ACE. Engineering Academy. Hyderabad Delhi Bhopal Pune Bhubaneswar Bengaluru Lucknow Patna Chennai Vijayawada Visakhapatnam Tirupati Kukatpally Kolkata

Size: px
Start display at page:

Download "ACE. Engineering Academy. Hyderabad Delhi Bhopal Pune Bhubaneswar Bengaluru Lucknow Patna Chennai Vijayawada Visakhapatnam Tirupati Kukatpally Kolkata"

Transcription

1 ES D: 5 CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr engluru Lucknow Ptn Chenni ijywd iskhptnm irupti Kuktplly Kolkt H.O: 4, Floor, hmn Plz, Opp. Methodist School, bids, Hyderbd-5, Ph: , , , ESE- 8 (Prelims) - Offline est Series est-9 ELECCL ENGNEENG SUJEC: ELECC CCUS ND FELDS MEL SCENCE SOLUONS. ns: () Sol: he dots indicte tht when current entering ut, = = di M dt the dotted terminl of one coil, voltge induced is positive t the dotted terminl of. ns: (c) other coil. Sol: Given circuit, Given circuit, i i M i 5 L L Coil Coil 4 Here current entering the dotted terminl of coil. induced voltge is positive t the dotted pplying KL, 5( ) 4 = = 5i terminl of coil. = di M dt CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

2 : : Electricl Engineering 3. ns: (c) Sol: Given grph 6 () 4 () 3 (4) 5 (3) 7 Number of possible trees = [ r ][ r ] Where, [ r ] is the reduced incidence mtrix ncidence mtrix, for the given grph is () () (3) (4) y tking the (4) node s reference, educed incidence mtrix, [ r ] = [ r ][ r ] = 4 = [ r ][ r ] = 3 3 = 4(9 ) (3) (3) = = 4 Number of possible trees = 4 4. ns: () Sol: Given networks, 5 N Fig. i N 3 Fig. pplying reciprocity theorem to Fig () N y using linerity principle, N 3 b Fig.3 CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

3 : 3 : ESE - 8 (Prelims) Offline est Series 3 = 3 With respect to the terminls nd b the short circuit current SC = = 3 Similrly with respect to the terminls nd b the Norton s equivlent resistnce N is 4 i = SC 4 i = 5. ns: () 4 3 = 6 Sol: Given network, H N b N Fig.4 b N x 3 x Fig () is the energized version of Fig. (4) N = 5 = 4 he Notron s equivlent of Fig. (3) with respect to terminls nd b is hen the Fig. () becomes b 5 b N N =4 sc =3 i N =4 b sc =3 ssume voltge source of vlue o hving frequency of 4 rd/sec is pplied cross the circuit then x = x /F x j.5 pplying KL in the loop, o x j3.5 3 x = o j3.5 3 = o = = o 4 j3.5 Circuit power fctor = cos(4.85) j4 3 x =.755 lgging CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

4 : 4 : Electricl Engineering 6. ns: () Sol: Given network, When nd terminls re open circuited i = hen the equivlent network becomes i= i CE Engineering cdemy j 5 j 5 i i th th s there is no source to drive the bove circuit th = 7. ns: (b) Sol: Given network, Here the power is consumed only in the resistor nd its vlue is P D Y.. () Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt Y j5 j5

5 : 5 : ESE - 8 (Prelims) Offline est Series Now connect blnced str lod, ech of resistnce vlue s shown below Power consumed P s 3 N 3N Y Ps. () s () = () Y = N Y Y pplying KL, ( ) = = D =. 9. ns: () Sol: Given network,. C 5F F F F 8. ns: (d) Sol: Given network, nitil chrge in C = 5C nitil voltge cross cpcitor C is q C 5 5 he equivlent, circuit fter the switch is closed is = D C =5F 5F CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

6 : 6 : Electricl Engineering Convert into Lplce domin (s) s (s) Cs Cs. ns: (c) Sol: Given network F /5 3H /s (s) Cs (s) s C nd (s) (s) Cs. Cs s C Stedy stte vlue of v(t) is = = s Lt s(s) s Lt s. s(cs ) = 5 Stedy stte voltge cross F cpcitor = 5 Chrge in the F cpcitor q = C = 5 = 5 C he dul of the bove network is. ns: (b) Sol: he wve form is s shown below 4 rms rms / 3/ / rms (4) H dt 6 / 8 5 3F t CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

7 : 7 : ESE - 8 (Prelims) Offline est Series. ns: (b) Sol: Given circuit 6Ω b Ω 8 3Ω he bove circuit cn be redrwn s L C L C t the lower cut off frequency, L C L C Net rectnce = 4. ns: () 6 3 b 8 Sol: i C C Under stedy stte condition c = = 8 8 nd i(t)= e t/c Energy dissipted by the resistor otl power delivered by the sources = 8 8 = 34W 3. ns: (d) m Sol: t the cut off frequency L C E E E i e dt t / C t / C e / C C. dt C 6 5mJ C CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

8 : 8 : Electricl Engineering 5. ns: () Sol: We know, when two, -port networks re connected in prllel, their individul Y- prmeters gets dded. First, we need to convert given CD prmeters to Y-prmeters. For -port network Y-prmeters re Y Y () Y Y CD prmeters () C D Mke = to find Y & Y Eqution () becomes = Y = D D Y = C D = C D (3) Y C D C D nd = eqution (3) C D C D = Y = put this vlue in Y-prmeter mtrix in terms of CD prmeter is Y D C D Similrly, =, to find Y & Y From eqution () = Y = Y = C D C D = C D C D = ut = Y or Y eq = Y Y = D C D D C D ` CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

9 : 9 : ESE - 8 (Prelims) Offline est Series Y or Y eq = D C D Now, gin connect bck to CD prmeters D C D D Mke = = = D =.5 D / D / 4 Mke =, eqution (4) becomes = & = = C = C = = D C D D C D D C D = C C D C 6. ns: (c) Sol: Given network function F s s s s 3.5 D he pole zero pttern for the bove network function is s shown below j 3 s we cn see from bove pole zero plot poles nd zeros lternte on negtive rel xis nd nerest to the origin is pole. t cn be relized s C impednce function or L dmittnce function. 7. ns: () Sol: ssume the circuit is in stedy stte before the switch opens. he inductor will cts s short circuit. hen the circuit t t= is CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

10 : : Electricl Engineering i i x ( ) he equivlent network becomes 3Ω Ω / 3Ω i L ( ) /3 Equivlent resistnce seen by the voltge source is = 3 i = i x ( ) = i ns: () Sol: Y = = 4 3 = = Equivlent resistnce seen by the port is = = 3 6 = 6 9. ns: (d) Sol: Given network 6 Y = 6 3 / s we re unble to write interms of nd therefore Y prmeters doesn't exist. /3. ns: () /4 Sol: For prllel resonnt circuit, dmittnce, Y jc L Susceptnce = C L he plot of susceptnce is s shown below CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

