2. v = 3 4 c. 3. v = 4c. 5. v = 2 3 c. 6. v = 9. v = 4 3 c

Size: px
Start display at page:

Download "2. v = 3 4 c. 3. v = 4c. 5. v = 2 3 c. 6. v = 9. v = 4 3 c"

Transcription

1 Vesion 074 Exam Final Daf swinney (55185) 1 This pin-ou should have 30 quesions. Muliple-choice quesions may coninue on he nex column o page find all choices befoe answeing poins AballofmassM ishownowadhegound fom a heigh H above Eah wih a speed (gh) 1/. A ficionalfoce of consan magniude (3/4)M g acs opposie o he diecion of moion. How long does i ake he ball o each he gound? H 1. g 1 H. g 3. 4( H 1) g coec H 4. 4 g H 5. 4 g ( ) H g H 7. g 8. ( H ) g Apply he kinemaic equaion of moion in he y diecion y = y 0 +v 0y + 1 a y o he ball. Fis calculae he acceleaion fom he momenum pinciple: F ne,y = = 1 4 = ma y. Hence, a y = (1/4)g. Now leing T be he ime of fligh and using y f = 0,y 0 = H,v 0y = (gh) 1/,a y = (1/4)g we have he equaion: 0 = H (gh) 1/ T 1 8 gt which can be solved using he quadaic equaion. Hence gh ± gh T = g/4 and aking T > 0 gives H T = 4 g ( 1) poins An elecon of mass m has a speed of v. A wha speed would he aio of he magniudes of he elaivisic and non-elaivisic momena be equal o? 3 1. v = 4 c coec. v = 3 4 c 3. v = 4c 4 4. v = 3 c 5. v = 3 c 6. v = 3 c 1 7. v = 4 c 5 8. v = 4 c 9. v = 4 3 c v = c The magniude of he elaivisic momenum is p = γmv = mv 1 v c.

2 Vesion 074 Exam Final Daf swinney (55185) and he non-elaivisic momenum so he aio is p p n = = p n = mv, 1 1 v c so by squaing boh sides we obain 4 = and wih a lile algeba 1 1 v c v c = 3 4 Now we muliply each side by c and ake he squae oo of boh sides o ge 3 v = 4 c poins A paicle of mass m moves along he x axis as descibed by x() = A 3 B, due o an applied foce F x (). Wha powe P() does he foce delive o he paicle? 1.P() = m(6a B)(3A B)coec. Zeo, because he objec s velociy is insananeously consan 3. P() = m(6a+b)(a 3 B ) 4. P() = m(6a B)(3A B) 5.P() = m(3a B)(3A B) 6. P() = m(6a B)(3A +B) 7. P() = m(3a B)(3A B) 8. P() = m(6a+b)(3a B).. 9. P() = m(6a B)(A 3 +B ) 10. P() = m(6a B)(A 3 B ) Thus x = A 3 A v x = dx d = 3A B and a x = d x = (6A B), so d F x = ma x = m(6a B). P = F v = F x v x = m(6a B)(3A B) poins When you ae moving up a consan speed in an elevao, hee ae wo foces acing on you: he floo pushing up on you (F 1 ) and gaviy pulling down (F ). Wha is he elaionship beween he magniudeoff 1 andf andhephysical pinciple ha explains his elaionship? 1. F 1 = F fom he momenum pinciple. coec. I depends on which diecion he elevao is moving. 3. F 1 = F fom he pinciple of ecipociy. 4. F 1 > F fom he pinciple of ecipociy. 5. F 1 < F fom he pinciple of ecipociy. 6. F 1 < F fom he momenum pinciple. 7. F 1 > F fom he momenum pinciple.

3 Vesion 074 Exam Final Daf swinney (55185) 3 Since he speed is consan, hee is no change in momenum. The momenum pinciple saes ha he ne foce mus heefoe be zeo, which equies F 1 = F poins A plane of mass m is obiing a sa of mass M inaciculapahofadiusr. Foasysem consising of only he plane and he sun, whaisheoalenegyofhesyseminems ofm, M, R,andGheunivesalgaviaional consan? Assume he sun is moionless and ha he gaviaional poenial enegy goes o zeo a infinie sepaaion. 1. GM m R. GM m 4R 3. 4GM m R 4. GM m 4R 5. GM m R coec 6. 0 Theefoe he oal enegy is given by K +U = GM m R poins A ubbe ball is dopped fom es ono he floo, andbounces back upohesameheigh fom which i saed. Ignoe he foce of ficion due o he ai. Which of he following ses of plos mos accuaely depic his moion? (The foce plos depic he foce on he ball by he envionmen.) y 1. y. v y v y F y F y 7. GM m R 8. GM m R 9. 4GM m R Since he plane is moving on a cicula obi, mv R = GM m R, which implies mv = GM m R. Theefoe, K = 1 mv = GM n R. The gaviaional poenial enegy is given by U = GM m R. y 3. coec y 4. y 5. v y v y v y F y F y F y

4 Vesion 074 Exam Final Daf swinney (55185) 4 Since hee is a consan foce, gaviy, downwad, he plo of he y-posiion should be paabolic wih negaive slope whose magniude is inceasing ove ime, unil i his he floo. A his poin he slope should swich sign and poin upwad and decease in magniude ove ime. The velociy should be iniially 0 m/s since he ball saed fom es, and decease linealy unil i his he floo, a which poin i is vey quickly given a boos o a posiive value, and againconinues o decease linealy. The foce should be always a negaive consan value, excep fo when he ball his he floo, a which poin i should be a naow posiive peak o indicae he bief upwad foce exeed on he ball by he floo poins A mass aached o a sping is given an iniial displacemen x 0 and an iniial velociy v 0. If he posiion of he mass is given by x() = Asin(ω+α), wha is he phase angle α? ( ) 1. α = co 1 x0 ωv ( 0 ). α = an 1 ωx0 coec v ( 0 3. α = co 1 ωx ) 0 v ( 0 4. α = co 1 x ) 0 ωv ( 0 5. α = an 1 ωx ) 0 v ( 0 ) 6. α = an 1 x0 ωv ( 0 ) 7. α = co 1 ωx0 v ( 0 8. α = an 1 x ) 0 ωv ( ) α = cos 1 v α = sin 1( x ) 0 ω Hee, use he iniial posiion and iniial velociy o solve fo α. The iniial posiion is x( = 0) = Asin(α) = x 0 and he iniial velociy is v( = 0) = ωacos(α) = v 0. Now dividing x 0 by v 0 eliminaes A o give: ( ) α = an 1 x0 ωv poins If a apeze ais oaes once each second while sailing hough he ai, and conacs o educe he oaional ineia o one hid of wha i was, how many oaions pe second will esul? 1. 1/9 oaions pe second.. 1/3 oaions pe second oaion pe second oaions pe second oaions pe second. coec The ais will oae 3 imes pe second. By he consevaion of angula momenum, he ais will incease oaion ae by 3. Tha is, I 1 ω 1 = I ω I 1 ω 1 = I 1 3 3ω poins Two wies wih equal lenghs ae made of pue coppe. The diamee of wie A is wice he diamee of wie B. You make caeful measuemens and compue Young s modulus fo boh wies. Wha do you find? 1. Y A = Y B coec. Y A > Y B 3. Y A < Y B Since boh wies ae made of coppe, Y A = Y B poins

