UNIT # 12 (PART - I)

Size: px
Start display at page:

Download "UNIT # 12 (PART - I)"

Transcription

1 JEE-Pysics od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 MODER PHYSICS (tomic ad ucla pysics) EXERCISE I c 6V c. V c. P(D) t /. T, T B ; T +B 6. so, fist alf livs (by ) xt alf livs (by B) xt tus alf livs (by +B) 8 ( Total igt alf livs) dp (P si ) F F t F psi [ umb of poto] () si 7. I poto lctic ffct t maximum vlocity of will cospodig to KE max & ot a lss ta it. 5. KE max 6. Fo tsold fqucy, KE max ( ) Isatuatio w I K 7. K max V s max K.5 K.5.5 V volts.5 98 Å V S. E k. K.E. max. fqucy of ligt dpds o poptis of catod UIT # (PRT - I) I 6. itsity bcoms t v v 5 v 8 ms 6 M 7. M M t t M t 8. () T / t t 6. days c mv ; () () T / c mv mv mv mv mv v v 9. (a) P c. K K (b) c c. (c) i c c K < K. Gat wok fuctio gat itcpt t. D bogli wavs a idp of sap & siz of t objct.. D bogli wavs a pobability wavs ad a applicabl fo all t objcts. Wav atu is obsvd fo t small paticls lik lctos.. K.E. qv p m K p ; q q q & V is sam m K m m

2 JEE-Pysics 5. (so sam) p 6. ; mk K kt 5.5 Å mkt T m kt 7. Maximum poto gy.6 V (mittd) So K max V Hc stoppig pottial is 9.6 V So V ca stop 8. R(Z ) Fo K li,, R( ) R...(i) ad R(9 ) R 8...(ii) 9 9 Dividig q. (i) by (ii), w gt 8. o. of lcto tat ca accommodat i t sll Total umb of lmts () + () + () + () 6.6V 9. E. V. E E Z E E Z E E Z 7 Z 9 6 Z Z 6 6. E max fo to 9. R(Z ) Fo wavlgt of K, to 875 R R (Z )...(i) 675 R ad R[Z B ]...(ii) By solvig q. (i) & (ii) w gt Z 6 ad Z B [Fou lmts li btw ts two]. mi V so 6. mi.6 Å. Caactistic X ays cospods to t tasitio of lctos fom o sll to aot.. x ( ). Q 7(5.6) + [(7.6)] Q 7. MV 7. Wav umb.97 ow i sis limit cospods to to Wav umb fo sis limit E.6 +.6() 79. V. C 5 C 5. () c V m 6. E 59 kv.m 7. Hig atomic o. ad ig mltig poit. 5. H p BE [( ).5] 9.5 MV 6. Duto H Q BE of poduct BE of actat [8 MV (. MV)] [8.].6 MV 7. K Q 8. p 8 5 t t 9. [ ] 5. 9 days alf livs, lft i...5% 8 Disitgatd % od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 9

3 JEE-Pysics 5. t t () () t t T / t days 5. 6% o aly / m 5. R M w. () L EXERCISE II (B) E c Z (C) v (D) K 7. R,. (a) o c c c.6z U c c c c.6.6z K max.v ;.7 V E V to..vå 7. Stoppig pottial fqucy wav lgt Satuatio cut at of potolcto missio. lso, K.E. max, P 8. () mt () B () T B T.5 V () B mke mt 9. K max V.5V K max.7v at catod K max (.7 + ) V at aod If polaity is vd, o ac at collcto.. t T / log T / T ma. ssumig to b + 69 E D C B B od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65. K.6. V U 7..V L k U k mv 5. U ; F mv k ; m v m (costat), lso V U m k m, K.E. mv 6 m 6 U, m t total gy T.E. U K.E. m m t t : t tim t : t Dcayd i tim t ( ) ( t ) Pobability tat a adioactiv ucli dos ot dcay i t to t : t t. dd quatio H H + p + () Q[ [m ( H )+m(p)+m()]+m( H )] 9 MV (B) 6 W Q t. is balacd bot i mass umb & atomic o. ( ) 5. + V s ; V s ; V s H fqucy of ici ligt ad poptis of mitt c 6. E Fo scod xcitd stat to fist xcitd stat E c c 5 9 6

4 JEE-Pysics Fo fist xcitd stat to goud xcitd stat c c E E 5 E c 7 () E 7 (B) E c 5 (C) P P 5 P 7 7. P.E. (K.E.) T.E. (P.E.) + (K.E.) T.E. (K.E.) + (K.E.) T.E. (K.E.) T.E. K.E. K.E.. V 6.6 m.6z 8.. Z; 9.8. So a lcto of KE 9.8V ca tasf its gy to tis atom. 9. Room tmpatu Upo absoptio xcitatios tak plac to may ig stats wic upo d-xcitatio mit all U.V., ifad ad visibl ligt.. Room tmpatu so lyma sis 6. mi V if V t ( mi ) 7. o. of collisio p lcto icas t itsity icass Z BE/ 8..7, t ( t ) Dcayd amout 9. P (.7) (.6) (.6) log T / ya c, P b c b 6% if P P b Sic > b > b b 7.V.6V. U C k.6v E C E.6V m i ts qustios C + 7. V. W av, ducd mass Kq mv mv ; mv. K >. V fo ilastic collisio. dcay : H, so bot Z & dcass. dcay : +, so will ot cag but Z will cag (dcass) dcay :, so will ot cag but Z will cag (icass) dcay : o cag i & Z. 5. V V mi volt. volt kv. (a) P c (b) i (c) % %. W av wok is do by oly lctic fild. Tus if E v, v dcass, & tus momtum of lcto dcass & vic vsa, wil i magtic fild v mais costat.. Fo lcto db 5 Å 5. I poto lctic ffct oly o to o Itactio.. t, ' t t 5. V 9 c, 9 t c V, V if V V + V amoic pogssio od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 9

5 JEE-Pysics od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p V V V V S 6V V V S V 7. J ( ) So J ( ) 8. E E.6 (Z ).6.6 Z () Z E E.6 Z Z.6.6 Z Z E E.6 Z.6 Z E E.6 (.) (E )(E ) (.6) Z Z (.) (E E ) (E E ) (E )(E ) (.6) Z (E )(E ) Z 9. C 5; t 5 obits a ivolvd upo comig to scod xcitd stat so t xcitd stat is 6 t [ d, d, t, 5 t, 6 t ]. O comig fom gy is gat ta, lss ta o qual to gy cospodig to. V V V a 6 a 8. T f Ti T 7 m m. o of spctal lis ( ) 5; E ; c E 95m c. (a) E.6 mv 5 (b) mv 5. Excitatio upto is quid so tat visibl lgt is mittd upo d-xcitatio. 6. So quid gy.6 9.V T T 8 7. t xcitd stat ( ) C 8. Z L ;.5 ; f Z (f L) Z Costat fo all obits. 9. K K & K, K a typ of atom. 5. Egy lasd (BE) poduct (BE) actat t 5. t, (t t ) T t t 5. Radioactivity law is valid fo lag sampls T 5. T ; R ; R ( ) T log log ; T ( ) (R R )T (log ) ( ) (R R )T 5. Fial poduct stat (R R ) d 5 5. t t 9

6 JEE-Pysics Matc t colum EXERCISE III. v,ke, J, v but ad v. Fo giv atomic umb, gy ad c fqucy of K sis is mo ta L sis. I o sis also li as mo gy o fqucy compad to tat of li.. Cosid two quatios V s mv max v...(i) o. of potolctos jctd/sc Itsity...(ii) () s fqucy is icasd kpig itsity costat. V s will icass, m(v ) will icas. max (B) s fqucy is icasd ad itsity is dcasd. V s will icas, m(v ) will icas ad max satuatio cut will dcas. (C) Its wok fuctio is icasd poto missio may stop. (D) If itsity is icasd ad fqucy is dcasd. Satuatio cut will icas.. () I alf lif activ sampl duc R Compsi o. Fo Balm sis, (low) ;, (ig) I tasitio (VI), Poto of Balm sis is absobd.. I tasitio II : E. V, E.85 V E.55 V; E c c 87 m. E. Wavlgt of adiatio m Å E Å.V So diffc of gy sould b. V (appox) Hc ad (.6)V (.5)V Tasitio is V.. Fo logst wavlgt, gy diffc sould b miimum.so i visibl potio of ydog atom, miimum gy is i tasitio VI & IV. Compsi o. i qf. M u v v v. v v v v M t M u M d M d 6 6. t magtic momt i tat cas will b zo. Compsi o. Q CV d V Dcay umb of ucli is (B) t w dcay costat, t/ t/ (C) R () t / t / T () / / Equivalt sistac. V R 6V 6 I 8 6 c P w umb of potos ici p uit tim. lso I Ic P 6 8 ( )(6.6 )( ) 6 9 ( )(.6 ) od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 9

7 JEE-Pysics m Å 687 Å.6.6 Wic cam i t ag of oag ligt.. Stoppig pottial V S 8V ad KE V S KE 8V Compsi o. Rat of poductio of B dpds o t dcayig d at () : B is dcayig simultaously wit two ats d B B d B B umb of ucli of 'B' is. B will icas w > ( + ) as iitially > +., as bot will dcay compltly : tfo B is icoct EXERCISE IV(). umb of potos fallig/s [fo poit souc].(i) Fo mtal tsold wavlgt is (ii) (iii). m o 5 m 5Å Fo mtal tsold wavlgt is.5 m o m Å c o : : 5 Mtal bcaus lis i visibl wavlgt ag. c. W av V, V Fom gap, V V lso slops of t gap J / sc 5 5. Maximum kitic gy of poto lctos K max mv max c ow lt Å t 6Å c v max 9 c v max 8 7c V od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 So fo w distac ' 9 Is 8m Is m 9 9 lso satuatd cut V d is idp of. 8. (i) V S.6V (ii) I s.6. E.7575V m E 5.66V Lt wok fuctio b V (.7575 ), V (5.66 ) V.87 V 6. KE max, lso E poto/tim c (i) W itsity of ligt is dcasd umb of potos dcass but KE max mais sam (ii) W mittig sufac is cagd, cags. So KE max cags. If mitt is cagd t +v o. of potolctos bcoms zo. (iii) Icasig, c 7. Egy ici / aa of sp / sc Egy ici o atom. Egy of o poto c J.55V 95

