Atom, Avogadro Number and Atomic Cosmology
|
|
- Julius Riley
- 5 years ago
- Views:
Transcription
1 Aom, Avogadro Numbr and Aomi Cosmology U. V.S. Sshavaharam, S. Lakshminarayana and B.V.S.T. Sai onorary fauly, I-SRV, Alakauri, ydrabad-5, AP, India. mail: D. of Nular Physis, Andhra Univrsiy, Visakhaanam-, AP, India. D. of ahmais and Com. Sin & ngg, unur ngg. Collg, unur-9, AP, India. Absra: If ligh is oming from h aomi mar of h galaxy, hn h obsrvd rdshif an b inrrd as an indx of h galai aomi mar ligh mission mhanism. Clarly saking rdshif may no b onnd wih galaxy rding. Th roosd basi ida is - during osmi voluion, as ag of h hydrogn aom inrass, mid hoon nrgy inrass. If so urrn osmologial hangs may b rfld in any xising aom. A any givn osmi im, ubbl lngh an b onsidrd as h graviaional or lromagni inraion rang. By highlighing h six major shoromings of modrn osmology, in his ar an am is mad o vrify h osmi alraion in a quanum mhanial aroah. Th four ossibl assumions ar : ) Rdud Plank s onsan inrass wih osmi im. ) Bing a rimordial volving blak hol and ubbl s onsan bing h angular vloiy, univrs is always roaing wih ligh sd. ) Aomi graviaional onsan is squard Avogadro numbr ims h lassial graviaional onsan and ) Aomi graviaional onsan or h lassial graviaional onsan shows disr bhavior. This may b h roo aus of disr naur of rvolving lron s angular momnum. Wih rfrn o h rsn aomi and nular hysial onsans, obaind ubbl s onsan is (67.88 o 7.) km/s/ and is vry los o h rommndd valu. This is a rmarkabl oinidn and sms o lay a vial rol in fuur unifid hysis. Kywords: Rdud Plank s onsan; ubbl lngh; ubbl mass; ubbl volum; ubbl dnsiy; Cosmi rd shif; CBR mraur; Avogadro numbr; Aomi graviaional onsan;. INTRODUCTION This ar is an udad vrsion and a rviw of h auhors rnly ublishd work Unifid Cons in Cosmi, Aomi and Nular Physis []. In hysis hisory, for any nw ida or obsrvaion or nw modl - a h vry bginning hir xisn was vry doubful. Th bs xamls wr : ) xisn of aom ) xisn of quanum of nrgy ) xisn of ingral naur of angular momnum ) xisn of wav mhanis 5) Six quarks having fraional harg 6) Confusion in onfirming h xisn of muon/ion 7) xisn of Blak hols 8) Blak hol radiaion 9) insin s osmologial Lambda rm ) Cosmi rd shif ) Disovry of CBR and ) Alraing univrs and so on [-6]. any hysiiss hink abou h ossibl variaion of h fin sruur raio and xrimns ar in rogrss. In a horial aroah, a varying has bn roosd as a hararisi and unifid way of solving roblms in osmology and asrohysis. or rnly, horial inrs in varying onsans (no jus ) has bn moivad by sring hory and ohr suh roosals for going byond h Sandard odl of aril hysis. In Oobr Wbb al [7] rord a variaion in dndn on boh rdshif and saial dirion. r i should b nod ha, h on - variaion of alha dirly and indirly is giving a lu o hink abou h ossibl variaion of h rdud Plank s onsan or Plank s onsan. This is a vry snsiiv oin and nds srong xrimnal vidn and vigorous horial analysis. Bu ill oday from ground basd laboraory xrimns no variaion was noid in h magniud of h fin sruur raio. In his ar auhors mad an am o sudy his omliad issu in a horial way. In undrsanding h basi ons of unifiaion or TO, rol of dark nrgy and dark mar is insignifian. vn hough hr wr a numbr ars/books ublishd on osmology, h am for a omrhnsiv sudy on his subj, ould wih omaraiv sudis wih h modrn osmology on on hand and wih h modrn aomi hysis on h ohr, was no mad by anybody so far. Th rsn sudy an b onsidrd as a bginning roj in his fild. Cosmologial obsrvaions hrough ground lso or salli lso is a normal rai. In his ar undr onsidraion, i an b suggsd haurrn osmologial hangs an b undrsood by
2 Aom, Avogadro Numbr and Aomi Cosmology sudying h aom and aomi nulus hrough ground basd xrimns. I is an inrsing ar of h sudy of osmology and fundamnal inraions. So far no insiu has akn his subj for R&D. This ida is qui uniqu, naural and h onnss in h subjs of osmology and fundamnal inraions an b liminad. Th fuur sin gnraion an ado his roosd on as a hararisi rfrn for h fuur sinifi obsrvaions, analysis and xrimns. I is an inrsing ida and yars of aomi, nular and osmi hysis an b rfind and unifid. In bwn h fla univrs and h losd univrs, hr is on omromis. Tha is ubbl volum. ubbl volum an b onsidrd as a ky ool in osmology and unifiaion. Som osmologiss us h rm ubbl volum o rfr o h volum of h obsrvabl univrs. Wih rfrn o h ah s rinil [] and h ubbl volum, a any osmi im, if ubbl mass is h rodu of osmi riial dnsiy and h ubbl volum, hn i an b suggsd ha, wihin h ubbl volum, ah and vry oin in fr sa is inflund by h ubbl mass. W bgin his ar wih h six major shoromings of modrn osmology.. ajor shoromings of modrn osmology A) If ligh is oming from h aomi mar of h galaxy, hn rdshif an b inrrd as an indx of h galai aomi mar ligh mission mhanism. In no way i sms onnd wih galaxy rding. B) If osmi xansion is oninuous and alraing and rdshif is a masur of osmi xansion, ra of inras in rdshif an b onsidrd as a masur of osmi ra of xansion. Thn hr is no ossibiliy o obsrv a onsan rd shif. rly by simaing galaxy disan (insad of simaing galaxy rding sd) on anno vrify h osmi alraion. C) Dro in osmi mraur an b onsidrd as a masur of osmi xansion and ra of dras in osmi mraur an b onsidrd as a masur of osmi ra of xansion. Bu if ra of dras in mraur is vry small and is byond h so of urrn xrimnal vrifiaion, hn h wo ossibl sas ar: a) osmi mraur is drasing a a vry slow ra and univrs is xanding a a vry slow ra and b) hr is no obsrvabl hrmal xansion and hr is no obsrvabl osmi xansion. D) If Dark nrgy is h major ouom of h alraing univrs, i is vry imoran o no ha - in undrsanding h basi ons of unifiaion or ohr fundamnal aras of hysis, rol of dark nrgy is vry insignifian. ) So far no ground basd xrimn onfirmd h xisn of dark nrgy. Thr is no singl lu or dfiniion or vidn o any of h naural hysial roris of (h assumd) dark nrgy. F) Dimnsionally i is ossibl o show ha, h dimnsions of ubbl s onsan and angular vloiy ar sam. If so onsidring ubbl s onsan mrly as an xansion aramr may no b orr.. Isoroy may b bs ossibl in a losd xanding univrs If univrs is rally alraing, basd on h ubbl s law [], for h obsrvr - h rding or alraing galaxy mus show a oninuous inras in is rd shif! Som says: insananously rd shif anno inras du o h limid hoon sd. If osmi alraion bgan 5 