UGC POINT LEADING INSTITUE FOR CSIR-JRF/NET, GATE & JAM. are the polar coordinates of P, then. 2 sec sec tan. m 2a m m r. f r.

Size: px
Start display at page:

Download "UGC POINT LEADING INSTITUE FOR CSIR-JRF/NET, GATE & JAM. are the polar coordinates of P, then. 2 sec sec tan. m 2a m m r. f r."

Transcription

1 UGC POINT LEADING INSTITUE FOR CSIR-JRF/NET, GATE & JAM Solution (TEST SERIES ST PAPER) Dat: No 5. Lt a b th adius of cicl, dscibd by th aticl P in fig. if, a th ola coodinats of P, thn acos Diffntial quation of th obit is H, And hnc Now, d u u f d J u u u acos o sc u a du sc tan d a and du sc sc tan d a J u d u f u J u sc sc sc tan u d a Ju sc sc sc sc a J u sc J u 8J a..8 au. 5 a 8Ja Thus f. 5 o f 5 Thus th foc ais as th ins fifth ow of th distanc. In shical coodinats: h sin cos, y sin sin, z cos sin cos cos cos sin sin y sin sin cos sin sin cos z cos sin F K / V Fd V K / K / d L sin K / Thus, L T V y z V, y, z o L sin V,, Thfo, L o H L : Siilaly ( sin ) / H K and sin 7-G ND FLOOR, JIA SARAI, NEAR IIT, NEW DELHI- 6 Tl: -65, Mobs: , E-ail: info@ugcoint.in Wbsit:

2 H K / sin cosc H K /. Accoding to Liouilli s tho, th has olu occuid by a collction of syst ols, ains unchangd in agnitud und ti aluation. F K Ag a K Ag K Ag a Coa with a K Ag K Ag, f K A g K A g f / / 5. Potntial is gin by V Now ut a a a a ; dv..() d a a dv d Again diffntiat quation () d V a a V ''.() 5 d Now ut th alu of in quation V '' a a 5 a a a a a V " V " a a T T a 7-G ND FLOOR, JIA SARAI, NEAR IIT, NEW DELHI- 6 Tl: -65, Mobs: , E-ail: info@ugcoint.in Wbsit:

3 6. () 7. Fist w show that tansfoation is canonical q dq qd dq PdQ dq q / q d qd dq q dq qd q dq dq d d q This is fct diffntial so it is canonical tansfoation w ay wit th tansfoation quation as q Q tan q tan Q sc Q P sc Q; q tan Q o This fo suggsts itslf th fo of th gnating function F q F F q, P Q Intgating atially, w gt F q dq f Q Wh f is function of Q to b th dtind tan Qd f Q tan Qd f Q F Q Ealuat sc Q f ' Q f 'Q 8. () 9. (). (). (). (). (). () 5. () 6. () 7. () 8. () 9. (). (). (). (). Hints: Thus bd qd o bd qd., q sin d cos dq / q / / dq PdQ dq q cos q cos / q cos dq qsin d sin cos dq sin dq q cos d / / d q sin Which is act diffntial and hnc tansfoation is canonical 7-G ND FLOOR, JIA SARAI, NEAR IIT, NEW DELHI- 6 Tl: -65, Mobs: , E-ail: info@ugcoint.in Wbsit:

4 / Q / Q log q cos o q cos O 5. () / Q q cos Q o q / cos Fo this tansfoation, w tak F F Q F F q, Q F Q Thus cos O Q o F tan cosntant, Q F cos If th constant of intgation is zo Q F tanp 6. T T, T, T and T d T T G, o k cos dt i a z a z b z z V gz 7. L T V L a a b z z gz t iˆ i ˆj d tj ˆ dt V ˆ t j 8 t E 5iˆ 8ˆj ˆ ˆ ˆ L 5i 8 j 8 j 8ˆ i ˆj 8kˆ H q H q q q q q ; q q ; H q L ; L q H, so that 7-G ND FLOOR, JIA SARAI, NEAR IIT, NEW DELHI- 6 Tl: -65, Mobs: , E-ail: info@ugcoint.in Wbsit:

5 . qq q q q q qq q q qq q q q qq qq q qq q q qq q q qq q q dq q dt 8 I I I yy Izz 8 8 Ia Along th lin I 5. () h. W known that, E hc E So gbb hc Th g-facto cosonding to J = stat is, hc g B B hc B B. CG.6 c (). Th wa nubs cosonding to Raan lins a 75 c and 95 c c c If b th wa nub of th citing lin, and b th ibational Raan dislacnt thn 75 c and 95 c 75 c 95 c 9.5 c 7-G ND FLOOR, JIA SARAI, NEAR IIT, NEW DELHI- 6 Tl: -65, Mobs: , E-ail: info@ugcoint.in Wbsit:

6 This is sa as th ibational constant of th olcul HF, that is 9.5 c Hnc th ibational fquncy of th olcul is 9 c 9.5 c. c s osc. Hz 5. Lt b th locity of lcton (ass, chag ) oling in a Boh obit of hydogn ato Z of adius. Th condition of chanical stability of th lcton is 6. Th quantu condition is nh n =,, Ths tow quation gi nh and nh Th nub of aluation of th lcton in th obit scond is c f R c n h 8 h c n n Fo th n= stat th fquncy of aluation is Rc f Substituting th gin alu of R and th known alu of c, w gt f s 8. T Z s Fo Li and HZ, and sctily T Li 8 T H O H 8 T T 8.65 c 9.6 c Li 7. Th agntic ont of an ato is which LS couling holds has th agnitud J g J h g J J g J J B h Wh B is th Boh agnton and g is Land s g-facto gin by J J LL S S g JJ Fo th P stat, w ha L, S and J =, so that 7-G ND FLOOR, JIA SARAI, NEAR IIT, NEW DELHI- 6 Tl: -65, Mobs: , E-ail: info@ugcoint.in Wbsit:

