fiziks Institute for NET/JRF, GATE, IIT JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES NUCLEAR AND PARTICLE PHYSICS NET/JRF (JUNE-2011)

Size: px
Start display at page:

Download "fiziks Institute for NET/JRF, GATE, IIT JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES NUCLEAR AND PARTICLE PHYSICS NET/JRF (JUNE-2011)"

Transcription

1 Institut fo NET/JRF, GTE, IIT JM, JEST, TIFR and GRE in PHYSICL SCIENCES Had offic fiziks, H.No., G.F, Jia Saai, Na IIT, Hauz Khas, Nw Dlhi 6 Phon: / NUCLER ND PRTICLE PHYSICS NET/JRF (JUNE-) 64 Q. Th adius of a 9Cu nuclus is masud to b cm. (). Th adius of a 7 Mg nuclus can b stimatd to b.86 - cm (b) 5. - cm.6 - cm cm Solution: Sinc R R ( ) / / / RMg Mg 7 RCu Cu 64 RMg RMg cm. RCu 4 4 (B). Th oot-man-squa (.m.s) ngy of a nuclon in a nuclus of atomic numb in its gound stat vais as: 4/ / / / (b) Q. bam of pions (π ) is incidnt on a poton tagt, giving is to th pocss π p n π π (). ssuming that th dcay pocds though stong intactions, th total isospin I and its thid componnt I fo th dcay poducts, a 5 5 I, I (b) I, I 5 I, I I, I 5 Solution: π p n π π ; I :, I : (B). Using isospin symmty, th coss-sction fo th abov pocss can b latd to that of th pocss π n pπ π (b) π p nπ π π n pπ π π p nπ π Banch offic nand Institut of Mathmatics, 8 B/6, Jia Saai, Na IIT Hauz Khas, Nw Dlhi 6 Wbsit: fiziks.physics@gmail.com

2 Institut fo NET/JRF, GTE, IIT JM, JEST, TIFR and GRE in PHYSICL SCIENCES NET/JRF (DEC-) 5 89 Q. ccoding to th shll modl th spin and paity of th two nucli 5 Sb and 8 S a, spctivly, 5 and 5 (b) 5 and and 7 7 and Q4. Th diffnc in th Coulomb ngy btwn th mio nucli 4 C and Mn 5 is 6.MV. ssuming that th nucli hav a sphically symmtic chag distibution and that is appoximatly. MV-fm, th adius of th 49 5 Mn nuclus is m 5. - m (b) m m 5 ΔW (b) R ( Z Z ) ( 5 4 ) 4.9 m. NET/JRF (JUNE-) 7 Q5. Th gound stat of Pb nuclus has spin-paity 5 J p, whil th fist xcitd stat p has J.Th lctomagntic adiation mittd whn th nuclus maks a tansition fom th fist xcitd stat to gound stat a E and E (b) M o E E o M M o M Solution: No paity chang; ΔJ, Fo Fo E typ, ( ) l l l Δπ, (fo no paity chang l ) l M typ, Δ ( ) π, (fo no paity chang l ) ΔJ, No paity chang E ; ΔJ, No paity chang M Had offic fiziks, H.No., G.F, Jia Saai, Na IIT, Hauz Khas, Nw Dlhi 6 Phon: / Banch offic nand Institut of Mathmatics, 8 B/6, Jia Saai, Na IIT Hauz Khas, Nw Dlhi 6 Wbsit: fiziks.physics@gmail.com

3 Institut fo NET/JRF, GTE, IIT JM, JEST, TIFR and GRE in PHYSICL SCIENCES Q6. Th dominant intactions undlying th following pocsss. K p π, B. K K μ μ, C. Σ p π a : stong, B: lctomagntic and; C: wak (b) : stong, B: wak and; C: wak : wak, B: lctomagntic and; C: stong : wak, B: lctomagntic and; C: wak () K p π (Stong intaction) I : (Consvd) (B) μ μ K K (Elctomagntic intaction) (C) Σ p π (Wak intaction) I : (Not consvd) NET/JRF (JUNE-) Q7. Th binding ngy of a light nuclus ( Z, ) in MV is givn by th appoximat fomula B (, Z ) wh givn is 4 ( N Z ) / / 6 Z N Z is th nuton numb. Th valu of Z of th most stabl isoba fo a / 6 / (b) 64 4 / B Solution: Z Z Z Z / 6 Had offic fiziks, H.No., G.F, Jia Saai, Na IIT, Hauz Khas, Nw Dlhi 6 Phon: / Banch offic nand Institut of Mathmatics, 8 B/6, Jia Saai, Na IIT Hauz Khas, Nw Dlhi 6 Wbsit: fiziks.physics@gmail.com

4 Institut fo NET/JRF, GTE, IIT JM, JEST, TIFR and GRE in PHYSICL SCIENCES Q8. spin-/ paticl undgos th dlay B C D wh it is known that B andc a also spin-/ paticls. Th complt st of allowd valus of th spin of th paticl D is 5,,,,,,... (b), 5 7 only,,,,... Solution: Spin of th lft sid and combind spin of th poducts must b sam to consv th spin angula momntum consvation law. Q9. Muons a poducd though th annihilation of paticl a and its antiplaticl, namly th pocss a a μ μ muon has a st mass of 5 MV/c and its pop lif tim is μ s. If th cnt of mass ngy of th collision is. GV in th laboatoy fam that coincids with th cnt-of-mass fam, thn th faction of muons that will dcay bfo thy ach a dtcto placd 6 km away fom th intaction point is (b) (b) Solution: N t λt N λt γτ N N 6 whτ s,. γ and t sc. 8 t N Thus. γτ N Had offic fiziks, H.No., G.F, Jia Saai, Na IIT, Hauz Khas, Nw Dlhi 6 Phon: / Banch offic nand Institut of Mathmatics, 8 B/6, Jia Saai, Na IIT Hauz Khas, Nw Dlhi 6 Wbsit: fiziks.physics@gmail.com 4

