MHT-CET 5 (PHYSICS) PHYSICS CENTERS : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPUR / BOKARO / DUBAI # 1
|
|
- Ursula Cross
- 5 years ago
- Views:
Transcription
1 1. (D) Givn, mass f th rckts, m = 5000 kg; Exhaust spd, v = 800 m/s Acclratin, a = 0 m/s m Lt is amunt f gas pr scnd, t Frc = m (a + g) mu m a g t m 800 m a g t m kg sc t 800 PHYSICS. (D) Frm th cnsrvatin f linar mmntum, w hav m v m v m m v v 15v v m s. (A) Givn, m r km m 7 10 rad sc Using th rlatin, w hav F mr N. (B) Givn, mass f th by, m = 0 kg, nrgy in n brad = 1 kj = 1 10 J = 1000 J Efficincy f th by = 8%; gravitatinal acclratin = 9.8 m/s Whn th fficincy f by is 8%; thn actual nrgy is cnsumd by th by is givn by J... i Th nrgy cnsumd by th by in climbing h mtr is givn by mgh 09.8 h 9 h... ii Nw aftr quating ths tw valus f nrgis frm quatins (i) and (ii), w gt 9h h 15m 9 CENTES : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPU / BOKAO / DUBAI # 1
2 5. (D) Acclratin du t gravity at a hight g0 gh (Whr g0 is acclratin du t gravity at th surfac f th arth) adius f arth = 600 km Acclratin du t gravity at a hight is givn by h gh g0 1 g0 h Or g 0 1 (Whr h is th hight frm th surfac f arth) Or 1 1 h 600 h 1 Or h km 6. (B) Givn, F Kr 5/ du But F dr du Kr 5/ dr du Kr 5/ dr 5/ du Kr dr / U Kr U r / 7. (D) Angular mmntum, L p mv GM GM m 0 v0 0 0 L m GM 0 8. (B) T As w knwn that, P r And V r T 16Tr Thus PV r r CENTES : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPU / BOKAO / DUBAI #
3 PV r 9. (C) Givn, mass f th bdy, m = 00 gm = 0. kg, hight, h = 00 m, g = 10 m/s Ptntial nrgy f th bdy is givn by UP mgh J 10. (B) Vlcity at th tp = 00 cs 60 = 100 m/s Nw applying th law f cnsrvatin f linar mmntum w find that th particls ging upwards and dwnwards shuld hav qual mmntum. Thus, th initial mmntum f th cmpsit particl is transfrrd t th third particl. m m 100 v Hnc, v = 00 m/s 11. (D) Mmnt f inrtia, 1 I m kg m 1. (D) Givn, initial vlcity u = 0, distanc travlld, s = 10 cm = 1. m, Numbr f scnd, n = 8 Th distanc travlld by th bdy is givn by a sn ut n 1 a a m s a (D) Givn, dpth f lak = 00 m, dcrass in vlum f ball = 0.1% Bulk mdulus is givn by p hg B V V N m 1. (B) Givn, hight f th fall = 500 m, spcific hat f watr, c =. kj/kg, CENTES : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPU / BOKAO / DUBAI #
4 Ptntial nrgy = Hat incrasd in watr mgh mc gh C c (C) Frquncy f clsd rgan pip is half that f pn rgan pip npn ncls Whn pn pip is dippd in watr upt half its lngth, thn it will bhav lik a cls pip f half lngth. Frquncy f pip is invrsly prprtinal t its lngth. npn Nw frquncy, n npn n frquncy rmains sam r f f 16. (C) Givn, frquncy f = 500 Hz, vlcity v = 50 m/s, phas v 50 By th frmula, 0.7m f 500 Als w knw that x mtr 1 cm (D) Frm d-brgli thry th wavlngth Plancks cnstant Mmntum Hnc, if m mmntum is dubld, thn d-brgli will b halvd. 18. (B) Givn, frquncy f wav, n = 100 Hz, Distanc 10 cm 0 cm Frm th frmula, w hav v n cm sc 0 m s 19. (C) Givn, vlcity f surc, v 0 km hr, actual frquncy f sund, 000 Hz, vlcity f sund 10 km hr Frm th Dpplr s ffct, whn th surc is travlling twards th bsrvr, thn apparnt frquncy is givn by v ' v v' CENTES : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPU / BOKAO / DUBAI #
