More informationDistributed Control for the Parallel DC Linked Modular Shunt Active Power Filters under Distorted Utility Voltage Condition
Dtrbted Control for the Parallel DC Lnked Modlar Shnt Actve Power Flter nder Dtorted Utlty Voltage Condton Reearch Stdent: Adl Salman Spervor: Dr. Malabka Ba School of Electrcal and Electronc Engneerng
More informationNUMERICAL DIFFERENTIATION
NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the
More informationInformation Acquisition in Global Games of Regime Change (Online Appendix)
Informaton Acquton n Global Game of Regme Change (Onlne Appendx) Mchal Szkup and Iabel Trevno Augut 4, 05 Introducton Th appendx contan the proof of all the ntermedate reult that have been omtted from
More informationSnce h( q^; q) = hq ~ and h( p^ ; p) = hp, one can wrte ~ h hq hp = hq ~hp ~ (7) the uncertanty relaton for an arbtrary state. The states that mnmze t
8.5: Many-body phenomena n condensed matter and atomc physcs Last moded: September, 003 Lecture. Squeezed States In ths lecture we shall contnue the dscusson of coherent states, focusng on ther propertes
More informationFigure 1 Siemens PSSE Web Site
Stability Analyi of Dynamic Sytem. In the lat few lecture we have een how mall ignal Lalace domain model may be contructed of the dynamic erformance of ower ytem. The tability of uch ytem i a matter of
More informationUNIVERSITY OF TORONTO Faculty of Arts and Science. December 2005 Examinations STA437H1F/STA1005HF. Duration - 3 hours
UNIVERSITY OF TORONTO Faculty of Arts and Scence December 005 Examnatons STA47HF/STA005HF Duraton - hours AIDS ALLOWED: (to be suppled by the student) Non-programmable calculator One handwrtten 8.5'' x
More informationAPPROXIMATE FUZZY REASONING BASED ON INTERPOLATION IN THE VAGUE ENVIRONMENT OF THE FUZZY RULEBASE AS A PRACTICAL ALTERNATIVE OF THE CLASSICAL CRI
Kovác, Sz., Kóczy, L.T.: Approxmate Fuzzy Reaonng Baed on Interpolaton n the Vague Envronment of the Fuzzy Rulebae a a Practcal Alternatve of the Clacal CRI, Proceedng of the 7 th Internatonal Fuzzy Sytem
More information290 IEEE TRANSACTIONS ON CIRCUITS AND SYSTEMS I: FUNDAMENTAL THEORY AND APPLICATIONS, VOL. 45, NO. 3, MARCH H d (e j! ;e j!
9 IEEE TRANSACTIONS ON CIRCUITS AND SYSTEMS I: FUNDAMENTAL THEORY AND APPLICATIONS, VOL. 45, NO. 3, MARCH 998 Transactons Brefs Two-Dmensonal FIR Notch Flter Desgn Usng Sngular Value Decomoston S.-C. Pe,
More informationDynamics and Control of 6-DOF Shaking Table with Bell Crank Structure
ICCS2005 June 2-5, KINTEX, Gyeongg-Do, Korea Dynamc and Control of 6-DOF Shakng Table wth Bell Crank Structure Duek-Jae Jeon*, Sung-Ho Park, Young-Jn Park, Youn-Sk Park, Hyoung-Eu Km and Jong-Won Park
More informationSupporting Information. Hydroxyl Radical Production by H 2 O 2 -Mediated. Conditions
Supportng Informaton Hydroxyl Radcal Producton by H 2 O 2 -Medated Oxdaton of Fe(II) Complexed by Suwannee Rver Fulvc Acd Under Crcumneutral Frehwater Condton Chrtopher J. Mller, Andrew L. Roe, T. Davd
More informationBallot Paths Avoiding Depth Zero Patterns
Ballot Paths Avodng Depth Zero Patterns Henrch Nederhausen and Shaun Sullvan Florda Atlantc Unversty, Boca Raton, Florda nederha@fauedu, ssull21@fauedu 1 Introducton In a paper by Sapounaks, Tasoulas,
More informationDifference Equations
Dfference Equatons c Jan Vrbk 1 Bascs Suppose a sequence of numbers, say a 0,a 1,a,a 3,... s defned by a certan general relatonshp between, say, three consecutve values of the sequence, e.g. a + +3a +1
More informationCOMPLEX NUMBERS AND QUADRATIC EQUATIONS
COMPLEX NUMBERS AND QUADRATIC EQUATIONS INTRODUCTION We know that x 0 for all x R e the square of a real number (whether postve, negatve or ero) s non-negatve Hence the equatons x, x, x + 7 0 etc are not
More informationUNIT 7. THE FUNDAMENTAL EQUATIONS OF HYPERSURFACE THEORY
