Performance of Microstrip Directional Coupler Using Synthesis Technique

Size: px
Start display at page:

Download "Performance of Microstrip Directional Coupler Using Synthesis Technique"

Transcription

1 ISSN: Vl., Issu, March 0 Prrmanc Micrstrip Dirctinal uplr Using Synthsis Tchniqu Vijayan T Asst. Prssr, Dpt E&I, Bharath Univrsity, hnnai-60007, India ABSTRAT: Th intrducd dsign mthd rquirs nly th inrmatin th prt impdancs, th cupling lvl, and th pratinal rquncy. Th dsign charts that giv all th physical dimnsins, including th lngth th dirctinal cuplr vrsus rquncy and dirnt cupling lvls, ar givn r alumina, Tln, RO00, FR, and RF-60, which ar widly usd in micrwav applicatins. Furthr wrk includs validatin analytical rsults using a planar lctrmagntic simulatin tl (IED) and xprimntal vriicatin. KEYWORDS: upld lins, dirctinal cuplrs, micrstrip. I. INTRODUTION Micrstrip dirctinal cuplrs hav bn cmmnly usd in micrwav systms r masuring transmittd and rlctd pwr with accuracy. Thy hav svral advantags. Such as manuacturability, Fig. Tw-lin micrstrip dirctinal cuplr rpatability, and lw cst. Extnsiv rsarch has bn cnductd n th dsign micrstrip dirctinal cuplrs du t thir widsprad applicatin. Th xisting dsign prcdurs in th litratur dpnd n knwldg th physical gmtry th dirctinal cuplr. As a rsult, availabl dsign charts giv physical dimnsins th dirctin al cuplr vrsus vn-and dd-md impdancs th dirctinal cuplr. Hwvr, in practic, th physical lngth th dirctinal cuplr is initially unknwn t th dsignr. Dsignrs hav nly inrmatin abut th prt impdancs, th rquird cupling lvl, and th pratinal rquncy at th initial stag thir dsign. Bcaus this, it is quit cumbrsm t us xisting dsign chats with n prir knwldg th gmtry th dirctinal cuplr. This rquirs svral itratins t inali th dsign.th gmtry a symmtrical micr strip dirctinal cuplr is shwn in ig.. Th mthds givn by Bryant and Wiss [] and Kirschning and Jansn [] ar amng th irst rliabl and accurat mthds t btain inrmatin n cupld micrstrip transmissin lins. Many rsarchrs usd tchniqus similar t th ns prsntd in [] and [] and studid micr strip dirctinal cuplr dsign r mr than 0 yars. Hwvr, dsign charts in th litratur giv nly th physical paramtrs th dirctinal cuplr vrsus th vn-and ddmd impdancs and, as a rsult, ar nt practically applicabl n ral applicatins. On has t us ths charts and wrk backward t btain th rquird dsign paramtrs r b dirctinal cuplrs. This is a quit tdius and inicint way digning any RF/micrwav dvic. Akhtarad tal. [] giv a dsign mthd that sms t rlct th dsign prcdur that inds an applicatin in practic. In [], th synthsis tchniqu is usd, and it has an intrmdiat stp calculating th strip width th singl micr strip lin that crrspnds t vn-and dd-md impdancs th cupld lins. Hwvr, sm critical crrctins hav t b applid t th rmulatins givn in [] t hav accurat rsults. Thr ar tw sparat crrctins rprtd by Hintn [] and Gupta tal. [5] r th wrk in []. Althugh th rrr sms t b rducd in cmparisn t th n in th riginal wrk [] with th applicatin ach crrctin, th rrr can still b mr than 0% r th lw-prmittivity matrials such as Tln and r small valus shap and spacing ratis i th crrctin in [] and [5] ar nt mplyd tgthr. W rprt that whn th crrctins in [] and [5] ar mplyd tgthr, th accuracy th rsults incrass and th rrr rducs t within pyright t IJAREEIE 76