5 Hz 068 Hz 0. (B) Givn, magnitud f th first vctr, A, Magnitud f th scnd vctr, B 5 and angl btwn thm, Th dt prducts f tw vctrs is givn by A.B A Bcs 5cs (B) As w knw, Trqu = frc distanc Hnc, dimnsins f trqu = dimnsins f frc dimnsins f distanc = [MLT ] [L] = [ML T ]. (C) Givn, lngth f th rd, I = 0 cm = 0. m Frquncy, 000 Hz Lngth f th rd, L 0. Or m Hnc, th vlcity f sund in gas is givn by v m s. (A) Givn, critical angl, C = 0 Accrding t law f ttal intrnal rflctin, Vlcity f light in mdium sin C Vlcity f light f air Vlcity f light in mdium sin 0 Vlcity f light f air Thus, vlcity f light in mdium = vlcity f light in air m s. (B) Givn, mass f th plant. M MP (whr is th radius f th arth) 9 Wight f bdy n th arth, w 50 N Accrding th law f gravitatin th wight f th bdy (r frc f gravity) GMm M w CENTES : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPU / BOKAO / DUBAI # 5
6 w M P Hnc, w p M p (Whr w is th wight n th plant) Or p p 50 M w M p p 9 50 w 00 N 9 5. (D) Lt th tmpratur f th mixtur b Hat givn by xygn nc T v Hat rcivd by nitrgn nc T v Thus C But 6. (D) In th systm, whr Q 0 it mans n hat ntrs r lavs in a systm during th prcss. This prcss is calld adiabatic prcss. 7. (B) If cnstant prssur, V T V T V T V T T T T T T T T T U C T T PV 1 T v 8. (B) Accrding t Sttan s law th ttal radiant nrgy CENTES : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPU / BOKAO / DUBAI # 6
7 Q CA T T Q 1 Q T Hnc,... i Q1 T1 Q and T K Frm quatin (i), T / 1/ T 1000 T K 9. (B) Gain in kintic nrgy = wrk But, wrk Fscs q E y cs qey 0. (C) Lt fur capacitanc ar cnnctd in paralll capacitanc f ach capacitr = C 6 C 5 10 farad V 00 vlt Charg n ach capacitr, Q CV culmb 1. (A) Th pwr f hatr is givn by, V 110 P W 10. (A) As w knw, dw 0 p MH sin d cs p 0 cs MH MH 1. (A r C) Hat prducd is rsistanc f wir 0 vltag V 10 V CENTES : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPU / BOKAO / DUBAI # 7
8 V 10 Hat prducd, H t 1 0 Hat rquird fr ic t mlt = ml But 10 1 ml 0 Hnc, 10 1 m m g s. (C) Th intrnal rsistanc ar cnnctd in paralll s th quivalnt rsistanc is 11 1 rq Nw, currnt passing thrugh is E i amp r Pwr is givn by 5. (B) P i W Fr a thin prism, dviatin D Whn th prism is placd in air, thn a D 1 A 0 p I A A 1 A... i Whn th prism is dippd in watr, thn a w 0 Dw q 1 A 1 A a w 9 1 A 1 A 8 A... ii 8 A Dw 1 Thrfr, 8 D A n 6. (A) Accrding t Bhr s thry, vlcity f th lctrn in th innrmst rbit is highst. CENTES : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPU / BOKAO / DUBAI # 8