11 : : ESE - 8 (Prelims) Offline est Series L t t = is = C L di = di dt dt = di dt t t = is = /sec. L. ns: (b) Sol: For. ns: (c) Sol: ssume the circuit is in stedy stte before the switch is chnged from to b inductor will cts s short circuit. hen the circuit is C driving point impednce function C driving point dmittnce function L driving point impednce function L driving point dmittnce function Poles nd zeros should lternte only on negtive rel xis i( ) 3. ns: (b) s (s 3) Sol: Given Z(S) = s (s ) he pole zero pttern is s shown below i( ) =. nd initil voltge cross the cpcitor is C ( ) = t t= the equivlent circuit is b i L. j 3 s we cn see the poles nd zeros lternte on negtive rel xis nd nerest to the origin is pole. t cn be relized s C driving point impednce CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

12 : : Electricl Engineering s 3 Z(S) = = s(s ) 3/ s / s he network for the bove impednce function is s shown below 4 F F 3 wo energy storge elements re present. 5. ns: (b) Sol: he equivlent network t t= is i L ( ) = = t t= the network is 5 i L ( ) 4. ns: (d) Sol: t t= the circuit is s ( ) i(t) F c ( ) = 5 S ( t= ) = 5 = 5 Convert into Lplce domin 6. ns: (d) Sol: t t = the network is C (s) 5 s s i L ( ) C 5 (s) s s v C (t) = 5 u(t) t t= u(t= ) = v C ( ) = 5 5 = s i L ( ) = = t t= the network is CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

13 : 3 : ESE - 8 (Prelims) Offline est Series H 3 H 8. ns: (b) Sol: Q Convert the bove circuit into Lplce domin pplying KCL t node '' (s) (s) (s) = s 3 s (s) (s) = 3 s 3 s 3 9 s s t (t) = 7. ns: () v (t) = 3 e 4.5 t Sol: Sttement- is correct becuse in cse of chrged bodies of rbitrry shpe, it is difficult to find the ctul distnce between them. s (s) 3 s Sttement- is incorrect s Coulomb s lw is vlid only when the point chrges re t rest. Consider string, the net force on string is given s, F F F C cos Where, F F C F C Q 4 nd = 6 Q F cos6 4 Q 4 3Q.. () 8 For string to brek due to electrosttic force, F 3 From eqution -, 3Q Q C Q F Fig.() 3 Q 8 8 or, Qmin 8, CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

14 : 4 : Electricl Engineering 9. ns: (d) Sol: Given dt, H = /m Let, be the current in the loop nd be the rdius of the loop, then H t the centre of the loop is given s, H H H / m H H Fig.() & H H 4H 3. ns: () H Sol: Given dt, J kx ˆ 5y ˆ x 4 8 / m y hen for stedy current i.e, chrge entering nd leving cross-section of the conductor to be equl t ny time,. J {Continuity eqution,.j t but v = constnt} â x x â y k5 = k = 5 y â z y. v kx â 5y â x y CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

15 : 5 : ESE - 8 (Prelims) Offline est Series 3. ns: (c) Sol:..( ) (correct) i.e, divergence of curl of vector is lwys zero.. (.) (correct) i.e; curl of grdient of sclr is lwys zero. ds.d (correct) 3. s L he bove expression is the Stoke s theorem which sys tht closed line integrl of vector is equl to the surfce integrl of the curl of tht vector. dv.ds (incorrect) 4. s Guss s diversion theorems is given s,. dv.ds v 3. ns: (b) s Which sys tht closed surfce integrl of vector is equl to the volume integrl of the diversion of tht vector. Sol: Electric flux: ccording to Guss s lw, the surfce integrl of the electric field intensity gives the mount of electric flux. q E.ds electricl 33. ns: (c) Sol: Sttement- is correct For liner dielectric Polriztion (P) E (Electric field) P = e E e is susceptblity (con stnt for liner dielectric) cpcitor with liner dielectric hs cpcitnce independent of the chrge on the pltes nd their potentil difference, rther the cpcitnce is equl to the rtio of the chrge on the plte to tht of the potentil difference between them. C = Q Sttement- is correct s the cpcitor is connected to bttery, hence voltge is fixed. Let Q d nd Q be the chrge on the pltes for dielectric nd ir cse, then, Qd Cd Cd r d Q C C d = r Q d = Q r = ut, r = e = e = Coulombs unit of Coulombs / Newton meter e = Newton-meter /Coulombs. CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

16 : 6 : Electricl Engineering 34. ns: (b) Sol: pplying Guss s lw, D.ds Q enclosed 4 D(4r) 3 D = 3 3r 3 t the surfce of the sphere, r = D = 35. ns: (d) 3 O Sphericl Gussin surfce Fig. Sol: Sttement - is correct s ngle between r nd r is 9 o, therefore, r.( r) = Sttement - is correct s.r ˆ ˆ ˆ. xˆ x x x yˆ zˆ.r 3 x y z x y z Sttement 3 is correct s,.(r.r) ˆ ˆ ˆ x y z. x y z x x x ˆ ˆ ˆ = x x y y z z r = ( xˆ x yˆ ˆ y z z ) = r Sttement-4 is correct s, ngle between nd r is 9 o herefore,.( r ) = 36. ns: (d) Sol: s the sphere is conducting nd hs potentil on its surfce (grounded) Hence, = = Where, nd re the potentil t points nd due to q nd q, hence For = q q 4(d ) 4( b) For =, q q 4(d ) 4( b) Eqn () q = Eqn () q = b b d d ( b) q (d ) ( b) q (d ) d bd b = d bd b = bd = bd b = d (3) = () =.. () CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

17 : 7 : ESE - 8 (Prelims) Offline est Series hen, q= q = 37. ns: () q d q d d d d q (4) d Sol: onic polriztion tkes plce by displcement of ctions nd nions. t is independent of temperture i = e m onic Polrizbility is inversely proportionl to the squre of nturl frequency () 38. ns: (b) Sol: Polriztion (P) = ( r )E = (8 ) 3 = ns: (b) Sol: f the rdius X =.55, more stble configurtion is possible with three nions bonding with ction. his form stble structure only upto n X vlue of.5 for.55 < X <.5 the nions do not touch ech other. 4. ns: (c) 4. ns: () 4. ns: (b) Sol: ne ne ns: (c) Sol: H C = = m /-s H C = 5 C c 8 c = 64.5 c c C =.3 K 44. ns: (b) Sol: J c = 45. ns: () 64.5 ic H C H Sol: sed on F.London nd H.London reserch, C 8 mgnetic flux density is llowed by super conductor up to some lyers from the surfce. CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