2 ISSN: Vl., Issu, March 0 % with th xprimntal rsults, vn whn using lw-prmittivity matrials such as Tln and FR. This is rprtd by Erglu [6]. Hwvr, in [6], th mthd has nly bn applid n Tln and FR, and dsign charts and paramtrs hav nt bn givn r discussd. Dsign charts ar critical in th dsign prcss and mak it pssibl t dsign dirctinal cuplrs withut using any quatins. In additin, th mthd accuracy has nt bn vriid using dirnt dilctric matrials br. Furthrmr, th applicatin th crrctins n th rmulatins has nt bn prsntd. In this papr, a thr-stp dign prcdur with accurat clsd rmulas that giv a cmplt dsign symmtrical tw-lin micrstrip dirctinal cuplrs that includ th physical lngth at th dsird pratinal rquncy is intrducd. Our dsign prcdur rquirs knwldg th prt trminatin impdancs, th cupling lvl, and th pratinal rquncy. W als giv th dsign charts that ar mst ndd by th dsignr. Our dsign charts btaind r th iv mst ppular matrials usd in micrwav applicatins: alumina, Tln, RO00, FR, RF-60. In th dsign charts, th cupling lvl is givn vrsus th physical dimnsins th dirctinal cuplr. W als prvid dsign charts that shw th physical lngth th dirctinal cuplr l vrsus th rquncy r th givn cupling lvl. W validatd ur analytical rsults with th planar lctrmagntic (EM) simulatin tl [7] and thn xprimntally vriid thm. W shw that th rrr btwn th analytical and th simulatin rsults is rducd t b within 0.% r high-prmittivity matrials lik alumina. Th cmplt dsign a tw-lin micrstrip dirctinal cuplr can b btaind r th irst tim using ur rsults in this papr. A dsignr can us ithr th clsd-rm slutins r th dsign charts prsntd hr t hav a cmplt dsign. II. FORMULATION AND SOLUTIONS In ral wrld nginring applicatins, th physical paramtrs th dirctinal cuplrs ar unknwn t th dsignr at th bginning th dsign. Th nly inrmatin availabl t th dsignr at th bginning dsign is th prt trminatin impdancs, th cupling lvl, and th pratinal rquncy. In practic, th trminatin impdanc r ach prt th dirctinal cuplr is dsird t b 50Ω r mst applicatins. Th matchd systm is accmplishd whn th charactristic impdanc = is qual t th prt impdanc. Th xisting dsign prcdur bgins with inding th vn-and dd-md impdancs and by using th charts givn r w/ h and s / h.thn, th dsignr nds t calculat th cupling lvl and th charactristic impdanc. I it ds nt givn th dsird cupling lvl, prcdur nds t b rpatd until th spciicatins ar mt. This prcdur is quit cumbrsm. Furthrmr, thr sms t b n dsign chart availabl r th physical lngth th dirctinal cuplr. Th physical lngth th dirctinal cuplr l r cupld lins dpnds n th ctiv prmittivity cnstant ε th structur ar knwn. Th analytical mthd that is givn by Bahl [8] sms t b accurat and is adaptd in this papr t ind th physical lngth th dirctinal cuplr. In this papr, w us th mthd prpsd by Akhtarad tal. [] t btain th spacing rati s / h and th shap rati w/ h th dirctinal cuplr illustratd in Fig.. W cncurrntly apply th crrctins givn in [] and [5]. Th physical lngth th dirctinal cuplr is btaind using th mthd givn in [8]. As utlind in sctin. W assum that th prt impdancs, which ar qual and rrrd t as th rward cupling lvl, and th pratinal rquncy, ar knwn paramtrs at th bginning th dsign. Basd n th knwn paramtrs, th prpsd dsign prcdur has th llwing thr stps. Stp -Find Evn- and Odd-Md Impdancs Th vn and dd impdancs and th micrstrip cuplr givn in Fig. can b und rm = () = 0 () Whr rward cupling rquirmnt and is givn in dcibls. Stp -Find Physical Dimnsins w/ h and s / h Th physical dimnsins th dirctinal cuplr ar und using th synthsis mthd prpsd in [] and applying th crrctins givn in [] and [5]. Whn th crrctins ar mplyd, w gt th llwing quatin r th spacing rati s / h th cuplr in Fig.: pyright t IJAREEIE 76

3 ISSN: Vl., Issu, March 0 w w csh csh - - csh h s h s s h w w csh - csh h s h s w h s w h and s gmtry, rspctivly. () ar th shap ratis r th quivalnt singl cas that crrspnds t vn and dd-md w h s is mdiid trm r th shap rati and is dirnt rm th n that is givn in [] and [5] and ar dtaild blw. w h is th crrctd shap rati r th singl micrstrip lin, and it is xprssd as [] w h 8 whr 7 R r r xp r R xp r -. R r R (5) s and s w h s, rspctivly. Thy givn as s (6) ar th charactristic impdancs that crrspnd t singl micrstrip shap ratis w h s s (7) w w w w s (8) s h s h h s h Th crrctd trm w h in () is givn as [5] s w w w (0) h s h s h s Th updatd rmula in () givs accurat rsults r th spacing rati s h th symmtrical tw-lin micrstrip dirctinal cuplr whn usd with (). Atr th spacing rati s h r th cupld lins is und, w can prcd t ind w h r th cupld lins, as dscribd in []. Th shap rati r th cupld lins is - s w h csh d - () h whr w csh g g - d h s () s g csh () h Stp -Find th Physical Lngth th Dirctinal uplr: Th physical lngth th dirctinal cuplr is btaind using c l () 8 whr c *0 m s, and is pratinal rquncy in hrt. Hnc, th lngth th dirctinal cuplr can b und i th ctiv prmittivity cnstant can b und using th mthd dscribd in [8] as llws: (5) and ar th ctiv prmittivity cnstants th cupld structur r dd and vn mds, rspctivly. and dpnds n vn- and dd-md capacitanc and as (9) () and pyright t IJAREEIE 76

4 ISSN: Vl., Issu, March 0 (6a) (6b), is th capacitanc with air as dilctric. All th capacitancs ar givn as capacitanc pr unit lngth. ) Evn-Md apacitanc alculatin: Th vn-md capacitanc is (7) p p is th paralll plat capacitanc and is dind as w p r (8) h whr w h is und in Sctin.B. is th ringing capacitanc du t th micrstrips bing takn aln as i thy wr a singl strip, which is qual t s p - (9) c Hr, s is th ctiv prmittivity cnstant a singl strip micrstrip, which can b xprssd as r r - s - Fw h (0) whr w is givn by th llwing h w 0.0- w h Fw h h w quatin:,, r h w r h () r w A xp h 0h A tanh -0.xp.-.5 () s h s s ) Odd-Md apacitanc calculatin: Th dd-md capacitanc is p ga gd () ga is th capacitanc trm in dd md r th ringing ild acrss th gap in th air rgin. It can b writtn as K k ga (5) Kk whr K k K k ln, 0 k - k k ln - k s h k s w h h 0.5 k, 0.5 k (6) (7) k - k (8) gd rprsnts th capacitanc in dd md r th ringing ild acrss th gap in th dilctric rgin. It can b und using pyright t IJAREEIE 76

