Gauge Institute Journal, Vol. 11, No. 3, August 2015

Size: px
Start display at page:

Download "Gauge Institute Journal, Vol. 11, No. 3, August 2015"

Transcription

1 Gaug Institut Jounal, Vol., o. 3, August 05 Th uton as a Collasd-Hydogn Atom: Zo Point Engy & ucla Binding Engy, X Rays & Gamma Rays, ucla Focs & Bonding utonic Elctons Oitals, and uton Stas vic0@comcast.nt May 05 Astact: A nuton may disintgat into a oton, an lcton, and an antinutino. In Gavitational Collas, lctons and otons comin into nutons. W stalish that th uton is a Collasd-Hydogn Atom comosd of an lcton and a oton: Th Elcton has -4 st Oit Radius m, Sd 5,558,34 m/sc, 3.5 (Sd in Hydogn).

2 Gaug Institut Jounal, Vol., o. 3, August 05 Fquncy cycls/scond, 9 3,7 (Hydogn Elcton Fquncy), in th ang of Had X Rays: Quantum of Angula Momntum ( ), Zo Point Engy -767 V, 564 (Hydogn s Zo Point Engy) with hoton fquncy cycls/sc. Th Poton has st Oit Radius m, Sd 7,905,45 m/sc, (Hydogn Poton Sd). ) Fquncy cycls/sc, 0 3,3 (Hydogn Poton Fquncy), in th ang of Gamma Rays: Quantum of Angula Momntum ( ), ucla Binding Engy -36, 308 V, Elcton Oit Radius 4.5 Poton Oit Radius, ) Had X Rays, and Gamma ays: 553 (Hydogn s ucla Engy Binding) Had X Rays, a du to a uton s xcitd lcton tuning fom a high ngy Oit to a low ngy Oit

3 Gaug Institut Jounal, Vol., o. 3, August 05 Gamma Rays a du to a uton s xcitd oton tuning fom a high ngy Oit to a low ngy Oit 3) Kl s 3 d Law fo th uton: T T M - 4» 8 m -, v, c V c is consistnt with th modl of th uton as a Collasd Hydogn 4) uton Sin Angula Momntum: ( ) Th Assumtion of (0.5) is off y 57% 5) Elctic Collas Vsus Gavitational Collas: Th Elctic Foc twn th lcton and th oton is (Gavitational Foc). Thus, a uton sta is catd y Elctic Collas. 6) Total Binding Engy: Th uton s Total Binding Engy is 7) ucla Foc: 553 (Hydogn s Total Binding Engy). Th uton s ucla Foc is 305,000 (Hydogn s ucla Foc), and 836 (uton s Zo Point Engy Foc) 8) Mini Molcula Bonding: 3

4 Gaug Institut Jounal, Vol., o. 3, August 05 A uclus comosd of a Poton and a uton is a Mini On-Elcton Molcul H +, with an lcton that oits th two otons. 9) uclus Bonding: Th utons suly lctons which Oitals aout th uclus ond th otons, and nsu th uclus Staility. 0) uton Stas Bonding: In uton Stas, th Gavitational Focs a ngligil comad to th ucla Bonding, which ks th sta ackd togth. ) utonic Elctons Oitals: uton s lctons oit th nuclus, and k th otons ondd Kywods: Suatomic, Photon, uton Radius, lcton Radius, Comosit Paticls, Quak, lcton, Poton, Poton Radius, uton, Gaviton, Radiation Engy, Kintic Engy, Gavitational Engy, Rotation Engy, Elctic Engy, Oital Magntic Engy, Sin Magntic Engy, Cntital Foc, Lontz Foc, Elctic Chag, Mass-Engy, Wav-aticl, Intia Momnts, ucla Stuctu, uclus Staility, ucla Foc, ucla Bonding, Oitals, ucla Binding Engy, Zo 4

5 Gaug Institut Jounal, Vol., o. 3, August 05 Point Engy, Elctomagntic Sctum, X Ray, Gamma Ray, Boh Modl, Hydogn Atom, Radiation Pow Equiliium, uton Sta, PhysicsAstonomyClassificationSchm: 4.0-c, 4.0.Dh, 4.60Cd, 4.60.Ef, 4.60.Fg, q, 4.65.Bt, 4.70.Bh, y, 47.3.C, , B, 6.05.J-, 6.05.fm, Contnts Th uton in Radioactivity, in Astohysics, and in th uclus. X Rays Lin Sctum Povs th xistnc of an Oiting Elcton in th uton. Th Elcton and Poton Oits 3. Radiation Pow Equiliium, and th uton s Intia Momnts Th Elcton s Zo Point Engy 6. Th Poton s ucla Engy 7. Th uton s Mass-Engy 8. Th Poton s Oit Radius 5

6 Gaug Institut Jounal, Vol., o. 3, August Th Poton s Sd 0. Th Poton s Fquncy. Th Elcton s Sd. Th uton s Radius 3. Th Elcton s Fquncy 4. Th Elcton s Quantum of Angula Momntum 5. Th Poton s Quantum of Angula Momntum 6. uton s Zo Point Engy 7. uton s ucla Engy Binding 8. ucla Foc and Zo Point Engy Foc 9. Gamma Rays Oigin is uton s Poton 0. Kl s 3 d law fo th uton is consistnt with th uton s Modl as a Collasd-Hydogn Atom. uton Sin Angula Momntum. Elctic Collas Vsus Gavitational Collas 3. uton s Binding Engy 4. ucla Focs, ucla Bonding, uclus Staility, and uton Stas Rfncs 6

7 Gaug Institut Jounal, Vol., o. 3, August 05 Th uton in Radioactivity, in Astohysics, and in th uclus 0. Th uton in Radioactivity It is wll-stalishd that in th wak intaction, a nuton disintgats into a oton, an lcton, and an antinutino. This may suggst that a uton is comosd of ths th stal aticls. But if such suggstion was v mad, it has no tac in Atomic Physics Txtooks. 0. Th uton in Astohysics It is fimly livd that in th Gavitational Collas of a sta into a uton Sta, lctons and otons comin into nutons. Again, this may suggst that a uton is a Collasd-Hydogn Atom, comosd of an lcton, and a Poton. But such suggstion has no tac in Astohysics Txtooks. 0.3 Th uton as a Collasd-Hydogn Atom Thus, th dscition of uton as a Collasd-Hydogn Atom dwlls in th ackgound of majo Physics discilins, and may 7

8 Gaug Institut Jounal, Vol., o. 3, August 05 not considd a Hyothsis. It may dscid tt as a fact that has to sustantiatd, and xlod. Th fundamntal thoy of th uton is dismissd y assuming th uton to a vaiation of th Poton. Howv, X Rays Emission, and Comutations confim that th uton is a Collasd-Hydogn Atom. This Modl of th uton oints to th oigin of X Rays, vals th souc of th ucla Focs, and offs a lival xlanation to th Staility of th uclus. 0.4 ucla Focs ucla focs w suggstd to account fo th inding of th otons and th nutons in th nuclus. But no ogss was mad in th undstanding of ths focs. As Quaks w suggstd as su-nuclons, thi inding was attiutd to a su-nucla foc, and th inding of nuclons was attiutd to lftov su-nucla focs. This amounts to u sculation aout involvd xchang of gluons, quaks, and a Pion fo luck [Wikidia, ucla Focs]. At th nd, it mains uncla. What a th focs? Lftovs of th stong foc do not tll us much. 8

9 Gaug Institut Jounal, Vol., o. 3, August 05. How do thy oat? Exchang of this, and that dos not claify how th focs oat. 3. How th lctic ulsion twn otons is solvd? At th distanc twn th otons in th uclus, th lctic foc is fomidal too. 4. How do utons contiut to th staility of th nuclus? W cannot tll th diffnc if in th Wikidia animatd faiytal aout th xchang of Quaks, and Gluons, and Pion, th uton will lacd with a Poton. 0.5 ucla Stuctu It is livd that th mo otons in th nuclus, th mo nutons a ncssay to k it stal. But th is no xlanation to how that gat staility is achivd. In aticula, non of th modls fo th nuclus [Wikidia, ucla Stuctu] accounts fo th ulsion twn th otons, and fo th nign lctic nutality of th nutons. How dos th nutal uton hl to dcas th ulsion twn th otons? 0.6 ucla Radiation It is livd that X-Rays oiginat in th nuclus, ut th ocss 9