billion yars ago, hn during is alrad rding journy, h galaxy mus show a oninuous inras in rd shif - whhr h hang is du o as alrad rding or rsn alrad rding. Thr is no suh vidn. In his onnion - h aroria ida an b sad as follows: ) Rdshif is a masur of xansion and ) Ra of inras in rd shif is a masur of osmi ra of xansion. This ida an b suord by anohr siml on: ) Dro in osmi mraur is a masur of osmi xansion and ) Ra of dras in osmi mraur is a masur of osmi ra of xansion. I an b suggsd ha, A) In a losd xanding univrs, in andm wih xansion ra, insananously hrmal wavs undrgo oninuous srhing in all dirions wih rs o h nr of h losd univrs and h losd boundary. B) Whn h xansion ra is vry slow. i. raially zro xansion ra, srhing in hrmal wavs is almos zro and on an obsrv uniform hrmal wavlngh in all dirions. C) In a fla univrs, whr hr is no boundary and no nr, i may no b ossibl.. ubbl s oinion on Cosmi rdshif In 97 ubbl [] suggsd ha Th rd shifs ar mor asily inrrd as vidn of moion in h lin of sigh away from h arh as vidn ha h nbula in all dirions ar rushing away from us and ha h farhr away hy ar, h fasr hy ar rding. This inrraion lnds islf dirly o horis of xanding univrs. Th inrraion is no univrsally ad, bu vn h mos auious of us admi ha rd shifs ar vidn of ihr an xanding univrs or of som hihro unknown rinil of naur Ams hav bn mad o aain h nssary rision wih h inh, and h rsuls aar o b U. V. S. Sshavaharam, Prof. S. Lakshminarayana and Prof. B.V.S.T. Sai
3 Aom, Avogadro Numbr and Aomi Cosmology signifian. If hy ar valid, i sms likly ha h rd-shifs may no b du o an xanding univrs, and muh of h urrn sulaion on h sruur of h univrs may rquir r-xaminaion. Th signifian daa, howvr, wr nssarily obaind a h vry limi of a singl insrumn, and hr wr no ossibl mans of hking h rsuls by indndn vidn. Thrfor h rsuls mus b ad for h rsn as suggsiv rahr han dfiniiv. W may rdi wih onfidn ha h inh will ll us whhr h rd shifs mus b ad as vidn of a raidly xanding univrs, or aribud o som nw rinil in naur. Whavr may b h answr, h rsul may b wlomd as anohr major onribuion o h xloraion of h univrs.. insin s oinion on unifiaion of lromagni and graviaional inraions So, why no h whol univrs? Th onsquns of a sinning univrs sms o b rofound [9-], naural and osmi ollas an b rvnd. Thus osmi (ligh sd) roaion an b onsidrd as an alrnaiv o h famous rulsiv graviy on. Wih a siml drivaion i is ossibl o show ha, ubbl s onsan rrsns osmologial angular vloiy. Assum ha, a lan of mass and siz R roas wih angular vloiy and linar vloiy v in suh a way ha, fr or loosly bound aril of mass m lying on is quaor gains a kini nrgy qual o onial nrgy as, m mv () R v and = R v () R R R No ha, insin, mor han any ohr hysiis, unroubld by ihr quanum unrainy or lassial omlxiy, blivd in h ossibiliy of a oml, rhas final, hory of vryhing. [,]. also blivd ha h fundamnal laws and rinils ha would mbody suh a hory would b siml, owrful and bauiful. Physiiss ar an ambiious lo, bu insin was h mos ambiious of all. is dmands of a fundamnal hory wr xrmly srong. If a hory onaind any arbirary faurs or undrmind aramrs hn i was dfiin, and h dfiiny oind h way o a dr and mor rofound and mor rdiiv hory. Thr should b no fr aramrs no arbirarinss. Aording o his hilosohy, lromagnism mus b unifid wih gnral rlaiviy, so ha on ould no simly imagin ha i did no xis. Furhrmor, h xisn of mar, h mass and h harg of h lron and h roon (h only lmnary arils rognizd bak in h 9s), wr arbirary faurs. On of h main goals of a unifid hory should b o xlain h xisn and alula h roris of mar.. In his ar auhors mad an am o undrsand h basi ons of unifiaion via aril osmology [5,6]..5 Th osmi riial dnsiy and is dimnsional analysis Rn findings from h Univrsiy of ihigan suggs ha h sha of h Big Bang migh b mor omliad han rviously hough, and ha h arly univrs sun on an axis. A lf-handd and righ-handd imrin on h sky as rordly rvald by galaxy roaion would imly h univrs was roaing from h vry bginning and raind an ovrwhlmingly srong angular momnum [8]. alaxis sin, sars sin, and lans sin. i. Linar vloiy of lan s roaion is qual o fr aril s sa vloiy. Wihou any xrnal owr or nrgy, s aril gains sa vloiy by viru of lan s roaion. Using his ida, Blak hol radiaion and origin of osmi rays an b undrsood. No ha if arh omls on roaion in on hour hn fr arils lying on h quaor will g sa vloiy. Now wriing, R, v 8 8 = Or () R U. V. S. Sshavaharam, Prof. S. Lakshminarayana and Prof. B.V.S.T. Sai Dnsiy, = 8 In ral im, his obaind dnsiy may or may no b qual o 8 h aual dnsiy. Bu h raio, ral ral () may hav som hysial maning. Th mos imoran oin o b nod hr, is ha, as far as dimnsions and unis ar onsidrd, from quaion (), i is vry lar ha, roorionaliy onsan bing, 8 angular vloiy dnsiy (5) quaion () is similar o fla modl on of osmi riial dnsiy
4 Aom, Avogadro Numbr and Aomi Cosmology 8 (6) Comaring quaions () and (6) dimnsionally and onually, i.. wih = 8 8 (7) and (8) I is vry lar ha, dimnsions of ubbl s onsan mus b radian/sond. In any hysial sysm undr sudy, for any on siml hysial aramr hr will no b wo diffrn unis and hr will no b wo diffrn hysial manings. This is a siml lu and brings osmi roaion ino iur. This is ossibl in a losd univrs only. Cosmi modls ha dnds on his riial dnsiy may onsidr angular vloiy of h univrs in h la of ubbl s onsan. In h sns, osmi roaion an b inludd in h xising modls of osmology. Thn h rm riial dnsiy simly aars as h shrial volum dnsiy of h losd and xanding univrs.. POSSIBL ASSUPTIONS IN UNIFID COSIC PYSICS Th ossibl assumions in unifid osmi hysis an b xrssd in h following way [-],[-5]: A) ubbl lngh / an b onsidrd as h graviaional or lromagni inraion rang. B) Bing a rimordial volving blak hol and angular vloiy bing, univrs is always roaing wih ligh sd [-]. C) Aomi graviaional onsan [8-5] is squard Avogadro numbr ims h lassial graviaional onsan. Thus, whr A N (9) A is h Aomi graviaional onsan, N is h lassial is h Avogadro numbr and graviaional onsan. No ha, N an b onsidrd as h raio of lassial for limi and wak for magniud [,]. D) Aomi graviaional onsan or h lassial graviaional onsan shows disr bhaviour as n. A or N n. whr n,,,.. ) Rdud Plank s onsan inrass wih osmi im []. Thus a any givn osmi im, d( ) ) is a masur of osmi ra of xansion. I is d ossibl o show ha, onial nrgy of lron in hydrogn aom