Version 2.1 NE05 - LRC Series Circuit

Size: px
Start display at page:

Download "Version 2.1 NE05 - LRC Series Circuit"

Transcription

1 ersn. NE05 - Seres rcu Expermen NE05 Inucr -essr-apacr () Seres rcu abrary Manual Deparmen Physcs he Unversy Hng Kng Ams emnsrae varus prperes an seres crcu such as:. Phase erence beween penal erence acrss he crcu elemens an curren he crcu.. esnan requency a seres crcu. 3. Impeance he crcu uner eren alernang crcu (A..) requences. Sel-learnng maeral: hery - Backgrun Inrman Summary: rcu S S S S Impenence, Z Phase erence wh Phasr agram 0 leas by 90 lags n by 90 leas lags n by 90 an by 90 S eerence Phasr Denn: A.. (a) a.c. an.c. In a rec curren (.c.) he r velcy s n ne recn nly. mmn surce.c. s a baery. In an alernang curren (a.c.), he recn he r velcy reverses, usually many mes a secn. A.c. s cmmnly generae by an a.c. generar. he eec a.c. are essenally he same as hse.c. Bh are sasacry r heang an lghng purpses. ac c.. Fgure :.Snusal a.c. Fgure :.cnsan.c. Page

2 ersn. (b) erms. Per, requency an angular requency O sn P - O P NE05 - Seres rcu Fgure 3: sne uncn me graph An alernang curren r e.m.. vares percally wh me n magnue an recn. he smples a.c. uncn s a sne uncn an s shwn n Fgure 3. he general equan a sne uncn s shwn belw. y Amplue Asn Inal Angular phase requency me One cmplee alernan s calle a cycle an he number cycles ccurrng n ne secn s erme he requency ( ) he alernang quany. he SI un requency s he herz (Hz) an was prevusly he cycle per secn. he requency he elecrcy supply n Hng Kng s 50Hz whch means ha he uran ne cycle, knwn as he per ( ), s /50 = 0.0s. In general. elanshps beween per, requency an angular requency: () r () (3). Smples rm a.c. he smples an ms mpran alernang e.m.. can be represene by a sne curve an s sa have a snusal waverm. I can be expresse by he equan: sn 0 (4) where s he e.m.. a me, 0 s he peak r maxmum e.m.. an s a cnsan whch equals where s he requency he e.m.. Smlarly, r a snusal alernang curren we may wre sn 0 (5) 3. 4 mpran values A.. a. Insananeus value, s ene as he e.m.., penal erence, curren an pwer a.c. a ceran me. Is mahemacal expressn a me r penal erence: sn ; r urren: sn. Page

3 ersn. a. Peak value, NE05 - Seres rcu s ene as maxmum r mnmum nsananeus value a.c. Is mahemacal expressn r penal erence an curren are a. Average value/ Mean value, P an Q sn s ene as he mean value a ceran perc quany P s represene by he nan P.I s mahemacal expressn s P 0 P ) -mean-square value (r.m.s. value) a. Denn: he -mean-square (r.m.s.) value an alernang curren (als calle he eecve value) s he seay rec curren whch cnvers elecrcal energy her rms energy n a gven ressance a he same rae as a.c. Alhugh he nsananeus value (curren r e.m..) s varyng,. he average rae a whch supples elecrcal energy he lamp equals he seay rae supply by he.c. ( hs aspec whch s en mpran. b. Pr: In general, cnserng he energy supple a ressr wh ressance, c.. ) an n pracce s.c. P ac.. P c.. Fgure 4: Schemac agrams r a.c. an.c. wh same average pwer upu I he average pwer upu crcus n Fgure 4 s equal,.e. P P c... c. a. c... mean value (6) c.. mean value c (7) square r he mean value he square he curren (8). c. r. m. s. I he a.c. s snusal (.e. he surce s a sne uncn) hen... mean value sn (0) r m s () r. m. s. mean value sn r. m. s. () sn 0 (9) Usually, he symbl mean value r average value a quany x s nae by x r x Usually, he symbl r-mean-square a quany x s nae by x r x Page 3

4 ersn. Graphcally, he area Pac.. curve s equal ha Pc.. NE05 - Seres rcu curve as shwn n Fgure 5. P ac P c P peak P Fgure 5: Pwer generae vs. me graphs r a.c. an.c. surces c. Why mean-square-value sne uncn, 0 cs / ( ) ( ) cs ( ) ecr agram r Phasr agram P y sn P ' Meh : Meh : / 0 sn 0 sn sn / sn ( ) 0? Q sn cs Q sn cs sn cs sn cs sn sn Y O O ' y Y sn Y Fgure 6: ang vecr an alernang quany A snusal alernang quany can be represene by a rang vecr (en calle a Phasr) as shwn n Fgure 6. I s calle a Phasr agram. An alernang quany y Y sn where Y s he peak value he quany an s requency. I he lne OP has lengh Y (.e. raus an magnary crcle) an raes n an anclckwse recn abu O OP; ' ' OP n Oy ' a me (measure rm he me when OP passes hrugh wh unrm angular velcy, he prjecn OO ' ) s I OP s rece as shwn Fgure 6 by he arrw n, hen we can say ha he prjecn n Y sn. Oy ' he Page 4

5 ersn. rang vecr OP gves he value a any nsan he snusal quany beng snusal, can be erve smlarly rm unrm mn n a crcle.) y Y sn y Y sn Y Y y y NE05 - Seres rcu. (Smple harmnc mn, y esulan phasr y y Fgure 7: Phase erence beween w alernang quanes he Phasr agram s very useul r represenng w snusal quanes whch have he same requency r same angular requency bu are n n phase (.e. quanes y an y erence beween hem s, wh 0 ) he wave rms w such an he crrespnng vecr agram are shwn n Fgure 7 r me. he phase y laggng, an hs phase angle s manane beween hem as he vecrs rae. Beng vecrs hey can be ae by he parallelgram law hey represen smlar quanes, e.g. p.s. r currens Algebracally an are expresse by he equans: y Y sn an y Y sn y y essr: (a) essance n a.c. crcu he ressance, ene by, measures he ably a ressr ppse he passage curren hrugh. he rmula r he ressance a cnucr s l A (3) where s he elecrcal ressvy he maeral, l s he lengh, an A s crss-secn area he cnucr. Fr hmc maeral, he curren passng hrugh s recly prprnal penal erence acrss ha maeral..e. Obeys Ohm s law., where s a cnsan. (b) Pure ressve crcu he curren I hrugh a ressr 3 s n phase wh he vlage apple. S Fgure 8: Schemac agram pure ressance crcu 3 Symbl ressr cul be IE-syle ( ) r Amercan-syle ( ). Page 5

6 ersn. eerrng he Fgure 8, he a.c. surce s a snusal vlage..e. e apple penal erence acrss ressr, (4) Where sn s he peak value penal erence acrss he ressr. S NE05 - Seres rcu Accrng Ohm s law, he curren s als a snusal uncn. an n phase wh vlage apple sn (5) e Where Hence an (6) s he peak value curren passng hrugh he ressr. As a resul, are n phase, als sn (7) I, r. m. s (8) r. m. s. ke he case n.c., he peak curren an penal erence acrss. passng hrugh a ressr epens n bh he ressance apacance n a.c. crcus (a) Denn A smple capacr 4 cnsss w parallel recangular cnucng plaes separae by a elecrc (.e. ar, plymers, quarz an glass ec), where a elecrc s a kn nsular whch can be plarze by applyng an elecrc el. When a capacr s cmpleely charge by a baery (.e..c. surce), cnans equal bu ppse charges n he w plaes,.e. ne plae gans elecrns an he her lses he same amun elecrns hrugh he crcu. I he charge sre by a ceran capacr s Q, acually means ha ne plae sres charge Q, an he her plae sres charge Q. Please ne ha here s n curren pass hrugh he capacr by usng.c. surce. Bu here s a vrual curren passng hrugh he capacr by usng a.c. surce. he capacance, ene by, s ene as he charge sre per un vlage apple he capacr. In mahemacal rm, we have Q (9) where Q s he charge sre an s he penal erence acrss he plaes. In SI uns, - capacance s measure n aras ( F ) r J. apacance s a measure he capacy sre charge an hereby elecrcal energy 5. he capacance s an nrnsc prpery ha cul be calculae by knwng he mensn an maeral use. 4 Symbl capacr cul be ( ). Page 6