10 Gaug Institut Jounal, Vol., o. 3, August 05 y which thy a oducd is not cla, [Wikidia, X Ray]. In fact, X Rays Emission ovs th xistnc of an oiting lcton in th uton, and Gamma Ray Emission ovs th xistnc of an oiting oton in th uton. 0

11 Gaug Institut Jounal, Vol., o. 3, August 05. X-Rays Lin Sctum Povs th Existnc of an Oiting Elcton in th uton It has n osvd that X Rays a mittd whn a matial is omadd with a am of lctons o ions. Continuous lctomagntic sctum indicats that som lctons in th am dclat y lctons in th atomic shlls, and som may acclat towads th otons in th nuclus But aks of a lin sctum that show u in th X Ray Sctum a oducd just as th Otical sctum is gnatd: Elctons in th am ush an lcton to a high oit, and whn that xcitd lcton tuns to a low oit, it mits a hoton of X Ray Radiation. It is cla that lin sctum of X Rays Emission mandats an oiting lcton. What is disutd is that this lcton may in th nuclus itslf. Evn th lcton that coms out of a disintgating nuton, is

12 Gaug Institut Jounal, Vol., o. 3, August 05 not nough vidnc fo th livs that th cannot any lcton in th nuton. Thus, th lcton that mits an X Rays hoton has n sculatd to long to th inn shlls of th havy lmnts which omadmnt gnats X Rays, and Gamma Rays Howv, thos inn shlls lctons don t mov fast nough: Th lcton shlls suounding th nuclus a not ngtic nough to yild mo than otical fquncis, and at most, soft X Rays. Ou comutations ov that Gound Oit Elcton Dos not Radiat Gamma Rays. And vn Had X Rays must oiginat in th uclus. Gamma Rays mission quis oiting otons in th uclus.

13 Gaug Institut Jounal, Vol., o. 3, August 05. Th Elcton and Poton Oits Th lcton oits th oton to gnat th cntital foc that counts th lctic attaction twn th lcton and th oton. That attaction acclats th lcton towads th oton, and th lcton adiats ngy, that could caus it to sial onto th oton, and hav th atom collas In [Dan4] w xlaind that to comnsat fo th adiation ngy lost y th lcton, and vnt its sialing onto th oton, th oton must oiting th lcton, acclating towads it, and adiating it with ngy that ks th Atom in quiliium, and in xistnc. Th lcton s oit is lag than th oton s oit, and to find th lcton s oit, and sd, w assum that th oton is at st with sct to th lcton. Thus, th quations fo th lcton s oit and sd, in which th oton s motion will nglctd, a only aoximat. Closd Oits To stay within th nuton s oundais, 3

14 Gaug Institut Jounal, Vol., o. 3, August 05 th lcton, and th oton should hav closd oits.. Cntal Focs By [Routh,. 74], a closd oit sults fom a cntal foc that is ootional to th invs squa of th distanc,(such as th Coulom lctic foc) o dictly to th distanc(such as th cntital foc). Th lcton s chag, and th oton s chag suly th lctomagntic focs to clos thi oits..3 Oits Staility By [Routh,.80] Cntal Foc oits a stal. That is, thy a oundd in a ing twn two cicls. Th staility of th nuton indicats a stal lcton oit, and a stal oton oit..4 Plana Motion Sinc th lctic foc is invs squad law foc, Th lcton s oit, and th oton s oit will stay in th sam lan, and will not gnat a sh Th lan of motion of a aticl tuns aound to gnat a sh only und a non-invs squad law foc. 4

15 Gaug Institut Jounal, Vol., o. 3, August 05 [Chandaskha,. 95]..5 Sds, and Oits Radii Dnot th oton sd in its oit y V V c. / Th adius of th oton s oit is. Th lcton s sd in its oit v v / c Th adius of th lcton s oit, which is th nuton adius,.. 5

16 Gaug Institut Jounal, Vol., o. 3, August Radiation Pow Equiliium, and th uton s Intia Momnts Th lcton is attactd to th oton y th foc m - a 4 0. It is acclatd towads th oton y a - m 40, and adiats hotons into th oton fild. 3. Th Elcton s Radiation Pow is æ - ö ç 6 6 ç ø a ç 3 3 0c m 0c çè 40 Th Poton has an oit within th lcton s oit, with adius, fa small than th lcton s oit adius. Th oton is attactd to th lcton, with acclation 6

17 Gaug Institut Jounal, Vol., o. 3, August 05 A - M 4 0, and adiats hotons into th lcton s fild. 3. Th Poton s Radiation Pow is æ ö - A c 6 M 0c ç 0 è ø At quiliium, th Radiation Pow asod y th oton, quals th Radiation Pow asod y th lcton. æ æ ö - ö - 3» 3 6 m 0c M 0c èç ø ç 0 è ø H, w us» caus ach fomula assums that on aticl is moving whil th oth aticl is stationay. This Elctodynamics quality lads to a suisingly uly mchanical condition: th quality of th Rlativistic Intia Momnts of th lcton and th oton. That is, 3.3 Th uton s Intia Momnts Balanc 7

18 Gaug Institut Jounal, Vol., o. 3, August 05 Th uton is Elctodynamically stal if and only th Intia Momnts of its lcton and oton a qual m M» - - 8

19 Gaug Institut Jounal, Vol., o. 3, August Th uton s Foc Balanc Poof: m M Th Foc alanc quation fo th lcton is Dividing oth sids y c, 40 m v -. m - 40c m 0, 4, 0 7, 9

20 Gaug Institut Jounal, Vol., o. 3, August 05 m Th Foc alanc quation fo th oton is Dividing oth sids y c, - 40 M V M - 4 0c, 0 7, Thfo, m M M » Poof: Dividing th uton s Intia Momnts Balanc 3.3, m M» - -, 0

21 Gaug Institut Jounal, Vol., o. 3, August 05 y th uton s Foc alanc 4., w otain m M - -»,,». M may stimatd oughly y m, as in [Dan4]. 4.3 M m» 4.5 Poof: Fom th Intia Momnts Balanc, 3.3, m M» - - M -» 4 m Evn if 0.5, and 0., thn, -., 4 - -»

22 Gaug Institut Jounal, Vol., o. 3, August 05 In fact, w ll hav» 0.73,» , and 4 - -» 0.99». Thfo, M 0.99» m » 4.5.

23 Gaug Institut Jounal, Vol., o. 3, August Th Elcton's Zo Point Engy 5. Th Elcton s Elctic Binding Engy U lctic c 5. Th Elcton s Magntic Engy U magntic m 4 0 n (4 ) m 0v Poof: Th cunt du to th lcton s chag that tuns n cycls/scond is I n Th Magntic Engy of this cunt is [Bnson,.486] By [Fisch,.97] L LI. 0 m 0 m. Thus, th magntic ngy du to th lcton chag is 3

24 Gaug Institut Jounal, Vol., o. 3, August 05 m0( n ) m 4 0 n w 4 m 0v. (4 ) 5.3 Th Elcton s Magntic Engy in its uton s Oit Poof: is ngligil comad to its Elctic Engy U U magntic lctic m 0v (4 ) 4 v 4 c 4 0 In th following w ll aoximat» Thfo, »» Th Elcton s Rotation Engy m c v

25 Gaug Institut Jounal, Vol., o. 3, August 05 Poof: Fom th alanc twn th Cntital and Elctic focs on th lcton in its uton oit, - 40 m v m v - 4 Sustituting c m0, and 4 m 0, c. 0,. 5.5 Th Elcton s Total Binding Engy ( Zo Point Engy) U» 0 lcton inding 7 c 4 0 Poof: c lcton inding» U c c

26 Gaug Institut Jounal, Vol., o. 3, August Th Elcton s Total Engy Ulcton» mc + c 7 0 mc

27 Gaug Institut Jounal, Vol., o. 3, August Th Poton's ucla Engy 6. Th Poton s Elctic Binding Engy U lctic c 6. Th Poton s Magntic Engy U magntic m 4 0 n (4 ) 0 m V Poof: Th cunt du to th Poton s chag - that tuns n cycls/scond is I - n Th Magntic Engy of this cunt is [Bnson,.486] By [Fisch,.97] L LI. 0 m 0 m. 7