5 r s 0.0 gd ln cth 0.65 h s h Sinc ISSN: Vl., Issu, March 0 (9) r - r c (0) () c thn w can writ () c c () Substituting (7), (), (), and () in t (6) givs th vn and dd-md ctiv prmittivitis and. Whn (6) is substitutd int (5), w can ind th ctiv prmittivity cnstant th cupld structur. Nw, () can b usd t calculatd th physical lngth th dirctinal cuplr at th pratinal rquncy..6.. vs [s/h] Alumina Tln RO00 FR RF- 60 [s/h] Fig upling in (db) s h vrsus cupling lvl r alumina, Tln, RO00, FR, and RF-60. TABLE DESIGN PARAMETERS OF A TWO-LINE MIROSTRIP DIRETIONAL OUPLER AT 00 MHZ FOR 50 Z O III. DESIGN HARTS In this sctin, w giv th dsign charts t btain a cmplt dsign r a tw-lin symmtrical micrstrip dirctinal cuplr r th llwing iv dirnt matrials: ) alumina; ) Tln; ) RO00; ) FR; 5) RF-60. Fig. givs th spacing rati s h th dirctinal cuplr vrsus dirnt cupling lvls. Fig. givs th shap rati th pyright t IJAREEIE 765

6 ISSN: Vl., Issu, March 0 w h vrsus dirnt cupling lvls. Fig. -8 giv th physical lngth l th dirctinal cuplr dirctinal cuplr vrsus rquncy at dirnt cupling lvls r -0dB..5 vs [w/h] Alumina Tln RO00 FR RF- 60 [w/h] Fig upling (db) w h vrsus cupling lvl r alumina, Tln, RO00, FR, and RF x Alumina Dirctinal uplr Lngth (in) Frquncy (MH) Fig.. Dirctinal cuplr lngth l vrsus rquncy r alumina at -0(dB), cupling. 6 x Tln Dirctinal uplr Lngth (in) Frquncy (MH) Fig. 5. Dirctinal cuplr lngth l vrsus rquncy r Tln at -0(dB), cupling. 5.5 x 06 5 RO00 Dirctinal uplr Lngth (in) Frquncy (MH) Fig. 6. Dirctinal cuplr lngth l vrsus rquncy r RO00 at -0(dB), cupling. 5 x 06.5 FR Dirctinal uplr Lngth (in) Frquncy (MH) Fig. 7. Dirctinal cuplr lngth l vrsus rquncy r FR at -0(dB), cupling. pyright t IJAREEIE 766

7 ISSN: Vl., Issu, March 0.5 x 06 RF - 60 Dirctinal uplr Lngth (in) Frquncy (MH) Fig. 8. Dirctinal cuplr lngth l vrsus rquncy r RF-60 at -0(dB), cupling. IV.ONLUSION In this papr, a practical and cmplt mthd t hav a symmtrical tw-lin micrstrip dirctinal cuplr has bn prsntd by analytically intrducing a thr-stp dsign prcdur. Our dsign prcdur rquirs knwldg th prt trminatin impdancs, th cupling lvl, and th pratinal rquncy, which ar th thr paramtrs that ar knwn at th bginning th dsign in practic. Th dsign charts that giv th shap and spacing ratis vrsus dirnt cupling lvls r iv dirnt matrials that hav rlativ prmittivitis btwn.08 r 9.8 ar prsntd. W als giv dsign charts that shw th physical lngth th dirctinal cuplr vrsus rquncy at dirnt cupling lvls r th iv matrials. REFERENES [] Abdullah Erglu, and Jay Kyn L, Th mplt Dsign Micrstrip Dirctinal uplrs Using th Synthsis Tchniqu IEEE Transactin n instrumntatin and masurmnt, vl.57, n., Dcmbr [] T.G.Bryant and J.A.Wiss, Paramtrs micrstrip transmissin lins and cupld pairs micrstrip lins, IEEE Trans. Micrw. Thry Tch., vl. MTT-6, n., pp.0-07, Dc [] M.Kirschning and R.H.Jansn, Accurat wid-rang dsign quatins r th rquncy-dpndnt charactristic paralll cupld micrstrip lins, IEEE Trans. Mirw. Thry Tch., vl. MTT-, n., pp Jan. 98. [] S.Akhtarad, T.R.Rwwbtham, and P.B.Jns, Th dsign cupld micrstrip lins, IEEE Trans. Micrw. Thry Tch., vl. MTT-, n.6, pp. 86-9, Jun [5] J.J.Hintn, On dsign cupld micrstrip lins, IEEE Trans. Micrw. Thry Tch., vl. MTT-8, n., p. 7, mar [6] K..Gupta, R.Garg, and R.hadha, mputr-aidd Dsign Micrwav circuits. Nrwd, MA: Artch Hus, 98, ch.. [7] A. Erglu, Practical dsign micrstrip dirctinal cuplrs, in prc. IEEE AP-S, Jul. 9-, 006, pp [8] I.Bhal, Lumpd Elmnts r RF and Micrwav circuits. Nrwd, MA: Artch Hus, 00. [9] Dilctric nstant Rrnc Guid. [nlin].availabl:htpp://clipprcntrls.cm/in/dilctric_cnstants.html [0] Mat lab vrsin 7.. [] Transimmisin lins prprtis a strip n a dilctric sht n a plan, IEEE Trans. Micrwav Thry Tch., vl. MTT-5, pp. 6-67, Aug [] H.A.Whlr, Transmissin-lin prprtis paralll strips sparatd by dilctric sht, IEEE Trans. Micrwav Thry Tch., vl. MTT-, pp. 7-85, mar [] G.Plicky and H.L. Stvr, paralll-cupld lins n micrstrip, Txas instrumnts, inc, Rpt [], haractristics cupld micrstrip lins, RA Rv., vl., pp , spt pyright t IJAREEIE 767

Lecture 26: Quadrature (90º) Hybrid.