7 ersn. NE05 - Seres rcu Fr parallel plaes nly, he penal erence an elecrc el acrss he capacr wh separan an surace area A surace are: ur E (0) ur Q Q ur Q E E 4 r 4 r A surace By elmnang E ur n he abve equans, r a parallel-plae capacr, he capacance s () A where s he permvy he elecrc maeral separang he w plaes, beween he plaes, an A s he verlappng area w plaes. (b) Flw a.c. hrugh a capacr ma, r. m. s. ma () s he separan 000F.5 0.3A Fgure 9: Phase erence beween 000F an.5 0.3A As shwn n Fgure 9, a 000F capacr s cnnece n seres wh a.5, 0.3 A lamp, an a.c. supply, he lamp as expece, es n lgh. Is here any curren lw? Wh a r.m.s. 50 Hz supply, s nearly ully l. he a.c. s apparenly lwng hrugh he capacr. In ac, he capacr s beng charge, scharge, charge n he ppse recn an scharge agan, y mes per secn (he requency he a.c.), an he chargng an schargng currens lwng hrugh he lamp lgh. N curren acually passes hrugh he capacr (snce s plaes are separae by an nsular(.e. elecrc maeral) bu appears s an we alk as. A curren wul ceranly be recre by an a.c. mllammeer. (c) Phase relanshps When a.c. lws hrugh an eal ressr (havng n capacance r nucance) he curren an penal erence reach her peak values a he same nsan,.e. hey are n phase. hs s n s r a capacr. Fr a capacr, he curren hrugh s seen lea he penal erence acrss by nequarer a cycle,.e. he curren reaches s maxmum value ne-quarer a cycle bere he penal erence reaches s peak value. Page 7

8 ersn. NE05 - Seres rcu, sn O A cs Fgure 0: Phase erence beween an nserng a pure capacance crcu as shwn n Fgure, curren an apple penal erence are u sep because curren lw s a maxmum mmeaely an uncharge capacr s cnnece an a.c. supply. here s as ye n charge n he capacr ppse he arrval charge. hus a O he apple penal erence, hugh mmenarly zer, s ncreasng a s maxmum rae (he slpe he angen a O he penal erence graph s a maxmum) an s he rae lw charge he curren, s als a maxmum. Beween O an A he penal erence n he capacr s ncreasng Q less. A A Q he apple penal erence s ncreasng bu a a ecreasng rae, he charge bu less quckly, whch means ha he chargng curren s s a maxmum an r a bre mmen s cnsan. he charge n he capacr wll als be a maxmum an cnsan. he rae lw charge s herere zer, Q.e. he curren s zer. he phase erence beween an can hus be explane. () Mahemacal reamen nserng a pure capacance crcu as shwn n Fgure, le a penal erence apple acrss a capacance an le s value a me be gven by where,, sn (3) s s peak value an where s he requency he supply. be S Fgure : Schemac agram pure capacance crcu he charge Q n he capacance a me s Q (4) Fr he curren lwng hrugh he capacr we can wre Page 8

9 ersn. = rae change charge Q (5) NE05 - Seres rcu Q Q (Denn capacance) ( uv) u v v u (6) Q ( ) 0 as capacance s a cnsan an nepenen (7) Q (quen rule) where u an v are uncn Q, sn, sn (8) (sn ) sn Q where an are cnsan an nepenen, sn (9) Q sn cs an, where s a cnsan an nepenen, cs (30), cs (3) Mahemacally, snce cs sn Equan (3) becmes,, cs, sn By cmparng, sn wh, sn, he curren hrugh capacr (a csne uncn) hus leas he apple penal erence (a sne uncn) by ne quarer a cycle r, as s en sae, by raans 6 r 90 ( cycle beng regare as raans r 360 ) as shwn n (3) Fgure 0. e, (33) cs (34) Accrng equan (33), 6 Whu speccally menne, all angle shul be n erms raans raher han egree. Page 9

10 ersn. (35) NE05 - Seres rcu he ra r.m.s. penal erence ha curren equal he ra peak value penal erence ha curren. r. m. s., (36) r. m. s. By subsung equan (35) n equan (36) an r. m. s. (37) r. m. s. hs expressn resembles whch enes ressance, replacng. he quany s aken as a measure he ppsn a capacr a.c. an s calle capacve reacance r. m. s.. Hence, (38) he hm s he SI un r. m. s. he un s - s (herz) an ha s he erm - hen has uns A. I s clear ha ecreases as an ncrease. s eacance s n be cnuse wh ressance; n he laer elecrcal pwer s sspae, whereas s n n a reacance. Inucr (a) Denn An nucr 7 s a evce srng energy n magnec el, r example cls r slens (.e. a seres cls). he nucance, ene by, s he ably ha an nucr sre energy n a magnec el. In parcular, he erm sel-nucance s use escrbe he behavr generang an ppsng elecrmve rce (r calle back e.m..) prprnal he rae change n curren n a crcu. I s Faraay s aw 8,.e. back (39) r back (40) 7 Symbl an nucr/ a slen cul be wh errmagnec maerals ( ) r whu errmagnec maerals ( ). N B N 8 back NA NA where BA l, N B, N s he number urns l n cls n he slen, s he lengh he slen, A s he crss-secnal area slen an s he curren passng hrugh he slen N A N A back an cmparng back l l l Page 0

11 ersn. Fr an nnely lng slen, he nucance s N A (4) l NE05 - Seres rcu, where s he permeably he maeral nse he slen, N s he number urns cls n he slen, A s he crss-secn area he cl, l s he lengh he cl. he SI un nucance s n henrys. (e) Phase relanshps An nucr n an a.c. crcu as shwn n Fgure 3 behaves lke a capacr n ha causes a phase erence beween he apple penal erence an he curren. In hs case, hwever, he curren lags n he penal erence by ne-quarer a cycle (.e. 90 ) as shwn n Fgure., cs sn O A back back back, cs Fgure : Phase erence beween an In Fgure, a O, he curren s zer bu s rae ncrease s a maxmum (as gven by he slpe he angen he curren graph a O r max ) whch means, r an nucr cnsan nucance, ha he rae change lux s als a maxmum ( B A max )9. herere by Faraay s law he back e.m.. (r calle nuce e.m..)s a maxmum ( max ) bu, by enz s law, negave sgn snce acs ppse he curren change. A A he curren an lux are mmenarly a maxmum an cnsan. her rae change s zer (slpe angen curren graph s zer a A r 0 an B A max ) an s he back e.m.. s zer ( nuce 0 ). I he nucr has neglgble ressance, hen a every nsan he apple penal erence mus be nearly equal an ppse he back e.m.. (.e. nuce ). he penal erence acs n he cl whls he e.m.. acs back upn he surce, jus lke w rces acng n eren bes. nuce 9 Fr a lng slen, N B B l Page

12 ersn. () Mahemacal reamen S NE05 - Seres rcu Fgure 3: Schemac agram pure nucance crcu In hs case, s smpler sar wh a pure nucance curren as shwn n Fgure 3. nser an nucr wh nucance hrugh whch curren lws a me where where, sn (4) s s peak value an where s he requency he supply. he back e.m.. (r calle nuce e.m..) n he nucr ue changng curren s back (43) Subsung equan (4) n equan (43) back sn (44) s a cnsan an nepenen back sn (45) sn Q sn cs an where s a cnsan an Q nepenen where s a cnsan an nepenen cs (46) Assumng he nucr has zer ressance, hen r curren lw he apple penal erence mus be equal an ppse he back e.m.., hence (47) Subsung equan (46) n equan (47) cs (48) he apple penal erence s gven by, cs (49) back back where where s he requency he supply an, s s peak value. Accrng equan (48) s gven by, (50) he ra r.m.s. penal erence ha curren equal he ra peak value penal erence ha curren. r. m. s.,.e. Q (5) r. m. s. Subsung equan (50) n equan (5) an Page