5 Institut fo NET/JRF, GTE, IIT JM, JEST, TIFR and GRE in PHYSICL SCIENCES JRF/NET-(DEC-) Q. Th intinsic lctic dipol momnt of a nuclus Z X incass with Z, but indpndnt of (b) dcass with Z, but indpndnt of is always zo incass with Z and Q. ccoding to th shll modl, th total angula momntum (in units of ) and th paity 7 of th gound stat of th Li nuclus is with ngativ paity (b) with positiv paity with positiv paity 7 with ngativ paity Solution: Z, N 4 Z /, l Fo odd ; ( s )( p ) / / j and paity ( ). NET/JRF (JUNE-4) Q. Th cntly-discovd Higgs boson at th LHC xpimnt has a dcay mod into a photon and a Z boson. If th st masss of th Higgs and Z boson a 5 GV/c and 9 GV/c spctivly, and th dcaying Higgs paticl is at st, th ngy of th photon will appoximatly b 5 GV (b) 5 GV GV 5 GV Solution: ssum H is symbol of Higgs boson, H E γ EH E E H Z ( 5) ( 9) 5 GV Z γ Had offic fiziks, H.No., G.F, Jia Saai, Na IIT, Hauz Khas, Nw Dlhi 6 Phon: / Banch offic nand Institut of Mathmatics, 8 B/6, Jia Saai, Na IIT Hauz Khas, Nw Dlhi 6 Wbsit: fiziks.physics@gmail.com 5

6 Institut fo NET/JRF, GTE, IIT JM, JEST, TIFR and GRE in PHYSICL SCIENCES Q. In a classical modl, a scala (spin-) mson consists of a quak and an antiquak bound by a potntial b V () a - wh a MV fm and b MV fm. If th masss of th quak and antiquak a ngligibl, th mass of th mson can b stimatd as appoximatly 4 MV/c (b) 8 MV/c 5 MV/c 45 MV/c (b) Solution: t quilibium spaation th potntial is minimum, thus th quilibium spaation can b dtmind as DV d () b a b a MVfm MVfm fm Th quilibium spaation btwn paticls is also stimatd by unctainty pincipl cδt c ( wh, ΔEΔt ) ΔE Wh, c is th vlocity of th vitual mson MV. fm c ΔE ΔE ( MV ) Using abov two lation ΔE 8MV th mass of th mson MV. fm ΔE ( MV ) Δ E Δ m c fm ΔE Δ m 8MV / c c Had offic fiziks, H.No., G.F, Jia Saai, Na IIT, Hauz Khas, Nw Dlhi 6 Phon: / Banch offic nand Institut of Mathmatics, 8 B/6, Jia Saai, Na IIT Hauz Khas, Nw Dlhi 6 Wbsit: fiziks.physics@gmail.com 6

7 Institut fo NET/JRF, GTE, IIT JM, JEST, TIFR and GRE in PHYSICL SCIENCES Q4. Consid th fou pocsss (i) p n v NET/JRF (DEC-4) (ii) Λ p v Solution: (i) (iii) π v (iv) π γ γ which of th abov is/a fobiddn fo f paticls? only (ii) (b) (ii) and (iv) (i) and (iv) (i) and (ii) p n ν [Not allowd] It violat ngy consvation. Th mass of poton is lss than mass of nuton. F poton is stabl and can not dcay to nuton. Poton can dcay to nuton only insid th nuclus, wh ngy violation is takn ca by Hisnbg unctainty pincipl. (ii) Λ [Not allowd]. In this dcay chag is not consvd p ν (iii) π ν [allowd though Wak intaction] (iv) π γ γ [allowd though Elctomagntic intaction] Q5. In dp inlastic scatting lctons a scattd off potons to dtmin if a poton has any intnal stuctu. Th ngy of th lcton fo this must b at last V (b).5 V.5 V.5 V (b) Solution: Th intnal stuctu of poton can only b dtmind if th wavlngth of th incoming lcton is naly qual to th siz of th poton i.. λ ( ) / 5 R. fm. fm. m ccoding to d-bogli lation, h λ p h me This can b also wittn as λ Α 5 E V ( ) Had offic fiziks, H.No., G.F, Jia Saai, Na IIT, Hauz Khas, Nw Dlhi 6 Phon: / Banch offic nand Institut of Mathmatics, 8 B/6, Jia Saai, Na IIT Hauz Khas, Nw Dlhi 6 Wbsit: fiziks.physics@gmail.com 7

8 Institut fo NET/JRF, GTE, IIT JM, JEST, TIFR and GRE in PHYSICL SCIENCES 5 5 E( V).4 5 (. λ Α ) E.4 Th bt suitabl answ is option (b). Q6. If th binding ngy B of a nuclus (mass numb and chag Z ) is givn by wh B a V a S a / sym ( Z ) a Z C / av 6 MV, as 6 MV, asym 4 MV and a C. 75MV, thn fo th most stabl isoba fo a nuclus with 6 is 68 (b) db Solution: Fo th most stabl isoba fo a nuclus ( Z ) ( ) / V Z az C / dz ( ) asym ( ) 6 Z 4 Z 6 Z ( Z 6) Z ( ) Z 6 9Z 4Z 6 6 Z 8. NET/JRF (JUNE-5) Q7. Th action D D 4 H π cannot pocd via stong intactions bcaus it ns. Solution: violats th consvation of angula momntum bayon numb D D H π (Not consvd) 4 I : This isopin is not consvd in abov action. (b) lctic chag isospin Had offic fiziks, H.No., G.F, Jia Saai, Na IIT, Hauz Khas, Nw Dlhi 6 Phon: / Banch offic nand Institut of Mathmatics, 8 B/6, Jia Saai, Na IIT Hauz Khas, Nw Dlhi 6 Wbsit: fiziks.physics@gmail.com 8

9 Institut fo NET/JRF, GTE, IIT JM, JEST, TIFR and GRE in PHYSICL SCIENCES Q8. Lt us appoximat th nucla potntial in th shll modl by a th dimnsional isotopic hamonic oscillato. Sinc th lowst two ngy lvls hav angula momnta ns. l and l spctivly, which of th following two nucli hav magic numbs of potons and nutons? 4 6 H and O (b) D and 8 B 4 H and 8 B H and C 6 Solution: and 4 H has Z, N Z N magic numbs (,8,,8,5,8,6 ) 6 8O has 8, 8 Q9. Th cham quak s assignd a cham quantum numb C. How should th Gllmann- ns. Nishijima fomula fo lctic chag b modifid fo fou flavos of quaks? I ( BS C) (b) I ( B S C) I ( B S C) I ( B S C) Solution: Fom Gll-Mann-Nishijima fomula Q I ( B S) Fo Quak it is gnalizd as Q I ( B S C) NET/JRF (DEC-5) Q. Consid th following pocsss involving f paticls (i) n p v (ii) p n π (iii) p n π π π (iv) p v n Which of th following statmnts is tu? Pocss (i) obys all consvation laws (b) Pocss (ii) consvs bayon numb, but violats ngy-momntum consvation pocss (iii) is not allowd by stong intaction but is allowd by wak intactions Pocss (iv) consvs bayon numb, but violats lpton numb consvation Had offic fiziks, H.No., G.F, Jia Saai, Na IIT, Hauz Khas, Nw Dlhi 6 Phon: / Banch offic nand Institut of Mathmatics, 8 B/6, Jia Saai, Na IIT Hauz Khas, Nw Dlhi 6 Wbsit: fiziks.physics@gmail.com 9

