Nine lectures for the Maths II course given to first year physics students in the Spring Term. Lecturer: Professor Peter Main

Size: px
Start display at page:

Download "Nine lectures for the Maths II course given to first year physics students in the Spring Term. Lecturer: Professor Peter Main"

Transcription

1 Nine leces o e Ms II cose gien o is e psics sens in e Sping Tem. Lece: Poesso Pee Min Ao e cose Tis cose sows o ow o ieenie n inege ncions o seel iles. I is pesene s n eension o e clcls o le now wic els wi single ile. I is il memics o psiciss since we lie in - imensionl wol giing s les ee iles n z o escie i. Yo will me goo se o is ms in e memicl psics coses in e secon e. Te ge oo o ne is wien in e lngge o memics. Glileo Glilei p://www-ses.o.c./~pm/pmwe/ecing.m

2 Pil ieeniion So o cn ieenie ncions o one ile. Fo ncions o seel iles we m pocee s ollows: Fo cline o is n eig e olme is V = I is consn e e o cnge o V w is V π I is consn e e o cnge o V w is π V I o n e iles we cn sill se ese esls n esigne e eiies s pil eiies. Tese e wien s: I V = wee n e iles en V π n π V Te opeion we e cie o is o pil ieeniion. Te ecipe is es o ieenie pill w one ile eg ll oe iles s consns. Noion Fncions: z = z Pil eiies: z z A moe son noion is oen ope: z z z z Deiniion Fo ncion o one ile: i = en δ δ δ lim Simill we cn wie o : δ δ δ lim δ δ δ lim i.e. pil ieeniion is ciee ieeniing w one ile wile eeping e oes consn. Te genelision o ncions o n nme o iles sol e oios. Geomeicl inepeion z = gies sce i.e. e le o e ncion is ploe in e z-iecion. δ δ

3 z gies e slope o e lines consn gies e slope o e lines consn Emple I e cos Solion: e cos e cos e Cion! in n sin e cos sin I someing cn go wong i will. Hee s n emple o wee o cn esil me ig mise in pil ieeniion. Te elionsips eween Cesin n pol cooines will gie s some simple epessions o ieenie: = cos = sin cosθ θ cn cosθ cosθ I ppes eeoe cosθ!! Te po occs ecse o slc noion. Le s se e complee smol o e pil eiies: θ cosθ cosθ n ee is no eson o e n picl elionsip eween ese wo eiies since ieen iles e el consn n ieen ncions e een ieenie. Moe coecl: om = cos we oin = sec secθ n we in s epece. θ θ θ onl i e sme iles e el consn ing e ieeniion.

4 Hige oe pil eiies Js s o ncions o one ile we m eine ige oe eiies: Te is oe eiies o e n so wic cn lso e wien s wic cn lso e wien s Mie eiies e lso possile ecse e o ncions o n : wic cn lso e wien s wic cn lso e wien s Fonel we e e simpliing c poie ll e eiies eis n e coninos i.e. e opeos n comme. Oe eiies eis e.g. Emple Sow = o = e cos lso Solion: om peios emple we e e cos e cos e sin e cos sin lso e cos e sin n we in Emple e cos e sin e cos sin = Sow = sin ep- sisies onl o =. Tis is Lplce s eqion pil ieenil eqion wic is e impon in memicl psics. Yo will mee i gin in secon e coses.

5 Solion: sin ep cos ep sin ep sin ep sin ep sin ep wen = Tol ieenil Gien e mon wic e ncion cnges wen o iles cnge simlneosl is clle e ol ieenil n is eine s: Le s epess is in ems o pil eiies. Since en Simill Aing n gies Neglecing secon oe smll qniies en gies Te is em in e inl epession is me om e pil eiie wic gies e e o cnge o wi mliplie e cnge in. Te poc eeoe gies e cnge in e o e cnge in. Liewise e secon em gies e cnge in e o e cnge in. I is seen e ol cnge in e ol ieenil is e sm o e cnges e o sis in n sepel. 5

6 Emple Fin e cnge in = e. n o.5 especiel. Solion: wen = : δ δ δ wen e les o n e cnge om o e e δ e δ e δ = e + wen =..5: = e. +. =. e =.9 Te cl cnge is: =..5 =.8.78 =.9 Implici ieeniion I = is eemines s ncion o o ice es i.e. is n implici ncion o since i is no eine eplicil. Tee e wo ws o eemining / in is siion e is o wic o m e seen eoe: δ. ieenie ems in s noml: ieenie ems in s noml: ieenie ems in sing e poc le: emple: cos ieeniing gies sin n n lgeic engemen gies sin sin. since = i.e. consn en = so giing emple: cos sin sin wic is n esie clclion n e is one. Fncion o ncion Fo ncions o single ile we le now o n en

7 7 Tis is someimes clle e cin le. I cn e eene o e cse wee we e ncion o seel iles. Le n en: n Emple I n in cn Beoe soling e polem le s me se we cn ieenie e cn ncion. I o ememe e sn inegl C cn en ieeniing o sies gies immeiel cn Anoe w o oing i is o le = cn en = n sec cn Solion: Use is esl o sole e oiginl polem: Le = / en we e = cn n is ncion o single ile. We lso e n Teeoe cn Also cn Emple Gien in n Solion: We cnno ieenie e epession compleel ecse e ncion is no gien. Howee we cn me some pogess ows e eiies s ollows. Le = en e ncion ecomes n Ten n Emple Sow = - sisies e eqion φ φ wee is n i ieenile ncion n is consn. Solion: Using e sme memicl ies s in e peios emple e powe o clcls is emonse wen we sow e eqion is sisie n

8 8 nnown ncion. Te eqion nown s e we eqion is n impon one in memicl psics s i escies e eio o mn ins o we. Le = en n lso ecomes φ φ φ φ φ φ Cin le I we e gien n en m e epesse s ncion o lone. Te complee eiie / eeoe eiss n i cn e epesse in ems o pil eiies s ollows. Te ol ieenil o is I eeoe ollows i.e. wo ems o e om peiosl gien o ncion o single ile. Emple I e n = = - eemine / wo ieen ws. Solion: Epess s ncion o en e e e e Use e cin le e e e Cin le gin A moe genel epession o e cin le ecomes necess wen we e wee n. Usll wien s: Using ll smols: n

9 9 Dieenil opeos Yo e een sing ieenil opeos o some ime een i o en clle em nme. Fo emple o ieenie o ppl e opeo o poce e esl. Tis m e wien s. Simill. Yo cn ppl e opeo wice s in. Fo : n Moe complice opeos cn ise o wi n. Te cin le gies n is m e wien in ems o ieenil opeos s Te le-n opeo is o e se wen is in ems o n ; e ig-n opeo is o e se wen is in ems o n. Te opeos peom e sme opeion n e eeoe eqilen. Tis m e wien s Te ig-n opeo ells o o ieenie pill w n mlipl en is o e pil eiie w mliplie. Emple I = + wee = n = in sing wo ieen opeos. Solion:. Ssie o n in n se e opeo : giing. Lee in ems o n n se e opeo : Te pil eiies in e opeo e n So

