ATOMIC STRUCTURE EXERCISE # 1

Size: px
Start display at page:

Download "ATOMIC STRUCTURE EXERCISE # 1"

Transcription

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 E.6 E ().6.6 e E (e + ).6.6 e E (Li + ).6 E (Be + ).6 As B 6. E 78. kcal/mol.6 e.6 e E.6 kcal/mol fo atom m/sec. 9. (A) Eegy of goud state () e +.6 e 5. e (B) P.E. of Ist obit of -atom ( P.E.)T.E..6e 7.e (C) Eegy of II excited state(ii ) e () () (D) I.E. E.8 9 J J. E 5.6 (5).5 e. Li + & e + bot ave same o. of electo so spectum patte will be simila.li + e +. mq 5. x.p put value p. 5 kg ms 6. Obital agula mometum () ( ). fo 8. M 5 s, s p 6, s p 6 d 5, s M + s, s p 6, s p 6 d, s 9. + s, s p 6, s p 6 d (upaied () de ) 6 Fe+ s s p 6 s p 6 d 6 (upaied de ) 8 Ni+ s s p 6 s p 6 d 7 (upaied de ) (Li ) / / () / / 8. Let state () () (Li + ). d 7 9 Cu+ s s p 6 s p 6 d 9 (upaied de ) state () () Total spi () K e s L 8e s p M e s p 6 d N e s fo d e,. Cl s s p 6 s p 6 Fo last e, l, m ±

2 5. (A) v.8 6 v o v v (B) f o f v / f / (C) / [T ] F m v ( / ) F F / 7. Cage i agula mometum ( ) () ( ) is a itege value (( ) ) so as (B,C) So as (A,B,D) ATOMIC STRUCTURE EXERCISE #..6z E as move away fom te ucleus te eegy iceases, ece eegy is maximum at ifiite distace fom te ucleus. ( ). We electo jump ige level to lowe level, it emit te poto lowe level to ige level, It absob poto. ece 's' oly absob poto because it is lowest eegy level. 's'. R I balme seies, electo jumps ige eegy level to d eegy level. ece tid lie fom we electo jump fift eegy level to eegy level. 5 (, d 5 ). 7 Rb s s p 6 s p 6 d s p 6 5s m s 5 +/ 5. Aufbau's piciple : electo fills i obital iceasig ode of eegy level A 7 7. >,m to + s ½ Te value of cm is wog, m,,, +, + 8. ud's ule 9. C s s p 6 s p 6 d 5 s ; M + s s p 6 s p 6 d 5 s i.e. it epeset bot goud state ad catioic fom.. Fe + s s p 6 s p 6 d 5. Scodige equatio gives oly, l ad m quatum umbe, spi quatum umbe is ot elated to scodige equatio., l m. + m + m K.E. m e [ ] mc e e mc [ ] mk.e. m mass of euto ; m p mass of poto m m p atomic mass (m + m p ) [m ~ m p ] (8 + 6) m p atomic mass ( + ) 6 m p % icease 6.8 %

3 5. R fo sotest wave legt, R z x R R fo logest wave legt of paca seies, R z R 6. (IE) (IE) z Li 6 x J/atom ME R x A 7. Fe + s s p 6 s p 6 d 6 8. upaied electo () Magatic momet () ( ) BM (6) obital agula mometum () ( ) () 6 e ME M e 6 E p ; p ME M E M E ; ece e p 9. Cu + s s p 6 s p 6 d all te electo ae paied ; ece it is paamagatic (). Li (g) Li + + e 5 Li + (g) Li + + e a KJ/mol. Li + (g) Li + + e b KJ/mol. b b (IE ) (IE) (IE) z 9 Li (IE ) 87 KJ/mol Li 5 + a (IE ) a 76 KJ/mol Li Li p. R R ( ) ( ) st lie of lyme seies, d lie of lyme seies, d lie of lyme seies,. Te aode ay/caal ay idepedet to te electode mateial.. Eegy ode decide fom ( + ) ule ;( + ) is miimum eegy is miimum ; if ( + ) value is equal, lowe te value of '' lowe te eegy.. 5. (( + ) ; ( + ) ; ( + ), '' ) / 9 e > e > e > e ;.5 R mv. 5.8 mete 6. Acc to paulis a obital accomdate maximum two electo, ece paulis exclusio piciple voilates. ( ) 7. Fo d yz, xy ad xz ae odal pale ode ( ) 6 9. x y + y 8 O 8 + y 9 y 9 x x ece x Na Na peset i d peiod No of euto mole of Na.6. Mole of euto... E ev m.8 + K.E. K.E e K.E E e v v.8 6 m/s

4 . Fequecy v z/ T / z Fequecy z T T z. Radial ode () ( ) Agula ode () s, 5p x, 6 dxy avig adial ode. agula ode i all 's' obital i zeo. / 8 / ('s' ). s-obital is speical ece it is o-diectioal. (s-). B.E. I.E. (I.E.) ay atom (I.E.) z..6 z z 9 z E E e 5. x p x.p (p) (v) 8m v m v m 5. () it is a solutio of scodige wave equatio. 6. [acc to de-boglie teoy] 7. m y.5 m x, v y.75 v x mv x, m xv y x m yv y y.5m x.75 v y 5. A x 8. Obital agula mometum () ( ) s p d f 8. m ( +) m 5. M + s s p 6 s p 6 d 5. Acc to ( + ) ule, afte p, ( +) s always filled. 5. Ni + s s p 6 s p 6 d 8 magatic momet () ( ) () T z T T / l,,,,, s, p, d, f, g 8. Fom ( + ) ule, same as Q. 9. Te value of to ( ) Numbe of electo fo give value of (+) ece () ( ). v mv m m. Acc to scodige model e beave as wave oly. (e ). Te maximum pobability of fidig a electo is decibe te obital, wic is deote by. ( ). m e mv m v c c m v v v e m m c 5. E E v, E v E E v E E v, E v v + v v v v v v v v 5 5. E C E B E B E A E C E A add equatio () ad () E C E A put i equatio ()...(i)...(ii)...(iii)