13 ersn.. Hence, hs expressn resembles r. m. s., (5) r. m. s. whch enes ressance, NE05 - Seres rcu replacng. he quany s aken as a measure he ppsn an nucr a.c. an s calle nucve reacance r. m. s. (53) r. m. s. Phasr agrams r pure ressance, pure capacance an pure nucance crcu he vecr agram r a pure ressance n an a.c. crcu. he curren s n phase wh apple penal erence (.e. phase erence = 0 r 360 ) as shwn n Fgure 4. he vecr agram r a pure capacance (.e.. nne elecrc ressance) n an a.c. crcu. he curren leas he apple penal erence by 90.(.e. phase erence = 90 ) as shwn n Fgure 5. Fr a pure nucance (.e. zer ressance), n hs case he curren erence by 90.(.e. phase erence = 90 ) as shwn n Fgure 6. Fgure 4: Phasr agram an seres A.. crcu Fgure 5: Phasr agram an Suppse an alernang penal erence lags n he apple penal Fgure 6: Phasr agram an s apple acrss a ressance an a capacance n seres as shwn n Fgure 7. Because n seres arrangemen. he same curren lws hrugh each cmpnen an s he reerence vecr wll be ha represenng. he penal erence acrss s n phase wh shwn n Fgure 8., an, ha acrss, lags n by 90 (r S raans) he vecr agram s as eerence Phasr Fgure 7: Schemac seres crcu. Fgure 8: Phasr agram seres crcu he vecr sum an equals he apple penal erence S hence S Page 3

14 ersn. Bu an he quany where (54) S s he capacve reacance S (55) (56) S s calle he mpeance Z NE05 - Seres rcu an equals, hence he crcu an measures s ppsn a.c. I has ressve an reacve cmpnens an lke bh s measure n hms. Hence (57) S Z Als, rm he vecr agram we see ha he curren leas by S a phase angle whch s less han 90 (r less han raans) an s gven by an (58) seres A.. crcu he analyss n Fgure 9 s smlar as seres A.. crcu bu n hs case he penal erence leas n he curren an he penal erence acrss s agan n phase wh. As acrss bere he apple penal erence S S equals he vecr sum (59) S an, an s S eerence Phasr Fgure 9: Schemac seres crcu. Fgure 0: Phasr agram seres crcu Bu an where s he reacance an equals, hence Hence he mpeance Z S (60) S (6) s gven by S Z (6) Als, rm he vecr agram we see ha he curren lags n S by a phase angle whch s less han 90 (r less han raans) an s gven by an (63) Page 4

15 ersn. NE05 - Seres rcu seres a.c. crcu A crcu as shwn n Fgure cnsss an nucr, a ressr an a capacr s calle an crcu. I can be cnnece n seres r n parallel. In hs expermen, nly he seres crcu s cuse. In any seres crcu, all crcu elemens share he same curren a any pn n he crcu..e. ( ) ( ) ( ) ( ) (64) S he crcu rms a smple harmnc scllar r curren an resnance ccurs uner specc cnns. S S eerence Phasr Fgure : Schemac seres crcu. Fgure : Phasr agram seres crcu Accrng he analyss n, seres crcus, leas he curren (reerence) vecr by 90, lags n by 90, an.e. n anphase r u phase. s n phase wh. I s greaer han,r n her wrs,. he vecr sum recn Bu he reacance an s greaer han are herere 80 (hal a cycle) u phase,, her resul s n he an equals he apple penal erence S, herere (65) S, an where an equals, hence Hence he al mpeance S S s he reacance (66) (67) Z al s gven by S Zal (68) r Zal (69) an equals an s Page 5

16 ersn. Als, rm he vecr agram we see ha he curren lags n less han 90 (r less han Elecrcal resnance Seres resnance Impenence ) raans an s gven by an (70) Z al an S (7) NE05 - Seres rcu by a phase angle whch s urren n a crcu resnance rcu seres resnance cnns: 0 Frequency he a.c. surce Fgure 3: Fgures mpenence vs. requency an curren resnance Zal he equan (68) jus erve r he al mpeance Z al n a seres crcu shws ha Z vares wh he requency he apple penal erence snce an bh epen n.he relanshps are shwn n upper panel Fgure 3. an ncreases wh, ( Q ) an ecreases wh ( Q ), s assume be nepenen (bu can vary). A a ceran requency, calle he resnan requency when an Z al has s mnmum value, beng equal ( Q Zal ). he crcu behaves as pure Page 6

17 ersn. NE05 - Seres rcu ressance snce he capacve reacance an nucve reacance cancel each her an he curren has a maxmum value (gven by ). he phase angle (gven by an ) s zer, he apple penal erence an he curren are n phase an here s as sa be resnance. S Accrng equan (68), s bane rm Zal (7), ha s By subsung equans (38) an (53) n equan (7), (73) r 4 (74) I s n henrys an A resnan requency he a.c. surce s maxmum. n aras, (75) wll be n herz., he physcal sgncan s ha he energy ranser crcu rm Page 7

18 ersn. NE05 - Seres rcu Expermen : Fnng he resnan requency hrugh curves ng Seup Prceures. Se up he PASO 750 Inerace an he cmpuer an sar DaaSu.. nnec banana plug pach crs n he OUPU prs n he PASO 750 Inerace. Fgure 4. nnecng pwer surce he Inerace he rcu bar as seres crcu 3. nnec he lage Sensrs n he nerace. Fgure 5. lage Sensr n hannel A r measurng p.. acrss ressr, Fgure 6. lage Sensr n hannel B r measurng p.. acrss nucr Fgure 7. lage Sensr n hannel r measurng p.. acrss capacr, 4. Ensure he crcu s cnnece he 00 ressr, 00 F capacr, 8. mh nucr n seres an 3 vlage sensrs wh each elecrnc cmpnens Page 8

19 ersn. Expermenal Prceure NE05 - Seres rcu Fgure 8. nguran he Fgure 9. Panel sgnal generar crcu. Open he DaaSu wrkng le NE05_EP_UID.s. lck Save Acvy As uncn creae yur grup le where UID shul be yur/yur parner Unversy n.(e.g. NE05_EP_ s). lck he plus sgn nex Measuremens An Sample ae n he Sgnal Generar as shwn n Fgure 9. Ajus he Sample ae 0000 Hz. he Sgnal Generar s se Au s wll sar an sp aumacally when yu sar an sp measurng aa. 3. Se he Amplue an requency 0 Hz he Sgnal Generar an press ener respecvely 4. lck Sar sar measuremen. 5. Wach he Graphs penal erence acrss nucr, ressr an capacr me respecvely. All curves are shul be a sne uncn. 6. Wa r runnng abu 5 secns. 7. lck Sp sp measuremen. 8. Hghlgh he prn he waverm sarng rm 0 secn, a leas w cmplee cycles. 9. lck he F l an all curves as sne uncn 0. By clckng Save Acvy as, save he le as EP_UID_Hz.s whch means exsng applyng requency. versus Fgure 30 Save Acvy As Fgure 3 Save Acvy As Page 9

20 ersn.. ecr he Amplue an Phase sne ng curve vlage acrss capacr nucr versus me respecvely n he able. he wrkshee. lck Delee All Daa uns elee all he aa pns. NE05 - Seres rcu, ressr an Fgure 3 Delee A Daa uns 3. epea sep (4) sep () wh changng he requency n sep () an he le name n sep (9) accrngly. he measuremen requences are lse n he rs clumn able. n he wrkshee. Expermen : Daa Analyss expermen Expermenal Prceure. Open he DaaSu wrkng le NE05_EP_UID.s. lck Save Acvy As uncn creae yur grup le where UID shul be yur/yur parner Unversy n.(e.g. NE05_EP_ s). In DaaSu, w ables are shwn..e. able he penal erence acrss he nucr versus requency an he penal erence acrss he capacr versus requency are shwn. Fgure 33. ables vs. requency an vs. requency Fgure 34. Inser ws by rgh clck n he able 3. Ener he Amplue an wh eren requences recre n he able. wrkshee as he p.. acrss nucr an p.. acrss capacr n he ables shwn n he DaaSu. Page 0