8 JEE-Pysics o. of poto stikig atom/sc o. of potos/ aa c c E w E' E,' c E E So w wavlgt Sic % 8. d bogli v u + at 8 mk mv E d t m Et Et 9. Fom t figu it is cla tat (P+). /.5 Å / (.5.)Å.5 Å o Å m. d Bogli wavlgt is giv by p Km K kitic gy of lcto (6.6 ) m (9. )( ) 7 K.5 J V 5.8 V.(i) Kitic gy of lcto i t obits of ydog ad ydog lik atoms Total gy Kitic gy. V (ii) T d Bogli wavlgt is giv by P Km K kitic gy of lcto Substitutig t valus, w av. Fom t giv coditios :. ad E E (.+7)V7.V E E ( ) V. V Equatio () () givs E E 7. V o Z (.6) 9 7. Z (.6) (5/6) 7. Z 9 Z Fom quatio () Z (.6) 7. () (.6) 7.. / R R B B 7R R 9 6 p 7 : 6 ; B p 5. ssumig Bo's modl to b applicabl to t H atom too; Egy of lcto.6 V 5. V iitial gy of lcto Egy of poto mittd 5 V c.8mm E (6.6 J s) 9 (..6 J)(9. kg) 6.6 m o 6.6 Å. (i) Magtic momt I m Poducd is t obit (ii) fo ydog Magtic momt M B m B si B 8m m (i)opatig voltag kv,.5% gy fo x ay 99.5 V (ii) Vlocity of ici mv V v V.6 m m/s 9 od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65

9 JEE-Pysics 7. Giv K 7 pm 7 Å E K E L c V Å 7Å K 7. 6 kv Tus E L E K 7 6 kv kv 7 6 kv 5 86 kv 8. Total mass aiilatd m MV c Total gy poducdmc MV c c Egy of poto.5 MV 9. H H H Q c..pm E.5 MV Q [ 7.] MV.6 MV. mi c V Å V t kv : mi. Å Wavlgt of K is idp of applid pottial. Fo K X ay : c.6 Z E K. ow at t/ tim, activ factio ( t ) / (.6)½.8 So dcayd factio i t/ tim is o % U T H m ( ) u E mc.76 MV If it mits poto spotaously, t quatio is ot balacd i tms of atoms & mass umb. U Pa H m ( )u.65 u m is gativ, so actio is ot spotaous. 5. Lt at t, capacito stats discagig t at tim t, activity of adioactiv sampl R R t cag o capacito Q Q t/rc ow R Q R Q t t RC R Q It is idp of tim if R C t avg C t Rc 6 RC j od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 K 6 Z Å b K mi g ad giv tat 6 bz g. Z 6 8 Z 6 Z 7.9. t ad t t t t t t, fo. ctivity of x ctivity of y o x x y y L M. 69 x ( T ) x y / x ( T ) ( T ) O Q P y x y L M. 69 ( T ) / y O QP 7 9. ft t tim activ factio 6 6 t ] 97. f/ EXERCISE IV(B) f/ Pottial at wic lcto stop comig out f f f fom sp, V f f f fom sp, V ft coctio (i) V + V V + V (V fial commo pottial) V f f (ii) Fo sp : 7f V kq f 7f f R Q fr o. of lctos flows k

10 JEE-Pysics. Pow of souc J/sc Egy of poto c.67v 6 o. of potos mittd /sc o. of potos stikig o sp of.6 m / m o. of potos passig toug aptu potos o. of potos ici / aa o sc (assumig aptu to act as a scoday poit souc) 6. poto flux 5..6 potos / m sc o. of potos ici o cto /sc.6.5 Poto cut.6 W t ls of f.6 m is usd, v.m v u f v. Tus imag will b at. m fom t ls i t dictio opposit to t sc. Distac btw sc & imag 5.7 m o. of potos stikig ls o. of potos stikig t aptu.5 6 potos. Potos tasmittd toug t ls poto/s Tis w situatio, poit souc mittig.8 6 potos/ sc of 6Å is kpt at 5.7 m away fom t sc. Tus potos stikig / aa of sc poto/sc.57 Elctos mittd.9.57 Cut.8 E p.67 V ; V K.E. max.67 V; V S.67 V.5 c. Egy of poto wit Å.V c Egy of poto wit 65Å 7.5V 98. Pow of souc 5 W fo W Cut % Cut. lso v max 65 V max 5 KE KE max 65 max 5 (. ) (7.5 ) c.v t 6Å E c V.V c V.8V 5 c V.6V 6 Ligt avig wavlgt 6 Å will ot b abl to jct lctos. Poto cut ( ) w o. of potos of ligt ici avig wavlgt Å o. of potos of ligt ici avig wavlgt 5Å. H c c c I a itcptd cm m Poto cut ( ) ( )(5 ) Momtum of paticls & Sic paticls a iical, mass of bot paticls a sam. od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65

11 JEE-Pysics mv & mv ; v v v ˆ ˆ COM i j v v v i j v v v v COM ˆ ˆ COM COM mv m v v mv mv 6. (i) E 7..6 Z 9 Z 5 (iii) 8.(i) (ii) k k.v. 9 J E max.5 V E mi.7 V mv mv E total 8 de P (loss of gy p sc) d P 8 t d 8 P 8 d P od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 (ii) E V 6.5 V 9 6 (iii) E.6 Z V c V.6 5V 6.Å (iv) (KE) st obit mv 9. (. 5) 9.6 (PE) st obit KE 688V 6 L ().5 (v) Radius (R ) z 5 V.6 m 7. Lt o. of lvl of xcitd stat C 6 (spctal lis) (d xcitd stats) o. of xcitd stat lvl +.7V (Lvl B) (Lvl ) (i) Picipal quatum o. of iitially xcitd lvl B (ii).7 k 6 6 k.7.v Ioisatio gy (iii) 9.(i) 6P ( )t c t Fo, (to collaps ad fall ito uclus) c t / t 8 sc c 9 8 mv mv ad m m Z m (iii) E t.6 E.6 8V. Lt t ag of Eat b t ya ad iitially bot w pst as ; u 8 t / t / t /.5 u 5 8 t /. u8 u 5 9 t.8 t yas. X B o. of uclus disitgatd xt t x 99

12 JEE-Pysics Fo t x x Disitgatio Egy lasd E x Egy utilizd fo mltig Mass of ic mltd E x L F E x.5. D T + P Mass dfct M M Poduct M Ractat m. amu ad amu 9.5 E mc. MV T D H m(mass dfct) M poduct M Ractat [ ] [.69+.] [ ] m.888 E m(9.5) 7.58 MV E duto E total T otal E gy T otal M ass 7.MV m m D (.).8%. (Tak a sampl of Cm atoms) dcay 96 Cm 8 96 Pu + H H m ( ) u.557 u E mc MV Egy lasd i t dcay of o atom E E fissio + E MV Total gy lasd fom t dcay of all atoms.75 MV.6 8 J Pow output Total gy lasd ma lif watts. Lt t amout of R b x 7.6 ucli lft aft 7.6 day Dcay costat.69 t.8 6 /. 6 sc /sc ctivity o. of paticls o. of utos poducd ucli.5 6 g 5. M t Tus momtum of tis mass Mv, v vlcity of mass at tim t M t v Lt at tim, dfct mass is jctd wit lativ vlocity v v jct/gam v + v Lia momtum of M at tim (t+) (M dm) (v+dv) + dm(v v ) Sic f xt (M dm) (v+dv) + dm (v v ) Mv (M dm) dv dmv v dm dv dm v v dv M dm M dm M M v v M t But M t M t ; M v v v t t M 6. Poductio of adioactiv ucli /sc Disitgatio d t ay tim t t d t t ucli disitgatd t t Egy usd i wat atig Total gy poducd E t t t.e t ms T.E t / T ms t od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65

13 JEE-Pysics EXERCISE V() TOMIC STRUCTURE & X- RY. Egy quid to ioiz a atom fom t obit is.6 + V.6 E V.V. Egy quid to mov a lcto fom a obit.6 Z is + V. So, to mov t lcto fom t fist xcitd stat of Li + is.6 E V. Ioizatio pottial will b lowst fo t atom i wic t lctos a t fatst fom t uclus. So, t atom wit t lagst siz will av t lcto t fatst fom t ucli, c to mov t lcto fom tis atom will b asist. So, t atom wit last ioizatio pottial is 55 Cs.. T wavlgts ivolvd i t spctum of dutium D a sligtly difft fom tat of ydog spctum; bcaus masss of two ucli a difft. 6. T gy of mittd poto is dictly popotioal to t diffc of t two gy lvls.tis diffcs is maximum btw lvl () ad lvl () c poto fo maximum gy will b libatd fo tis tasitio oly.. Rquid gy.6 (Z) V.6 () 8.8 V. umb of lis C C ()() (). Egy L ( ) I ( ) w µ ducd mass so gy (m m ) mm. Egy of adiatio mittd E E Z. Wok fuctio a Cu m m m m 6 E Z E Z ( ) ( ) PHOTOELECTRIC EFFECT W W.5 W. Cu a c W a Cu f WCu a 5. Covalt bodig lcto cloud ovlappig gio lcto pobability dsity wav atu of lcto 7. Wv a atom gts d-xcitd fom ig to t low obit, it mits adiatio of a giv fqucy 6. f mv, f mv m v v f f od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 8. E f f E T potos of igst fqucy will b mittd, fo t tasitio i wic E is maximum, i.., fom to. k mv mv k (idp o ) mv ad idp of. T mv is 7. Total cag i momtum fom a flcti g sufac P P P T momtum of ici adiatio Hc, momtum tasfd E c E P c

14 JEE-Pysics 8. ccodig to Eisti's quatio of potolctic ffct fw +K max K max ()f W K max 7. d cos i d cos i 8. d cos i db mv V 5 volt q t W T slop of K vs f gap is wic is a fudamtal costat ad sam fo all mtals at all itsifis. c 9. W V, max? ; W V m V max max c m-v max m. 9. E k c.68 By solvig it. V. o. of potos mittig p scod fom a souc of pow P is (5 ) P wavlgt mittig c o P 5 P 5 d tis wavlgt coms i X ay gio. 9.5 m 5Å. Potocut Itsity Itsity du to poit souc at m is I s distac is ducd to alf, t potocut du to poit souc will icas by a facto of.. T d-bogli wavlgts ad kitic gy of a f lcto a latd as 5. Radioactivity ucla Pysics w a is umb of alf-livs. If T / 5 yas t i 5 yas, 8 8 K mk K. ccodig to Eisti's toy of potolctic ffct Egy of ici poto W + V W 6. V; V 5 V Egy of ici poto. V T wavlgt cospodig to tis gy is m wic falls i t ultaviolt gio.. T potolctic pomo is a istataous pomo, c t tim tak by a lcto to com out of mtal is appoximatly sc (foud xpimtally).. Wit t icas i wavlgt gy of t poto dcass. Tfo t KE of t lcto comig out fom t catod also dcass. Du to wic t will b a small dcas i plat cut ad oc bcoms mo ta tsold wavlgt lcto will ot com out fom t catod ad c cut will bcom zo. 5. T latio btw gy (E) of a poto ad momtum (P) associatd wit t poto is E pc T cospodig momtum E v p c c 6. Toug t compoud ca mit all t fou paticls amly lctos, potos, H + ad utos. But t paticl uto ca't b dflctd i t magtic fild, sic it is a utal paticl. Hc, t dflctabl paticls a potos, lctos ad H U U H Lt coil spd b V t by COLM u V u V 9. Rat of disitgatio at ay istat is dictly popotioal to t umb of udcayd ucli at tat istat, i.., d W dcay costat W a giv tat at t d disitgatio 5 miut at t 5 miut d disitgatio - 5 miut t od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65