5 5 6. E E E z (fo atom) (fo e + atom) 5 7. Fist Excitatio potetial () E E + 6 e 5 8., ; 5 ; 6 5 ; ( )( ) , total umbe of stectum lie ae (5 ) lyme Balme Pasce bactt lie i visible eigo. ATOMIC STRUCTURE EXERCISE # Compeesi o #. C s s p 6 s p 6 d 5 s M + s s p 6 s p 6 d 5 s Fe + s s p 6 s p 6 d 6 Co + s s p 6 s p 6 d 5. ( ).7 ( + ) + + ( + ) ( ) Numbe of upaied electo + [A] s s. Fe + [A] d 5 Ti + [A] d Co + [A] d 6 all ae avig upaied electo ece paamagetic & coloued.. Fe [A] d 6 s ud's ad Pauli's piciple is voileted. ( ) ATOMIC STRUCTURE. Distace to be tavelled fom mas to eat 8 7 km () 8 m elocity 8 8 Time D/ m/sec 8.66 sec.. ( a ) I.P. E E E ( 5.6) 5.6 l.v. ( b ) E [ ( 5.)] 5. l.v. E (m).9m Spi quatum umbe (m s ),, tat is oe obital accomodate maximum e ((m s ),, e ) Numbe of elemet i ay peiod p (fo eve peiod o.) umbe of elemet 6. fo g - sub-sell 5,,,, {g - subsell} umbe of electo ( + ) 9 8 umbe of obital ( + ) 9 ay obital ca ave moe two electo EXERCISE # [A] ( c ) E.8 ( 5.6) l.v..5 (.m).88 7 m ( d ) (i) E 5.6 ( 6) (ii) E 5.6 ( ) J e E.77 9 e

6 . J () J [6.6 5 ] E L m R.9 7 m m.? [fist lie] [secod lie] R 9 Å R...(i) R...(ii) R R R (i) (ii) 86 Å 9...(i)... (ii) ( ).7 m... (iii) we will solve te tee equatio ad we will get R.96 7 m 9. E kj/mole J/mole. IE 85.. Radius 6(R) T.E..6 l.v..85 l.v..6 9 J..7 E eg 7 Joule.7 E.7 J.E egs (b) (m) cm.7 5 cm. E I.E..7 eg/atom (m ).7 7 J m m Å m Å () ~ 5.,, E.6 ( ) kj / mole 99.5 kj/mol e

7 6. ( i ) E.6.6 []. x v t ( i i ). R 8. e x x 7..8 mole (.8 Na) atoms 7% IIId eegy level.8 Na.7 5% IId eegy level.8 Na.5 E E E.8 N A.7 IE N A.5 IE 9.68 atom 8. Numbe of atom i d obit.5 N A Numbe of atom i d obit.5 N A Total eegy evolve.5 N A (E E )+.5N A (E E ) 9. Agula mometum. e e (m) o.5 () m m 9 m.6 m.6 6 m ( ) 5 6 Å R 6 5 x Å x 8 sec oud m so, o. of evolutios ( ) / E of Ist Bo obit o.6 (i m) (m) 9 Å. 7 9 R 65 z E (. + 7).6 E E.8 8 g / atom E (E E ) m.89 6 m/sec.89 8 cm/sec

8 6. 7. ( a ) ( / ) N Å 8 p.86 Å ( b ) E.7 IE 6 ( c ) IE.7 6 e max E IE k E IE B.E kj/mole w v e/atom v v v E e E 97.9 kj/mol E 5.67 e. + E + E w + E w + E w w w w [ ] w w 6.6 ( 5. 5 ) w w w E E E w w E E...(i)...(ii) w 8.9 kj/mol w E. e (m) 6 m.6 Å. (KE) max stoppig potetial () stoppig potetial.6 5. U avg. 8 kj m U avg U avg m Å volt x m v 6.66 x.67 7 kg x x.5 m e Cu [A]. s, d 9 o o. of ex cage pai ( ) 5 6 Total excages E of ligt absobed i oe poto ( E) absobed Let potos ae absobed, teefoe, ( ) Total eegy absobed() absobed Now, E of ligt e-emitted out i oe poto emitted (E)

9 Let potos ae e-emitted te, ( ) o Eegy coveted ito K.E J % of eegy used i kietic eegy Total eegy e-emitted out emitted % As give E absobed 7 absobed. + B.. B 7 E e-emitted out emitted 7 emitted 7 58 absobed 5.57 v B v B BE 9 kj / mole Å e/mole v o (m).. mole Na No. of potos (m) m.9 7 m 5. Eegy equied to beak bod 6. Eegy give to I molecule J Also eegy used fo beakig up of I molecule J Eegy used i impatig kietic eegy to two I atoms [.7.98] 9 J K.E./iodie atom [(.7.98)/] J Å.88 pm m 5. cm/sec 5 Å m 5 P m m g 5 m 5. v m/sec v. x J/molecule J Eegy of poto used fo tis pupose J Eegy left afte dissociatio of bod ( ) m.x.x 5.7 x.7 9..

10 ATOMIC STRUCTURE. Give tat m cm. 9 m. 7 cm ad v v v R R v R...(i) Fo lie I of Balme seies R 9678 o Fo lie II of Balme seies ; R 9678 o Tus give electoic tasitio occus fom 6 t to t sell. Also by eq. (i) (6 t t ) v cm. E ext kj/mol D.E kj/mol P RT.8. T.E kJ. E(ev) (m) Eegy of st poto.8 e 8.5 Eegy of st poto.79 e. E e (E 5. e) EXERCISE # [B]. Sice we obtai 6 emissio lies, it meas electo comes fom t obit eegy emitted is equal to, less ta ad moe ta.7 e. So it ca be li tis : (6 t.7 e ) E E.7 e, E E <.7 e, E E >.7 e (a), (E E ) atom (E E ) (b) IP.6.6 (.9). e (c) Maximum eegy emittede E (E E ).75 (.9).5e Miimum eegy emittede E (E E ).66 (.9).7e 5. E 7.e(7 +.) E E 7e E.e( ) 7 e.89 E. 9.6 e E E 7. e E 7. + E. e E Å E c J.75e So electo will excite to t eegy level ad we comeback umbe of emissio lie will be 6. miimum eegy emitted E E.66 e (t 6 ) 5 E m 88 Å 7. (a) ke q J (b) At distace d 5 m let K.E. is x J ad PE k qq d PE. J By eegy cosevatio : 6. x +. x.6 J, ke PE (.6 ) d d.8 m 9 9