is dirly roorional o. Bohr s sond osula whih suggss ha onial nrgy of lron in hydrogn aom is invrsly roorional o sms o b a oinidn [5,5]. ) Pas ligh quana mid from agd galaxy will hav lss nrgy and show a rd shif wih rfrn o h riving galaxy. During journy ligh quana will no los nrgy and hr will b no hang in ligh wavlngh. ) Th basi or original dfiniion of rsn/urrn rdshif z sms o b U. V. S. Sshavaharam, Prof. S. Lakshminarayana and Prof. B.V.S.T. Sai z bu no z. () h r is h nrgy of hoon a our galaxy and h is h nrgy of hoon a h obsrvd galaxy whn i was mid. Similarly is h wav lngh of ligh rivd from obsrvd galaxy and is h wav lngh of ligh in laboraory. No ha, basd on h inrasing valu of h Plank s onsan, rsn rd shif z will b dirly roorional o our galaxy and obsrvd galaxy ag diffrn or im akn by ligh o rah our galaxy from h old galaxy. Thus z and z. () r is h roorionaliy onsan. In his way an b inororad dirly. Tim akn by ligh o rah our galaxy or h ag diffrn of our galaxy and obsrvd galaxy an b xrssd as, z. () z. () In his way, h basi and original dfiniion of galaxy rding and alraing univrs ons an b liminad and a dlraing or xandd univrs on an b oninud wihou any diffiuly. Now h fundamnal qusion o b answrd is: If h, how o dfin h rd shif?. In h aks h rol of
5 Aom, Avogadro Numbr and Aomi Cosmology sion.7, onsidring w roosd a siml soluion o his roblm. Wih diffrn galaxis and wih diffrn, z z z () whr,,,.. rrsns diffrn galaxis. In an alrnaiv way h auhors roos h following onduring osmi voluion agd ydrogn aom mis nrgi hoon. Clarly saking, as ag of h hydrogn aom inrass, i mis hoon wih inrasd quanum of nrgy. Thus as ligh quana mid from old galaxy will hav lss nrgy and show a rd shif wih rfrn o our galaxy. During journy ligh quana will no los nrgy and hr will b no hang in ligh wavlngh. ) A any givn osmi im, h Shwarzshild radius of univrs is whr (5) is h osmi mass a ha im. Wih his ida, a any givn osmi im, osmi siz an b onsraind o a maximum insad of infiniy. Th osmi mass an b xrssd as. (6) I an b alld as h ubbl mass'. Thus h osmi volum dnsiy aks h following wll known riial dnsiy form,. 8 v I an b alld as h osmi ubbl dnsiy.. APPLICATIONS OF T PROPOSD ASSUPTIONS (7) Similar o and los o h Plank sal and wih rfrn and, a o h fundamnal hysial onsans fundamnal mass uni an b onsrud as kg. I an b onsidrd as a hararisi fundamnal unifid hargd mass uni. I is noid ha, h raio lays a vry inrsing rol in fiing h osmi mar dnsiy and hrmal nrgy dnsiy.. Cosmi ar Dnsiy Aroximaly rlaion bwn osmi volum dnsiy and mar dnsiy an b xrssd as v m m ln (8) 8 No ha, a rsn obaind mar dnsiy m an b omard wih h lliial and siral galaxy mar dnsiy. Basd on h avrag mass-o-ligh raio for any galaxy [5].5 h gram/m m - (9) whr for any galaxy, /L alaxy = /L Sun and h numbr: 7 h.7. No ha Km/s/ lliial galaxis robably omris abou 6% of h galaxis in h univrs and siral galaxis ar hough o mak u abou % of h galaxis in h univrs. Almos 8% of h galaxis ar in h form of lliial and siral galaxis. For siral galaxis, h - 9 and for lliial galaxis, h -. For our galaxy innr ar, h - 6. Thus h avrag h - is vry los o 8 o 9 and is orrsonding mar dnsiy is (5.88 o 6.6) - gram/m... Cosmi Thrmal nrgy Dnsiy a is h radiaion nrgy b is h Win s dislamn onsan, raio of osmi volum nrgy dnsiy and osmi hrmal nrgy an b xrssd as A any givn osmi im, if onsan and v ln at 8 8 r, a 5 h b 5 5 kb k B () kb kb.997. Thus in a lassial aroah, b b indndn of h Plank s onsan, radiaion onsan an. xrssd as abov. vn wih rfrn o quanum mhanis also, Win s onsan is a osmologial onsan. This is a vry snsiiv oin o b disussd. Win s law is basd on h lassial aroah [5,55]. Wih rfrn o Win s dislamn law, i an b undrsood 5 U. V. S. Sshavaharam, Prof. S. Lakshminarayana and Prof. B.V.S.T. Sai
6 Aom, Avogadro Numbr and Aomi Cosmology ha, for any blak body, mos srongly mid hrmal wav lngh is invrsly roorional o is absolu mraur Wih rfrn o h urrn magniud of h Plank s onsan, aura valu of h Win s onsan an b simad and ha obaind magniud an b onsidrd as a onsan hroughou h osmi im. If so, a any givn osmi im, hrmal nrgy dnsiy an b xrssd as at ln 8 () If is los o 7 km/s/, obaind CBR mraur [56,57] is.7 K. Thus i an b suggsd ha, a any givn osmi im, mar nrgy dnsiy an b onsidrd as h gomri man of hrmal-nrgy dnsiy and volum-nrgy dnsiy. m at at v 8.. Wavlngh of h CB radiaion () Auhors noid wo aroxima mhods for simaing h CB radiaion. omri man of h mhods is fiing wih h obsrvaional daa auraly. hod-: Wih rfrn o h Win s dislamn law, wav lngh of h mos srongly mid CB radiaion an b xrssd as v m ln () m No ha his xrssion is fr from h radiaion onsans. If is los o 7 km/s/, obaind (mos srongly mid) wavlngh of h CB radiaion is.7 mm. hod-: Pair arils raion and annihilaion in fr sa - is an inrsing ida. In h xanding univrs, by onsidring h roosd hargd and is air annihilaion as a hararisi osmi hnomna, origin of h isoroi CB radiaion an b addrssd.. Thrmal nrgy an b xrssd as k T B Basd on Win s dislamn law, B m () b bk (5) T If is los o 7 km/s/, obaind (mos srongly mid) wavlngh of h CB radiaion is.8 mm. hod-: Considring h gomri man wav lngh of wav lngh obaind from mhods- and, wav lngh of h mos srongly mid CB radiaion an b xrssd as bk B m ln (6) bkb m ln (7) If is los o 7 km/s/, obaind (mos srongly mid) wavlngh of h CB radiaion is.6 mm. In his way, in a smi mirial aroah, h obsrvd CB radiaion mraur an b undrsood. Clarly saking, v ln m m (8) m (9) bkb 5 and.856 m sms o b a lassial onsan and an b onsidrd as a hararisi lassial hrmal wav lngh. Th mos imoran oin is ha, as h blak hol univrs is xanding, is xansion ra an b d vrifid wih m. Prsn obsrvaions indias ha, d CB radiaion is smooh and uniform. Thus i an b suggsd ha, a rsn hr is no dabl osmi xansion or osmi alraion.. Abou h osmi im A any givn osmi im, i an b suggsd ha, r, R at 8 8 R is h osmi radius a im and is h imaginary disan ravlld by ligh in im. From rlaion (). ln R 8 () () In his way his roosal diffrs from h xising on of.. Thorially i is a vry snsiiv roblm whhr o onsidr or no o onsidr h dnsiy raio 6 U. V. S. Sshavaharam, Prof. S. Lakshminarayana and Prof. B.V.S.T. Sai
