( ) ( ) ( ) ( ) ( ) # B x ( ˆ i ) ( ) # B y ( ˆ j ) ( ) # B y ("ˆ ( ) ( ) ( (( ) # ("ˆ ( ) ( ) ( ) # B ˆ z ( k )
|
|
- Julianna Gibson
- 5 years ago
- Views:
Transcription
1 Emple 1: A positie chge with elocit is moing though unifom mgnetic field s shown in the figues below. Use the ight-hnd ule to detemine the diection of the mgnetic foce on the chge. Emple 1 ˆ i = ˆ ˆ i = ˆ ˆ = ˆ i ˆ = ˆ i ˆ ˆ i = ˆ i ˆ = ˆ i ˆ i = = ˆ ˆ = ˆ i ˆ F M = q ˆ i F M = q ˆ i F M = q ˆ F M = q ˆ j ˆ j z o out F M = q ˆ i ˆ i F M = q ˆ i ˆ i ˆ i F M = q ˆ F M = q ˆ z o in 1 Emple 1 F M = q z ˆ F M = q z ˆ F M = q z ˆ i o left F M = q F M F M = q ˆ i z ˆ F M = q z ˆ i ˆ F M = q z z ˆ z ˆ i F M = q z ˆ i q z Emple : A negtie chge with elocit is moing though unifom mgnetic field s shown in the figues below. Use the ight-hnd ule to detemine the diection of the mgnetic foce on the chge. Qudnt to nd 3 4 Emple F M = q Emple F M = q F M = q ˆ z F M = q z ˆ F M = q z ˆ i F M = q z ˆ i o left F M = q z ˆ ˆ i F M = q z ˆ ˆ i F M = q z ˆ j F M = q z o up F M = q F M = q F M = q F M = No foce F M = q ˆ i F M = q z ˆ i z ˆ ˆ z ˆ j z ˆ i F M = q z ˆ i q z F M = q z ˆ Qudnt F M to nd 5 6
2 Emple 3: A bem of potons moes t m/s though unifom mgnetic field with mgnitude T tht is diected long the positie z-is. The elocit of ech poton lies in the z-plne t n ngle of 3 to the z-is. Find the foce on the poton. 7 Emple 3 q = C, = 31 5 m z - plne 3 wt z - is s = Tˆ, F M =? = ˆ i z ˆ = sin ˆ i cos ˆ = 3 z F M = q F M = q sin ˆ i cos ˆ F M = q sin F M = q sin ˆ ˆ i ˆ cos ˆ ˆ ˆ j cos F M = q sin ˆ j 31 5 m F M = C F M = N ˆ j s sin3 T o in F M = q = qsin F M = C 31 5 m F M = N Tsin3 s 8 Emple 4: q A pticle with chge of e nd mss of g entes mgnitude field with mgnitude of 4 T s shown in the figue boe. The speed of the pticle is m/s. Dw the pth of the pticle s it moes though the field. b. Find the dius of the pth. 9 Emple 4 q = C, m = 31 7 g, = m s ˆ i, = 4 T ˆ q. th of pticle F M = q = qˆ i ˆ = q ˆ i ˆ = q The initil foce is upwds nd the pticle continues in cicul pth. b. =? F M = q = m = m = m 31 7 g m q = s = m C 4 T 1 Emple 5:!V = V - - -e - - An electon cceletes fom est though potentil diffeence of V nd then entes mgnetic field with stength of.5 T.. b. c. Wht is the speed of the electon just befoe it entes the mgnetic field? Wht is the foce on the electon s it moes though the field? Descibe the pth of the electon s it moes though the field. 11 Emple 5 q = C, m = g, V = V, =.5 Tˆ!V = V F M = q - F M = eˆ i ˆ - F -e M = e ˆ i ˆ - F M = eˆ j F M = e -. =? b. F M =? K = U = qv F M = q = K K 1 = qv F M = qsin = q 1 m = qv F M = m m.5 T s s qv = C V F M = N m g c. Descible pth = m Cicul pth upwd. 1 s
3 Emple 6: A stight hoizontl wie cies cuent of 5 A fom west to est in egion whee thee is hoizontl mgnetic field towd the nothest with mgnitude of 1. T nd ngle 45. Find the mgnitude nd diection of the foce on 1 m section of the wie. Emple 6 = 5 A, l = 1 m, = 1. T45, F =? F = d l fo unifom - fields F = l F = lˆ i ˆ i F = l ˆ i ˆ i ˆ i F = l ˆ F = l ˆ = l sin ˆ F = 5 A 1 m 1. T sin45 ˆ F = 4.4 Nˆ lso F = l = lsin F = 5 A 1 m 1. T sin45 13 F F = 4.4 N 14 Emple 7:! L A conducto with stight segment of length L pependicul to the -plne, followed b semicicle section of dius, nd finll stight segment with length L pllel to the - is cies cuent in mgnetic field diected in the positie z diection. Find the totl mgnetic foce on the conducto. 15 Emple 7 df = d l d l = d ˆ l nd = ˆ ˆ l = cos ˆ i sin ˆ j ˆ l = sinˆ i cos d l d l = d sinˆ i cos ˆ df = d sinˆ i cos df df = d sinˆ i ˆ d cos ˆ 16 Emple 7 df = d sinˆ i ˆ d cos ˆ Emple 7 df = sind ˆ i ˆ df = sind cosd ˆ cosd ˆ i F = sind cosd ˆ i F = cos ] sin ˆ i ] F = cos cos F = 11 F = sin sin ˆ i ˆ i ˆ i = 17 L d F d l F = Thee is onl - componet due to smmet. The foce on the stight section of length L is : F = L = Lˆ i ˆ = L ˆ i ˆ The totl foce on the wie is : F = L ˆ j = L d l df 18
