19.1 Electrical Potential Energy. Special Case 1. v B

Size: px
Start display at page:

Download "19.1 Electrical Potential Energy. Special Case 1. v B"

Transcription

1 9. lectcl Potentl neg Specl Ce We elee tet chge between the plte o cpcto. Dung ome tme t moe om to B How e the ntl nd nl peed nd B elted? pp Sole th poblem b ung the concept o electcl potentl eneg B

2 9. lectcl Potentl neg P: lectcl Potentl neg o the tet chge nde the cpcto: wok done b ou gnt the electcl oce to moe the tet chge om the zeo P eeence pont to ptcul locton.e. P uncton o the locton o oce ou need to ppl to moe ound (lowl): pp pp pp Chooe the negte plte (hee ) to be the zeo P eeence pont

3 3 9. lectcl Potentl neg P: lectcl Potentl neg o the tet chge nde the cpcto: wok done b ou gnt the electcl oce to moe the tet chge om the zeo P eeence pont to ptcul locton.e. P uncton o the locton o pp oce ou need to ppl to moe ound (lowl): pp Reew : WORK done b contnt oce ( coθ ) W C, θ ngle between dplcement C nd P (W pp ) pp coθ But ( coθ ) etcl component o nd mgntude o pp : pp P C Chooe the negte plte (hee ) to be the zeo P eeence pont θ Th n mgn moement pp

4 4 9. lectcl Potentl neg P: lectcl Potentl neg o the tet chge nde the cpcto: wok done b ou gnt the electcl oce to moe the tet chge om the zeo P eeence pont to ptcul locton.e. P uncton o the locton o oce ou need to ppl to moe ound (lowl): ( coθ ) W C, θ ngle between dplcement pp nd P B (W pp ) B pp B coθ B Reew : WORK done b contnt oce But ( coθ B ) etcl component o B B nd mgntude o pp : pp P B B C C Chooe the negte plte (hee ) to be the zeo P eeence pont θ B Th n mgn moement pp pp B

5 9. lectcl Potentl neg P: lectcl Potentl neg o the tet chge nde the cpcto: wok done b ou gnt the electcl oce to moe the tet chge om the zeo P eeence pont to ptcul locton.e. P uncton o the locton o oce ou need to ppl to moe ound (lowl): pp pp pp pp Reew : WORK done b contnt oce ( coθ ) W C, θ ngle between dplcement C nd C Chooe the negte plte (hee ) to be the zeo P eeence pont B P (W pp ) pp coθ P B (W pp ) B pp B coθ B B P ( ) 5

6 9. lectcl Potentl neg We now nclude electc potentl eneg P pt o the totl eneg tht n object cn he: m Iω mgh P Tnlton knetc eneg Rottonl knetc eneg k Reew: Wok-neg Theoem: wok done on n object chnge n t knetc eneg W K, whee K½ m Lw o Coneton o neg: In the bence o dpte oce, Knetc eneg potentl eneg contnt O: K P... Gttonl potentl eneg ltc potentl eneg lectcl potentl eneg nd combnng thee two: W (P) P -P 6

7 9. lectcl Potentl neg Wok-neg Theoem Chnge n knetc eneg o the tet chge t moe unde the nluence o the cpcto electc eld om to B eul to the wok done b the electc eld K m W B B B m coθ ( B Th epeon n ld onl o contnt oce ) θ pp Coneton o neg In the bence o dpte oce (e.g. YOU, but ou e not ntectng wth the tem hee), the totl eneg KP coneed untt: K m B Note: B B W B ( P) B m ( m P Wok done BY the electc eld chnge n P om to B (P B ) B B P ) Chooe the negte plte (hee ) to be the zeo P eeence pont B 7

8 8 mple: (hozontl) pllel plte cpcto he the ollowng ttbute: e o plte: 4.5m Plte epton:.cm Q chge o Q.5µC plced on the top plte, nd Q on the bottom plte. poton (m.67-7 kg) h ntl eloct o.5 6 m/ n the hozontl decton when njected nto the gp. The njecton pont ectl hl the dtnce between the two plte. You m neglect gt. / () nd t nl peed t che nto the bottom plte. (b) nd the ngle φ between the nl eloct nd the noml to the bottom plte -Q φ

9 9 Q.5µC, 4.5m,.m, m.67-7 kg,.5 6 m/,.6-9 C nd (), nd (b)φ Q / -Q φ

10 Q.5µC, 4.5m,.m, m.67-7 kg,.5 6 m/,.6-9 C nd (), nd (b)φ Q / -Q φ φ

11 Q.5µC, 4.5m,.m, m.67-7 kg,.5 6 m/,.6-9 C nd (), nd (b)φ Q Conde wok done on the poton b the electc eld: W P σ ε 5.65 W 9.4 Q ε 5 6 (.6 W ( K) N/C 9 J (4.5 m C)(5.65 m (.5 )[8.85 m ( / ) 5 m( -6 C) C N/C)(.m) /(N m ) )... (wok - eneg theoem) / -Q φ W / m (W / m) (W / m) 6 6 (9.4 kg m () (.5 m/) 7.67 kg (b) n the ecto decompoton dgm o / ).83 6 m/ φ nφ φ n 6.5 m/ m/ φ 55.3 o

12 W STOPPD HR ON JN 3 TH NXT THR SLIDS R OR YOUR INORMTION ONLY

13 Q.5µC, 4.5m,.m, m.67-7 kg,.5 6 m/,.6-9 C nd (), nd (b)φ Method (): contnt downwd oce: me pojectle moton (Secton 3.3) umng the poton tt t (,) Hozontl njecton, The electceld puel n the decton,, whee / m / m t, Q ε t, t t (4.5 m It conenent hee to ole o the downwd cceleton : σ ε (.6 9 t t (.5 )[8.85 C)( N/C) /(N m 7 3 / m (9.4 N) /(.67 kg) 5.43 m/ Thee wee ectl the me lue we hd n the emple nolng njectng poton long on eb. Hee the njecton pependcul to C) C 9.4 N Q / - Q 5.65 ) 4 5 N/C φ 3