10 Institut fo NET/JRF, GTE, IIT JM, JEST, TIFR and GRE in PHYSICL SCIENCES ns.: (b) Solution: (i) n p v spin q (consvd) (not consvd) L (not consvd) (ii) Bayon numb is consvd but ngy and momntum consvation violatd. (iii) spin is not consvd (iv) obys all consvation laws. Q. Of th nucli of mass numb 5, th binding ngy calculatd fom th liquid dop modl (givn that th cofficints fo th Coulomb and th asymmty ngy a ac ns.: Solution:.7 MV and a.5 MV spctivly) is a maximum fo 5 54 Z sym X (b) 4 5 4a a 4a a / / a c c / / a c 8a a 8aa a c ( ) ( ) Z / Z I 5 T Sb 5 / Z Had offic fiziks, H.No., G.F, Jia Saai, Na IIT, Hauz Khas, Nw Dlhi 6 Phon: / Banch offic nand Institut of Mathmatics, 8 B/6, Jia Saai, Na IIT Hauz Khas, Nw Dlhi 6 Wbsit: fiziks.physics@gmail.com

Problem Solving Session 1: Electric Dipoles and Torque

Problem Solving Session 1: Electric Dipoles and Torque MASSACHUSETTS INSTITUTE OF TECHNOLOGY Dpatmnt of Physics 8.02 Poblm Solving Sssion 1: Elctic Dipols and Toqu Sction Tabl (if applicabl) Goup Mmbs Intoduction: In th fist poblm you will lan to apply Coulomb

More information

Chapter 3. Electric Potential

Chapter 3. Electric Potential Chapt 3 Elctic Potntial 3.1 Potntial and Potntial Engy...3-3. Elctic Potntial in a Unifom Fild...3-5 3.3 Elctic Potntial du to Point Chags...3-6 3.3.1 Potntial Engy in a Systm of Chags...3-8 3.4 Continuous

More information

Handout 3. Free Electron Gas in 2D and 1D

Handout 3. Free Electron Gas in 2D and 1D Handout 3 F lcton Gas in D and D In this lctu ou will lan: F lcton gas in two dinsions and in on dinsion Dnsit o Stats in -spac and in ng in low dinsions C 47 Sping 9 Fahan Rana Conll Univsit lcton Gass

More information

Gravity and the Earth Newtonian Gravity and Earth Rotation Effects

Gravity and the Earth Newtonian Gravity and Earth Rotation Effects Gavity and th Eath Nwtonian Gavity and Eath Rotation Effcts Jams R. Clynch, 003 I. Nwtonian Gavity A. Nwtonian Gavitational Foc B. Nwtonian Gavitational Fild C. Nwtonian Gavitational Potntial D. Gavity

More information

1240 ev nm 2.5 ev. (4) r 2 or mv 2 = ke2

1240 ev nm 2.5 ev. (4) r 2 or mv 2 = ke2 Chapte 5 Example The helium atom has 2 electonic enegy levels: E 3p = 23.1 ev and E 2s = 20.6 ev whee the gound state is E = 0. If an electon makes a tansition fom 3p to 2s, what is the wavelength of the

More information

Traffic Flow Analysis (2)

Traffic Flow Analysis (2) Traffic Flow Analysis () Statistical Proprtis. Flow rat distributions. Hadway distributions. Spd distributions by Dr. Gang-Ln Chang, Profssor Dirctor of Traffic safty and Oprations Lab. Univrsity of Maryland,

More information

Question 3: How do you find the relative extrema of a function?

Question 3: How do you find the relative extrema of a function? ustion 3: How do you find th rlativ trma of a function? Th stratgy for tracking th sign of th drivativ is usful for mor than dtrmining whr a function is incrasing or dcrasing. It is also usful for locating

More information

Physics. Lesson Plan #9 Energy, Work and Simple Machines David V. Fansler Beddingfield High School

Physics. Lesson Plan #9 Energy, Work and Simple Machines David V. Fansler Beddingfield High School Physics Lsson Plan #9 Engy, Wok an Simpl Machins Davi V. Fansl Bingfil High School Engy an Wok Objctivs: Dscib th lationship btwn wok an ngy; Display an ability to calculat wok on by a foc; Intify th foc

More information

Tank Level GPRS/GSM Wireless Monitoring System Solutions

Tank Level GPRS/GSM Wireless Monitoring System Solutions Tank Lvl GPRS/GSM Wilss Monitoing Systm Solutions HOLYKELL TECHNOLOGY CO.LTD May,2014 Ⅰ. Solution Rquimnts 1. Intoduction Th solution is mainly including: wilss data tansciv tminal, lvl snso and PC sv

More information

Chapter 22. Outside a uniformly charged sphere, the field looks like that of a point charge at the center of the sphere.

Chapter 22. Outside a uniformly charged sphere, the field looks like that of a point charge at the center of the sphere. Chapte.3 What is the magnitude of a point chage whose electic field 5 cm away has the magnitude of.n/c. E E 5.56 1 11 C.5 An atom of plutonium-39 has a nuclea adius of 6.64 fm and atomic numbe Z94. Assuming

More information

New Basis Functions. Section 8. Complex Fourier Series

New Basis Functions. Section 8. Complex Fourier Series Nw Basis Functions Sction 8 Complx Fourir Sris Th complx Fourir sris is prsntd first with priod 2, thn with gnral priod. Th connction with th ral-valud Fourir sris is xplaind and formula ar givn for convrting

More information

Newton s Law of Gravitation

Newton s Law of Gravitation Physics 106 Lctu 9 Nwton s Law of Gavitation SJ 7 th Ed.: Chap 1.1 to, 1.4 to 5 Histoical ovviw Nwton s invs-squa law of avitation i oc Gavitational acclation Supposition Gavitation na th Eath s sufac

More information

QUANTITATIVE METHODS CLASSES WEEK SEVEN

QUANTITATIVE METHODS CLASSES WEEK SEVEN QUANTITATIVE METHODS CLASSES WEEK SEVEN Th rgrssion modls studid in prvious classs assum that th rspons variabl is quantitativ. Oftn, howvr, w wish to study social procsss that lad to two diffrnt outcoms.