10 Emple eeminion o ieenil opeos Gien = n = epess e opeos n in ems o n. Solion: Te cin le gies n Te pil eiies e: ; ; ; so e opeos ecome: Yo cn se n meo o lie o sole e eqions e ecommene meo is o se Cme s le: eeoe n Cme s le I o en seen Cme s le eoe ee i is s pplie oe. I is ecommene s i nees less lgeic mniplion n oe meos wen pplie o pi o simlneos eqions. Fo e eqions: + = + = e solion is epesse in ems o eeminns s: Te nnowns e n n e pen o eeminns is: Te ls eeminn cll i conins e o le n sie coeiciens. Te eeminn o is nnown is wi e is colmn eplce e s. Te eeminn o n nnown is wi e n colmn eplce e s. sole ese eqions o n

11 Commen Cn we oi ing o sole eqions oing e clclion in ieen w? Fo emple o wi n e cin le gies so e opeos e giing iecl wi n eqilen epession o. Howee on e oole. Te eiie oe is no e ecipocl o in e peios emple. Hee is ncion o n so e ll smol o e eiie is wees in e emple is ncion o n i.e. e eiie is. To oin e eqions = n = will e o e sole o n o epess em s ncions o n. Tis is consiel moe iicl s n soling e eqions in e emple so o cn win is w. Cnge o iles Cesin o pol Sow wee is ncion o n o e eqilen ncion o n n = cos = sin i.e. e epession is cnge om Cesin o pol cooines. Te epession isel is p o Lplce s eqion. Fom e cin le: cos sin sin cos Sole ese eqions o n o gie: cos sin n sin cos Tese epessions lso poie e opeos neee o oin e secon oe eiies: sin cos sin cos Epn e opeo: sin cos sin sin cos cos Now ieenie ememeing o se e poc le wee i pplies: sin cos sin cos sin sin cos sin cos sin cos

12 Collec lie ems n p em in logicl oe: sin sin sin sin cos A simil nlsis gies e epession o : θ θ sin cos cos sin sin Aing em ogee gies e eqie esl: Tlo seies o ncion o wo iles Fo ncion o single ile we e: n n n!! '''! '' ' o leniel: n n n!! '''! ' ' ' Tese wo epessions e e sme wi = +. Fncions o seel iles cn e ee in simil w. Fo wo iles eine e ieenil opeo D. Te Tlo epnsion o o e poin is en:!!! D n D D D n wee D n mens ppl e ieenil opeo n imes o n ele e esl e poin. Le s loo D : Tis is e sme memicl om s inomil epnsion. Wiing o ll e ems in e Tlo epnsion p o oe gies:!! Te lenie om is oine ping = + = + :!!

13 Emple Epn = ep sin s powe seies o e poin / o ems o e secon egee. Hence oin n ppoime le o. /. = ep sin / = e = sin ep sin / = e = cos ep sin / = = sin ep sin / = e = cos ep sin + cos sin ep sin / = = - sin ep sin + cos ep sin / = -e Te Tlo seies o / is: Ping in e les o e eiies gies: ep sin e e e e e e Fo =. n = / e ppoime le o. /.. Usel pope Fo ncions o single ile: e Te coec le o. / ep.sin. I cn e wien s PQ en Tlo epnsion o = [Tlo epnsion o P] [Tlo epnsion o Q] Fo ncion o wo iles: I cn e wien s PQ en Tlo epnsion o = [Tlo epnsion o P] [Tlo epnsion o Q]

14 Inegion Recll e e ne ce is gien inegion: Elemen o e = lim Tol e In e limi s ol e Dole inegls Le s een is ie o gie n epession o e olme ne sce. Te ncion z = gies e sce n e olme eween is n gien egion in e -plne is e olme o e clcle. Te olme ssocie wi ec elemen o e in e -plne is n e sm o ese gies e esie olme. Howee is is one in e ssemic mnne. Le e olme e one : Top z = Boom -plne Sies ce ABCD Le e ce ABC e = Le e ce ADC e = Now e n elemen slice o consn. A D δ = φ C Elemen o olme = Teeoe olme o elemen slice lim δ B = φ lim So ol olme ne sce In is ole inegl noe e is inegion is oe wee is ee s consn. Dole inegls e no nomll wien in is w e moe commonl epesse wio ces s: o In e oe nlsis i is possile o inecnge e oles o n o oin secon ole inegl eql in le o e is. Ting elemen slices o consn les o e ole inegl:

15 Volme ne sce = c wee e olme is one on e le = ψ n on e ig = ψ. We cn eeoe eqe e wo ole inegls: c n we e cnge e oe o inegion. On e le we inege oe is oling consn en inege oe. On e ig inege oe is oling consn en inege oe. Noe e limis on e wo ole inegls e e ieen. o escie e sme iel o inegion. Cnging e oe o inegion Howee e Yo cn onl sel ece e limis on ole inegl wing e iel o inegion. Te e ollowing inegl s n emple. Te limis on e inegion oe sow e iel o inegion is one e lines = n =. Teeoe e iel o inegion is s sown in e igm wi going om o / s gien e limis on e inegion oe. On ineging oe is e igm sows goes om e line o. Tese eeoe om e limis on e inegl n e nge o is seen o e < < /. We eeoe e: In is secon emple e ole inegl s o e spli ino e sm o wo inegls o ccommoe e ieen lowe limis wen ineging oe is. c = ψ A = D B = = ψ C wen < 5

16 I is impon e iel o inegion sol e e sme eoe n e cnging e oe o inegion. Emples eling ole inegls. Ele oe e e one = n =. Vei e sme esl is oine wen e oe o inegion is eese. Solion: Te limis on e inegls e o e oine om igm o e iel o inegion. Ineging oe is: Ineging oe is: Ele sin Solion: Tee is no es w o peoming e inegion oe so consie cnging e oe o inegion. Tis cn onl e one ploing o e iel o inegion is. Te inegl ecomes sin Noe sin is consn in e inegion oe so i cn e en o o inegl. Te inegion oe is now iil: sin sin sin n e inegion oe now ecomes possile ecse e inegn s cnge. Use e ssiion en n e inegl ecomes:

17 sin cos Sepion o iles In e specil cse wee e limis o inegion e consn no ncions o e iles n e inegn is o e om FG we e: F G c F G Tis is e poc o wo single inegls cn e ele inepenenl o ec oe. c Dole inegls in pol cooines = cos; = sin Uni ecos ˆ n θˆ e eine o lie in e iecions o incesing n especiel. Cnging om Cesins o pols in ole inegl is n emple o ssiing o o iles simlneosl. θˆ ˆ is n elemen o e in e -plne. Te eqilen elemen o e in e -plne is: = i.e. elemen o e = = Noe is no eplce e imensions e wong! A A Cnge o oe o inegion ccos cos ccos = cos Te eqion = cos gies cicle o is cene on. Ce line in cicle: inege oe consn. Sig line in cicle: inege oe consn. Emple Ele wee R is e egion one + = R 7