14 Q.5µC, 4.5m,.m, m.67-7 kg,.5 6 m/,.6-9 C nd (), nd (b)φ The poblem h mpled to : whee 5.43 Net : ole o tme t bottom plte :, 3 om pojectle moton : t t t, t, t ( m/ t whch the poton che nto the t t Q / - Q. m m/ 8 6 m/ )(.9 ).45 t m/ φ.5 6 m/, nd 6 6 () (.5 m/) (.45 m/) (b) n the ecto decompoton dgm o.83 6 m/ φ tnφ φ tn 6.5 m/ 6.45 m/ 55.3 o 4

15 Q.5µC, 4.5m,.m, m.67-7 kg,.5 6 m/,.6-9 C nd (), nd (b)φ Q The poblem h mpled to : whee, t, Net : ole o tme t bottom plte : 5.43 t, 3 m/ t whch the poton che nto the t / om pojectle moton : t t t ( t m/. m m/ )(.9 8 t.9 8 -Q ).45 6 m/ φ.5 6 m/, nd 6 6 () (.5 m/) (.45 m/) (b) n the ecto decompoton dgm o.83 6 m/ φ tnφ φ tn 6.5 m/ 6.45 m/ 55.3 o 5

16 9. lectcl Potentl neg Specl Ce P o tet chge n the electc eld o ouce chge : () men uncton o dtnce P( ) k ***Deton o () om () eue ntegl clculu lectc eld ceted b pont chge : (dgm dwn umng >) () Decton: pontng dectl w om t n pont. () Mgntude gen b Coulomb Lw ( ) k *** () () Th omul wok een one o both chge e negte 6

17 9. lectcl Potentl neg Totl Potentl eneg o tem o pont chge We tt wth thee pont chge:,, 3 k U P o, j U j k j j U U U3 U 3 k U U 3 3 k 3 3 The oell potentl eneg the mount o wok eued o n etenl gent to emble th et o chge th cn be done n deent w, o emple: () Bng n om (no cot), W (b) Bng n om : W U (c) Bng n 3 om : W 3 U 3 U 3 Totl W W W UU U 3 U 3 Cn do th n n ode nd obtn the SM eult tendng to N pont chge k N j U j j j k j j Thee e N(N-)/ dtnct p 7

18 9. The lectc Potentl Deence DINITION O LCTRIC POTNTIL The electc potentl t gen pont the electc potentl eneg o mll tet chge dded b the chge tel: V P o SI Unt o lectc Potentl: joule/coulomb olt (V) ( V ) B P o B V B V P o B W o B lectcl Potenetl Deence om to B deence, pe unt chge, o the P o tet chge WOULD HV om locton to locton B P k, V k k V ( ) B B P B k B, V B k B 8

19 9.3 The lectc Potentl Deence Ceted b Pont Chge 9 mple The Potentl o Pont Chge Ung zeo eeence potentl t nnt***, detemne the mount b whch pont chge o C lte the electc potentl t pot.m w when the chge () pote nd (b) negte.

20 9.3 The lectc Potentl Deence Ceted b Pont Chge mple The Potentl o Pont Chge Ung zeo eeence potentl t nnt***, detemne the mount b whch pont chge o C lte the electc potentl t pot.m w when the chge () pote nd (b) negte. () (b) V k 9 8 ( 8.99 N m C )( 4. C) 3 V V k. m 9 8 ( 8.99 N m C )( 4. C) 3 V. m *** In Ch. 6 ou lened tht the choce o the eeence zeo o gttonl potentl eneg bt. Th lo tue o P nd hence o the electc potentl V. The choce o zeo t nnt onl ld o collecton o pont chge, nd not o pllel plte cpcto o nnte we

21 9.3 The lectc Potentl Deence Ceted b Pont Chge W V W V W V... Σ(... coθ ) Σ( coθ )... mple The Totl lectc Potentl t locton nd B, nd the totl electc potentl.

22 9.3 The lectc Potentl Deence Ceted b Pont Chge You lened n chpte 6 tht the wok done b deent oce (o emple, hee, b the electc eld o deent pont chge) dd cl. dect coneuence, the totl electcl potentl lo the cl um o nddul potentl (o emple, thoe om deent pont chge: W V W V W V... Σ(... coθ ) Σ( coθ )... mple The Totl lectc Potentl t locton nd B, nd the totl electc potentl. k V V V k Sml (but DIRNT) eult o V B V V B ( 8.99 N m C )( 8. C) ( 8.99 N m C )( 8. C) 4 V. m.6 m ( 8.99 N m C )( 8. C) ( 8.99 N m C )( 8. C).4 m.4 m V

23 9.3 The lectc Potentl Deence Ceted b Pont Chge 3 mple Whee the Potentl eul to Zeo? Two pont chge e ed n plce. The pote chge nd the negte chge. On the lne tht pe though the chge, how mn plce e thee t whch the totl potentl zeo? Whee e the?