28 Gaug Institut Jounal, Vol., o. 3, August 05 Thus, th magntic ngy du to th Poton s chag is 4 m 0 ( n) m 0 n W 4 m 0V (4 ). 6.3 Th Poton s Magntic Engy in its uton Oit is ngligil comad to its Elctic Engy Poof: U U magntic lctic m 0V (4 ) 4 0 V 4 c 4 Aoximating» , U U magntic -5 lctic »» Th Poton s Rotation Engy 8

29 Gaug Institut Jounal, Vol., o. 3, August 05 M c - 0 V 7 Poof: Fom th alanc twn th Cntital and Elctic focs on th Poton in its uton oit, M V - 4 0, M - 4 V 0. Sustituting c m0, and 4 m 0, c Th Poton s Total Binding Engy is th ucla Engy U» 0 oton inding 7 c» 4 0 Poof: c oton» U c 9

30 Gaug Institut Jounal, Vol., o. 3, August 05 c Th Poton s Total Engy Uoton» Mc + c 7 0» Mc U U oton inding lcton inding» 4.5 Poof: U U oton inding 0 0 lcton inding 7 7 c c»

31 Gaug Institut Jounal, Vol., o. 3, August Th uton s Mass-Engy 7. Th uton s Mass-Engy Equation Poof: æ ö M -M - m» ç çè ø Dm M c Unu ton, Dividing y c, U + U oton lcton, Mc c mc 7 c 7 0 0» æ ö M -M - m» 7 0 ç + çè ø. 3

32 Gaug Institut Jounal, Vol., o. 3, August Th Poton s Oit Radius 8. Sustituting 7 æ ö» + 0 Dm çè ø C, -7 M» Kg, -7 M» Kg, -3 m» Kg, ( ) 0» D m By 4.3,» » ( ) »

33 Gaug Institut Jounal, Vol., o. 3, August Th Hydogn Poton Oit Radius is 553 (uton s Poton Oit Radius) Poof: By [Dan4,.], th Hydogn Poton Oit Radius is in H m M in H in »

34 Gaug Institut Jounal, Vol., o. 3, August Th Poton s Sd 9. æ 4 ö æ ö ç ç 7 7 ç0 M è ø çè0 M ø +ç -ç» 0 Poof: Fom th Foc Balanc, 4., M - 7 0» 7 0 M - æ 4 ö æ ö ç ç 7 7 ç0 M è ø çè0 M ø +ç -ç» 0. Sustituting C, -7 M» Kg, -5» m -38 ( ) 0» 0 M

35 Gaug Institut Jounal, Vol., o. 3, August 05 æ ö ç ç 7 çè0 M ø ç» » Using MAPLE > with(rootfinding): > > » Th uton s Poton s Sd Poof: V c» ( )c V 7, 905,45 m/sc. 35

36 Gaug Institut Jounal, Vol., o. 3, August 05» 7, 905,45 m/sc. 9.6 Th Hydogn Poton s Sd V 330, 40 m/sc. in H Poof: In Hydogn Atom, v H H 40 H m. mv HHv H 4 w HH 0, w in H w H a» 37 c, H 40 c c adians/sc By [Dan4,.], th Hydogn Poton Angula Vlocity is M W 4 -in-h» w-in-h. m

37 Gaug Institut Jounal, Vol., o. 3, August 05 V W -in-h -in-h -in-h 7» , 40 m/sc 9.7 Th uton s Poton Sd is Poof: 4 ( Hydogn Poton Sd) V V -in- -in-h 7, 905,45 330, 40» 4. 37

38 Gaug Institut Jounal, Vol., o. 3, August Th Poton Fquncy 0. Th uton s Poton Angula Vlocity V W adians/sc Poof: V W» 7, 905,45 m/sc m adians/sc. 0. Th Hydogn Elcton Angula Vlocity 6 w H adians/sc Poof: In th Hydogn Atom, v H H 40 H m. mv HHv H 4 w HH 0, 38

39 Gaug Institut Jounal, Vol., o. 3, August 05 w H a» 37 c, H 40 c c adians/sc 0.3 Th Hydogn Poton Angula Vlocity 7 W H adians/sc Poof: By [Dan4,.], th Hydogn Poton Angula Vlocity M W 4 H» wh. m Th uton s Poton Fquncy W Poof: W adians/sc 39

40 Gaug Institut Jounal, Vol., o. 3, August Th Hydogn Poton Fquncy W H cycls/sc Poof: W 7 H cycls/sc Th uton s Poton Fquncy is 3,3 ( Hydogn Poton Fquncy) Poof: W in WH W in H W ,3. 40

41 Gaug Institut Jounal, Vol., o. 3, August 05. Th Elcton s Sd. æ 8 ö æ ö m ç ç 0 m è ø è ø» 0 Poof: Fom th Foc alanc fo th lcton, 4., m - 7 0, Sustituting fom 4., Squaing oth sids, 7 0 m -,»,» - m 7 0, æ 8 ö æ ö m ç ç 0 m è ø è ø» 0. Sustituting -5» , , 4

42 Gaug Institut Jounal, Vol., o. 3, August ( ) m ( ) m æ ö ç. çè ø ( ) -( )» ( ) -( ) 0 Dnoting º x, w sk th zos of th olynomial f ( x) x + ( ) x -( ) twn x 0, and x. Using wton s Itations x j+ xj - f ( x ) j f '( x ) j x xj - j+ xj x j ( ) ( ) x W osv that If x j > 0.05, thn x j + < x j. That is, th itations dcas. j 4

43 Gaug Institut Jounal, Vol., o. 3, August 05 Stating with x 0.05, and otaind with a calculato x» 0.04 x 3» x 4» x 5» Mal Root-Finding Pogam quis zo. W took x 0.0 Mal Inut and Outut follow: > with(rootfinding): > x to to th ight of th >

44 Gaug Institut Jounal, Vol., o. 3, August 05.5 Th uton s Elcton Sd v 5,558,34 m/sc. Poof: c c 5,558,34 m/sc..6 Th Hydogn Elcton Sd v B a c,89, 78 m/sc.» 37 Poof: In th Hydogn Atom, v H H 40 H m. mv HHv H 4 0, v H 4 c, c 0 a» 37,89,78 m/sc..7 Th uton s Elcton Sd is 3.5 ( Hydogn Elcton Sd) Poof: 5,558,34 3.5,89, 78». 44

45 Gaug Institut Jounal, Vol., o. 3, August 05. Th uton s Radius. -» Poof: Sustituting , , Th Hydogn Radius is ~563 (uton Radius) Poof: Poof: M M -» 4» m - m, caus 4 - -»

46 Gaug Institut Jounal, Vol., o. 3, August Th Elcton s Fquncy 3. Th Elcton s Angula Vlocity v 0 w adians/sc Poof: w» v 5,558,34 m/sc m adians/sc. 3. Th Elcton s Fquncy w Poof: n w adians/sc

47 Gaug Institut Jounal, Vol., o. 3, August Th Hydogn Elcto n Angula Vlocity vh 6 w adians/sc H H Poof: w H v H H»,89,78 m/sc m adians/sc. 3.4 Th Hydogn Elcton Fquncy w H cycls/sc Poof: wh cycls/sc. 3.5 Th uton s Elcton Fquncy is 3,7 (Hydogn Elcton Fquncy) 47

48 Gaug Institut Jounal, Vol., o. 3, August 05 Poof: w w H w w H ,

49 Gaug Institut Jounal, Vol., o. 3, August Th Elcton s Quantum of Angula Momntum Th Elcton s Quantum of Angula Momntum is th Angula Momntum of th lcton s st oit 4. Th Elcton s Quantum of Angula Momntum m - v By dict comuting (with many aoximat valus), w otain 4. ( ) Poof: - -( ) m - v -3-4 ( )( )0 (5,558,34)( )0-34 ( )0 ( ). 49

50 Gaug Institut Jounal, Vol., o. 3, August 05 Altnativly, w hav m v a,» wh a 4 c» 37 0 is th Fin Stuctu Constant Poof: - 40 m v. m c - Angula Momntum, 4 c 0 4 c a 0 37 a. In th ocdings w usd th valu 4.4 ( ) 50