11 8. pe du, sice F d Å m.9 Fo stable atom F mv ke mv so mv, PE mv...()...() E (ii).59.(a). m, E (ev). W 5 e A.65A.65 m e ke E W 75 e 75 volt T.E () (b) 5 A A. A Fom bo's postulate mv puttig tis i equatio () m m m puttig tis i equatio () T.E. E m m 6 6 m 6 m k e m k e 6 9.(a) (E E ) 68 e (E E ) z 6 (b) (ke) E e (c) Eegy equied E 89.6 e.5 m E IP R.8 8 J J E E.8 8 J E E E J c m (c) sice p dp d d dp (. ) d m. Sice electo is i some exited state of e + so it's eegy.6 e so eegy eed to exitatio is also <.6 e & oly fo ydoge E E <.6 e. So. Now fo e + tis eegy is equal to te eegy gap of d ad 6t obit so iitial state is ad fial state is 6. e +.6 e <.6 e E E <.6 e e + d 6t 6. mv R 8R 9.65

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

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

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

ANSWERS, HINTS & SOLUTIONS HALF COURSE TEST VII (Main)

ANSWERS, HINTS & SOLUTIONS HALF COURSE TEST VII (Main) AIITS-HT-VII-PM-JEE(Mai)-Sol./7 I JEE Advaced 06, FIITJEE Studets bag 6 i Top 00 AIR, 7 i Top 00 AIR, 8 i Top 00 AIR. Studets fom Log Tem lassoom/ Itegated School Pogam & Studets fom All Pogams have qualified

More information

ATOMIC STRUCTURE. Gas at low pressure (10-4 atm) Production of a shadow of the solid object by cathode rays

ATOMIC STRUCTURE. Gas at low pressure (10-4 atm) Production of a shadow of the solid object by cathode rays CATHODE R AYS (Discove y of e - ) ATOMIC STRUCTURE V > 0,000 volts Gas at low pessue (0-4 atm) - Catode + Aode vaccum pump (Ivisible ays) (Catode ays) I 859, Julius plucke stated te study of coductio of

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

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

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

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

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

Electron states in a periodic potential. Assume the electrons do not interact with each other. Solve the single electron Schrodinger equation: KJ =

Electron states in a periodic potential. Assume the electrons do not interact with each other. Solve the single electron Schrodinger equation: KJ = Electo states i a peiodic potetial Assume the electos do ot iteact with each othe Solve the sigle electo Schodige equatio: 2 F h 2 + I U ( ) Ψ( ) EΨ( ). 2m HG KJ = whee U(+R)=U(), R is ay Bavais lattice

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

The Pigeonhole Principle 3.4 Binomial Coefficients

The Pigeonhole Principle 3.4 Binomial Coefficients Discete M athematic Chapte 3: Coutig 3. The Pigeohole Piciple 3.4 Biomial Coefficiets D Patic Cha School of Compute Sciece ad Egieeig South Chia Uivesity of Techology Ageda Ch 3. The Pigeohole Piciple

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

( ) ( ) Last Time. 3-D particle in box: summary. Modified Bohr model. 3-dimensional Hydrogen atom. Orbital magnetic dipole moment

( ) ( ) Last Time. 3-D particle in box: summary. Modified Bohr model. 3-dimensional Hydrogen atom. Orbital magnetic dipole moment Last Time 3-dimensional quantum states and wave functions Couse evaluations Tuesday, Dec. 9 in class Deceasing paticle size Quantum dots paticle in box) Optional exta class: eview of mateial since Exam

More information

GRAVITATIONAL FORCE IN HYDROGEN ATOM

GRAVITATIONAL FORCE IN HYDROGEN ATOM Fudametal Joual of Mode Physics Vol. 8, Issue, 015, Pages 141-145 Published olie at http://www.fdit.com/ GRAVITATIONAL FORCE IN HYDROGEN ATOM Uiesitas Pedidika Idoesia Jl DR Setyabudhi No. 9 Badug Idoesia

More information

Physics 235 Final Examination December 4, 2006 Solutions

Physics 235 Final Examination December 4, 2006 Solutions Physics 35 Fi Emitio Decembe, 6 Soutios.. Fist coside the two u quks. They e idetic spi ½ ptices, so the tot spi c be eithe o. The Pui Picipe equies tht the ove wvefuctio be echge tisymmetic. Sice the

More information

Ch 3.4 Binomial Coefficients. Pascal's Identit y and Triangle. Chapter 3.2 & 3.4. South China University of Technology

Ch 3.4 Binomial Coefficients. Pascal's Identit y and Triangle. Chapter 3.2 & 3.4. South China University of Technology Disc ete Mathem atic Chapte 3: Coutig 3. The Pigeohole Piciple 3.4 Biomial Coefficiets D Patic Cha School of Compute Sciece ad Egieeig South Chia Uivesity of Techology Pigeohole Piciple Suppose that a

More information

By the end of this section you will be able to prove the Chinese Remainder Theorem apply this theorem to solve simultaneous linear congruences

By the end of this section you will be able to prove the Chinese Remainder Theorem apply this theorem to solve simultaneous linear congruences Chapte : Theoy of Modula Aithmetic 8 Sectio D Chiese Remaide Theoem By the ed of this sectio you will be able to pove the Chiese Remaide Theoem apply this theoem to solve simultaeous liea cogueces The

More information

ANSWER KEY PHYSICS. Workdone X

ANSWER KEY PHYSICS. Workdone X ANSWER KEY PHYSICS 6 6 6 7 7 7 9 9 9 0 0 0 CHEMISTRY 6 6 6 7 7 7 9 9 9 0 0 60 MATHEMATICS 6 66 7 76 6 6 67 7 77 7 6 6 7 7 6 69 7 79 9 6 70 7 0 90 PHYSICS F L l. l A Y l A ;( A R L L A. W = (/ lod etesio

More information

a) The average (mean) of the two fractions is halfway between them: b) The answer is yes. Assume without loss of generality that p < r.

a) The average (mean) of the two fractions is halfway between them: b) The answer is yes. Assume without loss of generality that p < r. Solutios to MAML Olympiad Level 00. Factioated a) The aveage (mea) of the two factios is halfway betwee them: p ps+ q ps+ q + q s qs qs b) The aswe is yes. Assume without loss of geeality that p

More information

EXAMPLES. Leader in CBSE Coaching. Solutions of BINOMIAL THEOREM A.V.T.E. by AVTE (avte.in) Class XI

EXAMPLES. Leader in CBSE Coaching. Solutions of BINOMIAL THEOREM A.V.T.E. by AVTE (avte.in) Class XI avtei EXAMPLES Solutios of AVTE by AVTE (avtei) lass XI Leade i BSE oachig 1 avtei SHORT ANSWER TYPE 1 Fid the th tem i the epasio of 1 We have T 1 1 1 1 1 1 1 1 1 1 Epad the followig (1 + ) 4 Put 1 y

More information

MODERN PHYSICS - 1. Work function Metal (ev)

MODERN PHYSICS - 1. Work function Metal (ev) MODERN PHYSICS - PHOTOELECTRIC EFFECT : We eletomageti adiatios of suitable wavelegt ae iidet o a metalli sufae te eletos ae emitted, tis peomeo is alled poto eleti effet.. Potoeleto : Te eleto emitted

More information

Early 1900 s Max Planck derives the blackbody intensity spectrum assuming each atom to be an oscillator emitting and absorbing photons discretely.