21 ersn. NE05 - Seres rcu 4. Aer enerng he aa, w se aa pns shwn n he graph he DaaSu. F he aa pns p.. acrss nucr by Fng l an chse prprnal ; an he aa pns p.. acrss capacr by Fng l an chse nverse as shwn n gure 35 an 36 respecvely. Fgure 35. Fng cnguran Prprnal Fgure 36. Fng cnguran Inverse F 5. w bes curves are shwn an hey nersec a a pn. Use he Zm Selec see he eal he nersec pn. Use he Smar l rea he x an y crnaes he nersecn pn (.e. (x, y)). 6. By clckng Save Acvy as, save he le as Exp_UID.s. (e.g. Exp_ s) 7. mplee he able. able.3 n wrkshee. Expermen 3: Knwng he prperes he crcu a resnan requency Expermenal Prceure. epea he prceure llusrae n Expermen by usng he resnan requency un n able.3 n wrkshee, cmplee he able 3. n wrkshee. eerences: apacr:. haper 6, Physcs r Scenss an Engneers wh Mern Physcs 8 h En, Jhn Jewe an aymn Serway Inucr:. haper 3, Physcs r Scenss an Engneers wh Mern Physcs 8 h En, Jhn Jewe an aymn Serway Alernang rcu an crcu: 3. haper 33, Physcs r Scenss an Engneers wh Mern Physcs 8 h En, Jhn Jewe an aymn Serway 4. hp://hyperphyscs.phy-asr.gsu.eu/hbase/elecrc/rlcser.hml Inucance a slen: 5. hp://hyperphyscs.phy-asr.gsu.eu/hbase/magnec/ncur.hml#c Page

Experiment NE05 Inductor -Resistor-Capacitor (LRC) Series Circuit Laboratory Manual Department of Physics The University of Hong Kong

Experiment NE05 Inductor -Resistor-Capacitor (LRC) Series Circuit Laboratory Manual Department of Physics The University of Hong Kong Expermen NE05 Inucr -essr-apacr () Seres rcu abrary Manual Deparmen Physcs The Unversy Hng Kng Ams T emnsrae varus prperes an seres crcu such as:. Phase erence beween penal erence acrss he crcu elemens

More information

R th is the Thevenin equivalent at the capacitor terminals.

R th is the Thevenin equivalent at the capacitor terminals. Chaper 7, Slun. Applyng KV Fg. 7.. d 0 C - Takng he derae f each erm, d 0 C d d d r C Inegrang, () ln I 0 - () I 0 e - C C () () r - I 0 e - () V 0 e C C Chaper 7, Slun. h C where h s he Theenn equalen

More information

Energy Storage Devices

Energy Storage Devices Energy Srage Deces Objece f ecure Descrbe The cnsrucn f an nducr Hw energy s sred n an nducr The elecrcal prperes f an nducr Relanshp beween lage, curren, and nducance; pwer; and energy Equalen nducance

More information

10. A.C CIRCUITS. Theoretically current grows to maximum value after infinite time. But practically it grows to maximum after 5τ. Decay of current :

10. A.C CIRCUITS. Theoretically current grows to maximum value after infinite time. But practically it grows to maximum after 5τ. Decay of current : . A. IUITS Synopss : GOWTH OF UNT IN IUIT : d. When swch S s closed a =; = d. A me, curren = e 3. The consan / has dmensons of me and s called he nducve me consan ( τ ) of he crcu. 4. = τ; =.63, n one

More information

2015 Sectional Physics Exam Solution Set

2015 Sectional Physics Exam Solution Set . Crrec answer: D Ne: [quan] denes: uns quan WYSE cadec Challenge 05 Secnal Phscs Ea SOLUTION SET / / / / rce lengh lengh rce enu ass lengh e a) / ass ass b) energ c) wrk lengh e pwer energ e d) (crrec

More information

Physics 20 Lesson 9H Rotational Kinematics

Physics 20 Lesson 9H Rotational Kinematics Phyc 0 Len 9H Ranal Knemac In Len 1 9 we learned abu lnear mn knemac and he relanhp beween dplacemen, velcy, acceleran and me. In h len we wll learn abu ranal knemac. The man derence beween he w ype mn

More information

21.9 Magnetic Materials

21.9 Magnetic Materials 21.9 Magneic Maerials The inrinsic spin and rbial min f elecrns gives rise he magneic prperies f maerials è elecrn spin and rbis ac as iny curren lps. In ferrmagneic maerials grups f 10 16-10 19 neighbring

More information

Chapter 2 Linear Mo on

Chapter 2 Linear Mo on Chper Lner M n .1 Aerge Velcy The erge elcy prcle s dened s The erge elcy depends nly n he nl nd he nl psns he prcle. Ths mens h prcle srs rm pn nd reurn bck he sme pn, s dsplcemen, nd s s erge elcy s

More information

Prerna Tower, Road No 2, Contractors Area, Bistupur, Jamshedpur , Tel (0657) ,

Prerna Tower, Road No 2, Contractors Area, Bistupur, Jamshedpur , Tel (0657) , R Prerna wer, Rad N, Cnracrs Area, Bsupur, Jamshedpur 83, el (657)89, www.prernaclasses.cm JEE MAN 3 PAR A PHYSCS. A unfrm cylnder f lengh and mass M havng crss secnal area A s suspended, wh s lengh vercal,

More information

Chapter 6: AC Circuits

Chapter 6: AC Circuits Chaper 6: AC Crcus Chaper 6: Oulne Phasors and he AC Seady Sae AC Crcus A sable, lnear crcu operang n he seady sae wh snusodal excaon (.e., snusodal seady sae. Complee response forced response naural response.

More information

The Buck Resonant Converter

The Buck Resonant Converter EE646 Pwer Elecrnics Chaper 6 ecure Dr. Sam Abdel-Rahman The Buck Resnan Cnverer Replacg he swich by he resnan-ype swich, ba a quasi-resnan PWM buck cnverer can be shwn ha here are fur mdes f pera under

More information

Notes on Inductance and Circuit Transients Joe Wolfe, Physics UNSW. Circuits with R and C. τ = RC = time constant

Notes on Inductance and Circuit Transients Joe Wolfe, Physics UNSW. Circuits with R and C. τ = RC = time constant Nes n Inducance and cu Tansens Je Wlfe, Physcs UNSW cus wh and - Wha happens when yu clse he swch? (clse swch a 0) - uen flws ff capac, s d Acss capac: Acss ess: c d s d d ln + cns. 0, ln cns. ln ln ln

More information

A Novel High Frequency Isolated Full-Bridge Three-Level AC/AC Converter

A Novel High Frequency Isolated Full-Bridge Three-Level AC/AC Converter Jurnal f Indusral and Inellgen Infrman Vl. 3,., March 05 A vel Hgh Frequency Islaed Full-Brdge hree-level AC/AC Cnverer Zeyu Xang and Le L Cllege f Auman, anjng Unversy f Scence and echnlgy, anjng, Chna

More information

First-order piecewise-linear dynamic circuits

First-order piecewise-linear dynamic circuits Frs-order pecewse-lnear dynamc crcus. Fndng he soluon We wll sudy rs-order dynamc crcus composed o a nonlnear resse one-por, ermnaed eher by a lnear capacor or a lnear nducor (see Fg.. Nonlnear resse one-por

More information

A capacitor consists of two conducting plates, separated by an insulator. Conduction plates: e.g., Aluminum foil Insulator: air, mica, ceramic, etc

A capacitor consists of two conducting plates, separated by an insulator. Conduction plates: e.g., Aluminum foil Insulator: air, mica, ceramic, etc 3//7 haper 6 apacors and Inducors Makng preparaon for dynamc crcus, whch hae far more applcaons han he sac crcus we hae learned so far. 6. apacors Sore energy n elecrc feld nsulaor onducng plaes A capacor

More information

Lesson 2 Transmission Lines Fundamentals

Lesson 2 Transmission Lines Fundamentals Lesson Transmsson Lnes Funamenals 楊尚達 Shang-Da Yang Insue of Phooncs Technologes Deparmen of Elecrcal Engneerng Naonal Tsng Hua Unersy Tawan Sec. -1 Inroucon 1. Why o scuss TX lnes srbue crcus?. Crera

More information

Different kind of oscillation

Different kind of oscillation PhO 98 Theorecal Qeson.Elecrcy Problem (8 pons) Deren knd o oscllaon e s consder he elecrc crc n he gre, or whch mh, mh, nf, nf and kω. The swch K beng closed he crc s copled wh a sorce o alernang crren.