Lecture 26: Quadrature (90º) Hybrid. Whits, EE 48/58 Lctur 26 Pag f Lctur 26: Quadratur (9º) Hybrid. Back in Lctur 23, w bgan ur discussin f dividrs and cuplrs by cnsidring imprtant gnral prprtis f thrand fur-prt ntwrks. This was fllwd by

More information

. This is made to keep the kinetic energy at outlet a minimum.

. This is made to keep the kinetic energy at outlet a minimum. Runnr Francis Turbin Th shap th blads a Francis runnr is cmplx. Th xact shap dpnds n its spciic spd. It is bvius rm th quatin spciic spd (Eq.5.8) that highr spciic spd mans lwr had. This rquirs that th

More information

Lecture 27: The 180º Hybrid.

Lecture 27: The 180º Hybrid. Whits, EE 48/58 Lctur 7 Pag f 0 Lctur 7: Th 80º Hybrid. Th scnd rciprcal dirctinal cuplr w will discuss is th 80º hybrid. As th nam implis, th utputs frm such a dvic can b 80º ut f phas. Thr ar tw primary

More information

Even/Odd Mode Analysis of the Wilkinson Divider

Even/Odd Mode Analysis of the Wilkinson Divider //9 Wilkinn Dividr Evn and Odd Md Analyi.dc / Evn/Odd Md Analyi f th Wilkinn Dividr Cnidr a matchd Wilkinn pwr dividr, with a urc at prt : Prt Prt Prt T implify thi chmatic, w rmv th grund plan, which

More information

Sensors and Actuators Introduction to sensors

Sensors and Actuators Introduction to sensors Snsrs and Actuatrs Intrductin t snsrs Sandr Stuijk (s.stuijk@tu.nl) Dpartmnt f Elctrical Enginring Elctrnic Systms APAITIVE IUITS (haptr., 7., 9., 0.6,.,.) apaciti snsr capacitanc dpnds n physical prprtis

More information

Chapter 2 Linear Waveshaping: High-pass Circuits

Chapter 2 Linear Waveshaping: High-pass Circuits Puls and Digital Circuits nkata Ra K., Rama Sudha K. and Manmadha Ra G. Chaptr 2 Linar Wavshaping: High-pass Circuits. A ramp shwn in Fig.2p. is applid t a high-pass circuit. Draw t scal th utput wavfrm

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

Microwave Engineering

Microwave Engineering Micrwav Enginring hng-hsing Hsu Dpartmnt f Elctrical Enginring Natinal Unitd Univrsity Outlin. Transmissin Lin Thry. Transmissin Lins and Wavguids Gnral lutins fr TEM, TE, and TM wavs ; Paralll Plat wavguid

More information

LECTURE 5 Guassian Wave Packet

LECTURE 5 Guassian Wave Packet LECTURE 5 Guassian Wav Pact 1.5 Eampl f a guassian shap fr dscribing a wav pact Elctrn Pact ψ Guassian Assumptin Apprimatin ψ As w hav sn in QM th wav functin is ftn rprsntd as a Furir transfrm r sris.

More information

ECE 344 Microwave Fundamentals

ECE 344 Microwave Fundamentals ECE 44 Microwav Fundamntals Lctur 08: Powr Dividrs and Couplrs Part Prpard By Dr. hrif Hkal 4/0/08 Microwav Dvics 4/0/08 Microwav Dvics 4/0/08 Powr Dividrs and Couplrs Powr dividrs, combinrs and dirctional

More information

Another Explanation of the Cosmological Redshift. April 6, 2010.

Another Explanation of the Cosmological Redshift. April 6, 2010. Anthr Explanatin f th Csmlgical Rdshift April 6, 010. Jsé Francisc García Juliá C/ Dr. Marc Mrncian, 65, 5. 4605 Valncia (Spain) E-mail: js.garcia@dival.s h lss f nrgy f th phtn with th tim by missin f

More information

Topic 5: Discrete-Time Fourier Transform (DTFT)

Topic 5: Discrete-Time Fourier Transform (DTFT) ELEC36: Signals And Systms Tpic 5: Discrt-Tim Furir Transfrm (DTFT) Dr. Aishy Amr Cncrdia Univrsity Elctrical and Cmputr Enginring DT Furir Transfrm Ovrviw f Furir mthds DT Furir Transfrm f Pridic Signals

More information

Part 7: Capacitance And Capacitors

Part 7: Capacitance And Capacitors Part 7: apacitanc And apacitors 7. Elctric harg And Elctric Filds onsidr a pair of flat, conducting plats, arrangd paralll to ach othr (as in figur 7.) and sparatd by an insulator, which may simply b air.