Early 1900 s Max Planck derives the blackbody intensity spectrum assuming each atom to be an oscillator emitting and absorbing photons discretely. Peludes to Quatum Mechaics ~ 900 90 Blackbody Radiatio A blackbody absobs all icidet adiatio without eflectio o scatteig. The adiatio emitted fom a blackbody adiato by vitue of its tempeatue shows a chaacteistic

More information

CHEMISTRY. Section I. Sol.7[A] MnO + 8H + 5e Mn H. Sol.1 [D]; Sol.2 [C]; Sol.3 [D]; Sol.4 [A];

CHEMISTRY. Section I. Sol.7[A] MnO + 8H + 5e Mn H. Sol.1 [D]; Sol.2 [C]; Sol.3 [D]; Sol.4 [A]; ` HEMISTY Sectio I TAET OUSE FO IIT-JEE ALL HASE HEMISTY, MATHEMATIS & HYSIS TEST # &, TM - 6(I & II) (TAKE HOME) AE I & II (HINTS & SOLUTIONS) AE-I DATE :7-- Sol [D]; Sol []; Sol [D]; Sol [A]; Sol Sol6

More information

Experimental Fact: E = nhf

Experimental Fact: E = nhf CHAPTR 3 The xperimetal Basis of Quatum PHYS-3301 Lecture 4 Sep. 6, 2018 3.1 Discovery of the X Ray ad the lectro 3.2 Determiatio of lectro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio

More information

PHYSICS 4E FINAL EXAM SPRING QUARTER 2010 PROF. HIRSCH JUNE 11 Formulas and constants: hc =12,400 ev A ; k B. = hf " #, # $ work function.

PHYSICS 4E FINAL EXAM SPRING QUARTER 2010 PROF. HIRSCH JUNE 11 Formulas and constants: hc =12,400 ev A ; k B. = hf  #, # $ work function. PHYSICS 4E FINAL EXAM SPRING QUARTER 1 Fomulas and constants: hc =1,4 ev A ; k B =1/11,6 ev/k ; ke =14.4eVA ; m e c =.511"1 6 ev ; m p /m e =1836 Relativistic enegy - momentum elation E = m c 4 + p c ;

More information

KEY. Math 334 Midterm II Fall 2007 section 004 Instructor: Scott Glasgow

KEY. Math 334 Midterm II Fall 2007 section 004 Instructor: Scott Glasgow KEY Math 334 Midtem II Fall 7 sectio 4 Istucto: Scott Glasgow Please do NOT wite o this exam. No cedit will be give fo such wok. Rathe wite i a blue book, o o you ow pape, pefeably egieeig pape. Wite you

More information

7. QUANTUM THEORY OF THE ATOM

7. QUANTUM THEORY OF THE ATOM 7. QUANTUM TEORY OF TE ATOM Solutions to Practice Problems Note on significant figures: If te final answer to a solution needs to be rounded off, it is given first wit one nonsignificant figure, and te

More information

Physics 201 Final Exam December

Physics 201 Final Exam December Physics 01 Fial Exam December 14 017 Name (please prit): This test is admiistered uder the rules ad regulatios of the hoor system of the College of William & Mary. Sigature: Fial score: Problem 1 (5 poits)

More information

Technical Report: Bessel Filter Analysis

Technical Report: Bessel Filter Analysis Sasa Mahmoodi 1 Techical Repot: Bessel Filte Aalysis 1 School of Electoics ad Compute Sciece, Buildig 1, Southampto Uivesity, Southampto, S17 1BJ, UK, Email: sm3@ecs.soto.ac.uk I this techical epot, we

More information

= 5! 3! 2! = 5! 3! (5 3)!. In general, the number of different groups of r items out of n items (when the order is ignored) is given by n!

= 5! 3! 2! = 5! 3! (5 3)!. In general, the number of different groups of r items out of n items (when the order is ignored) is given by n! 0 Combiatoial Aalysis Copyight by Deiz Kalı 4 Combiatios Questio 4 What is the diffeece betwee the followig questio i How may 3-lette wods ca you wite usig the lettes A, B, C, D, E ii How may 3-elemet

More information

Greatest term (numerically) in the expansion of (1 + x) Method 1 Let T

Greatest term (numerically) in the expansion of (1 + x) Method 1 Let T BINOMIAL THEOREM_SYNOPSIS Geatest tem (umeically) i the epasio of ( + ) Method Let T ( The th tem) be the geatest tem. Fid T, T, T fom the give epasio. Put T T T ad. Th will give a iequality fom whee value

More information

On a Problem of Littlewood

On a Problem of Littlewood Ž. JOURAL OF MATHEMATICAL AALYSIS AD APPLICATIOS 199, 403 408 1996 ARTICLE O. 0149 O a Poblem of Littlewood Host Alze Mosbache Stasse 10, 51545 Waldbol, Gemay Submitted by J. L. Bee Received May 19, 1995

More information

DANIEL YAQUBI, MADJID MIRZAVAZIRI AND YASIN SAEEDNEZHAD

DANIEL YAQUBI, MADJID MIRZAVAZIRI AND YASIN SAEEDNEZHAD MIXED -STIRLING NUMERS OF THE SEOND KIND DANIEL YAQUI, MADJID MIRZAVAZIRI AND YASIN SAEEDNEZHAD Abstact The Stilig umbe of the secod id { } couts the umbe of ways to patitio a set of labeled balls ito

More information

JEE(MAIN) 2018 TEST PAPER WITH SOLUTION (HELD ON SUNDAY 08 th APRIL, 2018) PART C PHYSICS. Ans. (4) Sol. l. Þ k n = ALLEN. Þ k g k n = hc L.