7 g J B B 8. Th Dol half-intnsity badth in ts of walngth is gin by.66 c RT Wh R is unisal gas constant, T is Klin tatu and is atoic wight. Putting th gin alus w ha J / ol K 5K / s.99 Kg / ol a.a 9. Th wa nub of th adiation absobd in a otational tansition fo J to J+ is gin by B J Wh J fs to th low stat Fo a tansition fo J = to J =, w ha B But.68c gin O B.68 c B. c Again th wa nub of th adiation absobd in th tansition J =5 Gin by B J wh J fs to low stat B.68 c 5.c Th cosonding wa lngth is c. c. If I stands fo th hai isoto, thn O i i i In ts of walngth, w wit H And i 5 / / icon i.6 icon.8 icon. [ icon = c ].758 is 7-G ND FLOOR, JIA SARAI, NEAR IIT, NEW DELHI- 6 Tl: -65, Mobs: , E-ail: info@ugcoint.in Wbsit:

8 . Whn lctons acclatd though a otntial V stik a lagst, th aiu fquncy a (o iniu walngth in ) of th ittd X-ay hoton is gin by c V ha h Th iniu oltag fo.a X-ay hoton is hc V in in Js. s 9.6 C J / C. V. Th fin-stuctu lins of a band a sntd by ' " ' " B B B B Wh is th wa nub of th band-oigin (null-lin) and constants in th two stats inold in tansition. Coaing it with th gin quation, w gt 5798 c ' ".85 B B c ' ".68 B B c ' B and Th saation btwn th null-lin and th band-had is gin by had ' B B" B ' B ".85 c.68 c. Th oulation at of ll N is dn t Rdt N dt dn dt R/ N So ln R / N t constant Lt us assu that constant = K ln R / N t k Suos, t, N K ln R So quation () bcos as R/ N ln t R / R R t N N R t 5.5 c If all th atos ha a lif ti, thn " B a th otational 7-G ND FLOOR, JIA SARAI, NEAR IIT, NEW DELHI- 6 Tl: -65, Mobs: , E-ail: info@ugcoint.in Wbsit:

9 t/ Hnc N t R h P Thsold Thshold N Gin that P. ; s and. Pow thshold P thsold Choiu ions cubic cntit, h P thsold hc PThshold J 9 N Pow thshold PThshold. W.KW 5. () 6. () 7. () 8. Th aity of stat is dfind as wh, L is obital angula ontu of th stat fo ositi aity, th alu of obital angula ontu a L = and L =. Accoding to cto ato odl, th Total angula ontu is J L S... L S Fo L=, J= S= by J= L+S Fo L=, J = S= by J = L-S Hnc th o cobination fo L and S a L =, S = z and L =, S = 9. Sinc O C O ha no annt diol ont. Hnc it dos not show absotion lins but O C S has annt diol ont. Hnc it will show absotion lins. 5. () 7-G ND FLOOR, JIA SARAI, NEAR IIT, NEW DELHI- 6 Tl: -65, Mobs: , E-ail: info@ugcoint.in Wbsit:

II.3. DETERMINATION OF THE ELECTRON SPECIFIC CHARGE BY MEANS OF THE MAGNETRON METHOD

II.3. DETERMINATION OF THE ELECTRON SPECIFIC CHARGE BY MEANS OF THE MAGNETRON METHOD II.3. DETEMINTION OF THE ELETON SPEIFI HGE Y MENS OF THE MGNETON METHOD. Wok pupos Th wok pupos is to dtin th atio btwn th absolut alu of th lcton chag and its ass, /, using a dic calld agnton. In this

More information

Radiation Equilibrium, Inertia Moments, and the Nucleus Radius in the Electron-Proton Atom

Radiation Equilibrium, Inertia Moments, and the Nucleus Radius in the Electron-Proton Atom 14 AAPT SUER EETING innaolis N, July 3, 14 H. Vic Dannon Radiation Equilibiu, Intia onts, and th Nuclus Radius in th Elcton-Poton Ato H. Vic Dannon vic@gaug-institut.og Novb, 13 Rvisd July, 14 Abstact

More information

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics Atoic and olcular Physics JEST Q. Th binding nrgy of th hydrogn ato (lctron bound to proton) is.6 V. Th binding nrgy of positroniu (lctron bound to positron) is (a).6 / V (b).6 / 8 V (c).6 8 V (d).6 V.6

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

Mon. Tues. 6.2 Field of a Magnetized Object 6.3, 6.4 Auxiliary Field & Linear Media HW9

Mon. Tues. 6.2 Field of a Magnetized Object 6.3, 6.4 Auxiliary Field & Linear Media HW9 Fi. on. Tus. 6. Fild of a agntid Ojct 6.3, 6.4 uxiliay Fild & Lina dia HW9 Dipol t fo a loop Osvation location x y agntic Dipol ont Ia... ) ( 4 o I I... ) ( 4 I o... sin 4 I o Sa diction as cunt B 3 3

More information

The local orthonormal basis set (r,θ,φ) is related to the Cartesian system by:

The local orthonormal basis set (r,θ,φ) is related to the Cartesian system by: TIS in Sica Cooinats As not in t ast ct, an of t otntias tat w wi a wit a cnta otntias, aning tat t a jst fnctions of t istanc btwn a atic an so oint of oigin. In tis cas tn, (,, z as a t Coob otntia an