5 Vesion 074 Exam Final Daf swinney (55185) 5 The moe massive Eah and he less massive moon ae aaced o each ohe by he gaviaional foce. Is he acceleaion expeienced by he Eah due o his gaviaional ineacion wih he moon is geae han, less han, o he same as he acceleaion expeienced by he moon? 1. Unable o deemine. less han coec 3. geae han 4. he same as The gaviaional foces expeienced by he Eah and moon ae he same, bu he Eah is much moe massive so he acceleaion i expeiences is much less han ha expeienced by he moon poins Conside a hin unifom od of mass M and lengh L. L Wha is he oaional ineia of he od abou a poin a disance L fom he neaes end of he od, along he line of he od? 1. Sill he same, since empy space has no mass and hus no oaional ineia M L 3. 1 M L 7. M (L) = 4M L M L coec M L M L Accoding o he paallel axis heoem, I p = I cm + M h, whee h is he disance fom he CM o he new paallel axis pivo poin p. In his case, he oaional ineia of he od abou is cene of mass is 1 1 M L. (We don cae abou he oaional ineia abou is end; hee is no heoem elaing ha oaional ineia o any abiay axis oaional ineia.) The addiional disance h fomheceneofmassohenewpivopoin is L+ L = 3L, so he new oaional ineia is ( ) M L = M L poins A ball moves in he diecion of he aow labeleddinhefollowingdiagam. Theballis suck by a sick ha biefly exes a foce on he ball in he diecion of he aow labeled f. Which aowdescibeshediecionof p, he change in he ball s momenum? g h f a e b d c M L M L 6. Zeo. 1. e. h 3. c

6 Vesion 074 Exam Final Daf swinney (55185) 6 4. d 5. a 6. g 7. f coec 8. b Recall he definiion of impulse: Impulse = F ne = p. Theefoe, whaeve diecion he ne foce poins in is he same diecion as he change in he ball s momenum. We ae oldha he foceisinhe diecionlabeledf so pisalso in he diecion labeled f poins A flywheel slows fom an iniial angula velociy ω 0 o es in ime T. If he angula acceleaion α is consan, wha is he angula displacemen θ? 1. ω 0 T. ω 0T 3. ω 0 T 4. ω 0 T 5. 1 ω 0T 6. ω 0 T 7. 1 ω 0 T 8. ω 0 T 9. 1 ω 0T ω 0T coec Foconsanangulaacceleaion,ω = ω 0 + αt, bu since he flywheel comes o a sop, ω = 0. Hence α = ω 0 /T. The angula displacemen θ fo consan α and θ 0 = 0isa ime T θ = ω 0 T + 1 αt Subsiuing α = ω 0 /T, we have θ = ω 0 T + 1 ( ω 0/T)T = 1 ω 0T poins Given: The baleship and enemy ships 1 and lie along a saigh line. Neglec ai ficion. baleship 1 Conside he moion of he wo pojeciles fied a = 0. Thei iniial speeds ae boh v 0 bu hey ae fied wih diffeen iniial angles θ 1 and θ. Wha is he aio of he maximum heighs, h 1 of he pojecile dieced a ship 1 and h dieced a ship, ha he shells each? 1. h 1 h = sinθ 1 sinθ. h 1 h = cos θ 1 cos θ 3. h 1 h = sin θ 1 sin θ coec 4. h 1 h = sinθ sinθ 1 5. h 1 h = sin θ sin θ 1 6. h 1 h = anθ anθ 1 7. h 1 h = 1

7 Vesion 074 Exam Final Daf swinney (55185) 7 8. h 1 h = an θ 1 an θ 9. h 1 h = cos θ cos θ h 1 h = cosθ 1 cosθ A is maximum heigh, he y componen of is velociy veco is 0, so 0 = v y = v y gh h = v y g = v sin θ g Theefoe, he aio of he heighs is h 1 h = v 0 sin θ 1 g v 0 sin θ g = sin θ 1 sin θ poins The figue below shows wo negaively chaged objecs and one posiively chaged objec. Wha is he diecion of he ne elecic foce on he posiively chaged objec? Choose you answe fom he diagam labeled I-IX VII 4. II 5. VIII 6. VI 7. V 8. IV 9. IX We need o keep in mind he expession fo he magniude of elecic foce: F = 1 q 1 q 4πǫ 0. The foce is dependen on disance, wih less disance meaning geae foce. The posiively chaged objec is aaced elecomagneically o boh of he negaively chaged objecs, bu since i is close o he one onhe igh, he aacive foce beween i and he negaive chage on he igh will be songe. Theefoe he ne elecic foce poins owad he igh poins A paicle moves in he x-diecion as indicaed in he posiion vs. ime plo below. I VIII II VII III VI IV V IX zeo ne foce 1. III coec. I A poin P, he mass has 1. negaive velociy and negaive acceleaion.. negaive velociy and posiive acceleaion. 3. posiive velociy and negaive acceleaion. coec

8 Vesion 074 Exam Final Daf swinney (55185) 8 4. posiive velociy and zeo acceleaion. 5. negaive velociy and zeo acceleaion. 6. zeo velociy bu is acceleaing (posiively o negaively). 7. zeo velociy and zeo acceleaion. 8. posiive velociy and posiive acceleaion. The velociy is posiive because he slope of he cuve a P is posiive. The acceleaion is negaive because he cuve is concave down a P poins Conside he following diagam. A B If angle beween B and C is a igh angle, which of he following ae accuae veco elaions? I. A B = C II. B C = A III. B B + C C = A A IV. B B C C = A A 1. IV. III, IV 3. II, III coec 4. I, II 5. I, IV 6. III C 7. I 8. II, IV 9. II 10. I, III Adding C o B gives A hence B C = A. Also, aking he do poduc of each side of his elaion wih iself gives bu B C = 0 so ( B C) ( B C) = A A B B + C C = A A whichisjushepyhagoeantheoem: B + C = A poins A od has a pivo a one end and is fee o oae wihou ficion a he ohe end, as shown. A foce F is applied o he fee end a an angle θ o he od ceaing a oque τ abou he pivo. If insead he same foce is applied pependiculaoheod,awhadisancedfomhe pivo should i be applied in ode o poduce he same ne oque τ abou he pivo? 1. d = L/cosθ. d = L 3. d = L 4. d = L/sinθ 5. d = L/ anθ L m θ F