7 Aom, Avogadro Numbr and Aomi Cosmology. Whn 8, at, 8 If is h rsn lromagni inraion rang, R and osmi im an b obaind as 5 9. s. Prsn, 8 at 8 at 77 rillion yars. ().5. Th Cosmologial Fin Sruur Raio In hysis, h fin-sruur raio ( ) is a fundamnal hysial onsan, namly h ouling onsan hararizing h srngh of h lromagni inraion. Bing a dimnsionlss quaniy, i has onsan numrial valu in all sysms of unis. If v rsn osmi volum nrgy dnsiy and is h at is h rsn osmi hrmal nrgy dnsiy, i is noid ha, at ln. v () No ha, from unifiaion oin of viw, ill oday rol of dark nrgy or dark mar is unlar and undidd. Thir laboraory or hysial xisn is also no y onfirmd. In his riial siuaion his aliaion an b onsidrd as a ky ool in aril osmology. No ha larg dimnsionlss onsans and omound hysial onsans rfl an inrinsi rory of naur. A rsn abov rlaion aks h following form. ln at () A rsn if obsrvd CBR mraur is T.75 K, obaind 7.5 Km/s/. Afr simlifiaion, i an b inrrd as follows. Toal hrmal nrgy in h rsn ubbl volum an b xrssd as, T at (5) h rsn lromagni onial an b xrssd as (6) Now invrs of h rsn fin sruur raio an b xrssd as T ln (7) r, in RS, dnominaor may b a rrsnaion of oal hrmal nrgy in half of h osmi shr or hrmal nrgy of any on ol of h osmi shr. Thus a any osmi im, T ln Whn, at and,. 8 (8) In his way, in a unifid mannr, h rsn fin sruur raio an b fid. From his rlaion i is ossibl o say ha, d osmologial ra of hang in fin sruur raio, d may b onsidrd as an indx of h fuur osmi alraion. any hysiiss hink i s ossibl variaion and xrimns ar in rogrss. Sifially, a varying has bn roosd as a way of solving roblms in osmology and asrohysis. or rnly, horial inrs in varying onsans (no jus ) has bn moivad by sring hory and ohr suh roosals for going byond h Sandard odl of aril hysis. In Oobr Wbb al. rord a variaion in dndn on boh rdshif and saial dirion [7]. Till oday from ground basd laboraory xrimns no variaion was noid in h magniud of h fin sruur raio. Smi mirially o a good aroximaion, i is noid ha, x ln ln x (9) 7 U. V. S. Sshavaharam, Prof. S. Lakshminarayana and Prof. B.V.S.T. Sai
8 Aom, Avogadro Numbr and Aomi Cosmology r x. If,. Wih his rlaion and wih rfrn o h urrn magniud of h fin sruur raio, obaind valu of h rsn ubbl s onsan is los o 7.75 km/s/..6. Th Cosmologial Rdud Plank s Consan From abov rlaions a any im an b simad and hus h osmologial rdud Plank s onsan an b obaind wih h xising dfiniion, () Wih his ida, magni momns of lron, nuron and roon an b xrssd as x m. m () whr x is a faor o b drmind. In as of lron, x, for nuron, x, and for roon, x. From abov rlaions i an b gussd ha, hr xiss a srong inronnion in bwn univrs and h ydrogn aom. Wih many numrial oinidns i is noid ha, m m () m r m an b onsidrd as h numbr of lrons in h rsn univrs of mass, If so, rsn ubbl s onsan an b xrssd as m m 7.7 km/s/ Thus i is ossibl o guss ha,. () m m onsan () Anohr vry inrsing rlaion is m m mm (5) R R No ha hr, R is h rms radius of roon [58-6]. If lron rvolvs round h roon, his xrssion an b givn a han. Th wo bs quod valus of h rms radius of roon ar.8768(69)fm and.88(67) fm [58, 59]. If so, rsn ubbl s onsan an b xrssd as mm R If o 7.69 km/s/ (6) R fm 7.69 km/s/ and if R.8768 fm km/s/. This an b omard wih h rn valu (67.8 ±.77) km/s/. rommndd by Ad, P. A. R.; Aghanim, N.; Armiag- Calan, C.; al. [57] on arh. Anohr hararisi and inrsing rlaion is h h or Now from rlaions (7) and (9) whr (7) m m (8) R R R R m m R m m. Plas no ha no arbirary aramr is involvd in his xrssion. From unifiaion oin of viw his an b givn a han. onsidring o. Disr naur of. n m,. n m or. (9) an b obaind by n whr n,,... Comard n sms o b raial. I dirly lads o quanum graviy. Thn h disr naur of h roosd aomi graviaional onsan an b xrssd as N n.. Anyhow, i has o b disussd in dh. From rlaion (5) fin sruur raio an b xrssd as m R m (5) 8 U. V. S. Sshavaharam, Prof. S. Lakshminarayana and Prof. B.V.S.T. Sai
9 Aom, Avogadro Numbr and Aomi Cosmology r m is h lassial radius of lron and is h assumd rsn graviaional and lromagni inraion rang. In his ar w ar showing h diffrn ossibl ways fiing h Plank s onsan. Whhr i follows a naural logarihmi rlaion or a linar rlaion o b onfirmd. Now h fundamnal qusion o b answrd is- ow varis wih im? Answr an b obaind by analysing all h abov rlaions. I has b vrifid from h as and fuur galaxy ag and rdshif daa analysis..7. lron s Chararisi Ponial nrgy and h osmi rd shif In ydrogn aom, by rial-rror, i is noid ha, mm. m Am (5) This is an obsrvaion. r, LS = 7.56 V and RS = 7.8 V. r rror is.55%. Thus in hydrogn aom onial nrgy of lron an b xrssd as mm o. m Am (5) On simlifiaion and onsidring h assumd variabl naur of form., abov xrssion aks h following siml mm o Am (5) r rror is.77%. Wih rfrn o h rror bars [58] in h magniuds of N,, his rlaion an b givn a han. If oal nrgy is half of h onial nrgy, a rsn, in hydrogn aom, lron s hararisi disr oal nrgy [8,9] an b xrssd as mm oal n. A m whr n =,,,..A any givn osmi im, oal n. A m mm Thus i an b suggsd ha, oal (5) (55). Plas no ha, from Bohr s hory of hydrogn aom, oal. Auhors ar working on his onual varian. Soluion mainly dnds uon h origin of and i aks som im o rsolv h issu. Now wih rfrn o Bohr s sond osula, in h as, a any galaxy, mid hoon nrgy an b xrssd as Pho mm h Am n n mm Am n n Pho whr n n.a rsn mid hoon nrgy an b xrssd as mm h Pho Am n n (56) (57) Now for any quanum jum, in h as i an b shown ha, Am n n mm (58) Corrsonding o his obaind, from h rlaion is orrsonding an b simad. From and from rlaions () or (7) orrsonding CBR mraur an b simad. Thus for any galaxy, whr was laying a ky rol, orrsonding rsn osmi rd shif an b xrssd as Pho Pho z (59) Pho Now, aroximaly from rlaion () im akn by ligh o ravl from obsrvd galaxy o our galaxy or h ag diffrn of our galaxy and h obsrvd galaxy an b xrssd as z (6) Obaind has o b vrifid wih ohr dvlod absolu mhods of galaxy ag simaion. If rsn rdshif aroahs uniy, i an b suggsd ha, vn hough rsn osmi im is 7 rillion yars, our galaxy an no riv a ligh ha was mid rior o from h bginning of osmi voluion..8. Bohr radius of hydrogn aom From abov rlaions, a rsn Bohr radii in hydrogn aom an b xrssd as n. A m an mm Clarly wriing, (6) 9 U. V. S. Sshavaharam, Prof. S. Lakshminarayana and Prof. B.V.S.T. Sai