18 : 8 : Electricl Engineering London penetrtion depth: t is the depth from the surfce of super conductor upto which flux density is decresed by 63%. = e X L = Flux density t depth X = flux density t surfce of super conductor L = London penetrtion depth 5. ns: () Sol: he hysteresis loop of ferromgnetic mteril depends on. emperture. Crystllogrphic imperfection 3. Cold working 5. ns: () Sol: M 46. ns: (d) Sol: Hll ngle tn H = =.4.=.4 H = tn (.4) H =.349 [] [] [] H 47. ns: () 48. ns: (c) Sol: otl mgnetic moment = N i = 5 3 ( ) = = 4 3 -m 49. ns: () Sol: Mgnetic flux density (b) = 88 4 Wb/m Field strength (H) = /m = H 4 88 = ns: (b) Sol: Mgneto rheologicl mterils hs the bility to increse viscosity drsticlly with pplied field. 53. ns: () 54. ns: (c) 55. ns: (d) 56. ns: () Sol: Wiess-Domin heory: sed on Wiess Domin theory in domin ll the dipoles re ligned in prticulr direction. f the mgnetic field is pplied Domin growth = 7 tkes plce in the field direction nd t higher field, inside domin dipole reltion tkes plce. CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

19 : 9 : ESE - 8 (Prelims) Offline est Series 57. ns: () Sol: Output voltge = t g p = = ns: (d) Sol: G-s compound is zinc blende structure 59. ns: (b) = o 6. ns: (d) Sol: X (,, ) Y,, Z Sol: 4 4 d h k 6. ns: (d) Sol: he bullet proof jocket is mde up of rmid fiber reinforced polymer (F) with reinforcement phse is rmid nd mtrix phse is polymer. CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

20 : : Electricl Engineering 6. ns: (d) Sol: he bonding in cermics is predominntly ionic, it consists of nions nd ctions. he crystl structure of cermics is influenced by the rdius rtios of the ions. he coordintion number depends on the rdius of the bonding ions. Cermics re clssified ccording to their crystl structure s X, X, X 3 nd X 4 types. Exmples under ech type re given below: X : NCl, CsCl, Zns X : SiO, CF, PuO, ho X 3 : io 3, SrZrO 3, SrSnO 3 X 4 : Mgl O 4, Fel O ns: (c) Sol: f the temperture of metl increses, the lttice vibrtion in the crystl structure increses. Hence collision frequency increses nd relxtion time decreses. Due to tht resistivity of metl increses. 64. ns: (c) Sol: Cermics hve high melting point nd cn with stnd high temperture. 65. ns: (b) Sol: Lplcin eqution () ut we know, from Poisson s eqution herefore Lplcin eqution is true for chrge free region where = Every physicl problem must contin tlest one conducting boundry but my contin more thn one. Solution of Lplce s eqution with two different methods (vlid methods) led to sme solution. Since E field is hrmonic (conservtive). 66. ns: (d) Sol: Sttement is incorrect s S. ds Mxwell eqution:.ds i.e., net flux leving closed surfce is zero. When surfce is open.ds m weber Sttement is correct s ubes of mgnetic flux hve no source (or) sink i.e. monopoles do not exist in cse of mgnetic field. N S CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

21 : : ESE - 8 (Prelims) Offline est Series 67. ns: () So sttement () is flse. Sol: When C field is pplied to dielectric mteril, then dielectric constnt of mteril is no longer rel t is hving both rel prt s well s imginry prt r = r j r j r prt (mginry prt) of r is due to power loss in mteril. When C field is pplied to dielectric 7. ns: (b) 73. ns: (b) Sol: Poly crystl mterils re stronger thn single crystl mteril becuse they require more stresses to initite slip nd yielding. Poly crystlline mterils there re mny preferred plnes nd direction for different grins due to their rndom orienttion. mteril, r becomes complex quntity s result power loss in dielectric mteril. 68. ns: (b) Sol: he ntiferro mgnetic mteril depends on Neel s lw = C N nti ferro pr 74. ns: () Sol: io 3 crystl is Ferroelectric mteril upto o C, due to non-centro symmetric (symmetric) structure. ut bove C it become centro-symmetric nd hence it looses its ferroelectric chrcter. 75. ns: (d) 69. ns: (d) N Sol: mpressed voltge = ( j9) Current = (3 j4) Complex power, S = * = ( j9) (3 j4) = (66 j3) Sol: Sttement is incorrect becuse when there is no chrge inside the conductor the electric field inside conductor is zero not infinity. Sttement is correct s el power = 66 W Sttement () is flse. 7. ns: (b) 7. ns: (d) Sol: Equivlent network obtined from - Y trnsformtion reltion is vlid for ny frequency. Guss lw: Electric flux leving ny closed surfce is equl to the chrge enclosed. n cse of conductor s the chrge enclosed by ny closed surfce inside conductor is zero hence there should not be ny electric field inside the conductor. CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

22 CE Engineering cdemy Hyderbd Delhi hopl Pune hubneswr Lucknow Ptn engluru Chenni ijywd izg irupti Kuktplly Kolkt

ACE. Engineering Academy. Hyderabad Delhi Bhopal Pune Bhubaneswar Bengaluru Lucknow Patna Chennai Vijayawada Visakhapatnam Tirupati Kukatpally Kolkata

ACE. Engineering Academy. Hyderabad Delhi Bhopal Pune Bhubaneswar Bengaluru Lucknow Patna Chennai Vijayawada Visakhapatnam Tirupati Kukatpally Kolkata ES D: 5 CE Engineering cdemy Hyderd Delhi hopl Pune huneswr engluru Lucknow Ptn Chenni ijywd iskhptnm irupti Kuktplly Kolkt H.O: 4, Floor, hmn Plz, Opp. Methodist School, ids, Hyderd-5, Ph: 4-33448, 4-33449,

More information

200 points 5 Problems on 4 Pages and 20 Multiple Choice/Short Answer Questions on 5 pages 1 hour, 48 minutes

200 points 5 Problems on 4 Pages and 20 Multiple Choice/Short Answer Questions on 5 pages 1 hour, 48 minutes PHYSICS 132 Smple Finl 200 points 5 Problems on 4 Pges nd 20 Multiple Choice/Short Answer Questions on 5 pges 1 hour, 48 minutes Student Nme: Recittion Instructor (circle one): nme1 nme2 nme3 nme4 Write

More information

CAPACITORS AND DIELECTRICS

CAPACITORS AND DIELECTRICS Importnt Definitions nd Units Cpcitnce: CAPACITORS AND DIELECTRICS The property of system of electricl conductors nd insultors which enbles it to store electric chrge when potentil difference exists between

More information

Exam 1 Solutions (1) C, D, A, B (2) C, A, D, B (3) C, B, D, A (4) A, C, D, B (5) D, C, A, B

Exam 1 Solutions (1) C, D, A, B (2) C, A, D, B (3) C, B, D, A (4) A, C, D, B (5) D, C, A, B PHY 249, Fll 216 Exm 1 Solutions nswer 1 is correct for ll problems. 1. Two uniformly chrged spheres, nd B, re plced t lrge distnce from ech other, with their centers on the x xis. The chrge on sphere

More information

Summary of equations chapters 7. To make current flow you have to push on the charges. For most materials:

Summary of equations chapters 7. To make current flow you have to push on the charges. For most materials: Summry of equtions chpters 7. To mke current flow you hve to push on the chrges. For most mterils: J E E [] The resistivity is prmeter tht vries more thn 4 orders of mgnitude between silver (.6E-8 Ohm.m)