More information

(a) The centripetal acceleration of a point on the equator of the Earth is given by v2. The velocity of the earth can be found by taking the ratio of

(a) The centripetal acceleration of a point on the equator of the Earth is given by v2. The velocity of the earth can be found by taking the ratio of Homewok VI Ch. 7 - Poblems 15, 19, 22, 25, 35, 43, 51. Poblem 15 (a) The centipetal acceleation of a point on the equato of the Eath is given by v2. The velocity of the eath can be found by taking the

More information

fiziks Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES (c) 2

fiziks Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES (c) 2 Istitut f NT/JRF, GT, IIT-JM, JST, TIFR ad GR i PHYSICL SCINCS JST 5 Pat : Mak Qustis Q. cicula lp f adius R, cais a uifm li chag dsity. Th lctic fild, calculatd at a distac z dictly abv th ct f th lp,

More information

Concepts in Theoretical Physics

Concepts in Theoretical Physics Concepts in Theoretical Physics Lecture 6: Particle Physics David Tong e 2 The Structure of Things 4πc 1 137 e d ν u Four fundamental particles Repeated twice! va, 9608085, 9902033 Four fundamental forces

More information

Masses in Atomic Units

Masses in Atomic Units Nuclear Composition - the forces binding protons and neutrons in the nucleus are much stronger (binding energy of MeV) than the forces binding electrons to the atom (binding energy of ev) - the constituents

More information

FXA 2008. Candidates should be able to : Describe how a mass creates a gravitational field in the space around it.

FXA 2008. Candidates should be able to : Describe how a mass creates a gravitational field in the space around it. Candidates should be able to : Descibe how a mass ceates a gavitational field in the space aound it. Define gavitational field stength as foce pe unit mass. Define and use the peiod of an object descibing

More information

Instruction: Solving Exponential Equations without Logarithms. This lecture uses a four-step process to solve exponential equations:

Instruction: Solving Exponential Equations without Logarithms. This lecture uses a four-step process to solve exponential equations: 49 Instuction: Solving Eponntil Equtions without Logithms This lctu uss fou-stp pocss to solv ponntil qutions: Isolt th bs. Wit both sids of th qution s ponntil pssions with lik bss. St th ponnts qul to

More information

12.1. FÖRSTER RESONANCE ENERGY TRANSFER

12.1. FÖRSTER RESONANCE ENERGY TRANSFER ndei Tokmakoff, MIT epatment of Chemisty, 3/5/8 1-1 1.1. FÖRSTER RESONNCE ENERGY TRNSFER Föste esonance enegy tansfe (FR) efes to the nonadiative tansfe of an electonic excitation fom a dono molecule to

More information

Exam 3: Equation Summary

Exam 3: Equation Summary MASSACHUSETTS INSTITUTE OF TECHNOLOGY Depatment of Physics Physics 8.1 TEAL Fall Tem 4 Momentum: p = mv, F t = p, Fext ave t= t f t= Exam 3: Equation Summay total = Impulse: I F( t ) = p Toque: τ = S S,P

More information

Before attempting to connect or operate this product, please read these instructions carefully and save this manual for future use.

Before attempting to connect or operate this product, please read these instructions carefully and save this manual for future use. Modl No. RAID Boad Instuctions WJ-NDB301 Bfo attmpting to connct o opat this poduct, plas ad ths instuctions cafully and sav this manual fo futu us. Waning: All ok latd to th installation of this poduct

More information

DEGRADATION MODEL OF BREAST IMAGING BY DISPERSED RADIATION

DEGRADATION MODEL OF BREAST IMAGING BY DISPERSED RADIATION THE PUBLISHING HOUSE PROCEEDINGS OF THE ROMANIAN ACADEMY, Sis A, OF THE ROMANIAN ACADEMY Volum 1, Numb 4/011, pp. 347 35 DEGRADATION MODEL OF BREAST IMAGING BY DISPERSED RADIATION Migul BUSTAMANTE 1, Gastón

More information

Lecture 3: Diffusion: Fick s first law

Lecture 3: Diffusion: Fick s first law Lctur 3: Diffusion: Fick s first law Today s topics What is diffusion? What drivs diffusion to occur? Undrstand why diffusion can surprisingly occur against th concntration gradint? Larn how to dduc th

More information

Displacement, Velocity And Acceleration

Displacement, Velocity And Acceleration Displacement, Velocity And Acceleation Vectos and Scalas Position Vectos Displacement Speed and Velocity Acceleation Complete Motion Diagams Outline Scala vs. Vecto Scalas vs. vectos Scala : a eal numbe,

More information

Incorporating Statistical Process Control and Statistical Quality Control Techniques into a Quality Assurance Program

Incorporating Statistical Process Control and Statistical Quality Control Techniques into a Quality Assurance Program Incooating Statistical Pocss Contol and Statistical Quality Contol Tchniqus into a Quality Assuanc Pogam Robyn Sikis U.S. Cnsus Buau Puos Incooat SPC and SQC mthods into quality assuanc ogam Monito and

More information

12. Rolling, Torque, and Angular Momentum

12. Rolling, Torque, and Angular Momentum 12. olling, Toque, and Angula Momentum 1 olling Motion: A motion that is a combination of otational and tanslational motion, e.g. a wheel olling down the oad. Will only conside olling with out slipping.

More information

Section 7.4: Exponential Growth and Decay

Section 7.4: Exponential Growth and Decay 1 Sction 7.4: Exponntial Growth and Dcay Practic HW from Stwart Txtbook (not to hand in) p. 532 # 1-17 odd In th nxt two ction, w xamin how population growth can b modld uing diffrntial quation. W tart

More information

Lecture 33: Quantum Mechanical Spin

Lecture 33: Quantum Mechanical Spin Lctu 33: Quantu Mcancal pn Py85 Fall 9 Intnc pn Epcally w av foun tat ot patcl av an atonal ntnal g of fo call pn T tn-glac pnt 9): Eac typ of patcl a a ct nub of ntnal tat: tat --> pn _ 3 tat --> pn Etc.