9 Vesion 074 Exam Final Daf swinney (55185) 9 6. d = L cosθ 7. d = L/ 8. d = L sinθ coec 9. d = L anθ 10. d = 5 L The foce geneaes a oque of τ = F Lsinθ, so he disance is L sinθ poins How fas mus a olle coase ca go hough a cicula dip fo you o feel hee imes as heavy as usual, due o he upwad foce of he sea on you boom being hee imes as lage as usual? The cene of he ca moves alongaciculaacofadiusrasinhefigue below. R v 9. v = gr gr 10. v = A he boom of a hill (o a dip ), he ne foce on he ide is upwad. The foce by he sea on he ide is also upwad, and in his case has a magniude of 3. The ne foce on he ide is F ne = F sea +F gav 0, m v,0 = 0,3,0 + 0,,0 R m v R = v = gr poins The enegy levels of a paicula quanum objec ae 8. ev, 6.4 ev, and 1.8 ev. If a collecion of hese objecs is bombaded by an elecon beam so ha hee ae some objecs in each excied sae, wha ae he enegies of he phoons ha will be emied? ev, 1.8 ev, 6.4 ev. 1.8 ev, 14.6 ev, 4.6 ev 1. v = 3 gr. v = gr 3. v = gr 4. v = gr 5. v = gr coec 6. v = 1 gr 7. v = 3gR 8. v = 3gR ev, 6.4 ev, 1.8 ev ev, 6.4 ev, 1.8 ev ev, 6.4 ev, 4.6 ev coec ev, 6.4 ev, 4.6 ev ev, 4.6 ev, 10 ev ev, 6.4 ev, 1.8 ev ev, 10 ev, 8. ev ev, 8. ev, 14.6 ev

10 Vesion 074 Exam Final Daf swinney (55185) ev, 6.4 ev, 4.6 ev is he coec answe. The 3 emied phoons coespond o 3 ansiions beween he saes. Label hem as E 1 = 8. ev E = 6.4 ev E 3 = 1.8 ev Then he possible ansiions ae given by E phoon = E 1, = E 1 E = 8. ev+6.4 ev = 1.8 ev E phoon = E 1,3 = E 1 E 3 = 8. ev+1.8 ev = 6.4 ev E phoon = E,3 = E E 3 = 6.4 ev+1.8 ev = 4.6 ev poins Wha is he appoximae diamee of a coppe aom in mees? m m m m m coec Anaomisabou 0.1nm indiamee which is m poins A ypicalhuman die is000 foodcaloiespe day. Each food caloie is he enegy equivalen of J. Wha ishe powe consumpion fo a ypical human die? W coec W W 4. 1W W W 7. 10W W W Each day a peson consumes 000 caloies. Muliplying 000 caloies by J pe caloiegiveshedailyenegyinakeinj.then muliplying 4 hous pe day imes 60 minues pe hou imes 60 sec pe min gives he numbeofsecondsinaday. Dividingheoal enegy inakeinjoules by he imeove which he enegy is consumed in seconds gives he powe consumpion in a die, i.e., m m = m m m poins The following gaph epesens a hypoheical poenial enegy cuve fo a paicle of mass m.

11 Vesion 074 Exam Final Daf swinney (55185) 11 U() 9U 0 6U 0 3U 0 O 0 0 If he paicle is eleased fom es a posiion 0, wha will be is speed v a posiion 0? 1. v = U0 m U0. v = 4m 1U0 3. v = m coec 8U0 4. v = m 6U0 5. v = m 4U0 6. v = m 10U0 7. v = m U0 8. v = m U0 9. v = m The oal enegy of he paicle is conseved. So he change of he poenial enegy is conveed ino he kineic enegy of he paicle, which gives 1 mv = 9U 0 3U 0 1U0 v = m poins TwoobjecsshaeaoalenegyE = E 1 +E. Thee ae 5 ways o aange an amoun of enegy E 1 in he fis objec and 10 ways o aangeanamoun ofenegy E inhesecond objec. How many diffeen ways ae hee o aange he oal enegy E = E 1 +E so ha hee is E 1 in he fis objec and E in he ohe? 1. 14! 5!9! 15!. 5!10! ! 4!10! coec The oal numbe of micosaes o numbe of ways of aanging enegy in he sysem is he poduc of he numbe of ways of aanging he enegy in especive objecs, i.e. Ω oal = Ω 1 Ω poins A ball of mass M collides head-on and inelasically wih a ball of mass 3M. Befoe he collision, he ball of mass M is moving o he igh a speed v 0 and he ball of mass 3M is moving o he lef a he same speed v 0. M v 0 v 0 3M Afe he collision, he ball of mass 3M is moving o he lef a speed v 0. Wha is he aio of he final kineic enegy o he iniial kineic enegy?

12 Vesion 074 Exam Final Daf swinney (55185) 1 v v 0 The aio of he final o iniial kineic enegy is jus M 3M Wha facion of he iniial kineic enegy is los in he collision? coec K f K i = (1/)M v 0 M v 0 = poins A block of mass m is on a ficionless plane inclined a θ wih espec o he hoizonal and is pushed a a consan velociy up he plane by a foce F ha is inclined a α wih espec o he hoizonal. Gaviy acs downwad wih a magniude F α m θ Take componens of p i = p f along he line of he collision o obain ( v0 ) M v 0 (3M)v 0 = M v (3M) v 0 = v + 3v 0 v = v 0. Thus K i = 1 [ M v 0 +(3M)v0 ] = M v 0, K f = 1 [ ( v0 ) ( v0 ) ] M +(3M) = 1 ( 1 M v ) = 1 4 M v 0, and Wha is he magniude of he applied foce F applied o he block in ems of,θ, and α? 1. F = cosα(anα+anθ). F = anα(sinα+cosθ) 3. F = cosα(coα+coθ) 4. F = cosα(anα+coθ) coec 5. F = sinα(anα+anθ) 6. F = coα(sinα+cosθ) 7. F = coα(cosα+sinθ) 8. F = anα(cosα+sinθ) 9. F = sinα(coα+coθ) 10. F = sinα(anα+coθ)