More information

Physics 24 Exam 1 February 18, 2014

Physics 24 Exam 1 February 18, 2014 Exm Totl / 200 Physics 24 Exm 1 Februry 18, 2014 Printed Nme: Rec. Sec. Letter: Five multiple choice questions, 8 points ech. Choose the best or most nerly correct nswer. 1. The totl electric flux pssing

More information

DIRECT CURRENT CIRCUITS

DIRECT CURRENT CIRCUITS DRECT CURRENT CUTS ELECTRC POWER Consider the circuit shown in the Figure where bttery is connected to resistor R. A positive chrge dq will gin potentil energy s it moves from point to point b through

More information

Physics 1402: Lecture 7 Today s Agenda

Physics 1402: Lecture 7 Today s Agenda 1 Physics 1402: Lecture 7 Tody s gend nnouncements: Lectures posted on: www.phys.uconn.edu/~rcote/ HW ssignments, solutions etc. Homework #2: On Msterphysics tody: due Fridy Go to msteringphysics.com Ls:

More information

Problems for HW X. C. Gwinn. November 30, 2009

Problems for HW X. C. Gwinn. November 30, 2009 Problems for HW X C. Gwinn November 30, 2009 These problems will not be grded. 1 HWX Problem 1 Suppose thn n object is composed of liner dielectric mteril, with constnt reltive permittivity ɛ r. The object

More information

Sample Exam 5 - Skip Problems 1-3

Sample Exam 5 - Skip Problems 1-3 Smple Exm 5 - Skip Problems 1-3 Physics 121 Common Exm 2: Fll 2010 Nme (Print): 4 igit I: Section: Honors Code Pledge: As n NJIT student I, pledge to comply with the provisions of the NJIT Acdemic Honor

More information

Reference. Vector Analysis Chapter 2

Reference. Vector Analysis Chapter 2 Reference Vector nlsis Chpter Sttic Electric Fields (3 Weeks) Chpter 3.3 Coulomb s Lw Chpter 3.4 Guss s Lw nd pplictions Chpter 3.5 Electric Potentil Chpter 3.6 Mteril Medi in Sttic Electric Field Chpter

More information

This final is a three hour open book, open notes exam. Do all four problems.

This final is a three hour open book, open notes exam. Do all four problems. Physics 55 Fll 27 Finl Exm Solutions This finl is three hour open book, open notes exm. Do ll four problems. [25 pts] 1. A point electric dipole with dipole moment p is locted in vcuum pointing wy from

More information

Physics 202, Lecture 10. Basic Circuit Components

Physics 202, Lecture 10. Basic Circuit Components Physics 202, Lecture 10 Tody s Topics DC Circuits (Chpter 26) Circuit components Kirchhoff s Rules RC Circuits Bsic Circuit Components Component del ttery, emf Resistor Relistic Bttery (del) wire Cpcitor

More information

Chapter 6 Electrostatic Boundary Value Problems. Dr. Talal Skaik

Chapter 6 Electrostatic Boundary Value Problems. Dr. Talal Skaik Chpter 6 Electrosttic Boundry lue Problems Dr. Tll Skik 1 1 Introduction In previous chpters, E ws determined by coulombs lw or Guss lw when chrge distribution is known, or potentil is known throughout

More information

Physics 3323, Fall 2016 Problem Set 7 due Oct 14, 2016

Physics 3323, Fall 2016 Problem Set 7 due Oct 14, 2016 Physics 333, Fll 16 Problem Set 7 due Oct 14, 16 Reding: Griffiths 4.1 through 4.4.1 1. Electric dipole An electric dipole with p = p ẑ is locted t the origin nd is sitting in n otherwise uniform electric

More information

The Velocity Factor of an Insulated Two-Wire Transmission Line

The Velocity Factor of an Insulated Two-Wire Transmission Line The Velocity Fctor of n Insulted Two-Wire Trnsmission Line Problem Kirk T. McDonld Joseph Henry Lbortories, Princeton University, Princeton, NJ 08544 Mrch 7, 008 Estimte the velocity fctor F = v/c nd the

More information

Lecture 13 - Linking E, ϕ, and ρ

Lecture 13 - Linking E, ϕ, and ρ Lecture 13 - Linking E, ϕ, nd ρ A Puzzle... Inner-Surfce Chrge Density A positive point chrge q is locted off-center inside neutrl conducting sphericl shell. We know from Guss s lw tht the totl chrge on

More information

Reading from Young & Freedman: For this topic, read the introduction to chapter 24 and sections 24.1 to 24.5.

Reading from Young & Freedman: For this topic, read the introduction to chapter 24 and sections 24.1 to 24.5. PHY1 Electricity Topic 5 (Lectures 7 & 8) pcitors nd Dielectrics In this topic, we will cover: 1) pcitors nd pcitnce ) omintions of pcitors Series nd Prllel 3) The energy stored in cpcitor 4) Dielectrics

More information

Physics 2135 Exam 1 February 14, 2017

Physics 2135 Exam 1 February 14, 2017 Exm Totl / 200 Physics 215 Exm 1 Ferury 14, 2017 Printed Nme: Rec. Sec. Letter: Five multiple choice questions, 8 points ech. Choose the est or most nerly correct nswer. 1. Two chrges 1 nd 2 re seprted

More information

I1 = I2 I1 = I2 + I3 I1 + I2 = I3 + I4 I 3

I1 = I2 I1 = I2 + I3 I1 + I2 = I3 + I4 I 3 2 The Prllel Circuit Electric Circuits: Figure 2- elow show ttery nd multiple resistors rrnged in prllel. Ech resistor receives portion of the current from the ttery sed on its resistnce. The split is

More information

Physics Graduate Prelim exam

Physics Graduate Prelim exam Physics Grdute Prelim exm Fll 2008 Instructions: This exm hs 3 sections: Mechnics, EM nd Quntum. There re 3 problems in ech section You re required to solve 2 from ech section. Show ll work. This exm is

More information

Designing Information Devices and Systems I Spring 2018 Homework 8

Designing Information Devices and Systems I Spring 2018 Homework 8 EECS 16A Designing Informtion Devices nd Systems I Spring 2018 Homework 8 This homework is due Mrch 19, 2018, t 23:59. Self-grdes re due Mrch 22, 2018, t 23:59. Sumission Formt Your homework sumission

More information

Candidates must show on each answer book the type of calculator used.