9 7. (C) Limit f rslutin f tlscp radian d sc 5 0.0scnd 8. (C) As w knw, nrgy f pht lctrns, hc E h E jul V V 8 1 Nw, h mvmax 1 mv max h V 9. (A) adius f a nuclus changs with nucln numbr A f th nuclus as 15 1/ A m 1/ A Hnc, 1/ A 1 1 1/ 8 1/ 1 1 Thrfr, radius f sulphur nuclus is largr than that f hlium by factr f. 0. (A) Givn, 0.95, IE 100 ma Ic 0.95 IE I c I c 95 ma CENTES : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPU / BOKAO / DUBAI # 9
10 1. (C) Currnt acrss 0 rsistr is 0.8 A. Currnt thrugh th paralll rsistanc f A 6 Ttal currnt acrss A Nw ptntial drp acrss rsistr 1..8 V. (D) Whn th pl f a bar magnt is pinting in th nrth dirctin, th magntic lins pass thrugh th magnt and th null pint li n th quatrial-lin f bar magnt.. (D).m.f. f first battry, E1 V.m.f. f scnd battry, E = 8 V Intrnal rsistanc f first battry, r 1 1 Intrnal rsistanc f scnd battry, r Circuit rsistanc, 9 Frm th Kirchhff s currnt law, w hav ir i ir i1 i9 i 8 0 r 1i 1 r i A 1 Nw ptntial diffrnc acrss PQ, 1 VlPQ i 9 V. (A) Mass f th bullt, m = g = 0.0 kg Initial vlcity u = 10 m/s Distanc travlld by th bullt, s = 1 cm = 0.1 m latin fr th final vlcity is givn by v u as v u as Or 0 10 a Or a 0. Hnc, rsistanc xrtd by th blck, F ma N m s (minus sign rprsnts rtardatin f bullt) 5. (C) Magntic mmnt f bar magnt, M 0 A m Magntic fild intnsity, H 0.5 N A m CENTES : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPU / BOKAO / DUBAI # 10
11 Angl f dflctin, 0 Cupl rquird t dflct th magnt M H sin sin 0 5 Nm 6. (C) Magntic mmnt f ach magntic, M1 M M Sinc tw magntic mmnts ar placd prpndicular t ach thr, hnc, nt magntic mmnt M M M M 1 7. (B) Distanc btwn tw atms.7å d.7 Atmic radius, r 1.85Å Nw, atmic radius, r a Whr, a lattic paramtr r 1.85 a 1.85 a.7å.å 8. (A) Whn th wavs which scillats prpndicularly t th dirctin f prpagatin ar knwn as th transvrs wavs and als th transvrs wavs can b prducd in slids ths which ar having sm rigidly. As w knw that th gass d nt hav any rigidly. Thrfr, transvrs wavs can nt b prducd in gass. 9. (B) Displacmnt, x a 0 a1t a t Vlcity f th particl, dx da0 a1t a t v dt dt a1 a t Acclratin f th particl, dv d a1 a t a dt dt a a 50. (B) Bcaus f air rsistanc is takn int cnsidratin s th hrizntal vlcity f th bmb is dcrasd, whil th arplan is mving with cnstant spd. Nw it is clar that bmb will fall n th arth bhind th arplan. CENTES : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPU / BOKAO / DUBAI # 11
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 informationSensors 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 informationChapter 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 informationLECTURE 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 informationLecture 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.