15 JEE-Pysics O multiplyig bot sids by w gt () ( ) t 5 5 t Takig logaitm o bot sids w gt l l (5) l 5 l 5. l. t. 8 av b mittd av b mittd + av b mittd ducs atomic umb by icass atomic umb by + dcass atomic umb by So, Z ff 9 (8 ) + ( ) ( ) Itsity of gamma adiatio w it passs toug x is I 8 I I I x 6...(i) ad I I x...(ii) 8 6 x x 6 ad x mm 7. W kow tat, w, a t adioactiv ucli lft aft -alf livs a t iitial umb of ucli ad is umb of alf-livs, / 8 8. uclus duig dcay mits (H + ), (lctos), o utio; it dos ot mit potos duig dcay. Tfo T / 5 5 mi.. I od to fus two ucli agaist pulsio, t pulsiv pottial gy as to b supplid by kitic gy i.., PEKE 7.7 kt 8. Radius of a ucli (Mass umb) / l / R T 5 5 R 7 X, 9. 7 Li 5 R T R l 6 fmi od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p T T.7 9 k. pplyig cosvatio of momtum, w gt m v m v m v m v / lso, R m m R / m R R : m R R. Giv tat H H H gy Total B.E. of dutium uclus. MV Total B.E. of H uclus 8 MV O cosvatig gy o bot sids w gt (Egy) Duto (Egy) H + Egy lasd. 8 + E E 8..6 MV 5. t t closst poit of appoac Iitial KE Fial PE kq q / m 5. cm X Li H 7 Z O cosvatig atomic umb ad mass umbs o bot sids, w gt (7+) Z (+) 5 Hc, X B Z 5 5. Cag o -paticl Cag o tagt uclus Z W t -paticl is pojctd towads t tagt uclus, t at, t -paticl coms to momtay st. Tis positio fom tagt uclus is kow as distac of closst appoac. pplyig law of cosvatio of gy, w gt K z mv, Z, v m Li P B T paticl tat will b mittd wit Byllium will b Gamma adiatios. 5. T gy spctum of -paticls mittd fom a adioactiv souc is (E) E E

16 JEE-Pysics 5. I a ucla actio t gy mais cosvd p Li H 7 gy of potos + 7(5.6) ( 7.6) gy of poto 7.8 MV 6. Z X ( ) ( Z 6 ) ( + ) Z 8 ( ) Z 8 o. of utos Z o. of potos Z 8 Z 8 5. ucla bidig gy [Expctd mass of uclus-ctual mass of uclus]c 6. t / T t T & t T Expctd mass of uclus 8M p + 9M ctual mass of uclus M ucla bidig gy [8M p +9M M ]c 5 5. Gamma ay is a lctomagtic adiatio, du to t missio of gamma ay, it t mass umb ot t atomic umb cags. Toug t daugt uclus is sam as pat uclus but still t is a diffc i t two, i.., t daugt uclus so obtaid is pst i o of t xcitd stats ad ot i t goud stat Giv tat T T / x av Y.69 Y X.69. R. R Y X Y X X s dcay at of Y is mo ta t lmt X; c Y will dcay fast ta X Total kitic gy of poducts Y ( t t ) T (t t ) T t t T t t mi. 6. 5m M+ m m ' p' p ccodig to Cosvatio of lia momtum P' P. Tfo ' 6 5. Rlasd gy [ ] EXERCISE V-B. T cotiuous X ay spctum is sow i figu. ll wavlgts > mi a foud, w E ( 8 ) J.7 MV Total gy lasd p p m m (mass dfct) c (w m M giv) mi p M M (M m) c m p m c M M v m m c v c M M 6. Bcaus gy is lasig Bidig gy p uclo of poduct > tat of pat E > E. mi 75 Å V(i volt) H, V is t applid voltag (i Å) Å 9 Å W (V). 9. m m. umb of ucli dcass xpitially d t ad Rat of dcay Tfo, dcay pocss lasts upto t. Tfo a giv uclus may dcay at ay tim aft t. od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65

17 JEE-Pysics od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65. Sic, t wavlgt () is icasig w ca say tat t galaxy is cdig. Doppl ffct ca b giv by ' c v c v c v 76 c v c + v.6 c.6 v v.6c.6 c v c v 8...(i).6. m / s.6 v. 7 m/s If w tak t appoximatio t quatio (i) ca b v witt as c...(ii) Fom v.c ( 8 ) 656 m/s v. 8 m/s Wic is almost qual to t pvious asw. So, w may us quatio (ii) also. 5. tomic umb of o is. By t missio of two paticls, atomic umb will b ducd by. Tfo, atomic umb of t ukow lmt will b Z 6 Similaly mass umb of t ukow lmt will b Ukow uclus is cabo (, Z6). 6. Fom law of cosvatio of momtum, P P (i opposit dictios) ow d Bogli wavlgt is giv by [ Plak's costat] Sic, momtum (p) of bot t paticls is qual, tfo / 7. Bot t bta ays ad t catod ays a mad up of lctos. So, oly optio (a) is coct. (b) Gamma ays a lctomagtic wavs. (c) lpa paticls a doubly ioizd lium atoms ad (d) Potos ad utos av appoximatly t sam mass. 8. (t / ) x (t ma ) y x y x x < y Rat of dcay Iitially umb of atoms () of bot a qual but sic y > x, tfo, y will dcay at a fast at ta x. y p 9. Radius of a uclus is giv by R R / (w R.5 5 m).5 / 5 m H, is t mass umb ad mass of t uaium uclus will b m m p m p mass of poto (.67 7 kg) Dsity 7 mass m (.67 kg) volum (.5 m) R. 7 kg/m 5. Egy is lasd i a pocss w total bidig gy of t uclus ( bidig gy p uclo umb of uclos) is icasd o w ca say, w total bidig gy of poducts is mo ta t actats. By calculatio w ca s tat oly i cas of optio (c), tis apps. Giv : W Y Bidig gy of actats MV ad bidig gy of poducts (6 8.5) MV > 9 MV. Rc. I ydog atom E. lso E m w m is t mass of t lcto. H, t lcto as b placd by a paticl wos mass is doubl of a lcto. Tfo, fo tis ypottical atom gy i t obit will b Rc giv by E T logst wavlgt max (o miimum gy) poto will cospod to t tasitio of paticl fom to. c E E Rc max. KE (wit positiv sig) Pottial gy U is gativ ad Z U U. [bcaus ] (wit gativ sig) max 8 5R Similaly total gy E (wit gativ sig) Tfo, w a lcto jumps fom som xcitd stat to t goud stat, valu of will dcas. Tfo, kitic gy will icas (wit positiv sig), pottial gy ad total gy will also icas but wit gativ sig. Tus, fially kitic gy will icas, wil pottial ad total gis will dcas. 5

18 JEE-Pysics. Miimum wavlgt of cotiuous X ay spctum. is giv by mi (i Å) 75 E(i V) H, E gy of ici lctos (i V) gy cospodig to miimum wavlgt mi of X ays E 8 kv 8 V 75 mi (i Å) 8.55 lso t gy of t ici lctos (8 kv) is mo ta t ioizatio gy of t K sll lctos (i kv). Tfo, caactistic X ay spctum will also b obtaid bcaus gy of ici lcto is ig oug to kock out t lcto fom K o L slls. x (t) t (t) t x (Iitially bot av sam umb of ucli say ) t / t 9t, x ad x 9 t t 9 5. Egy of ifad adiatio is lss ta t gy of ultaviolt adiatio. I optios (a), (b) ad (c), gy lasd will b mo, wil i optio (d) oly, gy lasd will b lss... q i t t i t Substitutig i..6 9 C ad t s w gt, 6 R R...(i) H R activity of adioactiv substac aft R alf livs (giv) 6 Substitutig i quatio (i), w gt t ()t / () ( s) s. Duig dcay atomic umb (Z) ad mass umb () dos ot cag. So, t coct optio is (c) bcaus i all ot optios it Z, o bot is/a cagig.. U V V du V F d tis foc will povid t cssay ctiptal foc. mv V Hc, v V...(i) m 6. Wavlgt k is idp of t acclatig voltag (V), wil t miimum wavlgt c is ivsly popotioal to V. Tfo, as V is icasd, k mais ucagd w as c dcass o k c will icas. 7. Duig dcay, a uto is tasfomd ito a poto ad a lcto. Tis is wy atomic umb (Z umb of potos) icass by o ad mass umb ( umb of potos + utos) mais ucagd duig bta dcay. 8. T total umb of atoms ca it mai costat (as i optio a) o ca v icas (as i optios b ad c). Ty will cotiuously dcas wit tim. Tfo, (d) is t appopiat optio. 9. I scod xcitd stat, So, H Li wil E Z ad Z H, Z Li So, E Li 9 E H o E H < E Li Moov, mv...(ii) Dividig quatio (ii) by (i). m W av : m V m. ( m ) z (.5 Å) (.5)Å m z m 5 fo Fm 57 (t outmost sll) ad z (5) 5. ucla dsity is costat c, mass volum m V. 6. Giv tat K + K 5.5 MV...(i) Fom cosvatio of lia momtum, p p K (6m) K (m) as P Km K 5 K...(ii) Solvig quatio (i) ad (ii). W gt K KE of paticl 5. MV od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 6