18 8 Solion: Coneing o pol cooines will simpli o e inegn n e escipion o e iel o inegion. = cos = sin = Emple Ele 5 Solion: Tnsom o pol cooines o simpli e inegn: = cos = sin = cos cos Tee is sepion o iles so is is poc o wo single inegls. Use e ieni cos = cos n le + = en = 5 5 cos Tiple inegls Te memicl ies gie s ole inegls cn esil e eene o iple inegls: Inegn = z Fiel o inegion = olme in D spce Elemen o olme = z = V Repee inegl: z z In oe o el wi iple inegls we nee o loo D cooine ssems. Speicl pol cooines A poin P z in Cesin cooines is lso in speicl pols wee = sin cos = sin sinz = cos + = = ˆ θˆ φˆ

19 A P ni ecos ˆ θˆ φˆ e eine o lie in e iecions o incesing n especiel. Tese ecos om ig-ne oogonl cooine ssem poin. A sce o consn is spee A sce o consn is cone A sce o consn is semi-ininie plne Tese sces inesec e poin Te elemen o olme is mos esil oine geomeicll: Te o in e igm s sies o sin n Tis mes e elemen o olme = V = z = sin = sin Clinicl pol cooines A poin P z in Cesin cooines is lso z in clinicl pols wee = cos = sin z = z A P ni ecos ˆ θˆ zˆ in e iecions o incesing z om n oogonl ig-ne ssem P. A sce o consn is cline A sce o consn is semi-ininie plne A sce o consn z is n ininie plne Tese sces inesec e poin z. Te elemen o olme is oine geomeicll: Te o in e igm s sies o n z Tis mes e elemen o olme = V = z = z = z ẑ ˆ θˆ 9

20 Soli ngle Now we e ino D cooine ssems le s loo e mesemen o ngles in ee-imensionl spce. I will e es o s wi ngles o e mili wi in wo-imensionl spce: Te igm sows n c o cicle o is. Te leng o e c is. Te ngle is e io o e leng o e c o e is i.e. leng o c is ins. I e c is lengene o complee e cicle e ngle ecomes cicmeence o cicle ins. is In D ngles e clle soli ngles e e eine in simil w o ngles in D. Te igm sows p o spee o is wic sens soli ngle is cene. e o speicl sce Te ngle is eine s is o spee seins. I e sce is eene o complee spee e soli ngle e cene ecomes sce e o e spee seins. is o e spee Soli ngles e se in psics o emple o escie e D ngle ino wic soce o iion m ie. Emple o iple inegl A simple illsion o e se o iple inegl is o clcle e olme o spee o is. Solion: Use speicl pol cooines n inege e elemen o olme oe e spee. V spee V θ sin θ sin θ θ.. Me se o nesn e ssignmen o e limis: Te inegion oe is long line om e oigin o e sce o e spee. Te inegion oe oes is line o e oigin o sweep o e e o semicicle. Te inegion oe oes e semicicle o e z-is o sweep o e olme o e spee. Te limis on e ollowing iple inegl lso gie e iel o inegion s spee: c o cicle cp o spee sin θ θ..

21 Cn e olme o e spee ell e zeo? In speicl pols e elemen o olme V is sin In e is inegl e nge o is om o so V is lws posiie. Howee in e secon inegl V is negie oe l is nge cncelling o e posiie coniion o e inegl n ening p wi zeo. I o inen o e negie olme en e secon inegl is peecl coec o nee o e we o w o e oing. Dimensions in inegls emples o pplicions in psics I epesens e olme ne sce w oes z z epesen? Te ole inegl onl epesens olme i n ll e e imensions o leng. Te imension o e inegn is en leng wic is olme. We e le se iple inegl o eemine e olme o spee go c n cec e imensions e coec. No eeing is mese in mees n we nee o consie e imensions o e qniies in e inegl wen ppling i o psics. Te ing o noe is e smols ec. e no js lels emining o o e iles oe wic o peom e inegion e e lso psicl qniies wi imensions. Le s loo some emples o ow o consc ios inegls o pplicions in psics.. A egion o spce conins n elecic cge ensi o z coloms/m. W is e ol cge in picl olme V? Cge in elemen o olme = z z Teeoe ol cge in olme V = V. Volme o iel o inegion = V ρ z z V m. coloms.. Te spee o picle cnges wi ime s. Fin e isnce elle in ime T. Disnce elle in ime = Teeoe ol isnce elle in ime T = mees.. Te ensi o in see o meil ies s g/m. Fin is ol mss. Mss o elemen o e = Teeoe ol mss o see = M = R T g wee R eines e spe o e see. 5. Te men ensi o e see in e peios emple is oine iiing e ol mss e e i.e. men ensi = g/m wee A is e A e o e see. Simil inegls will eemine e ege le o ncion in D o D spce: Aege o eween = n = is R

22 Aege o z wiin e olme V = V V z z. Anoe impon se o inegls is o eemine e cene o mss o n ojec. Using e sme in see is in emple e mss is g so is momen o e -is is g m. Te ol momen o e -is is eeoe n is ms e eql o M wee M is e ol mss R n is e -cooine o e cene o mss. We eeoe e o e cooines o e cene o mss: n M M R 7. A sligl moe enos se o mliple inegl is in e clclion o momen o inei. Te momen o inei o poin mss m isnce om e is o oion is m. Fo o o ensi z g/m e poin mss z is z z I z is e oion is e isnce om e is o e poin mss is Te momen o inei o e poin mss is eeoe Teeoe e momen o inei o e complee o = Emple R V z z z z Fin e posiion o e cenoi o niom soli cone o eig n se is R. Solion: Te cenoi is e cene o mss o o o niom ensi. B smme e cenoi lies on e cone is so onl e z-cooine is eqie. Using e inegls in e peios emples e z- cooine o e cenoi is gien : z V cone z V Tee is coice o cooine ssem clinicl pols will e e esies. Elemen o olme = V = z Te ce sce o e cone is gien e iple inegl is R z so z R V z R z R z R R z z z z z z z R B e olme o e cone is gien V R R so z R

23 Volme o cone I o ogoen o nee nown e oml o e olme o cone se in e peios emple we cn eie i ee. We e le ece e limis on iple inegl escie cone so we cn immeiel se em ee: V cone V Emple cone z z R z z R R z R z Deemine e ol mss n men ensi o o occping e posiie ocn wee n z e ll posiie one + + z = n wose ensi is z = z g/m. W e e psicl imensions o e consn? Using is esl conim e psicl imensions o o nswes o p e coec. Solion Mss o elemen o olme = z V g Teeoe ol mss = V z V g Use speicl pol cooines: = sin cos; = sin sin; z = cosv = sin ol mss sin θ cosθ sinφ cosφ sin θ θ φ 5 sin θ cosθ θ sinφ cosφ φ le = sin en = cos lso se e ieni sin cos = sin cos φ sinφ φ 8 g Men ensi = ol mss olme 8 g m Te imensions o n z e ll mees. Since z is ensi is imensions ms e g m - wien s [z] = g m - Tis mes [] m = g m - so [] = g m - Te mss o e ojec is 8 g. Fom e oe we e [ ] = g m - m = g Te men ensi o e ojec is 8 g m - n [ ] = g m - m = g m -.