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

Mon. Tues. Wed. Lab Fri Electric and Rest Energy

Mon. Tues. Wed. Lab Fri Electric and Rest Energy Mon. Tus. Wd. Lab Fi. 6.4-.7 lctic and Rst ngy 7.-.4 Macoscoic ngy Quiz 6 L6 Wok and ngy 7.5-.9 ngy Tansf R 6. P6, HW6: P s 58, 59, 9, 99(a-c), 05(a-c) R 7.a bing lato, sathon, ad, lato R 7.b v. i xal

More information

6.Optical and electronic properties of Low

6.Optical and electronic properties of Low 6.Optical and lctonic poptis of Low dinsional atials (I). Concpt of Engy Band. Bonding foation in H Molculs Lina cobination of atoic obital (LCAO) Schoding quation:(- i VionV) E find a,a s.t. E is in a

More information

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals Hydogn atom Engy lvls and wav functions Obital momntum, lcton spin and nucla spin Fin and hypfin intaction Hydogn obitals Hydogn atom A finmnt of th Rydbg constant: R ~ 109 737.3156841 cm -1 A hydogn mas

More information

E F. and H v. or A r and F r are dual of each other.

E F. and H v. or A r and F r are dual of each other. A Duality Thom: Consid th following quations as an xampl = A = F μ ε H A E A = jωa j ωμε A + β A = μ J μ A x y, z = J, y, z 4π E F ( A = jω F j ( F j β H F ωμε F + β F = ε M jβ ε F x, y, z = M, y, z 4π

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

Formula overview. Halit Eroglu, 04/2014 With the base formula the following fundamental constants and significant physical parameters were derived.

Formula overview. Halit Eroglu, 04/2014 With the base formula the following fundamental constants and significant physical parameters were derived. Foula ovviw Halit Eolu, 0/0 With th bas foula th followin fundantal onstants and sinifiant physial paats w divd. aiabl usd: Spd of liht G Gavitational onstant h lank onstant α Fin stutu onstant h dud lank

More information

( ) 4. Jones Matrix Method 4.1 Jones Matrix Formulation A retardation plate with azimuth angle y. V û ë y û. év ù év ù év. ë y û.

( ) 4. Jones Matrix Method 4.1 Jones Matrix Formulation A retardation plate with azimuth angle y. V û ë y û. év ù év ù év. ë y û. 4. Jons Mati Mthod 4. Jons Mati Foulation A tadation plat with aziuth angl Yh; 4- Linal polaizd input light é = ë û Dcoposd into th slow and ast noal ods és é cos sin é = sin cos ë- û ë û R ( ), otation

More information

Regn. No. North Delhi : 33-35, Mall Road, G.T.B. Nagar (Opp. Metro Gate No. 3), Delhi-09, Ph: ,

Regn. No. North Delhi : 33-35, Mall Road, G.T.B. Nagar (Opp. Metro Gate No. 3), Delhi-09, Ph: , 1. Section-A contains 0 Multiple Choice Questions (MCQ). Each question has 4 choices (a), (b), (c) and (d), for its answer, out of which ONLY ONE is correct. From Q.1 to Q.10 carries 1 Marks and Q.11 to

More information

Molecules and electronic, vibrational and rotational structure

Molecules and electronic, vibrational and rotational structure Molculs and ctonic, ational and otational stuctu Max on ob 954 obt Oppnhim Ghad Hzbg ob 97 Lctu ots Stuctu of Matt: toms and Molculs; W. Ubachs Hamiltonian fo a molcul h h H i m M i V i fs to ctons, to

More information

CBSE-XII-2013 EXAMINATION (MATHEMATICS) The value of determinant of skew symmetric matrix of odd order is always equal to zero.

CBSE-XII-2013 EXAMINATION (MATHEMATICS) The value of determinant of skew symmetric matrix of odd order is always equal to zero. CBSE-XII- EXAMINATION (MATHEMATICS) Cod : 6/ Gnal Instuctions : (i) All qustions a compulso. (ii) Th qustion pap consists of 9 qustions dividd into th sctions A, B and C. Sction A compiss of qustions of

More information

ES 330 Electronics II Homework # 5 (Fall 2016 Due Wednesday, October 4, 2017)

ES 330 Electronics II Homework # 5 (Fall 2016 Due Wednesday, October 4, 2017) Pag1 Na olutions E 33 Elctonics II Howok # 5 (Fall 216 Du Wdnsday, Octob 4, 217) Pobl 1 (25 pots) A coon-itt aplifi uss a BJT with cunt ga = 1 whn biasd at I =.5 A. It has a collcto sistanc of = 1 k. (a)

More information

9 Kinetic Theory of Gases

9 Kinetic Theory of Gases Contnt 9 Kintic hory of Gass By Liw Sau oh 9. Ial gas quation 9. rssur of a gas 9. Molcular kintic nrgy 9.4 h r..s. sp of olculs 9.5 Dgrs of fro an law of quipartition of nrgy 9.6 Intrnal nrgy of an ial

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

PH672 WINTER Problem Set #1. Hint: The tight-binding band function for an fcc crystal is [ ] (a) The tight-binding Hamiltonian (8.