24 9.3 The lectc Potentl Deence Ceted b Pont Chge mple Whee the Potentl eul to Zeo? Two pont chge e ed n plce. The pote chge nd the negte chge. On the lne tht pe though the chge, how mn plce e thee t whch the totl potentl zeo? Whee e the? 4 ) (, 3 3 ) (, ) (, : 3ce k k V > < < < > < < < tneou oot: < md e not comptble

25 9.5 Cpcto nd Delectc pllel plte cpcto cont o two metl plte, one cng chge nd the othe cng chge. It common to ll the egon between the plte wth n electcll nultng ubtnce clled delectc. cpcto dece degned to toe eneg nd chge..g. debllto cont o lge cpcto tht dchge cuent (low o chge) when the pddle e ppled to ptent In electcl ccut the oten e ued to tblze electc potentl 5

26 9.5 Cpcto nd Delectc TH RLTION BTWN CHRG ND POTNTIL DIRNC OR CPCITOR The mgntude o the chge n ech plce o the cpcto dectl popotonl to the mgntude o the potentl deence between the plte. CV The cpctnce C the popotonlt contnt. SI Unt o Cpctnce: coulomb/olt d () C/V C /J Memo d C V coulomb d olt nce Btn : Itl 6

27 9.5 Cpcto nd Delectc TH CPCITNC O PRLLL PLT CPCITOR Smplet ce: /cuum gp (no delectc ) V potentl deence om the to the plte (b th denton, V o cpcto lw pote) chge on the plte ( on the plte) e o the plte d plte epton/gp Note the deent notton ued b the tetbook o th ecton V d lectceld n cuum/ (downwd) : ( P) V ( V ) C C V W ε [ ( coθ ) ] Potentl deence between plte (ddng out σ ε, Hee the ubcpt ndcte the pecl ce o Chnge n potentl eneg o tet chge ( ) ε d d d ε, - V θ 8 cuum/ gp om - to : o ) : - Pllel plte cpcto lled wth cuum/ ε C C d 7

28 9.5 Cpcto nd Delectc mple: pllel plte cpcto he the ollowng ttbute: e o plte: 4.5m Plte epton: d.cm The gp lled wth nd t cpctnce C V d - 8

29 9.5 Cpcto nd Delectc mple: pllel plte cpcto he the ollowng ttbute: e o plte: 4.5m Plte epton: d.cm The gp lled wth nd t cpctnce C V d Pllel plte cpcto lled wth cuum/ ε d C C - C C [ C /(N m (. m).99 n )](4.5 m ) Note tht d () e lge cpctnce Th 4.5 m plte t. cm epton ge onl ~ n 9

30 3 Cpcto n eneg toge dece: It tke wok (.e. eneg) to chge up cpcto om zeo chge to (zeo potentl to V). V V W ( )V V/C The gue how cpcto t chge, potentl deence V (between the plte nd the plte). To ncee nd V, we moe mll mount o chge om the plte to the plte. Th eue wok done BY n etenl gent, GINST the electc eld: P WXT W (done b the electc eld) ( ) d ( ) V e o the hded tpe nv. gph

31 Cpcto n eneg toge dece: (contnued) V V neg U e o tngle W ( )V ½ V ½ /C V/C To chge cpcto to (, V) om (,), the totl mount o wok e encloed b the blue tngle, whch the eneg toed n the cpcto. neg U C but CV neg U CV 3

32 3 mple: Pllel plte cpcto e o plte: 4.5m Plte epton: d.cm Plte chge:.5µc The gp lled wth () nd the oltge (potentl deence) o the cpcto. (b) nd the eneg toed n th cpcto d -

33 mple: Pllel plte cpcto e o plte: 4.5m Plte epton: d.cm Plte chge:.5µc The gp lled wth neg U C CV () nd the oltge (potentl deence) o the cpcto. (b) nd the eneg toed n th cpcto d.5 () V C.99 (b) neg U CV / C 9 9 (.5 C C 4.3 V 9.99 C / J 9 4 (.99 C / J)(.3 V) C) /(.99 9 ).7 J - pplcton: Tpcl debllto he bnk o cpcto chged up to ~ V nd uull n eneg o up to ~ J deleed to the ptent Th men C U/V.4 m Redent l? So how do we mke cpctnce much bgge (ppo. 5 )? 33

Kinematics Quantities. Linear Motion. Coordinate System. Kinematics Quantities. Velocity. Position. Don t Forget Units!

Kinematics Quantities. Linear Motion. Coordinate System. Kinematics Quantities. Velocity. Position. Don t Forget Units! Knemtc Quntte Lner Phyc 11 Eyre Tme Intnt t Fundmentl Tme Interl t Dened Poton Fundmentl Dplcement Dened Aerge g Dened Aerge Accelerton g Dened Knemtc Quntte Scler: Mgntude Tme Intnt, Tme Interl nd Speed

More information

Uniform Circular Motion

Uniform Circular Motion Unfom Ccul Moton Unfom ccul Moton An object mong t constnt sped n ccle The ntude of the eloct emns constnt The decton of the eloct chnges contnuousl!!!! Snce cceleton s te of chnge of eloct:!! Δ Δt The

More information

E-Companion: Mathematical Proofs

E-Companion: Mathematical Proofs E-omnon: Mthemtcl Poo Poo o emm : Pt DS Sytem y denton o t ey to vey tht t ncee n wth d ncee n We dene } ] : [ { M whee / We let the ttegy et o ech etle n DS e ]} [ ] [ : { M w whee M lge otve nume oth

More information

a = Acceleration Linear Motion Acceleration Changing Velocity All these Velocities? Acceleration and Freefall Physics 114

a = Acceleration Linear Motion Acceleration Changing Velocity All these Velocities? Acceleration and Freefall Physics 114 Lner Accelerton nd Freell Phyc 4 Eyre Denton o ccelerton Both de o equton re equl Mgntude Unt Drecton (t ector!) Accelerton Mgntude Mgntude Unt Unt Drecton Drecton 4/3/07 Module 3-Phy4-Eyre 4/3/07 Module

More information

x=0 x=0 Positive Negative Positions Positions x=0 Positive Negative Positions Positions

x=0 x=0 Positive Negative Positions Positions x=0 Positive Negative Positions Positions Knemtc Quntte Lner Moton Phyc 101 Eyre Tme Intnt t Fundmentl Tme Interl Defned Poton x Fundmentl Dplcement Defned Aerge Velocty g Defned Aerge Accelerton g Defned Knemtc Quntte Scler: Mgntude Tme Intnt,

More information

AP Physics C: Mechanics

AP Physics C: Mechanics 08 AP Phyc C: Mechnc ee-repone Queton 08 The College Bod. College Bod, Advnced Plcement Pogm, AP, AP Centl, nd the con logo e egteed tdemk of the College Bod. Vt the College Bod on the Web: www.collegebod.og.