More information

NUCLEAR MAGNETIC RESONANCE

NUCLEAR MAGNETIC RESONANCE 19 Jul 04 NMR.1 NUCLEAR MAGNETIC RESONANCE In this expeiment the phenomenon of nuclea magnetic esonance will be used as the basis fo a method to accuately measue magnetic field stength, and to study magnetic

More information

QCD --- Quantum Chromodynamics

QCD --- Quantum Chromodynamics Outlin QCD --- Quantum Chromodynamics QCD Principls Quantum fild thory, analogy with QED Vrtx, coupling constant Colour rd, grn or blu Gluons Quark and Gluon Intractions Confinmnt Asymptotic Frdom QCD

More information

A Model for Antenna-Plasma Wave Coupling towards Control of Uniformity in Slot-Excited Microwave Discharges

A Model for Antenna-Plasma Wave Coupling towards Control of Uniformity in Slot-Excited Microwave Discharges J. Plasa Fusion Rs. SERIES, Vol. 9 () A Modl fo Antnna-Plasa Wav Couling towads Contol of Unifoity in Slot-Excitd Micowav Dischags Daichi SAWADA, Akihio TSUJI, Takanoi KITSUDO, Yasuyoshi YASAKA, and Hioasa

More information

PY1052 Problem Set 8 Autumn 2004 Solutions

PY1052 Problem Set 8 Autumn 2004 Solutions PY052 Poblem Set 8 Autumn 2004 Solutions H h () A solid ball stats fom est at the uppe end of the tack shown and olls without slipping until it olls off the ight-hand end. If H 6.0 m and h 2.0 m, what

More information

HEAT TRANSFER ANALYSIS OF LNG TRANSFER LINE

HEAT TRANSFER ANALYSIS OF LNG TRANSFER LINE Scintific Jounal of Impact Facto(SJIF): 3.34 Intnational Jounal of Advanc Engining and sach Dvlopmnt Volum,Issu, Fbuay -05 HEAT TANSFE ANALYSIS OF LNG TANSFE LINE J.D. Jani -ISSN(O): 348-4470 p-issn(p):

More information

Ra atoms and ions: production and spectroscopy Testing the Standard Model in Heavy Nuclei H.W. Wilschut

Ra atoms and ions: production and spectroscopy Testing the Standard Model in Heavy Nuclei H.W. Wilschut atoms and ions: production and spctroscopy Tsting th Standard Modl in Havy Nucli H.W. Wilschut TRIµP group TRIµP =Trappd dioactiv Isotops, µ-laboratoris for fundamntal Physics KVI - Univrsity of Groningn

More information

MODERN ATOMIC THEORY AND THE PERIODIC TABLE

MODERN ATOMIC THEORY AND THE PERIODIC TABLE CHAPTER 10 MODERN ATOMIC THEORY AND THE PERIODIC TABLE SOLUTIONS TO REVIEW QUESTIONS 1. Wavelength is defined as the distance between consecutive peaks in a wave. It is generally symbolized by the Greek

More information

Load Balancing Algorithm Based on QoS Awareness Applied in Wireless Networks

Load Balancing Algorithm Based on QoS Awareness Applied in Wireless Networks , pp.191-195 http://x.oi.og/10.14257/astl.2015.111.37 Loa Balancing Algoithm Bas on QoS Awanss Appli in Wilss Ntwoks CHEN Xiangqian, MA Shaohui Dpatmnt of Comput Scinc an Tchnology, Hnan Mchanic an Elctical

More information

Financial Mathematics

Financial Mathematics Financial Mathatics A ractical Guid for Actuaris and othr Businss rofssionals B Chris Ruckan, FSA & Jo Francis, FSA, CFA ublishd b B rofssional Education Solutions to practic qustions Chaptr 7 Solution

More information

2 r2 θ = r2 t. (3.59) The equal area law is the statement that the term in parentheses,

2 r2 θ = r2 t. (3.59) The equal area law is the statement that the term in parentheses, 3.4. KEPLER S LAWS 145 3.4 Keple s laws You ae familia with the idea that one can solve some mechanics poblems using only consevation of enegy and (linea) momentum. Thus, some of what we see as objects

More information

Mathematics. Mathematics 3. hsn.uk.net. Higher HSN23000

Mathematics. Mathematics 3. hsn.uk.net. Higher HSN23000 hsn uknt Highr Mathmatics UNIT Mathmatics HSN000 This documnt was producd spcially for th HSNuknt wbsit, and w rquir that any copis or drivativ works attribut th work to Highr Still Nots For mor dtails

More information

Vibrational Spectroscopy

Vibrational Spectroscopy Vibrational Spctroscopy armonic scillator Potntial Enrgy Slction Ruls V( ) = k = R R whr R quilibrium bond lngth Th dipol momnt of a molcul can b pandd as a function of = R R. µ ( ) =µ ( ) + + + + 6 3

More information

CHAPTER 8 PRACTICE TEST QUESTIONS (END OF CHAPTER 7 TOO)

CHAPTER 8 PRACTICE TEST QUESTIONS (END OF CHAPTER 7 TOO) CHAPTER 8 PRACTICE TEST QUESTIONS (END OF CHAPTER 7 TOO) Information that most likely will be on the front cover of your exam: h i Z 2 ΔE = @ 2.18 x 10 @ 18 f Z 2 f J j @ k n f 2 n i 2 1. Which of the

More information

Free Electron Fermi Gas (Kittel Ch. 6)

Free Electron Fermi Gas (Kittel Ch. 6) Free Electron Fermi Gas (Kittel Ch. 6) Role of Electrons in Solids Electrons are responsible for binding of crystals -- they are the glue that hold the nuclei together Types of binding (see next slide)

More information

I N S T I T U T D E S T A T I S T I Q U E B I O S T A T I S T I Q U E E T S C I E N C E S A C T U A R I E L L E S (I S B A)

I N S T I T U T D E S T A T I S T I Q U E B I O S T A T I S T I Q U E E T S C I E N C E S A C T U A R I E L L E S (I S B A) I S T I T U T D E S T A T I S T I Q U E B I O S T A T I S T I Q U E E T S C I E C E S A C T U A R I E L L E S (I S B A UIVERSITÉ CATHOLIQUE DE LOUVAI D I S C U S S I O P A P E R 0/5 SOLVECY REQUIREMET

More information

2. Illustration of the Nikkei 225 option data

2. Illustration of the Nikkei 225 option data 1. Introduction 2. Illustration of the Nikkei 225 option data 2.1 A brief outline of the Nikkei 225 options market τ 2.2 Estimation of the theoretical price τ = + ε ε = = + ε + = + + + = + ε + ε + ε =

More information

Chem 115 POGIL Worksheet - Week 4 Moles & Stoichiometry Answers

Chem 115 POGIL Worksheet - Week 4 Moles & Stoichiometry Answers Key Questions & Exercises Chem 115 POGIL Worksheet - Week 4 Moles & Stoichiometry Answers 1. The atomic weight of carbon is 12.0107 u, so a mole of carbon has a mass of 12.0107 g. Why doesn t a mole of

More information

Widths of spectral lines

Widths of spectral lines Widths of spectral lines Real spectral lines are broadened because: Energy levels are not infinitely sharp. Atoms are moving relative to observer. 3 mechanisms determine profile φ(ν) Quantum mechanical