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 informationSAFE 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 informationN J of oscillators in the three lowest quantum
. a) Calculat th fractinal numbr f scillatrs in th thr lwst quantum stats (j,,,) fr fr and Sl: ( ) ( ) ( ) ( ) ( ).6.98. fr usth sam apprach fr fr j fr frm q. b) .) a) Fr a systm f lcalizd distinguishabl
More informationModern 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 informationA 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 informationEven/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 information1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by:
Elctromagntic Induction. Lorntz forc on moving charg Point charg moving at vlocity v, F qv B () For a sction of lctric currnt I in a thin wir dl is Idl, th forc is df Idl B () Elctromotiv forc f s any
More information5 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 informationClassical Magnetic Dipole
Lctur 18 1 Classical Magntic Dipol In gnral, a particl of mass m and charg q (not ncssarily a point charg), w hav q g L m whr g is calld th gyromagntic ratio, which accounts for th ffcts of non-point charg
More informationELECTROMAGNETIC INDUCTION CHAPTER - 38
. (a) CTOMAGNTIC INDUCTION CHAPT - 38 3 3.dl MT I M I T 3 (b) BI T MI T M I T (c) d / MI T M I T. at + bt + c s / t Volt (a) a t t Sc b t Volt c [] Wbr (b) d [a., b.4, c.6, t s] at + b. +.4. volt 3. (a)
More informationWorksheet 1: Electrostatics
Wrksht : lctrstatics ) xplain why it is lctrns and nt prtns which ar thught t b xchangd in lctrstatic intractins. ) A strip f actat and a strip f silk ar rubbd tgthr. What can b said abut th chargs bfr
More information22/ 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 informationPrinciples of Humidity Dalton s law
Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid
More informationLecture 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 informationPhys101 Final Code: 1 Term: 132 Wednesday, May 21, 2014 Page: 1
Phys101 Final Cde: 1 Term: 1 Wednesday, May 1, 014 Page: 1 Q1. A car accelerates at.0 m/s alng a straight rad. It passes tw marks that are 0 m apart at times t = 4.0 s and t = 5.0 s. Find the car s velcity
More informationExam 2 Thursday (7:30-9pm) It will cover material through HW 7, but no material that was on the 1 st exam.
Exam 2 Thursday (7:30-9pm) It will covr matrial through HW 7, but no matrial that was on th 1 st xam. What happns if w bash atoms with lctrons? In atomic discharg lamps, lots of lctrons ar givn kintic
More informationDeepak 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 informationModel of the Electron
Mdl f th Elctrn Ph.M. Kanarv * Th intrprtatin f sm f thrtical fundatins f physics will b changd. Planck s cnstant is knwn t b n f such fundatins, which srvs as a basis f quantum mchanics [1], [3], [6],
More informationDUAL NATURE OF MATTER AND RADIATION
Chaptr 11 DUAL NATURE OF MATTER AND RADIATION Intrdctin Light xhibit dal natr - wav natr and particl natr. In Phnmna lik Intrfrnc, diffrctin tc wav natr is xhibitd. In pht lctric ffct, cmptn ffct tc particl
More informationHigh Energy Physics. Lecture 5 The Passage of Particles through Matter
High Enrgy Physics Lctur 5 Th Passag of Particls through Mattr 1 Introduction In prvious lcturs w hav sn xampls of tracks lft by chargd particls in passing through mattr. Such tracks provid som of th most
More informationCosmological and Intrinsic Redshifts. November 19, 2010.
Csmlgical and Intrinsic Rdshifts Nvmbr 19, 21. Jsé Francisc García Juliá C/ Dr. Marc Mrncian, 65, 5. 4625 Valncia (Spain) E-mail: js.garcia@dival.s Abstract In a rcnt articl, a singl tird light mchanism,
More informationPHYS ,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 informationTopic 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 informationUniversity of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination
Univrsity of Illinois at Chicago Dpartmnt of hysics hrmodynamics & tatistical Mchanics Qualifying Eamination January 9, 009 9.00 am 1:00 pm Full crdit can b achivd from compltly corrct answrs to 4 qustions.