PH672 WINTER Problem Set #1. Hint: The tight-binding band function for an fcc crystal is [ ] (a) The tight-binding Hamiltonian (8. PH67 WINTER 5 Poblm St # Mad, hapt, poblm # 6 Hint: Th tight-binding band function fo an fcc cstal is ( U t cos( a / cos( a / cos( a / cos( a / cos( a / cos( a / ε [ ] (a Th tight-binding Hamiltonian (85

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

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

ESCI 341 Atmospheric Thermodynamics Lesson 16 Pseudoadiabatic Processes Dr. DeCaria

ESCI 341 Atmospheric Thermodynamics Lesson 16 Pseudoadiabatic Processes Dr. DeCaria ESCI 34 Atmohi hmoynami on 6 Puoaiabati Po D DCaia fn: Man, A an FE obitaill, 97: A omaion of th uialnt otntial tmatu an th tati ngy, J Atmo Si, 7, 37-39 Btt, AK, 974: Futh ommnt on A omaion of th uialnt

More information

Physics 240: Worksheet 15 Name

Physics 240: Worksheet 15 Name Physics 40: Woksht 15 Nam Each of ths poblms inol physics in an acclatd fam of fnc Althouh you mind wants to ty to foc you to wok ths poblms insid th acclatd fnc fam (i.. th so-calld "won way" by som popl),

More information

Problem Set 4 Solutions Distributed: February 26, 2016 Due: March 4, 2016

Problem Set 4 Solutions Distributed: February 26, 2016 Due: March 4, 2016 Probl St 4 Solutions Distributd: Fbruary 6, 06 Du: March 4, 06 McQuarri Probls 5-9 Ovrlay th two plots using Excl or Mathatica. S additional conts blow. Th final rsult of Exapl 5-3 dfins th forc constant

More information

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

Shape parameterization

Shape parameterization Shap paatization λ ( θ, φ) α ( θ ) λµ λµ, φ λ µ λ axially sytic quaupol axially sytic octupol λ α, α ± α ± λ α, α ±,, α, α ±, Inian Institut of Tchnology opa Hans-Jügn Wollshi - 7 Octupol collctivity coupling

More information

Orbital Angular Momentum Eigenfunctions

Orbital Angular Momentum Eigenfunctions Obital Angula Moentu Eigenfunctions Michael Fowle 1/11/08 Intoduction In the last lectue we established that the opeatos J Jz have a coon set of eigenkets j J j = j( j+ 1 ) j Jz j = j whee j ae integes

More information

1973 AP Calculus AB: Section I

1973 AP Calculus AB: Section I 97 AP Calculus AB: Sction I 9 Minuts No Calculator Not: In this amination, ln dnots th natural logarithm of (that is, logarithm to th bas ).. ( ) d= + C 6 + C + C + C + C. If f ( ) = + + + and ( ), g=

More information

Calculus Revision A2 Level

Calculus Revision A2 Level alculus Rvision A Lvl Tabl of drivativs a n sin cos tan d an sc n cos sin Fro AS * NB sc cos sc cos hain rul othrwis known as th function of a function or coposit rul. d d Eapl (i) (ii) Obtain th drivativ

More information

School of Electrical Engineering. Lecture 2: Wire Antennas

School of Electrical Engineering. Lecture 2: Wire Antennas School of lctical ngining Lctu : Wi Antnnas Wi antnna It is an antnna which mak us of mtallic wis to poduc a adiation. KT School of lctical ngining www..kth.s Dipol λ/ Th most common adiato: λ Dipol 3λ/

More information

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS It is not possibl to find flu through biggr loop dirctly So w will find cofficint of mutual inductanc btwn two loops and thn find th flu through biggr loop Also rmmbr M = M ( ) ( ) EDT- (JEE) SOLUTIONS

More information

KCET 2016 TEST PAPER WITH ANSWER KEY (HELD ON WEDNESDAY 4 th MAY, 2016)

KCET 2016 TEST PAPER WITH ANSWER KEY (HELD ON WEDNESDAY 4 th MAY, 2016) . Th maimum valu of Ë Ë c /. Th contraositiv of th convrs of th statmnt If a rim numbr thn odd If not a rim numbr thn not an odd If a rim numbr thn it not odd. If not an odd numbr thn not a rim numbr.

More information

1997 AP Calculus AB: Section I, Part A

1997 AP Calculus AB: Section I, Part A 997 AP Calculus AB: Sction I, Part A 50 Minuts No Calculator Not: Unlss othrwis spcifid, th domain of a function f is assumd to b th st of all ral numbrs for which f () is a ral numbr.. (4 6 ) d= 4 6 6

More information

Sample Test 2. GENERAL PHYSICS PH 221-3A (Dr. S. Mirov) Test 2 (10/10/07) ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.

Sample Test 2. GENERAL PHYSICS PH 221-3A (Dr. S. Mirov) Test 2 (10/10/07) ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS. GENERAL PHYSICS PH -3A (Dr. S. Mirov) Test (0/0/07) Sample Test STUDENT NAME: _Key STUDENT id #: -------------------------------------------------------------------------------------------------------------------------------------------

More information

QUESTION 1 [25 points]

QUESTION 1 [25 points] (Fist) QUESTION 1 [5 points] An object moves in 1 dimension It stats at est and unifomly acceleates at 5m/s fo s It then moves with constant velocity fo 4s It then unifomly acceleates at m/s until it comes

More information

Shor s Algorithm. Motivation. Why build a classical computer? Why build a quantum computer? Quantum Algorithms. Overview. Shor s factoring algorithm

Shor s Algorithm. Motivation. Why build a classical computer? Why build a quantum computer? Quantum Algorithms. Overview. Shor s factoring algorithm Motivation Sho s Algoith It appas that th univs in which w liv is govnd by quantu chanics Quantu infoation thoy givs us a nw avnu to study & tst quantu chanics Why do w want to build a quantu coput? Pt