More information

Chapter I Vector Analysis

Chapter I Vector Analysis . Chpte I Vecto nlss . Vecto lgeb j It s well-nown tht n vecto cn be wtten s Vectos obe the followng lgebc ules: scl s ) ( j v v cos ) ( e Commuttv ) ( ssoctve C C ) ( ) ( v j ) ( ) ( ) ( ) ( (v) he lw

More information

PHYS 2421 Fields and Waves

PHYS 2421 Fields and Waves PHYS 242 Felds nd Wves Instucto: Joge A. López Offce: PSCI 29 A, Phone: 747-7528 Textook: Unvesty Physcs e, Young nd Feedmn 23. Electc potentl enegy 23.2 Electc potentl 23.3 Clcultng electc potentl 23.4

More information

Remember: When an object falls due to gravity its potential energy decreases.

Remember: When an object falls due to gravity its potential energy decreases. Chapte 5: lectc Potental As mentoned seveal tmes dung the uate Newton s law o gavty and Coulomb s law ae dentcal n the mathematcal om. So, most thngs that ae tue o gavty ae also tue o electostatcs! Hee

More information

Chapter 21: Electric Charge and Electric Field

Chapter 21: Electric Charge and Electric Field Chpte : lectc Chge nd lectc Feld lectc Chge Known b ncent Geeks s el s 600 BC Sttc electct: electc chge v fcton (see lso fg.) (Attempted) pth bll demo nd/o scotch tpe demo: knds of popetes objects wth

More information

Physics 15 Second Hour Exam

Physics 15 Second Hour Exam hc 5 Second Hou e nwe e Mulle hoce / ole / ole /6 ole / ------------------------------- ol / I ee eone ole lee how ll wo n ode o ecee l ced. I ou oluon e llegle no ced wll e gen.. onde he collon o wo 7.

More information

MATHEMATICS II PUC VECTOR ALGEBRA QUESTIONS & ANSWER

MATHEMATICS II PUC VECTOR ALGEBRA QUESTIONS & ANSWER MATHEMATICS II PUC VECTOR ALGEBRA QUESTIONS & ANSWER I One M Queston Fnd the unt veto n the deton of Let ˆ ˆ 9 Let & If Ae the vetos & equl? But vetos e not equl sne the oespondng omponents e dstnt e detons

More information

Physics 1502: Lecture 2 Today s Agenda

Physics 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 information

Electric Potential. and Equipotentials

Electric 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 information

6.6 The Marquardt Algorithm

6.6 The Marquardt Algorithm 6.6 The Mqudt Algothm lmttons of the gdent nd Tylo expnson methods ecstng the Tylo expnson n tems of ch-sque devtves ecstng the gdent sech nto n tetve mtx fomlsm Mqudt's lgothm utomtclly combnes the gdent

More information

Physics 120 Spring 2007 Exam #1 April 20, Name

Physics 120 Spring 2007 Exam #1 April 20, Name Phc 0 Spng 007 E # pl 0, 007 Ne P Mulple Choce / 0 Poble # / 0 Poble # / 0 Poble # / 0 ol / 00 In eepng wh he Unon College polc on cdec hone, ued h ou wll nehe ccep no pode unuhozed nce n he copleon o

More information

U>, and is negative. Electric Potential Energy

U>, 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 information

Calculus 241, section 12.2 Limits/Continuity & 12.3 Derivatives/Integrals notes by Tim Pilachowski r r r =, with a domain of real ( )

Calculus 241, section 12.2 Limits/Continuity & 12.3 Derivatives/Integrals notes by Tim Pilachowski r r r =, with a domain of real ( ) Clculu 4, econ Lm/Connuy & Devve/Inel noe y Tm Plchow, wh domn o el Wh we hve o : veco-vlued uncon, ( ) ( ) ( ) j ( ) nume nd ne o veco The uncon, nd A w done wh eul uncon ( x) nd connuy e he componen

More information

Example 2: ( ) 2. $ s ' 9.11" 10 *31 kg ( )( 1" 10 *10 m) ( e)

Example 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 information

Rigid Body Dynamics. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018

Rigid Body Dynamics. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018 Rg Bo Dnmcs CSE169: Compute Anmton nstucto: Steve Roteneg UCSD, Wnte 2018 Coss Pouct k j Popetes of the Coss Pouct Coss Pouct c c c 0 0 0 c Coss Pouct c c c c c c 0 0 0 0 0 0 Coss Pouct 0 0 0 ˆ ˆ 0 0 0

More information

Torque generation with Electrical Machines. Industrial Electrical Engineering and Automation Lund University, Sweden

Torque generation with Electrical Machines. Industrial Electrical Engineering and Automation Lund University, Sweden Toqe geneton wth Electcl Mchne Indtl Electcl Engneeng nd Atoton nd Unvet, Sweden Toqe genetng phenoen Indtl Electcl Engneeng nd Atoton Condcto n gnetc feld Ion hpe n gnetc feld 3 Electottc 4 Pezotcton

More information

2 dependence in the electrostatic force means that it is also

2 dependence in the electrostatic force means that it is also lectc Potental negy an lectc Potental A scala el, nvolvng magntues only, s oten ease to wo wth when compae to a vecto el. Fo electc els not havng to begn wth vecto ssues woul be nce. To aange ths a scala

More information

CHAPTER 2 ELECTRIC FIELD

CHAPTER 2 ELECTRIC FIELD lecticity-mgnetim Tutil (QU PROJCT) 9 CHAPTR LCTRIC FILD.. Intductin If we plce tet chge in the pce ne chged d, n electttic fce will ct n the chge. In thi ce we pek f n electic field in thi pce ( nlgy