13 Vesion 074 Exam Final Daf swinney (55185) 13 We apply he Momenum Pinciple F ne = m a. Le he x-diecion o be o he igh and hey-diecionobeup. Thenefoceineach diecion of his coodinae sysem is and F x,ne = F cosα N sinθ F y,ne = F sinα+n cosθ We apply he Momenum Pinciple and since he velociy is consan, he acceleaion is a = 0. Thus, he equaion in he x-diecion gives N = F cosα sinθ. Plugging his ino he y-equaion gives F sinα+f cosα cosθ = sinθ o eaanging his gives F cosα(anα+coθ) = finally solving fo F gives F = cosα(anα+coθ) poins A block of mass m slides up a amp wih ficion ha makes an angle θ wih he hoizonal. The block has an iniial velociy v 0 as i sas up he amp and hen avels a disance L along he amp befoe coming momenaily o es. L v 0 How much wok did kineic ficion do on he block beween is saing poin and he poin i came o momenay es? ( ) 1. m gl sinθ v 0 coec. L ( ) 3. m gl sinθ + v 0 4. L sinθ 5. L cosθ ( ) 6. m gl cosθ v 0 7. Zeo 8. m( v 0 9. m( v mv 0 ) +gl cosθ ) gl sinθ θ L L sinθ If we ake he gaviaional poenial enegy o be zeo a he poin whee he block has is iniial speed, hen fom E = K +U g E i = 1 mv 0 +0 and E f = 0+L sinθ. The wok done by ficion, a nonconsevaive foce, is hus ( ) W f = E f E i = m gl sinθ v poins Which of he following gaphs coesponds o a sysem of one elecon and one poon ha sa ou fa apa, moving owad each ohe (ha is, hei iniial velociies ae

14 Vesion 074 Exam Final Daf swinney (55185) 14 nonzeo and hey ae heading saigh a each ohe)? Noe ha he hoizonal and veical axes in each plo ae he sepaaion beween he paicles and enegy, especively. 1. None of hese gaphs could epesen he enegies of he sysem. 6. U K K +U K +U K. U 7. K K +U U K K +U 3. U 4. K U K +U coec When he elecon and poon ae vey fa away hei poenial enegy poenial enegy ends o zeo, and since hey have nonzeo iniial velociies, his means ha hey have a posiive kineic enegy and hence a posiive oal enegy. As he elecons ge close, due o hei Coulomb aacion, i.e., U 1/, hei kineic enegies inceases as he poenial enegy deceases. Thus he coec answe K K +U is. 5. K +U K U U poins A small sphee of mass m is conneced o he end of a cod of lengh and oaes in a veical cicle abou a fixed poin O. The ensionfoceexeedbyhecodonhesphee is denoed by T.

15 Vesion 074 Exam Final Daf swinney (55185) 15 diecion, so θ O F c = mv = T cosθ. Wha is he equaion fo he ne foce in he adial diecion when he cod makes an angle θ wih he veical? 1. None of hese keywods: poins Jane swings fom a vine, acing ou an ac as in he following figue.. T sinθ = + mv 3. T sinθ = + mv cosθ anθ 4. T sinθ = + mv 5. T +sinθ = + mv When she is a he boom of he swing, which aow bes descibes he diecion of he ae of change of Jane s momenum? 6. T +cosθ = + mv 7. T cosθ = + mv coec VII VIII I II III 8. T sinθ = mv 9. T sinθ = mv anθ 1. VII VI V IV O. II T θ 3. V θ The cenipeal foce is F c = mv This cenipeal foce is povided by he ension foce and he adial componen of he weigh. In his case, hey ae in opposie. 4. IV 5. I coec 6. VIII 7. III 8. VI

16 Vesion 074 Exam Final Daf swinney (55185) 16 A he lowes poin Jane s momenum is hoizonal. A sho ime befoe Jane eaches he lowes poin, he momenum veco has a downwad componen, while a ime afe eaching his lowes poin, his momenum veco has an upwad componen; hese momena ae equal in magniude. Theefoe, he change in momenum, p, is upwad, in diecion I.

PHYS PRACTICE EXAM 2

PHYS PRACTICE EXAM 2 PHYS 1800 PRACTICE EXAM Pa I Muliple Choice Quesions [ ps each] Diecions: Cicle he one alenaive ha bes complees he saemen o answes he quesion. Unless ohewise saed, assume ideal condiions (no ai esisance,

More information

WORK POWER AND ENERGY Consevaive foce a) A foce is said o be consevaive if he wok done by i is independen of pah followed by he body b) Wok done by a consevaive foce fo a closed pah is zeo c) Wok done

More information

KINEMATICS OF RIGID BODIES

KINEMATICS OF RIGID BODIES KINEMTICS OF RIGID ODIES In igid body kinemaics, we use he elaionships govening he displacemen, velociy and acceleaion, bu mus also accoun fo he oaional moion of he body. Descipion of he moion of igid

More information

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can. 1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule

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

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

Relative and Circular Motion

Relative and Circular Motion Relaie and Cicula Moion a) Relaie moion b) Cenipeal acceleaion Mechanics Lecue 3 Slide 1 Mechanics Lecue 3 Slide 2 Time on Video Pelecue Looks like mosly eeyone hee has iewed enie pelecue GOOD! Thank you

More information

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion

More information

Physics 2001/2051 Moments of Inertia Experiment 1

Physics 2001/2051 Moments of Inertia Experiment 1 Physics 001/051 Momens o Ineia Expeimen 1 Pelab 1 Read he ollowing backgound/seup and ensue you ae amilia wih he heoy equied o he expeimen. Please also ill in he missing equaions 5, 7 and 9. Backgound/Seup

More information

P h y s i c s F a c t s h e e t

P h y s i c s F a c t s h e e t P h y s i c s F a c s h e e Sepembe 2001 Numbe 20 Simple Hamonic Moion Basic Conceps This Facshee will:! eplain wha is mean by simple hamonic moion! eplain how o use he equaions fo simple hamonic moion!

More information

KINEMATICS IN ONE DIMENSION

KINEMATICS IN ONE DIMENSION KINEMATICS IN ONE DIMENSION PREVIEW Kinemaics is he sudy of how hings move how far (disance and displacemen), how fas (speed and velociy), and how fas ha how fas changes (acceleraion). We say ha an objec

More information

The Production of Polarization

The Production of Polarization Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview

More information

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias

More information

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay)

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay) Secions 3.1 and 3.4 Eponenial Funcions (Gowh and Decay) Chape 3. Secions 1 and 4 Page 1 of 5 Wha Would You Rahe Have... $1million, o double you money evey day fo 31 days saing wih 1cen? Day Cens Day Cens

More information

Lecture 17: Kinetics of Phase Growth in a Two-component System:

Lecture 17: Kinetics of Phase Growth in a Two-component System: Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien

More information

Lecture 22 Electromagnetic Waves

Lecture 22 Electromagnetic Waves Lecue Elecomagneic Waves Pogam: 1. Enegy caied by he wave (Poyning veco).. Maxwell s equaions and Bounday condiions a inefaces. 3. Maeials boundaies: eflecion and efacion. Snell s Law. Quesions you should

More information

156 There are 9 books stacked on a shelf. The thickness of each book is either 1 inch or 2

156 There are 9 books stacked on a shelf. The thickness of each book is either 1 inch or 2 156 Thee ae 9 books sacked on a shelf. The hickness of each book is eihe 1 inch o 2 F inches. The heigh of he sack of 9 books is 14 inches. Which sysem of equaions can be used o deemine x, he numbe of