More information

ELEG 205 Fall Lecture #10. Mark Mirotznik, Ph.D. Professor The University of Delaware Tel: (302)

ELEG 205 Fall Lecture #10. Mark Mirotznik, Ph.D. Professor The University of Delaware Tel: (302) EEG 05 Fall 07 ecure #0 Mark Mirznik, Ph.D. Prfessr The Universiy f Delaware Tel: (3083-4 Email: mirzni@ece.udel.edu haper 7: apacirs and Inducrs The apacir Symbl Wha hey really lk like The apacir Wha

More information

2/20/2013. EE 101 Midterm 2 Review

2/20/2013. EE 101 Midterm 2 Review //3 EE Mderm eew //3 Volage-mplfer Model The npu ressance s he equalen ressance see when lookng no he npu ermnals of he amplfer. o s he oupu ressance. I causes he oupu olage o decrease as he load ressance

More information

Experiment 6: STUDY OF A POSITION CONTROL SERVOMECHANISM

Experiment 6: STUDY OF A POSITION CONTROL SERVOMECHANISM Expermen 6: STUDY OF A POSITION CONTROL SERVOMECHANISM 1. Objecves Ths expermen prvdes he suden wh hands-n experence f he peran f a small servmechansm. Ths sysem wll be used fr mre cmplex wrk laer n he

More information

Rheological Models. In this section, a number of one-dimensional linear viscoelastic models are discussed.

Rheological Models. In this section, a number of one-dimensional linear viscoelastic models are discussed. helgcal Mdels In hs secn, a number f ne-dmensnal lnear vscelasc mdels are dscussed..3. Mechancal (rhelgcal) mdels The wrd vscelasc s derved frm he wrds "vscus" + "elasc"; a vscelasc maeral exhbs bh vscus

More information

A New Structure of Buck-Boost Z-Source Converter Based on Z-H Converter

A New Structure of Buck-Boost Z-Source Converter Based on Z-H Converter Jurnal f Operan and Auman n wer Engneerng l. 4, N., ec., ages: 7-3 hp://jape.uma.ac.r A New rucure f Buck-Bs Z-urce nverer Based n Z-H nverer E. Babae*,. Ahmadzadeh Faculy f Elecrcal and mpuer Engneerng,

More information

AP Physics 1 MC Practice Kinematics 1D

AP Physics 1 MC Practice Kinematics 1D AP Physics 1 MC Pracice Kinemaics 1D Quesins 1 3 relae w bjecs ha sar a x = 0 a = 0 and mve in ne dimensin independenly f ne anher. Graphs, f he velciy f each bjec versus ime are shwn belw Objec A Objec

More information

The Components of Vector B. The Components of Vector B. Vector Components. Component Method of Vector Addition. Vector Components

The Components of Vector B. The Components of Vector B. Vector Components. Component Method of Vector Addition. Vector Components Upcming eens in PY05 Due ASAP: PY05 prees n WebCT. Submiing i ges yu pin ward yur 5-pin Lecure grade. Please ake i seriusly, bu wha cuns is wheher r n yu submi i, n wheher yu ge hings righ r wrng. Due

More information

DEEP UNFOLDING FOR MULTICHANNEL SOURCE SEPARATION SUPPLEMENTARY MATERIAL

DEEP UNFOLDING FOR MULTICHANNEL SOURCE SEPARATION SUPPLEMENTARY MATERIAL DEEP UNFOLDING FOR MULTICHANNEL SOURCE SEPARATION SUPPLEMENTARY MATERIAL Sco Wsdom, John Hershey 2, Jonahan Le Roux 2, and Shnj Waanabe 2 Deparmen o Elecrcal Engneerng, Unversy o Washngon, Seale, WA, USA

More information

In the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!") i+1,q - [(!

In the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!) i+1,q - [(! ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL The frs hng o es n wo-way ANOVA: Is here neracon? "No neracon" means: The man effecs model would f. Ths n urn means: In he neracon plo (wh A on he horzonal

More information

Chapters 2 Kinematics. Position, Distance, Displacement

Chapters 2 Kinematics. Position, Distance, Displacement Chapers Knemacs Poson, Dsance, Dsplacemen Mechancs: Knemacs and Dynamcs. Knemacs deals wh moon, bu s no concerned wh he cause o moon. Dynamcs deals wh he relaonshp beween orce and moon. The word dsplacemen

More information

Let s treat the problem of the response of a system to an applied external force. Again,

Let s treat the problem of the response of a system to an applied external force. Again, Page 33 QUANTUM LNEAR RESPONSE FUNCTON Le s rea he problem of he response of a sysem o an appled exernal force. Agan, H() H f () A H + V () Exernal agen acng on nernal varable Hamlonan for equlbrum sysem

More information

Revision: June 12, E Main Suite D Pullman, WA (509) Voice and Fax

Revision: June 12, E Main Suite D Pullman, WA (509) Voice and Fax .: apacors Reson: June, 5 E Man Sue D Pullman, WA 9963 59 334 636 Voce an Fax Oerew We begn our suy of energy sorage elemens wh a scusson of capacors. apacors, lke ressors, are passe wo-ermnal crcu elemens.

More information

Convection and conduction and lumped models

Convection and conduction and lumped models MIT Hea ranfer Dynamc mdel 4.3./SG nvecn and cndcn and lmped mdel. Hea cnvecn If we have a rface wh he emperare and a rrndng fld wh he emperare a where a hgher han we have a hea flw a Φ h [W] () where

More information

Chapter 5. Circuit Theorems

Chapter 5. Circuit Theorems Chaper 5 Crcu Theorems Source Transformaons eplace a olage source and seres ressor by a curren and parallel ressor Fgure 5.-1 (a) A nondeal olage source. (b) A nondeal curren source. (c) Crcu B-conneced

More information

Solution in semi infinite diffusion couples (error function analysis)

Solution in semi infinite diffusion couples (error function analysis) Soluon n sem nfne dffuson couples (error funcon analyss) Le us consder now he sem nfne dffuson couple of wo blocks wh concenraon of and I means ha, n a A- bnary sysem, s bondng beween wo blocks made of

More information

Use 10 m/s 2 for the acceleration due to gravity.

Use 10 m/s 2 for the acceleration due to gravity. ANSWERS Prjecle mn s he ecrl sum w ndependen elces, hrznl cmpnen nd ercl cmpnen. The hrznl cmpnen elcy s cnsn hrughu he mn whle he ercl cmpnen elcy s dencl ree ll. The cul r nsnneus elcy ny pn lng he prblc

More information

P a g e 5 1 of R e p o r t P B 4 / 0 9

P a g e 5 1 of R e p o r t P B 4 / 0 9 P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e

More information

Unit-I (Feedback amplifiers) Features of feedback amplifiers. Presentation by: S.Karthie, Lecturer/ECE SSN College of Engineering

Unit-I (Feedback amplifiers) Features of feedback amplifiers. Presentation by: S.Karthie, Lecturer/ECE SSN College of Engineering Uni-I Feedback ampliiers Feaures eedback ampliiers Presenain by: S.Karhie, Lecurer/ECE SSN Cllege Engineering OBJECTIVES T make he sudens undersand he eec negaive eedback n he llwing ampliier characerisics:

More information

A L A BA M A L A W R E V IE W

A L A BA M A L A W R E V IE W A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N

More information

Kinematics Review Outline

Kinematics Review Outline Kinemaics Review Ouline 1.1.0 Vecrs and Scalars 1.1 One Dimensinal Kinemaics Vecrs have magniude and direcin lacemen; velciy; accelerain sign indicaes direcin + is nrh; eas; up; he righ - is suh; wes;

More information

( ) () we define the interaction representation by the unitary transformation () = ()