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

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

Chapter 33 Gauss s Law

Chapter 33 Gauss s Law Chaptr 33 Gauss s Law 33 Gauss s Law Whn askd t find th lctric flux thrugh a clsd surfac du t a spcifid nn-trivial charg distributin, flks all t ftn try th immnsly cmplicatd apprach f finding th lctric

More information

A Unified Theory of rf Plasma Heating. J.e. Sprott. July 1968

A Unified Theory of rf Plasma Heating. J.e. Sprott. July 1968 A Unifid Thry f rf Plasma Hating by J.. Sprtt July 968 PLP 3 Plasma Studis Univrsity f iscnsin INTRODUCfION In this papr, th majr rsults f PLP's 86 and 07 will b drivd in a mr cncis and rigrus way, and

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

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark Answr omwork 5 PA527 Fall 999 Jff Stark A patint is bing tratd with Drug X in a clinical stting. Upon admiion, an IV bolus dos of 000mg was givn which yildd an initial concntration of 5.56 µg/ml. A fw

More information

5 Curl-free fields and electrostatic potential

5 Curl-free fields and electrostatic potential 5 Curl-fr filds and lctrstatic tntial Mathmaticall, w can gnrat a curl-fr vctr fild E(,, ) as E = ( V, V, V ), b taking th gradint f an scalar functin V (r) =V (,, ). Th gradint f V (,, ) is dfind t b

More information

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic

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

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

The Frequency Response of a Quarter-Wave Matching Network

The Frequency Response of a Quarter-Wave Matching Network 4/1/29 Th Frquncy Rsons o a Quartr 1/9 Th Frquncy Rsons o a Quartr-Wav Matchg Ntwork Q: You hav onc aga rovidd us with conusg and rhas uslss ormation. Th quartr-wav matchg ntwork has an xact SFG o: a Τ

More information

PHYS-333: Problem set #2 Solutions

PHYS-333: Problem set #2 Solutions PHYS-333: Problm st #2 Solutions Vrsion of March 5, 2016. 1. Visual binary 15 points): Ovr a priod of 10 yars, two stars sparatd by an angl of 1 arcsc ar obsrvd to mov through a full circl about a point

More information

General Notes About 2007 AP Physics Scoring Guidelines

General Notes About 2007 AP Physics Scoring Guidelines AP PHYSICS C: ELECTRICITY AND MAGNETISM 2007 SCORING GUIDELINES Gnral Nots About 2007 AP Physics Scoring Guidlins 1. Th solutions contain th most common mthod of solving th fr-rspons qustions and th allocation

More information

ECE602 Exam 1 April 5, You must show ALL of your work for full credit.

ECE602 Exam 1 April 5, You must show ALL of your work for full credit. ECE62 Exam April 5, 27 Nam: Solution Scor: / This xam is closd-book. You must show ALL of your work for full crdit. Plas rad th qustions carfully. Plas chck your answrs carfully. Calculators may NOT b

More information

Deepak Rajput

Deepak Rajput Q Prov: (a than an infinit point lattic is only capabl of showing,, 4, or 6-fold typ rotational symmtry; (b th Wiss zon law, i.. if [uvw] is a zon axis and (hkl is a fac in th zon, thn hu + kv + lw ; (c

More information

PHYS ,Fall 05, Term Exam #1, Oct., 12, 2005

PHYS ,Fall 05, Term Exam #1, Oct., 12, 2005 PHYS1444-,Fall 5, Trm Exam #1, Oct., 1, 5 Nam: Kys 1. circular ring of charg of raius an a total charg Q lis in th x-y plan with its cntr at th origin. small positiv tst charg q is plac at th origin. What

More information

What are those βs anyway? Understanding Design Matrix & Odds ratios

What are those βs anyway? Understanding Design Matrix & Odds ratios Ral paramtr stimat WILD 750 - Wildlif Population Analysis of 6 What ar thos βs anyway? Undrsting Dsign Matrix & Odds ratios Rfrncs Hosmr D.W.. Lmshow. 000. Applid logistic rgrssion. John Wily & ons Inc.

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

Chapter 2: Examples of Mathematical Models for Chemical Processes

Chapter 2: Examples of Mathematical Models for Chemical Processes Chaptr 2: Exampls Mathmatical Mdls r Chmical Prcsss In this chaptr w dvlp mathmatical mdls r a numbr lmntary chmical prcsss that ar cmmnly ncuntrd in practic. W will apply th mthdlgy discussd in th prvius

More information

Modern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom

Modern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom Mdrn Physics Unit 5: Schrödingr s Equatin and th Hydrgn Atm Lctur 5.6: Enrgy Eignvalus f Schrödingr s Equatin fr th Hydrgn Atm Rn Rifnbrgr Prfssr f Physics Purdu Univrsity 1 Th allwd nrgis E cm frm th

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator. Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r

More information

Extraction of Doping Density Distributions from C-V Curves

Extraction of Doping Density Distributions from C-V Curves Extraction of Doping Dnsity Distributions from C-V Curvs Hartmut F.-W. Sadrozinski SCIPP, Univ. California Santa Cruz, Santa Cruz, CA 9564 USA 1. Connction btwn C, N, V Start with Poisson quation d V =

More information

EE 119 Homework 6 Solution

EE 119 Homework 6 Solution EE 9 Hmwrk 6 Slutin Prr: J Bkr TA: Xi Lu Slutin: (a) Th angular magniicatin a tlcp i m / th cal lngth th bjctiv ln i m 4 45 80cm (b) Th clar aprtur th xit pupil i 35 mm Th ditanc btwn th bjctiv ln and

More information

A Brief and Elementary Note on Redshift. May 26, 2010.