24

Classification of Equations Characteristics

Classification of Equations Characteristics Clssiiion o Eqions Cheisis Consie n elemen o li moing in wo imensionl spe enoe s poin P elow. The ph o P is inie he line. The posiion ile is s so h n inemenl isne long is s. Le he goening eqions e epesene

More information

Some algorthim for solving system of linear volterra integral equation of second kind by using MATLAB 7 ALAN JALAL ABD ALKADER

Some algorthim for solving system of linear volterra integral equation of second kind by using MATLAB 7 ALAN JALAL ABD ALKADER . Soe lgoi o solving syse o line vole inegl eqion o second ind by sing MATLAB 7 ALAN JALAL ABD ALKADER College o Edcion / Al- Msnsiiy Univesiy Depen o Meics تقديم البحث :-//7 قبول النشر:- //. Absc ( /

More information

Invert and multiply. Fractions express a ratio of two quantities. For example, the fraction

Invert and multiply. Fractions express a ratio of two quantities. For example, the fraction Appendi E: Mnipuling Fions Te ules fo mnipuling fions involve lgei epessions e el e sme s e ules fo mnipuling fions involve numes Te fundmenl ules fo omining nd mnipuling fions e lised elow Te uses of

More information

ME 141. Engineering Mechanics

ME 141. Engineering Mechanics ME 141 Engineeing Mechnics Lecue 13: Kinemics of igid bodies hmd Shhedi Shkil Lecue, ep. of Mechnicl Engg, UET E-mil: sshkil@me.bue.c.bd, shkil6791@gmil.com Websie: eche.bue.c.bd/sshkil Couesy: Veco Mechnics

More information

Faraday s Law. To be able to find. motional emf transformer and motional emf. Motional emf

Faraday s Law. To be able to find. motional emf transformer and motional emf. Motional emf Objecie F s w Tnsfome Moionl To be ble o fin nsfome. moionl nsfome n moionl. 331 1 331 Mwell s quion: ic Fiel D: Guss lw :KV : Guss lw H: Ampee s w Poin Fom Inegl Fom D D Q sufce loop H sufce H I enclose

More information

ISSUES RELATED WITH ARMA (P,Q) PROCESS. Salah H. Abid AL-Mustansirya University - College Of Education Department of Mathematics (IRAQ / BAGHDAD)

ISSUES RELATED WITH ARMA (P,Q) PROCESS. Salah H. Abid AL-Mustansirya University - College Of Education Department of Mathematics (IRAQ / BAGHDAD) Eoen Jonl of Sisics n Poiliy Vol. No..9- Mc Plise y Eoen Cene fo Resec Tinin n Develoen UK www.e-onls.o ISSUES RELATED WITH ARMA PQ PROCESS Sl H. Ai AL-Msnsiy Univesiy - Collee Of Ecion Deen of Meics IRAQ

More information

Axis. Axis. Axis. Solid cylinder (or disk) about. Hoop about. Annular cylinder (or ring) about central axis. central axis.

Axis. Axis. Axis. Solid cylinder (or disk) about. Hoop about. Annular cylinder (or ring) about central axis. central axis. Insucos: Fiel/che/Deweile PYSICS DEPATENT PY 48 Em ch 5, 5 Nme pin, ls fis: Signue: On m hono, I he neihe gien no eceie unuhoie i on his eminion. YOU TEST NUBE IS TE 5-DIGIT NUBE AT TE TOP OF EAC PAGE.

More information

Ch.4 Motion in 2D. Ch.4 Motion in 2D

Ch.4 Motion in 2D. Ch.4 Motion in 2D Moion in plne, such s in he sceen, is clled 2-dimensionl (2D) moion. 1. Posiion, displcemen nd eloci ecos If he picle s posiion is ( 1, 1 ) 1, nd ( 2, 2 ) 2, he posiions ecos e 1 = 1 1 2 = 2 2 Aege eloci

More information

1. Kinematics of Particles

1. Kinematics of Particles 1. Kinemics o Picles 1.1 Inoducion o Dnmics Dnmics - Kinemics: he sud o he geome o moion; ele displcemen, eloci, cceleion, nd ime, wihou eeence o he cuse o he moion. - Kineics: he sud o he elion eising

More information

Physics 201, Lecture 5

Physics 201, Lecture 5 Phsics 1 Lecue 5 Tod s Topics n Moion in D (Chp 4.1-4.3): n D Kinemicl Quniies (sec. 4.1) n D Kinemics wih Consn Acceleion (sec. 4.) n D Pojecile (Sec 4.3) n Epeced fom Peiew: n Displcemen eloci cceleion

More information

15/03/1439. Lecture 4: Linear Time Invariant (LTI) systems

15/03/1439. Lecture 4: Linear Time Invariant (LTI) systems Lecre 4: Liner Time Invrin LTI sysems 2. Liner sysems, Convolion 3 lecres: Implse response, inp signls s coninm of implses. Convolion, discree-ime nd coninos-ime. LTI sysems nd convolion Specific objecives

More information

The sphere of radius a has the geographical form. r (,)=(acoscos,acossin,asin) T =(p(u)cos v, p(u)sin v,q(u) ) T.

The sphere of radius a has the geographical form. r (,)=(acoscos,acossin,asin) T =(p(u)cos v, p(u)sin v,q(u) ) T. Che 5. Dieeil Geome o Sces 5. Sce i meic om I 3D sce c be eeseed b. Elici om z =. Imlici om z = 3. Veco om = o moe geel =z deedig o wo mees. Emle. he shee o dis hs he geoghicl om =coscoscossisi Emle. he

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

PHYSICS 102. Intro PHYSICS-ELECTROMAGNETISM

PHYSICS 102. Intro PHYSICS-ELECTROMAGNETISM PHYS 0 Suen Nme: Suen Numbe: FAUTY OF SIENE Viul Miem EXAMINATION PHYSIS 0 Ino PHYSIS-EETROMAGNETISM Emines: D. Yoichi Miyh INSTRUTIONS: Aemp ll 4 quesions. All quesions hve equl weighs 0 poins ech. Answes

More information

Chapter 4 Circular and Curvilinear Motions

Chapter 4 Circular and Curvilinear Motions Chp 4 Cicul n Cuilin Moions H w consi picls moing no long sigh lin h cuilin moion. W fis su h cicul moion, spcil cs of cuilin moion. Anoh mpl w h l sui li is h pojcil..1 Cicul Moion Unifom Cicul Moion

More information

f(x) dx with An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples dx x x 2

f(x) dx with An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples dx x x 2 Impope Inegls To his poin we hve only consideed inegls f() wih he is of inegion nd b finie nd he inegnd f() bounded (nd in fc coninuous ecep possibly fo finiely mny jump disconinuiies) An inegl hving eihe

More information

Motion on a Curve and Curvature

Motion on a Curve and Curvature Moion on Cue nd Cuue his uni is bsed on Secions 9. & 9.3, Chpe 9. All ssigned edings nd execises e fom he exbook Objecies: Mke cein h you cn define, nd use in conex, he ems, conceps nd fomuls lised below:

More information

Physics 232 Exam I Feb. 13, 2006

Physics 232 Exam I Feb. 13, 2006 Phsics I Fe. 6 oc. ec # Ne..5 g ss is ched o hoizol spig d is eecuig siple hoic oio. The oio hs peiod o.59 secods. iiil ie i is oud o e 8.66 c o he igh o he equiliiu posiio d oig o he le wih eloci o sec.