19 JEE-Pysics 7. Satuatio cut is popotioal to itsity wil stoppig pottial icass wit icas i fqucy. Hc, f a f b wil I a < I b 8. me c E o / E 9. ctivity ducs fom 6 dps to dps i days. It implis tat alf lif of t adioactiv sampl is days. I 8 days (o 5. Momtum of stikig lctos p Kitic gy of stikig lctos K p m m Tis also, maximum gy of X ay potos. Tfo, c m m c od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 two alf livs) activity will mai t of t iitial activity. Hc, t iitial activity of t sampl is 6 dps dps. T fist poto will xcit t ydog atom (i goud stat) i fist xcitd stat (as E E.V). Hc duig d xcitatio a poto of.v will b lasd. T scod poto of gy 5V ca iois t atom. Hc t balac gy i..,(5.6)v. V is taid by t lcto. Tfo, by t scod poto a lcto of gy. V will b lasd.. Z Z (Z ) Z Solvig tis, w gt Z 6. ( H ) 8 O 6 Mass dfct m {(.6) 5.999}. amu Egy lasd p oxyg ucli (.) (9. 8) MV. MV. ft two alf livs / t factio of ucli will mai udcayd. / t factio will dcay. Hc, t pobability tat a uclus dcays i two alf livs is /.. T sis i U V gio is Lym sis. Logst wavlgt cospods to miimum gy wic occus i tasitio fom to. R...(i) T smallst wavlgt i t ifad gio cospods to maximum gy of Pasc sis. R...(ii) Solvig quatio (i) ad (ii), w gt 8.5 m 6. Rst mass of pat uclus sould b gat ta t st mass of daugt ucli. 7. s fo cotiuous X ays mi c so cut off V wavlgt dpds o t acclatig pottial ad is idp of atu of tagt. 8. ctivity & T / So 5 ( ) & ( ) T T T T m ligt caot mit lcto fo mtal of wok fuctio V, so satuat cut dcass fo P to Q to R. lso V sp > V sq > V s. Egy ici Pow(tim) M C Q So momtum E c ( mw) ( s) kg m / sc. Du to mass dfct (wic is fially sposibl fo t bidig gy of t uclus), mass of a uclus is always lss ta t sum of masss of its costitut paticls.. is mad up of potos plus utos. Tfo, mass of uclus, M < (m p + m ) lso, avi t uclus, mo is t mass dfct. Tus, (m + m p ) M > (m p + m ) M (m p + m )>M M M < M + (m p + m ) ow sic M < (m p + m ) M < M. 7

20 JEE-Pysics. Tim piod, T v (i t stat) i.. T But ad Tfo, T Hc,. Fom t latio, V c Giv T 8T c V Tis is quatio of staigt li. Slop is ta c c c c : : : : : :.m.m.m Å 5Å 5 Å Violt colou as wavlgt Å. So violt colou ca jct potolctos fom mtal ad mtal.. ( ) Fo < < 5, o fusio mass umb fo compoud uclus is lss ta Bidig gy p uclo mais sam o gy is lasd ( B ) Fo 5 < <, o fusio mass umb fo compoud uclus is btw & Bidig gy p uclo icass Egy is lasd. ( C ) Fo < <, o fissio, t mass umb of poduct ucli will b btw 5 & Bidig gy p uclo dcass o gy is lasd ( D ) Fo < < 6, o fissio, t mass umb of poduct ucli will b btw & Bidig gy p uclo icass Egy is lasd. 5 gula momtum a 9a lso a Z Z Fo d- xci tati o Rz R Fo to : 9 R 9 R Fo to : 9 R 9 5R Fo to : R R Matc t colum. (i) Egy of capacito is lss / cv tfo p. (ii) wok is do o t gas c gy icass tfo q. (iii) W mass dcass its gy icass. (iv) w cut flows gy of magtic fild is gatd tfo t. (B) wok is do o t gas (C) mass is ducd ad mass dfct is covtd ito gy. (D) mass dcass du to mass dfct. Matcig List Typ. Compltig actio i list II 5 5 () 8 O 7 8 () 9 U () 8 Bi 8 9 () 9 Pu 57 + dcay) T (lpa dcay) Pb (Poto missio) La (Fissio) Compsio Basd Qustio Compsi o#..v H.V.6V.V H +.V 6.V.6V 5.V Fo H atom E. V, Tis gos to xcit H + io fom to od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 8

21 JEE-Pysics. Fo visibl gio E <. V ad i tis cas E. ( 6).6 V c E V Å 8Å.8 7 m.6v. Ratio of kitic gy Sic & Z K Z K Z K fo H, Z fo H + K Compsi o#. Du to t ig tmpatu dvlopd as a sult of collisio & fusio causs t co of fusio acto to plasma. Compsio. E I I / I I 8 I. E E 8 I 8 I I.87 kgm Momt of itia of CO molcul about ct of mass : mm I w m m. KT T Kqq KT Kqq T K T K 6 I I.87 m m 6 5 / m m 6 Paagap 5.. m Po Pb H Q od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65. t > 5 t > 5 t 6 > 5 Compsi o#. E. p m... (i) p... (ii) By quatio (i) ad (ii) E [ m ( ) m(a ) a fo statioay wav o stig fixd at bot d] E a (6.6 ) E m a (. ) (6.6 ) E 8 mv 9. mv v m v m(a) M M M C Total gy lasd Po Pb H [( ) ( )] 9 MV [.588] 9 MV 5.76 MV Kitic gy of paticl 6 Q 5.76 MV MV 59 KV 5.9. Oly i optio (C); sum of masss of poduct is lss t sum of mass of actat M alpa Subjctiv fo actio H H 6 Li. s M Li < M Duto +. (i) Lt at tim t, umb of adioactiv ucli a. t at of fomatio of ucli of d Solvig tis quatio, w gt [ ( ) t ]...(i) d d t 9

22 JEE-Pysics (ii) (i) Substitutig ad t t / quatio (i) w gt, (ii) Substitutig ad t i quatio (i), w gt () i E 5 E 5 E.8 V E 5 E 5 E.5 V > V E E E.6 V E E E. V > V Hc, t gy of mittd potos i t ag of V ad V a. V duig combiatio ad.8 V ad.6 aft combiatio.. Giv wok fuctio W.9 V Wavlgt of ici ligt, m. Lt goud stat gy (i V) b E T, fom t giv coditio E E V Egy of ici ligt, E c (Substitutig t valus of, c ad ).V Tfo, maximum kitic gy of potolcto K max E W (..9). V ow t situatio is as sow blow : E E V E ' V...(i) ad E E.8 V E E.8 V K max.v 5 E 5.V E.8 V...(ii) -paticls + H i fout xcitd stat o 5 (Z) H + Egy of lcto i t xcitd stat of H + (5) will b E 5 (.6) Z E 5.6 V () (5). V Tfo, gy lasd duig t combiatio. (.). V Similaly gis i ot gy stats of H + will () b E.6 () () E.6 () () E.6. V 6. V.6V T possibl tasitios a E 5 E 5 E. V < V Fom quatio (i) ad (ii), 5 5 Fom quatio umb (ii), E (.8) V () (.8) V E 7.6 V E (.6)Z Z E.6 E mi E E E E ( ) E mi.58 V Z.6 7 ( 7.6) V E E 6 7 E 9 od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65

23 . Egy of ici poto, 5.(i) E i.6 V J J Egy ici p uit aa p uit (itsity) J o. of potos ici o uit aa i uit tim Tfo, umb of potos ici p uit tim o giv aa (. m ) (.8 8 ) (. ).8 But oly.8% of ici potos mit potolctos o. of potolctos mittd p scod ().5 (.8 ) 6.5 K mi ad K max E i wok fuctio K max 5. V (.6 5.6) V 5. V Lt at tim tt, umb of ucli of Y ad Z a Y ad Z. T Rat quatios of t populatio of X,Y ad Z a d X...(i) X X d Y...(ii) X X Y Y (iii) 6.(i) T populatio of X at tis momt, JEE-Pysics X Xt ( ) (.) (6.8) X.9 9 Y X Y X (.9 9 ) [Fom quatio (iv)] (.) ( / ) Z X Y Z. 9 Giv mass of paticl, m. amu ad mass of daugt uclus M.6 amu, d Bogli wavlgt of paticl, m So, momtum of paticl would b p p.5 9 kg m/s kg m/s Fom law of cosvatio of lia momtum, tis sould also b qual to t lia momtum t daugt uclus (i opposit dictio). Lt K ad K b t kitic gis of paticl ad daugt uclus. T total kitic gy i t fial stat is: K K + K p m p M od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 d Z...(iii) Y Y X (ii) Giv Y (t) Yt Xt X Fo Y to b maximum Y d Y (t) i.. X X Y Y... (iv) (fom quatio (ii)) X Xt Yt X t X ( ) Y [ ] X Y Y t Y t ( X Y )t () X X Y X Y t X ( )t Y X Y X X Y Y Substitutig t valus of X ad Y, w av. t 5() (. / ) / t6.8 s. (ii) p m M p M m Mm amu.67 7 kg Substitutig t valus, w gt 9 (.5 ) M m K M m 7 p (..6)(.67 ) 7 7 (..67 )(.6.67 ) K J MV 6.5 MV.6 K6.5 MV 6.5 Mass dfct, m amu.67 amu 9.7 Tfo, mass of pat uclus mass of paticl + mass of daugt uclus+mass dfct (m) ( )amu 7.6 amu

24 JEE-Pysics 7. T acto poducs MW pow o 9 W pow of 9 J/s of pow. T acto is to fuctio fo y. Tfo, total gy wic t acto will supply i y is E (pow) (tim) ( 9 J/s) ( 65 6 s).56 7 J But sic t fficicy of t acto is oly %, tfo actual gy dd is tims of it o.56 8 J. O uaium atom libats MV of gy o.6 o. J of gy. So, umb of uaium atoms dd a o umb of kg mols of uaium dd a (i) umb of potolctos mittd upto t s a (o. of potos fallig i uit aa i uit tim) (aa tim) 6 6 [()6 (5 ) ()] 5. 7 (ii) t tim ts cag o plat, q +(5. 7 ) (.6 9 ) 8. C ad cag o plat B, q B (.7 8. ) 5.7 C Elctic fild btw t plats E (q q ) B 8.(i) Hc, total mass of uaium quid is m ()M (6.7) (5) kg m 87 kg m.87 kg Total 6 lis a mittd. Tfo ( ) 6 So, tasitio is takig plac btw m t gy stat ad (m + ) t gy stat. E m.85v Z.6 m.85 Z m.5...(i) Similaly E m+.5 V (5.7 8.) E (5 )(8.85 ) C (iii) Egy of potolctos at plat E W (5 ) V V Icas i gy of potolctos (Ed) joul (Ed) V ( ) ( ) V V Egy of potolctos at plat B ( + )V V. E Rc (Z b) Fo K sis, b Rc(Z ) (ii) z z.6.5 (m ) (m ) Solvig quatio (i) ad (ii) fo z ad m. W gt m ad z...(ii) Smallst wavlgt cospods to maximum diffc of gis wic is obviously E m+ E m. E max.5 (.85).6 V mi c 5. m. E.6 max 9. a of plats 5 m distac btw t plats d cm m Substitutig t valus,. 8 (. 7 ) ( 8 )(Z ) (Z ) 697 Z Z. Maximum kitic gy of t potolctos would b K max E W (5 ) V V Tfo, t stoppig pottial is V. Satuatio cut dpds o t itsity of ligt ici. W t itsity is doubld t satuatio cut will also bcom two fold. T cospodig gaps a sow i figu. od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65