( ) () we define the interaction representation by the unitary transformation () = () Hgher Order Perurbaon Theory Mchael Fowler 3/7/6 The neracon Represenaon Recall ha n he frs par of hs course sequence, we dscussed he chrödnger and Hesenberg represenaons of quanum mechancs here n he chrödnger

More information

β A Constant-G m Biasing

β A Constant-G m Biasing p 2002 EE 532 Anal IC Des II Pae 73 Cnsan-G Bas ecall ha us a PTAT cuen efeence (see p f p. 66 he nes) bas a bpla anss pes cnsan anscnucance e epeaue (an als epenen f supply lae an pcess). Hw h we achee

More information

Dr. Kasra Etemadi February 20, 2007

Dr. Kasra Etemadi February 20, 2007 Dr. Kasra Eeadi February, 7 Seady-Sae Sinusidal Analysis Sinusidal Surces: Elecric pwer disribued fr residences and businesses Radi cunicain All signal f pracical ineres are cpsed f sinusidal cpnens Furier

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Lnear Response Theory: The connecon beween QFT and expermens 3.1. Basc conceps and deas Q: ow do we measure he conducvy of a meal? A: we frs nroduce a weak elecrc feld E, and hen measure

More information

Energy Storage Devices

Energy Storage Devices Energy Sorage Deces Objece of Lecure Descrbe he consrucon of a capacor and how charge s sored. Inroduce seeral ypes of capacors Dscuss he elecrcal properes of a capacor The relaonshp beween charge, olage,

More information

Square law expression is non linear between I D and V GS. Need to operate in appropriate region for linear behaviour. W L

Square law expression is non linear between I D and V GS. Need to operate in appropriate region for linear behaviour. W L MOS Feld-Effec Trassrs (MOSFETs ecure # 4 MOSFET as a Amplfer k ( S Square law express s lear bewee ad. Need perae apprprae reg fr lear behaur. Cpyrgh 004 by Oxfrd Uersy Press, c. MOSFET as a Amplfer S

More information

Variants of Pegasos. December 11, 2009

Variants of Pegasos. December 11, 2009 Inroducon Varans of Pegasos SooWoong Ryu bshboy@sanford.edu December, 009 Youngsoo Cho yc344@sanford.edu Developng a new SVM algorhm s ongong research opc. Among many exng SVM algorhms, we wll focus on

More information

Dishonest casino as an HMM

Dishonest casino as an HMM Dshnes casn as an HMM N = 2, ={F,L} M=2, O = {h,} A = F B= [. F L F L 0.95 0.0 0] h 0.5 0. L 0.05 0.90 0.5 0.9 c Deva ubramanan, 2009 63 A generave mdel fr CpG slands There are w hdden saes: CpG and nn-cpg.

More information

5.1 Angles and Their Measure

5.1 Angles and Their Measure 5. Angles and Their Measure Secin 5. Nes Page This secin will cver hw angles are drawn and als arc lengh and rains. We will use (hea) represen an angle s measuremen. In he figure belw i describes hw yu

More information

Physics 107 HOMEWORK ASSIGNMENT #20

Physics 107 HOMEWORK ASSIGNMENT #20 Physcs 107 HOMEWORK ASSIGNMENT #0 Cutnell & Jhnsn, 7 th etn Chapter 6: Prblems 5, 7, 74, 104, 114 *5 Cncept Smulatn 6.4 prves the ptn f explrng the ray agram that apples t ths prblem. The stance between

More information

Diode rectifier with capacitive DC link

Diode rectifier with capacitive DC link . Converers Dode recfer wh capacve DC lnk 4 e lne lne D D 3 C v v [] e e D D 4 4 5 5 Fgure.: A sngle-phase dode recfer wh a capacve DC lnk. [s] Fgure.: ne-o-neural volage and DC sde volage for a sngle-phase

More information

II. Light is a Ray (Geometrical Optics)

II. Light is a Ray (Geometrical Optics) II Lgh s a Ray (Geomercal Opcs) IIB Reflecon and Refracon Hero s Prncple of Leas Dsance Law of Reflecon Hero of Aleandra, who lved n he 2 nd cenury BC, posulaed he followng prncple: Prncple of Leas Dsance:

More information

FI 3103 Quantum Physics

FI 3103 Quantum Physics /9/4 FI 33 Quanum Physcs Aleander A. Iskandar Physcs of Magnesm and Phooncs Research Grou Insu Teknolog Bandung Basc Conces n Quanum Physcs Probably and Eecaon Value Hesenberg Uncerany Prncle Wave Funcon

More information

CAPACITANCE AND INDUCTANCE

CAPACITANCE AND INDUCTANCE APAITANE AND INDUTANE Inroduces wo passve, energy sorng devces: apacors and Inducors LEARNING GOALS APAITORS Sore energy n her elecrc feld (elecrosac energy) Model as crcu elemen INDUTORS Sore energy n

More information

[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5

[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5 TPG460 Reservor Smulaon 08 page of 5 DISCRETIZATIO OF THE FOW EQUATIOS As we already have seen, fne dfference appromaons of he paral dervaves appearng n he flow equaons may be obaned from Taylor seres

More information

i-clicker Question lim Physics 123 Lecture 2 1 Dimensional Motion x 1 x 2 v is not constant in time v = v(t) acceleration lim Review:

i-clicker Question lim Physics 123 Lecture 2 1 Dimensional Motion x 1 x 2 v is not constant in time v = v(t) acceleration lim Review: Reiew: Physics 13 Lecure 1 Dimensinal Min Displacemen: Dx = x - x 1 (If Dx < 0, he displacemen ecr pins he lef.) Aerage elciy: (N he same as aerage speed) a slpe = a x x 1 1 Dx D x 1 x Crrecin: Calculus

More information

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17 EES 16A Designing Informaion Devices and Sysems I Spring 019 Lecure Noes Noe 17 17.1 apaciive ouchscreen In he las noe, we saw ha a capacior consiss of wo pieces on conducive maerial separaed by a nonconducive

More information

Physics 111. Exam #1. September 28, 2018

Physics 111. Exam #1. September 28, 2018 Physics xam # Sepember 8, 08 ame Please read and fllw hese insrucins carefully: Read all prblems carefully befre aemping slve hem. Yur wrk mus be legible, and he rganizain clear. Yu mus shw all wrk, including

More information

Microelectronic Circuits. Feedback. Ching-Yuan Yang

Microelectronic Circuits. Feedback. Ching-Yuan Yang Mcrelecrnc rcu Feedback hng-yuan Yang Nanal hung-hng Unvery Deparmen Elecrcal Engneerng Oulne The General Feedback Srucure Sme Prpere Negave Feedback The Fur Bac Feedback Tplge The Sere-Shun Feedback mpler

More information

LabQuest 24. Capacitors

LabQuest 24. Capacitors Capaciors LabQues 24 The charge q on a capacior s plae is proporional o he poenial difference V across he capacior. We express his wih q V = C where C is a proporionaliy consan known as he capaciance.

More information

Time-interval analysis of β decay. V. Horvat and J. C. Hardy

Time-interval analysis of β decay. V. Horvat and J. C. Hardy Tme-nerval analyss of β decay V. Horva and J. C. Hardy Work on he even analyss of β decay [1] connued and resuled n he developmen of a novel mehod of bea-decay me-nerval analyss ha produces hghly accurae

More information

FTCS Solution to the Heat Equation

FTCS Solution to the Heat Equation FTCS Soluon o he Hea Equaon ME 448/548 Noes Gerald Reckenwald Porland Sae Unversy Deparmen of Mechancal Engneerng gerry@pdxedu ME 448/548: FTCS Soluon o he Hea Equaon Overvew Use he forward fne d erence

More information

Example: MOSFET Amplifier Distortion

Example: MOSFET Amplifier Distortion 4/25/2011 Example MSFET Amplfer Dsoron 1/9 Example: MSFET Amplfer Dsoron Recall hs crcu from a prevous handou: ( ) = I ( ) D D d 15.0 V RD = 5K v ( ) = V v ( ) D o v( ) - K = 2 0.25 ma/v V = 2.0 V 40V.