Candidates must show on each answer book the type of calculator used. UNIVERSITY OF EAST ANGLIA School of Mthemtics My/June UG Exmintion 2007 2008 ELECTRICITY AND MAGNETISM Time llowed: 3 hours Attempt FIVE questions. Cndidtes must show on ech nswer book the type of clcultor

More information

Lecture 1: Electrostatic Fields

Lecture 1: Electrostatic Fields Lecture 1: Electrosttic Fields Instructor: Dr. Vhid Nyyeri Contct: nyyeri@iust.c.ir Clss web site: http://webpges.iust.c. ir/nyyeri/courses/bee 1.1. Coulomb s Lw Something known from the ncient time (here

More information

University of Alabama Department of Physics and Astronomy. PH126: Exam 1

University of Alabama Department of Physics and Astronomy. PH126: Exam 1 University of Albm Deprtment of Physics nd Astronomy PH 16 LeClir Fll 011 Instructions: PH16: Exm 1 1. Answer four of the five questions below. All problems hve equl weight.. You must show your work for

More information

Name Class Date. Match each phrase with the correct term or terms. Terms may be used more than once.

Name Class Date. Match each phrase with the correct term or terms. Terms may be used more than once. Exercises 341 Flow of Chrge (pge 681) potentil difference 1 Chrge flows when there is between the ends of conductor 2 Explin wht would hppen if Vn de Grff genertor chrged to high potentil ws connected

More information

ELE B7 Power Systems Engineering. Power System Components Modeling

ELE B7 Power Systems Engineering. Power System Components Modeling Power Systems Engineering Power System Components Modeling Section III : Trnsformer Model Power Trnsformers- CONSTRUCTION Primry windings, connected to the lternting voltge source; Secondry windings, connected

More information

196 Circuit Analysis with PSpice: A Simplified Approach

196 Circuit Analysis with PSpice: A Simplified Approach 196 Circuit Anlysis with PSpice: A Simplified Approch i, A v L t, min i SRC 5 μf v C FIGURE P7.3 () the energy stored in the inductor, nd (c) the instntneous power input to the inductor. (Dul of Prolem

More information

State space systems analysis (continued) Stability. A. Definitions A system is said to be Asymptotically Stable (AS) when it satisfies

State space systems analysis (continued) Stability. A. Definitions A system is said to be Asymptotically Stable (AS) when it satisfies Stte spce systems nlysis (continued) Stbility A. Definitions A system is sid to be Asymptoticlly Stble (AS) when it stisfies ut () = 0, t > 0 lim xt () 0. t A system is AS if nd only if the impulse response

More information

Chapter 7 Steady Magnetic Field. september 2016 Microwave Laboratory Sogang University

Chapter 7 Steady Magnetic Field. september 2016 Microwave Laboratory Sogang University Chpter 7 Stedy Mgnetic Field september 2016 Microwve Lbortory Sogng University Teching point Wht is the mgnetic field? Biot-Svrt s lw: Coulomb s lw of Mgnetic field Stedy current: current flow is independent

More information

Higher Checklist (Unit 3) Higher Checklist (Unit 3) Vectors

Higher Checklist (Unit 3) Higher Checklist (Unit 3) Vectors Vectors Skill Achieved? Know tht sclr is quntity tht hs only size (no direction) Identify rel-life exmples of sclrs such s, temperture, mss, distnce, time, speed, energy nd electric chrge Know tht vector

More information

Designing Information Devices and Systems I Discussion 8B

Designing Information Devices and Systems I Discussion 8B Lst Updted: 2018-10-17 19:40 1 EECS 16A Fll 2018 Designing Informtion Devices nd Systems I Discussion 8B 1. Why Bother With Thévenin Anywy? () Find Thévenin eqiuvlent for the circuit shown elow. 2kΩ 5V

More information

Overview. Before beginning this module, you should be able to: After completing this module, you should be able to:

Overview. Before beginning this module, you should be able to: After completing this module, you should be able to: Module.: Differentil Equtions for First Order Electricl Circuits evision: My 26, 2007 Produced in coopertion with www.digilentinc.com Overview This module provides brief review of time domin nlysis of

More information

10/25/2005 Section 5_2 Conductors empty.doc 1/ Conductors. We have been studying the electrostatics of freespace (i.e., a vacuum).

10/25/2005 Section 5_2 Conductors empty.doc 1/ Conductors. We have been studying the electrostatics of freespace (i.e., a vacuum). 10/25/2005 Section 5_2 Conductors empty.doc 1/3 5-2 Conductors Reding Assignment: pp. 122-132 We hve been studying the electrosttics of freespce (i.e., vcuum). But, the universe is full of stuff! Q: Does

More information

Physics 712 Electricity and Magnetism Solutions to Final Exam, Spring 2016

Physics 712 Electricity and Magnetism Solutions to Final Exam, Spring 2016 Physics 7 Electricity nd Mgnetism Solutions to Finl Em, Spring 6 Plese note tht some possibly helpful formuls pper on the second pge The number of points on ech problem nd prt is mrked in squre brckets

More information

Unit 3: Direct current and electric resistance Electric current and movement of charges. Intensity of current and drift speed. Density of current in

Unit 3: Direct current and electric resistance Electric current and movement of charges. Intensity of current and drift speed. Density of current in Unit 3: Direct current nd electric resistnce Electric current nd movement of chrges. ntensity of current nd drift speed. Density of current in homogeneous currents. Ohm s lw. esistnce of homogeneous conductor

More information

Conducting Ellipsoid and Circular Disk

Conducting Ellipsoid and Circular Disk 1 Problem Conducting Ellipsoid nd Circulr Disk Kirk T. McDonld Joseph Henry Lbortories, Princeton University, Princeton, NJ 08544 (September 1, 00) Show tht the surfce chrge density σ on conducting ellipsoid,

More information

Problem Set 3 Solutions

Problem Set 3 Solutions Msschusetts Institute of Technology Deprtment of Physics Physics 8.07 Fll 2005 Problem Set 3 Solutions Problem 1: Cylindricl Cpcitor Griffiths Problems 2.39: Let the totl chrge per unit length on the inner

More information

2. THE HEAT EQUATION (Joseph FOURIER ( ) in 1807; Théorie analytique de la chaleur, 1822).

2. THE HEAT EQUATION (Joseph FOURIER ( ) in 1807; Théorie analytique de la chaleur, 1822). mpc2w4.tex Week 4. 2.11.2011 2. THE HEAT EQUATION (Joseph FOURIER (1768-1830) in 1807; Théorie nlytique de l chleur, 1822). One dimension. Consider uniform br (of some mteril, sy metl, tht conducts het),

More information

POLYPHASE CIRCUITS. Introduction:

POLYPHASE CIRCUITS. Introduction: POLYPHASE CIRCUITS Introduction: Three-phse systems re commonly used in genertion, trnsmission nd distribution of electric power. Power in three-phse system is constnt rther thn pulsting nd three-phse

More information

ragsdale (zdr82) HW2 ditmire (58335) 1

ragsdale (zdr82) HW2 ditmire (58335) 1 rgsdle (zdr82) HW2 ditmire (58335) This print-out should hve 22 questions. Multiple-choice questions my continue on the next column or pge find ll choices before nswering. 00 0.0 points A chrge of 8. µc

More information

Designing Information Devices and Systems I Spring 2018 Homework 7

Designing Information Devices and Systems I Spring 2018 Homework 7 EECS 16A Designing Informtion Devices nd Systems I Spring 2018 omework 7 This homework is due Mrch 12, 2018, t 23:59. Self-grdes re due Mrch 15, 2018, t 23:59. Sumission Formt Your homework sumission should

More information

#6A&B Magnetic Field Mapping

#6A&B Magnetic Field Mapping #6A& Mgnetic Field Mpping Gol y performing this lb experiment, you will: 1. use mgnetic field mesurement technique bsed on Frdy s Lw (see the previous experiment),. study the mgnetic fields generted by

More information

IMPORTANT. Read these directions carefully:

IMPORTANT. Read these directions carefully: Physics 208: Electricity nd Mgnetism Finl Exm, Secs. 506 510. 7 My. 2004 Instructor: Dr. George R. Welch, 415 Engineering-Physics, 845-7737 Print your nme netly: Lst nme: First nme: Sign your nme: Plese

More information

MORE FUNCTION GRAPHING; OPTIMIZATION. (Last edited October 28, 2013 at 11:09pm.)