More information:2;$-$(01*%<*=,-./-*=0;"%/;"-*
!"#$%'()%"*#%*+,-./-*+01.2(.*3+456789*!"#$%"'()'*+,-."/0.%+1'23"45'46'7.89:89'/' ;8-,"$4351415,8:+#9' Dr. Ptr T. Gallaghr Astrphyscs Rsarch Grup Trnty Cllg Dubln :2;$-$(01*%
More informationExam 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 informationIntroduction to Condensed Matter Physics
Introduction to Condnsd Mattr Physics pcific hat M.P. Vaughan Ovrviw Ovrviw of spcific hat Hat capacity Dulong-Ptit Law Einstin modl Dby modl h Hat Capacity Hat capacity h hat capacity of a systm hld at
More informationBORH S DERIVATION OF BALMER-RYDBERG FORMULA THROUGH QUANTUM MECHANICS
BORH S DERIVATION OF BALMER-RYDBERG FORMULA THROUGH QUANTUM MECHANICS Musa D. Abdullahi Umaru Musa Yar adua Univrsity, P.M.B. 18 Katsina, Katsina Stat, Nigria musadab@utlk.cm Abstract Accrding t classical
More informationChapter 8: Electron Configurations and Periodicity
Elctron Spin & th Pauli Exclusion Principl Chaptr 8: Elctron Configurations and Priodicity 3 quantum numbrs (n, l, ml) dfin th nrgy, siz, shap, and spatial orintation of ach atomic orbital. To xplain how
More informationKinetic theory says that molecules are in constant motion. Perfume molecules moving across the room are evidence of this.
Chaptr 13- Th Stats f Mattr Gass- indfinit vum and shap, w dnsity. Liquids- dfinit vum, indfinit shap, and high dnsity. Sids- dfinit vum and shap, high dnsity Sids and iquids hav high dnsitis bcaus thir
More informationELEG 413 Lecture #6. Mark Mirotznik, Ph.D. Professor The University of Delaware
LG 43 Lctur #6 Mrk Mirtnik, Ph.D. Prfssr Th Univrsity f Dlwr mil: mirtni@c.udl.du Wv Prpgtin nd Plritin TM: Trnsvrs lctrmgntic Wvs A md is prticulr fild cnfigurtin. Fr givn lctrmgntic bundry vlu prblm,
More informationJournal of Theoretics
Jurnal f Thrtics PLANCK S CONSTANT AND THE MODEL OF THE ELECTRON Ph. M. Kanarv Th Kuban Stat Agrarian Univrsity. Dpartmnt f Thrtical Mchanics. Dctr f Txnical Scincs, Prfssr. E-mail: kanphil@mail.kuban.ru
More informationBackground: 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 informationMAXIMA-MINIMA EXERCISE - 01 CHECK YOUR GRASP
EXERCISE - MAXIMA-MINIMA CHECK YOUR GRASP. f() 5 () 75 f'() 5. () 75 75.() 7. 5 + 5. () 7 {} 5 () 7 ( ) 5. f() 9a + a +, a > f'() 6 8a + a 6( a + a ) 6( a) ( a) p a, q a a a + + a a a (rjctd) or a a 6.
More informationMAGNETIC MONOPOLE THEORY
AGNETIC ONOPOLE THEORY S HUSSAINSHA Rsarch schlar f ECE, G.Pullaiah Cllg f Enginring and Tchnlgy, Kurnl, Andhra Pradsh, India Eail: ssshaik80@gail.c Cll: +91 9000390153 Abstract: Th principal bjctiv f
More informationElements 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 informationLecture 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 informationSolution to HW14 Fall-2002
Slutin t HW14 Fall-2002 CJ5 10.CQ.003. REASONING AND SOLUTION Figures 10.11 and 10.14 shw the velcity and the acceleratin, respectively, the shadw a ball that underges unirm circular mtin. The shadw underges
More informationEE 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 informationDefinition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.