More information

JEE(MAIN) 2018 TEST PAPER WITH SOLUTIONS (HELD ON SUNDAY 08 th APRIL, 2018) PART B MATHEMATICS ALLEN

JEE(MAIN) 2018 TEST PAPER WITH SOLUTIONS (HELD ON SUNDAY 08 th APRIL, 2018) PART B MATHEMATICS ALLEN . The integal sin cos 5 5 (sin cos sin sin cos cos ) is equal to () ( tan ) C () cot C () cot C () ( tan ) C (whee C is a constant of integation) Ans. () Let I sin cos d [(sin cos )(sin cos )] sin cos

More information

CHAPTER 5 CIRCULAR MOTION AND GRAVITATION

CHAPTER 5 CIRCULAR MOTION AND GRAVITATION 84 CHAPTER 5 CIRCULAR MOTION AND GRAVITATION CHAPTER 5 CIRCULAR MOTION AND GRAVITATION 85 In th pious chapt w discussd Nwton's laws of motion and its application in simpl dynamics poblms. In this chapt

More information

Solid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch

Solid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch Solid stat physics Lctu 3: chmical bonding Pof. D. U. Pitsch Elcton chag dnsity distibution fom -ay diffaction data F kp ik dk h k l i Fi H p H; H hkl V a h k l Elctonic chag dnsity of silicon Valnc chag

More information

ORBITAL TO GEOCENTRIC EQUATORIAL COORDINATE SYSTEM TRANSFORMATION. x y z. x y z GEOCENTRIC EQUTORIAL TO ROTATING COORDINATE SYSTEM TRANSFORMATION

ORBITAL TO GEOCENTRIC EQUATORIAL COORDINATE SYSTEM TRANSFORMATION. x y z. x y z GEOCENTRIC EQUTORIAL TO ROTATING COORDINATE SYSTEM TRANSFORMATION ORITL TO GEOCENTRIC EQUTORIL COORDINTE SYSTEM TRNSFORMTION z i i i = (coωcoω in Ωcoiinω) (in Ωcoω + coωcoiinω) iniinω ( coωinω in Ωcoi coω) ( in Ωinω + coωcoicoω) in icoω in Ωini coωini coi z o o o GEOCENTRIC

More information

GMm. 10a-0. Satellite Motion. GMm U (r) - U (r ) how high does it go? Escape velocity. Kepler s 2nd Law ::= Areas Angular Mom. Conservation!!!!

GMm. 10a-0. Satellite Motion. GMm U (r) - U (r ) how high does it go? Escape velocity. Kepler s 2nd Law ::= Areas Angular Mom. Conservation!!!! F Satllt Moton 10a-0 U () - U ( ) 0 f ow g dos t go? scap locty Kpl s nd Law ::= Aas Angula Mo. Consaton!!!! Nwton s Unsal Law of Gaty 10a-1 M F F 1) F acts along t ln connctng t cnts of objcts Cntal Foc

More information

TP A.31 The physics of squirt

TP A.31 The physics of squirt thnial proof TP A. Th physis of squirt supporting: Th Illustratd Prinipls of Pool and Billiards http://illiards.olostat.du y David G. Aliator, PhD, PE ("Dr. Dav") thnial proof originally postd: 8//7 last

More information

Physics 202, Lecture 5. Today s Topics. Announcements: Homework #3 on WebAssign by tonight Due (with Homework #2) on 9/24, 10 PM

Physics 202, Lecture 5. Today s Topics. Announcements: Homework #3 on WebAssign by tonight Due (with Homework #2) on 9/24, 10 PM Physics 0, Lctu 5 Today s Topics nnouncmnts: Homwok #3 on Wbssign by tonight Du (with Homwok #) on 9/4, 10 PM Rviw: (Ch. 5Pat I) Elctic Potntial Engy, Elctic Potntial Elctic Potntial (Ch. 5Pat II) Elctic

More information

Translation and Rotation Kinematics

Translation and Rotation Kinematics Tanslation and Rotation Kinematics Oveview: Rotation and Tanslation of Rigid Body Thown Rigid Rod Tanslational Motion: the gavitational extenal foce acts on cente-of-mass F ext = dp sy s dt dv total cm

More information

ANSWERS, HINTS & SOLUTIONS HALF COURSE TEST VIII PAPER-2

ANSWERS, HINTS & SOLUTIONS HALF COURSE TEST VIII PAPER-2 AIITS-HCT-VIII (Paper-)-PCM(Sol)-JEE(Advanced)/7 In JEE Advanced 06, FIITJEE Students bag 6 in Top 00 AIR, 7 in Top 00 AIR, 8 in Top 00 AIR. 4 Students from Long Term Classroom/ Integrated School Program

More information

Loss factor for a clamped edge circular plate subjected to an eccentric loading

Loss factor for a clamped edge circular plate subjected to an eccentric loading ndian ounal of Engining & Matials Scincs Vol., Apil 4, pp. 79-84 Loss facto fo a clapd dg cicula plat subjctd to an ccntic loading M K Gupta a & S P Niga b a Mchanical Engining Dpatnt, National nstitut

More information

Intro to QM due: February 8, 2019 Problem Set 12

Intro to QM due: February 8, 2019 Problem Set 12 Intro to QM du: Fbruary 8, 9 Prob St Prob : Us [ x i, p j ] i δ ij to vrify that th anguar ontu oprators L i jk ɛ ijk x j p k satisfy th coutation rations [ L i, L j ] i k ɛ ijk Lk, [ L i, x j ] i k ɛ

More information

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation Pof. D. I. Nass Phys57 (T-3) Sptmb 8, 03 Foui_Tansf_phys57_T3 Foui tansfoms (Chapt 5) Foui intgals a gnalizations of Foui sis. Th sis psntation a0 nπx nπx f ( x) = + [ an cos + bn sin ] n = of a function

More information

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers: APPM 6 Final 5 pts) Spring 4. 6 pts total) Th following parts ar not rlatd, justify your answrs: a) Considr th curv rprsntd by th paramtric quations, t and y t + for t. i) 6 pts) Writ down th corrsponding

More information

Note If the candidate believes that e x = 0 solves to x = 0 or gives an extra solution of x = 0, then withhold the final accuracy mark.