25 JEE-Pysics. Wavlgts cospodig to miimum wavlgt ( mi ) o maximum gy will mit potolctos avig maximum kitic gy. ( mi ) blogig to Balm sis ad lyig i t giv ag (5 m to 75 m) cospods to tasitio fom ( to ). H,. Lt b t umb of adioactiv ucli at tim t. umb of ucli dcayd i tim t a giv by ( t ), wic is also qual to t umb of bta paticls mittd duig t sam itval of tim. Fo t giv coditio, ( )...(i) Dividig quatio (ii) by (i), w gt ( +.75) ( )...(ii).6 E ().6.85V E () E E E.55 V K max Egy of poto wok fuctio V.V. Lt b t iitial umb of ucli of 8 U ft tim t, U H umb of alf livs.75...(iii) Lt us tak x T t abov quatio is x.75 x +.75 x.75 (.75) ()(.75) x ad t.5 9 t /.5 ad Pb U 9 U / Fom quatio (iii) it, but is ot accptd bcaus wic mas / U Pb.86 od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65. Hc, () () () () () () () Substitutig t giv valus,.69 (.986).95 s Ma lif t ma 6.97 s 5. (i) Fom t latio / W av / / / () 56 (ii) Z o. of utos 56 6 Rc f ka Rc (Z ) (Z ) Substitutig t giv valus of R, c ad Z. W gt f ka.55 8 Hz

26 JEE-Pysics 6. Fo < x <, PE E Kitic gy K Total gy PE E E E...(i) m(e ) Fo x >, PE 9. V s V S v s Kitic gy K Total gy E m(e )...(ii) Fom quatio (i) ad (ii), w av p mqv m q P d m q P P 8 d t t d t slop ya y.69 t /.86 giv tim is tims of t / slop costat atio. Giv T ½ 86 sc. d Factio t l 8 86 t % valu of p is 8. od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is Chapt Solutios. Th wavlgth of th pak is pic 3.898 K T 3.898 K 373K 885 This cospods to ifad adiatio.. Th tpatu is foud with 3.898 K pic T 3 9.898 K 50 T T 5773K 3. Th pow is 4 4 ( 0 ) P σ A T T ( ) ( )

More information

( ) L = D e. e e. Example:

( ) L = D e. e e. Example: xapl: A Si p juctio diod av acoss sctioal aa of, a accpto coctatio of 5 0 8 c -3 o t p-sid ad a doo coctatio of 0 6 c -3 o t -sid. T lif ti of ols i -gio is 47 s ad t lif ti of lctos i t p-gio is 5 s.

More information

( ) ( ) ( ) 2011 HSC Mathematics Solutions ( 6) ( ) ( ) ( ) π π. αβ = = 2. α β αβ. Question 1. (iii) 1 1 β + (a) (4 sig. fig.

( ) ( ) ( ) 2011 HSC Mathematics Solutions ( 6) ( ) ( ) ( ) π π. αβ = = 2. α β αβ. Question 1. (iii) 1 1 β + (a) (4 sig. fig. HS Mathmatics Solutios Qustio.778.78 ( sig. fig.) (b) (c) ( )( + ) + + + + d d (d) l ( ) () 8 6 (f) + + + + ( ) ( ) (iii) β + + α α β αβ 6 (b) si π si π π π +,π π π, (c) y + dy + d 8+ At : y + (,) dy 8(

More information

ENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles

ENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles ENGG 03 Tutoial Systms ad Cotol 9 Apil Laig Obctivs Z tasfom Complx pols Fdbac cotol systms Ac: MIT OCW 60, 6003 Diffc Equatios Cosid th systm pstd by th followig diffc quatio y[ ] x[ ] (5y[ ] 3y[ ]) wh

More information

4/20/2017. The Invention of the Modern Atom Early atomic models: Dalton model: Atom as billiard ball. The First Atomic Theorist.

4/20/2017. The Invention of the Modern Atom Early atomic models: Dalton model: Atom as billiard ball. The First Atomic Theorist. /0/017 AP PHYSICS NIT 7 Quatu Pysics, atoic, ad ucla pysics CHAPTER 7 Atoic Pysics T Ivtio of t Mod Ato Ealy atoic odls: T Fist Atoic Toist Dalto odl: Ato as billiad ball (Taslatio) Evytig is coposd of

More information

Galaxy Photometry. Recalling the relationship between flux and luminosity, Flux = brightness becomes

Galaxy Photometry. Recalling the relationship between flux and luminosity, Flux = brightness becomes Galaxy Photomty Fo galaxis, w masu a sufac flux, that is, th couts i ach pixl. Though calibatio, this is covtd to flux dsity i Jaskys ( Jy -6 W/m/Hz). Fo a galaxy at som distac, d, a pixl of sid D subtds

More information

8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions

8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions Solutios for HW 8 Captr 5 Cocptual Qustios 5.. θ dcrass. As t crystal is coprssd, t spacig d btw t plas of atos dcrass. For t first ordr diffractio =. T Bragg coditio is = d so as d dcrass, ust icras for

More information

Magnetic effects and the peculiarity of the electron spin in Atoms

Magnetic effects and the peculiarity of the electron spin in Atoms Magtic ffcts ad t pculiaity of t lcto spi i Atos Pit Za Hdik otz Nobl Piz 90 Otto t Nobl 9 Wolfgag Pauli Nobl 95 ctu Nots tuctu of Matt: Atos ad Molculs; W. Ubacs T obital agula otu of a lcto i obit iclassical

More information

Ch. 6 Free Electron Fermi Gas

Ch. 6 Free Electron Fermi Gas Ch. 6 lcto i Gas Coductio lctos i a tal ov fl without scattig b io cos so it ca b cosidd as if walitactig o f paticls followig idiac statistics. hfo th coductio lctos a fqutl calld as f lcto i gas. Coductio

More information

Potential Energy of the Electron in a Hydrogen Atom and a Model of a Virtual Particle Pair Constituting the Vacuum

Potential Energy of the Electron in a Hydrogen Atom and a Model of a Virtual Particle Pair Constituting the Vacuum Applid Physics Rsach; Vol 1, No 4; 18 ISSN 1916-9639 -ISSN 1916-9647 Publishd by Caadia Ct of Scic ad ducatio Pottial gy of th lcto i a Hydog Atom ad a Modl of a Vitual Paticl Pai Costitutig th Vacuum

More information

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom Today s topic Sttig up th Hydog Ato pobl Hydog ato pobl & Agula Motu Objctiv: to solv Schödig quatio. st Stp: to dfi th pottial fuctio Schatic of Hydog Ato Coulob s aw - Z 4ε 4ε fo H ato Nuclus Z What

More information

ATOMIC STRUCTURE EXERCISE # 1

ATOMIC STRUCTURE EXERCISE # 1 ATOMIC STRUCTURE EXERCISE #. A N A N 5 A N (5 ) 5 A 5 N. R R A /. (6) / cm 5. (6) / cm fm 5 m 5 fm. C 8. d m m A 6.75 m.59 A Fo atom.59 5. E.6 E ().6.6 e E (e + ).6.6 e E (Li + ).6 E (Be + ).6 As B 6.

More information

Mid Year Examination F.4 Mathematics Module 1 (Calculus & Statistics) Suggested Solutions

Mid Year Examination F.4 Mathematics Module 1 (Calculus & Statistics) Suggested Solutions Mid Ya Eamination 3 F. Matmatics Modul (Calculus & Statistics) Suggstd Solutions Ma pp-: 3 maks - Ma pp- fo ac qustion: mak. - Sam typ of pp- would not b countd twic fom wol pap. - In any cas, no pp maks

More information

A A A. p mu E mc K mc E p c m c. = d /dk. c = 3.00 x 10 8 m/s e = 1.60 x C 1 ev = 1.60 x J 1 Å = m M Sun = 2 x kg

A A A. p mu E mc K mc E p c m c. = d /dk. c = 3.00 x 10 8 m/s e = 1.60 x C 1 ev = 1.60 x J 1 Å = m M Sun = 2 x kg Physics 9HE-Mod Physics Fial Examiatio Mach 1, 14 (1 poits total) You may ta off this sht. ---------------------------------------------------------------------------------------------- Miscllaous data

More information

Session : Plasmas in Equilibrium

Session : Plasmas in Equilibrium Sssio : Plasmas i Equilibrium Ioizatio ad Coductio i a High-prssur Plasma A ormal gas at T < 3000 K is a good lctrical isulator, bcaus thr ar almost o fr lctros i it. For prssurs > 0.1 atm, collisio amog

More information

STRUCTURE OF ATOM -2 (Test)

STRUCTURE OF ATOM -2 (Test) STRUTURE OF TOM - (Test) o s Model, Hydoge Spectum, Potoelectic effect RE THE INSTRUTIONS REFULLY. Te test is of ous duatio.. Te maximum maks ae 75. 3. Tis test cosists of 55 questios. 4. Fo eac questio

More information

ELEC9721: Digital Signal Processing Theory and Applications

ELEC9721: Digital Signal Processing Theory and Applications ELEC97: Digital Sigal Pocssig Thoy ad Applicatios Tutoial ad solutios Not: som of th solutios may hav som typos. Q a Show that oth digital filts giv low hav th sam magitud spos: i [] [ ] m m i i i x c

More information

PART TEST-5 (PT-5) TARGET IIT-JEE 2011 CLASS-XII/XIII COURSE : ALL INDIA TEST SERIES (VIKALP)

PART TEST-5 (PT-5) TARGET IIT-JEE 2011 CLASS-XII/XIII COURSE : ALL INDIA TEST SERIES (VIKALP) PAT TEST-5 (PT-5) TAGET IIT-JEE CLASS-XII/XIII CUSE : ALL INDIA TEST SEIES (VIKALP) Hits & Solutio PAPE- PAT-I (Chmisty) H C H I th actio squc, C Cl NaH Na C H S Na C 7 NaH Na C AgN Na C (A) NaCl H Na

More information

and integrated over all, the result is f ( 0) ] //Fourier transform ] //inverse Fourier transform

and integrated over all, the result is f ( 0) ] //Fourier transform ] //inverse Fourier transform NANO 70-Nots Chapt -Diactd bams Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio. Idal cystals a iiit this, so th will b som iiitis lii about. Usually, th iiit quatity oly ists

More information

GRAVITATION. (d) If a spring balance having frequency f is taken on moon (having g = g / 6) it will have a frequency of (a) 6f (b) f / 6

GRAVITATION. (d) If a spring balance having frequency f is taken on moon (having g = g / 6) it will have a frequency of (a) 6f (b) f / 6 GVITTION 1. Two satllits and o ound a plant P in cicula obits havin adii 4 and spctivly. If th spd of th satllit is V, th spd of th satllit will b 1 V 6 V 4V V. Th scap vlocity on th sufac of th ath is

More information

The Hydrogen Atom. Chapter 7

The Hydrogen Atom. Chapter 7 Th Hyog Ato Chapt 7 Hyog ato Th vy fist pobl that Schöig hislf tackl with his w wav quatio Poucig th oh s gy lvls a o! lctic pottial gy still plays a ol i a subatoic lvl btw poto a lcto V 4 Schöig q. fo

More information

(Reference: sections in Silberberg 5 th ed.)