51 Gaug Institut Jounal, Vol., o. 3, August Th Poton s Quantum of Angula Momntum Th Poton s Quantum of Angula Momntum is th Angula Momntum of th Poton s st oit 5. Th Poton s Quantum of Angula Momntum M - V ( ) 5. M a V, -» ( ) wh a 4 c» 37 0 is th Fin Stuctu Constant Poof: - 40 M V. 5

52 Gaug Institut Jounal, Vol., o. 3, August 05 M c - Angula Momntum, 4 c 0 4 c a 0 37 a. 5

53 Gaug Institut Jounal, Vol., o. 3, August uton s Zo Point Engy Th lctical inding ngy will xist at tmatu zo, wh all thmal motions cas, and is calld Zo Point Engy. If th oton s motion is nglctd, th Zo Point Engy is th lcton s total inding ngy. 6. Poof: Elcton Binding æ a w ö h 40 ç è ø -U c w 40 40c w a / a w æ a w ö h ç è ø. 6. Th uton s st lcton oit has hoton s ngy æ a w ö - h ç è ø. 53

54 Gaug Institut Jounal, Vol., o. 3, August Th uton Gound stat Engy is Zo Point Engy æ a w ö h ç è ø. 6.4 uton s Zo Point Engy Poof: a - w V V 8-0 a w 37 é(6.580)0 V ù( )0 ( ) êë úû V -38 c ( ) 0 V Joul ( )0 ( )0 Joul V 6.5 Th Zo Point Engy Fquncy 767V cycls/scond h 54

55 Gaug Institut Jounal, Vol., o. 3, August 05 a w cycls/scond 8 Poof: 767V 767V h V cycls/scond a w ( ) cycls/scond uton s Zo Point Engy is 564 (Hydogn s Zo Point Engy) Poof:

56 Gaug Institut Jounal, Vol., o. 3, August uton s ucla Engy Binding Most of inding is du to th oiting oton s, and th Poton s inding Engy is th actual Zo Point Engy. 7. uton s ucla Engy Binding c a W Poof: a W W c W a c 7. uton s ucla Engy Binding is 4.5(uton s Zo Point Engy Binding) Poof: c 0 c

57 Gaug Institut Jounal, Vol., o. 3, August uton s ucla Engy Binding is (uton s Total Engy Binding) Poof: a W -36,68 V Poof: - -36, 308 V 8 0 a 37 é(6.580)0 V ù( )0 ( ) ë û -6 W ê ú 36, V -38 c ( ) 0 V Joul ( )0 ( )0 Joul 36, V 7.5 Hydogn s ucla Binding Engy 57

58 Gaug Institut Jounal, Vol., o. 3, August 05 æ a ö æacö 4 W ç çè ø H 0 H è in H ø H Poof: c æ a ö W H H 40 H 40c HH W. W çè in H ø a / in H æac ö ç è ø. H 7.6 Poof: 4 7 v æm H ö W H ( )0 adians/sc ç» çèm ø H M H w æ ö W H ç çèm ø v H H 4 c 37 ( ) - ( )0 4 ( ) æac ö V ç è ø H V 8 0 H 58

59 Gaug Institut Jounal, Vol., o. 3, August 05 c é(6.580)0 V ù ê ë ú û(.73735)0 ac H V c ( ) 0 V Joul H 0 (.73735)0 ( )0 Joul V. 7.8 uton s ucla Engy Binding is 553 (Hydogn s ucla Engy Binding) Poof: 36, 308 V V. 59

60 Gaug Institut Jounal, Vol., o. 3, August ucla Foc and Zo Point Engy Foc 8. uton s ucla Foc Hydogn s ucla Foc 4 0 H 8.3 uton s ucla Foc is 305,467(Hydogn s ucla Foc) Poof: H 0 H æ ö ç. çè ø By [Dan4, 4.4], H»

61 Gaug Institut Jounal, Vol., o. 3, August 05 æ ö ç -5 è ø 305, uton s ucla Foc is 836(uton s Zo Point Engy Foc) Poof: M m 0»

62 Gaug Institut Jounal, Vol., o. 3, August Gamma Rays Oigin is uton s Poton Soft X Rays a hotons at fquncis Had X Rays stat at 8 0 cycls/sc. 9 0 cycls/sc Th uton s Elcton Fquncy is in th ang of Had X Rays. Gamma Rays stat at Th uton s Poton Fquncy W wn cycls/sc, 0 0 cycls/sc n 0 is in th ang of Gamma Rays cycls/scond, Thus, th xistnc of Gamma Rays Radiation ovs that th uton is a condnsd Hydogn Atom, comosd of an lcton, and a oton. 6

63 Gaug Institut Jounal, Vol., o. 3, August 05 That is, 9. a uton s Poton xcitd fom its oit into a high oit, tuns to a low uton s Oit, and mits a Gamma Ray Photon 63

64 Gaug Institut Jounal, Vol., o. 3, August Kl s 3 d Law fo th uton, is Consistnt with th uton s Modl as a Collasd-Hydogn Atom wton s Gavitational foc on a lant oiting th sun at adius, with iod T is w Thfo, O, m M Plant Sun m w G. Plant Plant w GM. 3 Plant T Sun 4, GM 3 Constant which is Kl s 3 d Law fo Gavitation. Sinc th Sun too, oits th systm s cnt of Gavitation with a small adius Sun, m w GM m M W 3. 3 Plant Plant Plant Sun Plant Sun Sun Sun 64

65 Gaug Institut Jounal, Vol., o. 3, August 05 O, 3 æt ö m Plant æ ö Plant Plant ç è T ø M èç ø. Sun Sun Sun Fo th Elcton and Poton that comos th uton, 0. m M 3 3 w 4 W Poof: caus m - M - w 4 0 W 4 0,. 0. Kl s 3 d Law fo th uton is 3 - m æt ö æ ö T M ç çè ø - è ø Poof: Sustitut in 0. w ; W. T T 65

66 Gaug Institut Jounal, Vol., o. 3, August W M - w T 4» 8 T m - Poof: By 0., m æt ö ç - ç çèt ø M -. Sustituting fom 3.3, m M» - -, æt ö ç ç» çèt ø» M m Th Poton s Angula Vlocity Poof: M W» - 4 w m - Coma with Th discancy of is du to ou ounding os, and th calculato 66

67 Gaug Institut Jounal, Vol., o. 3, August 05 M - 4 w 8 m - W» 0 w adians/sc M 4 ( ) m»» »» W» ot that W in 0. was otaind fom ou uton s Mass- Engy Equation, 7.. That Mass-Engy quation yildd, with which w otaind, V c, and W. V / Thn,, and w usd to otain,, u c, and w u /. Thus, W in 6.4 dnds on th Mass-Engy Equation. vthlss, th clos sults of 0., and 0.4, stalish 0.5 Kl s 3 d Law fo th uton is consistnt with th uton s Mass-Engy Equation, and with th Modl of th uton as a Collasd-Hydogn Atom 67

68 Gaug Institut Jounal, Vol., o. 3, August 05. uton Sin Angula Momntum. uton Sin is th Sum of th Elcton and th Poton Angula Momntums m M æ ö +» 37 ç çè ø c c Poof: Th Foc on th uton s lcton is - 40 m c ( ) Th Angula Momntum of th Elcton gnats th Sin. m - c 4 c 0, m c 0 4 c c 0 7 Sustituting m c ha, wh a» 0 37 a. 68

69 Gaug Institut Jounal, Vol., o. 3, August 05 Similaly, th Angula Momntum of th Poton in its uton Oit, gnats th Sin M - Th uton Sin is th Sum c a m M æ ö + a ç çè ø c c a a / 37 / 37 +» +» Consquntly,. Th Assumtion that th uton s Sin is (0.5) is off y 57% 69

70 Gaug Institut Jounal, Vol., o. 3, August 05. Elctic Collas Vsus Gavitational Collas. Th Gavitational Foc twn th lcton and th Poton in th Hydogn Atom, o in th uton is ngligil with sct to th Elctical Foc twn thm Poof: Fo th uton, mm G c G mm Similaly, fo th Hydogn, ( ) 0 mm G H c G H mm