More information

WiH Wei He

WiH Wei He Sysem Idenfcaon of onlnear Sae-Space Space Baery odels WH We He wehe@calce.umd.edu Advsor: Dr. Chaochao Chen Deparmen of echancal Engneerng Unversy of aryland, College Par 1 Unversy of aryland Bacground

More information

(V 1. (T i. )- FrC p. ))= 0 = FrC p (T 1. (T 1s. )+ UA(T os. (T is

(V 1. (T i. )- FrC p. ))= 0 = FrC p (T 1. (T 1s. )+ UA(T os. (T is . Yu are repnible fr a reacr in which an exhermic liqui-phae reacin ccur. The fee mu be preheae he hrehl acivain emperaure f he caaly, bu he pruc ream mu be cle. T reuce uiliy c, yu are cniering inalling

More information

PHY305F Electronics Laboratory I. Section 2. AC Circuit Basics: Passive and Linear Components and Circuits. Basic Concepts

PHY305F Electronics Laboratory I. Section 2. AC Circuit Basics: Passive and Linear Components and Circuits. Basic Concepts PHY305F Elecrnics abrary I Secin ircui Basics: Passie and inear mpnens and ircuis Basic nceps lernaing curren () circui analysis deals wih (sinusidally) ime-arying curren and lage signals whse ime aerage

More information

CHAPTER 18: Electric Currents. Answers to Questions

CHAPTER 18: Electric Currents. Answers to Questions CHTE : Elecric Currens nswers Quesins. mpere-hurs measures charge. The ampere is a charge per uni ime, an he hur is a ime, s he pruc is charge. mpere-hur f charge is 6 Culmbs f charge.. n he circui (n

More information

2-D Momentum Conservation

2-D Momentum Conservation -D Mmentum Cnseratin Saleback Cllege Physics Department Purpse: T cnirm that linear mmentum is cnsere in tw-imensinal cllisins. T shw that kinetic energy is nearly cnsere in tw-imensinal near-elastic cllisins.

More information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 9 Hamlonan Equaons of Moon (Chaper 8) Wha We Dd Las Tme Consruced Hamlonan formalsm H ( q, p, ) = q p L( q, q, ) H p = q H q = p H = L Equvalen o Lagrangan formalsm Smpler, bu

More information

PHYS 1443 Section 001 Lecture #4

PHYS 1443 Section 001 Lecture #4 PHYS 1443 Secon 001 Lecure #4 Monda, June 5, 006 Moon n Two Dmensons Moon under consan acceleraon Projecle Moon Mamum ranges and heghs Reerence Frames and relae moon Newon s Laws o Moon Force Newon s Law

More information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 9 Hamlonan Equaons of Moon (Chaper 8) Wha We Dd Las Tme Consruced Hamlonan formalsm Hqp (,,) = qp Lqq (,,) H p = q H q = p H L = Equvalen o Lagrangan formalsm Smpler, bu wce as

More information

V.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS

V.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS R&RATA # Vol.) 8, March FURTHER AALYSIS OF COFIDECE ITERVALS FOR LARGE CLIET/SERVER COMPUTER ETWORKS Vyacheslav Abramov School of Mahemacal Scences, Monash Unversy, Buldng 8, Level 4, Clayon Campus, Wellngon

More information

Lecture 18: The Laplace Transform (See Sections and 14.7 in Boas)

Lecture 18: The Laplace Transform (See Sections and 14.7 in Boas) Lecure 8: The Lalace Transform (See Secons 88- and 47 n Boas) Recall ha our bg-cure goal s he analyss of he dfferenal equaon, ax bx cx F, where we emloy varous exansons for he drvng funcon F deendng on

More information

NAME: ANSWER KEY DATE: PERIOD. DIRECTIONS: MULTIPLE CHOICE. Choose the letter of the correct answer.

NAME: ANSWER KEY DATE: PERIOD. DIRECTIONS: MULTIPLE CHOICE. Choose the letter of the correct answer. R A T T L E R S S L U G S NAME: ANSWER KEY DATE: PERIOD PREAP PHYSICS REIEW TWO KINEMATICS / GRAPHING FORM A DIRECTIONS: MULTIPLE CHOICE. Chs h r f h rr answr. Us h fgur bw answr qusns 1 and 2. 0 10 20

More information

10.7 Temperature-dependent Viscoelastic Materials

10.7 Temperature-dependent Viscoelastic Materials Secin.7.7 Temperaure-dependen Viscelasic Maerials Many maerials, fr example plymeric maerials, have a respnse which is srngly emperaure-dependen. Temperaure effecs can be incrpraed in he hery discussed

More information

Midterm Exam. Thursday, April hour, 15 minutes

Midterm Exam. Thursday, April hour, 15 minutes Economcs of Grow, ECO560 San Francsco Sae Unvers Mcael Bar Sprng 04 Mderm Exam Tursda, prl 0 our, 5 mnues ame: Insrucons. Ts s closed boo, closed noes exam.. o calculaors of an nd are allowed. 3. Sow all

More information

Lecture 11 Inductance and Capacitance

Lecture 11 Inductance and Capacitance ecure Inducance and apacance EETRIA ENGINEERING: PRINIPES AND APPIATIONS, Fourh Edon, by Allan R. Hambley, 8 Pearson Educaon, Inc. Goals. Fnd he curren olage for a capacance or nducance gen he olage curren

More information

Introduction to Electronic circuits.

Introduction to Electronic circuits. Intrductn t Electrnc crcuts. Passve and Actve crcut elements. Capactrs, esstrs and Inductrs n AC crcuts. Vltage and current dvders. Vltage and current surces. Amplfers, and ther transfer characterstc.

More information

3 ) = 10(1-3t)e -3t A

3 ) = 10(1-3t)e -3t A haper 6, Sluin. d i ( e 6 e ) 0( - )e - A p i 0(-)e - e - 0( - )e -6 W haper 6, Sluin. w w (40)(80 (40)(0) ) ( ) w w w 0 0 80 60 kw haper 6, Sluin. i d 80 60 40x0 480 ma haper 6, Sluin 4. i (0) 6sin 4-0.7

More information

EG Low Voltage CMOS Fully Differential Current Feedback Amplifier with Controllable 3-dB Bandwidth

EG Low Voltage CMOS Fully Differential Current Feedback Amplifier with Controllable 3-dB Bandwidth EG0800330 Low olage CMS Fully Derenal Curren Feedback Ampler wh Conrollable 3dB Bandwdh Ahmed H. Madan 2, Mahmoud A. Ashour, Solman A. Mahmoud 2, and Ahmed M. Solman 3 adaon Engneerng Dep., NCT, EAEA Caro,

More information

PT380 MULTICHANNEL TIMER SPECIFICATIONS FEATURES PRODUCT CODE MODES OF OPERATION FUNCTIONS TERMINAL CONNECTION

PT380 MULTICHANNEL TIMER SPECIFICATIONS FEATURES PRODUCT CODE MODES OF OPERATION FUNCTIONS TERMINAL CONNECTION PT380 MULTICHANNEL TIMER 96 X 96 Mulichannel: 8 channels Channel perain mde: Parallel r Sequenial Muli range: 99.99 sec 999.9 hr Mdes : N Delay / Inerval / Cyclic N firs / Cyclic FF firs Sar up delay &

More information

Lecture 4 ( ) Some points of vertical motion: Here we assumed t 0 =0 and the y axis to be vertical.

Lecture 4 ( ) Some points of vertical motion: Here we assumed t 0 =0 and the y axis to be vertical. Sme pins f erical min: Here we assumed and he y axis be erical. ( ) y g g y y y y g dwnwards 9.8 m/s g Lecure 4 Accelerain The aerage accelerain is defined by he change f elciy wih ime: a ; In analgy,

More information

Fall 2009 Social Sciences 7418 University of Wisconsin-Madison. Problem Set 2 Answers (4) (6) di = D (10)

Fall 2009 Social Sciences 7418 University of Wisconsin-Madison. Problem Set 2 Answers (4) (6) di = D (10) Publc Affars 974 Menze D. Chnn Fall 2009 Socal Scences 7418 Unversy of Wsconsn-Madson Problem Se 2 Answers Due n lecure on Thursday, November 12. " Box n" your answers o he algebrac quesons. 1. Consder

More information

Displacement, Velocity, and Acceleration. (WHERE and WHEN?)