MORE FUNCTION GRAPHING; OPTIMIZATION. (Last edited October 28, 2013 at 11:09pm.) MORE FUNCTION GRAPHING; OPTIMIZATION FRI, OCT 25, 203 (Lst edited October 28, 203 t :09pm.) Exercise. Let n be n rbitrry positive integer. Give n exmple of function with exctly n verticl symptotes. Give

More information

Today in Physics 122: work, energy and potential in electrostatics

Today in Physics 122: work, energy and potential in electrostatics Tody in Physics 1: work, energy nd potentil in electrosttics Leftovers Perfect conductors Fields from chrges distriuted on perfect conductors Guss s lw for grvity Work nd energy Electrosttic potentil energy,

More information

Phys 6321 Final Exam - Solutions May 3, 2013

Phys 6321 Final Exam - Solutions May 3, 2013 Phys 6321 Finl Exm - Solutions My 3, 2013 You my NOT use ny book or notes other thn tht supplied with this test. You will hve 3 hours to finish. DO YOUR OWN WORK. Express your nswers clerly nd concisely

More information

Resistors. Consider a uniform cylinder of material with mediocre to poor to pathetic conductivity ( )

Resistors. Consider a uniform cylinder of material with mediocre to poor to pathetic conductivity ( ) 10/25/2005 Resistors.doc 1/7 Resistors Consider uniform cylinder of mteril with mediocre to poor to r. pthetic conductivity ( ) ˆ This cylinder is centered on the -xis, nd hs length. The surfce re of the

More information

Electricity and Magnetism

Electricity and Magnetism PHY472 Dt Provided: Formul sheet nd physicl constnts Dt Provided: A formul sheet nd tble of physicl constnts is ttched to this pper. DEPARTMENT OF PHYSICS & Autumn Semester 2009-2010 ASTRONOMY DEPARTMENT

More information

- 5 - TEST 2. This test is on the final sections of this session's syllabus and. should be attempted by all students.

- 5 - TEST 2. This test is on the final sections of this session's syllabus and. should be attempted by all students. - 5 - TEST 2 This test is on the finl sections of this session's syllbus nd should be ttempted by ll students. Anything written here will not be mrked. - 6 - QUESTION 1 [Mrks 22] A thin non-conducting

More information

west (mrw3223) HW 24 lyle (16001) 1

west (mrw3223) HW 24 lyle (16001) 1 west (mrw3223) HW 24 lyle (16001) 1 This print-out should hve 30 questions. Multiple-choice questions my continue on the next column or pge find ll choices before nswering. Reding ssignment: Hecht, sections

More information

Physics Jonathan Dowling. Lecture 9 FIRST MIDTERM REVIEW

Physics Jonathan Dowling. Lecture 9 FIRST MIDTERM REVIEW Physics 10 Jonthn Dowling Physics 10 ecture 9 FIRST MIDTERM REVIEW A few concepts: electric force, field nd potentil Electric force: Wht is the force on chrge produced by other chrges? Wht is the force

More information

The Wave Equation I. MA 436 Kurt Bryan

The Wave Equation I. MA 436 Kurt Bryan 1 Introduction The Wve Eqution I MA 436 Kurt Bryn Consider string stretching long the x xis, of indeterminte (or even infinite!) length. We wnt to derive n eqution which models the motion of the string

More information

Solutions to Physics: Principles with Applications, 5/E, Giancoli Chapter 16 CHAPTER 16

Solutions to Physics: Principles with Applications, 5/E, Giancoli Chapter 16 CHAPTER 16 CHAPTER 16 1. The number of electrons is N = Q/e = ( 30.0 10 6 C)/( 1.60 10 19 C/electrons) = 1.88 10 14 electrons.. The mgnitude of the Coulomb force is Q /r. If we divide the epressions for the two forces,

More information

Physics 202, Lecture 14

Physics 202, Lecture 14 Physics 202, Lecture 14 Tody s Topics Sources of the Mgnetic Field (Ch. 28) Biot-Svrt Lw Ampere s Lw Mgnetism in Mtter Mxwell s Equtions Homework #7: due Tues 3/11 t 11 PM (4th problem optionl) Mgnetic

More information

Physics 9 Fall 2011 Homework 2 - Solutions Friday September 2, 2011

Physics 9 Fall 2011 Homework 2 - Solutions Friday September 2, 2011 Physics 9 Fll 0 Homework - s Fridy September, 0 Mke sure your nme is on your homework, nd plese box your finl nswer. Becuse we will be giving prtil credit, be sure to ttempt ll the problems, even if you

More information

Homework Assignment 3 Solution Set

Homework Assignment 3 Solution Set Homework Assignment 3 Solution Set PHYCS 44 6 Ferury, 4 Prolem 1 (Griffiths.5(c The potentil due to ny continuous chrge distriution is the sum of the contriutions from ech infinitesiml chrge in the distriution.

More information

Introduction to Electronic Circuits. DC Circuit Analysis: Transient Response of RC Circuits

Introduction to Electronic Circuits. DC Circuit Analysis: Transient Response of RC Circuits Introduction to Electronic ircuits D ircuit Anlysis: Trnsient esponse of ircuits Up until this point, we hve een looking t the Stedy Stte response of D circuits. StedyStte implies tht nothing hs chnged

More information

Math 124A October 04, 2011

Math 124A October 04, 2011 Mth 4A October 04, 0 Viktor Grigoryn 4 Vibrtions nd het flow In this lecture we will derive the wve nd het equtions from physicl principles. These re second order constnt coefficient liner PEs, which model

More information

ARITHMETIC OPERATIONS. The real numbers have the following properties: a b c ab ac

ARITHMETIC OPERATIONS. The real numbers have the following properties: a b c ab ac REVIEW OF ALGEBRA Here we review the bsic rules nd procedures of lgebr tht you need to know in order to be successful in clculus. ARITHMETIC OPERATIONS The rel numbers hve the following properties: b b