71 Gaug Institut Jounal, Vol., o. 3, August 05 Consquntly,. uton Stas a Catd y Elctic Collas. Gavitational Focs a ngligil in th Collas. 7

72 Gaug Institut Jounal, Vol., o. 3, August uton s Binding Engy 3. Th uton s Total Binding Engy c 0 7 æ ö ç +» ( - - çè M M m) c ø ( )MV Poof: By 7., th Binding Engy is c 0 7 æ ö ç +» ( - - çè ø ) M M m c Dm J Sinc Joul 0 V, 60, MV (m c )MV Th Hydogn Atom Total Binding Engy c 0 æ ö ç 7 ç çè H ø ç V 7

73 Gaug Institut Jounal, Vol., o. 3, August 05 Poof: Sustituting fom [Dan4,.], H c æ ö ( ) 0 ( ) ç H - è ø J ( )0 V V. 3.3 Th uton s Total Binding Engy is aout 553 (Hydogn Total Binding Engy) Poof: V V». 73

74 Gaug Institut Jounal, Vol., o. 3, August ucla Focs, ucla Bonding, uclus Staility, and uton Stas Ov th shot distanc twn th uton s lcton and Poton, th lctic foc is nomous comad to th Hydogn lctic Foc: 4. Th Poton-Elcton Elctic Foc in th uton is 37,000 (Poton-Elcton Foc in th Hydogn) Poof: Sustitut H Hydogn Radius m -4» uton Radius m 0 H è 0 H æ ö ç ø æ ö ç -4 è ø 74

75 Gaug Institut Jounal, Vol., o. 3, August 05» 37, 000. This lctic foc is th souc of th ucla Foc that inds th otons in th uclus. Fo instanc, 4. A uclus mad of a Poton and a uton is a Mini On-Elcton Molcul H +, with two otons and on lcton that oits th two otons just as it dos in th H + molcul. Fo such Molcula Bonding s [Gil,.70]. This sot of Molcula Bonding in th uclus nsus th staility of th uclus amly, 4.3 ucla Bonding is a Mini Molcula Bonding Though Oitals of Elctons Sulid y th utons in th uclus. Hnc, 75

76 Gaug Institut Jounal, Vol., o. 3, August In uton Stas, th Gavitational Focs a ngligil comad to th uton s ucla Bonding, which ks th sta ackd togth 76

77 Gaug Institut Jounal, Vol., o. 3, August 05 Rfncs [Aaatzis] Thodo Aaatzis Rsnting Elctons, A Biogahical Aoach to Thotical Entitis U. of Chicago Pss, 006. [Bis] Athu Bis Concts of Modn Physics Fifth Edition, McGaw Hill, 995. [Bnson], Bnson Walt, Hais John, Stock Host, Lutz Holg, Handook of Physics, Sing, 00. [Chandaskha] S. Chandaskha, wton s Pinciia fo th Common Rad Clandon Pss, Oxfod, 995. [Bohm] David Bohm, Th Scial Thoy of Rlativity Routldg, 996. [Bon] Max Bon, Atomic Physics Blacki, 7 th Edition, 96. [Budn], Richad Budn, and Douglas Fais, umical Analysis, Fouth Edition, PWS-KET, 989. [CRC] CRC Handook of Chmisty and Physics CRC, 995. [Dan], Dannon H. Vic, Wav-Paticl Duality: d Bogli Wavs and Unctainty Gaug Institut Jounal Of Math and Physics, Vol., o. 4, ovm 006. [Dan], Dannon H. Vic, Photon s Sin, Diffaction, and Radius. Th On Photon Hyothsis, and Stod Photon Gaug Institut Jounal Of Math and Physics, Vol. 9, o., Fuay 03. [Dan3], Dannon H. Vic, Zo Point Engy and th Chag-Radiation Equation in Boh s Atom Gaug Institut Jounal Of Math and Physics, Vol. 8, o. 4, ovm 0. [Dan4], Dannon H. Vic, Radiation Equiliium, Intia Momnts, and th uclus Radius in th Elcton-Poton Atom Gaug Institut Jounal Of Math and Physics, Vol. 0, o. 3, August

78 Gaug Institut Jounal, Vol., o. 3, August 05 [d Bogli], Louis d Bogli, Hisng s Unctaintis and th Poailistic Inttation of Wav Mchanics Kluw Acadmic, 990. [Fynman] Richad Fynman, Th Fynman Lctus of Physics, Edison Wsly, 965. [Fisch] Fisch-Cis, A., C., Th Physics Comanion, IoP, 003. [Gil] Victo Gil, Oitals in Chmisty: A Modn Guid fo Studnts Camidg, 000. [Gigoiv], Igo S. Gigoiv, and Evgnii Z. Milikhov, Handook of Physical Constants, CRC, 997. [Kovtz] Attay Kovtz, Elctomagntic Thoy, Oxfod, 000. [Mac Ggo] Malcolm Mac Ggo Th Enigmatic Elcton Kluw, 99 [Maion] Jy Maion; Mak Hald, Classical Elctomagntic Radiation, Scond Edition, Acadmic Pss, 980. [Mackintosh], Ray Mackintosh, Jim Al-Khalili, Bjon Jonson, Tsa Pna, uclus: A ti into th Hat of Matt Scond Edition, Johns Hokins, 0. [Millikan], Millikan, Rot, Andws, Elctons (+ and -), Potons, Photons, utons, Msotons, and Cosmic Rays U. of Chicago, Rvisd Edition, 947. [ol] B. ol, umical Mthods: Itation Pogamming and Algaic Equations Oliv & Boyd, 964. [Panofsky] Wolfgang Panofsky; Mla Phillis, Classical Elcticity and Magntism, Scond Edition, Addison Wsly, 96. [Pak] Syil P. Pak, McGaw-Hill Encyclodia of Physics, Scond Edition, McGaw-Hill, 993. [PDG] Paticl Data Gou, at LBL, and CER () July 00 PARTICE PHYSICS BOOKLET, IOP Pulishing() Physical 78

79 Gaug Institut Jounal, Vol., o. 3, August 05 Rviw D, Paticls, Filds, Gavitation, and Cosmology, July 0, Pat I, Rviw of Paticl Physics, Volum 86, um, Amican Physical Socity. [Polyanin] Andi Polyanin; Alxi Chnoutsan, A Concis Handook of Mathmatics, Physics, and Engining Scincs, CRC, 0. [Pool] Chals P. Pool, Th Physics Handook Fundamntals and Ky Equations, Wily, 998. [Richadson], O.W. Richadson, Th Elcton Thoy of Matt Scond Edition, Camidg Univsity Pss, 96. [Rindl], Wolfgang Rindl, Rlativity Scial, Gnal, and Cosmological, Oxfod, 00. [Routh] Edwad, John Routh A Tatis on Dynamics of a Paticl, Stcht, 898. [Simulik], Volodimi Simulik, dito, What is th Elcton Aion, 005. [Skinn], Ray Skinn, Rlativity fo Scintists and Engins, Dov, 98. [Smith] Glnn S. Smith, An Intoduction to Classical Elctomagntic Radiation Camidg, 997. [Sigl] Sigl, Muay, Thotical Mchanics McGaw Hill, 967. [Stannad], Russll Stannad, Rlativity, Stling, 008. [Thomson] J. J. Thomson, Byond th Elcton Camidg U. Pss, 98. [Thomson] G. P. Thomson, Conduction of Elcticity Though Gass Volum I, Camidg U. Pss, 98. [Wagon] Rot Wagon, Poduction of Factional Chag in a Zo: w Fontis of Physics ditd y J.D. Faiank, B.S. Dav, C.W.F. Evitt, and P. F. Michlson, Fman, 988 [Woan] Woan, Gaham, Th Camidg Handook of Physics Fomulas, 79

80 Gaug Institut Jounal, Vol., o. 3, August 05 Camidg 000. htt://n.wikidia.og/wiki/lontz_tansfomation htt://n.wikidia.og/wiki/rlativity_thoy htt://n.wikidia.og/wiki/uton htt://n.wikidia.og/wiki/ucla_foc htt://n.wikidia.og/wiki/ucla_stuctu htt://n.wikidia.og/wiki/x_ay htt://n.wikidia.og/wiki/poton htt://n.wikidia.og/wiki/elcton htt://n.wikidia.og/wiki/hydogn_atom htt://n.wikidia.og/wiki/boh_modl htt://n.wikidia.og/wiki/uclon htt://n.wikidia.og/wiki/elctomagntic_sctum htt://uload.wikimdia.og/wikidia/commons/8/8a/elctomagn tic-sctum.ng 80