JEE(MAIN) 2018 TEST PAPER WITH SOLUTION (HELD ON SUNDAY 08 th APRIL, 2018) PART C PHYSICS. Ans. (4) Sol. l. Þ k n = ALLEN. Þ k g k n = hc L. 6. Te agula widt of te cetal maximum i a sigle slit diffactio patte is 60. Te widt of te slit is mm. Te slit is illumiated by moocomatic plae waves. If aote slit of same widt is made ea it, Youg s figes

More information

PHYS-3301 Lecture 9. CHAPTER 5 Wave Properties of Matter and Quantum Mechanics I. 5.3: Electron Scattering. Bohr s Quantization Condition

PHYS-3301 Lecture 9. CHAPTER 5 Wave Properties of Matter and Quantum Mechanics I. 5.3: Electron Scattering. Bohr s Quantization Condition CHAPTER 5 Wave Properties of Matter ad Quatum Mecaics I PHYS-3301 Lecture 9 Sep. 5, 018 5.1 X-Ray Scatterig 5. De Broglie Waves 5.3 Electro Scatterig 5.4 Wave Motio 5.5 Waves or Particles? 5.6 Ucertaity

More information

Prof. Dr. I. Nasser atomic and molecular physics -551 (T-112) February 20, 2012 Spin_orbit.doc. The Fine Structure of the Hydrogen Atom

Prof. Dr. I. Nasser atomic and molecular physics -551 (T-112) February 20, 2012 Spin_orbit.doc. The Fine Structure of the Hydrogen Atom Pof. D. I. Nasse atomic ad molecula physics -55 (T-) Febuay 0, 0 Spi_obit.doc The Fie Stuctue of the Hydoge Atom Whilst the pedictios of the quatum model of hydoge ae a vey good appoximatio to eality,

More information

Announcements: The Rydberg formula describes. A Hydrogen-like ion is an ion that

Announcements: The Rydberg formula describes. A Hydrogen-like ion is an ion that Q: A Hydogelike io is a io that The Boh odel A) is cheically vey siila to Hydoge ios B) has the sae optical spectu as Hydoge C) has the sae ube of potos as Hydoge ) has the sae ube of electos as a Hydoge

More information

Conditional Convergence of Infinite Products

Conditional Convergence of Infinite Products Coditioal Covegece of Ifiite Poducts William F. Tech Ameica Mathematical Mothly 106 1999), 646-651 I this aticle we evisit the classical subject of ifiite poducts. Fo stadad defiitios ad theoems o this

More information

Things you should know when you leave Discussion today for one-electron atoms:

Things you should know when you leave Discussion today for one-electron atoms: E = -R Thigs ou should kow whe ou leave Discussio toda for oe-electro atoms: = -.79 0-8 J = -.6eV ΔEmatter=E-Em ; Ioizatio Eerg=E E(iitial) ΔΕlight=hνlight= IE +KE. Cosider the followig eerg levels of

More information

Negative Exponent a n = 1 a n, where a 0. Power of a Power Property ( a m ) n = a mn. Rational Exponents =

Negative Exponent a n = 1 a n, where a 0. Power of a Power Property ( a m ) n = a mn. Rational Exponents = Refeece Popetie Popetie of Expoet Let a ad b be eal umbe ad let m ad be atioal umbe. Zeo Expoet a 0 = 1, wee a 0 Quotiet of Powe Popety a m a = am, wee a 0 Powe of a Quotiet Popety ( a b m, wee b 0 b)

More information

Homonuclear Diatomic Molecule

Homonuclear Diatomic Molecule Homouclea Datomc Molecule Eegy Dagam H +, H, He +, He A B H + eq = Agstom Bg Eegy kcal/mol A B H eq = Agstom Bg Eegy kcal/mol A B He + eq = Agstom Bg Eegy kcal/mol A He eq = Bg Eegy B Kcal mol 3 Molecula

More information

Using Difference Equations to Generalize Results for Periodic Nested Radicals

Using Difference Equations to Generalize Results for Periodic Nested Radicals Usig Diffeece Equatios to Geealize Results fo Peiodic Nested Radicals Chis Lyd Uivesity of Rhode Islad, Depatmet of Mathematics South Kigsto, Rhode Islad 2 2 2 2 2 2 2 π = + + +... Vieta (593) 2 2 2 =

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

Probability theory and mathematical statistics:

Probability theory and mathematical statistics: N.I. Lobachevsky State Uiversity of Nizhi Novgorod Probability theory ad mathematical statistics: Law of Total Probability. Associate Professor A.V. Zorie Law of Total Probability. 1 / 14 Theorem Let H

More information

ratio for cathode rays is very low.

ratio for cathode rays is very low. Q. 1 Which is not basic postulate of Dalton s atomic theory? Option 1 Atoms are neither created nor destroyed in a chemical reaction Option In a given compound, the relative number and kinds of atoms are

More information

JEE(MAIN) 2018 TEST PAPER WITH ANSWER (HELD ON SUNDAY 08 th APRIL, 2018) PART C PHYSICS. 64. The density of a material in the shape of a cube ALLEN

JEE(MAIN) 2018 TEST PAPER WITH ANSWER (HELD ON SUNDAY 08 th APRIL, 2018) PART C PHYSICS. 64. The density of a material in the shape of a cube ALLEN 6. The agula width of the cetal maximum i a sigle slit diffactio patte is 60. The width of the slit is mm. The slit is illumiated by moochomatic plae waves. If aothe slit of same width is made ea it, Youg

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

THE KENNESAW STATE UNIVERSITY HIGH SCHOOL MATHEMATICS COMPETITION PART II Calculators are NOT permitted Time allowed: 2 hours

THE KENNESAW STATE UNIVERSITY HIGH SCHOOL MATHEMATICS COMPETITION PART II Calculators are NOT permitted Time allowed: 2 hours THE 06-07 KENNESAW STATE UNIVERSITY HIGH SCHOOL MATHEMATICS COMPETITION PART II Calculators are NOT permitted Time allowed: hours Let x, y, ad A all be positive itegers with x y a) Prove that there are

More information

Solutions to Final Exam Review Problems

Solutions to Final Exam Review Problems . Let f(x) 4+x. Solutios to Fial Exam Review Problems Math 5C, Witer 2007 (a) Fid the Maclauri series for f(x), ad compute its radius of covergece. Solutio. f(x) 4( ( x/4)) ( x/4) ( ) 4 4 + x. Sice the

More information

Different kinds of Mathematical Induction

Different kinds of Mathematical Induction Differet ids of Mathematical Iductio () Mathematical Iductio Give A N, [ A (a A a A)] A N () (First) Priciple of Mathematical Iductio Let P() be a propositio (ope setece), if we put A { : N p() is true}

More information

A NOTE ON DOMINATION PARAMETERS IN RANDOM GRAPHS

A NOTE ON DOMINATION PARAMETERS IN RANDOM GRAPHS Discussioes Mathematicae Gaph Theoy 28 (2008 335 343 A NOTE ON DOMINATION PARAMETERS IN RANDOM GRAPHS Athoy Boato Depatmet of Mathematics Wilfid Lauie Uivesity Wateloo, ON, Caada, N2L 3C5 e-mail: aboato@oges.com

More information

CHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method

CHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method CHAPTER 5 : SERIES 5.1 Seies 5. The Sum of a Seies 5..1 Sum of Powe of Positive Iteges 5.. Sum of Seies of Patial Factio 5..3 Diffeece Method 5.3 Test of covegece 5.3.1 Divegece Test 5.3. Itegal Test 5.3.3

More information

Office: JILA A709; Phone ;

Office: JILA A709; Phone ; Office: JILA A709; Phoe 303-49-7841; email: weberjm@jila.colorado.edu Problem Set 5 To be retured before the ed of class o Wedesday, September 3, 015 (give to me i perso or slide uder office door). 1.