A Brief and Elementary Note on Redshift. May 26, 2010. A Brif and Elmntary Nt n Rdshift May 26, 2010. Jsé Francisc García Juliá C/ Dr. Marc Mrncian, 65, 5. 46025 Valncia (Spain) E-mail: js.garcia@dival.s Abstract A rasnabl xplanatin f bth rdshifts: csmlgical

More information

2008 AP Calculus BC Multiple Choice Exam

2008 AP Calculus BC Multiple Choice Exam 008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl

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

ph People Grade Level: basic Duration: minutes Setting: classroom or field site

ph People Grade Level: basic Duration: minutes Setting: classroom or field site ph Popl Adaptd from: Whr Ar th Frogs? in Projct WET: Curriculum & Activity Guid. Bozman: Th Watrcours and th Council for Environmntal Education, 1995. ph Grad Lvl: basic Duration: 10 15 minuts Stting:

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

Additivity of Capacitive and Inductive Coupling in Submicronic Interconnects

Additivity of Capacitive and Inductive Coupling in Submicronic Interconnects Additivity f apacitiv and Inductiv upling in Submicrnic Intrcnncts Jan-Etinn Lrival, Dnis Dschacht, Yvs Quéré, Thirry L Guguc, Fabric Hurt T cit this vrsin: Jan-Etinn Lrival, Dnis Dschacht, Yvs Quéré,

More information

cycle that does not cross any edges (including its own), then it has at least

cycle that does not cross any edges (including its own), then it has at least W prov th following thorm: Thorm If a K n is drawn in th plan in such a way that it has a hamiltonian cycl that dos not cross any dgs (including its own, thn it has at last n ( 4 48 π + O(n crossings Th

More information

Chapter 3 Lecture 14 Longitudinal stick free static stability and control 3 Topics

Chapter 3 Lecture 14 Longitudinal stick free static stability and control 3 Topics Chaptr 3 Lctur 14 Longitudinal stick fr static stability and control 3 Topics 3.4.4 Rquirmnt for propr stick forc variation 3.4.5 Fl of th stability lvl by th pilot Exampl 3.3 3.5 Dtrmination of stick-fr

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

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17)

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17) MCB37: Physical Biology of th Cll Spring 207 Homwork 6: Ligand binding and th MWC modl of allostry (Du 3/23/7) Hrnan G. Garcia March 2, 207 Simpl rprssion In class, w drivd a mathmatical modl of how simpl

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

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

Impedance (T) EELE 461/561 Digital System Design. Module #3 Interconnect Modeling with Distributed Elements Topics. Transmission Lines

Impedance (T) EELE 461/561 Digital System Design. Module #3 Interconnect Modeling with Distributed Elements Topics. Transmission Lines EEE 46/56 igital Systm sign Modul #3 ntrconnct Modling with istributd Elmnts Topics. mpdanc of Transmission ins Ttbook Rading Assignmnts Transmission ins mpdanc T - Transmission ins ar istributd lmnts

More information

Introduction to the quantum theory of matter and Schrödinger s equation

Introduction to the quantum theory of matter and Schrödinger s equation Introduction to th quantum thory of mattr and Schrödingr s quation Th quantum thory of mattr assums that mattr has two naturs: a particl natur and a wa natur. Th particl natur is dscribd by classical physics

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

Lenses & Prism Consider light entering a prism At the plane surface perpendicular light is unrefracted Moving from the glass to the slope side light

Lenses & Prism Consider light entering a prism At the plane surface perpendicular light is unrefracted Moving from the glass to the slope side light Lnss & Prism Considr light ntring a prism At th plan surac prpndicular light is unrractd Moving rom th glass to th slop sid light is bnt away rom th normal o th slop Using Snll's law n sin( ϕ ) = n sin(

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

FUNDAMENTAL AND SECOND HARMONIC AMPLITUDES IN A COLLISIONAL MAGNETOACTIVE PLASMA UDC B. M. Jovanović, B. Živković

FUNDAMENTAL AND SECOND HARMONIC AMPLITUDES IN A COLLISIONAL MAGNETOACTIVE PLASMA UDC B. M. Jovanović, B. Živković FACTA UNIVERSITATIS Sris: Physics, Chmistry and Tchnlgy Vl., N 5, 3, pp. 45-51 FUNDAMENTAL AND SECOND HARMONIC AMPLITUDES IN A COLLISIONAL MAGNETOACTIVE PLASMA UDC 533.9 B. M. Jvanvić, B. Živkvić Dpartmnt

More information

First derivative analysis

First 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 information

ECE 2210 / 00 Phasor Examples

ECE 2210 / 00 Phasor Examples EE 0 / 00 Phasor Exampls. Add th sinusoidal voltags v ( t ) 4.5. cos( t 30. and v ( t ) 3.. cos( t 5. v ( t) using phasor notation, draw a phasor diagram of th thr phasors, thn convrt back to tim domain

More information

0WAVE PROPAGATION IN MATERIAL SPACE

0WAVE PROPAGATION IN MATERIAL SPACE 0WAVE PROPAGATION IN MATERIAL SPACE All forms of EM nrgy shar thr fundamntal charactristics: 1) thy all tral at high locity 2) In traling, thy assum th proprtis of was 3) Thy radiat outward from a sourc

More information

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals. Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby

More information

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK Data Assimilation 1 Alan O Nill National Cntr for Earth Obsrvation UK Plan Motivation & basic idas Univariat (scalar) data assimilation Multivariat (vctor) data assimilation 3d-Variational Mthod (& optimal

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

1 1 1 p q p q. 2ln x x. in simplest form. in simplest form in terms of x and h.