More information

Lecture 5 Single factor design and analysis

Lecture 5 Single factor design and analysis Lectue 5 Sngle fcto desgn nd nlss Completel ndomzed desgn (CRD Completel ndomzed desgn In the desgn of expements, completel ndomzed desgns e fo studng the effects of one pm fcto wthout the need to tke

More information

Physics 2A Chapter 11 - Universal Gravitation Fall 2017

Physics 2A Chapter 11 - Universal Gravitation Fall 2017 Physcs A Chapte - Unvesal Gavtaton Fall 07 hese notes ae ve pages. A quck summay: he text boxes n the notes contan the esults that wll compse the toolbox o Chapte. hee ae thee sectons: the law o gavtaton,

More information

Satellite Orbits. Orbital Mechanics. Circular Satellite Orbits

Satellite Orbits. Orbital Mechanics. Circular Satellite Orbits Obitl Mechnic tellite Obit Let u tt by king the quetion, Wht keep tellite in n obit ound eth?. Why doen t tellite go diectly towd th, nd why doen t it ecpe th? The nwe i tht thee e two min foce tht ct

More information

ME306 Dynamics, Spring HW1 Solution Key. AB, where θ is the angle between the vectors A and B, the proof

ME306 Dynamics, Spring HW1 Solution Key. AB, where θ is the angle between the vectors A and B, the proof ME6 Dnms, Spng HW Slutn Ke - Pve, gemetll.e. usng wngs sethes n nltll.e. usng equtns n nequltes, tht V then V. Nte: qunttes n l tpee e vets n n egul tpee e sls. Slutn: Let, Then V V V We wnt t pve tht:

More information

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1 Rotatonal Knematcs Rgd Object about a Fxed Axs Westen HS AP Physcs 1 Leanng Objectes What we know Unfom Ccula Moton q s Centpetal Acceleaton : Centpetal Foce: Non-unfom a F c c m F F F t m ma t What we

More information

Physics 604 Problem Set 1 Due Sept 16, 2010

Physics 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 information

Answers to test yourself questions

Answers 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 information

Physics 11b Lecture #11

Physics 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 information

CHAPTER 29 ELECTRIC FIELD AND POTENTIAL EXERCISES

CHAPTER 29 ELECTRIC FIELD AND POTENTIAL EXERCISES HPTER ELETRI FIELD ND POTENTIL EXERISES. oulob Newton l M L T 4 k F.. istnce between k so, foce k ( F ( The weight of boy 4 N 4 N wt of boy So,. foce between chges 4 So, foce between chges.6 weight of

More information

Lesson 8: Work, Energy, Power (Sections ) Chapter 6 Conservation of Energy

Lesson 8: Work, Energy, Power (Sections ) Chapter 6 Conservation of Energy Lesson 8: Wok, negy, Powe (Sectons 6.-6.8) Chapte 6 Conseaton o negy Today we begn wth a ey useul concept negy. We wll encounte many amla tems that now hae ey specc dentons n physcs. Conseaton o enegy

More information

One-dimensional kinematics

One-dimensional kinematics Phscs 45 Fomula Sheet Eam 3 One-dmensonal knematcs Vectos dsplacement: Δ total dstance taveled aveage speed total tme Δ aveage veloct: vav t t Δ nstantaneous veloct: v lm Δ t v aveage acceleaton: aav t

More information

CHAPTER? 29 ELECTRIC FIELD AND POTENTIAL EXERCISES = 2, N = (5.6) 1 = = = = = Newton

CHAPTER? 29 ELECTRIC FIELD AND POTENTIAL EXERCISES = 2, N = (5.6) 1 = = = = = Newton Downloe fo HPTER? ELETRI FIELD ND POTENTIL EXERISES. oulob Newton l M L T 4 k F.. istnce between k so, foce k ( F ( The weight of boy 4 N 4 N wt of boy.5 So, foce between chges 4 So, foce between chges

More information

Introduction to Robotics (Fag 3480)

Introduction to Robotics (Fag 3480) Intouton to Robot (Fg 8) Vå Robet Woo (Hw Engneeeng n pple Sene-B) Ole Jkob Elle PhD (Mofe fo IFI/UIO) Føtemnuen II Inttutt fo Infomtkk Unvetetet Olo Sekjonlee Teknolog Intevenjonenteet Olo Unvetetkehu

More information

Section 35 SHM and Circular Motion

Section 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 information

Chapter 28 Sources of Magnetic Field

Chapter 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 information

CHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD

CHAPTER 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 information

v v at 1 2 d vit at v v 2a d

v v at 1 2 d vit at v v 2a d SPH3UW Unt. Accelerton n One Denon Pge o 9 Note Phyc Inventory Accelerton the rte o chnge o velocty. Averge ccelerton, ve the chnge n velocty dvded by the te ntervl, v v v ve. t t v dv Intntneou ccelerton

More information

SECTION (A) : FLUX AND FARADAY S LAWS OF ELECTROMAGNETIC INDUCTION

SECTION (A) : FLUX AND FARADAY S LAWS OF ELECTROMAGNETIC INDUCTION SETON () : FUX N FY S WS OF EETOMGNET NUTON. onsde the stuton shown n fg. The esstnceless we s sld on the fed ls wth nstnt velocty. f the we s eplced by esstnceless seccul we, the gntude of the nduced

More information

8. INVERSE Z-TRANSFORM

8. INVERSE Z-TRANSFORM 8. INVERSE Z-TRANSFORM The proce by whch Z-trnform of tme ere, nmely X(), returned to the tme domn clled the nvere Z-trnform. The nvere Z-trnform defned by: Computer tudy Z X M-fle trn.m ued to fnd nvere

More information

AP Physics C: Electricity and Magnetism

AP Physics C: Electricity and Magnetism 08 AP Physcs C: Electcty n Mgnetsm Fee-Response Questons 08 The College Bo. College Bo, Avnce Plcement Pogm, AP, AP Centl, n the con logo e egstee temks of the College Bo. Vst the College Bo on the Web:

More information

3.1 Magnetic Fields. Oersted and Ampere

3.1 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 information

( ) ( )()4 x 10-6 C) ( ) = 3.6 N ( ) = "0.9 N. ( )ˆ i ' ( ) 2 ( ) 2. q 1 = 4 µc q 2 = -4 µc q 3 = 4 µc. q 1 q 2 q 3

( ) ( )()4 x 10-6 C) ( ) = 3.6 N ( ) = 0.9 N. ( )ˆ i ' ( ) 2 ( ) 2. q 1 = 4 µc q 2 = -4 µc q 3 = 4 µc. q 1 q 2 q 3 3 Emple : Three chrges re fed long strght lne s shown n the fgure boe wth 4 µc, -4 µc, nd 3 4 µc. The dstnce between nd s. m nd the dstnce between nd 3 s lso. m. Fnd the net force on ech chrge due to the

More information

( ) ( ) Physics 111. Lecture 13 (Walker: Ch ) Connected Objects Circular Motion Centripetal Acceleration Centripetal Force Sept.

( ) ( ) 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 information

ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.

ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS. GNRAL PHYSICS PH -3A (D. S. Mov) Test (/3/) key STUDNT NAM: STUDNT d #: -------------------------------------------------------------------------------------------------------------------------------------------

More information

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface

General 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 information

ELECTRO - MAGNETIC INDUCTION

ELECTRO - 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 information

Lecture 9-3/8/10-14 Spatial Description and Transformation

Lecture 9-3/8/10-14 Spatial Description and Transformation Letue 9-8- tl Deton nd nfomton Homewo No. Due 9. Fme ngement onl. Do not lulte...8..7.8 Otonl et edt hot oof tht = - Homewo No. egned due 9 tud eton.-.. olve oblem:.....7.8. ee lde 6 7. e Mtlb on. f oble.

More information

Class Summary. be functions and f( D) , we define the composition of f with g, denoted g f by

Class Summary. be functions and f( D) , we define the composition of f with g, denoted g f by Clss Summy.5 Eponentil Functions.6 Invese Functions nd Logithms A function f is ule tht ssigns to ech element D ectly one element, clled f( ), in. Fo emple : function not function Given functions f, g:

More information

Course Updates. Reminders: 1) Assignment #8 available. 2) Chapter 28 this week.

Course 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 information

Chapter 21: Electric Charge and Electric Field

Chapter 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 information

Topics for Review for Final Exam in Calculus 16A

Topics for Review for Final Exam in Calculus 16A Topics fo Review fo Finl Em in Clculus 16A Instucto: Zvezdelin Stnkov Contents 1. Definitions 1. Theoems nd Poblem Solving Techniques 1 3. Eecises to Review 5 4. Chet Sheet 5 1. Definitions Undestnd the

More information

This immediately suggests an inverse-square law for a "piece" of current along the line.

This 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 information

Chapter 10 Angular Momentum

Chapter 10 Angular Momentum Chpte Angul omentum Conceptul Polems Tue o lse: () two vectos e exctl opposte n decton, the vecto poduct must e zeo. () The mgntude o the vecto poduct o two vectos s t mnmum when the two vectos e pependcul.

More information

Physics 121 Sample Common Exam 2 Rev2 NOTE: ANSWERS ARE ON PAGE 7. Instructions:

Physics 121 Sample Common Exam 2 Rev2 NOTE: ANSWERS ARE ON PAGE 7. Instructions: Physcs 121 Smple Common Exm 2 Rev2 NOTE: ANSWERS ARE ON PAGE 7 Nme (Prnt): 4 Dgt ID: Secton: Instructons: Answer ll 27 multple choce questons. You my need to do some clculton. Answer ech queston on the

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

III. Electromechanical Energy Conversion

III. Electromechanical Energy Conversion . Electoancal Enegy Coneson Schematc epesentaton o an toancal enegy coneson ece coppe losses coe losses (el losses) ancal losses Deental enegy nput om tcal souce: W V t Rt e t t W net ancal enegy output

More information

Chapter 25 Electric Potential

Chapter 25 Electric Potential Chpte 5 lectic Potentil consevtive foces -> potentil enegy - Wht is consevtive foce? lectic potentil = U / : the potentil enegy U pe unit chge is function of the position in spce Gol:. estblish the eltionship

More information

Two kurtosis measures in a simulation study

Two kurtosis measures in a simulation study Two kuto meue n multon tudy Ann M Fo Deptment o Quntttve Method o Economc nd Bune Scence Unvety o Mlno-Bcocc nn.o@unmb.t CNAM, P COMPSTAT 00 Augut 3, 00 Ovevew The IF (SIF) nd t ole n kuto tude Fom nequlty

More information

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

Prerna Tower, Road No 2, Contractors Area, Bistupur, Jamshedpur , Tel (0657) , R Pen Towe Rod No Conttos Ae Bistupu Jmshedpu 8 Tel (67)89 www.penlsses.om IIT JEE themtis Ppe II PART III ATHEATICS SECTION I (Totl ks : ) (Single Coet Answe Type) This setion ontins 8 multiple hoie questions.