More information

(b) What is the probability that a particle reaches the upper boundary n before the lower boundary m?

(b) What is the probability that a particle reaches the upper boundary n before the lower boundary m? MATH 529 The Boudary Problem The drukard s walk (or boudary problem) is oe of the most famous problems i the theory of radom walks. Oe versio of the problem is described as follows: Suppose a particle

More information

MIDTERM 3 CALCULUS 2. Monday, December 3, :15 PM to 6:45 PM. Name PRACTICE EXAM SOLUTIONS

MIDTERM 3 CALCULUS 2. Monday, December 3, :15 PM to 6:45 PM. Name PRACTICE EXAM SOLUTIONS MIDTERM 3 CALCULUS MATH 300 FALL 08 Moday, December 3, 08 5:5 PM to 6:45 PM Name PRACTICE EXAM S Please aswer all of the questios, ad show your work. You must explai your aswers to get credit. You will

More information

True Nature of Potential Energy of a Hydrogen Atom

True Nature of Potential Energy of a Hydrogen Atom True Nature of Potetial Eergy of a Hydroge Atom Koshu Suto Key words: Bohr Radius, Potetial Eergy, Rest Mass Eergy, Classical Electro Radius PACS codes: 365Sq, 365-w, 33+p Abstract I cosiderig the potetial

More information

Tutorial on Strehl ratio, wavefront power series expansion, Zernike polynomials expansion in small aberrated optical systems By Sheng Yuan

Tutorial on Strehl ratio, wavefront power series expansion, Zernike polynomials expansion in small aberrated optical systems By Sheng Yuan Tutoial on Stel atio, wavefont powe seies expansion, Zenike polynomials expansion in small abeated optical systems By Seng Yuan. Stel Ratio Te wave abeation function, (x,y, is defined as te distance, in

More information

Using Counting Techniques to Determine Probabilities

Using Counting Techniques to Determine Probabilities Kowledge ticle: obability ad Statistics Usig outig Techiques to Detemie obabilities Tee Diagams ad the Fudametal outig iciple impotat aspect of pobability theoy is the ability to detemie the total umbe

More information

( n x ( ) Last Time Exam 3 results. Question. 3-D particle in box: summary. Modified Bohr model. 3-D Hydrogen atom. r n. = n 2 a o

( n x ( ) Last Time Exam 3 results. Question. 3-D particle in box: summary. Modified Bohr model. 3-D Hydrogen atom. r n. = n 2 a o Last Time Exam 3 esults Quantum tunneling 3-dimensional wave functions Deceasing paticle size Quantum dots paticle in box) This week s honos lectue: Pof. ad histian, Positon Emission Tomogaphy Tue. Dec.

More information

ECEN 5014, Spring 2013 Special Topics: Active Microwave Circuits and MMICs Zoya Popovic, University of Colorado, Boulder

ECEN 5014, Spring 2013 Special Topics: Active Microwave Circuits and MMICs Zoya Popovic, University of Colorado, Boulder ECEN 5014, Spig 013 Special Topics: Active Micowave Cicuits ad MMICs Zoya Popovic, Uivesity of Coloado, Boulde LECTURE 7 THERMAL NOISE L7.1. INTRODUCTION Electical oise is a adom voltage o cuet which is

More information

Quantum Mechanics I. 21 April, x=0. , α = A + B = C. ik 1 A ik 1 B = αc.

Quantum Mechanics I. 21 April, x=0. , α = A + B = C. ik 1 A ik 1 B = αc. Quatum Mechaics I 1 April, 14 Assigmet 5: Solutio 1 For a particle icidet o a potetial step with E < V, show that the magitudes of the amplitudes of the icidet ad reflected waves fuctios are the same Fid

More information

Kinetics of Complex Reactions

Kinetics of Complex Reactions Kietics of Complex Reactios by Flick Colema Departmet of Chemistry Wellesley College Wellesley MA 28 wcolema@wellesley.edu Copyright Flick Colema 996. All rights reserved. You are welcome to use this documet

More information

CHAPTER 5. Theory and Solution Using Matrix Techniques

CHAPTER 5. Theory and Solution Using Matrix Techniques A SERIES OF CLASS NOTES FOR 2005-2006 TO INTRODUCE LINEAR AND NONLINEAR PROBLEMS TO ENGINEERS, SCIENTISTS, AND APPLIED MATHEMATICIANS DE CLASS NOTES 3 A COLLECTION OF HANDOUTS ON SYSTEMS OF ORDINARY DIFFERENTIAL

More information

Q.11 If S be the sum, P the product & R the sum of the reciprocals of a GP, find the value of

Q.11 If S be the sum, P the product & R the sum of the reciprocals of a GP, find the value of Brai Teasures Progressio ad Series By Abhijit kumar Jha EXERCISE I Q If the 0th term of a HP is & st term of the same HP is 0, the fid the 0 th term Q ( ) Show that l (4 36 08 up to terms) = l + l 3 Q3

More information

SEQUENCE AND SERIES NCERT

SEQUENCE AND SERIES NCERT 9. Overview By a sequece, we mea a arragemet of umbers i a defiite order accordig to some rule. We deote the terms of a sequece by a, a,..., etc., the subscript deotes the positio of the term. I view of

More information

MATH 10550, EXAM 3 SOLUTIONS

MATH 10550, EXAM 3 SOLUTIONS MATH 155, EXAM 3 SOLUTIONS 1. I fidig a approximate solutio to the equatio x 3 +x 4 = usig Newto s method with iitial approximatio x 1 = 1, what is x? Solutio. Recall that x +1 = x f(x ) f (x ). Hece,

More information

( ) 1 Comparison Functions. α is strictly increasing since ( r) ( r ) α = for any positive real number c. = 0. It is said to belong to