UNIT 7. THE FUNDAMENTAL EQUATIONS OF HYPERSURFACE THEORY ================================================================================================================================================================================================================================================
More informationLinear Form of the Radiative Transfer Equation Revisited. Bormin Huang
Lnear Form of the Radate Tranfer Equaton Reted Bormn Huang Cooerate Inttute for Meteorologcal Satellte Stude, Sace Scence and Engneerng Center Unerty of Wconn Madon The 5 th Internatonal TOVS Study Conference
More informationProblem 10.1: One-loop structure of QED
Problem 10.1: One-loo structure of QED In Secton 10.1 we argued form general rncles that the hoton one-ont and three-ont functons vansh, whle the four-ont functon s fnte. (a Verfy drectly that the one-loo
More informationStatistical Properties of the OLS Coefficient Estimators. 1. Introduction
ECOOMICS 35* -- OTE 4 ECO 35* -- OTE 4 Stattcal Properte of the OLS Coeffcent Etmator Introducton We derved n ote the OLS (Ordnary Leat Square etmator ˆβ j (j, of the regreon coeffcent βj (j, n the mple
More informationCombinational Circuit Design
Combnatonal Crcut Desgn Part I: Desgn Procedure and Examles Part II : Arthmetc Crcuts Part III : Multlexer, Decoder, Encoder, Hammng Code Combnatonal Crcuts n nuts Combnatonal Crcuts m oututs A combnatonal
More informationOn the SO 2 Problem in Thermal Power Plants. 2.Two-steps chemical absorption modeling
Internatonal Journal of Engneerng Reearch ISSN:39-689)(onlne),347-53(prnt) Volume No4, Iue No, pp : 557-56 Oct 5 On the SO Problem n Thermal Power Plant Two-tep chemcal aborpton modelng hr Boyadjev, P
More informationStart Point and Trajectory Analysis for the Minimal Time System Design Algorithm
Start Pont and Trajectory Analy for the Mnmal Tme Sytem Degn Algorthm ALEXANDER ZEMLIAK, PEDRO MIRANDA Department of Phyc and Mathematc Puebla Autonomou Unverty Av San Claudo /n, Puebla, 757 MEXICO Abtract:
More information= z 20 z n. (k 20) + 4 z k = 4
Problem Set #7 solutons 7.2.. (a Fnd the coeffcent of z k n (z + z 5 + z 6 + z 7 + 5, k 20. We use the known seres expanson ( n+l ( z l l z n below: (z + z 5 + z 6 + z 7 + 5 (z 5 ( + z + z 2 + z + 5 5
More informationSolution Methods for Time-indexed MIP Models for Chemical Production Scheduling
Ian Davd Lockhart Bogle and Mchael Farweather (Edtor), Proceedng of the 22nd European Sympoum on Computer Aded Proce Engneerng, 17-2 June 212, London. 212 Elever B.V. All rght reerved. Soluton Method for
More informationMore metrics on cartesian products
More metrcs on cartesan products If (X, d ) are metrc spaces for 1 n, then n Secton II4 of the lecture notes we defned three metrcs on X whose underlyng topologes are the product topology The purpose of
More informationFuzzy approach to solve multi-objective capacitated transportation problem
Internatonal Journal of Bonformatcs Research, ISSN: 0975 087, Volume, Issue, 00, -0-4 Fuzzy aroach to solve mult-objectve caactated transortaton roblem Lohgaonkar M. H. and Bajaj V. H.* * Deartment of
More informationWeek3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity
Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle
More informationPower-sum problem, Bernoulli Numbers and Bernoulli Polynomials.
Power-sum roblem, Bernoull Numbers and Bernoull Polynomals. Arady M. Alt Defnton 1 Power um Problem Fnd the sum n : 1... n where, n N or, usng sum notaton, n n n closed form. Recurrence for n Exercse Usng
More informationbounds compared to SB and SBB bounds as the former two have an index parameter, while the latter two
1 Queung Procee n GPS and PGPS wth LRD Traffc Input Xang Yu, Ian L-Jn Thng, Yumng Jang and Chunmng Qao Department of Computer Scence and Engneerng State Unverty of New York at Buffalo Department of Electrcal
More information( ) = ( ) + ( 0) ) ( )
EETOMAGNETI OMPATIBIITY HANDBOOK 1 hapter 9: Transent Behavor n the Tme Doman 9.1 Desgn a crcut usng reasonable values for the components that s capable of provdng a tme delay of 100 ms to a dgtal sgnal.