Note If the candidate believes that e x = 0 solves to x = 0 or gives an extra solution of x = 0, then withhold the final accuracy mark. . (a) Eithr y = or ( 0, ) (b) Whn =, y = ( 0 + ) = 0 = 0 ( + ) = 0 ( )( ) = 0 Eithr = (for possibly abov) or = A 3. Not If th candidat blivs that = 0 solvs to = 0 or givs an tra solution of = 0, thn withhold

More information

ADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS. Ghiocel Groza*, S. M. Ali Khan** 1. Introduction

ADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS. Ghiocel Groza*, S. M. Ali Khan** 1. Introduction ADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS Ghiocl Goza*, S. M. Ali Khan** Abstact Th additiv intgal functions with th cofficints in a comlt non-achimdan algbaically closd fild of chaactistic 0 a studid.

More information

Mechanics and Special Relativity (MAPH10030) Assignment 3

Mechanics and Special Relativity (MAPH10030) Assignment 3 (MAPH0030) Assignment 3 Issue Date: 03 Mach 00 Due Date: 4 Mach 00 In question 4 a numeical answe is equied with pecision to thee significant figues Maks will be deducted fo moe o less pecision You may

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

SEE LAST PAGE FOR SOME POTENTIALLY USEFUL FORMULAE AND CONSTANTS

SEE LAST PAGE FOR SOME POTENTIALLY USEFUL FORMULAE AND CONSTANTS Cicle instucto: Moow o Yethiaj Name: MEMORIL UNIVERSITY OF NEWFOUNDLND DEPRTMENT OF PHYSICS ND PHYSICL OCENOGRPHY Final Eam Phsics 5 Winte 3:-5: pil, INSTRUCTIONS:. Do all SIX (6) questions in section

More information

2 nd ORDER O.D.E.s SUBSTITUTIONS

2 nd ORDER O.D.E.s SUBSTITUTIONS nd ORDER O.D.E.s SUBSTITUTIONS Question 1 (***+) d y y 8y + 16y = d d d, y 0, Find the general solution of the above differential equation by using the transformation equation t = y. Give the answer in

More information

= x. ˆ, eˆ. , eˆ. 5. Curvilinear Coordinates. See figures 2.11 and Cylindrical. Spherical

= x. ˆ, eˆ. , eˆ. 5. Curvilinear Coordinates. See figures 2.11 and Cylindrical. Spherical Mathmatics Riw Polm Rholog 5. Cuilina Coodinats Clindical Sphical,,,,,, φ,, φ S figus 2. and 2.2 Ths coodinat sstms a otho-nomal, but th a not constant (th a with position). This causs som non-intuiti

More information

MATHEMATICS PAPER IB COORDINATE GEOMETRY(2D &3D) AND CALCULUS. Note: This question paper consists of three sections A,B and C.

MATHEMATICS PAPER IB COORDINATE GEOMETRY(2D &3D) AND CALCULUS. Note: This question paper consists of three sections A,B and C. MATHEMATICS PAPER IB COORDINATE GEOMETRY(D &D) AND CALCULUS. TIME : hrs Ma. Marks.75 Not: This qustion papr consists of thr sctions A,B and C. SECTION A VERY SHORT ANSWER TYPE QUESTIONS. 0X =0.If th portion

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

Radian Measure CHAPTER 5 MODELLING PERIODIC FUNCTIONS

Radian Measure CHAPTER 5 MODELLING PERIODIC FUNCTIONS 5.4 Radian Measue So fa, ou hae measued angles in degees, with 60 being one eolution aound a cicle. Thee is anothe wa to measue angles called adian measue. With adian measue, the ac length of a cicle is

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

CS 491 G Combinatorial Optimization

CS 491 G Combinatorial Optimization CS 49 G Cobinatorial Optiization Lctur Nots Junhui Jia. Maiu Flow Probls Now lt us iscuss or tails on aiu low probls. Thor. A asibl low is aiu i an only i thr is no -augnting path. Proo: Lt P = A asibl

More information

ENGI 4430 Non-Cartesian Coordinates Page xi Fy j Fzk from Cartesian coordinates z to another orthonormal coordinate system u, v, ˆ i ˆ ˆi

ENGI 4430 Non-Cartesian Coordinates Page xi Fy j Fzk from Cartesian coordinates z to another orthonormal coordinate system u, v, ˆ i ˆ ˆi ENGI 44 Non-Catesian Coodinates Page 7-7. Conesions between Coodinate Systems In geneal, the conesion of a ecto F F xi Fy j Fzk fom Catesian coodinates x, y, z to anothe othonomal coodinate system u,,

More information

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find BSE SMLE ER SOLUTONS LSS-X MTHS SET- BSE SETON Gv tht d W d to fd 7 7 Hc, 7 7 7 Lt, W ow tht Thus, osd th vcto quto of th pl z - + z = - + z = Thus th ts quto of th pl s - + z = Lt d th dstc tw th pot,,

More information

ALL INDIA TEST SERIES

ALL INDIA TEST SERIES Fom Classoom/Integated School Pogams 7 in Top 0, in Top 00, 54 in Top 00, 06 in Top 500 All India Ranks & 4 Students fom Classoom /Integated School Pogams & 7 Students fom All Pogams have been Awaded a

More information

INTEGRALS. Chapter 7. d dx. 7.1 Overview Let d dx F (x) = f (x). Then, we write f ( x)

INTEGRALS. Chapter 7. d dx. 7.1 Overview Let d dx F (x) = f (x). Then, we write f ( x) Chptr 7 INTEGRALS 7. Ovrviw 7.. Lt d d F () f (). Thn, w writ f ( ) d F () + C. Ths intgrls r clld indfinit intgrls or gnrl intgrls, C is clld constnt of intgrtion. All ths intgrls diffr y constnt. 7..