( ) 1 Comparison Functions. α is strictly increasing since ( r) ( r ) α = for any positive real number c. = 0. It is said to belong to Compaiso Fuctios I this lesso, we study stability popeties of the oautoomous system = f t, x The difficulty is that ay solutio of this system statig at x( t ) depeds o both t ad t = x Thee ae thee special

More information

Born-Oppenheimer Approximation and Nonadiabatic Effects. Hans Lischka University of Vienna

Born-Oppenheimer Approximation and Nonadiabatic Effects. Hans Lischka University of Vienna Bo-Oppeheie Appoxiatio ad Noadiabatic Effects Has Lischa Uivesity of Viea Typical situatio. Fac-Codo excitatio fo the iiu of the goud state. Covetioal dyaics possibly M* ad TS 3. Coical itesectio fuel

More information

Lecture 24: Observability and Constructibility

Lecture 24: Observability and Constructibility ectue 24: Obsevability ad Costuctibility 7 Obsevability ad Costuctibility Motivatio: State feedback laws deped o a kowledge of the cuet state. I some systems, xt () ca be measued diectly, e.g., positio

More information

Exercises and Problems

Exercises and Problems HW Chapter 4: Oe-Dimesioal Quatum Mechaics Coceptual Questios 4.. Five. 4.4.. is idepedet of. a b c mu ( E). a b m( ev 5 ev) c m(6 ev ev) Exercises ad Problems 4.. Model: Model the electro as a particle

More information

4. PERMUTATIONS AND COMBINATIONS Quick Review

4. PERMUTATIONS AND COMBINATIONS Quick Review 4 ERMUTATIONS AND COMBINATIONS Quick Review A aagemet that ca be fomed by takig some o all of a fiite set of thigs (o objects) is called a emutatio A emutatio is said to be a liea emutatio if the objects

More information

28 64 Ni is - g/mole Se (D)

28 64 Ni is - g/mole Se (D) EXERCISE-0 CHECK YOUR GRASP SELECT THE CORRECT ALTERNATIVE (ONLY ONE CORRECT ANSWER). Te element aving no neutron in te nucleus of its atom is - (A) ydrogen (B) nitrogen (C) elium (D) boron. Te particles

More information

Poornima University, For any query, contact us at: ,18

Poornima University, For any query, contact us at: ,18 AIEEE/1/MAHS 1 S. No Questios Solutios Q.1 he circle passig through (1, ) ad touchig the axis of x at (, ) also passes through the poit (a) (, ) (b) (, ) (c) (, ) (d) (, ) Q. ABCD is a trapezium such that

More information

IIT JAM Mathematical Statistics (MS) 2006 SECTION A

IIT JAM Mathematical Statistics (MS) 2006 SECTION A IIT JAM Mathematical Statistics (MS) 6 SECTION A. If a > for ad lim a / L >, the which of the followig series is ot coverget? (a) (b) (c) (d) (d) = = a = a = a a + / a lim a a / + = lim a / a / + = lim

More information

PLANCESS RANK ACCELERATOR

PLANCESS RANK ACCELERATOR PLANCESS RANK ACCELERATOR CHEMISTRY FOR JEE MAIN & ADVANCED 4+questios with topic wise exercises + problems of IIT-JEE & AIEEE exams of last 5 years 4 Levels of Exercises categorized ito JEE Mai & Advaced

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

Partial Differential Equations

Partial Differential Equations EE 84 Matematical Metods i Egieerig Partial Differetial Eqatios Followig are some classical partial differetial eqatios were is assmed to be a fctio of two or more variables t (time) ad y (spatial coordiates).

More information

Physics Equations Course Comparison

Physics Equations Course Comparison Physics Equatios Couse Compaiso Ietify you couse. You may use ay of the equatios beeath a to the left of you couse. Math A A PeCalculus Calculus AB o BC A to B is OR A:B is (Cocuet) (Cocuet) B B Algeba

More information

5.111 Lecture Summary #6 Monday, September 15, 2014

5.111 Lecture Summary #6 Monday, September 15, 2014 5.111 Lectue Summay #6 Monday, Septembe 15, 014 Readings fo today: Section 1.9 Atomic Obitals. Section 1.10 Electon Spin, Section 1.11 The Electonic Stuctue of Hydogen. (Same sections in 4 th ed.) Read

More information

2 Lecture 2: The Bohr atom (1913) and the Schrödinger equation (1925)

2 Lecture 2: The Bohr atom (1913) and the Schrödinger equation (1925) 1 Lectue 1: The beginnings of quantum physics 1. The Sten-Gelach expeiment. Atomic clocks 3. Planck 1900, blackbody adiation, and E ω 4. Photoelectic effect 5. Electon diffaction though cystals, de Boglie

More information

Partial match queries: a limit process

Partial match queries: a limit process Partial match queries: a limit process Nicolas Brouti Ralph Neiiger Heig Sulzbach Partial match queries: a limit process 1 / 17 Searchig geometric data ad quadtrees 1 Partial match queries: a limit process

More information

physicsandmathstutor.com

physicsandmathstutor.com physicsadmathstuto.com physicsadmathstuto.com Jue 005. A cuve has equatio blak x + xy 3y + 16 = 0. dy Fid the coodiates of the poits o the cuve whee 0. dx = (7) Q (Total 7 maks) *N03B034* 3 Tu ove physicsadmathstuto.com

More information

SAFE HANDS & IIT-ian's PACE EDT-10 (JEE) SOLUTIONS

SAFE HANDS & IIT-ian's PACE EDT-10 (JEE) SOLUTIONS . If their mea positios coicide with each other, maimum separatio will be A. Now from phasor diagram, we ca clearly see the phase differece. SAFE HANDS & IIT-ia's PACE ad Aswer : Optio (4) 5. Aswer : Optio

More information

Physics 232 Gauge invariance of the magnetic susceptibilty

Physics 232 Gauge invariance of the magnetic susceptibilty Physics 232 Gauge ivariace of the magetic susceptibilty Peter Youg (Dated: Jauary 16, 2006) I. INTRODUCTION We have see i class that the followig additioal terms appear i the Hamiltoia o addig a magetic

More information

INSTRUCTIONS/SUGGESTIONS. READ THIS CAREFULLY! OMIT ANY TWO (2) OF THE SEVEN 20 POINT QUESTIONS. OMIT ANY THREE (3) OF THE FOURTEEN 8 POINT QUESTIONS.