More information

Physics 207 Lecture 13

Physics 207 Lecture 13 Physics 07 Lecue 3 Physics 07, Lecue 3, Oc. 8 Agenda: Chape 9, finish, Chape 0 Sa Chape 9: Moenu and Collision Ipulse Cene of ass Chape 0: oaional Kineaics oaional Enegy Moens of Ineia Paallel axis heoe

More information

MOMENTUM CONSERVATION LAW

MOMENTUM CONSERVATION LAW 1 AAST/AEDT AP PHYSICS B: Impulse and Momenum Le us run an experimen: The ball is moving wih a velociy of V o and a force of F is applied on i for he ime inerval of. As he resul he ball s velociy changes

More information

Computer Propagation Analysis Tools

Computer Propagation Analysis Tools Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion

More information

AST1100 Lecture Notes

AST1100 Lecture Notes AST00 Lecue Noes 5 6: Geneal Relaiviy Basic pinciples Schwazschild geomey The geneal heoy of elaiviy may be summaized in one equaion, he Einsein equaion G µν 8πT µν, whee G µν is he Einsein enso and T

More information

The sudden release of a large amount of energy E into a background fluid of density

The sudden release of a large amount of energy E into a background fluid of density 10 Poin explosion The sudden elease of a lage amoun of enegy E ino a backgound fluid of densiy ceaes a song explosion, chaaceized by a song shock wave (a blas wave ) emanaing fom he poin whee he enegy

More information

1. VELOCITY AND ACCELERATION

1. VELOCITY AND ACCELERATION 1. VELOCITY AND ACCELERATION 1.1 Kinemaics Equaions s = u + 1 a and s = v 1 a s = 1 (u + v) v = u + as 1. Displacemen-Time Graph Gradien = speed 1.3 Velociy-Time Graph Gradien = acceleraion Area under

More information

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

Prerna Tower, Road No 2, Contractors Area, Bistupur, Jamshedpur , Tel (0657) ,  PART A PHYSICS Pena Towe, oad No, Conacos Aea, isupu, Jamshedpu 83, Tel (657)89, www.penaclasses.com AIEEE PAT A PHYSICS Physics. Two elecic bulbs maked 5 W V and W V ae conneced in seies o a 44 V supply. () W () 5 W

More information

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING MEEN 67 Handou # MODAL ANALYSIS OF MDOF Sysems wih VISCOS DAMPING ^ Symmeic Moion of a n-dof linea sysem is descibed by he second ode diffeenial equaions M+C+K=F whee () and F () ae n ows vecos of displacemens

More information

IB Physics Kinematics Worksheet

IB Physics Kinematics Worksheet IB Physics Kinemaics Workshee Wrie full soluions and noes for muliple choice answers. Do no use a calculaor for muliple choice answers. 1. Which of he following is a correc definiion of average acceleraion?

More information

Rotational Motion and the Law of Gravity

Rotational Motion and the Law of Gravity Chape 7 7 Roaional Moion and he Law of Gaiy PROBLEM SOLUTIONS 7.1 (a) Eah oaes adians (360 ) on is axis in 1 day. Thus, ad 1 day 5 7.7 10 ad s 4 1 day 8.64 10 s Because of is oaion abou is axis, Eah bulges

More information

Welcome Back to Physics 215!

Welcome Back to Physics 215! Welcome Back o Physics 215! (General Physics I) Thurs. Jan 19 h, 2017 Lecure01-2 1 Las ime: Syllabus Unis and dimensional analysis Today: Displacemen, velociy, acceleraion graphs Nex ime: More acceleraion

More information

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan Ground Rules PC11 Fundamenals of Physics I Lecures 3 and 4 Moion in One Dimension A/Prof Tay Seng Chuan 1 Swich off your handphone and pager Swich off your lapop compuer and keep i No alking while lecure

More information

New method to explain and calculate the gyroscopic torque and its possible relation to the spin of electron

New method to explain and calculate the gyroscopic torque and its possible relation to the spin of electron Laes Tends in Applied and Theoeical Mechanics New mehod o explain and calculae he gyoscopic oque and is possible elaion o he o elecon BOJIDAR DJORDJEV Independen Reseache 968 4- Dobudja see, Ezeovo, Vana

More information

4.5 Constant Acceleration

4.5 Constant Acceleration 4.5 Consan Acceleraion v() v() = v 0 + a a() a a() = a v 0 Area = a (a) (b) Figure 4.8 Consan acceleraion: (a) velociy, (b) acceleraion When he x -componen of he velociy is a linear funcion (Figure 4.8(a)),

More information

5-1. We apply Newton s second law (specifically, Eq. 5-2). F = ma = ma sin 20.0 = 1.0 kg 2.00 m/s sin 20.0 = 0.684N. ( ) ( )

5-1. We apply Newton s second law (specifically, Eq. 5-2). F = ma = ma sin 20.0 = 1.0 kg 2.00 m/s sin 20.0 = 0.684N. ( ) ( ) 5-1. We apply Newon s second law (specfcally, Eq. 5-). (a) We fnd he componen of he foce s ( ) ( ) F = ma = ma cos 0.0 = 1.00kg.00m/s cos 0.0 = 1.88N. (b) The y componen of he foce s ( ) ( ) F = ma = ma

More information

2.1: What is physics? Ch02: Motion along a straight line. 2.2: Motion. 2.3: Position, Displacement, Distance

2.1: What is physics? Ch02: Motion along a straight line. 2.2: Motion. 2.3: Position, Displacement, Distance Ch: Moion along a sraigh line Moion Posiion and Displacemen Average Velociy and Average Speed Insananeous Velociy and Speed Acceleraion Consan Acceleraion: A Special Case Anoher Look a Consan Acceleraion

More information

Unit 1 Test Review Physics Basics, Movement, and Vectors Chapters 1-3

Unit 1 Test Review Physics Basics, Movement, and Vectors Chapters 1-3 A.P. Physics B Uni 1 Tes Reiew Physics Basics, Moemen, and Vecors Chapers 1-3 * In sudying for your es, make sure o sudy his reiew shee along wih your quizzes and homework assignmens. Muliple Choice Reiew:

More information

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still. Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in

More information

Physics 101 Fall 2006: Exam #1- PROBLEM #1

Physics 101 Fall 2006: Exam #1- PROBLEM #1 Physics 101 Fall 2006: Exam #1- PROBLEM #1 1. Problem 1. (+20 ps) (a) (+10 ps) i. +5 ps graph for x of he rain vs. ime. The graph needs o be parabolic and concave upward. ii. +3 ps graph for x of he person

More information

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission

More information

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs.