4 Emple 7 Emple 7 d F = d l df = dlsin = dlsin9 = dl = d df = dfcos = dcos = cosd df = dfsin = dsin = sind d df l df df 19 df = cosd F = cosd F = sin] F = sin sin F = df = sind F = sind F = cos] d df l df df F = cos cos F = Emple 8: Emple 8 =.5 m = 5 A = 1. T =.5 m = 5 A =.5 m, N = 3 tuns, = 5 A, = 1. T, =? = 1. T A cicul coil.5 m in dius, with 3 tuns of wie, lies in hoizontl plne. t cies cuent of 5 A in the counteclocwise sense when iewed fom boe. The coil is in unifom mgnetic field diected towd the ight, with mgnitude 1. T. Find the toque on the coil. = NAsin = 3 5 A 1. T.5 m sin9 = 1.41 N m 1 Emple 9: q 1.3 m 1.4 m q A pi of point chges, q 1 = 5 µc nd q = -3 µc, e moing s shown boe with speed 1 = m/s nd = m/s. At this instnt find. the mgnetic field poduced t the oigin b. the mgnetic foce tht q 1 eets on q Emple 9 1 = m q s ˆ i 1 = 51 6 C 1 =.3 mˆ j ˆ 1 = 1 =.3 mˆ j 1.3 m = 1 = µ o q 1 1 ˆ T 51-6 C m A* 1 =.3 m m s * ˆ i 1 = T ˆ i = T ˆ 3 4
5 Emple 9 =.4 mˆ i q = 31 6 C = µ o q ˆ ˆ = ˆ i 1 7 T 31-6 C m A* =.4 m = T = m s m ˆ ˆ i = T s * ˆ i Emple 9 Emple 9b o = 1 = Tˆ Tˆ o = Tˆ q =.4 mˆ i.3 mˆ j.3 m.4 m 1 = q ˆ 1 = 1 =.3 mˆ i.3 mˆ j 1.5 m.4 m.3 m =.5 m =.8ˆ i Emple 9b 1 = µ o q 1 1 ˆ 1 1 Emple 1: 1 7 T C m A* 1 = F,1 = 31-6 C m 1 = Tˆ F,1 = q m F,1 = Nˆ i ˆ i.8ˆ i.6 s *.5 m Tˆ s 7 - A stight eticl conducto ling on the - is cies cuent fom = - to =. Find the stength nd diection of the mgnetic field fo point which lies on the -is. 8 Emple 1 d l = d = ˆ i = - ˆ = = ˆ i Emple 1 = µ d ˆ 3 Fom integl tbles: = µ d = C 3 d ˆ 3 1 = µ d l ˆ = µ d l = µ ˆ 3 3 = µ d i µ = ˆ i d 3 d ˆ 3 j ˆ i ˆ 9 = µ 1 ˆ = µ = µ ˆ ˆ 3
6 Emple 1 = µ fo >>, = nd = µ = µ infinitel long wie Emple 1 d l - = µ = d l ˆ = µ d l ˆ sin = µ = µ d 3 d Emple 11: Two long, stight, pllel wies pependicul to the plne, ech c cuent but in opposite diections.. b. 1 3d Wie Wie 1 X d d Find the mgnitude nd diection of the mgnetic field t points 1,, nd 3. Find the mgnitude nd diection of the mgnetic field t n point on the -is to the ight of wie in tems of the -coodinte of the point. d 3 Emple = d Wie Wie 1 X 1 = 4d 1 = 1 1 = µ µ 1 1 = µ 4d µ d 1 = µ 8d µ d 1 = µ 8d Emple 11 1 Wie Wie 1 X = d 1 = d = 1 = µ µ 1 = µ d µ d = µ d Wie Wie 1 X 3 1 = d = 3d 3 = 1 3 = µ 1 3 = µ d µ 3 = µ 3d µ 3d 3 = µ d µ 6d 35 1 Emple 11b Wie Wie 1 X d d 1 = d = d = 1 = µ 1 µ = d µ µ d = µ 1 d 1 d 1 = µ d d d = µ d d = µ d d 36
7 Emple 1: Two long wies pependicul to the -is c cuents of.4 A s shown below. oint 1 is locted t the oigin which is hlfw between the wies nd point is on the -is.3 m below the oigin. Find the mgnitude nd diection of the mgnetic field t points 1 nd m.3 m 37 Emple = =.4 m, 1 = =.4 A, 1 =? = T m.4 A A * 1 =.4 m * 1 = T j o 1 = T 7 ˆ 1 = µ = = 1 38 Emple 1 1 = =.5 m, 1 = =.4 A, =? 1.3 m 1.4 m =.5 m Emple 1 oth cuents out of the pge 1 =? = 1 = 1 = = sin 1 = 1 = = µ 1 7 T m.4 A sin A *.4 m = = T.5 m.5 m* * = Emple 1 oth cuents out of the pge 1 1 =.5 m Emple 13: Two stight, pllel, conducting cbles e 4.5 mm pt nd ech c cuent of 15, A in opposite diections. Find the foce between the cbles. = 1 = 1 = 1 cos 1 = µ o 1 7 T m.4 A 1 cos A *.3 m 1 = = T 1.5 m.5 m* * = 41 4
8 Emple 13 d = 4.5 mm, 1 = = 15, A in opposite diections, F l =? F,1 = 1 l ˆ F,1 = 1 l ˆ j F,1 = 1 l ˆ F,1 = 1 l ˆ i F,1 l = µ 1 d ˆ i d 1 = µ 1 = d = d 1 = µ T m 15, A 15, A A * F 1, = F,1 = = 1, N m m F 1, = l 1 F 1, = lˆ 1 F 1, = l 1 ˆ F 1, = l 1ˆ i F 1, l = µ 1 d ˆ i 43 Mgnetic field t the cente of single loop of cuent cing wie. = µ d 1sin9 = µ = µ d l ˆ A = Asin dl ˆ sin d l = d ˆ l dl = d d l = µ d µ = = µ = µ 44 Emple 14: d l = d ˆ Emple 14 = ˆ i sin cos ˆ z A cicul conducting loop with dius cies cuent. The loop lies in the z-plne t the oigin of the -is. Find the mgnetic field t point tht lies long the -is. z = d l d = cos sin ˆ d l d d l = d ˆ d l = d ˆ Emple 14 We he smmet nd -components cncel nd -components dd. dl = d - = µ = d l ˆ = µ d 1 1 cos Emple 14 = µ = µ d dl ˆ sin9 47 = µ d = µ 3 3 d 48