More information

() t. () t r () t or v. ( t) () () ( ) = ( ) or ( ) () () () t or dv () () Section 10.4 Motion in Space: Velocity and Acceleration

() t. () t r () t or v. ( t) () () ( ) = ( ) or ( ) () () () t or dv () () Section 10.4 Motion in Space: Velocity and Acceleration Secion 1.4 Moion in Spce: Velociy nd Acceleion We e going o dive lile deepe ino somehing we ve ledy inoduced, nmely () nd (). Discuss wih you neighbo he elionships beween posiion, velociy nd cceleion you

More information

CSE590B Lecture 4 More about P 1

CSE590B Lecture 4 More about P 1 SE590 Lece 4 Moe abo P 1 Tansfoming Tansfomaions James. linn Jimlinn.om h://coses.cs.washingon.ed/coses/cse590b/13a/ Peviosly On SE590b Tansfomaions M M w w w w w The ncion w w w w w w 0 w w 0 w 0 w The

More information

Rotations.

Rotations. oons j.lbb@phscs.o.c.uk To s summ Fmes of efeence Invnce une nsfomons oon of wve funcon: -funcons Eule s ngles Emple: e e - - Angul momenum s oon geneo Genec nslons n Noehe s heoem Fmes of efeence Conse

More information

Compressive modulus of adhesive bonded rubber block

Compressive modulus of adhesive bonded rubber block Songklnkin J. Sci. Tecnol. 0 (, -5, M. - Ap. 008 p://www.sjs.ps.c. Oiginl Aicle Compessive modls of desive bonded bbe block Coeny Decwykl nd Wiiy Tongng * Depmen of Mecnicl Engineeing, Fcly of Engineeing,

More information

LECTURE 5. is defined by the position vectors r, 1. and. The displacement vector (from P 1 to P 2 ) is defined through r and 1.

LECTURE 5. is defined by the position vectors r, 1. and. The displacement vector (from P 1 to P 2 ) is defined through r and 1. LECTURE 5 ] DESCRIPTION OF PARTICLE MOTION IN SPACE -The displcemen, veloci nd cceleion in -D moion evel hei veco nue (diecion) houh he cuion h one mus p o hei sin. Thei full veco menin ppes when he picle

More information

Science Advertisement Intergovernmental Panel on Climate Change: The Physical Science Basis 2/3/2007 Physics 253

Science Advertisement Intergovernmental Panel on Climate Change: The Physical Science Basis   2/3/2007 Physics 253 Science Adeisemen Inegoenmenl Pnel on Clime Chnge: The Phsicl Science Bsis hp://www.ipcc.ch/spmfeb7.pdf /3/7 Phsics 53 hp://www.fonews.com/pojecs/pdf/spmfeb7.pdf /3/7 Phsics 53 3 Sus: Uni, Chpe 3 Vecos

More information

D zone schemes

D zone schemes Ch. 5. Enegy Bnds in Cysls 5.. -D zone schemes Fee elecons E k m h Fee elecons in cysl sinα P + cosα cosk α cos α cos k cos( k + π n α k + πn mv ob P 0 h cos α cos k n α k + π m h k E Enegy is peiodic

More information

1. Find a basis for the row space of each of the following matrices. Your basis should consist of rows of the original matrix.

1. Find a basis for the row space of each of the following matrices. Your basis should consist of rows of the original matrix. Mh 7 Exm - Prcice Prolem Solions. Find sis for he row spce of ech of he following mrices. Yor sis shold consis of rows of he originl mrix. 4 () 7 7 8 () Since we wn sis for he row spce consising of rows

More information

2IV10/2IV60 Computer Graphics

2IV10/2IV60 Computer Graphics I0/I60 omper Grphics Eminion April 6 0 4:00 7:00 This eminion consis of for qesions wih in ol 6 sqesion. Ech sqesion weighs eqll. In ll cses: EXPLAIN YOUR ANSWER. Use skeches where needed o clrif or nswer.

More information

Special Vector Calculus Session For Engineering Electromagnetics I. by Professor Robert A. Schill Jr.

Special Vector Calculus Session For Engineering Electromagnetics I. by Professor Robert A. Schill Jr. pecil Vect Clculus essin Engineeing Electmgnetics I Pfess et. cill J. pecil Vect Clculus essin f Engineeing Electmgnetics I. imple cmputtin f cul diegence nd gdient f ect. [peicl Cdinte stem] Cul Diegence

More information

Homework 5 for BST 631: Statistical Theory I Solutions, 09/21/2006

Homework 5 for BST 631: Statistical Theory I Solutions, 09/21/2006 Homewok 5 fo BST 63: Sisicl Theoy I Soluions, 9//6 Due Time: 5:PM Thusy, on 9/8/6. Polem ( oins). Book olem.8. Soluion: E = x f ( x) = ( x) f ( x) + ( x ) f ( x) = xf ( x) + xf ( x) + f ( x) f ( x) Accoing

More information

Control Volume Derivation

Control Volume Derivation School of eospace Engineeing Conol Volume -1 Copyigh 1 by Jey M. Seizman. ll ighs esee. Conol Volume Deiaion How o cone ou elaionships fo a close sysem (conol mass) o an open sysem (conol olume) Fo mass

More information

Motion. ( (3 dim) ( (1 dim) dt. Equations of Motion (Constant Acceleration) Newton s Law and Weight. Magnitude of the Frictional Force

Motion. ( (3 dim) ( (1 dim) dt. Equations of Motion (Constant Acceleration) Newton s Law and Weight. Magnitude of the Frictional Force Insucos: ield/mche PHYSICS DEPARTMENT PHY 48 Em Sepeme 6, 4 Nme pin, ls fis: Signue: On m hono, I he neihe gien no eceied unuhoied id on his eminion. YOUR TEST NUMBER IS THE 5-DIGIT NUMBER AT THE TOP O

More information

Axis Thin spherical shell about any diameter

Axis Thin spherical shell about any diameter Insucos: Fiel/che/Deweile PYSICS DEPATET PY 48 Finl Em Apil 5, 5 me pin, ls fis: Signue: On m hono, I he neihe gien no eceie unuhoie i on his eminion. YOU TEST UBE IS TE 5-DIGIT UBE AT TE TOP OF EAC PAGE.

More information

10.3 The Quadratic Formula

10.3 The Quadratic Formula . Te Qudti Fomul We mentioned in te lst setion tt ompleting te sque n e used to solve ny qudti eqution. So we n use it to solve 0. We poeed s follows 0 0 Te lst line of tis we ll te qudti fomul. Te Qudti

More information

Physics 232 Exam I Feb. 14, 2005

Physics 232 Exam I Feb. 14, 2005 Phsics I Fe., 5 oc. ec # Ne..5 g ss is ched o hoizol spig d is eecuig siple hoic oio wih gul eloci o dissec. gie is i ie i is oud o e 8 c o he igh o he equiliiu posiio d oig o he le wih eloci o.5 sec..