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs. Physics 180A Fall 2008 Tes 1-120 poins Name Provide he bes answer o he following quesions and problems. Wach your sig figs. 1) The number of meaningful digis in a number is called he number of. When numbers

More information

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2 " P 1 = " #P L L,

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2  P 1 =  #P L L, Lecue 36 Pipe Flow and Low-eynolds numbe hydodynamics 36.1 eading fo Lecues 34-35: PKT Chape 12. Will y fo Monday?: new daa shee and daf fomula shee fo final exam. Ou saing poin fo hydodynamics ae wo equaions:

More information

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x WEEK-3 Reciaion PHYS 131 Ch. 3: FOC 1, 3, 4, 6, 14. Problems 9, 37, 41 & 71 and Ch. 4: FOC 1, 3, 5, 8. Problems 3, 5 & 16. Feb 8, 018 Ch. 3: FOC 1, 3, 4, 6, 14. 1. (a) The horizonal componen of he projecile

More information

2002 November 14 Exam III Physics 191

2002 November 14 Exam III Physics 191 November 4 Exam III Physics 9 Physical onsans: Earh s free-fall acceleraion = g = 9.8 m/s ircle he leer of he single bes answer. quesion is worh poin Each 3. Four differen objecs wih masses: m = kg, m

More information

Ferent equation of the Universe

Ferent equation of the Universe Feen equaion of he Univese I discoveed a new Gaviaion heoy which beaks he wall of Planck scale! Absac My Nobel Pize - Discoveies Feen equaion of he Univese: i + ia = = (... N... N M m i= i ) i a M m j=

More information

Solution: b All the terms must have the dimension of acceleration. We see that, indeed, each term has the units of acceleration

Solution: b All the terms must have the dimension of acceleration. We see that, indeed, each term has the units of acceleration PHYS 54 Tes Pracice Soluions Spring 8 Q: [4] Knowing ha in he ne epression a is acceleraion, v is speed, is posiion and is ime, from a dimensional v poin of view, he equaion a is a) incorrec b) correc

More information

Physics 131- Fundamentals of Physics for Biologists I

Physics 131- Fundamentals of Physics for Biologists I 10/3/2012 - Fundamenals of Physics for iologiss I Professor: Wolfgang Loser 10/3/2012 Miderm review -How can we describe moion (Kinemaics) - Wha is responsible for moion (Dynamics) wloser@umd.edu Movie

More information

x i v x t a dx dt t x

x i v x t a dx dt t x Physics 3A: Basic Physics I Shoup - Miderm Useful Equaions A y A sin A A A y an A y A A = A i + A y j + A z k A * B = A B cos(θ) A B = A B sin(θ) A * B = A B + A y B y + A z B z A B = (A y B z A z B y

More information

Two-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch

Two-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch Two-dimensional Effecs on he CS Ineacion Foces fo an Enegy-Chiped Bunch ui Li, J. Bisognano,. Legg, and. Bosch Ouline 1. Inoducion 2. Pevious 1D and 2D esuls fo Effecive CS Foce 3. Bunch Disibuion Vaiaion

More information

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a Kinemaics Paper 1 1. The graph below shows he ariaion wih ime of he acceleraion a of an objec from = o = T. a T The shaded area under he graph represens change in A. displacemen. B. elociy. C. momenum.

More information

Suggested Practice Problems (set #2) for the Physics Placement Test

Suggested Practice Problems (set #2) for the Physics Placement Test Deparmen of Physics College of Ars and Sciences American Universiy of Sharjah (AUS) Fall 014 Suggesed Pracice Problems (se #) for he Physics Placemen Tes This documen conains 5 suggesed problems ha are

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

Lecture 4 Kinetics of a particle Part 3: Impulse and Momentum

Lecture 4 Kinetics of a particle Part 3: Impulse and Momentum MEE Engineering Mechanics II Lecure 4 Lecure 4 Kineics of a paricle Par 3: Impulse and Momenum Linear impulse and momenum Saring from he equaion of moion for a paricle of mass m which is subjeced o an

More information

Summary:Linear Motion

Summary:Linear Motion Summary:Linear Moion D Saionary objec V Consan velociy D Disance increase uniformly wih ime D = v. a Consan acceleraion V D V = a. D = ½ a 2 Velociy increases uniformly wih ime Disance increases rapidly

More information

Displacement ( x) x x x

Displacement ( x) x x x Kinemaics Kinemaics is he branch of mechanics ha describes he moion of objecs wihou necessarily discussing wha causes he moion. 1-Dimensional Kinemaics (or 1- Dimensional moion) refers o moion in a sraigh

More information

Page 1 o 13 1. The brighes sar in he nigh sky is α Canis Majoris, also known as Sirius. I lies 8.8 ligh-years away. Express his disance in meers. ( ligh-year is he disance coered by ligh in one year. Ligh

More information

Physics 20 Lesson 5 Graphical Analysis Acceleration

Physics 20 Lesson 5 Graphical Analysis Acceleration Physics 2 Lesson 5 Graphical Analysis Acceleraion I. Insananeous Velociy From our previous work wih consan speed and consan velociy, we know ha he slope of a posiion-ime graph is equal o he velociy of

More information

EN221 - Fall HW # 7 Solutions

EN221 - Fall HW # 7 Solutions EN221 - Fall2008 - HW # 7 Soluions Pof. Vivek Shenoy 1.) Show ha he fomulae φ v ( φ + φ L)v (1) u v ( u + u L)v (2) can be pu ino he alenaive foms φ φ v v + φv na (3) u u v v + u(v n)a (4) (a) Using v

More information

Chapter 12: Velocity, acceleration, and forces

Chapter 12: Velocity, acceleration, and forces To Feel a Force Chaper Spring, Chaper : A. Saes of moion For moion on or near he surface of he earh, i is naural o measure moion wih respec o objecs fixed o he earh. The 4 hr. roaion of he earh has a measurable

More information

Sharif University of Technology - CEDRA By: Professor Ali Meghdari

Sharif University of Technology - CEDRA By: Professor Ali Meghdari Shaif Univesiy of echnology - CEDRA By: Pofesso Ali Meghai Pupose: o exen he Enegy appoach in eiving euaions of oion i.e. Lagange s Meho fo Mechanical Syses. opics: Genealize Cooinaes Lagangian Euaion

More information

Physics Notes - Ch. 2 Motion in One Dimension

Physics Notes - Ch. 2 Motion in One Dimension Physics Noes - Ch. Moion in One Dimension I. The naure o physical quaniies: scalars and ecors A. Scalar quaniy ha describes only magniude (how much), NOT including direcion; e. mass, emperaure, ime, olume,

More information

SUMMARY GENERAL STRATEGY IMPORTANT CONCEPTS APPLICATIONS. Problem Solving. Motion Diagrams. Pictorial Representation

SUMMARY GENERAL STRATEGY IMPORTANT CONCEPTS APPLICATIONS. Problem Solving. Motion Diagrams. Pictorial Representation The goal of Chape 1 has been o inoduce he fundamenal conceps of moion. GENERL STRTEGY Moion Diagams Help visualize moion. Povide a ool fo finding acceleaion vecos. Dos show posiions a equal ime inevals.