9 Emple 14 = µ 3 = µ 3 d Mgnetic Field of Cicul Loop = µ = µ 3 = = µ = µ 3 3 ˆ i on the is of cicul loop 49 5 Emple 15: Use Ampees Lw to deie the mgnetic field. A distnce fom long stight wie cing cuent. b. At the cente of solenoid with length L with N tuns cing cuent. c. A long clindicl conducto of dius cing unifom cuent. d. A long clindicl conducto of dius cing cuent whose cuent densit J is nonunifom nd ies s J = b, whee b is constnt nd is mesued fom the centl is of the clinde. 51 Emple 15 Long wie cing cuent d l = µ enc dl = µ = µ = µ d l 5 Emple 15b Solenoid of length L with N tuns cing cuent = d l Emple 15c Long clindicl conducto of dius cing unifom cuent d l < d l = µ enc dl = µ enc d l = µ enc = µ n s = µ n n = N numbe of tuns = L totl length = µ JA = µ = µ < 53 54
10 Emple 15c Long clindicl conducto of dius cing unifom cuent Emple 15c Long clindicl conducto of dius cing unifom cuent d l > = µ < = µ > d l = µ enc = µ dl = µ enc 1 = µ = µ > = Emple 15d Long clindicl conducto of dius cing cuent tht ies s J = b J = b enc = J da A = da = d enc = b d = b 3 d enc = b 4 = b 4 = so b = 4 enc = 4 4 < < Emple 15d Long clindicl conducto of dius cing cuent tht ies s J = b d l enc = 4 4 d l = µ enc dl = µ enc = µ 4 4 = µ 3 4 < < Emple 15d Long clindicl conducto of dius cing cuent tht ies s J = b d l enc = > d l = µ enc dl = µ enc = µ = µ Emple 15d Long clindicl conducto of dius cing 3 cuent tht ies s J = b = µ 3 4 < = µ 1 > = µ > = 59 6
(A) 6.32 (B) 9.49 (C) (D) (E) 18.97
Univesity of Bhin Physics 10 Finl Exm Key Fll 004 Deptment of Physics 13/1/005 8:30 10:30 e =1.610 19 C, m e =9.1110 31 Kg, m p =1.6710 7 Kg k=910 9 Nm /C, ε 0 =8.8410 1 C /Nm, µ 0 =4π10 7 T.m/A Pt : 10
More informationChapter 28 Sources of Magnetic Field
Chpte 8 Souces of Mgnetic Field - Mgnetic Field of Moving Chge - Mgnetic Field of Cuent Element - Mgnetic Field of Stight Cuent-Cying Conducto - Foce Between Pllel Conductos - Mgnetic Field of Cicul Cuent
More informationExample 2: ( ) 2. $ s ' 9.11" 10 *31 kg ( )( 1" 10 *10 m) ( e)
Emple 1: Two point chge e locted on the i, q 1 = e t = 0 nd q 2 = e t =.. Find the wok tht mut be done b n etenl foce to bing thid point chge q 3 = e fom infinit to = 2. b. Find the totl potentil eneg
More informationMAGNETIC EFFECT OF CURRENT & MAGNETISM
TODUCTO MAGETC EFFECT OF CUET & MAGETM The molecul theo of mgnetism ws given b Webe nd modified lte b Ewing. Oested, in 18 obseved tht mgnetic field is ssocited with n electic cuent. ince, cuent is due
More informationCourse Updates. Reminders: 1) Assignment #8 available. 2) Chapter 28 this week.
Couse Updtes http://www.phys.hwii.edu/~vne/phys7-sp1/physics7.html Remindes: 1) Assignment #8 vilble ) Chpte 8 this week Lectue 3 iot-svt s Lw (Continued) θ d θ P R R θ R d θ d Mgnetic Fields fom long
More informationELECTRO - MAGNETIC INDUCTION
NTRODUCTON LCTRO - MAGNTC NDUCTON Whenee mgnetic flu linked with cicuit chnges, n e.m.f. is induced in the cicuit. f the cicuit is closed, cuent is lso induced in it. The e.m.f. nd cuent poduced lsts s
More information1. The sphere P travels in a straight line with speed
1. The sphee P tels in stight line with speed = 10 m/s. Fo the instnt depicted, detemine the coesponding lues of,,,,, s mesued eltie to the fixed Oxy coodinte system. (/134) + 38.66 1.34 51.34 10sin 3.639
More informationPhysics 11b Lecture #11
Physics 11b Lectue #11 Mgnetic Fields Souces of the Mgnetic Field S&J Chpte 9, 3 Wht We Did Lst Time Mgnetic fields e simil to electic fields Only diffeence: no single mgnetic pole Loentz foce Moving chge
More informationSolutions to Midterm Physics 201
Solutions to Midtem Physics. We cn conside this sitution s supeposition of unifomly chged sphee of chge density ρ nd dius R, nd second unifomly chged sphee of chge density ρ nd dius R t the position of
More informationMAGNETIC FIELD INTRODUCTION
MAGNETIC FIELD INTRODUCTION It was found when a magnet suspended fom its cente, it tends to line itself up in a noth-south diection (the compass needle). The noth end is called the Noth Pole (N-pole),
More informationThis immediately suggests an inverse-square law for a "piece" of current along the line.