Dirctivity or Dirctiv Gain. 1 Dfinition1: Dirctivity Th ratio of th radiation intnsity in a givn dirction from th antnna to th radiation intnsity avragd ovr all dirctions. Dfinition2: Th avg U is obtaind
More informationThe 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 informationA 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 informationorbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the
Lctur 22-1 Byond Bohr Modl Unfortunatly, th classical visualization of th orbiting lctron turns out to b wrong vn though it still givs us a simpl way to think of th atom. Quantum Mchanics is ndd to truly
More informationSynchronous machines
Synchronous gnrator (altrnator): transorms mchanical nrgy into lctric nrgy; dsignd to gnrat sinusoidal oltags and currnts; usd in most powr plants, or car altrnators, tc. Synchronous motor: transorms lctric
More informationLecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e
8/7/018 Cours Instructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 3 Skin Dpth & Powr Flow Skin Dpth Ths & Powr nots Flow may contain
More informationFlipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System
Flipping Physics Lecture Ntes: Simple Harmnic Mtin Intrductin via a Hrizntal Mass-Spring System A Hrizntal Mass-Spring System is where a mass is attached t a spring, riented hrizntally, and then placed
More informationThree charges, all with a charge of 10 C are situated as shown (each grid line is separated by 1 meter).
Three charges, all with a charge f 0 are situated as shwn (each grid line is separated by meter). ) What is the net wrk needed t assemble this charge distributin? a) +0.5 J b) +0.8 J c) 0 J d) -0.8 J e)
More information"NEET / AIIMS " SOLUTION (6) Avail Video Lectures of Experienced Faculty.
07 NEET EXAMINATION SOLUTION (6) Avail Vide Lectures f Exerienced Faculty Page Sl. The lean exressin which satisfies the utut f this lgic gate is C = A., Whichindicates fr AND gate. We can see, utut C
More informationCoulomb s Law Worksheet Solutions
PHLYZIS ulb Law Wrkht Slutin. w charg phr 0 c apart attract ach thr with a frc f 3.0 0 6 N. What frc rult fr ach f th fllwing chang, cnir paratly? a Bth charg ar ubl an th itanc rain th a. b An uncharg,
More informationElectrical 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 informationEAcos θ, where θ is the angle between the electric field and
8.4. Modl: Th lctric flux flows out of a closd surfac around a rgion of spac containing a nt positiv charg and into a closd surfac surrounding a nt ngativ charg. Visualiz: Plas rfr to Figur EX8.4. Lt A
More informationUNIT-III-Dielectric and Magnetic properties of materials
UNIT-III-Dilctric and Magntic prprtis f matrials Syllabus: Dilctric cnstant and plarizatin f dilctric matrials - Typs f plarizatin Equatin fr intrnal fild in liquids and slids ( n dimnsinal) Clausius Mstti
More informationFUNDAMENTAL 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 informationELEC 372 LECTURE NOTES, WEEK 11 Dr. Amir G. Aghdam Concordia University
ELEC 37 LECTURE NOTES, WEE Dr Amir Aghdam Cncrdia Univrity Part f th nt ar adaptd frm th matrial in th fllwing rfrnc: Mdrn Cntrl Sytm by Richard C Drf and Rbrt H Bihp, Prntic Hall Fdback Cntrl f Dynamic
More informationNARAYANA 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 informationCHAPTER 6 WORK AND ENERGY
CHAPTER 6 WORK AND ENERGY CONCEPTUAL QUESTIONS 16. REASONING AND SOLUTION A trapeze artist, starting rm rest, swings dwnward n the bar, lets g at the bttm the swing, and alls reely t the net. An assistant,
More informationAcid Base Reactions. Acid Base Reactions. Acid Base Reactions. Chemical Reactions and Equations. Chemical Reactions and Equations
Chmial Ratins and Equatins Hwitt/Lyns/Suhki/Yh Cnptual Intgratd Sin During a hmial ratin, n r mr nw mpunds ar frmd as a rsult f th rarrangmnt f atms. Chaptr 13 CHEMICAL REACTIONS Ratants Prduts Chmial
More informationPH2200 Practice Final Exam Spring 2004
PH2200 Practic Final Exam Spring 2004 Instructions 1. Writ your nam and studnt idntification numbr on th answr sht. 2. This a two-hour xam. 3. Plas covr your answr sht at all tims. 4. This is a closd book
More informationSec 2.3 Modeling with First Order Equations
Sc.3 Modling with First Ordr Equations Mathmatical modls charactriz physical systms, oftn using diffrntial quations. Modl Construction: Translating physical situation into mathmatical trms. Clarly stat
More informationCOHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.
MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function
More informationFlipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System
Flipping Physics Lecture Ntes: Simple Harmnic Mtin Intrductin via a Hrizntal Mass-Spring System A Hrizntal Mass-Spring System is where a mass is attached t a spring, riented hrizntally, and then placed
More informationLast time. Resistors. Circuits. Question. Quick Quiz. Quick Quiz. ( V c. Which bulb is brighter? A. A B. B. C. Both the same
Last tim Bgin circuits Rsistors Circuits Today Rsistor circuits Start rsistor-capacitor circuits Physical layout Schmatic layout Tu. Oct. 13, 2009 Physics 208 Lctur 12 1 Tu. Oct. 13, 2009 Physics 208 Lctur
More informationQ1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string?
Term: 111 Thursday, January 05, 2012 Page: 1 Q1. A string f length L is fixed at bth ends. Which ne f the fllwing is NOT a pssible wavelength fr standing waves n this string? Q2. λ n = 2L n = A) 4L B)
More informationPHYS-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 informationDifferential Equations
UNIT I Diffrntial Equations.0 INTRODUCTION W li in a world of intrrlatd changing ntitis. Th locit of a falling bod changs with distanc, th position of th arth changs with tim, th ara of a circl changs
More informationHydrogen Atom and One Electron Ions
Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial
More informationLecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields
Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration
More informationEXST 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 information1997 AP Calculus AB: Section I, Part A
997 AP Calculus AB: Sction I, Part A 50 Minuts No Calculator Not: Unlss othrwis spcifid, th domain of a function f is assumd to b th st of all ral numbrs for which f () is a ral numbr.. (4 6 ) d= 4 6 6
More informationThe Electromagnetic Mass of a Charged Particle
In mmry f M.I. Kuligina (1914 1994) Th Elctrmagntic Mass f a Chargd Particl V.A. Kuligin, G.A. Kuligina, M.V. Krnva Dpartmnt f Physics, Stat Univrsity Univrsittskaya Sq. 1, Vrnh 394693, Russia A slutin
More informationChapter 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 informationGradebook & Midterm & Office Hours
Your commnts So what do w do whn on of th r's is 0 in th quation GmM(1/r-1/r)? Do w nd to driv all of ths potntial nrgy formulas? I don't undrstand springs This was th first lctur I actually larnd somthing
More informationWhy 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 informationIntroduction 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 informationEXERCISE - 01 CHECK YOUR GRASP
DIFFERENTIAL EQUATION EXERCISE - CHECK YOUR GRASP 7. m hn D() m m, D () m m. hn givn D () m m D D D + m m m m m m + m m m m + ( m ) (m ) (m ) (m + ) m,, Hnc numbr of valus of mn will b. n ( ) + c sinc
More informationSinusoidal Response Notes
ECE 30 Sinusoidal Rspons Nots For BIBO Systms AStolp /29/3 Th sinusoidal rspons of a systm is th output whn th input is a sinusoidal (which starts at tim 0) Systm Sinusoidal Rspons stp input H( s) output
More informationSection 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 informationOutline. Heat Exchangers. Heat Exchangers. Compact Heat Exchangers. Compact Heat Exchangers II. Heat Exchangers April 18, ME 375 Heat Transfer 1
Hat Exangr April 8, 007 Hat Exangr Larry artt Manial Engrg 375 Hat ranfr April 8, 007 Outl Bai ida f at xangr Ovrall at tranfr ffiint Lg-man tmpratur diffrn mtd Efftivn NU mtd ratial nidratin Hat Exangr
More informationMath 34A. Final Review
Math A Final Rviw 1) Us th graph of y10 to find approimat valus: a) 50 0. b) y (0.65) solution for part a) first writ an quation: 50 0. now tak th logarithm of both sids: log() log(50 0. ) pand th right
More information2008 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 informationCalculation of electromotive force induced by the slot harmonics and parameters of the linear generator
Calculation of lctromotiv forc inducd by th lot harmonic and paramtr of th linar gnrator (*)Hui-juan IU (**)Yi-huang ZHANG (*)School of Elctrical Enginring, Bijing Jiaotong Univrity, Bijing,China 8++58483,
More informationA 1 A 2. a) Find the wavelength of the radio waves. Since c = f, then = c/f = (3x10 8 m/s) / (30x10 6 Hz) = 10m.