More information

FM Applications of Integration 1.Centroid of Area

FM Applications of Integration 1.Centroid of Area FM Applicions of Inegrion.Cenroid of Are The cenroid of ody is is geomeric cenre. For n ojec mde of uniform meril, he cenroid coincides wih he poin which he ody cn e suppored in perfecly lnced se ie, is

More information

An object moving with speed v around a point at distance r, has an angular velocity. m/s m

An object moving with speed v around a point at distance r, has an angular velocity. m/s m Roion The mosphere roes wih he erh n moions wihin he mosphere clerly follow cure phs (cyclones, nicyclones, hurricnes, ornoes ec.) We nee o epress roion quniiely. For soli objec or ny mss h oes no isor

More information

Section P.1 Notes Page 1 Section P.1 Precalculus and Trigonometry Review

Section P.1 Notes Page 1 Section P.1 Precalculus and Trigonometry Review Secion P Noe Pge Secion P Preclculu nd Trigonomer Review ALGEBRA AND PRECALCULUS Eponen Lw: Emple: 8 Emple: Emple: Emple: b b Emple: 9 EXAMPLE: Simplif: nd wrie wi poiive eponen Fir I will flip e frcion

More information

Mathcad Lecture #4 In-class Worksheet Vectors and Matrices 1 (Basics)

Mathcad Lecture #4 In-class Worksheet Vectors and Matrices 1 (Basics) Mh Lr # In-l Workh Vor n Mri (Bi) h n o hi lr, o hol l o: r mri n or in Mh i mri prorm i mri mh oprion ol m o linr qion ing mri mh. Cring Mri Thr r rl o r mri. Th "Inr Mri" Wino (M) B K Poin Rr o

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

Average & instantaneous velocity and acceleration Motion with constant acceleration

Average & instantaneous velocity and acceleration Motion with constant acceleration Physics 7: Lecure Reminders Discussion nd Lb secions sr meeing ne week Fill ou Pink dd/drop form if you need o swich o differen secion h is FULL. Do i TODAY. Homework Ch. : 5, 7,, 3,, nd 6 Ch.: 6,, 3 Submission

More information

Technical Vibration - text 2 - forced vibration, rotational vibration

Technical Vibration - text 2 - forced vibration, rotational vibration Technicl Viion - e - foced viion, oionl viion 4. oced viion, viion unde he consn eenl foce The viion unde he eenl foce. eenl The quesion is if he eenl foce e is consn o vying. If vying, wh is he foce funcion.

More information

Hyperbolic Heat Equation as Mathematical Model for Steel Quenching of L-shape and T-shape Samples, Direct and Inverse Problems

Hyperbolic Heat Equation as Mathematical Model for Steel Quenching of L-shape and T-shape Samples, Direct and Inverse Problems SEAS RANSACIONS o HEA MASS RANSER Bos M Be As Bs Hpeo He Eo s Me Moe o See Qe o L-spe -spe Spes De Iese Poes ABIA BOBINSKA o Pss Mes es o L Ze See 8 L R LAIA e@o MARARIA BIKE ANDRIS BIKIS Ise o Mes Cope

More information

T h e C S E T I P r o j e c t

T h e C S E T I P r o j e c t T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T

More information

ANALYSIS OF KINEMATICS AND KINETOSTATICS OF FOUR-BAR LINKAGE MECHANISM BASED ON GIVEN PROGRAM

ANALYSIS OF KINEMATICS AND KINETOSTATICS OF FOUR-BAR LINKAGE MECHANISM BASED ON GIVEN PROGRAM SINTII POINGS IV INTNTIONL ONGSS "MINS. TNOLОGIS. MTILS." 7 - SUMM SSSION NLSIS O KINMTIS N KINTOSTTIS O OU- LINKG MNISM S ON GIVN POGM W ISSN - PINT ISSN - Pof.soc.. Shl Pof.soc.. Likj. * Pof.ss.. ji.

More information

AP Calculus AB Exam Review Sheet B - Session 1

AP Calculus AB Exam Review Sheet B - Session 1 AP Clcls AB Em Review Sheet B - Session Nme: AP 998 # Let e the nction given y e.. Find lim nd lim.. Find the solte minimm vle o. Jstiy tht yo nswe is n solte minimm. c. Wht is the nge o? d. Conside the

More information

GEOMETRY Properties of lines

GEOMETRY Properties of lines www.sscexmtuto.com GEOMETRY Popeties of lines Intesecting Lines nd ngles If two lines intesect t point, ten opposite ngles e clled veticl ngles nd tey ve te sme mesue. Pependicul Lines n ngle tt mesues

More information

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy

More information

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

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

More information

Dividing Algebraic Fractions

Dividing Algebraic Fractions Leig Eheme Tem Model Awe: Mlilig d Diidig Algei Fio Mlilig d Diidig Algei Fio d gide ) Yo e he me mehod o mlil lgei io o wold o mlil meil io. To id he meo o he we o mlil he meo o he io i he eio. Simill

More information

Derivatives of Inverse Trig Functions

Derivatives of Inverse Trig Functions Derivaives of Inverse Trig Fncions Ne we will look a he erivaives of he inverse rig fncions. The formlas may look complicae, b I hink yo will fin ha hey are no oo har o se. Yo will js have o be carefl

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

Axis. Axis. Axis. Solid cylinder (or disk) about. Hoop about. Annular cylinder (or ring) about central axis. central axis.

Axis. Axis. Axis. Solid cylinder (or disk) about. Hoop about. Annular cylinder (or ring) about central axis. central axis. Insucos: Fel/ce PYSICS DEPATET PY 48 Em Ocoe 3, 4 me pn, ls fs: Sgnue: On m ono, I e nee gen no ecee unuoe on s emnon. YOU TEST UBE IS TE 5-DIGIT UBE AT TE TOP OF EAC PAGE. Coe ou es nume on ou nswe see

More information

1. Viscosities: μ = ρν. 2. Newton s viscosity law: 3. Infinitesimal surface force df. 4. Moment about the point o, dm

1. 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

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

Outline. Part 1, Topic 3 Separation of Charge and Electric Fields. Dr. Sven Achenbach - based on a script by Dr. Eric Salt - Outline

Outline. Part 1, Topic 3 Separation of Charge and Electric Fields. Dr. Sven Achenbach - based on a script by Dr. Eric Salt - Outline S. Achench: PHYS 55 (P, Topic 3) Hnous p. Ouline slie # Cunell & Johnson Univesiy of Sskchewn Unegue Couse Phys 55 Inoucion o leciciy n Mgneism conucos & insulos 6 8.3 pllel ple cpcios 68 8.9, 9.5 enegy

More information

Mathematical Modeling

Mathematical Modeling ME pplie Engineering nlsis Chper Mhemicl Moeling Professor Ti-Rn Hsu, Ph.D. Deprmen of Mechnicl n erospce Engineering Sn Jose Se Universi Sn Jose, Cliforni, US Jnur Chper Lerning Ojecives Mhemicl moeling

More information

PHYSICS 1210 Exam 1 University of Wyoming 14 February points

PHYSICS 1210 Exam 1 University of Wyoming 14 February points PHYSICS 1210 Em 1 Uniersiy of Wyoming 14 Februry 2013 150 poins This es is open-noe nd closed-book. Clculors re permied bu compuers re no. No collborion, consulion, or communicion wih oher people (oher

More information

Physic 231 Lecture 4. Mi it ftd l t. Main points of today s lecture: Example: addition of velocities Trajectories of objects in 2 = =

Physic 231 Lecture 4. Mi it ftd l t. Main points of today s lecture: Example: addition of velocities Trajectories of objects in 2 = = Mi i fd l Phsic 3 Lecure 4 Min poins of od s lecure: Emple: ddiion of elociies Trjecories of objecs in dimensions: dimensions: g 9.8m/s downwrds ( ) g o g g Emple: A foobll pler runs he pern gien in he

More information

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes]

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes] ENGI 44 Avance alculus fo Engineeing Faculy of Engineeing an Applie cience Poblem e 9 oluions [Theoems of Gauss an okes]. A fla aea A is boune by he iangle whose veices ae he poins P(,, ), Q(,, ) an R(,,

More information

(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1.