More information

Week 8. Topic 2 Properties of Logarithms

Week 8. Topic 2 Properties of Logarithms Week 8 Topic 2 Popeties of Logithms 1 Week 8 Topic 2 Popeties of Logithms Intoduction Since the esult of ithm is n eponent, we hve mny popeties of ithms tht e elted to the popeties of eponents. They e

More information

ELECTROSTATICS. 4πε0. E dr. The electric field is along the direction where the potential decreases at the maximum rate. 5. Electric Potential Energy:

ELECTROSTATICS. 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 information

Chapter 2: Electric Field

Chapter 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 information

Assistant Professor: Zhou Yufeng. N , ,

Assistant 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 information

Effects of polarization on the reflected wave

Effects of polarization on the reflected wave Lecture Notes. L Ros PPLIED OPTICS Effects of polrzton on the reflected wve Ref: The Feynmn Lectures on Physcs, Vol-I, Secton 33-6 Plne of ncdence Z Plne of nterfce Fg. 1 Y Y r 1 Glss r 1 Glss Fg. Reflecton

More information

+ r Position Velocity

+ 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 information

Scalars and Vectors Scalar

Scalars and Vectors Scalar Scalas and ectos Scala A phscal quantt that s completel chaacteed b a eal numbe (o b ts numecal value) s called a scala. In othe wods a scala possesses onl a magntude. Mass denst volume tempeatue tme eneg

More information

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3 DEPATMENT OF CIVIL AND ENVIONMENTAL ENGINEEING FLID MECHANICS III Solutions to Poblem Sheet 3 1. An tmospheic vote is moelle s combintion of viscous coe otting s soli boy with ngul velocity Ω n n iottionl

More information

Capítulo. Three Dimensions

Capítulo. Three Dimensions Capítulo Knematcs of Rgd Bodes n Thee Dmensons Mecánca Contents ntoducton Rgd Bod Angula Momentum n Thee Dmensons Pncple of mpulse and Momentum Knetc Eneg Sample Poblem 8. Sample Poblem 8. Moton of a Rgd

More information

Math 4318 : Real Analysis II Mid-Term Exam 1 14 February 2013

Math 4318 : Real Analysis II Mid-Term Exam 1 14 February 2013 Mth 4318 : Rel Anlysis II Mid-Tem Exm 1 14 Febuy 2013 Nme: Definitions: Tue/Flse: Poofs: 1. 2. 3. 4. 5. 6. Totl: Definitions nd Sttements of Theoems 1. (2 points) Fo function f(x) defined on (, b) nd fo

More information

Chapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s:

Chapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s: Chpte 7 Kleene s Theoem 7.1 Kleene s Theoem The following theoem is the most impotnt nd fundmentl esult in the theoy of FA s: Theoem 6 Any lnguge tht cn e defined y eithe egul expession, o finite utomt,

More information

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law Physcs 11b Lectue # Electc Feld Electc Flux Gauss s Law What We Dd Last Tme Electc chage = How object esponds to electc foce Comes n postve and negatve flavos Conseved Electc foce Coulomb s Law F Same

More information

Phys 331: Ch 7,.2 More practice with Unconstrained Lagrange s Equations 1

Phys 331: Ch 7,.2 More practice with Unconstrained Lagrange s Equations 1 Phs 33: Ch 7 Moe ctce wth Unconstne gnge s Eutons We /3 hus / F / Mon /5 We /7 76-8 Genelze Vbles & Clsscl Hltonn (Recoen 79 f ou e h Phs 33) 8- -Bo Centl Foces Relte Coontes Reew E (Ch 5-7) HW7c (7 53

More information

HO 40 Solutions ( ) ˆ. j, and B v. F m x 10-3 kg = i + ( 4.19 x 10 4 m/s)ˆ. (( )ˆ i + ( 4.19 x 10 4 m/s )ˆ j ) ( 1.40 T )ˆ k.

HO 40 Solutions ( ) ˆ. j, and B v. F m x 10-3 kg = i + ( 4.19 x 10 4 m/s)ˆ. (( )ˆ i + ( 4.19 x 10 4 m/s )ˆ j ) ( 1.40 T )ˆ k. .) m.8 x -3 g, q. x -8 C, ( 3. x 5 m/)ˆ, and (.85 T)ˆ The magnetc force : F q (. x -8 C) ( 3. x 5 m/)ˆ (.85 T)ˆ F.98 x -3 N F ma ( ˆ ˆ ) (.98 x -3 N) ˆ o a HO 4 Soluton F m (.98 x -3 N)ˆ.8 x -3 g.65 m.98

More information

of Technology: MIT OpenCourseWare). (accessed MM DD, YYYY). License: Creative Commons Attribution- Noncommercial-Share Alike.

of Technology: MIT OpenCourseWare).   (accessed MM DD, YYYY). License: Creative Commons Attribution- Noncommercial-Share Alike. MIT OpenouseWe http://ocw.mit.edu 6.1/ESD.1J Electomgnetics nd pplictions, Fll 25 Plese use the following cittion fomt: Mkus Zhn, Eich Ippen, nd Dvid Stelin, 6.1/ESD.1J Electomgnetics nd pplictions, Fll

More information

Physics Exam II Chapters 25-29

Physics Exam II Chapters 25-29 Physcs 114 1 Exam II Chaptes 5-9 Answe 8 of the followng 9 questons o poblems. Each one s weghted equally. Clealy mak on you blue book whch numbe you do not want gaded. If you ae not sue whch one you do

More information

SOME REMARKS ON HORIZONTAL, SLANT, PARABOLIC AND POLYNOMIAL ASYMPTOTE

SOME REMARKS ON HORIZONTAL, SLANT, PARABOLIC AND POLYNOMIAL ASYMPTOTE D I D A C T I C S O F A T H E A T I C S No (4) 3 SOE REARKS ON HORIZONTAL, SLANT, PARABOLIC AND POLYNOIAL ASYPTOTE Tdeusz Jszk Abstct I the techg o clculus, we cosde hozotl d slt symptote I ths ppe the

More information

Energy Dissipation Gravitational Potential Energy Power

Energy Dissipation Gravitational Potential Energy Power Lectue 4 Chpte 8 Physics I 0.8.03 negy Dissiption Gvittionl Potentil negy Powe Couse wesite: http://fculty.uml.edu/andiy_dnylov/teching/physicsi Lectue Cptue: http://echo360.uml.edu/dnylov03/physicsfll.html

More information

MAGNETIC EFFECT OF CURRENT & MAGNETISM

MAGNETIC 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 information

Physics 110. Spring Exam #1. April 23, 2008

Physics 110. Spring Exam #1. April 23, 2008 hyc Spng 8 E # pl 3, 8 Ne Soluon Mulple Choce / oble # / 8 oble # / oble #3 / 8 ol / In keepng wh he Unon College polcy on cdec honey, ued h you wll nehe ccep no pode unuhozed nce n he copleon o h wok.