10 Aom, Avogadro Numbr and Aomi Cosmology a a n n an. ROL OF NUCLAR PYSICS n m m. A m N AND. To fi h rms radius of roon IN ATOIC AND Wih rfrn o h rms radius of roon [58,59], i is noid ha, R m Am m Am (65).855 fm whr (6) (6) (6). No ha, no arbirary aramr is involvd in his rlaion. Obaind valu is vry los o h rommndd rms radius of roon. This roosal may b givn a han. Any how hr i is a mus o jusify h rol of h raio m. Bu is inrraion sms o b vry omliad. Auhors ar working on his oinidn. Th wo imoran obsrvaions ar, ) Shwarzshild radius of roon whr h oraing graviaional onsan is N and ) raviaional and lromagni for raio of roon whr h oraing graviaional onsan is.. To fi h rsn ubbl s onsan From rlaions (6) and (65) m m m N m N From his omound rlaion, or simad in a unifid mannr. or m N m N an b (66) (67) Wih rfrn o rlaion (65) rsn magniud of ubbl s onsan an b xrssd as m m N rad/s 69.6 km/s/. (68) This an b omard wih h rn valu (rommndd by C. L. Bnn al [56] on Dmbr ) km/s/. This is a rmarkabl oinidn and sms o lay a vial rol in fuur unifid hysis. DISCUSSION & CONCLUSIONS Wih rfrn o h rsn ons of osmi alraion and wih laboraory xrimns on may no did whhr univrs is alraing or dlraing. any xrimns ar undr rogrss o d and onfirm h xisn of dark mar and dark nrgy. Along wih hs xrimns if on is willing o hink in his nw dirion, from aomi and nular inus, i may b ossibl o vrify h fuur osmi alraion. Wih h roosd ons and wih h advaning sin and hnology, from h ground basd laboraory xrimns, from im o im h on d / d an b u for xrimnal ss. Thr is no nd o dsign a nw xrimn. Wll sablishd xrimns ar alrady availabl by whih Plank s onsan an b simad. Alrnaivly in a horial way, h roosd aliaions or smi mirial rlaions an b givn a han and h subj of lmnary aril hysis and osmology an b sudid in a unifid mannr. I is ru ha h roosd rlaions ar sulaiv and uliar also. By using h roosd rlaions and alying hm in fundamnal hysis, in du ours hir rol or xisn an b vrifid. Wih hs rlaions, ubbl onsan an b simad from aomi and nular hysial onsans. If on is abl o driv hm wih a suiabl mahmaial modl, indndn of h osmi rdshif and CBR obsrvaions, h fuur osmi alraion an b vrifid from aomi and nular hysial onsans. In undrsanding h basi ons of unifiaion or TO, rol of dark nrgy and dark mar is insignifian. Basd on h roosd rlaions and aliaions, ubbl volum or ubbl mass, an b onsidrd as a ky ool in unifiaion as wll as osmology. Considring h roosd rlaions and ons i is ossibl o say ha hr xiss a srong rlaion bwn osmi ubbl mass, Avogadro numbr and unifiaion. Now h nw s of roosd rlaions ar on o h sin ommuniy. Whhr o onsidr hm or disard hm dnds on h hysial inrraions, logis, xrimns and obsrvaions. Th mysry an b rsolvd only wih furhr rsarh, analysis, disussions and nouragmn. U. V. S. Sshavaharam, Prof. S. Lakshminarayana and Prof. B.V.S.T. Sai
11 Aom, Avogadro Numbr and Aomi Cosmology ACKNOWLDNTS Th firs auhor is indbd o rofssor K. V. Krishna urhy, Chairman, Insiu of Sinifi Rsarh on Vdas (I-SRV), ydrabad, India and Shri K. V. R. S. urhy, formr sinis IICT (CSIR) ov. of India, Diror, Rsarh and Dvlomn, I-SRV, for hir valuabl guidan and gra suor in dvloing his subj. RFRNCS [] U. V. S. Sshavaharam, S. Lakshminarayana, B.V.S.T. Sai. Unifid Cons in Cosmi, Aomi and Nular Physis. lobal Journal of Sin Fronir Rsarh (A) Vol. Issu,.57-65, (). [] ubbl. P, A rlaion bwn disan and radial vloiy among xra-galai nbula, PNAS, 99, vol. 5, 99, [] ubbl,.p, Th -inh lso and som roblms i may solv. PASP, 59, 5-67, 97. [] Bruno Libundgu and Jsr Sollrman. A osmologial surris: h univrs alras. urohysis Nws () Vol. No. [5] P. J.. Pbls and Bhara Rara (). Th osmologial onsan and dark nrgy. Rviws of odrn Physis 75 (): [6] Saul Prlmur, Surnova, Dark nrgy and h Alraing Univrs, Amrian Insiu of Physis, Physis Today, 5-6, Aril. [7] Joshua Friman, ihal Turnr and Dragan urr, Dark nrgy and h Alraing Univrs. Ann. Rv. Asron. Asrohys.6: 85-, 8. [8] usaha Ishak, Rmarks on h Formulaion of h Cosmologial Consan/Dark nrgy Problms, Found Phys, 7,7 98, 7. [9] J. W. offa, odifid raviy Or Dark ar? Onlin Availabl: h://arxiv.org/abs/.95v [] Narlikar, J.V, Vishwakarma,R.. and Burbidg.., Inrraions of h Alraing Univrs, Th Publiaions of h Asronomial Soiy of h Paifi, Volum, Issu 8,. 9-96,. [] Arman Shafilooa, Varun Sahnib and Alxi A. Sarobinsky, Is osmi alraion slowing down? Phys. Rv. D 8,, 9. [] Narlikar J.V. Dir Paril Formulaion of ah's Prinil. insin Sudis, vol. 6: ah's Prinil: From Nwon's Buk o Quanum raviy, Birkhausr Boson, In. Prind in h Unid Sas [] awking S.W. A brif hisory of im. Banam Dll ublishing grou.998. [] David ross, insin and h sarh for Unifiaion. Currn sin, Vol. 89, No., 5 D 5. [5] P. A.. Dira. Th osmologial onsans. Naur, 9,, 97. [6] P. A.. Dira. A nw basis for osmology. Pro. Roy. So. A 65, 99, 98 [7] J.K. Wbb al. Indiaions of a saial variaion of h fin sruur onsan. Physial Rviw lrs, 7 (9) [8] ihal J. Longo, Dion of a Diol in h anddnss of Siral alaxis wih Rdshifs z ~., Phys. L. B 699, -9. [9] S.-C. Su and.-c. Chu. Is h univrs roaing? Asrohysial Journal, 7 5. doi:.88/- 67X/7//5. [] Sidharh,B... Is h Univrs Roaing? Prsaim Journal. Oobr, Vol., Issu 7, []. Kajari al. Roaion in rlaiviy and h roagaion of ligh. Prodings of h Inrnaional Shool of Physis "nrio Frmi", Cours CLXVIII,. 5-8 (9) [] Isvan Nmi al. Visualizing idas abou odl-y roaing univrss. odl-y Saims: isory and Nw Dvlomns. (9) [] arlo Samul Brman. A nral Rlaivisi Roaing voluionary Univrs. Asrohys. Sa Si.:9-,8 []. Chalin al. Tommy old Rvisid: Why Dos No Th Univrs Roa? AIP Conf.Pro.8:6-65, 6. h://arxiv.org/abs/asro-h/59. [5] Robr V nry. Nw Cosmi Cnr Univrs odl ahs igh of Big Bang's ajor Prdiions Wihou Th F-L Paradigm. CRN rrin, XT--, Ar. [6] Kur odl. Roaing Univrss in nral Rlaiviy Thory. Prodings of h inrnaional Congrss of ahmaiians in Cambridg, : 75-8, 95. [7] Dmiri Rabounski. On h Sd of Roaion of Isoroi Sa: Insigh ino h Rdshif Problm. Th Abraham Zlmanov Journal, Vol., 9, 8-. [8] auro Dorao. On boming osmi im and roaing univrss. Tim, Raliy and xrin (rovisional il), Royal Insiu of Philosohy Sris, Cambridg Univrsiy Prss,. [9] Yuri N. Obukhov. On hysial foundaions and obsrvaional ffs of osmi Roaion. Publishd in Colloquium on Cosmi Roaion, ds. Shrfnr, T. Chrobok and. Shfaa (Wissnshaf und Thnik Vrlag: Brlin, ) h://arxiv.org/abs/asro-h/86v,7augus. [] U.V.S. Sshavaharam, Physis of Roaing and xanding Blak ol Univrs, Progrss in Physis, vol., 7-,. [] U. V. S. Sshavaharam. Th Primordial Cosmi Blak ol and h Cosmi Axis of vil. Inrnaional Journal of Asronomy, (): -7 DOI:.59/j.asronomy.. [] U. V. S. Sshavaharam and S. Lakshminarayana.. Is Plank s onsan a osmologial variabl? Prodings of -nd Inrnaional Confrn on Thorial Physis. osow.. 7. Inrnaional Journal of Asronomy, (): -5 DOI:.59/j.asronomy... U. V. S. Sshavaharam, Prof. S. Lakshminarayana and Prof. B.V.S.T. Sai