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

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

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

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

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

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

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

Electromagnetic Schrödinger Equation of the Deuteron 2 H (Heavy Hydrogen)

Electromagnetic Schrödinger Equation of the Deuteron 2 H (Heavy Hydrogen) Wold Jounal of Nucla Scinc and Tchnology, 14, 4, 8-6 Publishd Onlin Octob 14 in SciRs. htt://www.sci.og/jounal/wjnst htt://dx.doi.og/1.46/wjnst.14.449 Elctomagntic Schöding Equation of th Duton H (Havy

More information

8 - GRAVITATION Page 1

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

More information

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

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

Chapter 1 The Dawn of Quantum Theory

Chapter 1 The Dawn of Quantum Theory Chapt 1 Th Dawn of Quantum Thoy * By th Lat 18 s - Chmists had -- gnatd a mthod fo dtmining atomic masss -- gnatd th piodic tabl basd on mpiical obsvations -- solvd th stuctu of bnzn -- lucidatd th fundamntals

More information

PHYS 272H Spring 2011 FINAL FORM B. Duration: 2 hours

PHYS 272H Spring 2011 FINAL FORM B. Duration: 2 hours PHYS 7H Sing 11 FINAL Duation: hous All a multil-choic oblms with total oints. Each oblm has on and only on coct answ. All xam ags a doubl-sidd. Th Answ-sht is th last ag. Ta it off to tun in aft you finish.

More information

PHYS 272H Spring 2011 FINAL FORM A. Duration: 2 hours

PHYS 272H Spring 2011 FINAL FORM A. Duration: 2 hours PHYS 7H Sing 11 FINAL Duation: hous All a multil-choic oblms with total oints. Each oblm has on and only on coct answ. All xam ags a doubl-sidd. Th Answ-sht is th last ag. Ta it off to tun in aft you finish.

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

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

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

More information

Collective Focusing of a Neutralized Intense Ion Beam Propagating Along a Weak Solenodial Magnetic Field

Collective Focusing of a Neutralized Intense Ion Beam Propagating Along a Weak Solenodial Magnetic Field Havy Ion Fusion Scinc Vitual National Laoatoy Collctiv Focusing of a Nutalizd Intns Ion Bam Popagating Along a Wak Solnodial Magntic Fild M. Dof (LLNL) In collaoation with I. Kaganovich, E. Statsv, and

More information

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

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

More information

Collisionless Hall-MHD Modeling Near a Magnetic Null. D. J. Strozzi J. J. Ramos MIT Plasma Science and Fusion Center

Collisionless Hall-MHD Modeling Near a Magnetic Null. D. J. Strozzi J. J. Ramos MIT Plasma Science and Fusion Center Collisionlss Hall-MHD Modling Na a Magntic Null D. J. Stoi J. J. Ramos MIT Plasma Scinc and Fusion Cnt Collisionlss Magntic Rconnction Magntic connction fs to changs in th stuctu of magntic filds, bought

More information

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

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

More information

Lecture 3.2: Cosets. Matthew Macauley. Department of Mathematical Sciences Clemson University

Lecture 3.2: Cosets. Matthew Macauley. Department of Mathematical Sciences Clemson University Lctu 3.2: Costs Matthw Macauly Dpatmnt o Mathmatical Scincs Clmson Univsity http://www.math.clmson.du/~macaul/ Math 4120, Modn Algba M. Macauly (Clmson) Lctu 3.2: Costs Math 4120, Modn Algba 1 / 11 Ovviw

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

GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL

GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL Ioannis Iaklis Haanas * and Michal Hany# * Dpatmnt of Physics and Astonomy, Yok Univsity 34 A Pti Scinc Building Noth Yok, Ontaio, M3J-P3,

More information

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.

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. 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

More information

NEWTON S THEORY OF GRAVITY

NEWTON S THEORY OF GRAVITY NEWTON S THEOY OF GAVITY 3 Concptual Qustions 3.. Nwton s thid law tlls us that th focs a qual. Thy a also claly qual whn Nwton s law of gavity is xamind: F / = Gm m has th sam valu whth m = Eath and m

More information

The theory of electromagnetic field motion. 6. Electron

The theory of electromagnetic field motion. 6. Electron Th thoy of lctomagntic fild motion. 6. Elcton L.N. Voytshovich Th aticl shows that in a otating fam of fnc th magntic dipol has an lctic chag with th valu dpnding on th dipol magntic momnt and otational

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

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

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

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

ECE theory of the Lamb shift in atomic hydrogen and helium

ECE theory of the Lamb shift in atomic hydrogen and helium Gaphical Rsults fo Hydogn and Hlium 5 Jounal of Foundations of Physics and Chmisty,, vol (5) 5 534 ECE thoy of th Lamb shift in atomic hydogn and hlium MW Evans * and H Eckadt ** *Alpha Institut fo Advancd

More information

(, ) which is a positively sloping curve showing (Y,r) for which the money market is in equilibrium. The P = (1.4)

(, ) which is a positively sloping curve showing (Y,r) for which the money market is in equilibrium. The P = (1.4) ots lctu Th IS/LM modl fo an opn conomy is basd on a fixd pic lvl (vy sticky pics) and consists of a goods makt and a mony makt. Th goods makt is Y C+ I + G+ X εq (.) E SEK wh ε = is th al xchang at, E

More information

Neutrino mass in tritium and rhenium single beta decay

Neutrino mass in tritium and rhenium single beta decay Nutino mass in titium and hnium singl bta dcay Rastislav Dvonicky Comnius Univsity, Batislava Slovakia in collaboation with.simkovic, K. Muto & R. Hodak Nutinos in Cosmology, in Asto-, Paticl- and Nucla

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

Electron spin resonance

Electron spin resonance Elcton sonanc 00 Rlatd topics Zman ffct, ngy quantum, quantum numb, sonanc, g-facto, Landé facto. Pincipl With lcton sonanc (ESR) spctoscopy compounds having unpaid lctons can b studid. Th physical backgound

More information

Strong Shear Formation by Poloidal Chain of Magnetic Islands

Strong Shear Formation by Poloidal Chain of Magnetic Islands Stong Sha Fomation by Poloidal Chain of Magntic Islands V.I. Maslo, F. Poclli* NSC Khako Institut of Physics & Tchnology, Khako, Ukain * Politcnico di Toino, Italy Objctis W will shown that: otical concti

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

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

DIELECTRICS MICROSCOPIC VIEW

DIELECTRICS MICROSCOPIC VIEW HYS22 M_ DILCTRICS MICROSCOIC VIW DILCTRIC MATRIALS Th tm dilctic coms fom th Gk dia lctic, wh dia mans though, thus dilctic matials a thos in which a stady lctic fild can st up without causing an appcial

More information

Kinetics. Central Force Motion & Space Mechanics

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

More information

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

Extinction Ratio and Power Penalty

Extinction Ratio and Power Penalty Application Not: HFAN-.. Rv.; 4/8 Extinction Ratio and ow nalty AVALABLE Backgound Extinction atio is an impotant paamt includd in th spcifications of most fib-optic tanscivs. h pupos of this application

More information

References. Basic structure. Power Generator Technologies for Wind Turbine. Synchronous Machines (SM)

References. Basic structure. Power Generator Technologies for Wind Turbine. Synchronous Machines (SM) Gnato chnologi fo Wind ubin Mhdad Ghandhai mhdad@kth. Rfnc 1. Wind Plant, ABB, chnical Alication Pa No.13.. WECC Wind Plant Dynamic Modling Guid, WECC Rnwabl Engy Modling ak Foc. 3. Wind ubin Plant Caabiliti

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

The Source of the Quantum Vacuum

The Source of the Quantum Vacuum Januay, 9 PROGRESS IN PHYSICS Volum Th Souc of th Quantum Vacuum William C. Daywitt National Institut fo Standads and Tchnology (tid), Bould, Coloado, USA E-mail: wcdaywitt@athlin.nt Th quantum vacuum

More information

College Prep Physics I Multiple Choice Practice Final #2 Solutions Northville High School Mr. Palmer, Physics Teacher. Name: Hour: Score: /zero

College Prep Physics I Multiple Choice Practice Final #2 Solutions Northville High School Mr. Palmer, Physics Teacher. Name: Hour: Score: /zero Collg Pp Phsics Multipl Choic Pactic inal # Solutions Nothvill High School M. Palm, Phsics Tach Nam: Hou: Sco: /zo You inal Exam will hav 40 multipl choic qustions woth 5 points ach.. How is cunt actd

More information

Chapter Six Free Electron Fermi Gas

Chapter Six Free Electron Fermi Gas Chapt Six Elcton mi Gas What dtmins if th cystal will b a mtal, an insulato, o a smiconducto? E Band stuctus of solids mpty stats filld stats mpty stats filld stats E g mpty stats filld stats E g Conduction

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

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

The Death of Stars - II.