More information

(A) 6.32 (B) 9.49 (C) (D) (E) 18.97

(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 information

Introduction to Numerical Integration Part II

Introduction to Numerical Integration Part II Introducton to umercl Integrton Prt II CS 75/Mth 75 Brn T. Smth, UM, CS Dept. Sprng, 998 4/9/998 qud_ Intro to Gussn Qudrture s eore, the generl tretment chnges the ntegrton prolem to ndng the ntegrl w

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School 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 information

NARAYANA I I T / P M T A C A D E M Y. C o m m o n Pr a c t i c e T e s t 0 9 XI-IC SPARK Date: PHYSICS CHEMISTRY MATHEMATICS

NARAYANA I I T / P M T A C A D E M Y. C o m m o n Pr a c t i c e T e s t 0 9 XI-IC SPARK Date: PHYSICS CHEMISTRY MATHEMATICS . (D). (B). (). (). (D). (A) 7. () 8. (B) 9. (B). (). (A). (D). (B). (). (B) NAAYANA I I T / T A A D E Y XIS-I-IIT-SA (..7) o m m o n c t i c e T e s t 9 XI-I SA Dte:..7 ANSWE YSIS EISTY ATEATIS. (B).

More information

PHYS102 - Electric Energy - Capacitors

PHYS102 - Electric Energy - Capacitors PHYS102 - lectric nerg - Cpcitors Dr. Suess Februr 14, 2007 Plcing Chrges on Conuctors................................................. 2 Plcing Chrges on Conuctors II................................................

More information

Lecture 10. Solution of Nonlinear Equations - II

Lecture 10. Solution of Nonlinear Equations - II Fied point Poblems Lectue Solution o Nonline Equtions - II Given unction g : R R, vlue such tht gis clled ied point o the unction g, since is unchnged when g is pplied to it. Whees with nonline eqution

More information

Chapter Linear Regression

Chapter Linear Regression Chpte 6.3 Le Regesso Afte edg ths chpte, ou should be ble to. defe egesso,. use sevel mmzg of esdul cte to choose the ght cteo, 3. deve the costts of le egesso model bsed o lest sques method cteo,. use

More information

2010 Sectional Physics Solution Set

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

More information

5.1 Estimating with Finite Sums Calculus

5.1 Estimating with Finite Sums Calculus 5.1 ESTIMATING WITH FINITE SUMS Emple: Suppose from the nd to 4 th hour of our rod trip, ou trvel with the cruise control set to ectl 70 miles per hour for tht two hour stretch. How fr hve ou trveled during

More information

Go over vector and vector algebra Displacement and position in 2-D Average and instantaneous velocity in 2-D Average and instantaneous acceleration

Go over vector and vector algebra Displacement and position in 2-D Average and instantaneous velocity in 2-D Average and instantaneous acceleration Mh Csquee Go oe eco nd eco lgeb Dsplcemen nd poson n -D Aege nd nsnneous eloc n -D Aege nd nsnneous cceleon n -D Poecle moon Unfom ccle moon Rele eloc* The componens e he legs of he gh ngle whose hpoenuse

More information

Unit_III Complex Numbers: Some Basic Results: 1. If z = x +iy is a complex number, then the complex number z = x iy is

Unit_III Complex Numbers: Some Basic Results: 1. If z = x +iy is a complex number, then the complex number z = x iy is Unt_III Comple Nmbes: In the sstem o eal nmbes R we can sole all qadatc eqatons o the om a b c, a, and the dscmnant b 4ac. When the dscmnant b 4ac

More information

Electric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin

Electric 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 information

1 Using Integration to Find Arc Lengths and Surface Areas

1 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 information

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER Edton CAPTER 8 VECTOR MECANCS FOR ENGNEERS: DYNAMCS Fednand P. Bee E. Russell Johnston, J. Lectue Notes: J. Walt Ole Teas Tech Unvest Knematcs of Rgd Bodes n Thee Dmensons 003 The McGaw-ll Companes, nc.

More information

Solving the Dirac Equation: Using Fourier Transform

Solving the Dirac Equation: Using Fourier Transform McNa Schola Reeach Jounal Volume Atcle Solvng the ac quaton: Ung oue Tanfom Vncent P. Bell mby-rddle Aeonautcal Unvety, Vncent.Bell@my.eau.edu ollow th and addtonal wok at: http://common.eau.edu/na Recommended

More information

AP Physics C: Electricity and Magnetism 2010 Free-Response Questions

AP Physics C: Electricity and Magnetism 2010 Free-Response Questions AP Phyc C: Electcty n Mgnet Fee-Repone Queton The College Bo The College Bo not-fo-poft ebehp octon whoe on to connect tuent to college ucce n oppotunty. Foune n 9, the College Bo copoe of oe thn 5,7 chool,

More information

24-2: Electric Potential Energy. 24-1: What is physics

24-2: Electric Potential Energy. 24-1: What is physics D. Iyad SAADEDDIN Chapte 4: Electc Potental Electc potental Enegy and Electc potental Calculatng the E-potental fom E-feld fo dffeent chage dstbutons Calculatng the E-feld fom E-potental Potental of a

More information

THIS PAGE DECLASSIFIED IAW E

THIS PAGE DECLASSIFIED IAW E THS PAGE DECLASSFED AW E0 2958 BL K THS PAGE DECLASSFED AW E0 2958 THS PAGE DECLASSFED AW E0 2958 B L K THS PAGE DECLASSFED AW E0 2958 THS PAGE DECLASSFED AW EO 2958 THS PAGE DECLASSFED AW EO 2958 THS

More information