Displacement, Velocity, and Acceleration. (WHERE and WHEN?) Dsplacemen, Velocy, and Acceleraon (WHERE and WHEN?) Mah resources Append A n your book! Symbols and meanng Algebra Geomery (olumes, ec.) Trgonomery Append A Logarhms Remnder You wll do well n hs class

More information

Scattering at an Interface: Oblique Incidence

Scattering at an Interface: Oblique Incidence Course Insrucor Dr. Raymond C. Rumpf Offce: A 337 Phone: (915) 747 6958 E Mal: rcrumpf@uep.edu EE 4347 Appled Elecromagnecs Topc 3g Scaerng a an Inerface: Oblque Incdence Scaerng These Oblque noes may

More information

V R. Electronics and Microelectronics AE4B34EM. Electronics and Microelectronics AE4B34EM. Voltage. Basic concept. Voltage.

V R. Electronics and Microelectronics AE4B34EM. Electronics and Microelectronics AE4B34EM. Voltage. Basic concept. Voltage. Elecroncs and Mcroelecroncs AEBEM. lecure basc elecronc crcu conceps ressors, capacors, nducors Elecroncs and Mcroelecroncs AEBEM Sudng maerals: server MOODLE hp://moodle.kme.fel.cvu.cz AEBEM Elecroncs

More information

IGEE 401 Power Electronic Systems. Solution to Midterm Examination Fall 2004

IGEE 401 Power Electronic Systems. Solution to Midterm Examination Fall 2004 Jós, G GEE 401 wer Electrnc Systems Slutn t Mdterm Examnatn Fall 2004 Specal nstructns: - Duratn: 75 mnutes. - Materal allwed: a crb sheet (duble sded 8.5 x 11), calculatr. - Attempt all questns. Make

More information

How about the more general "linear" scalar functions of scalars (i.e., a 1st degree polynomial of the following form with a constant term )?

How about the more general linear scalar functions of scalars (i.e., a 1st degree polynomial of the following form with a constant term )? lmcd Lnear ransformaon of a vecor he deas presened here are que general hey go beyond he radonal mar-vecor ype seen n lnear algebra Furhermore, hey do no deal wh bass and are equally vald for any se of

More information

Power Decoupling Method for Isolated DC to Single-phase AC Converter using Matrix Converter

Power Decoupling Method for Isolated DC to Single-phase AC Converter using Matrix Converter Pwer Decuplng Mehd fr Islaed DC Sngle-phase AC Cnverer usng Marx Cnverer Hrk Takahash, Nagsa Takaka, Raul Rber Rdrguez Guerrez and Jun-ch Ih Dep. f Elecrcal Engneerng Nagaka Unversy f Technlgy Nagaka,

More information

2010 Sectional Physics Solution Set

2010 Sectional Physics Solution Set . Crrec nwer: D WYSE CDEMIC CHLLENGE Secnl hyc E 00 Slun Se y 0 y 4.0 / 9.8 /.45 y. Crrec nwer: y 8 0 / 8 /. Crrec nwer: E y y 0 ( 4 / ) ( 4.9 / ) 5.6 y y 4. Crrec nwer: E 5. Crrec nwer: The e rce c n

More information

PRINCE SULTAN UNIVERSITY Department of Mathematical Sciences Final Examination Second Semester (072) STAT 271.

PRINCE SULTAN UNIVERSITY Department of Mathematical Sciences Final Examination Second Semester (072) STAT 271. PRINCE SULTAN UNIVERSITY Deparmen f Mahemaical Sciences Final Examinain Secnd Semeser 007 008 (07) STAT 7 Suden Name Suden Number Secin Number Teacher Name Aendance Number Time allwed is ½ hurs. Wrie dwn

More information

Bandlimited channel. Intersymbol interference (ISI) This non-ideal communication channel is also called dispersive channel

Bandlimited channel. Intersymbol interference (ISI) This non-ideal communication channel is also called dispersive channel Inersymol nererence ISI ISI s a sgnal-dependen orm o nererence ha arses ecause o devaons n he requency response o a channel rom he deal channel. Example: Bandlmed channel Tme Doman Bandlmed channel Frequency

More information

Department of Economics University of Toronto

Department of Economics University of Toronto Deparmen of Economcs Unversy of Torono ECO408F M.A. Economercs Lecure Noes on Heeroskedascy Heeroskedascy o Ths lecure nvolves lookng a modfcaons we need o make o deal wh he regresson model when some of

More information

Influence of Incident Illumination Angle on Capacitance of a Silicon Solar Cell under Frequency Modulation

Influence of Incident Illumination Angle on Capacitance of a Silicon Solar Cell under Frequency Modulation Research Jurnal f Appled Scences Engneerng and Technlgy 5(4): -8 0 ISSN: 040-7459; e-issn: 040-7467 Mawell Scenfc Organzan 0 Sumed: May 06 0 Acceped: June 08 0 Pulshed: Feruary 0 0 Influence f Incden Illumnan

More information

WebAssign HW Due 11:59PM Tuesday Clicker Information

WebAssign HW Due 11:59PM Tuesday Clicker Information WebAssgn HW Due 11:59PM Tuesday Clcker Inormaon Remnder: 90% aemp, 10% correc answer Clcker answers wll be a end o class sldes (onlne). Some days we wll do a lo o quesons, and ew ohers Each day o clcker

More information

University of Bahrain College of Science Dept. of Physics PHYCS 102 FINAL EXAM

University of Bahrain College of Science Dept. of Physics PHYCS 102 FINAL EXAM Unversty o Bahran College o Scence Dept. o Physcs PHYCS 10 FINAL XAM Date: 15/1/001 Tme:Two Hours Name:-------------------------------------------------ID#---------------------- Secton:----------------

More information

TSS = SST + SSE An orthogonal partition of the total SS

TSS = SST + SSE An orthogonal partition of the total SS ANOVA: Topc 4. Orhogonal conrass [ST&D p. 183] H 0 : µ 1 = µ =... = µ H 1 : The mean of a leas one reamen group s dfferen To es hs hypohess, a basc ANOVA allocaes he varaon among reamen means (SST) equally

More information

Chapter 6. Operational Amplifier. inputs can be defined as the average of the sum of the two signals.

Chapter 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 information

Phys1112: DC and RC circuits

Phys1112: DC and RC circuits Name: Group Members: Dae: TA s Name: Phys1112: DC and RC circuis Objecives: 1. To undersand curren and volage characerisics of a DC RC discharging circui. 2. To undersand he effec of he RC ime consan.

More information

CHAPTER II AC POWER CALCULATIONS

CHAPTER II AC POWER CALCULATIONS CHAE AC OWE CACUAON Conens nroducon nsananeous and Aerage ower Effece or M alue Apparen ower Coplex ower Conseraon of AC ower ower Facor and ower Facor Correcon Maxu Aerage ower ransfer Applcaons 3 nroducon

More information

Density Matrix Description of NMR BCMB/CHEM 8190

Density Matrix Description of NMR BCMB/CHEM 8190 Densy Marx Descrpon of NMR BCMBCHEM 89 Operaors n Marx Noaon Alernae approach o second order specra: ask abou x magnezaon nsead of energes and ranson probables. If we say wh one bass se, properes vary

More information

Position, Velocity, and Acceleration

Position, Velocity, and Acceleration rev 06/2017 Posiion, Velociy, and Acceleraion Equipmen Qy Equipmen Par Number 1 Dynamic Track ME-9493 1 Car ME-9454 1 Fan Accessory ME-9491 1 Moion Sensor II CI-6742A 1 Track Barrier Purpose The purpose

More information

AC Circuits AC Circuit with only R AC circuit with only L AC circuit with only C AC circuit with LRC phasors Resonance Transformers

AC Circuits AC Circuit with only R AC circuit with only L AC circuit with only C AC circuit with LRC phasors Resonance Transformers A ircuis A ircui wih only A circui wih only A circui wih only A circui wih phasors esonance Transformers Phys 435: hap 31, Pg 1 A ircuis New Topic Phys : hap. 6, Pg Physics Moivaion as ime we discovered

More information