Electomgnetic Theoy (EMT) Pof Rui, UNC Asheville, doctophys on YouTube Chpte T Notes The iot-svt Lw T nvese-sque Lw fo Mgnetism Compe the mgnitude of the electic field t distnce wy fom n infinite line
More informationU>, and is negative. Electric Potential Energy
Electic Potentil Enegy Think of gvittionl potentil enegy. When the lock is moved veticlly up ginst gvity, the gvittionl foce does negtive wok (you do positive wok), nd the potentil enegy (U) inceses. When
More informationCollection of Formulas
Collection of Fomuls Electomgnetic Fields EITF8 Deptment of Electicl nd Infomtion Technology Lund Univesity, Sweden August 8 / ELECTOSTATICS field point '' ' Oigin ' Souce point Coulomb s Lw The foce F
More informationSection 35 SHM and Circular Motion
Section 35 SHM nd Cicul Motion Phsics 204A Clss Notes Wht do objects do? nd Wh do the do it? Objects sometimes oscillte in simple hmonic motion. In the lst section we looed t mss ibting t the end of sping.
More informationWinter 2004 OSU Sources of Magnetic Fields 1 Chapter 32
Winte 4 OSU 1 Souces Of Mgnetic Fields We lened two wys to clculte Electic Field Coulomb's Foce de 4 E da 1 dq Q enc ˆ ute Foce Clcultion High symmety Wht e the nlogous equtions fo the Mgnetic Field? Winte
More informationChapter 21: Electric Charge and Electric Field
Chpte 1: Electic Chge nd Electic Field Electic Chge Ancient Gees ~ 600 BC Sttic electicit: electic chge vi fiction (see lso fig 1.1) (Attempted) pith bll demonsttion: inds of popeties objects with sme
More information858 Questions 1. O (iii) (iv) 11. O 2. O (i) (ii) 12. O 3. O (i) 13. (ii) 14. O 5. O 6. O 15. O O (i) (ii)
858 Chpte 30 Souces of the Mgnetic Field Questions denotes nswe vilble in Student Solutions Mnul/Stud Guide; O denotes objective question 1. O Wht cetes mgnetic field? Choose eve coect nswe. () sttion
More informationPhysics 1502: Lecture 2 Today s Agenda
1 Lectue 1 Phsics 1502: Lectue 2 Tod s Agend Announcements: Lectues posted on: www.phs.uconn.edu/~cote/ HW ssignments, solutions etc. Homewok #1: On Mstephsics this Fid Homewoks posted on Msteingphsics
More informationChapter 4 Two-Dimensional Motion
D Kinemtic Quntities Position nd Velocit Acceletion Applictions Pojectile Motion Motion in Cicle Unifom Cicul Motion Chpte 4 Two-Dimensionl Motion D Motion Pemble In this chpte, we ll tnsplnt the conceptul
More informationChapter 4 Kinematics in Two Dimensions
D Kinemtic Quntities Position nd Velocit Acceletion Applictions Pojectile Motion Motion in Cicle Unifom Cicul Motion Chpte 4 Kinemtics in Two Dimensions D Motion Pemble In this chpte, we ll tnsplnt the
More informationCHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD
ollege Physics Student s Mnul hpte 8 HAPTR 8: LTRI HARG AD LTRI ILD 8. STATI LTRIITY AD HARG: OSRVATIO O HARG. ommon sttic electicity involves chges nging fom nnocoulombs to micocoulombs. () How mny electons
More informationChapter 2: Electric Field
P 6 Genel Phsics II Lectue Outline. The Definition of lectic ield. lectic ield Lines 3. The lectic ield Due to Point Chges 4. The lectic ield Due to Continuous Chge Distibutions 5. The oce on Chges in
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 4 Due on Sep. 1, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt
More informationELECTROSTATICS. 4πε0. E dr. The electric field is along the direction where the potential decreases at the maximum rate. 5. Electric Potential Energy:
LCTROSTATICS. Quntiztion of Chge: Any chged body, big o smll, hs totl chge which is n integl multile of e, i.e. = ± ne, whee n is n intege hving vlues,, etc, e is the chge of electon which is eul to.6
More informationPX3008 Problem Sheet 1
PX38 Poblem Sheet 1 1) A sphee of dius (m) contins chge of unifom density ρ (Cm -3 ). Using Guss' theoem, obtin expessions fo the mgnitude of the electic field (t distnce fom the cente of the sphee) in
More informationPhysics Spring 2012 Announcements: Mar 07, 2012
Physics 00 - Sping 01 Announcements: Ma 07, 01 HW#6 due date has been extended to the moning of Wed. Ma 1. Test # (i. Ma ) will cove only chaptes 0 and 1 All of chapte will be coveed in Test #4!!! Test
More information+ r Position Velocity
1. The phee P tel in tight line with contnt peed of =100 m/. Fo the intnt hown, detemine the coeponding lue of,,,,, eltie to the fixed Ox coodinte tem. meued + + Poition Velocit e 80 e 45 o 113. 137 d
More informationElectric Potential. and Equipotentials
Electic Potentil nd Euipotentils U Electicl Potentil Review: W wok done y foce in going fom to long pth. l d E dl F W dl F θ Δ l d E W U U U Δ Δ l d E W U U U U potentil enegy electic potentil Potentil
More informationA moving charged particle creates a magnetic field vector at every point in space except at its position.