12 Aom, Avogadro Numbr and Aomi Cosmology [] U. V. S. Sshavaharam and S. Lakshminarayana.. Quanum hanis, Cosmi Alraion and CB Radiaion. lobal Journal of Sin Fronir Rsarh (A) Vol. Issu,.7, (). [] U. V. S. Sshavaharam and S. Lakshminarayana. Th Rdud Plank s Consan, ah s Prinil, Cosmi Alraion and h Blak ol Univrs. Journal of Physial Sin and Aliaion (A) () () - 7 [5] Abdus Salam. Srong Inraions, raviaion and Cosmology. Publ. in: NATO Advand Sudy Insiu, ri, Jun6-July 6, 97. [6] Salam A, Sivaram C. Srong raviy Aroah o QCD and Confinmn. od. Phys. L., 99, v. A8(), -6. [7] Rami. lmnary Parils as iro-univrss, and Srong Blak-hols : A Bi-Sal Aroah o raviaional and Srong Inraions. Prrin NSF-ITP--9. osd in h arxivs as h -rin hysis/559, and rfrns hrin. [8] U. V. S. Sshavaharam and S. Lakshminarayana, Rol of Avogadro numbr in grand unifiaion. adroni Journal. Vol-, No 5, O. 5. [9] U. V. S. Sshavaharam and S. Lakshminarayana, To onfirm h xisn of aomi graviaional onsan. adroni journal, Vol-, No, Aug. 79. [] U. V. S. Sshavaharam and S. Lakshminarayana.. SUSY and srong nular graviy in (-6) V mass rang. adroni journal, Vol-, No, Jun,.77 [] U. V. S. Sshavaharam and S. Lakshminarayana.. Srong nular graviy - a brif ror. adroni journal, Vol-, No, Aug... [] U. V. S. Sshavaharam and S. Lakshminarayana.. Nulus in Srong nular graviy. Prodings of h DA Sym. on Nul. Phys. 56 ().. [] U. V. S. Sshavaharam and S. Lakshminarayana. Ingral harg SUSY in Srong nular graviy. Prodings of h DA Sym. on Nul. Phys. 56 ().8. [] U. V. S. Sshavaharam and S. Lakshminarayana.. Aom, univrs and h fundamnal inraions. lobal Journal of Sin Fronir Rsarh (A) Vol. Issu 5,., (). [5] U. V. S. Sshavaharam and S. Lakshminarayana.. Alraing univrs and h xanding aom. adroni journal, Vol-5, No,.7. [6] U. V. S. Sshavaharam and S. Lakshminarayana. Pas, rsn and fuur of h Avogadro numbr. lobal Journal of Sin Fronir Rsarh (A) Vol. Issu 7,.7, (). [7] U. V. S. Sshavaharam and S. Lakshminarayana. To undrsand h four osmologial inraions. Inrnaional Journal of Asronomy, (5): 5- DOI:.59/j.asronomy.5.5. [8] U. V. S. Sshavaharam and S. Lakshminarayana. ubbl volum and h fundamnal inraions. Inrnaional Journal of Asronomy, (5): 87- DOI:.59/j.asronomy.5. [9] U. V. S. Sshavaharam and S. Lakshminarayana. olar lron mass and h basis of TO. Journal of Nular and Paril Physis, (6): - DOI:.59/j.jn.6. [5] U. V. S. Sshavaharam, S. Lakshminarayana. Logi Bhind h Squard Avogadro Numbr and SUSY. Inrnaional Journal of Alid and Naural Sins(IJANS) ISSN 9- Vol., Issu, ay, -. [5] N. Bohr. On h Consiuion of Aoms and oluls. (Par- ) Philos. ag. 6, 9 [5] N. Bohr. On h Consiuion of Aoms and oluls. (Par-, Sysms onaining only a Singl Nulus). Philos. ag. 6, 76, 9 [5] J.V. Narlikar, Inroduion o osmology, Cambridg Univ. Prss,, 9. [5] S.N.Bos. Plank s Law and Ligh Quanum yohsis. Zishrif fur Physik, 6, J. Amrian Journal of Physis.Vol. No., 976. Asrohys. Asr. 5, [55] hra J and Rhnbrg. Th isorial dvlomn of Quanum hory. Sringr Vrlog. Char [56] C. L. Bnn al, Nin-Yar Wilkinson irowav Anisoroy Prob (WAP) Obsrvaions: Final as and Rsuls. Submid o Asrohysial Journal Sulmn Sris. h://arxiv.org/abs/.55v. [57] Ad, P. A. R.; Aghanim, N.; Armiag-Calan, C.; al. (Plank Collaboraion). Plank rsuls. I. Ovrviw of rodus and sinifi rsuls ( arh ) Asronomy & Asrohysis (submid). arxiv:.56 (h://arxiv.org/abs/.56). [58] P. J. ohr and B.N. Taylor, CODATA Rommndd Valus of h Fundamnal Physial Consans.7. ://hysis.nis.gov/onsans. [59] ihal O. Dislr al. Th RS Charg Radius of h Proon and Zmah omns. Phys. L.B. 696: - 7, [6] Ingo Sik. On h rms-radius of h roon. Phys.L.B576:6-67, [6] igr and arsdn. On a diffus raion of h arils. Pro. Roy. So., Sr. A 8: 95-5, 99. [6]. Yukawa. On h Inraion of lmnary Parils. Pro. Phys. ah. So. Ja. 7 (8). 95. U. V. S. Sshavaharam, Prof. S. Lakshminarayana and Prof. B.V.S.T. Sai
Inadequacy of Modern Cosmology and Basics of Atomic Cosmology
Inadquay of odrn Cosmology and Basis of Aomi Cosmology U. V.S. Sshavaharam, S. Lakshminarayana and B.V.S.T. Sai Honorary fauly, I-SRV, Alakauri, Hydrabad-5, AP, India. mail: sshavaharam.uvs@gmail.om D.
More informationInadequacy of Hubble-Friedmann Cosmology and the Basics of Stoney Scale Black Hole Cosmology
Rviw Aril 1 4 5 6 7 8 9 1 11 1 1 14 15 16 17 18 19 1 4 5 6 7 8 9 1 4 5 6 7 8 9 4 41 4 4 44 45 46 47 48 49 5 Inadquay of Hubbl-Fridmann Cosmology and h Basis of ony al Blak Hol Cosmology U. V.. shavaharam
More informationUnified Concepts in Cosmic, Atomic and Nuclear Physics. By U. V. S. Seshavatharam, S. Lakshminarayana & B.V.S.T. Sai Andhra University
Global Journal of Sin Fronir sarh Physis and Sa Sin Volum 1 Issu 1 Vrsion 1. Yar Ty : Doubl Blind Pr viwd Inrnaional sarh Journal Publishr: Global Journals In. (US) Onlin ISSN: 49-466 & Prin ISSN: 975-5896
More informationFriedman cosmology: reconsideration and new results
Inrnaional Journal of Asronomy, Asrohysis and a in ; (: 6-6 Publishd onlin May, (h://www.onsinonlin.om/journal/aass Fridman osmology: ronsidraion and nw rsuls U. V.. shavaharam,. Lakshminarayana onorary
More informationIs Red Shift-An Index of Galactic Atomic Light Emission Mechanism?
Inrnaional Journal of Physis,, Vol., No., 9-6 Availabl onlin a h://ubs.siub.o/ij/// Sin and Eduaion Publishing DOI:.69/ij--- Is Rd Shif-An Indx of alai Aoi Ligh Eission hanis? U. V. S. Sshavahara,*, S.
More informationUnderstandingCosmicTemperatureRedshiftGrowthRateandAgeinStoneyScaleBlackHoleCosmology
Global Journal of in Fronir Rsarh: A Physis and pa in Volum Issu Vrsion. Yar Typ : Doubl Blind Pr Rviwd Inrnaional Rsarh Journal Publishr: Global Journals In. (UA Onlin IN: 9-66 & Prin IN: 975-5896 Undrsanding
More informationDecline Curves. Exponential decline (constant fractional decline) Harmonic decline, and Hyperbolic decline.
Dlin Curvs Dlin Curvs ha lo flow ra vs. im ar h mos ommon ools for forasing roduion and monioring wll rforman in h fild. Ths urvs uikly show by grahi mans whih wlls or filds ar roduing as xd or undr roduing.