More information

SOLUTIONS TO CONCEPTS CHAPTER

SOLUTIONS TO CONCEPTS CHAPTER 1. m = kg S = 10m Let, ccelertion =, Initil velocity u = 0. S= ut + 1/ t 10 = ½ ( ) 10 = = 5 m/s orce: = = 5 = 10N (ns) SOLUIONS O CONCEPS CHPE 5 40000. u = 40 km/hr = = 11.11 m/s. 3600 m = 000 kg ; v

More information

EMF Notes 9; Electromagnetic Induction ELECTROMAGNETIC INDUCTION

EMF Notes 9; Electromagnetic Induction ELECTROMAGNETIC INDUCTION EMF Notes 9; Electromgnetic nduction EECTOMAGNETC NDUCTON (Y&F Chpters 3, 3; Ohnin Chpter 3) These notes cover: Motionl emf nd the electric genertor Electromgnetic nduction nd Frdy s w enz s w nduced electric

More information

Electromagnetic Potentials and Topics for Circuits and Systems

Electromagnetic Potentials and Topics for Circuits and Systems C H A P T E R 5 Electromgnetic Potentils nd Topics for Circuits nd Systems In Chpters 2, 3, nd 4, we introduced progressively Mxwell s equtions nd studied uniform plne wves nd ssocited topics. Two quntities

More information

Phys102 General Physics II

Phys102 General Physics II Phys1 Generl Physics II pcitnce pcitnce pcitnce definition nd exmples. Dischrge cpcitor irculr prllel plte cpcitior ylindricl cpcitor oncentric sphericl cpcitor Dielectric Sls 1 pcitnce Definition of cpcitnce

More information

PHYSICS ASSIGNMENT-9

PHYSICS ASSIGNMENT-9 MPS/PHY-XII-11/A9 PHYSICS ASSIGNMENT-9 *********************************************************************************************************** 1. A wire kept long the north-south direction is llowed

More information

Version 001 Exam 1 shih (57480) 1

Version 001 Exam 1 shih (57480) 1 Version 001 Exm 1 shih 57480) 1 This print-out should hve 6 questions. Multiple-choice questions my continue on the next column or pge find ll choices before nswering. Holt SF 17Rev 1 001 prt 1 of ) 10.0

More information

Math 8 Winter 2015 Applications of Integration

Math 8 Winter 2015 Applications of Integration Mth 8 Winter 205 Applictions of Integrtion Here re few importnt pplictions of integrtion. The pplictions you my see on n exm in this course include only the Net Chnge Theorem (which is relly just the Fundmentl

More information

Phys 4321 Final Exam December 14, 2009

Phys 4321 Final Exam December 14, 2009 Phys 4321 Finl Exm December 14, 2009 You my NOT use the text book or notes to complete this exm. You nd my not receive ny id from nyone other tht the instructor. You will hve 3 hours to finish. DO YOUR

More information

Hints for Exercise 1 on: Current and Resistance

Hints for Exercise 1 on: Current and Resistance Hints for Exercise 1 on: Current nd Resistnce Review the concepts of: electric current, conventionl current flow direction, current density, crrier drift velocity, crrier numer density, Ohm s lw, electric

More information

Jackson 2.7 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Jackson 2.7 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell Jckson.7 Homework Problem Solution Dr. Christopher S. Bird University of Msschusetts Lowell PROBLEM: Consider potentil problem in the hlf-spce defined by, with Dirichlet boundry conditions on the plne

More information

Math 5440 Problem Set 3 Solutions

Math 5440 Problem Set 3 Solutions Mth 544 Mth 544 Problem Set 3 Solutions Aron Fogelson Fll, 213 1: (Logn, 1.5 # 2) Repet the derivtion for the eqution of motion of vibrting string when, in ddition, the verticl motion is retrded by dmping

More information

Theoretische Physik 2: Elektrodynamik (Prof. A.-S. Smith) Home assignment 4

Theoretische Physik 2: Elektrodynamik (Prof. A.-S. Smith) Home assignment 4 WiSe 1 8.1.1 Prof. Dr. A.-S. Smith Dipl.-Phys. Ellen Fischermeier Dipl.-Phys. Mtthis Sb m Lehrstuhl für Theoretische Physik I Deprtment für Physik Friedrich-Alexnder-Universität Erlngen-Nürnberg Theoretische

More information

Instructor(s): Acosta/Woodard PHYSICS DEPARTMENT PHY 2049, Fall 2015 Midterm 1 September 29, 2015

Instructor(s): Acosta/Woodard PHYSICS DEPARTMENT PHY 2049, Fall 2015 Midterm 1 September 29, 2015 Instructor(s): Acost/Woodrd PHYSICS DEPATMENT PHY 049, Fll 015 Midterm 1 September 9, 015 Nme (print): Signture: On m honor, I hve neither given nor received unuthorized id on this emintion. YOU TEST NUMBE

More information

Math 5440 Problem Set 3 Solutions

Math 5440 Problem Set 3 Solutions Mth 544 Mth 544 Problem Set 3 Solutions Aron Fogelson Fll, 25 1: Logn, 1.5 # 2) Repet the derivtion for the eqution of motion of vibrting string when, in ddition, the verticl motion is retrded by dmping

More information

Math 520 Final Exam Topic Outline Sections 1 3 (Xiao/Dumas/Liaw) Spring 2008

Math 520 Final Exam Topic Outline Sections 1 3 (Xiao/Dumas/Liaw) Spring 2008 Mth 520 Finl Exm Topic Outline Sections 1 3 (Xio/Dums/Liw) Spring 2008 The finl exm will be held on Tuesdy, My 13, 2-5pm in 117 McMilln Wht will be covered The finl exm will cover the mteril from ll of

More information

13.4 Work done by Constant Forces

13.4 Work done by Constant Forces 13.4 Work done by Constnt Forces We will begin our discussion of the concept of work by nlyzing the motion of n object in one dimension cted on by constnt forces. Let s consider the following exmple: push

More information

Chapter E - Problems

Chapter E - Problems Chpter E - Prolems Blinn College - Physics 2426 - Terry Honn Prolem E.1 A wire with dimeter d feeds current to cpcitor. The chrge on the cpcitor vries with time s QHtL = Q 0 sin w t. Wht re the current

More information

Lecture 5 Capacitance Ch. 25

Lecture 5 Capacitance Ch. 25 Lecture 5 pcitnce h. 5 rtoon - pcitnce definition nd exmples. Opening Demo - Dischrge cpcitor Wrm-up prolem Physlet Topics pcitnce Prllel Plte pcitor Dielectrics nd induced dipoles oxil cle, oncentric

More information

Conservation Law. Chapter Goal. 5.2 Theory

Conservation Law. Chapter Goal. 5.2 Theory Chpter 5 Conservtion Lw 5.1 Gol Our long term gol is to understnd how mny mthemticl models re derived. We study how certin quntity chnges with time in given region (sptil domin). We first derive the very

More information

Crystalline Structures The Basics

Crystalline Structures The Basics Crystlline Structures The sics Crystl structure of mteril is wy in which toms, ions, molecules re sptilly rrnged in 3-D spce. Crystl structure = lttice (unit cell geometry) + bsis (tom, ion, or molecule

More information

potentials A z, F z TE z Modes We use the e j z z =0 we can simply say that the x dependence of E y (1)

potentials A z, F z TE z Modes We use the e j z z =0 we can simply say that the x dependence of E y (1) 3e. Introduction Lecture 3e Rectngulr wveguide So fr in rectngulr coordintes we hve delt with plne wves propgting in simple nd inhomogeneous medi. The power density of plne wve extends over ll spce. Therefore

More information

Last Time emphasis on E-field. Potential of spherical conductor. Quick quiz. Connected spheres. Varying E-fields on conductor.