1 Pat 3: Magnetic Foce 3.1: Magnetic Foce & Field A. Chaged Paticles A moving chaged paticle ceates a magnetic field vecto at evey point in space ecept at its position. Symbol fo Magnetic Field mks units
More information1. Viscosities: μ = ρν. 2. Newton s viscosity law: 3. Infinitesimal surface force df. 4. Moment about the point o, dm
3- Fluid Mecnics Clss Emple 3: Newton s Viscosit Lw nd Se Stess 3- Fluid Mecnics Clss Emple 3: Newton s Viscosit Lw nd Se Stess Motition Gien elocit field o ppoimted elocit field, we wnt to be ble to estimte
More information( ) ( )( ) ˆ. Homework #8. Chapter 27 Magnetic Fields II.
Homewok #8. hapte 7 Magnetic ields. 6 Eplain how ou would modif Gauss s law if scientists discoveed that single, isolated magnetic poles actuall eisted. Detemine the oncept Gauss law fo magnetism now eads
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 3 Due on Sep. 14, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt
More informationAnswers to test yourself questions
Answes to test youself questions opic Descibing fields Gm Gm Gm Gm he net field t is: g ( d / ) ( 4d / ) d d Gm Gm Gm Gm Gm Gm b he net potentil t is: V d / 4d / d 4d d d V e 4 7 9 49 J kg 7 7 Gm d b E
More informationAPEX CARE INSTITUTE FOR TRB, SLET AND NET IN PHYSICS ELECTROMAGNETIC THEORY- SLET / NET QUESTION BANK
www.tbtnpsc.com ELECTROMAGNETC THEORY- SLET / NET QUESTON BANK. The electosttic potentil V(, ) in fee spce in egion whee the chge densit ρ is eo is given b V, e f. Given tht the -component of the electic
More informationMagnetic fields (origins) CHAPTER 27 SOURCES OF MAGNETIC FIELD. Permanent magnets. Electric currents. Magnetic field due to a moving charge.
Magnetic fields (oigins) CHAPTER 27 SOURCES OF MAGNETC FELD Magnetic field due to a moving chage. Electic cuents Pemanent magnets Magnetic field due to electic cuents Staight wies Cicula coil Solenoid
More informationPhysics 604 Problem Set 1 Due Sept 16, 2010
Physics 64 Polem et 1 Due ept 16 1 1) ) Inside good conducto the electic field is eo (electons in the conducto ecuse they e fee to move move in wy to cncel ny electic field impessed on the conducto inside
More informationr a + r b a + ( r b + r c)
AP Phsics C Unit 2 2.1 Nme Vectos Vectos e used to epesent quntities tht e chcteized b mgnitude ( numeicl vlue with ppopite units) nd diection. The usul emple is the displcement vecto. A quntit with onl
More informationMagnetic Field of a Wire
Magnetic Field of a Wie Fundamental Laws fo Calculating B-field Biot-Savat Law (long method, but woks always) Ampee s Law (high symmety) B-Field of a Staight Wie Fo a thin staight conducto caying cuent
More information13.5. Torsion of a curve Tangential and Normal Components of Acceleration
13.5 osion of cuve ngentil nd oml Components of Acceletion Recll: Length of cuve '( t) Ac length function s( t) b t u du '( t) Ac length pmetiztion ( s) with '( s) 1 '( t) Unit tngent vecto '( t) Cuvtue:
More information( )( )( ) ( ) + ( ) ( ) ( )
3.7. Moel: The magnetic fiel is that of a moving chage paticle. Please efe to Figue Ex3.7. Solve: Using the iot-savat law, 7 19 7 ( ) + ( ) qvsinθ 1 T m/a 1.6 1 C. 1 m/s sin135 1. 1 m 1. 1 m 15 = = = 1.13
More informationEinstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : ,
PE ELECTOSTATICS C Popeties of chges : (i) (ii) (iii) (iv) (v) (vi) Two kinds of chges eist in ntue, positive nd negtive with the popety tht unlike chges ttct ech othe nd like chges epel ech othe. Ecess
More informationr = (0.250 m) + (0.250 m) r = m = = ( N m / C )
ELECTIC POTENTIAL IDENTIFY: Apply Eq() to clculte the wok The electic potentil enegy of pi of point chges is given y Eq(9) SET UP: Let the initil position of q e point nd the finl position e point, s shown
More informationGeneral Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface
Genel Physics II Chpte 3: Guss w We now wnt to quickly discuss one of the moe useful tools fo clculting the electic field, nmely Guss lw. In ode to undestnd Guss s lw, it seems we need to know the concept
More information1 Using Integration to Find Arc Lengths and Surface Areas
Novembe 9, 8 MAT86 Week Justin Ko Using Integtion to Find Ac Lengths nd Sufce Aes. Ac Length Fomul: If f () is continuous on [, b], then the c length of the cuve = f() on the intevl [, b] is given b s
More informationChapter 22 The Electric Field II: Continuous Charge Distributions
Chpte The lectic Field II: Continuous Chge Distibutions Conceptul Poblems [SSM] Figue -7 shows n L-shped object tht hs sides which e equl in length. Positive chge is distibuted unifomly long the length
More informationUnit 6. Magnetic forces
Unit 6 Mgnetic foces 6.1 ntoduction. Mgnetic field 6. Mgnetic foces on moving electic chges 6. oce on conducto with cuent. 6.4 Action of unifom mgnetic field on flt cuent-cying loop. Mgnetic moment. Electic
More informationPhysics 122, Fall October 2012
hsics 1, Fall 1 3 Octobe 1 Toda in hsics 1: finding Foce between paallel cuents Eample calculations of fom the iot- Savat field law Ampèe s Law Eample calculations of fom Ampèe s law Unifom cuents in conductos?