(Reference: sections in Silberberg 5 th ed.) ALE. Atomic Structur Nam HEM K. Marr Tam No. Sctio What is a atom? What is th structur of a atom? Th Modl th structur of a atom (Rfrc: sctios.4 -. i Silbrbrg 5 th d.) Th subatomic articls that chmists

More information

They must have different numbers of electrons orbiting their nuclei. They must have the same number of neutrons in their nuclei.

They must have different numbers of electrons orbiting their nuclei. They must have the same number of neutrons in their nuclei. 37 1 How may utros ar i a uclus of th uclid l? 20 37 54 2 crtai lmt has svral isotops. Which statmt about ths isotops is corrct? Thy must hav diffrt umbrs of lctros orbitig thir ucli. Thy must hav th sam

More information

Quantization of Atomic Energy Levels

Quantization of Atomic Energy Levels Quatizatio o Atomic Egy Lvls Atomic Scta Th ist al clus to th tu atu ad stuctu o atoms 1 w ovidd by atomic scta Dcads bo uthod dvlod his modl o th atom ad Plack advacd his quatum thoy o blackbody adiatio,

More information

1985 AP Calculus BC: Section I

1985 AP Calculus BC: Section I 985 AP Calculus BC: Sctio I 9 Miuts No Calculator Nots: () I this amiatio, l dots th atural logarithm of (that is, logarithm to th bas ). () Ulss othrwis spcifid, th domai of a fuctio f is assumd to b

More information

RADIO-FREQUENCY WALL CONDITIONING FOR STEADY-STATE STELLARATORS

RADIO-FREQUENCY WALL CONDITIONING FOR STEADY-STATE STELLARATORS RAIO-FREQUENCY WALL CONIIONING FOR SEAY-SAE SELLARAORS Yu. S. Kulyk, V.E.Moisko,. Wauts, A.I.Lyssoiva Istitut of Plasma Physics, Natioal Scic Ct Khakiv Istitut of Physics ad chology, 68 Khakiv, Ukai Laboatoy

More information

STATISTICAL MECHANICS OF DIATOMIC GASES

STATISTICAL MECHANICS OF DIATOMIC GASES Pof. D. I. ass Phys54 7 -Ma-8 Diatomic_Gas (Ashly H. Cat chapt 5) SAISICAL MECHAICS OF DIAOMIC GASES - Fo monatomic gas whos molculs hav th dgs of fdom of tanslatoy motion th intnal u 3 ngy and th spcific

More information

Free carriers in materials

Free carriers in materials Lctu / F cais in matials Mtals n ~ cm -3 Smiconductos n ~ 8... 9 cm -3 Insulatos n < 8 cm -3 φ isolatd atoms a >> a B a B.59-8 cm 3 ϕ ( Zq) q atom spacing a Lctu / "Two atoms two lvls" φ a T splitting

More information

ALLEN. è ø = MB = = (1) 3 J (2) 3 J (3) 2 3 J (4) 3J (1) (2) Ans. 4 (3) (4) W = MB(cosq 1 cos q 2 ) = MB (cos 0 cos 60 ) = MB.

ALLEN. è ø = MB = = (1) 3 J (2) 3 J (3) 2 3 J (4) 3J (1) (2) Ans. 4 (3) (4) W = MB(cosq 1 cos q 2 ) = MB (cos 0 cos 60 ) = MB. at to Succss LLEN EE INSTITUTE KT (JSTHN) HYSIS 6. magntic ndl suspndd paalll to a magntic fild quis J of wok to tun it toug 60. T toqu ndd to mata t ndl tis position will b : () J () J () J J q 0 M M

More information

2011 HSC Mathematics Extension 1 Solutions

2011 HSC Mathematics Extension 1 Solutions 0 HSC Mathmatics Etsio Solutios Qustio, (a) A B 9, (b) : 9, P 5 0, 5 5 7, si cos si d d by th quotit ul si (c) 0 si cos si si cos si 0 0 () I u du d u cos d u.du cos (f) f l Now 0 fo all l l fo all Rag

More information

coulombs or esu charge. It s mass is about 1/1837 times the mass of hydrogen atom. Thus mass of electron is

coulombs or esu charge. It s mass is about 1/1837 times the mass of hydrogen atom. Thus mass of electron is 1 ATOMIC STRUCTURE Fudamtal Particls: Mai Fudamtal Particl : (a) Elctro: It is a fudamtal particl of a atom which carris a uit gativ charg. It was discovrd by J.J. Thomso (1897) from th studis carrid out

More information

Physics 43 HW #9 Chapter 40 Key

Physics 43 HW #9 Chapter 40 Key Pysics 43 HW #9 Captr 4 Ky Captr 4 1 Aftr many ours of dilignt rsarc, you obtain t following data on t potolctric ffct for a crtain matrial: Wavlngt of Ligt (nm) Stopping Potntial (V) 36 3 4 14 31 a) Plot

More information

5.61 Fall 2007 Lecture #2 page 1. The DEMISE of CLASSICAL PHYSICS

5.61 Fall 2007 Lecture #2 page 1. The DEMISE of CLASSICAL PHYSICS 5.61 Fall 2007 Lctu #2 pag 1 Th DEMISE of CLASSICAL PHYSICS (a) Discovy of th Elcton In 1897 J.J. Thomson discovs th lcton and masus ( m ) (and inadvtntly invnts th cathod ay (TV) tub) Faaday (1860 s 1870

More information

The tight-binding method

The tight-binding method Th tight-idig thod Wa ottial aoach: tat lcto a a ga of aly f coductio lcto. ow aout iulato? ow aout d-lcto? d Tight-idig thod: gad a olid a a collctio of wa itactig utal ato. Ovla of atoic wav fuctio i

More information

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges.

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges. Optio Chaptr Ercis. Covrgs to Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Divrgs 8 Divrgs Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Covrgs to Covrgs to 8 Proof Covrgs to π l 8 l a b Divrgt π Divrgt

More information

5.1 The Nuclear Atom

5.1 The Nuclear Atom Sav My Exams! Th Hom of Rvisio For mor awsom GSE ad lvl rsourcs, visit us at www.savmyxams.co.uk/ 5.1 Th Nuclar tom Qustio Papr Lvl IGSE Subjct Physics (0625) Exam oard Topic Sub Topic ooklt ambridg Itratioal

More information

ATOMIC STRUCTURE (ADVANCED) FOUNDATION BUILDER (OBJECTIVE) By law of conservation of mass and change the missing particle in neutron

ATOMIC STRUCTURE (ADVANCED) FOUNDATION BUILDER (OBJECTIVE) By law of conservation of mass and change the missing particle in neutron . (A) Li? e 6 ATOMIC STRUCTURE (ADVANCED) FOUNDATION BUILDER (OBJECTIVE) By law of coservatio of mass ad cage te missig particle i eutro. (D) e ratio lies i te sequece p l M Particle Cage Mass + + + p

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

While flying from hot to cold, or high to low, watch out below!

While flying from hot to cold, or high to low, watch out below! STANDARD ATMOSHERE Wil flying fom ot to cold, o ig to low, watc out blow! indicatd altitud actual altitud STANDARD ATMOSHERE indicatd altitud actual altitud STANDARD ATMOSHERE Wil flying fom ot to cold,

More information

Instrumentation for Characterization of Nanomaterials (v11) 11. Crystal Potential

Instrumentation for Characterization of Nanomaterials (v11) 11. Crystal Potential Istumtatio o Chaactizatio o Naomatials (v). Cystal Pottial Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio om cystal. Idal cystals a iiit this, so th will b som iiitis lii

More information

SAFE OPERATION OF TUBULAR (PFR) ADIABATIC REACTORS. FIGURE 1: Temperature as a function of space time in an adiabatic PFR with exothermic reaction.

SAFE OPERATION OF TUBULAR (PFR) ADIABATIC REACTORS. FIGURE 1: Temperature as a function of space time in an adiabatic PFR with exothermic reaction. he 47 Lctu Fall 5 SFE OPERION OF UBULR (PFR DIBI REORS I a xthmic acti th tmatu will ctiu t is as mvs alg a lug flw act util all f th limitig actat is xhaust. Schmatically th aiabatic tmatu is as a fucti

More information

Physics of the Interstellar and Intergalactic Medium

Physics of the Interstellar and Intergalactic Medium PYA0 Sior Sophistr Physics of th Itrstllar ad Itrgalactic Mdium Lctur 7: II gios Dr Graham M. arpr School of Physics, TCD Follow-up radig for this ad t lctur Chaptr 5: Dyso ad Williams (lss dtaild) Chaptr

More information

DISCRETE-TIME RANDOM PROCESSES

DISCRETE-TIME RANDOM PROCESSES DISCRT-TIM RNDOM PROCSSS Rado Pocsss Dfiitio; Ma ad vaiac; autocoatio ad autocovaiac; Ratiosip btw ado vaiabs i a sig ado pocss; Coss-covaiac ad coss-coatio of two ado pocsss; Statioa Rado Pocsss Statioait;

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

GRAVITATION 4) R. max. 2 ..(1) ...(2)

GRAVITATION 4) R. max. 2 ..(1) ...(2) GAVITATION PVIOUS AMCT QUSTIONS NGINING. A body is pojctd vtically upwads fom th sufac of th ath with a vlocity qual to half th scap vlocity. If is th adius of th ath, maximum hight attaind by th body

More information

ATOMIC STRUCTURE (MAIN) FOUNDATION BUILDER (OBJECTIVE) By law of conservation of mass and change the missing particle in neutron

ATOMIC STRUCTURE (MAIN) FOUNDATION BUILDER (OBJECTIVE) By law of conservation of mass and change the missing particle in neutron . (A) Li? e 6 4 ATOMIC STRUCTURE (MAIN) FOUNDATION BUILDER (OBJECTIVE) By law of coservatio of mass ad cage te missig particle i eutro. (D) e ratio lies i te sequece p l M Particle Cage Mass + + 4 0 +

More information

School of Aerospace Engineering Origins of Quantum Theory. Measurements of emission of light (EM radiation) from (H) atoms found discrete lines