(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1. Answers o Een Numbered Problems Chper. () 7 m s, 6 m s (b) 8 5 yr 4.. m ih 6. () 5. m s (b).5 m s (c).5 m s (d) 3.33 m s (e) 8. ().3 min (b) 64 mi..3 h. ().3 s (b) 3 m 4..8 mi wes of he flgpole 6. (b)

More information

Physics Worksheet Lesson 4: Linear Motion Section: Name:

Physics Worksheet Lesson 4: Linear Motion Section: Name: Physics Workshee Lesson 4: Liner Moion Secion: Nme: 1. Relie Moion:. All moion is. b. is n rbirry coorine sysem wih reference o which he posiion or moion of somehing is escribe or physicl lws re formule.

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

ENGR 1990 Engineering Mathematics The Integral of a Function as a Function

ENGR 1990 Engineering Mathematics The Integral of a Function as a Function ENGR 1990 Engineering Mhemics The Inegrl of Funcion s Funcion Previously, we lerned how o esime he inegrl of funcion f( ) over some inervl y dding he res of finie se of rpezoids h represen he re under

More information

Physics 101 Lecture 4 Motion in 2D and 3D

Physics 101 Lecture 4 Motion in 2D and 3D Phsics 11 Lecure 4 Moion in D nd 3D Dr. Ali ÖVGÜN EMU Phsics Deprmen www.ogun.com Vecor nd is componens The componens re he legs of he righ ringle whose hpoenuse is A A A A A n ( θ ) A Acos( θ) A A A nd

More information

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

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

More information

Ans: In the rectangular loop with the assigned direction for i2: di L dt , (1) where (2) a) At t = 0, i1(t) = I1U(t) is applied and (1) becomes

Ans: In the rectangular loop with the assigned direction for i2: di L dt , (1) where (2) a) At t = 0, i1(t) = I1U(t) is applied and (1) becomes omewok # P7-3 ecngul loop of widh w nd heigh h is siued ne ve long wie cing cuen i s in Fig 7- ssume i o e ecngul pulse s shown in Fig 7- Find he induced cuen i in he ecngul loop whose self-inducnce is

More information

Adrian Sfarti University of California, 387 Soda Hall, UC Berkeley, California, USA

Adrian Sfarti University of California, 387 Soda Hall, UC Berkeley, California, USA Innionl Jonl of Phoonis n Oil Thnolo Vol. 3 Iss. : 36-4 Jn 7 Rliisi Dnis n lonis in Unifol l n in Unifol Roin s-th Gnl ssions fo h loni 4-Vo Ponil in Sfi Unisi of Clifoni 387 So Hll UC Bkl Clifoni US s@ll.n

More information

Derivation of the differential equation of motion

Derivation of the differential equation of motion Divion of h iffnil quion of oion Fis h noions fin h will us fo h ivion of h iffnil quion of oion. Rollo is hough o -insionl isk. xnl ius of h ll isnc cn of ll (O) - IDU s cn of gviy (M) θ ngl of inclinion

More information

Chapter Primer on Differentiation

Chapter Primer on Differentiation Capter 0.01 Primer on Differentiation After reaing tis capter, you soul be able to: 1. unerstan te basics of ifferentiation,. relate te slopes of te secant line an tangent line to te erivative of a function,.

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

2D Motion WS. A horizontally launched projectile s initial vertical velocity is zero. Solve the following problems with this information.

2D Motion WS. A horizontally launched projectile s initial vertical velocity is zero. Solve the following problems with this information. Nme D Moion WS The equions of moion h rele o projeciles were discussed in he Projecile Moion Anlsis Acii. ou found h projecile moes wih consn eloci in he horizonl direcion nd consn ccelerion in he ericl

More information

Nonlocal Boundary Value Problem for Nonlinear Impulsive q k Symmetric Integrodifference Equation

Nonlocal Boundary Value Problem for Nonlinear Impulsive q k Symmetric Integrodifference Equation OSR ol o Mec OSR-M e-ssn: 78-578 -SSN: 9-765X Vole e Ve M - A 7 PP 95- wwwojolog Nolocl Bo Vle Poble o Nole lve - Sec egoeece Eo Log Ceg Ceg Ho * Yeg He ee o Mec Yb Uve Yj PR C Abc: A oe ole lve egoeece

More information

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is:

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is: . Homewok 3 MAE 8C Poblems, 5, 7, 0, 4, 5, 8, 3, 30, 3 fom Chpte 5, msh & Btt Point souces emit nuetons/sec t points,,, n 3 fin the flux cuent hlf wy between one sie of the tingle (blck ot). The flux fo

More information

Mathematics Paper- II

Mathematics Paper- II R Prerna Tower, Road No -, Conracors Area, Bisupur, Jamsedpur - 8, Tel - (65789, www.prernaclasses.com Maemaics Paper- II Jee Advance PART III - MATHEMATICS SECTION - : (One or more opions correc Type

More information

Physics Courseware Electromagnetism

Physics Courseware Electromagnetism Pysics Cousewae lectomagnetism lectic field Poblem.- a) Find te electic field at point P poduced by te wie sown in te figue. Conside tat te wie as a unifom linea cage distibution of λ.5µ C / m b) Find

More information

Angular Contac t Ball Bearings

Angular Contac t Ball Bearings High Pecision Angul Contct ll eings Stn Seies 1 Angul Contct ll eings Ult High-Spee Angul Contct ll eings Angul Contct ll eings Pt 4 1. ANGULAR CONTACT ALL EARINGS High Pecision Angul Contct ll eings (Stn

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

OH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9

OH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9 OH BOY! O h Boy!, was or igin a lly cr eat ed in F r en ch an d was a m a jor s u cc ess on t h e Fr en ch st a ge f or young au di enc es. It h a s b een s een by ap pr ox i ma t ely 175,000 sp ect at

More information

2-d Motion: Constant Acceleration

2-d Motion: Constant Acceleration -d Moion: Consan Acceleaion Kinemaic Equaions o Moion (eco Fom Acceleaion eco (consan eloci eco (uncion o Posiion eco (uncion o The eloci eco and posiion eco ae a uncion o he ime. eloci eco a ime. Posiion

More information

One of the common descriptions of curvilinear motion uses path variables, which are measurements made along the tangent t and normal n to the path of

One of the common descriptions of curvilinear motion uses path variables, which are measurements made along the tangent t and normal n to the path of Oe of he commo descipios of cuilie moio uses ph ibles, which e mesuemes mde log he ge d oml o he ph of he picles. d e wo ohogol xes cosideed sepely fo eey is of moio. These coodies poide ul descipio fo

More information

û s L u t 0 s a ; i.e., û s 0

û s L u t 0 s a ; i.e., û s 0 Te Hille-Yosida Teorem We ave seen a wen e absrac IVP is uniquely solvable en e soluion operaor defines a semigroup of bounded operaors. We ave no ye discussed e condiions under wic e IVP is uniquely solvable.