More information21 MAGNETIC FORCES AND MAGNETIC FIELDS
CHAPTER 1 MAGNETIC ORCES AND MAGNETIC IELDS ANSWERS TO OCUS ON CONCEPTS QUESTIONS 1. (d) Right-Hand Rule No. 1 gives the diection of the magnetic foce as x fo both dawings A and. In dawing C, the velocity
More information3.1 Magnetic Fields. Oersted and Ampere
3.1 Mgnetic Fields Oested nd Ampee The definition of mgnetic induction, B Fields of smll loop (dipole) Mgnetic fields in mtte: ) feomgnetism ) mgnetiztion, (M ) c) mgnetic susceptiility, m d) mgnetic field,
More informationObjects usually are charged up through the transfer of electrons from one object to the other.
1 Pat 1: Electic Foce 1.1: Review of Vectos Review you vectos! You should know how to convet fom pola fom to component fom and vice vesa add and subtact vectos multiply vectos by scalas Find the esultant
More informationElectricity & Magnetism Lecture 6: Electric Potential
Electicity & Mgnetism Lectue 6: Electic Potentil Tody s Concept: Electic Potenl (Defined in tems of Pth Integl of Electic Field) Electicity & Mgnesm Lectue 6, Slide Stuff you sked bout:! Explin moe why
More information10 m, so the distance from the Sun to the Moon during a solar eclipse is. The mass of the Sun, Earth, and Moon are = =
Chpte 1 nivesl Gvittion 11 *P1. () The un-th distnce is 1.4 nd the th-moon 8 distnce is.84, so the distnce fom the un to the Moon duing sol eclipse is 11 8 11 1.4.84 = 1.4 The mss of the un, th, nd Moon
More informationMagnetic Field. Conference 6. Physics 102 General Physics II
Physics 102 Confeence 6 Magnetic Field Confeence 6 Physics 102 Geneal Physics II Monday, Mach 3d, 2014 6.1 Quiz Poblem 6.1 Think about the magnetic field associated with an infinite, cuent caying wie.
More informationSEE LAST PAGE FOR SOME POTENTIALLY USEFUL FORMULAE AND CONSTANTS
Cicle instucto: Moow o Yethiaj Name: MEMORIL UNIVERSITY OF NEWFOUNDLND DEPRTMENT OF PHYSICS ND PHYSICL OCENOGRPHY Final Eam Phsics 5 Winte 3:-5: pil, INSTRUCTIONS:. Do all SIX (6) questions in section
More informationPY208 Matter & Interactions Final Exam S2005
PY Matte & Inteactions Final Exam S2005 Name (pint) Please cicle you lectue section below: 003 (Ramakishnan 11:20 AM) 004 (Clake 1:30 PM) 005 (Chabay 2:35 PM) When you tun in the test, including the fomula
More information1. A man pulls himself up the 15 incline by the method shown. If the combined mass of the man and cart is 100 kg, determine the acceleration of the
1. n pulls hiself up the 15 incline b the ethod shown. If the cobined ss of the n nd ct is 100 g deteine the cceletion of the ct if the n eets pull of 50 on the ope. eglect ll fiction nd the ss of the
More informationCalculate the electric potential at B d2=4 m Calculate the electric potential at A d1=3 m 3 m 3 m
MTE : Ch 13 5:3-7pm on Oct 31 ltenate Exams: Wed Ch 13 6:3pm-8:pm (people attending the altenate exam will not be allowed to go out of the oom while othes fom pevious exam ae still aound) Thu @ 9:-1:3
More informationJEE(Advanced) 2018 TEST PAPER WITH SOLUTION PHYSICS. (HELD ON SUNDAY 20 th MAY, 2018) PART-1 : PHYSICS. (C) L = mkr ALLEN
JEE(Advnced) 08 TEST PAPE WITH SOUTION (HED ON SUNDAY 0 th MAY, 08) PAT- : JEE(Advnced) 08/Ppe-. The potentil enegy of pticle of mss m t distnce fom fixed point O is given by V () k /, whee k is positive
More information( ) ( ) Physics 111. Lecture 13 (Walker: Ch ) Connected Objects Circular Motion Centripetal Acceleration Centripetal Force Sept.