More information

MATH 1080 Test 2-SOLUTIONS Spring

MATH 1080 Test 2-SOLUTIONS Spring MATH Tst -SOLUTIONS Spring 5. Considr th curv dfind by x = ln( 3y + 7) on th intrval y. a. (5 points) St up but do not simplify or valuat an intgral rprsnting th lngth of th curv on th givn intrval. =

More information

Regn. No. South Delhi : 28-A/11, Jia Sarai, Near-IIT Hauz Khas, New Delhi-16, Ph : ,

Regn. No. South Delhi : 28-A/11, Jia Sarai, Near-IIT Hauz Khas, New Delhi-16, Ph : , 1. Section-A contains 3 Multiple Choice Questions (MCQ). Each question has 4 choices,, and, for its answer, out of which ONLY ONE is correct. Fro Q.1 to Q.1 carries 1 Marks and Q.11 to Q.3 carries Marks

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

Ch04: Motion in two and three dimensions (2D and 3D)

Ch04: Motion in two and three dimensions (2D and 3D) Ch4: Motion in two and thee dimensions (D and 3D) Displacement, elocity and acceleation ectos Pojectile motion Cicula motion Relatie motion 4.: Position and displacement Position of an object in D o 3D

More information

Central Force Motion

Central Force Motion Cental Foce Motion Cental Foce Poblem Find the motion of two bodies inteacting via a cental foce. Examples: Gavitational foce (Keple poblem): m1m F 1, ( ) =! G ˆ Linea estoing foce: F 1, ( ) =! k ˆ Two

More information

( )( )( ) ( ) + ( ) ( ) ( )

( )( )( ) ( ) + ( ) ( ) ( ) 3.7. Moel: The magnetic fiel is that of a moving chage paticle. Please efe to Figue Ex3.7. Solve: Using the iot-savat law, 7 19 7 ( ) + ( ) qvsinθ 1 T m/a 1.6 1 C. 1 m/s sin135 1. 1 m 1. 1 m 15 = = = 1.13

More information

STUDENT NAME: STUDENT id #: NOTE: Clearly write out solutions and answers (circle the answers) by section for each part (a., b., c., etc.

STUDENT NAME: STUDENT id #: NOTE: Clearly write out solutions and answers (circle the answers) by section for each part (a., b., c., etc. GENERAL PHYSICS PH 1-3A (Dr. S. Mirov) Test 1 (09/17/07) Key STUDENT NAME: STUDENT id #: -------------------------------------------------------------------------------------------------------------------------------------------

More information

NARAYANA I I T / P M T A C A D E M Y. C o m m o n P r a c t i c e T e s t 1 6 XII STD BATCHES [CF] Date: PHYSIS HEMISTRY MTHEMTIS

NARAYANA I I T / P M T A C A D E M Y. C o m m o n P r a c t i c e T e s t 1 6 XII STD BATCHES [CF] Date: PHYSIS HEMISTRY MTHEMTIS . (D). (A). (D). (D) 5. (B) 6. (A) 7. (A) 8. (A) 9. (B). (A). (D). (B). (B). (C) 5. (D) NARAYANA I I T / P M T A C A D E M Y C o m m o n P r a c t i c T s t 6 XII STD BATCHES [CF] Dat: 8.8.6 ANSWER PHYSIS

More information

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim. MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function

More information

Previous Years Questions ( ) Segment-wise

Previous Years Questions ( ) Segment-wise Institute for IAS/ IFoS/ CSIR/ GATE Eaminations Preious Years Questions (98 ) Segment-wise Orinary Differential Equations an Laplace Transforms (Accoring to the New Syllabus Pattern) Paper - I 98 Sole

More information

Lecture 23: Central Force Motion

Lecture 23: Central Force Motion Lectue 3: Cental Foce Motion Many of the foces we encounte in natue act between two paticles along the line connecting the Gavity, electicity, and the stong nuclea foce ae exaples These types of foces

More information

MATHEMATICS PAPER IIB COORDINATE GEOMETRY AND CALCULUS. Note: This question paper consists of three sections A, B and C.

MATHEMATICS PAPER IIB COORDINATE GEOMETRY AND CALCULUS. Note: This question paper consists of three sections A, B and C. MATHEMATICS PAPER IIB COORDINATE GEOMETRY AND CALCULUS. Tim: 3hrs Ma. Marks.75 Not: This qustion papr consists of thr sctions A, B and C. SECTION -A Vry Short Answr Typ Qustions. 0 X = 0. Find th condition

More information

MAGNETIC FIELD INTRODUCTION

MAGNETIC FIELD INTRODUCTION MAGNETIC FIELD INTRODUCTION It was found when a magnet suspended fom its cente, it tends to line itself up in a noth-south diection (the compass needle). The noth end is called the Noth Pole (N-pole),

More information

Chapter 7. A Quantum Mechanical Model for the Vibration and Rotation of Molecules

Chapter 7. A Quantum Mechanical Model for the Vibration and Rotation of Molecules Chaptr 7. A Quantu Mchanica Mo for th Vibration an Rotation of Mocus Haronic osciator: Hook s aw: F k is ispacnt Haronic potntia: V F k k is forc constant: V k curvatur of V at quiibriu Nwton s quation:

More information

A 1 A 2. a) Find the wavelength of the radio waves. Since c = f, then = c/f = (3x10 8 m/s) / (30x10 6 Hz) = 10m.