1 1 1 p q p q. 2ln x x. in simplest form. in simplest form in terms of x and h. NAME SUMMER ASSIGNMENT DUE SEPTEMBER 5 (FIRST DAY OF SCHOOL) AP CALC AB Dirctions: Answr all of th following qustions on a sparat sht of papr. All work must b shown. You will b tstd on this matrial somtim

More information

+ f. e f. Ch. 8 Inflation, Interest Rates & FX Rates. Purchasing Power Parity. Purchasing Power Parity

+ f. e f. Ch. 8 Inflation, Interest Rates & FX Rates. Purchasing Power Parity. Purchasing Power Parity Ch. 8 Inlation, Intrst Rats & FX Rats Topics Purchasing Powr Parity Intrnational Fishr Ect Purchasing Powr Parity Purchasing Powr Parity (PPP: Th purchasing powr o a consumr will b similar whn purchasing

More information

Aim To manage files and directories using Linux commands. 1. file Examines the type of the given file or directory

Aim To manage files and directories using Linux commands. 1. file Examines the type of the given file or directory m E x. N o. 3 F I L E M A N A G E M E N T Aim To manag ils and dirctoris using Linux commands. I. F i l M a n a g m n t 1. il Examins th typ o th givn il or dirctory i l i l n a m > ( o r ) < d i r c t

More information

DIELECTRIC AND MAGNETIC PROPERTIES OF MATERIALS

DIELECTRIC AND MAGNETIC PROPERTIES OF MATERIALS DILCTRIC AD MAGTIC PROPRTIS OF MATRIALS Dilctric Proprtis: Dilctric matrial Dilctric constant Polarization of dilctric matrials, Typs of Polarization (Polarizability). quation of intrnal filds in liquid

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

Limiting value of higher Mahler measure

Limiting value of higher Mahler measure Limiting valu of highr Mahlr masur Arunabha Biswas a, Chris Monico a, a Dpartmnt of Mathmatics & Statistics, Txas Tch Univrsity, Lubbock, TX 7949, USA Abstract W considr th k-highr Mahlr masur m k P )

More information

Impedance Transformation and Parameter Relations

Impedance Transformation and Parameter Relations 8/1/18 Cours nstructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 4 mpdanc Transformation and Paramtr Rlations mpdanc Ths Transformation

More information

Effect of sampling on frequency domain analysis

Effect of sampling on frequency domain analysis LIGO-T666--R Ec sampling n rquncy dmain analysis David P. Nrwd W rviw h wll-knwn cs digial sampling n h rquncy dmain analysis an analg signal, wih mphasis n h cs upn ur masurmns. This discussin llws h

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

ME 354, MECHANICS OF MATERIALS LABORATORY COMPRESSION AND BUCKLING

ME 354, MECHANICS OF MATERIALS LABORATORY COMPRESSION AND BUCKLING ME 354, MECHANICS OF MATERIALS LABATY COMPRESSION AND BUCKLING 01 January 000 / mgj PURPOSE Th purps f this xrcis is t study th ffcts f nd cnditins, clumn lngth, and matrial prprtis n cmprssiv bhaviur

More information

Slide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS

Slide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS Slid DIGITAL SIGAL PROCESSIG UIT I DISCRETE TIME SIGALS AD SYSTEM Slid Rviw of discrt-tim signals & systms Signal:- A signal is dfind as any physical quantity that varis with tim, spac or any othr indpndnt

More information

Chapter 6 Folding. Folding

Chapter 6 Folding. Folding Chaptr 6 Folding Wintr 1 Mokhtar Abolaz Folding Th folding transformation is usd to systmatically dtrmin th control circuits in DSP architctur whr multipl algorithm oprations ar tim-multiplxd to a singl

More information

INTEGRATION BY PARTS

INTEGRATION BY PARTS Mathmatics Rvision Guids Intgration by Parts Pag of 7 MK HOME TUITION Mathmatics Rvision Guids Lvl: AS / A Lvl AQA : C Edcl: C OCR: C OCR MEI: C INTEGRATION BY PARTS Vrsion : Dat: --5 Eampls - 6 ar copyrightd

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

Least Favorable Distributions to Facilitate the Design of Detection Systems with Sensors at Deterministic Locations

Least Favorable Distributions to Facilitate the Design of Detection Systems with Sensors at Deterministic Locations Last Favorabl Distributions to Facilitat th Dsign o Dtction Systms with Snsors at Dtrministic Locations Bndito J. B. Fonsca Jr. Sptmbr 204 2 Motivation Rgion o intrst (city, park, stadium 3 Motivation

More information

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in Surfac plasmon rsonanc is snsitiv mchanism for obsrving slight changs nar th surfac of a dilctric-mtal intrfac. It is commonl usd toda for discovring th was in which protins intract with thir nvironmnt,

More information

Voltage, Current, Power, Series Resistance, Parallel Resistance, and Diodes

Voltage, Current, Power, Series Resistance, Parallel Resistance, and Diodes Lctur 1. oltag, Currnt, Powr, Sris sistanc, Paralll sistanc, and Diods Whn you start to dal with lctronics thr ar thr main concpts to start with: Nam Symbol Unit oltag volt Currnt ampr Powr W watt oltag

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

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let It is impossibl to dsign an IIR transfr function with an xact linar-phas It is always possibl to dsign an FIR transfr function with an xact linar-phas rspons W now dvlop th forms of th linarphas FIR transfr

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 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

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):.