School of Aerospace Engineering Origins of Quantum Theory. Measurements of emission of light (EM radiation) from (H) atoms found discrete lines Ogs of Quatu Thoy Masuts of sso of lght (EM adato) fo (H) atos foud dsct ls 5 4 Abl to ft to followg ss psso ν R λ c λwavlgth, νfqucy, cspd lght RRydbg Costat (~09,7677.58c - ),,, +, +,..g.,,.6, 0.6, (Lya

More information

Aakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics

Aakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics Aakash A UNIQUE PPRTUNITY T HELP YU FULFIL YUR DREAMS Fo Class XII Studying / Passd Studnts Physics, Chmisty & Mathmatics Rgistd ffic: Aakash Tow, 8, Pusa Road, Nw Dlhi-0005. Ph.: (0) 4763456 Fax: (0)

More information

Time : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120

Time : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120 Tim : hr. Tst Papr 8 D 4//5 Bch - R Marks : SINGLE CORRECT CHOICE TYPE [4, ]. If th compl umbr z sisfis th coditio z 3, th th last valu of z is qual to : z (A) 5/3 (B) 8/3 (C) /3 (D) o of ths 5 4. Th itgral,

More information

(Lecture 5) The Atomic Models

(Lecture 5) The Atomic Models (Lctu 5) Th Atomic Modls. Ruthfod Scattig Expimt Ruthfod α- 입자산란실험 : E. Ruthfod, Gig, Masd 9 년경. (Expimtal aagmt) /, 의비율로 α- 입자들이 9 이상으로편향.. Thomso Modl of th Atom Thomso modl plum-puddig modl dispsiv

More information

Chapter Taylor Theorem Revisited

Chapter Taylor Theorem Revisited Captr 0.07 Taylor Torm Rvisitd Atr radig tis captr, you sould b abl to. udrstad t basics o Taylor s torm,. writ trascdtal ad trigoomtric uctios as Taylor s polyomial,. us Taylor s torm to id t valus o

More information

ANSWER KEY WITH SOLUTION PAPER - 2 MATHEMATICS SECTION A 1. B 2. B 3. D 4. C 5. B 6. C 7. C 8. B 9. B 10. D 11. C 12. C 13. A 14. B 15.

ANSWER KEY WITH SOLUTION PAPER - 2 MATHEMATICS SECTION A 1. B 2. B 3. D 4. C 5. B 6. C 7. C 8. B 9. B 10. D 11. C 12. C 13. A 14. B 15. TARGET IIT-JEE t [ACCELERATION] V0 to V BATCH ADVANCED TEST DATE : - 09-06 ANSWER KEY WITH SOLUTION PAPER - MATHEMATICS SECTION A. B. B. D. C 5. B 6. C 7. C 8. B 9. B 0. D. C. C. A. B 5. C 6. D 7. A 8.

More information

Q Q N, V, e, Quantum Statistics for Ideal Gas and Black Body Radiation. The Canonical Ensemble

Q Q N, V, e, Quantum Statistics for Ideal Gas and Black Body Radiation. The Canonical Ensemble Quantum Statistics fo Idal Gas and Black Body Radiation Physics 436 Lctu #0 Th Canonical Ensmbl Ei Q Q N V p i 1 Q E i i Bos-Einstin Statistics Paticls with intg valu of spin... qi... q j...... q j...

More information

Effect of alternating current on electrolytic solutions

Effect of alternating current on electrolytic solutions IOSR Joual of Egiig (IOSRJEN) -ISSN: 2250-3021, p-issn: 2278-8719 Vol. 3, Issu 8 (August. 2013), V2 PP 51-59 Effct of altatig cut o lctolytic solutios Paatap Nadi Dpatmt Elctical Egiig, Wst Bgal Uivsity

More information

CHAPTER 5 CIRCULAR MOTION

CHAPTER 5 CIRCULAR MOTION CHAPTER 5 CIRCULAR MOTION and GRAVITATION 5.1 CENTRIPETAL FORCE It is known that if a paticl mos with constant spd in a cicula path of adius, it acquis a cntiptal acclation du to th chang in th diction

More information

Great Idea #4: Parallelism. CS 61C: Great Ideas in Computer Architecture. Pipelining Hazards. Agenda. Review of Last Lecture

Great Idea #4: Parallelism. CS 61C: Great Ideas in Computer Architecture. Pipelining Hazards. Agenda. Review of Last Lecture CS 61C: Gat das i Comput Achitctu Pipliig Hazads Gu Lctu: Jui Hsia 4/12/2013 Spig 2013 Lctu #31 1 Gat da #4: Paalllism Softwa Paalll Rqus Assigd to comput.g. sach Gacia Paalll Thads Assigd to co.g. lookup,

More information

Atomic Physics 4. Name: Date: 1. The de Broglie wavelength associated with a car moving with a speed of 20 m s 1 is of the order of. A m.

Atomic Physics 4. Name: Date: 1. The de Broglie wavelength associated with a car moving with a speed of 20 m s 1 is of the order of. A m. Name: Date: Atomic Pysics 4 1. Te de Broglie wavelegt associated wit a car movig wit a speed of 0 m s 1 is of te order of A. 10 38 m. B. 10 4 m. C. 10 4 m. D. 10 38 m.. Te diagram below sows tree eergy

More information

Kinetics. Central Force Motion & Space Mechanics

Kinetics. Central Force Motion & Space Mechanics Kintics Cntal Foc Motion & Spac Mcanics Outlin Cntal Foc Motion Obital Mcanics Exampls Cntal-Foc Motion If a paticl tavls un t influnc of a foc tat as a lin of action ict towas a fix point, tn t motion

More information

We first write the integrand into partial fractions and then integrate. By EXAMPLE 27 we have the identity

We first write the integrand into partial fractions and then integrate. By EXAMPLE 27 we have the identity Solutios 8 Complete solutios to Miscellaeous Eercise 8. We ave v v v m KE m vdv m v. We ave l l EA EA EAl W d. We ave W k d k k. Multiplyig bot sides by μ gives ( ) T dt T T μθ l T l ( T) l ( T) l T T

More information

The angle between L and the z-axis is found from

The angle between L and the z-axis is found from Poblm 6 This is not a ifficult poblm but it is a al pain to tansf it fom pap into Mathca I won't giv it to you on th quiz, but know how to o it fo th xam Poblm 6 S Figu 6 Th magnitu of L is L an th z-componnt

More information

Assignment Solutions- Dual Nature. September 19

Assignment Solutions- Dual Nature. September 19 Assignment Solutions- Dual Nature September 9 03 CH 4 DUAL NATURE OF RADIATION & MATTER SOLUTIONS No. Constants used:, = 6.65 x 0-34 Js, e =.6 x 0-9 C, c = 3 x 0 8 m/s Answers Two metals A, B ave work

More information

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted?

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted? All bodis at a tmpratur T mit ad absorb thrmal lctromagtic radiatio Blackbody radiatio I thrmal quilibrium, th powr mittd quals th powr absorbd How is blackbody radiatio absorbd ad mittd? 1 2 A blackbody

More information

ATOMIC PHYSICS PREVIOUS EAMCET QUESTIONS ENGINEERING

ATOMIC PHYSICS PREVIOUS EAMCET QUESTIONS ENGINEERING ATOMIC PHYSICS PREVIOUS EAMCET QUESTIONS ENGINEERING 9. Te work function of a certain metal is. J. Ten te maximum kinetic energy of potoelectrons emitted by incident radiation of wavelengt 5 A is: (9 E)

More information

Chapter 6 Perturbation theory

Chapter 6 Perturbation theory Ct 6 Ptutio to 6. Ti-iddt odgt tutio to i o tutio sst is giv to fid solutios of λ ' ; : iltoi of si stt : igvlus of : otool igfutios of ; δ ii Rlig-Södig tutio to ' λ..6. ; : gl iltoi ': tutio λ : sll

More information

H2 Mathematics Arithmetic & Geometric Series ( )

H2 Mathematics Arithmetic & Geometric Series ( ) H Mathmatics Arithmtic & Gomtric Sris (08 09) Basic Mastry Qustios Arithmtic Progrssio ad Sris. Th rth trm of a squc is 4r 7. (i) Stat th first four trms ad th 0th trm. (ii) Show that th squc is a arithmtic

More information

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx MONTGOMERY COLLEGE Dpartmt of Mathmatics Rockvill Campus MATH 8 - REVIEW PROBLEMS. Stat whthr ach of th followig ca b itgratd by partial fractios (PF), itgratio by parts (PI), u-substitutio (U), or o of

More information

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series Chatr Ifiit Sris Pag of Sctio F Itgral Tst Chatr : Ifiit Sris By th d of this sctio you will b abl to valuat imror itgrals tst a sris for covrgc by alyig th itgral tst aly th itgral tst to rov th -sris

More information

How many neutrino species?

How many neutrino species? ow may utrio scis? Two mthods for dtrmii it lium abudac i uivrs At a collidr umbr of utrio scis Exasio of th uivrs is ovrd by th Fridma quatio R R 8G tot Kc R Whr: :ubblcostat G :Gravitatioal costat 6.

More information

Q Q N, V, e, Quantum Statistics for Ideal Gas. The Canonical Ensemble 10/12/2009. Physics 4362, Lecture #19. Dr. Peter Kroll

Q Q N, V, e, Quantum Statistics for Ideal Gas. The Canonical Ensemble 10/12/2009. Physics 4362, Lecture #19. Dr. Peter Kroll Quantum Statistics fo Idal Gas Physics 436 Lctu #9 D. Pt Koll Assistant Pofsso Dpatmnt of Chmisty & Biochmisty Univsity of Txas Alington Will psnt a lctu ntitld: Squzing Matt and Pdicting w Compounds:

More information

Lecture #2: Wave Nature of the Electron and the Internal Structure of an Atom

Lecture #2: Wave Nature of the Electron and the Internal Structure of an Atom 5.61 Fall 013 Lctur # pag 1 Lctur #: Wav Natur of t Elctro ad t Itral Structur of a Atom Last tim: Surpris Ligt as particl 1. Potolctric ffct, spcially KE vs. ν. Ligt as packts of rgy, calld potos, E =

More information

2012 GCE A Level H2 Maths Solution Paper Let x,

2012 GCE A Level H2 Maths Solution Paper Let x, GCE A Level H Maths Solutio Pape. Let, y ad z be the cost of a ticet fo ude yeas, betwee ad 5 yeas, ad ove 5 yeas categoies espectively. 9 + y + 4z =. 7 + 5y + z = 8. + 4y + 5z = 58.5 Fo ude, ticet costs

More information

Probability & Statistics,

Probability & Statistics, Probability & Statistics, BITS Pilai K K Birla Goa Campus Dr. Jajati Kshari Sahoo Dpartmt of Mathmatics BITS Pilai, K K Birla Goa Campus Poisso Distributio Poisso Distributio: A radom variabl X is said

More information

Løsningsførslag i 4M

Løsningsførslag i 4M Norges tekisk aturviteskapelige uiversitet Istitutt for matematiske fag Side 1 av 6 Løsigsførslag i 4M Oppgave 1 a) A sketch of the graph of the give f o the iterval [ 3, 3) is as follows: The Fourier

More information

The Real Hydrogen Atom

The Real Hydrogen Atom T Ra Hydog Ato ov ad i fist od gt iddt of :.6V a us tubatio toy to dti: agti ffts si-obit ad yfi -A ativisti otios Aso av ab sift du to to sfitatio. Nd QD Dia q. ad dds o H wavfutio at sou of ti fid. Vy

More information

Auchmuty High School Mathematics Department Sequences & Series Notes Teacher Version

Auchmuty High School Mathematics Department Sequences & Series Notes Teacher Version equeces ad eies Auchmuty High chool Mathematics Depatmet equeces & eies Notes Teache Vesio A sequece takes the fom,,7,0,, while 7 0 is a seies. Thee ae two types of sequece/seies aithmetic ad geometic.