A 1 A 2. a) Find the wavelength of the radio waves. Since c = f, then = c/f = (3x10 8 m/s) / (30x10 6 Hz) = 10m. 1. Young s doubl-slit xprint undrlis th instrunt landing syst at ost airports and is usd to guid aircraft to saf landings whn th visibility is poor. Suppos that a pilot is trying to align hr plan with

More information

Simple Harmonic Motion

Simple Harmonic Motion Siple Haronic Motion Physics Enhanceent Prograe for Gifted Students The Hong Kong Acadey for Gifted Education and Departent of Physics, HKBU Departent of Physics Siple haronic otion In echanical physics,

More information

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( )

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( ) : PHYS 55 (Pat, Topic ) Eample Solutions p. Review of Foce Eample ( ) ( ) What is the dot poduct fo F =,,3 and G = 4,5,6? F G = F G + F G + F G = 4 +... = 3 z z Phs55 -: Foce Fields Review of Foce Eample

More information

Vectors for Physics. AP Physics C

Vectors for Physics. AP Physics C Vectors for Physics AP Physics C A Vector is a quantity that has a magnitude (size) AND a direction. can be in one-dimension, two-dimensions, or even three-dimensions can be represented using a magnitude

More information

HSC - BOARD MATHEMATICS (40) - SOLUTIONS

HSC - BOARD MATHEMATICS (40) - SOLUTIONS Date: 8..5 Q. (A) SECTION - I (i) (d) A () (ii) (c) A A I 6 6 6 A I 64 I I A A 6 (iii) (a) fg cos A cos HSC - BOARD - 5 MATHEMATICS (4) - SOLUTIONS cos cos ch () hy g fy c...(i) Comparing with A Hy By

More information

4.4 Linear Dielectrics F

4.4 Linear Dielectrics F 4.4 Lina Dilctics F stal F stal θ magntic dipol imag dipol supconducto 4.4.1 Suscptiility, mitivility, Dilctic Constant I is not too stong, th polaization is popotional to th ild. χ (sinc D, D is lctic

More information

1121 T Question 1

1121 T Question 1 1121 T1 2008 Question 1 ( aks) You ae cycling, on a long staight path, at a constant speed of 6.0.s 1. Anothe cyclist passes you, tavelling on the sae path in the sae diection as you, at a constant speed

More information

PHYS 1101 Practice problem set 5, Chapter 18: 4, 9, 15, 23, 27, 32, 40, 43, 55, 56, 59 1 = = = Nk T Nk T Nk T B 1 B 2 B 1

PHYS 1101 Practice problem set 5, Chapter 18: 4, 9, 15, 23, 27, 32, 40, 43, 55, 56, 59 1 = = = Nk T Nk T Nk T B 1 B 2 B 1 PHYS 0 Practice roble set, Chater 8: 4, 9,,, 7,, 40, 4,, 6, 9 8.4. Sole: (a he ean free ath of a olecule in a gas at teerature, olue V, and ressure is λ 00 n. We also know that λ λ V 4 π ( N V r Although,

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

ALL INDIA TEST SERIES

ALL INDIA TEST SERIES AITS-CRT-I PCM(S)-JEE(Main)/4 From assroom/integrated School Programs 7 in Top, in Top, 54 in Top, 6 in Top 5 All India Ranks & 4 Students from assroom /Integrated School Programs & 7 Students from All

More information

r cos, and y r sin with the origin of coordinate system located at

r cos, and y r sin with the origin of coordinate system located at Lectue 3-3 Kinematics of Rotation Duing ou peious lectues we hae consideed diffeent examples of motion in one and seeal dimensions. But in each case the moing object was consideed as a paticle-like object,

More information

Solutions to Supplementary Problems

Solutions to Supplementary Problems Solution to Supplmntay Poblm Chapt Solution. Fomula (.4): g d G + g : E ping th void atio: G d 2.7 9.8 0.56 (56%) 7 mg Fomula (.6): S Fomula (.40): g d E ping at contnt: S m G 0.56 0.5 0. (%) 2.7 + m E

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

Vaiatin f. A ydn balln lasd n t n ) Clibs u wit an acclatin f 6x.8s - ) Falls dwn wit an acclatin f.8x6s - ) Falls wit acclatin f.8 s - ) Falls wit an acclatin f.8 6 s-. T wit f an bjct in t cal in, sa

More information

Collisions between electrons and ions

Collisions between electrons and ions DRAFT 1 Collisions btwn lctrons and ions Flix I. Parra Rudolf Pirls Cntr for Thortical Physics, Unirsity of Oxford, Oxford OX1 NP, UK This rsion is of 8 May 217 1. Introduction Th Fokkr-Planck collision

More information

ESCI 342 Atmospheric Dynamics I Lesson 3 Fundamental Forces II

ESCI 342 Atmospheric Dynamics I Lesson 3 Fundamental Forces II Reading: Matin, Section. ROTATING REFERENCE FRAMES ESCI 34 Atmospheic Dnamics I Lesson 3 Fundamental Foces II A efeence fame in which an object with zeo net foce on it does not acceleate is known as an

More information

( ) ( )( ) ˆ. Homework #8. Chapter 28

( ) ( )( ) ˆ. Homework #8. Chapter 28 Hoewok #8. Chapte 8 1** A sall cuent eleent at the oigin has a length of. and caies a cuent of. A in the +z diection. Find the agnitude of the agnetic field due to this eleent and indicate its diection

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