More information

High Voltage Cables. Figure 5.1 - Layout of three, single-core cables

High Voltage Cables. Figure 5.1 - Layout of three, single-core cables High oltag Cabls 5.0 High oltag Cabls High oltag Cabls a usd whn undgound tansmission is quid. Ths cabls a laid in ducts o may b buid in th gound. Unlik in ovhad lins, ai dos not fom pat of th insulation,

More information

The effect on the Asian option price times between the averaging. Mark Ioffe

The effect on the Asian option price times between the averaging. Mark Ioffe 866 U Naos Plaza u 566 Nw Yok NY 7 Pho: 3 355 Fa: 4 668 fo@gach.co www.gach.co h ffc o h sa opo pc s bw h avagg Mak Ioff bsac h acl s o h calculao of h pc of sa opo. I pacula w aalz h ffc o h opo pc s

More information

University of Maryland Fraternity & Sorority Life Spring 2015 Academic Report

University of Maryland Fraternity & Sorority Life Spring 2015 Academic Report University of Maryland Fraternity & Sorority Life Academic Report Academic and Population Statistics Population: # of Students: # of New Members: Avg. Size: Avg. GPA: % of the Undergraduate Population

More information

Lab M4: The Torsional Pendulum and Moment of Inertia

Lab M4: The Torsional Pendulum and Moment of Inertia M4.1 Lab M4: The Tosional Pendulum and Moment of netia ntoduction A tosional pendulum, o tosional oscillato, consists of a disk-like mass suspended fom a thin od o wie. When the mass is twisted about the

More information

by John Donald, Lecturer, School of Accounting, Economics and Finance, Deakin University, Australia

by John Donald, Lecturer, School of Accounting, Economics and Finance, Deakin University, Australia Studnt Nots Cost Volum Profit Analysis by John Donald, Lcturr, School of Accounting, Economics and Financ, Dakin Univrsity, Australia As mntiond in th last st of Studnt Nots, th ability to catgoris costs

More information

Chem 115 POGIL Worksheet - Week 4 Moles & Stoichiometry

Chem 115 POGIL Worksheet - Week 4 Moles & Stoichiometry Chem 115 POGIL Worksheet - Week 4 Moles & Stoichiometry Why? Chemists are concerned with mass relationships in chemical reactions, usually run on a macroscopic scale (grams, kilograms, etc.). To deal with

More information

Basic Nuclear Concepts

Basic Nuclear Concepts Section 7: In this section, we present a basic description of atomic nuclei, the stored energy contained within them, their occurrence and stability Basic Nuclear Concepts EARLY DISCOVERIES [see also Section

More information

Design for Cyclic Loading

Design for Cyclic Loading Dsign o Cyclic Loading 1. Compltly vsing cyclic stss and ndanc stngth A ply vsing o cyclic stss mans whn th stss altnats btwn qal positiv and ngativ pak stsss sinsoidally ding ach 300 cycl o opation, as

More information

Factors that Influence Memory

Factors that Influence Memory Ovlaning Factos that Influnc Mmoy Continu to study somthing aft you can call it pfctly. Psychology 390 Psychology of Laning Stvn E. Mi, Ph.D. Listn to th audio lctu whil viwing ths slids 1 2 Oganization

More information

From Quantum to Matter 2006

From Quantum to Matter 2006 From Quantum to Matter 006 Why such a course? Ronald Griessen Vrije Universiteit, Amsterdam AMOLF, May 4, 004 vrije Universiteit amsterdam Why study quantum mechanics? From Quantum to Matter: The main

More information

Group Theory and Chemistry

Group Theory and Chemistry Group Theory and Chemistry Outline: Raman and infra-red spectroscopy Symmetry operations Point Groups and Schoenflies symbols Function space and matrix representation Reducible and irreducible representation

More information

The force between electric charges. Comparing gravity and the interaction between charges. Coulomb s Law. Forces between two charges

The force between electric charges. Comparing gravity and the interaction between charges. Coulomb s Law. Forces between two charges The foce between electic chages Coulomb s Law Two chaged objects, of chage q and Q, sepaated by a distance, exet a foce on one anothe. The magnitude of this foce is given by: kqq Coulomb s Law: F whee

More information

Chapter 7. Electron Structure of the Atom. Chapter 7 Topics

Chapter 7. Electron Structure of the Atom. Chapter 7 Topics Chapter 7 Electron Structure of the Atom Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 1 Chapter 7 Topics 1. Electromagnetic radiation 2. The Bohr model of

More information

ME 612 Metal Forming and Theory of Plasticity. 6. Strain

ME 612 Metal Forming and Theory of Plasticity. 6. Strain Mtal Forming and Thory of Plasticity -mail: azsnalp@gyt.du.tr Makin Mühndisliği Bölümü Gbz Yüksk Tknoloji Enstitüsü 6.1. Uniaxial Strain Figur 6.1 Dfinition of th uniaxial strain (a) Tnsil and (b) Comprssiv.

More information

Chapter 21. Magnetic Forces and Magnetic Fields

Chapter 21. Magnetic Forces and Magnetic Fields Chapter 21 Magnetic Forces and Magnetic Fields 21.1 Magnetic Fields The needle of a compass is permanent magnet that has a north magnetic pole (N) at one end and a south magnetic pole (S) at the other.

More information

http://www.wwnorton.com/chemistry/tutorials/ch14.htm Repulsive Force

http://www.wwnorton.com/chemistry/tutorials/ch14.htm Repulsive Force ctivation nrgis http://www.wwnorton.com/chmistry/tutorials/ch14.htm (back to collision thory...) Potntial and Kintic nrgy during a collision + + ngativly chargd lctron cloud Rpulsiv Forc ngativly chargd

More information

CHEM 1411 Chapter 5 Homework Answers

CHEM 1411 Chapter 5 Homework Answers 1 CHEM 1411 Chapter 5 Homework Answers 1. Which statement regarding the gold foil experiment is false? (a) It was performed by Rutherford and his research group early in the 20 th century. (b) Most of

More information

THE NAVAJO NATION Department of Personnel Management JOB VACANCY ANNOUNCEMENT INFORMATION SYSTEMS TECHNICIAN

THE NAVAJO NATION Department of Personnel Management JOB VACANCY ANNOUNCEMENT INFORMATION SYSTEMS TECHNICIAN THE NAVAJO NATION Dpatmnt of Psonnl Managmnt JOB VACANCY ANNOUNCEMENT REQUISITION NO: EPA0158783 DATE POSTED: 06/30/14 POSITION NO: 241518 CLOSING DATE: 07/14/14 POSITION TITLE: INFORMATION SYSTEMS TECHNICIAN

More information

PHYSICS 111 HOMEWORK SOLUTION #13. May 1, 2013

PHYSICS 111 HOMEWORK SOLUTION #13. May 1, 2013 PHYSICS 111 HOMEWORK SOLUTION #13 May 1, 2013 0.1 In intoductoy physics laboatoies, a typical Cavendish balance fo measuing the gavitational constant G uses lead sphees with masses of 2.10 kg and 21.0

More information

YouthWorks Youth Works (yüth- w rkz), n.