Physics Lectue 3 (Wlke: Ch. 6.4-5) Connected Objects Cicul Motion Centipetl Acceletion Centipetl Foce Sept. 30, 009 Exmple: Connected Blocks Block of mss m slides on fictionless tbletop. It is connected
More informationExam 2 Solutions. Note that there are several variations of some problems, indicated by choices in parentheses. + R 1 2
PHY49 Fll 5 Acot, Woodd Exm Solution Note tht thee e evel vition of ome poblem, indicted by choice in penthee. Poblem : Two light bulb hve eitnce of Ω nd 3Ω. They e connected in pllel co V line. Wht i
More informationGet Solution of These Packages & Learn by Video Tutorials on EXERCISE-1
FEE Downlod Study Pckge fom website: www.tekoclsses.com & www.mthsbysuhg.com Get Solution of These Pckges & Len by Video Tutoils on www.mthsbysuhg.com EXECISE- * MAK IS MOE THAN ONE COECT QUESTIONS. SECTION
More informationHow Electric Currents Interact with Magnetic Fields
How Electic Cuents nteact with Magnetic Fields 1 Oested and Long Wies wote these notes to help ou with vaious diectional ules, and the equivalence between the magnetism of magnets and the magnets of electic
More informationWork, Potential Energy, Conservation of Energy. the electric forces are conservative: ur r
Wok, Potentil Enegy, Consevtion of Enegy the electic foces e consevtive: u Fd = Wok, Potentil Enegy, Consevtion of Enegy b b W = u b b Fdl = F()[ d + $ $ dl ] = F() d u Fdl = the electic foces e consevtive
More informationELECTROSTATICS. Syllabus : Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road PE 1
PE ELECTOSTATICS Syllbus : Electic chges : Consevtion of chge, Coulumb s lw-foces between two point chges, foces between multiple chges; supeposition pinciple nd continuous chge distibution. Electic field
More informationFaraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law
Faaday s Law Faaday s Epeiments Chapte 3 Law of nduction (emf( emf) Faaday s Law Magnetic Flu Lenz s Law Geneatos nduced Electic fields Michael Faaday discoeed induction in 83 Moing the magnet induces
More information2/26/2014. Magnetism. Chapter 20 Topics. Magnets and Magnetic Fields. Magnets and Magnetic Fields. Magnets and Magnetic Fields
Magnets and Magnetic ields Magnetism Howee, if you cut a magnet in half, you don t get a noth pole and a south pole you get two smalle magnets. ectue otes Chapte 20 Topics Magnets and Magnetic ields Magnets
More informationChapter 8. Ch.8, Potential flow
Ch.8, Voticit (epetition) Velocit potentil Stem function Supeposition Cicultion -dimensionl bodies Kutt-Joukovskis lift theoem Comple potentil Aismmetic potentil flow Rotting fluid element Chpte 4 Angul
More informationChapter 23 Electrical Potential
hpte Electicl Potentil onceptul Polems [SSM] A poton is moved to the left in unifom electic field tht points to the ight. Is the poton moving in the diection of incesing o decesing electic potentil? Is
More informationMagnetic Fields Due to Currents
PH -C Fall 1 Magnetic Fields Due to Cuents Lectue 14 Chapte 9 (Halliday/esnick/Walke, Fundamentals of Physics 8 th edition) 1 Chapte 9 Magnetic Fields Due to Cuents In this chapte we will exploe the elationship
More informationMATHEMATICS IV 2 MARKS. 5 2 = e 3, 4
MATHEMATICS IV MARKS. If + + 6 + c epesents cicle with dius 6, find the vlue of c. R 9 f c ; g, f 6 9 c 6 c c. Find the eccenticit of the hpeol Eqution of the hpeol Hee, nd + e + e 5 e 5 e. Find the distnce
More informationCh 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2!
Ch 30 - Souces of Magnetic Field 1.) Example 1 Detemine the magnitude and diection of the magnetic field at the point O in the diagam. (Cuent flows fom top to bottom, adius of cuvatue.) Fo staight segments,
More informationPhysics 111. Uniform circular motion. Ch 6. v = constant. v constant. Wednesday, 8-9 pm in NSC 128/119 Sunday, 6:30-8 pm in CCLIR 468
ics Announcements dy, embe 28, 2004 Ch 6: Cicul Motion - centipetl cceletion Fiction Tension - the mssless sting Help this week: Wednesdy, 8-9 pm in NSC 128/119 Sundy, 6:30-8 pm in CCLIR 468 Announcements
More informationF Q E v B MAGNETOSTATICS. Creation of magnetic field B. Effect of B on a moving charge. On moving charges only. Stationary and moving charges
MAGNETOSTATICS Ceation of magnetic field. Effect of on a moving chage. Take the second case: F Q v mag On moving chages only F QE v Stationay and moving chages dw F dl Analysis on F mag : mag mag Qv. vdt
More information16.1 Permanent magnets
Unit 16 Magnetism 161 Pemanent magnets 16 The magnetic foce on moving chage 163 The motion of chaged paticles in a magnetic field 164 The magnetic foce exeted on a cuent-caying wie 165 Cuent loops and
More information1 2 U CV. K dq I dt J nqv d J V IR P VI
o 5 o T C T F 9 T K T o C 7.5 L L T V VT Q mct nct Q F V ml F V dq A H k TH TC dt L pv nt Kt nt CV ideal monatomic gas 5 CV ideal diatomic gas w/o vibation V W pdv V U Q W W Q e Q Q e Canot H C T T S C
More information3-Axis Vector Magnet: Construction and Characterisation of Split Coils at RT. Semester Project Petar Jurcevic
3-Axis Vecto Magnet: Constuction and Chaacteisation of Split Coils at RT Semeste Poject Peta Jucevic Outline Field Calculation and Simulation Constuction Details Field Calculations Chaacteization at RT
More informationReview for 2 nd Midterm
Review fo 2 nd Midtem Midtem-2! Wednesday Octobe 29 at 6pm Section 1 N100 BCC (Business College) Section 2 158 NR (Natual Resouces) Allowed one sheet of notes (both sides) and calculato Coves Chaptes 27-31
More informationLecture 11: Potential Gradient and Capacitor Review:
Lectue 11: Potentil Gdient nd Cpcito Review: Two wys to find t ny point in spce: Sum o Integte ove chges: q 1 1 q 2 2 3 P i 1 q i i dq q 3 P 1 dq xmple of integting ove distiution: line of chge ing of
More informationElectric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin
1 1 Electic Field + + q F Q R oigin E 0 0 F E ˆ E 4 4 R q Q R Q - - Electic field intensity depends on the medium! Electic Flux Density We intoduce new vecto field D independent of medium. D E So, electic
More informationContinuous Charge Distributions
Continuous Chge Distibutions Review Wht if we hve distibution of chge? ˆ Q chge of distibution. Q dq element of chge. d contibution to due to dq. Cn wite dq = ρ dv; ρ is the chge density. = 1 4πε 0 qi
More informationIntroduction: Vectors and Integrals
Intoduction: Vectos and Integals Vectos a Vectos ae chaacteized by two paametes: length (magnitude) diection a These vectos ae the same Sum of the vectos: a b a a b b a b a b a Vectos Sum of the vectos:
More informationCHAPTER 25 ELECTRIC POTENTIAL
CHPTE 5 ELECTIC POTENTIL Potential Diffeence and Electic Potential Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic foce on the paticle given by F=E. When
More informationProf. Anchordoqui Problems set # 12 Physics 169 May 12, 2015
Pof. Anchodoqui Poblems set # 12 Physics 169 My 12, 2015 1. Two concentic conducting sphees of inne nd oute dii nd b, espectively, cy chges ±Q. The empty spce between the sphees is hlf-filled by hemispheicl
More informationDYNAMICS. Kinetics of Particles: Newton s Second Law VECTOR MECHANICS FOR ENGINEERS: Ninth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.