The Death of Stars - II. Th Dath of Stars - II. Larning Objctivs! How can w us H-R diagrams to masur th ag of star clustrs (and hnc th ag of our Univrs)?! Why do high and low mass stars volv diffrntly? How ar havy lmnts such as

More information

Bohr model and dimensional scaling analysis of atoms and molecules

Bohr model and dimensional scaling analysis of atoms and molecules Boh modl and dimnsional scaling analysis of atoms and molculs Atomic and molcula physics goup Faculty: Postdocs: : Studnts: Malan Scully udly Hschbach Siu Chin Godon Chn Anatoly Svidzinsky obt Muawski

More information

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28 Chapt 10 Phys 3 Lctu 8 Dffacton Dffacton: gnal Fsnl vs. Faunhof dffacton Sval cohnt oscllatos Sngl-slt dffacton Dffacton Gmald, 1600s: dffacto, dvaton of lght fom lna popagaton Dffacton s a consqunc of

More information

(most) due to long range e m forces i.e. via atomic collisions or due to short range nuclear collisions or through decay ( = weak interactions)

(most) due to long range e m forces i.e. via atomic collisions or due to short range nuclear collisions or through decay ( = weak interactions) Spring 01, P67, YK Monday January 30, 01 8 Obsrvabl particl dtction ffcts ar : (most) du to long rang m forcs i.. via atomic collisions or du to short rang nuclar collisions or through dcay ( = wak intractions)

More information

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28 Chapt 10 Phys 3 Lctu 8 Dffacton Dffacton: gnal Fsnl vs. Faunhof dffacton Sval cohnt oscllatos Sngl-slt dffacton Dffacton Gmald, 1600s: dffacto, dvaton of lght fom lna popagaton Dffacton s a consqunc of

More information

EE243 Advanced Electromagnetic Theory Lec # 22 Scattering and Diffraction. Reading: Jackson Chapter 10.1, 10.3, lite on both 10.2 and 10.

EE243 Advanced Electromagnetic Theory Lec # 22 Scattering and Diffraction. Reading: Jackson Chapter 10.1, 10.3, lite on both 10.2 and 10. Appid M Fa 6, Nuuth Lctu # V //6 43 Advancd ctomagntic Thoy Lc # Scatting and Diffaction Scatting Fom Sma Obcts Scatting by Sma Dictic and Mtaic Sphs Coction of Scatts Sphica Wav xpansions Scaa Vcto Rading:

More information

ARDB Technical Note -Draft-11/4/97 µµ Pion Collection from an Intense Proton Beam in a Plasma

ARDB Technical Note -Draft-11/4/97 µµ Pion Collection from an Intense Proton Beam in a Plasma ARDB Tchnical Not -Daft-//97 µµ Pion Collction fom an ntns Poton Bam in a Plasma B. Shadwick, D. Whittum, and J. Wutl Th µµ collid conct quis an intns oton am smashing into a tagt to mak ions that susquntly

More information

3.46 PHOTONIC MATERIALS AND DEVICES Lecture 10: LEDs and Optical Amplifiers

3.46 PHOTONIC MATERIALS AND DEVICES Lecture 10: LEDs and Optical Amplifiers 3.46 PHOTONIC MATERIALS AND DEVICES Lctu 0: LEDs and Optical Amplifis Lctu Rfncs:. Salh, M. Tich, Photonics, (John-Wily, Chapts 5-6. This lctu will viw how lctons and hols combin in smiconductos and nat

More information

Study on the Classification and Stability of Industry-University- Research Symbiosis Phenomenon: Based on the Logistic Model

Study on the Classification and Stability of Industry-University- Research Symbiosis Phenomenon: Based on the Logistic Model Jounal of Emging Tnds in Economics and Managmnt Scincs (JETEMS 3 (1: 116-1 Scholalink sach Institut Jounals, 1 (ISS: 141-74 Jounal jtms.scholalinksach.og of Emging Tnds Economics and Managmnt Scincs (JETEMS

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

217Plus TM Integrated Circuit Failure Rate Models

217Plus TM Integrated Circuit Failure Rate Models T h I AC 27Plu s T M i n t g at d c i c u i t a n d i n d u c to Fa i lu at M o d l s David Nicholls, IAC (Quantion Solutions Incoatd) In a pvious issu o th IAC Jounal [nc ], w povidd a highlvl intoduction

More information

Chapter 4. QUANTIZATION IN FIVE DIMENSIONS

Chapter 4. QUANTIZATION IN FIVE DIMENSIONS Chat QUANTIZATION IN FIVE DIMENSIONS Th cding dvlomnt ovids a tmndous walth o mathmatical abstactions Howv th sms within it no adily aant mthod o intting th nw ilds I th aas to b no hysical ntity which

More information

ดร. สมศ กด แดงต บ ห องพ ก 617 โทร 5777 ห องว จ ย k46 โทร 585 Email: tst@maiol, kasmos47@yaoo Psonal Wbsit : www.sc.maiol.ac.t/scy/o_ol/somsak.tml Cous (1 st alf wbsit: www.sc.maiol.ac.t/scy/couss/scy415_9.tml

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

2. Laser physics - basics

2. Laser physics - basics . Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"

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

Kepler s problem gravitational attraction

Kepler s problem gravitational attraction Kele s oblem gavitational attaction Summay of fomulas deived fo two-body motion Let the two masses be m and m. The total mass is M = m + m, the educed mass is µ = m m /(m + m ). The gavitational otential

More information

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals. Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby

More information

STiCM. Select / Special Topics in Classical Mechanics. STiCM Lecture 11: Unit 3 Physical Quantities scalars, vectors. P. C.

STiCM. Select / Special Topics in Classical Mechanics. STiCM Lecture 11: Unit 3 Physical Quantities scalars, vectors. P. C. STiCM Slct / Spcial Topics in Classical Mchanics P. C. Dshmukh Dpatmnt of Phsics Indian Institut of Tchnolog Madas Chnnai 600036 pcd@phsics.iitm.ac.in STiCM Lctu 11: Unit 3 Phsical Quantitis scalas, vctos.

More information

STRIPLINES. A stripline is a planar type transmission line which is well suited for microwave integrated circuitry and photolithographic fabrication.