INSTRUCTIONS/SUGGESTIONS. READ THIS CAREFULLY! OMIT ANY TWO (2) OF THE SEVEN 20 POINT QUESTIONS. OMIT ANY THREE (3) OF THE FOURTEEN 8 POINT QUESTIONS. 1 INSTRUCTIONS/SUGGESTIONS. READ TIS CAREFULLY! OMIT ANY TWO (2) OF TE SEVEN 20 POINT QUESTIONS. OMIT ANY TREE (3) OF TE FOURTEEN 8 POINT QUESTIONS. INDICATE ON TE NEXT PAGE WIC 5 QUESTIONS ARE NOT TO

More information

Multi-Electron Atoms-Helium

Multi-Electron Atoms-Helium Multi-lecto Atos-Heliu He - se s H but with Z He - electos. No exct solutio of.. but c use H wve fuctios d eegy levels s sttig poit ucleus sceeed d so Zeffective is < sceeig is ~se s e-e epulsio fo He,

More information

Q. No. PHYSICS CHEMISTRY MATHEMATICS

Q. No. PHYSICS CHEMISTRY MATHEMATICS AITS-CRT-I (Paper-)-PCM(Sol)-JEE(Advaced)/5 FIITJEE Studets From All Programs have bagged 4 i Top 00, 66 i Top 00 ad 74 i Top 500 All Idia Raks. FIITJEE Performace i JEE (Advaced), 04: 5 FIITJEE Studets

More information

P. JOY MINOR TEST (ATOMIC STRUCTURE) TIME : 1½ Hrs. IIT-JEE CHEMISTRY SINGLE OPTION CORRECT (+3, 1) M.M. 130

P. JOY MINOR TEST (ATOMIC STRUCTURE) TIME : 1½ Hrs. IIT-JEE CHEMISTRY SINGLE OPTION CORRECT (+3, 1) M.M. 130 MINOR TEST (ATOMI STRUTURE) (PHYSIAL) HEMISTRY TIME : 1½ Hrs. SINGLE OPTION ORRET (+3, 1) M.M. 130 Q.1 When the azimuthal quantum number has the value of 2, the number of orbitals possible are : (A) 0

More information

Inverse Matrix. A meaning that matrix B is an inverse of matrix A.

Inverse Matrix. A meaning that matrix B is an inverse of matrix A. Iverse Matrix Two square matrices A ad B of dimesios are called iverses to oe aother if the followig holds, AB BA I (11) The otio is dual but we ofte write 1 B A meaig that matrix B is a iverse of matrix

More information

Disjoint Sets { 9} { 1} { 11} Disjoint Sets (cont) Operations. Disjoint Sets (cont) Disjoint Sets (cont) n elements

Disjoint Sets { 9} { 1} { 11} Disjoint Sets (cont) Operations. Disjoint Sets (cont) Disjoint Sets (cont) n elements Disjoit Sets elemets { x, x, } X =, K Opeatios x Patitioed ito k sets (disjoit sets S, S,, K Fid-Set(x - etu set cotaiig x Uio(x,y - make a ew set by combiig the sets cotaiig x ad y (destoyig them S k

More information

Quantum Theory Assignment 3

Quantum Theory Assignment 3 Quatum Theory Assigmet 3 Assigmet 3.1 1. Cosider a spi-1/ system i a magetic field i the z-directio. The Hamiltoia is give by: ) eb H = S z = ωs z. mc a) Fid the Heiseberg operators S x t), S y t), ad

More information

Shedding light on atomic energy levels (segment of Hydrogen spectrum)

Shedding light on atomic energy levels (segment of Hydrogen spectrum) 3.0 ev.85 ev.55 ev.69 ev Fri. 8.4-.7 More Eergy Quatizatio RE 8.b Mo. Tues. Wed. Lab Fri. 9.-., (.8) Mometum ad Eergy i Multiparticle Systems 9.3 Rotatioal Eergy Quiz 8 Review Exam (Ch 5-8) Exam (Ch 5-8)

More information

Sums of Involving the Harmonic Numbers and the Binomial Coefficients

Sums of Involving the Harmonic Numbers and the Binomial Coefficients Ameica Joual of Computatioal Mathematics 5 5 96-5 Published Olie Jue 5 i SciRes. http://www.scip.og/oual/acm http://dx.doi.og/.46/acm.5.58 Sums of Ivolvig the amoic Numbes ad the Biomial Coefficiets Wuyugaowa

More information

Physics 7440, Solutions to Problem Set # 8

Physics 7440, Solutions to Problem Set # 8 Physics 7440, Solutios to Problem Set # 8. Ashcroft & Mermi. For both parts of this problem, the costat offset of the eergy, ad also the locatio of the miimum at k 0, have o effect. Therefore we work with

More information

Consider unordered sample of size r. This sample can be used to make r! Ordered samples (r! permutations). unordered sample

Consider unordered sample of size r. This sample can be used to make r! Ordered samples (r! permutations). unordered sample Uodeed Samples without Replacemet oside populatio of elemets a a... a. y uodeed aagemet of elemets is called a uodeed sample of size. Two uodeed samples ae diffeet oly if oe cotais a elemet ot cotaied

More information

Lecture #5: Begin Quantum Mechanics: Free Particle and Particle in a 1D Box

Lecture #5: Begin Quantum Mechanics: Free Particle and Particle in a 1D Box 561 Fall 013 Lecture #5 page 1 Last time: Lecture #5: Begi Quatum Mechaics: Free Particle ad Particle i a 1D Box u 1 u 1-D Wave equatio = x v t * u(x,t): displacemets as fuctio of x,t * d -order: solutio

More information

1.3 Convergence Theorems of Fourier Series. k k k k. N N k 1. With this in mind, we state (without proof) the convergence of Fourier series.

1.3 Convergence Theorems of Fourier Series. k k k k. N N k 1. With this in mind, we state (without proof) the convergence of Fourier series. .3 Covergece Theorems of Fourier Series I this sectio, we preset the covergece of Fourier series. A ifiite sum is, by defiitio, a limit of partial sums, that is, a cos( kx) b si( kx) lim a cos( kx) b si(

More information

d y f f dy Numerical Solution of Ordinary Differential Equations Consider the 1 st order ordinary differential equation (ODE) . dx

d y f f dy Numerical Solution of Ordinary Differential Equations Consider the 1 st order ordinary differential equation (ODE) . dx umerical Solutio o Ordiar Dieretial Equatios Cosider te st order ordiar dieretial equatio ODE d. d Te iitial coditio ca be tae as. Te we could use a Talor series about ad obtai te complete solutio or......!!!

More information