Ninth E CHPTER VECTOR MECHNICS OR ENGINEERS: DYNMICS edinnd P. ee E. Russell Johnston, J. Lectue Notes: J. Wlt Ole Texs Tech Univesity Kinetics of Pticles: Newton s Second Lw The McGw-Hill Copnies, Inc.
More informationChapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic fields. Chapter 28: Magnetic fields
Chapte 8: Magnetic fiels Histoically, people iscoe a stone (e 3 O 4 ) that attact pieces of ion these stone was calle magnets. two ba magnets can attact o epel epening on thei oientation this is ue to
More informationThe Law of Biot-Savart & RHR P θ
The Law of iot-savat & RHR P R dx x Jean-aptiste iot élix Savat Phys 122 Lectue 19 G. Rybka Recall: Potential Enegy of Dipole Wok equied to otate a cuentcaying loop in a magnetic field Potential enegy
More informationN for static friction and N
Fiction: Epeimentll the following fetues e obseed to be tue of the foce of fiction: ) Fiction lws opposes the motion. The foce is dissiptie nd its diection is pllel to the sufce of the object in motion.
More informationπ,π is the angle FROM a! TO b
Mth 151: 1.2 The Dot Poduct We hve scled vectos (o, multiplied vectos y el nume clled scl) nd dded vectos (in ectngul component fom). Cn we multiply vectos togethe? The nswe is YES! In fct, thee e two
More informationAssistant Professor: Zhou Yufeng. N , ,
Aitnt Pofeo: Zhou Yufeng N3.-0-5, 6790-448, yfzhou@ntu.edu.g http://www3.ntu.edu.g/home/yfzhou/coue.html . A pojectile i fied t flling tget hown. The pojectile lee the gun t the me intnt tht the tget dopped
More informationSTD: XI MATHEMATICS Total Marks: 90. I Choose the correct answer: ( 20 x 1 = 20 ) a) x = 1 b) x =2 c) x = 3 d) x = 0
STD: XI MATHEMATICS Totl Mks: 90 Time: ½ Hs I Choose the coect nswe: ( 0 = 0 ). The solution of is ) = b) = c) = d) = 0. Given tht the vlue of thid ode deteminnt is then the vlue of the deteminnt fomed
More informationUnit 7: Sources of magnetic field
Unit 7: Souces of magnetic field Oested s expeiment. iot and Savat s law. Magnetic field ceated by a cicula loop Ampèe s law (A.L.). Applications of A.L. Magnetic field ceated by a: Staight cuent-caying
More informationAQA Maths M2. Topic Questions from Papers. Circular Motion. Answers
AQA Mths M Topic Questions fom Ppes Cicul Motion Answes PhysicsAndMthsTuto.com PhysicsAndMthsTuto.com Totl 6 () T cos30 = 9.8 Resolving veticlly with two tems Coect eqution 9.8 T = cos30 T =.6 N AG 3 Coect
More information= ΔW a b. U 1 r m 1 + K 2
Chpite 3 Potentiel électiue [18 u 3 mi] DEVOIR : 31, 316, 354, 361, 35 Le potentiel électiue est le tvil p unité de chge (en J/C, ou volt) Ce concept est donc utile dns les polèmes de consevtion d énegie
More informationElecto Magnetism iot Savat s Law and Ampee s Cicuital Law 1. A cuent is flowing due noth along a powe line. The diection of the magnetic field above it, neglecting the eath s field is: (1) Noth () East
More informationChapter 24. Gauss s Law
Chpte 24 Guss s Lw CHAPTR OUTLIN 24.1 lectic Flux 24.2 Guss s Lw 24.3 Appliction of Guss s Lw to Vious Chge Distibutions 24.4 Conductos in lectosttic uilibium 24.5 Foml Deivtion of Guss s Lw In tble-top
More informationSources of Magnetic Fields (chap 28)
Souces of Magnetic Fields (chap 8) In chapte 7, we consideed the magnetic field effects on a moving chage, a line cuent and a cuent loop. Now in Chap 8, we conside the magnetic fields that ae ceated by
More information( ) ( )( ) ˆ. Homework #8. Chapter 28
Hoewok #8. Chapte 8 1** A sall cuent eleent at the oigin has a length of. and caies a cuent of. A in the +z diection. Find the agnitude of the agnetic field due to this eleent and indicate its diection
More informationELECTROSTATICS. JEE-Physics ELECTRIC CHARGE
J-Physics LCTIC CHAG LCTOSTATICS Chge is the popety ssocited with mtte due to which it poduces nd epeiences electicl nd mgnetic effects. The ecess o deficiency of electons in body gives the concept of
More information6. Gravitation. 6.1 Newton's law of Gravitation
Gvittion / 1 6.1 Newton's lw of Gvittion 6. Gvittion Newton's lw of gvittion sttes tht evey body in this univese ttcts evey othe body with foce, which is diectly popotionl to the poduct of thei msses nd
More informationModule 18: Outline. Magnetic Dipoles Magnetic Torques
Module 18: Magnetic Dipoles 1 Module 18: Outline Magnetic Dipoles Magnetic Toques 2 IA nˆ I A Magnetic Dipole Moment μ 3 Toque on a Cuent Loop in a Unifom Magnetic Field 4 Poblem: Cuent Loop Place ectangula
More information