More information

1. Kinematics I: Position and Velocity

1. Kinematics I: Position and Velocity 1. Kinemaics I: Posiion and Velociy Inroducion The purpose of his eperimen is o undersand and describe moion. We describe he moion of an objec by specifying is posiion, velociy, and acceleraion. In his

More information

One-Dimensional Kinematics

One-Dimensional Kinematics One-Dimensional Kinemaics One dimensional kinemaics refers o moion along a sraigh line. Een hough we lie in a 3-dimension world, moion can ofen be absraced o a single dimension. We can also describe moion

More information

Physics 3A: Basic Physics I Shoup Sample Midterm. Useful Equations. x f. x i v x. a x. x i. v xi v xf. 2a x f x i. y f. a r.

Physics 3A: Basic Physics I Shoup Sample Midterm. Useful Equations. x f. x i v x. a x. x i. v xi v xf. 2a x f x i. y f. a r. Physics 3A: Basic Physics I Shoup Sample Miderm Useful Equaions A y Asin A A x A y an A y A x A = A x i + A y j + A z k A * B = A B cos(θ) A x B = A B sin(θ) A * B = A x B x + A y B y + A z B z A x B =

More information

r r r r r EE334 Electromagnetic Theory I Todd Kaiser

r r r r r EE334 Electromagnetic Theory I Todd Kaiser 334 lecoagneic Theoy I Todd Kaise Maxwell s quaions: Maxwell s equaions wee developed on expeienal evidence and have been found o goven all classical elecoagneic phenoena. They can be wien in diffeenial

More information

Physics C Rotational Motion Name: ANSWER KEY_ AP Review Packet

Physics C Rotational Motion Name: ANSWER KEY_ AP Review Packet Linea and angula analogs Linea Rotation x position x displacement v velocity a T tangential acceleation Vectos in otational motion Use the ight hand ule to detemine diection of the vecto! Don t foget centipetal

More information

Two Coupled Oscillators / Normal Modes

Two Coupled Oscillators / Normal Modes Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own

More information

Of all of the intellectual hurdles which the human mind has confronted and has overcome in the last fifteen hundred years, the one which seems to me

Of all of the intellectual hurdles which the human mind has confronted and has overcome in the last fifteen hundred years, the one which seems to me Of all of he inellecual hurdles which he human mind has confroned and has overcome in he las fifeen hundred years, he one which seems o me o have been he mos amazing in characer and he mos supendous in

More information

Physics 4A Chapter 8: Dynamics II Motion in a Plane

Physics 4A Chapter 8: Dynamics II Motion in a Plane Physics 4A Chapte 8: Dynamics II Motion in a Plane Conceptual Questions and Example Poblems fom Chapte 8 Conceptual Question 8.5 The figue below shows two balls of equal mass moving in vetical cicles.

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

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8.

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8. Kinemaics Vocabulary Kinemaics and One Dimensional Moion 8.1 WD1 Kinema means movemen Mahemaical descripion of moion Posiion Time Inerval Displacemen Velociy; absolue value: speed Acceleraion Averages

More information

7 Wave Equation in Higher Dimensions

7 Wave Equation in Higher Dimensions 7 Wave Equaion in Highe Dimensions We now conside he iniial-value poblem fo he wave equaion in n dimensions, u c u x R n u(x, φ(x u (x, ψ(x whee u n i u x i x i. (7. 7. Mehod of Spheical Means Ref: Evans,

More information

Chapter 3 Kinematics in Two Dimensions

Chapter 3 Kinematics in Two Dimensions Chaper 3 KINEMATICS IN TWO DIMENSIONS PREVIEW Two-dimensional moion includes objecs which are moing in wo direcions a he same ime, such as a projecile, which has boh horizonal and erical moion. These wo

More information

Potential Energy and Conservation of Energy

Potential Energy and Conservation of Energy Potential Enegy and Consevation of Enegy Consevative Foces Definition: Consevative Foce If the wok done by a foce in moving an object fom an initial point to a final point is independent of the path (A

More information

Lecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light

Lecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light Lecue 5 Chape 3 lecomagneic Theo, Phoons, and Ligh Gauss s Gauss s Faada s Ampèe- Mawell s + Loen foce: S C ds ds S C F dl dl q Mawell equaions d d qv A q A J ds ds In mae fields ae defined hough ineacion

More information

2001 November 15 Exam III Physics 191

2001 November 15 Exam III Physics 191 1 November 15 Eam III Physics 191 Physical Consans: Earh s free-fall acceleraion = g = 9.8 m/s 2 Circle he leer of he single bes answer. quesion is worh 1 poin Each 3. Four differen objecs wih masses:

More information

Some Basic Information about M-S-D Systems

Some Basic Information about M-S-D Systems Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,

More information

Lecture 16 (Momentum and Impulse, Collisions and Conservation of Momentum) Physics Spring 2017 Douglas Fields

Lecture 16 (Momentum and Impulse, Collisions and Conservation of Momentum) Physics Spring 2017 Douglas Fields Lecure 16 (Momenum and Impulse, Collisions and Conservaion o Momenum) Physics 160-02 Spring 2017 Douglas Fields Newon s Laws & Energy The work-energy heorem is relaed o Newon s 2 nd Law W KE 1 2 1 2 F

More information

PHYSICS 220 Lecture 02 Motion, Forces, and Newton s Laws Textbook Sections

PHYSICS 220 Lecture 02 Motion, Forces, and Newton s Laws Textbook Sections PHYSICS 220 Lecure 02 Moion, Forces, and Newon s Laws Texbook Secions 2.2-2.4 Lecure 2 Purdue Universiy, Physics 220 1 Overview Las Lecure Unis Scienific Noaion Significan Figures Moion Displacemen: Δx

More information

Chapter 7. Interference

Chapter 7. Interference Chape 7 Inefeence Pa I Geneal Consideaions Pinciple of Supeposiion Pinciple of Supeposiion When wo o moe opical waves mee in he same locaion, hey follow supeposiion pinciple Mos opical sensos deec opical

More information

~v = x. ^x + ^y + ^x + ~a = vx. v = v 0 + at. ~v P=A = ~v P=B + ~v B=A. f k = k. W tot =KE. P av =W=t. W grav = mgy 1, mgy 2 = mgh =,U grav

~v = x. ^x + ^y + ^x + ~a = vx. v = v 0 + at. ~v P=A = ~v P=B + ~v B=A. f k = k. W tot =KE. P av =W=t. W grav = mgy 1, mgy 2 = mgh =,U grav PHYSICS 5A FALL 2001 FINAL EXAM v = x a = v x = 1 2 a2 + v 0 + x 0 v 2 = v 2 0 +2a(x, x 0) a = v2 r ~v = x ~a = vx v = v 0 + a y z ^x + ^y + ^z ^x + vy x, x 0 = 1 2 (v 0 + v) ~v P=A = ~v P=B + ~v B=A ^y