YouthWorks Youth Works (yüth- w rkz), n. YouthWorks Youth Works(yüth- w rkz),n. 1. Baltimor City s summr jobs program. 2. Crats carr pathways for Baltimor City youth. 3. Givs Baltimor mployrs opportunitis to train thir futur workforc. Opportunity

More information

A Note on Approximating. the Normal Distribution Function

A Note on Approximating. the Normal Distribution Function Applid Mathmatical Scincs, Vol, 00, no 9, 45-49 A Not on Approimating th Normal Distribution Function K M Aludaat and M T Alodat Dpartmnt of Statistics Yarmouk Univrsity, Jordan Aludaatkm@hotmailcom and

More information

Flavour Physics. Tim Gershon University of Warwick. 31 March 2014

Flavour Physics. Tim Gershon University of Warwick. 31 March 2014 Flavour Physics Tim Gershon University of Warwick 31 March 2014 Outline Lecture 1 what is flavour physics? some history, some concepts, some theory charged lepton physics What is flavour physics? Parameters

More information

What is Energy conservation Rate in the Universe?

What is Energy conservation Rate in the Universe? Thermal Equilibrium Energy conservation equation Heating by photoionization Cooling by recombination Cooling by brehmsstralung Cooling by collisionally excited lines Collisional de-excitation Detailed

More information

Cloud and Big Data Summer School, Stockholm, Aug., 2015 Jeffrey D. Ullman

Cloud and Big Data Summer School, Stockholm, Aug., 2015 Jeffrey D. Ullman Cloud and Big Data Summr Scool, Stockolm, Aug., 2015 Jffry D. Ullman Givn a st of points, wit a notion of distanc btwn points, group t points into som numbr of clustrs, so tat mmbrs of a clustr ar clos

More information

Electronegativity and Polarity

Electronegativity and Polarity and Polarity N Goalby Chemrevise.org Definition: is the relative tendency of an atom in a molecule to attract electrons in a covalent bond to itself. is measured on the Pauling scale (ranges from 0 to

More information

Objectives 404 CHAPTER 9 RADIATION

Objectives 404 CHAPTER 9 RADIATION Objectives Explain the difference between isotopes of the same element. Describe the force that holds nucleons together. Explain the relationship between mass and energy according to Einstein s theory

More information

Vector Calculus: Are you ready? Vectors in 2D and 3D Space: Review

Vector Calculus: Are you ready? Vectors in 2D and 3D Space: Review Vecto Calculus: Ae you eady? Vectos in D and 3D Space: Review Pupose: Make cetain that you can define, and use in context, vecto tems, concepts and fomulas listed below: Section 7.-7. find the vecto defined

More information

Gauss Law. Physics 231 Lecture 2-1

Gauss Law. Physics 231 Lecture 2-1 Gauss Law Physics 31 Lectue -1 lectic Field Lines The numbe of field lines, also known as lines of foce, ae elated to stength of the electic field Moe appopiately it is the numbe of field lines cossing

More information

PERIODIC TABLE OF GROUPS OF ELEMENTS Elements can be classified using two different schemes.

PERIODIC TABLE OF GROUPS OF ELEMENTS Elements can be classified using two different schemes. 1 PERIODIC TABLE OF GROUPS OF ELEMENTS Elements can be classified using two different schemes. Metal Nonmetal Scheme (based on physical properties) Metals - most elements are metals - elements on left

More information

Events and Constraints: A Graphical Editor for Capturing Logic Requirements of Programs

Events and Constraints: A Graphical Editor for Capturing Logic Requirements of Programs Evnts and Constaints: A Gaphical Edito fo Captuing Logic Rquimnts of Pogams Magat H. Smith Bll Laboatois Rm. 2C-407 600 Mountain Avnu Muay Hill, NJ 07974 mhs@sach.bll-labs.com Gad J. Holzmann Bll Laboatois

More information

Atomic and Nuclear Physics Laboratory (Physics 4780)

Atomic and Nuclear Physics Laboratory (Physics 4780) Gamma Ray Spectroscopy Week of September 27, 2010 Atomic and Nuclear Physics Laboratory (Physics 4780) The University of Toledo Instructor: Randy Ellingson Gamma Ray Production: Co 60 60 60 27Co28Ni *

More information

Vacuum Technology. Kinetic Theory of Gas. Dr. Philip D. Rack

Vacuum Technology. Kinetic Theory of Gas. Dr. Philip D. Rack Kinetic Theory of Gas Assistant Professor Department of Materials Science and Engineering University of Tennessee 603 Dougherty Engineering Building Knoxville, TN 3793-00 Phone: (865) 974-5344 Fax (865)

More information

Agilent Basics of Measuring the Dielectric Properties of Materials. Application Note

Agilent Basics of Measuring the Dielectric Properties of Materials. Application Note Agilnt Basics of Masuing th Dilctic Poptis of Matials Application Not Contnts Intoduction...3 Dilctic thoy...4 Dilctic Constant...4 Pmability...7 Elctomagntic popagation...8 Dilctic mchanisms...10 Ointation

More information

The example is taken from Sect. 1.2 of Vol. 1 of the CPN book.

The example is taken from Sect. 1.2 of Vol. 1 of the CPN book. Rsourc Allocation Abstract This is a small toy xampl which is wll-suitd as a first introduction to Cnts. Th CN modl is dscribd in grat dtail, xplaining th basic concpts of C-nts. Hnc, it can b rad by popl

More information

Experiment 6: Centripetal Force

Experiment 6: Centripetal Force Name Section Date Intoduction Expeiment 6: Centipetal oce This expeiment is concened with the foce necessay to keep an object moving in a constant cicula path. Accoding to Newton s fist law of motion thee

More information

WAVES AND ELECTROMAGNETIC RADIATION

WAVES AND ELECTROMAGNETIC RADIATION WAVES AND ELECTROMAGNETIC RADIATION All waves are characterized by their wavelength, frequency and speed. Wavelength (lambda, ): the distance between any 2 successive crests or troughs. Frequency (nu,):

More information

PHYSICS 206a HOMEWORK #11 SOLUTIONS

PHYSICS 206a HOMEWORK #11 SOLUTIONS PHYSICS 0a HOEWORK # SOLUTIONS. Using Nwton s law of gavitation, div th acclation du to gavity xpincd by an objct of ass at th sufac of th Eath. Show that this acclation is indpndnt of th ass of th objct.