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

10. Euler's equation (differential momentum equation)

10. Euler's equation (differential momentum equation) 3 Ele's eqaion (iffeenial momenm eqaion) Inisci flo: µ eslan of foces mass acceleaion Inisci flo: foces case b he esse an fiel of foce In iecion: ) ( a o a If (), ) ( a a () If cons he nknon aiables ae:,,,

More information

ÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s

ÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s MÜHENDİSLİK MEKANİĞİ. HAFTA İMPULS- MMENTUM-ÇARPIŞMA Linea oenu of a paicle: The sybol L denoes he linea oenu and is defined as he ass ies he elociy of a paicle. L ÖRNEK : THE LINEAR IMPULSE-MMENTUM RELATIN

More information

Coupled Mass Transport and Reaction in LPCVD Reactors

Coupled Mass Transport and Reaction in LPCVD Reactors ople Ma Tanpo an eaion in LPV eao ile A in B e.g., SiH 4 in H Sepaae eao ino o egion, inaafe & annla b - oniniy Eqn: : onveion-iffion iffion-eaion Eqn Ampion! ile peie i in majo aie ga e.g., H isih 4!

More information

Circuits 24/08/2010. Question. Question. Practice Questions QV CV. Review Formula s RC R R R V IR ... Charging P IV I R ... E Pt.

Circuits 24/08/2010. Question. Question. Practice Questions QV CV. Review Formula s RC R R R V IR ... Charging P IV I R ... E Pt. 4/08/00 eview Fomul s icuis cice s BL B A B I I I I E...... s n n hging Q Q 0 e... n... Q Q n 0 e Q I I0e Dischging Q U Q A wie mde of bss nd nohe wie mde of silve hve he sme lengh, bu he dimee of he bss

More information

A Kalman filtering simulation

A Kalman filtering simulation A Klmn filering simulion The performnce of Klmn filering hs been esed on he bsis of wo differen dynmicl models, ssuming eiher moion wih consn elociy or wih consn ccelerion. The former is epeced o beer

More information

3.4 Conic sections. In polar coordinates (r, θ) conics are parameterized as. Next we consider the objects resulting from

3.4 Conic sections. In polar coordinates (r, θ) conics are parameterized as. Next we consider the objects resulting from 3.4 Conic sections Net we consier the objects resulting from + by + cy + + ey + f 0. Such type of cures re clle conics, becuse they rise from ifferent slices through cone In polr coorintes r, θ) conics

More information

3.1 Velocity: m s. x t. dx dt. x t (1) 3.2 Acceleration: v t. v t. dv dt. (2) s. 3.3 Impulse: (3) s. lim. lim

3.1 Velocity: m s. x t. dx dt. x t (1) 3.2 Acceleration: v t. v t. dv dt. (2) s. 3.3 Impulse: (3) s. lim. lim . unen n eie quniie n uni unen Phi quniie e hoe h n e ie efine, n fo whih he uni e hoen ii, inepenen of ohe phi quniie. o. unen uni Uni So Dienion engh Mee Tie Seon T M Kiog g M uen ineni Apee A igh ineni

More information

4. Runge-Kutta Formula For Differential Equations

4. Runge-Kutta Formula For Differential Equations NCTU Deprme o Elecrcl d Compuer Egeerg 5 Sprg Course by Pro. Yo-Pg Ce. Ruge-Ku Formul For Derel Equos To solve e derel equos umerclly e mos useul ormul s clled Ruge-Ku ormul

More information

A study Of Salt-Finger Convection In a Nonlinear Magneto-Fluid Overlying a Porous Layer Affected By Rotation

A study Of Salt-Finger Convection In a Nonlinear Magneto-Fluid Overlying a Porous Layer Affected By Rotation Innion on o Mchnic & Mchonic Engining IMME-IEN Vo: No: A O -ing Concion In Nonin Mgno-i Oing oo Ac Roion M..A-hi Ac hi o in -ing concion in o o nonin gno-i oing oo c oion. o in h i i gon Ni-o qion n in

More information

Reinforcement learning

Reinforcement learning CS 75 Mchine Lening Lecue b einfocemen lening Milos Huskech milos@cs.pi.edu 539 Senno Sque einfocemen lening We wn o len conol policy: : X A We see emples of bu oupus e no given Insed of we ge feedbck

More information

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218 Chper Moion long srigh line 9/9/05 Physics 8 Gols for Chper How o describe srigh line moion in erms of displcemen nd erge elociy. The mening of insnneous elociy nd speed. Aerge elociy/insnneous elociy

More information

Physics 232 Exam II Mar. 28, 2005

Physics 232 Exam II Mar. 28, 2005 Phi 3 M. 8, 5 So. Se # Ne. A piee o gl, ide o eio.5, h hi oig o oil o i. The oil h ide o eio.4.d hike o. Fo wh welegh, i he iile egio, do ou ge o eleio? The ol phe dieee i gie δ Tol δ PhDieee δ i,il δ

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

Applications of these ideas. CS514: Intermediate Course in Operating Systems. Problem: Pictorial version. 2PC is a good match! Issues?

Applications of these ideas. CS514: Intermediate Course in Operating Systems. Problem: Pictorial version. 2PC is a good match! Issues? CS514: Inmi Co in Oing Sm Poo Kn imn K Ooki: T liion o h i O h h k h o Goi oool Dii monioing, h, n noiiion gmn oool, h 2PC n 3PC Unling hm: om hing n ong om o onin, om n mng ih k oi To, l look n liion

More information

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba THE INTEACTION OF ADIATION AND MATTE: SEMICLASSICAL THEOY PAGE 26 III. EVIEW OF BASIC QUANTUM MECHANICS : TWO -LEVEL QUANTUM SYSTEMS : The lieaue of quanum opics and lase specoscop abounds wih discussions

More information

Example: Two Stochastic Process u~u[0,1]

Example: Two Stochastic Process u~u[0,1] Co o Slo o Coco S Sh EE I Gholo h@h. ll Sochc Slo Dc Slo l h PLL c Mo o coco w h o c o Ic o Co B P o Go E A o o Po o Th h h o q o ol o oc o lco q ccc lco l Bc El: Uo Dbo Ucol Sl Ab bo col l G col G col

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 11 PARAMETRIC EQUATIONS AND POLAR COORDINATES

CHAPTER 11 PARAMETRIC EQUATIONS AND POLAR COORDINATES CHAPTER PARAMETRIC EQUATIONS AND POLAR COORDINATES. PARAMETRIZATIONS OF PLANE CURVES., 9, _ _ Ê.,, Ê or, Ÿ. 5, 7, _ _.,, Ÿ Ÿ Ê Ê 5 Ê ( 5) Ê ˆ Ê 6 Ê ( 5) 7 Ê Ê, Ÿ Ÿ $ 5. cos, sin, Ÿ Ÿ 6. cos ( ), sin (

More information