More information

MATH Midterm Solutions

MATH Midterm Solutions MATH 2113 - Midtem Solutios Febuay 18 1. A bag of mables cotais 4 which ae ed, 4 which ae blue ad 4 which ae gee. a How may mables must be chose fom the bag to guaatee that thee ae the same colou? We ca

More information

ln x = n e = 20 (nearest integer)

ln x = n e = 20 (nearest integer) H JC Prlim Solutios 6 a + b y a + b / / dy a b 3/ d dy a b at, d Giv quatio of ormal at is y dy ad y wh. d a b () (,) is o th curv a+ b () y.9958 Qustio Solvig () ad (), w hav a, b. Qustio d.77 d d d.77

More information

8 - GRAVITATION Page 1

8 - GRAVITATION Page 1 8 GAVITATION Pag 1 Intoduction Ptolmy, in scond cntuy, gav gocntic thoy of plantay motion in which th Eath is considd stationay at th cnt of th univs and all th stas and th plants including th Sun volving

More information

EE 232 Lightwave Devices Lecture 3: Basic Semiconductor Physics and Optical Processes. Optical Properties of Semiconductors

EE 232 Lightwave Devices Lecture 3: Basic Semiconductor Physics and Optical Processes. Optical Properties of Semiconductors 3 Lightwav Dvics Lctur 3: Basic Smicoductor Physics ad Optical Procsss Istructor: Mig C. Wu Uivrsity of Califoria, Brly lctrical girig ad Computr Scics Dpt. 3 Lctur 3- Optical Proprtis of Smicoductors

More information

University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015

University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015 Uiversity of Wasigto Departmet of Cemistry Cemistry 453 Witer Quarter 15 Lecture 14. /11/15 Recommeded Text Readig: Atkis DePaula: 9.1, 9., 9.3 A. Te Equipartitio Priciple & Eergy Quatizatio Te Equipartio

More information

BINOMIAL THEOREM An expression consisting of two terms, connected by + or sign is called a

BINOMIAL THEOREM An expression consisting of two terms, connected by + or sign is called a BINOMIAL THEOREM hapte 8 8. Oveview: 8.. A epessio cosistig of two tems, coected by + o sig is called a biomial epessio. Fo eample, + a, y,,7 4 5y, etc., ae all biomial epessios. 8.. Biomial theoem If

More information

3.1 Atomic Structure and The Periodic Table

3.1 Atomic Structure and The Periodic Table Sav My Exams! Th Hom of Rvisio For mor awsom GSE ad lvl rsourcs, visit us at www.savmyxams.co.uk/ 3. tomic Structur ad Th Priodic Tabl Qustio Par Lvl IGSE Subjct hmistry (060) Exam oard ambridg Itratioal

More information

Acoustics and electroacoustics

Acoustics and electroacoustics coustics and lctoacoustics Chapt : Sound soucs and adiation ELEN78 - Chapt - 3 Quantitis units and smbols: f Hz : fqunc of an acoustical wav pu ton T s : piod = /f m : wavlngth= c/f Sound pssu a : pzt

More information

BINOMIAL THEOREM NCERT An expression consisting of two terms, connected by + or sign is called a

BINOMIAL THEOREM NCERT An expression consisting of two terms, connected by + or sign is called a 8. Oveview: 8.. A epessio cosistig of two tems, coected by + o sig is called a biomial epessio. Fo eample, + a, y,,7 4, etc., ae all biomial 5y epessios. 8.. Biomial theoem BINOMIAL THEOREM If a ad b ae

More information

Dual Nature of Matter and Radiation

Dual Nature of Matter and Radiation Higr Ordr Tinking Skill Qustions Dual Natur of Mattr and Radiation 1. Two bas on of rd ligt and otr of blu ligt of t sa intnsity ar incidnt on a tallic surfac to it otolctrons wic on of t two bas its lctrons

More information

Problem Value Score Earned No/Wrong Rec -3 Total

Problem Value Score Earned No/Wrong Rec -3 Total GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL of ELECTRICAL & COMPUTER ENGINEERING ECE6 Fall Quiz # Writt Eam Novmr, NAME: Solutio Kys GT Usram: LAST FIRST.g., gtiit Rcitatio Sctio: Circl t dat & tim w your Rcitatio

More information

SOLVED EXAMPLES. Ex.1 If f(x) = , then. is equal to- Ex.5. f(x) equals - (A) 2 (B) 1/2 (C) 0 (D) 1 (A) 1 (B) 2. (D) Does not exist = [2(1 h)+1]= 3

SOLVED EXAMPLES. Ex.1 If f(x) = , then. is equal to- Ex.5. f(x) equals - (A) 2 (B) 1/2 (C) 0 (D) 1 (A) 1 (B) 2. (D) Does not exist = [2(1 h)+1]= 3 SOLVED EXAMPLES E. If f() E.,,, th f() f() h h LHL RHL, so / / Lim f() quls - (D) Dos ot ist [( h)+] [(+h) + ] f(). LHL E. RHL h h h / h / h / h / h / h / h As.[C] (D) Dos ot ist LHL RHL, so giv it dos

More information

An Insight into Differentiation and Integration

An Insight into Differentiation and Integration Differetiatio A Isigt ito Differetiatio a Itegratio Differetiatio is basically a task to fi out ow oe variable is cagig i relatio to aoter variable, te latter is usually take as a cause of te cage. For

More information

Progression. CATsyllabus.com. CATsyllabus.com. Sequence & Series. Arithmetic Progression (A.P.) n th term of an A.P.

Progression. CATsyllabus.com. CATsyllabus.com. Sequence & Series. Arithmetic Progression (A.P.) n th term of an A.P. Pogessio Sequece & Seies A set of umbes whose domai is a eal umbe is called a SEQUENCE ad sum of the sequece is called a SERIES. If a, a, a, a 4,., a, is a sequece, the the expessio a + a + a + a 4 + a

More information

Lecture 7 Testing Nonlinear Inequality Restrictions 1

Lecture 7 Testing Nonlinear Inequality Restrictions 1 Eco 75 Lecture 7 Testig Noliear Iequality Restrictios I Lecture 6, we discussed te testig problems were te ull ypotesis is de ed by oliear equality restrictios: H : ( ) = versus H : ( ) 6= : () We sowed

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

Photon Energy (Particle Like)

Photon Energy (Particle Like) L8 Potovoltaic Lctu : Caactitic of Sunligt. Todd J. Kai tjkai@c.montana.du patmnt of lctical and Comput ngining Montana Stat Univity - Bozman Wav Paticl uality Ligt bav a bot a wav and a paticl Wav Popti

More information

Ideal crystal : Regulary ordered point masses connected via harmonic springs

Ideal crystal : Regulary ordered point masses connected via harmonic springs Statistical thrmodyamics of crystals Mooatomic crystal Idal crystal : Rgulary ordrd poit masss coctd via harmoic sprigs Itratomic itractios Rprstd by th lattic forc-costat quivalt atom positios miima o

More information

LESSON 15: COMPOUND INTEREST

LESSON 15: COMPOUND INTEREST High School: Expoeial Fuctios LESSON 15: COMPOUND INTEREST 1. You have see this fomula fo compoud ieest. Paamete P is the picipal amou (the moey you stat with). Paamete is the ieest ate pe yea expessed

More information

MOS transistors (in subthreshold)

MOS transistors (in subthreshold) MOS tanito (in ubthhold) Hitoy o th Tanito Th tm tanito i a gnic nam o a olid-tat dvic with 3 o mo tminal. Th ild-ct tanito tuctu wa it dcibd in a patnt by J. Lilinld in th 193! t took about 4 ya bo MOS

More information

Discussion 02 Solutions

Discussion 02 Solutions STAT 400 Discussio 0 Solutios Spig 08. ~.5 ~.6 At the begiig of a cetai study of a goup of pesos, 5% wee classified as heavy smoes, 30% as light smoes, ad 55% as osmoes. I the fiveyea study, it was detemied

More information

A novel analytic potential function applied to neutral diatomic molecules and charged lons

A novel analytic potential function applied to neutral diatomic molecules and charged lons Vol., No., 84-89 (00 http://dx.doi.o/0.46/s.00.08 Natual Scic A ovl aalytic pottial fuctio applid to utal diatomic molculs ad chad los Cha-F Yu, Cha-Ju Zhu, Cho-Hui Zha, Li-Xu So, Qiu-Pi Wa Dpatmt of physics,

More information

Physics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas

Physics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas Physics 111 Lctu 38 (Walk: 17.4-5) Phas Chang May 6, 2009 Lctu 38 1/26 Th Th Basic Phass of Matt Solid Liquid Gas Squnc of incasing molcul motion (and ngy) Lctu 38 2/26 If a liquid is put into a sald contain

More information

DUAL NATURE OF RADIATION AND MATTER

DUAL NATURE OF RADIATION AND MATTER DUAL NATURE OF RADIATION AND MATTER Important Points: 1. J.J. Tomson and Sir William Crookes studied te discarge of electricity troug gases. At about.1 mm of Hg and at ig voltage invisible streams called

More information

Physics 302 Exam Find the curve that passes through endpoints (0,0) and (1,1) and minimizes 1

Physics 302 Exam Find the curve that passes through endpoints (0,0) and (1,1) and minimizes 1 Physis Exam 6. Fid th urv that passs through dpoits (, ad (, ad miimizs J [ y' y ]dx Solutio: Si th itgrad f dos ot dpd upo th variabl of itgratio x, w will us th sod form of Eulr s quatio: f f y' y' y

More information