More informationBasics of Atomic Cosmology - Part-1
Bai of Aomi Comology - Par- U. V. S. Shavaharam, S. Lakhminarayana and B.V.S.T. Sai Honorary fauly, I-SERVE, Alakauri, Hydrabad-5, AP, India. Email: havaharam.uv@gmail.om D. of Nular Phyi, Andhra Univriy,
More informationCritical Review on Cosmologically Strengthening Hydrogen Atom
Fronirs of Asronomy, Asrohysics and Cosmology, 5, Vol., No., 37-4 Availabl onlin a h://ubs.sciub.com/faac///5 cinc and Educaion Publishing DOI:.69/faac---5 Criical Rviw on Cosmologically rnghning Hydrogn
More informationReliability Analysis of a Bridge and Parallel Series Networks with Critical and Non- Critical Human Errors: A Block Diagram Approach.
Inrnaional Journal of Compuaional Sin and Mahmais. ISSN 97-3189 Volum 3, Numr 3 11, pp. 351-3 Inrnaional Rsarh Puliaion Hous hp://www.irphous.om Rliailiy Analysis of a Bridg and Paralll Sris Nworks wih
More informationDouble Slits in Space and Time
Doubl Slis in Sac an Tim Gorg Jons As has bn ror rcnly in h mia, a am l by Grhar Paulus has monsra an inrsing chniqu for ionizing argon aoms by using ulra-shor lasr ulss. Each lasr uls is ffcivly on an
More informationMEM 355 Performance Enhancement of Dynamical Systems A First Control Problem - Cruise Control
MEM 355 Prformanc Enhancmn of Dynamical Sysms A Firs Conrol Problm - Cruis Conrol Harry G. Kwany Darmn of Mchanical Enginring & Mchanics Drxl Univrsiy Cruis Conrol ( ) mv = F mg sinθ cv v +.2v= u 9.8θ
More informationLecture 1: Numerical Integration The Trapezoidal and Simpson s Rule
Lcur : Numrical ngraion Th Trapzoidal and Simpson s Rul A problm Th probabiliy of a normally disribud (man µ and sandard dviaion σ ) vn occurring bwn h valus a and b is B A P( a x b) d () π whr a µ b -
More informationEconomics 302 (Sec. 001) Intermediate Macroeconomic Theory and Policy (Spring 2011) 3/28/2012. UW Madison
Economics 302 (Sc. 001) Inrmdia Macroconomic Thory and Policy (Spring 2011) 3/28/2012 Insrucor: Prof. Mnzi Chinn Insrucor: Prof. Mnzi Chinn UW Madison 16 1 Consumpion Th Vry Forsighd dconsumr A vry forsighd
More informationAdvanced Queueing Theory. M/G/1 Queueing Systems
Advand Quung Thory Ths slds ar rad by Dr. Yh Huang of Gorg Mason Unvrsy. Sudns rgsrd n Dr. Huang's ourss a GMU an ma a sngl mahn-radabl opy and prn a sngl opy of ah sld for hr own rfrn, so long as ah sld
More informationLecture 4: Laplace Transforms
Lur 4: Lapla Transforms Lapla and rlad ransformaions an b usd o solv diffrnial quaion and o rdu priodi nois in signals and imags. Basially, hy onvr h drivaiv opraions ino mulipliaion, diffrnial quaions
More informationA New Wave Equation of the Electron
Journal of Modrn Physis,,, -6 doi:.436/jmp..9 Publishd Onlin Spmbr (hp://www.sirp.org/journal/jmp) A Nw Wav Equaion of h Elron Absra Arbab I. Arbab Dparmn of Physis, Fauly of Sin, Univrsiy of Kharoum,
More informationUNIT #5 EXPONENTIAL AND LOGARITHMIC FUNCTIONS
Answr Ky Nam: Da: UNIT # EXPONENTIAL AND LOGARITHMIC FUNCTIONS Par I Qusions. Th prssion is quivaln o () () 6 6 6. Th ponnial funcion y 6 could rwrin as y () y y 6 () y y (). Th prssion a is quivaln o
More informationOn the Speed of Heat Wave. Mihály Makai
On h Spd of Ha Wa Mihály Maai maai@ra.bm.hu Conns Formulaion of h problm: infini spd? Local hrmal qulibrium (LTE hypohsis Balanc quaion Phnomnological balanc Spd of ha wa Applicaion in plasma ranspor 1.
More informationBoyce/DiPrima 9 th ed, Ch 7.8: Repeated Eigenvalues
Boy/DiPrima 9 h d Ch 7.8: Rpad Eignvalus Elmnary Diffrnial Equaions and Boundary Valu Problms 9 h diion by William E. Boy and Rihard C. DiPrima 9 by John Wily & Sons In. W onsidr again a homognous sysm
More informationA Study of the Solutions of the Lotka Volterra. Prey Predator System Using Perturbation. Technique
Inrnionl hmil orum no. 667-67 Sud of h Soluions of h o Volrr r rdor Ssm Using rurion Thniqu D.Vnu ol Ro * D. of lid hmis IT Collg of Sin IT Univrsi Vishnm.. Indi Y... Thorni D. of lid hmis IT Collg of
More informationAR(1) Process. The first-order autoregressive process, AR(1) is. where e t is WN(0, σ 2 )
AR() Procss Th firs-ordr auorgrssiv procss, AR() is whr is WN(0, σ ) Condiional Man and Varianc of AR() Condiional man: Condiional varianc: ) ( ) ( Ω Ω E E ) var( ) ) ( var( ) var( σ Ω Ω Ω Ω E Auocovarianc
More informationVoltage v(z) ~ E(z)D. We can actually get to this wave behavior by using circuit theory, w/o going into details of the EM fields!
Considr a pair of wirs idal wirs ngh >, say, infinily long olag along a cabl can vary! D olag v( E(D W can acually g o his wav bhavior by using circui hory, w/o going ino dails of h EM filds! Thr
More informationCPSC 211 Data Structures & Implementations (c) Texas A&M University [ 259] B-Trees
CPSC 211 Daa Srucurs & Implmnaions (c) Txas A&M Univrsiy [ 259] B-Trs Th AVL r and rd-black r allowd som variaion in h lnghs of h diffrn roo-o-laf pahs. An alrnaiv ida is o mak sur ha all roo-o-laf pahs
More informationInstitute of Actuaries of India
Insiu of Acuaris of India ubjc CT3 Probabiliy and Mahmaical aisics Novmbr Examinaions INDICATIVE OLUTION Pag of IAI CT3 Novmbr ol. a sampl man = 35 sampl sandard dviaion = 36.6 b for = uppr bound = 35+*36.6
More informationCharging of capacitor through inductor and resistor
cur 4&: R circui harging of capacior hrough inducor and rsisor us considr a capacior of capacianc is conncd o a D sourc of.m.f. E hrough a rsisr of rsisanc R, an inducor of inducanc and a y K in sris.
More informationSection 4.3 Logarithmic Functions
48 Chapr 4 Sion 4.3 Logarihmi Funions populaion of 50 flis is pd o doul vry wk, lading o a funion of h form f ( ) 50(), whr rprsns h numr of wks ha hav passd. Whn will his populaion rah 500? Trying o solv
More informationRatio-Product Type Exponential Estimator For Estimating Finite Population Mean Using Information On Auxiliary Attribute
Raio-Produc T Exonnial Esimaor For Esimaing Fini Poulaion Man Using Informaion On Auxiliar Aribu Rajsh Singh, Pankaj hauhan, and Nirmala Sawan, School of Saisics, DAVV, Indor (M.P., India (rsinghsa@ahoo.com
More informationAn Indian Journal FULL PAPER. Trade Science Inc. A stage-structured model of a single-species with density-dependent and birth pulses ABSTRACT
[Typ x] [Typ x] [Typ x] ISSN : 974-7435 Volum 1 Issu 24 BioTchnology 214 An Indian Journal FULL PAPE BTAIJ, 1(24), 214 [15197-1521] A sag-srucurd modl of a singl-spcis wih dnsiy-dpndn and birh pulss LI
More informationMidterm exam 2, April 7, 2009 (solutions)
Univrsiy of Pnnsylvania Dparmn of Mahmaics Mah 26 Honors Calculus II Spring Smsr 29 Prof Grassi, TA Ashr Aul Midrm xam 2, April 7, 29 (soluions) 1 Wri a basis for h spac of pairs (u, v) of smooh funcions
More informationLecture 2: Current in RC circuit D.K.Pandey
Lcur 2: urrn in circui harging of apacior hrough Rsisr L us considr a capacior of capacianc is conncd o a D sourc of.m.f. E hrough a rsisr of rsisanc R and a ky K in sris. Whn h ky K is swichd on, h charging
More informationCHAPTER 9 Compressible Flow
CHPTER 9 Corssibl Flow Inrouion 9. v R. kv. R or R k k Rk k Char 9 / Corssibl Flow S of Soun 9.4 Subsiu Eq. 4.5.8 ino Eq. 4.5.7 an ngl onial nrgy hang: Q WS u~ u~. Enhaly is fin in Throynais as h u~ v
More informationIs red shift an index of galactic atomic light emission mechanism?