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

Kinematics in two dimensions

Kinematics in two dimensions Lecure 5 Phsics I 9.18.13 Kinemaics in wo dimensions Course websie: hp://facul.uml.edu/andri_danlo/teaching/phsicsi Lecure Capure: hp://echo36.uml.edu/danlo13/phsics1fall.hml 95.141, Fall 13, Lecure 5

More information

Physics 107 TUTORIAL ASSIGNMENT #8

Physics 107 TUTORIAL ASSIGNMENT #8 Physics 07 TUTORIAL ASSIGNMENT #8 Cutnell & Johnson, 7 th edition Chapte 8: Poblems 5,, 3, 39, 76 Chapte 9: Poblems 9, 0, 4, 5, 6 Chapte 8 5 Inteactive Solution 8.5 povides a model fo solving this type

More information

3.012 Fund of Mat Sci: Bonding Lecture 1 bis. Photo courtesy of Malene Thyssen,

3.012 Fund of Mat Sci: Bonding Lecture 1 bis. Photo courtesy of Malene Thyssen, 3.012 Fund of Ma Sci: Bonding Lecue 1 bis WAVE MECHANICS Phoo couesy of Malene Thyssen, www.mfoo.dk/malene/ 3.012 Fundamenals of Maeials Science: Bonding - Nicola Mazai (MIT, Fall 2005) Las Time 1. Playes:

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

Position, Velocity, and Acceleration

Position, Velocity, and Acceleration rev 06/2017 Posiion, Velociy, and Acceleraion Equipmen Qy Equipmen Par Number 1 Dynamic Track ME-9493 1 Car ME-9454 1 Fan Accessory ME-9491 1 Moion Sensor II CI-6742A 1 Track Barrier Purpose The purpose

More information

Physics 1114: Unit 5 Hand-out Homework (Answers)

Physics 1114: Unit 5 Hand-out Homework (Answers) Physics 1114: Unit 5 Hand-out Homewok (Answes) Poblem set 1 1. The flywheel on an expeimental bus is otating at 420 RPM (evolutions pe minute). To find (a) the angula velocity in ad/s (adians/second),

More information

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws Chaper 5: Phenomena Phenomena: The reacion (aq) + B(aq) C(aq) was sudied a wo differen emperaures (98 K and 35 K). For each emperaure he reacion was sared by puing differen concenraions of he 3 species

More information

Physics 111. Exam #1. January 24, 2011

Physics 111. Exam #1. January 24, 2011 Physics 111 Exam #1 January 4, 011 Name Muliple hoice /16 Problem #1 /8 Problem # /8 Problem #3 /8 Toal /100 ParI:Muliple hoice:irclehebesansweroeachquesion.nyohermarks willnobegivencredi.eachmuliple choicequesionisworh4poinsoraoalo

More information

Orthotropic Materials

Orthotropic Materials Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε

More information

!!"#"$%&#'()!"#&'(*%)+,&',-)./0)1-*23)

!!#$%&#'()!#&'(*%)+,&',-)./0)1-*23) "#"$%&#'()"#&'(*%)+,&',-)./)1-*) #$%&'()*+,&',-.%,/)*+,-&1*#$)()5*6$+$%*,7&*-'-&1*(,-&*6&,7.$%$+*&%'(*8$&',-,%'-&1*(,-&*6&,79*(&,%: ;..,*&1$&$.$%&'()*1$$.,'&',-9*(&,%)?%*,('&5

More information

SPH3U1 Lesson 03 Kinematics

SPH3U1 Lesson 03 Kinematics SPH3U1 Lesson 03 Kinemaics GRAPHICAL ANALYSIS LEARNING GOALS Sudens will Learn how o read values, find slopes and calculae areas on graphs. Learn wha hese values mean on boh posiion-ime and velociy-ime

More information

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security 1 Geneal Non-Abiage Model I. Paial Diffeenial Equaion fo Picing A. aded Undelying Secuiy 1. Dynamics of he Asse Given by: a. ds = µ (S, )d + σ (S, )dz b. he asse can be eihe a sock, o a cuency, an index,

More information

Guest Lecturer Friday! Symbolic reasoning. Symbolic reasoning. Practice Problem day A. 2 B. 3 C. 4 D. 8 E. 16 Q25. Will Armentrout.

Guest Lecturer Friday! Symbolic reasoning. Symbolic reasoning. Practice Problem day A. 2 B. 3 C. 4 D. 8 E. 16 Q25. Will Armentrout. Pracice Problem day Gues Lecurer Friday! Will Armenrou. He d welcome your feedback! Anonymously: wrie somehing and pu i in my mailbox a 111 Whie Hall. Email me: sarah.spolaor@mail.wvu.edu Symbolic reasoning

More information

Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions

Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions Inenaional Mahemaical Foum, Vol 8, 03, no 0, 463-47 HIKARI Ld, wwwm-hikaicom Combinaoial Appoach o M/M/ Queues Using Hypegeomeic Funcions Jagdish Saan and Kamal Nain Depamen of Saisics, Univesiy of Delhi,

More information

MECHANICS OF MATERIALS Poisson s Ratio

MECHANICS OF MATERIALS Poisson s Ratio Fouh diion MCHANICS OF MATRIALS Poisson s Raio Bee Johnson DeWolf Fo a slende ba subjeced o aial loading: 0 The elongaion in he -diecion is accompanied b a conacion in he ohe diecions. Assuming ha he maeial

More information

Chapter 5. really hard to start the object moving and then, once it starts moving, you don t have to push as hard to keep it moving.

Chapter 5. really hard to start the object moving and then, once it starts moving, you don t have to push as hard to keep it moving. Chapte 5 Fiction When an object is in motion it is usually in contact with a viscous mateial (wate o ai) o some othe suface. So fa, we have assumed that moving objects don t inteact with thei suoundings

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

Best test practice: Take the past test on the class website

Best test practice: Take the past test on the class website Bes es pracice: Take he pas es on he class websie hp://communiy.wvu.edu/~miholcomb/phys11.hml I have posed he key o he WebAssign pracice es. Newon Previous Tes is Online. Forma will be idenical. You migh

More information

CHAPTER 5: Circular Motion; Gravitation

CHAPTER 5: Circular Motion; Gravitation CHAPER 5: Cicula Motion; Gavitation Solution Guide to WebAssign Pobles 5.1 [1] (a) Find the centipetal acceleation fo Eq. 5-1.. a R v ( 1.5 s) 1.10 1.4 s (b) he net hoizontal foce is causing the centipetal

More information