Last Time emphasis on E-field. Potential of spherical conductor. Quick quiz. Connected spheres. Varying E-fields on conductor. Lst Time emphsis on Efiel Electric flux through surfce Guss lw: Totl electric flux through close surfce proportionl to chrge enclose Q " E = E = 4$k e Q % o Chrge istribution on conuctors Chrge ccumultes

More information

SUMMER KNOWHOW STUDY AND LEARNING CENTRE

SUMMER KNOWHOW STUDY AND LEARNING CENTRE SUMMER KNOWHOW STUDY AND LEARNING CENTRE Indices & Logrithms 2 Contents Indices.2 Frctionl Indices.4 Logrithms 6 Exponentil equtions. Simplifying Surds 13 Opertions on Surds..16 Scientific Nottion..18

More information

Special Relativity solved examples using an Electrical Analog Circuit

Special Relativity solved examples using an Electrical Analog Circuit 1-1-15 Specil Reltivity solved exmples using n Electricl Anlog Circuit Mourici Shchter mourici@gmil.com mourici@wll.co.il ISRAE, HOON 54-54855 Introduction In this pper, I develop simple nlog electricl

More information

Improper Integrals, and Differential Equations

Improper Integrals, and Differential Equations Improper Integrls, nd Differentil Equtions October 22, 204 5.3 Improper Integrls Previously, we discussed how integrls correspond to res. More specificlly, we sid tht for function f(x), the region creted

More information

Homework Assignment 5 Solution Set

Homework Assignment 5 Solution Set Homework Assignment 5 Solution Set PHYCS 44 3 Februry, 4 Problem Griffiths 3.8 The first imge chrge gurntees potentil of zero on the surfce. The secon imge chrge won t chnge the contribution to the potentil

More information

7.1 Integral as Net Change and 7.2 Areas in the Plane Calculus

7.1 Integral as Net Change and 7.2 Areas in the Plane Calculus 7.1 Integrl s Net Chnge nd 7. Ares in the Plne Clculus 7.1 INTEGRAL AS NET CHANGE Notecrds from 7.1: Displcement vs Totl Distnce, Integrl s Net Chnge We hve lredy seen how the position of n oject cn e

More information

WELCOME TO THE LECTURE

WELCOME TO THE LECTURE WELCOME TO THE LECTURE ON DC MOTOR Force on conductor If conductor is plced in mgnetic field nd current is llowed to flow through the conductor, the conductor will experience mechnicl force. N S Electric

More information

Homework Assignment 6 Solution Set

Homework Assignment 6 Solution Set Homework Assignment 6 Solution Set PHYCS 440 Mrch, 004 Prolem (Griffiths 4.6 One wy to find the energy is to find the E nd D fields everywhere nd then integrte the energy density for those fields. We know

More information

10 Vector Integral Calculus

10 Vector Integral Calculus Vector Integrl lculus Vector integrl clculus extends integrls s known from clculus to integrls over curves ("line integrls"), surfces ("surfce integrls") nd solids ("volume integrls"). These integrls hve

More information

PART 1 MULTIPLE CHOICE Circle the appropriate response to each of the questions below. Each question has a value of 1 point.

PART 1 MULTIPLE CHOICE Circle the appropriate response to each of the questions below. Each question has a value of 1 point. PART MULTIPLE CHOICE Circle the pproprite response to ech of the questions below. Ech question hs vlue of point.. If in sequence the second level difference is constnt, thn the sequence is:. rithmetic

More information

Consequently, the temperature must be the same at each point in the cross section at x. Let:

Consequently, the temperature must be the same at each point in the cross section at x. Let: HW 2 Comments: L1-3. Derive the het eqution for n inhomogeneous rod where the therml coefficients used in the derivtion of the het eqution for homogeneous rod now become functions of position x in the

More information

Hung problem # 3 April 10, 2011 () [4 pts.] The electric field points rdilly inwrd [1 pt.]. Since the chrge distribution is cylindriclly symmetric, we pick cylinder of rdius r for our Gussin surfce S.

More information

Physics 121 Sample Common Exam 1 NOTE: ANSWERS ARE ON PAGE 8. Instructions:

Physics 121 Sample Common Exam 1 NOTE: ANSWERS ARE ON PAGE 8. Instructions: Physics 121 Smple Common Exm 1 NOTE: ANSWERS ARE ON PAGE 8 Nme (Print): 4 Digit ID: Section: Instructions: Answer ll questions. uestions 1 through 16 re multiple choice questions worth 5 points ech. You

More information

( dg. ) 2 dt. + dt. dt j + dh. + dt. r(t) dt. Comparing this equation with the one listed above for the length of see that

( dg. ) 2 dt. + dt. dt j + dh. + dt. r(t) dt. Comparing this equation with the one listed above for the length of see that Arc Length of Curves in Three Dimensionl Spce If the vector function r(t) f(t) i + g(t) j + h(t) k trces out the curve C s t vries, we cn mesure distnces long C using formul nerly identicl to one tht we

More information

Math 116 Calculus II

Math 116 Calculus II Mth 6 Clculus II Contents 5 Exponentil nd Logrithmic functions 5. Review........................................... 5.. Exponentil functions............................... 5.. Logrithmic functions...............................

More information

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics Solid Stte Physics JEST-0 Q. bem of X-rys is incident on BCC crystl. If the difference between the incident nd scttered wvevectors is K nxˆkyˆlzˆ where xˆ, yˆ, zˆ re the unit vectors of the ssocited cubic

More information

P812 Midterm Examination February Solutions

P812 Midterm Examination February Solutions P8 Midterm Exmintion Februry s. A one dimensionl chin of chrges consist of e nd e lterntively plced with neighbouring distnce. Show tht the potentil energy of ech chrge is given by U = ln. 4πε Explin qulittively

More information

Physics Lecture 14: MON 29 SEP

Physics Lecture 14: MON 29 SEP Physics 2113 Physics 2113 Lecture 14: MON 29 SEP CH25: Cpcitnce Von Kleist ws le to store electricity in the jr. Unknowingly, he h ctully invente novel evice to store potentil ifference. The wter in the

More information

Flow in porous media

Flow in porous media Red: Ch 2. nd 2.2 PART 4 Flow in porous medi Drcy s lw Imgine point (A) in column of wter (figure below); the point hs following chrcteristics: () elevtion z (2) pressure p (3) velocity v (4) density ρ

More information