More informationStatistics for Managers Using Microsoft Excel/SPSS Chapter 14 Multiple Regression Models
Statstcs for Managers Usng Mcrosoft Excel/SPSS Chapter 14 Multple Regresson Models 1999 Prentce-Hall, Inc. Chap. 14-1 Chapter Topcs The Multple Regresson Model Contrbuton of Indvdual Independent Varables
More informationn α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0
MODULE 2 Topcs: Lnear ndependence, bass and dmenson We have seen that f n a set of vectors one vector s a lnear combnaton of the remanng vectors n the set then the span of the set s unchanged f that vector
More informationChapter 8. Potential Energy and Conservation of Energy
Chapter 8 Potental Energy and Conservaton of Energy In ths chapter we wll ntroduce the followng concepts: Potental Energy Conservatve and non-conservatve forces Mechancal Energy Conservaton of Mechancal
More informationAGC Introduction
. Introducton AGC 3 The prmary controller response to a load/generaton mbalance results n generaton adjustment so as to mantan load/generaton balance. However, due to droop, t also results n a non-zero
More informationA MODIFIED METHOD FOR SOLVING SYSTEM OF NONLINEAR EQUATIONS
Journal of Mathematcs and Statstcs 9 (1): 4-8, 1 ISSN 1549-644 1 Scence Publcatons do:1.844/jmssp.1.4.8 Publshed Onlne 9 (1) 1 (http://www.thescpub.com/jmss.toc) A MODIFIED METHOD FOR SOLVING SYSTEM OF
More informationSupplementary Notes for Chapter 9 Mixture Thermodynamics
Supplementary Notes for Chapter 9 Mxture Thermodynamcs Key ponts Nne major topcs of Chapter 9 are revewed below: 1. Notaton and operatonal equatons for mxtures 2. PVTN EOSs for mxtures 3. General effects
More informationMODERN systems theory has its roots in electrical. Why RLC realizations of certain impedances need many more energy storage elements than expected
Why RLC realzaton of certan mpedance need many more energy torage element than expected Tmothy H. Hughe arxv:6.0658v [c.sy] Jan 08 btract It a gnfcant and longtandng puzzle that the retor, nductor, capactor
More informationImage Registration for a Series of Chest Radiograph Images
Proceedng of the 5th WE Internatonal Conference on gnal Proceng, Itanbul, Turkey, May 7-9, 006 (pp179-184) Image Regtraton for a ere of Chet Radograph Image Omar Mohd. Rjal*, Norlza Mohd. Noor, hee Lee
More informationChapter.4 MAGNETIC CIRCUIT OF A D.C. MACHINE
Chapter.4 MAGNETIC CIRCUIT OF A D.C. MACHINE The dfferent part of the dc machne manetc crcut / pole are yoke, pole, ar ap, armature teeth and armature core. Therefore, the ampere-turn /pole to etablh the
More informationCHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE
CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE Analytcal soluton s usually not possble when exctaton vares arbtrarly wth tme or f the system s nonlnear. Such problems can be solved by numercal tmesteppng
More informationRICCI TYPE IDENTITIES FOR BASIC DIFFERENTIATION AND CURVATURE TENSORS IN OTSUKI SPACES 1
wnov Sad J. Math. wvol., No., 00, 7-87 7 RICCI TYPE IDENTITIES FOR BASIC DIFFERENTIATION AND CURVATURE TENSORS IN OTSUKI SPACES Svetlav M. Mnčć Abtract. In the Otuk ace ue made of two non-ymmetrc affne
More informationQuick Visit to Bernoulli Land
Although we have een the Bernoull equaton and een t derved before, th next note how t dervaton for an uncopreble & nvcd flow. The dervaton follow that of Kuethe &Chow ot cloely (I lke t better than Anderon).
More informationLecture # 02: Pressure measurements and Measurement Uncertainties
AerE 3L & AerE343L Lecture Notes Lecture # 0: Pressure measurements and Measurement Uncertantes Dr. Hu H Hu Deartment of Aerosace Engneerng Iowa State Unversty Ames, Iowa 500, U.S.A Mechancal Pressure
More informationCorrelations in Underwater Acoustic Particle Velocity and Pressure Channels H. Guo 1, A. Abdi 1, A. Song 2, and M.Badiey 2
Correlaton n Underwater Acoutc Partcle Veloct Preure Channel H. Guo A. Ad A. Song M.Bade Center for Wrele Councaton Sgnal Proceng Reearch et. of Electrcal Couter Engneerng New Jere Inttute of Technolog
More information