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):. Division of Mchanics Lund Univrsity MULTIBODY DYNMICS Examination 7033 Nam (writ in block lttrs):. Id.-numbr: Writtn xamination with fiv tasks. Plas chck that all tasks ar includd. clan copy of th solutions

More information

1 Isoparametric Concept

1 Isoparametric Concept UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric

More information

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction Int. J. Opn Problms Compt. Math., Vol., o., Jun 008 A Pry-Prdator Modl with an Altrnativ Food for th Prdator, Harvsting of Both th Spcis and with A Gstation Priod for Intraction K. L. arayan and. CH. P.

More information

ECE 407 Computer Aided Design for Electronic Systems. Instructor: Maria K. Michael. Overview. CAD tools for multi-level logic synthesis:

ECE 407 Computer Aided Design for Electronic Systems. Instructor: Maria K. Michael. Overview. CAD tools for multi-level logic synthesis: 407 Computr Aidd Dsign for Elctronic Systms Multi-lvl Logic Synthsis Instructor: Maria K. Michal 1 Ovrviw Major Synthsis Phass Logic Synthsis: 2-lvl Multi-lvl FSM CAD tools for multi-lvl logic synthsis:

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

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the Copyright itutcom 005 Fr download & print from wwwitutcom Do not rproduc by othr mans Functions and graphs Powr functions Th graph of n y, for n Q (st of rational numbrs) y is a straight lin through th

More information

The Open Economy in the Short Run

The Open Economy in the Short Run Economics 442 Mnzi D. Chinn Spring 208 Social Scincs 748 Univrsity of Wisconsin-Madison Th Opn Economy in th Short Run This st of nots outlins th IS-LM modl of th opn conomy. First, it covrs an accounting

More information

Why is a E&M nature of light not sufficient to explain experiments?

Why is a E&M nature of light not sufficient to explain experiments? 1 Th wird world of photons Why is a E&M natur of light not sufficint to xplain xprimnts? Do photons xist? Som quantum proprtis of photons 2 Black body radiation Stfan s law: Enrgy/ ara/ tim = Win s displacmnt

More information

NARAYANA I I T / P M T A C A D E M Y. C o m m o n P r a c t i c e T e s t 1 6 XII STD BATCHES [CF] Date: PHYSIS HEMISTRY MTHEMTIS

NARAYANA I I T / P M T A C A D E M Y. C o m m o n P r a c t i c e T e s t 1 6 XII STD BATCHES [CF] Date: PHYSIS HEMISTRY MTHEMTIS . (D). (A). (D). (D) 5. (B) 6. (A) 7. (A) 8. (A) 9. (B). (A). (D). (B). (B). (C) 5. (D) NARAYANA I I T / P M T A C A D E M Y C o m m o n P r a c t i c T s t 6 XII STD BATCHES [CF] Dat: 8.8.6 ANSWER PHYSIS

More 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

6. Negative Feedback in Single- Transistor Circuits

6. Negative Feedback in Single- Transistor Circuits Lctur 8: Intrductin t lctrnic analg circuit 36--366 6. Ngativ Fdback in Singl- Tranitr ircuit ugn Paprn, 2008 Our aim i t tudy t ffct f ngativ fdback n t mall-ignal gain and t mall-ignal input and utput

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

Exercise 1. Sketch the graph of the following function. (x 2

Exercise 1. Sketch the graph of the following function. (x 2 Writtn tst: Fbruary 9th, 06 Exrcis. Sktch th graph of th following function fx = x + x, spcifying: domain, possibl asymptots, monotonicity, continuity, local and global maxima or minima, and non-drivability

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

GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES. Eduard N. Klenov* Rostov-on-Don, Russia

GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES. Eduard N. Klenov* Rostov-on-Don, Russia GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES Eduard N. Klnov* Rostov-on-Don, Russia Th articl considrs phnomnal gomtry figurs bing th carrirs of valu spctra for th pairs of th rmaining additiv

More information

Electrical Energy and Capacitance

Electrical Energy and Capacitance haptr 6 Elctrical Enrgy and apacitanc Quick Quizzs. (b). Th fild xrts a forc on th lctron, causing it to acclrat in th dirction opposit to that of th fild. In this procss, lctrical potntial nrgy is convrtd

More information

Chapter 6: Polarization and Crystal Optics

Chapter 6: Polarization and Crystal Optics Chaptr 6: Polarization and Crystal Optics * P6-1. Cascadd Wav Rtardrs. Show that two cascadd quartr-wav rtardrs with paralll fast axs ar quivalnt to a half-wav rtardr. What is th rsult if th fast axs ar

More information

Analysis and Design of Basic Interconnects (Part 1)

Analysis and Design of Basic Interconnects (Part 1) Analysis and Dsign f Basic Intcnncts (Pat ) Outlin Tw-wi lins and caxial lins Stiplin Stiplin gmty and fild distibutin Chaactizing stiplins Micstip lin Micstip gmty and fild distibutin Chaactizing micstip

More information

Lecture 2a. Crystal Growth (cont d) ECE723

Lecture 2a. Crystal Growth (cont d) ECE723 Lctur 2a rystal Grwth (cnt d) 1 Distributin f Dpants As a crystal is pulld frm th mlt, th dping cncntratin incrpratd int th crystal (slid) is usually diffrnt frm th dping cncntratin f th mlt (liquid) at

More information