More information

HOMEWORK FOR UNIT 5-1: FORCE AND MOTION

HOMEWORK FOR UNIT 5-1: FORCE AND MOTION Nam Dat Partnrs HOMEWORK FOR UNIT 51: FORCE AND MOTION 1. You ar givn tn idntial springs. Dsrib how you would dvlop a sal of for (i., a mans of produing rpatabl fors of a varity of sizs) using ths springs.

More information

PHY4604 Introduction to Quantum Mechanics Fall 2004 Practice Test 3 November 22, 2004

PHY4604 Introduction to Quantum Mechanics Fall 2004 Practice Test 3 November 22, 2004 PHY464 Introduction to Quantum Mechanics Fall 4 Practice Test 3 November, 4 These problems are similar but not identical to the actual test. One or two parts will actually show up.. Short answer. (a) Recall

More information

Nuclear Physics. Nuclear Physics comprises the study of:

Nuclear Physics. Nuclear Physics comprises the study of: Nuclear Physics Nuclear Physics comprises the study of: The general properties of nuclei The particles contained in the nucleus The interaction between these particles Radioactivity and nuclear reactions

More information

α α λ α = = λ λ α ψ = = α α α λ λ ψ α = + β = > θ θ β > β β θ θ θ β θ β γ θ β = γ θ > β > γ θ β γ = θ β = θ β = θ β = β θ = β β θ = = = β β θ = + α α α α α = = λ λ λ λ λ λ λ = λ λ α α α α λ ψ + α =

More information

Section 5 Molecular Electronic Spectroscopy (lecture 9 ish)

Section 5 Molecular Electronic Spectroscopy (lecture 9 ish) Section 5 Molecular Electronic Spectroscopy (lecture 9 ish) Previously: Quantum theory of atoms / molecules Quantum Mechanics Vl Valence Molecular Electronic Spectroscopy Classification of electronic states

More information

Basic Concepts in Nuclear Physics

Basic Concepts in Nuclear Physics Basic Concepts in Nuclear Physics Paolo Finelli Corso di Teoria delle Forze Nucleari 2011 Literature/Bibliography Some useful texts are available at the Library: Wong, Nuclear Physics Krane, Introductory

More information

Description. Rc NPT G 1/8 1/4 3/8 1/2 3/4. With drain cock Drain guide 1/8 Drain guide 1/4 Drain cock with barb fitting: For ø6 x ø4 nylon tube

Description. Rc NPT G 1/8 1/4 3/8 1/2 3/4. With drain cock Drain guide 1/8 Drain guide 1/4 Drain cock with barb fitting: For ø6 x ø4 nylon tube M Mist Sparator to M Micro Mist Sparator to Sris M ominal filtration rating: 0.3 µm Sris ominal filtration rating: µm How to Ordr Mist Sparator Micro Mist Sparator, M, Option/Smi-standard: Slct on ach

More information

Bohr Model Calculations for Atoms and Ions

Bohr Model Calculations for Atoms and Ions Bohr Model Calculations for Atoms and Ions Frank Riou Department of Chemistry College of St. nedict St. Johnʹs University St. Joseph, MN 56374 Abstract A debroglie Bohr model is described that can be used

More information

AP* Atomic Structure & Periodicity Free Response Questions KEY page 1

AP* Atomic Structure & Periodicity Free Response Questions KEY page 1 AP* Atomic Structure & Periodicity ree Response Questions KEY page 1 1980 a) points 1s s p 6 3s 3p 6 4s 3d 10 4p 3 b) points for the two electrons in the 4s: 4, 0, 0, +1/ and 4, 0, 0, - 1/ for the three

More information

Implied volatility formula of European Power Option Pricing

Implied volatility formula of European Power Option Pricing Impli volatility fomula of Euopan Pow Option Picing Jingwi Liu * ing hn chool of Mathmatics an ystm cincs, Bihang Univsity, LMIB of th Ministy of Eucation,, Bijing, 009, P.R hina Abstact:W iv th impli

More information

[ ] These are the motor parameters that are needed: Motor voltage constant. J total (lb-in-sec^2)

[ ] These are the motor parameters that are needed: Motor voltage constant. J total (lb-in-sec^2) MEASURING MOOR PARAMEERS Fil: Motor paramtrs hs ar th motor paramtrs that ar ndd: Motor voltag constant (volts-sc/rad Motor torqu constant (lb-in/amp Motor rsistanc R a (ohms Motor inductanc L a (Hnris

More information

13- What is the maximum number of electrons that can occupy the subshell 3d? a) 1 b) 3 c) 5 d) 2

13- What is the maximum number of electrons that can occupy the subshell 3d? a) 1 b) 3 c) 5 d) 2 Assignment 06 A 1- What is the energy in joules of an electron undergoing a transition from n = 3 to n = 5 in a Bohr hydrogen atom? a) -3.48 x 10-17 J b) 2.18 x 10-19 J c) 1.55 x 10-19 J d) -2.56 x 10-19

More information

Solutions to Problems in Goldstein, Classical Mechanics, Second Edition. Chapter 7

Solutions to Problems in Goldstein, Classical Mechanics, Second Edition. Chapter 7 Solutions to Problems in Goldstein, Classical Mechanics, Second Edition Homer Reid April 21, 2002 Chapter 7 Problem 7.2 Obtain the Lorentz transformation in which the velocity is at an infinitesimal angle

More information

Nuclear Physics and Radioactivity

Nuclear Physics and Radioactivity Nuclear Physics and Radioactivity 1. The number of electrons in an atom of atomic number Z and mass number A is 1) A 2) Z 3) A+Z 4) A-Z 2. The repulsive force between the positively charged protons does

More information

Reach Versus Competition in Channels with Internet and Traditional Retailers

Reach Versus Competition in Channels with Internet and Traditional Retailers Rach Vsus Comptition in Channls with Intnt and Taditional Rtails Bai R Nault Haskayn School of Businss, Univsity of Calgay, Calgay, Albta, Canada, nault@ucalgayca Mohammad S Rahman Haskayn School of Businss,

More information

Lecture 3: Optical Properties of Bulk and Nano. 5 nm

Lecture 3: Optical Properties of Bulk and Nano. 5 nm Lecture 3: Optical Properties of Bulk and Nano 5 nm The Previous Lecture Origin frequency dependence of χ in real materials Lorentz model (harmonic oscillator model) 0 e - n( ) n' n '' n ' = 1 + Nucleus

More information