1. Young s doubl-slit xprint undrlis th instrunt landing syst at ost airports and is usd to guid aircraft to saf landings whn th visibility is poor. Suppos that a pilot is trying to align hr plan with
More informationContemporary, atomic, nuclear, and particle physics
Contmporary, atomic, nuclar, and particl physics 1 Blackbody radiation as a thrmal quilibrium condition (in vacuum this is th only hat loss) Exampl-1 black plan surfac at a constant high tmpratur T h is
More informationChemical Physics II. More Stat. Thermo Kinetics Protein Folding...
Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg
More informationPart 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 informationRadiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017
Th following qustions ar to b answrd individually. Usful information such as tabls with dtctor charactristics and graphs with th proprtis of matrials ar availabl in th cours wb sit: http://www.lip.pt/~patricia/fisicadaradiacao.
More information1. In the given figure PQRS is a parallelogram. Find the coordinates of R.
Tst Assss Achiv Class : 9 CLASS : 9 Mathmatics 1. In th givn figur PQRS is a paralllogram. Find th coordinats of R. Y S(2, 3) R O P(1, 0) Q(5, 0) X (5, 2) (5, 3) (6, 2) (6, 3) 2. Th prpndicular distanc
More informationGUC (Dr. Hany Hammad) 11/2/2016
GUC (D. Han Hammad) //6 ctu # 7 Magntic Vct Ptntial. Radiatin fm an lmnta Dipl. Dictivit. Radiatin Rsistanc. Th ng Dipl Th half wavlngth Dipl Dictivit. Radiatin Rsistanc. Tavling wav antnna. Th lp antnna.
More informationP3-4 (a) Note: This problem can have many solutions as data fitting can be done in many ways. Using Arrhenius Equation For Fire flies: T(in K)
# Hnc "r k " K ( $ is th rquird rat law. P- Solution is in th dcoding algorithm availabl sparatly from th author. P-4 (a Not: This problm can hav many solutions as data fitting can b don in many ways.
More informationMicrowave 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 information2. Background Material
S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds
More informationUnfired pressure vessels- Part 3: Design
Unfird prssur vssls- Part 3: Dsign Analysis prformd by: Analysis prformd by: Analysis vrsion: According to procdur: Calculation cas: Unfird prssur vssls EDMS Rfrnc: EF EN 13445-3 V1 Introduction: This
More informationQ x = cos 1 30 = 53.1 South
Crdinatr: Dr. G. Khattak Thursday, August 0, 01 Page 1 Q1. A particle mves in ne dimensin such that its psitin x(t) as a functin f time t is given by x(t) =.0 + 7 t t, where t is in secnds and x(t) is
More information= m. Suppose the speed of a wave on a string is given by v = Κ τμ
Phys101 First Majr-11 Zer Versin Sunday, Octber 07, 01 Page: 1 Q1. Find the mass f a slid cylinder f cpper with a radius f 5.00 cm and a height f 10.0 inches if the density f cpper is 8.90 g/cm 3 (1 inch
More informationPHA 5127 Answers Homework 2 Fall 2001
PH 5127 nswrs Homwork 2 Fall 2001 OK, bfor you rad th answrs, many of you spnt a lot of tim on this homwork. Plas, nxt tim if you hav qustions plas com talk/ask us. Thr is no nd to suffr (wll a littl suffring
More information