STRIPLINES. A stripline is a planar type transmission line which is well suited for microwave integrated circuitry and photolithographic fabrication. STIPLINES A tiplin i a plana typ tanmiion lin hih i ll uitd fo mioav intgatd iuity and photolithogaphi faiation. It i uually ontutd y thing th nt onduto of idth, on a utat of thikn and thn oving ith anoth

More information

FI 3103 Quantum Physics

FI 3103 Quantum Physics 7//7 FI 33 Quantum Physics Axan A. Iskana Physics of Magntism an Photonics sach oup Institut Tknoogi Banung Schoing Equation in 3D Th Cnta Potntia Hyognic Atom 7//7 Schöing quation in 3D Fo a 3D pobm,

More information

ROLE OF FLUCTUATIONAL ELECTRODYNAMICS IN NEAR-FIELD RADIATIVE HEAT TRANSFER

ROLE OF FLUCTUATIONAL ELECTRODYNAMICS IN NEAR-FIELD RADIATIVE HEAT TRANSFER ROLE OF FLUCTUATIONAL ELECTRODYNAMICS IN NEAR-FIELD RADIATIE HEAT TRANSFER Mathiu Fancou and M. Pina Mngüç Radiativ Tansf Laboatoy, Dpatmnt of Mchanical Engining Univsity of Kntucky, Lington, KY 456-53,

More information

Quantum Mechanics and General Relativity: Creation Creativity. Youssef Al-Youssef, 2 Rama Khoulandi. University of Aleppo, Aleppo, Syria

Quantum Mechanics and General Relativity: Creation Creativity. Youssef Al-Youssef, 2 Rama Khoulandi. University of Aleppo, Aleppo, Syria Quantum Mechanics and Geneal Relativity: Ceation Ceativity Youssef Al-Youssef, Rama Khoulandi Univesity of Aleppo, Aleppo, Syia Abstact This aticle is concened with a new concept of quantum mechanics theoy

More information

PH300 Modern Physics SP11 Final Essay. Up Next: Periodic Table Molecular Bonding

PH300 Modern Physics SP11 Final Essay. Up Next: Periodic Table Molecular Bonding PH Modrn Physics SP11 Final Essay Thr will b an ssay portion on th xam, but you don t nd to answr thos qustions if you submit a final ssay by th day of th final: Sat. 5/7 It dosnʼt mattr how smart you

More information

Get Solution of These Packages & Learn by Video Tutorials on GRAVITATION

Get Solution of These Packages & Learn by Video Tutorials on  GRAVITATION FEE Download Study Packag fom wbsit: www.tkoclasss.com & www.mathsbysuhag.com Gt Solution of Ths Packags & an by Vido Tutoials on www.mathsbysuhag.com. INTODUCTION Th motion of clstial bodis such as th

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLMNTARY INFORMATION. Dtmin th gat inducd bgap cai concntation. Th fild inducd bgap cai concntation in bilay gaphn a indpndntly vaid by contolling th both th top bottom displacmnt lctical filds D t

More information

be two non-empty sets. Then S is called a semigroup if it satisfies the conditions

be two non-empty sets. Then S is called a semigroup if it satisfies the conditions UZZY SOT GMM EGU SEMIGOUPS V. Chinndi* & K. lmozhi** * ssocit Pofsso Dtmnt of Mthmtics nnmli Univsity nnmling Tmilnd ** Dtmnt of Mthmtics nnmli Univsity nnmling Tmilnd bstct: In this w hv discssd bot th

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

Estimation of a Random Variable

Estimation of a Random Variable Estimation of a andom Vaiabl Obsv and stimat. ˆ is an stimat of. ζ : outcom Estimation ul ˆ Sampl Spac Eampl: : Pson s Hight, : Wight. : Ailin Company s Stock Pic, : Cud Oil Pic. Cost of Estimation Eo

More information

2. Bose-Einstein Fusion (BEF)

2. Bose-Einstein Fusion (BEF) UNIFYING THEORY OF LOW-ENERGY NUCLEAR REACTION AND TRANSMUTATION PROCESSES IN DEUTERATED/HYDROGENATED METALS, ACOUSTIC CAVITATION, GLOW DISCHARGE, AND DEUTERON BEAM EXPERIMENTS YEONG E. KIM AND ALEXANDER

More information

Green Dyadic for the Proca Fields. Paul Dragulin and P. T. Leung ( 梁培德 )*

Green Dyadic for the Proca Fields. Paul Dragulin and P. T. Leung ( 梁培德 )* Gn Dyadic fo th Poca Filds Paul Dagulin and P. T. Lung ( 梁培德 )* Dpatmnt of Physics, Potland Stat Univsity, P. O. Box 751, Potland, OR 9707-0751 Abstact Th dyadic Gn functions fo th Poca filds in f spac

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

Chapter 22 The Electric Field II: Continuous Charge Distributions

Chapter 22 The Electric Field II: Continuous Charge Distributions Chapte The lectic Field II: Continuous Chage Distibutions A ing of adius a has a chage distibution on it that vaies as l(q) l sin q, as shown in Figue -9. (a) What is the diection of the electic field

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

An Elementary Approach to a Model Problem of Lagerstrom

An Elementary Approach to a Model Problem of Lagerstrom An Elmntay Appoach to a Modl Poblm of Lagstom S. P. Hastings and J. B. McLod Mach 7, 8 Abstact Th quation studid is u + n u + u u = ; with bounday conditions u () = ; u () =. This modl quation has bn studid

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

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the Lctur 22-1 Byond Bohr Modl Unfortunatly, th classical visualization of th orbiting lctron turns out to b wrong vn though it still givs us a simpl way to think of th atom. Quantum Mchanics is ndd to truly

More information

Inertia identification based on adaptive interconnected Observer. of Permanent Magnet Synchronous Motor

Inertia identification based on adaptive interconnected Observer. of Permanent Magnet Synchronous Motor Intnational Jounal of Rsach in Engining and Scinc (IJRES) ISSN (Onlin): 232-9364, ISSN (Pint): 232-9356 www.ijs.og Volum 3 Issu 9 ǁ Sptmb. 25 ǁ PP.35-4 Intia idntification basd on adaptiv intconnctd Obsv

More information

Elements of Statistical Thermodynamics

Elements of Statistical Thermodynamics 24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,

More information

Keywords: Auxiliary variable, Bias, Exponential estimator, Mean Squared Error, Precision.

Keywords: Auxiliary variable, Bias, Exponential estimator, Mean Squared Error, Precision. IN: 39-5967 IO 9:8 Ctifid Intnational Jounal of Engining cinc and Innovativ Tchnolog (IJEIT) Volum 4, Issu 3, Ma 5 Imovd Exonntial Ratio Poduct T Estimato fo finit Poulation Man Ran Vija Kuma ingh and

More information

Atomic energy levels. Announcements:

Atomic energy levels. Announcements: Atomic nrgy lvls Announcmnts: Exam solutions ar postd. Problm solving sssions ar M3-5 and Tusday 1-3 in G-140. Will nd arly and hand back your Midtrm Exam at nd of class. http://www.colorado.du/physics/phys2170/

More information

MOS transistors (in subthreshold)

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

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration

More information

A STUDY OF PROPERTIES OF SOFT SET AND ITS APPLICATIONS

A STUDY OF PROPERTIES OF SOFT SET AND ITS APPLICATIONS Intnational sach Jounal of Engining and Tchnology IJET -ISSN: 2395-0056 Volum: 05 Issu: 01 Jan-2018 wwwijtnt p-issn: 2395-0072 STDY O POPETIES O SOT SET ND ITS PPLITIONS Shamshad usain 1 Km Shivani 2 1MPhil

More information

D-Cluster Dynamics and Fusion Rate by Langevin Equation

D-Cluster Dynamics and Fusion Rate by Langevin Equation D-Clust Dynamics an Fusion at by Langvin Equation kito Takahashi** an Noio Yabuuchi High Scintific sach Laboatoy Maunouchi-4-6, Tsu, Mi, 54-33 Japan **Osaka Univsity STCT Conns matt nucla ffct, spcially

More information

The failure of the classical mechanics

The failure of the classical mechanics h failur of th classical mchanics W rviw som xprimntal vidncs showing that svral concpts of classical mchanics cannot b applid. - h blac-body radiation. - Atomic and molcular spctra. - h particl-li charactr

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

A Cold Genesis Theory of Fields and Particles

A Cold Genesis Theory of Fields and Particles 1 A Cold Gnsis Thoy of Filds and Paticls Th discovis must b publishd (Galilo Galili, pincipl of scinc) 1.1 Intoduction Th abandonmnt of th concpt of th in th xplanation of th micophysics phnomna, though

More information

(( )( )) = = S p S p = S p p m ( )

(( )( )) = = S p S p = S p p m ( ) 36 Chapt 3. Rnoalization Toolit Poof of th oiginal Wad idntity o w nd O p Σ i β = idβ γ is p γ d p p π π π p p S p = id i d = id i S p S p d π β γ γ γ i β i β β γ γ β γ γ γ p = id is p is p d = Λ p, p.

More information

C-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0)

C-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0) An ltntiv to th us of hypolic dclin cuvs Ppd y: Sfim Ltd S E R A F I M info@sfimltd.com P. +44 (02890 4206 www.sfimltd.com Contnts Contnts... i Intoduction... Initil ssumptions... Solving fo cumultiv...

More information