Inrnaional Journal of Phyi,, Vol., No., 9-6 Availabl onlin a hp://pub.ipub.o/ijp/// Sin and Eduaion Publihing DOI:.69/ijp--- I rd hif an indx of galai aoi ligh iion hani? U. V.S. Shavahara, S. Lakhinarayana
More informationOn the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument
Inrnaional Rsarch Journal of Applid Basic Scincs 03 Aailabl onlin a wwwirjabscom ISSN 5-838X / Vol 4 (): 47-433 Scinc Eplorr Publicaions On h Driais of Bssl Modifid Bssl Funcions wih Rspc o h Ordr h Argumn
More informationMicroscopic Flow Characteristics Time Headway - Distribution
CE57: Traffic Flow Thory Spring 20 Wk 2 Modling Hadway Disribuion Microscopic Flow Characrisics Tim Hadway - Disribuion Tim Hadway Dfiniion Tim Hadway vrsus Gap Ahmd Abdl-Rahim Civil Enginring Dparmn,
More informationChapter 6. PID Control
Char 6 PID Conrol PID Conrol Mo ommon onrollr in h CPI. Cam ino u in 930 wih h inroduion of numai onrollr. Exrmly flxibl and owrful onrol algorihm whn alid rorly. Gnral Fdbak Conrol Loo D G d Y E C U +
More informationTransfer function and the Laplace transformation
Lab No PH-35 Porland Sa Univriy A. La Roa Tranfr funcion and h Laplac ranformaion. INTRODUTION. THE LAPLAE TRANSFORMATION L 3. TRANSFER FUNTIONS 4. ELETRIAL SYSTEMS Analyi of h hr baic paiv lmn R, and
More information4.1 The Uniform Distribution Def n: A c.r.v. X has a continuous uniform distribution on [a, b] when its pdf is = 1 a x b
4. Th Uniform Disribuion Df n: A c.r.v. has a coninuous uniform disribuion on [a, b] whn is pdf is f x a x b b a Also, b + a b a µ E and V Ex4. Suppos, h lvl of unblivabiliy a any poin in a Transformrs
More informationCSE 245: Computer Aided Circuit Simulation and Verification
CSE 45: Compur Aidd Circui Simulaion and Vrificaion Fall 4, Sp 8 Lcur : Dynamic Linar Sysm Oulin Tim Domain Analysis Sa Equaions RLC Nwork Analysis by Taylor Expansion Impuls Rspons in im domain Frquncy
More informationApplied Statistics and Probability for Engineers, 6 th edition October 17, 2016
Applid Saisics and robabiliy for Enginrs, 6 h diion Ocobr 7, 6 CHATER Scion - -. a d. 679.. b. d. 88 c d d d. 987 d. 98 f d.. Thn, = ln. =. g d.. Thn, = ln.9 =.. -7. a., by symmry. b.. d...6. 7.. c...
More informationEstimation of Metal Recovery Using Exponential Distribution
Inrnaional rd Journal o Sinii sarh in Enginring (IJSE).irjsr.om Volum 1 Issu 1 ǁ D. 216 ǁ PP. 7-11 Esimaion o Mal ovry Using Exponnial Disribuion Hüsyin Ankara Dparmn o Mining Enginring, Eskishir Osmangazi
More informationH is equal to the surface current J S
Chapr 6 Rflcion and Transmission of Wavs 6.1 Boundary Condiions A h boundary of wo diffrn mdium, lcromagnic fild hav o saisfy physical condiion, which is drmind by Maxwll s quaion. This is h boundary condiion
More informationEXERCISE - 01 CHECK YOUR GRASP
DIFFERENTIAL EQUATION EXERCISE - CHECK YOUR GRASP 7. m hn D() m m, D () m m. hn givn D () m m D D D + m m m m m m + m m m m + ( m ) (m ) (m ) (m + ) m,, Hnc numbr of valus of mn will b. n ( ) + c sinc
More informationSpring 2006 Process Dynamics, Operations, and Control Lesson 2: Mathematics Review
Spring 6 Procss Dynamics, Opraions, and Conrol.45 Lsson : Mahmaics Rviw. conx and dircion Imagin a sysm ha varis in im; w migh plo is oupu vs. im. A plo migh imply an quaion, and h quaion is usually an
More informationPhys463.nb Conductivity. Another equivalent definition of the Fermi velocity is
39 Anohr quival dfiniion of h Fri vlociy is pf vf (6.4) If h rgy is a quadraic funcion of k H k L, hs wo dfiniions ar idical. If is NOT a quadraic funcion of k (which could happ as will b discussd in h
More informationa dt a dt a dt dt If 1, then the poles in the transfer function are complex conjugates. Let s look at f t H t f s / s. So, for a 2 nd order system:
Undrdamd Sysms Undrdamd Sysms nd Ordr Sysms Ouu modld wih a nd ordr ODE: d y dy a a1 a0 y b f If a 0 0, hn: whr: a d y a1 dy b d y dy y f y f a a a 0 0 0 is h naural riod of oscillaion. is h daming facor.
More informationStability Analysis of Three Species Model in Series Mutualism with Bionomic and Optimal Harvesting of Two Terminal Species
Inrnaional Journal of Sinifi an Innovaiv Mahmaial Rsarh (IJSIMR) Volum, Issu, Dmbr, PP -5 ISS 7-7X (Prin) & ISS 7- (Onlin) www.arjournals.org Sabiliy nalysis of Thr Sis Mol in Sris Muualism wih Bionomi
More information7.4 QUANTUM MECHANICAL TREATMENT OF FLUCTUATIONS *
Andri Tokmakoff, MIT Dparmn of Chmisry, 5/19/5 7-11 7.4 QUANTUM MECANICAL TREATMENT OF FLUCTUATIONS * Inroducion and Prviw Now h origin of frquncy flucuaions is inracions of our molcul (or mor approprialy
More information5. An object moving along an x-coordinate axis with its scale measured in meters has a velocity of 6t
AP CALCULUS FINAL UNIT WORKSHEETS ACCELERATION, VELOCTIY AND POSITION In problms -, drmin h posiion funcion, (), from h givn informaion.. v (), () = 5. v ()5, () = b g. a (), v() =, () = -. a (), v() =
More information2.1. Differential Equations and Solutions #3, 4, 17, 20, 24, 35
MATH 5 PS # Summr 00.. Diffrnial Equaions and Soluions PS.# Show ha ()C #, 4, 7, 0, 4, 5 ( / ) is a gnral soluion of h diffrnial quaion. Us a compur or calculaor o skch h soluions for h givn valus of h
More informationFinal Exam : Solutions
Comp : Algorihm and Daa Srucur Final Exam : Soluion. Rcuriv Algorihm. (a) To bgin ind h mdian o {x, x,... x n }. Sinc vry numbr xcp on in h inrval [0, n] appar xacly onc in h li, w hav ha h mdian mu b
More informationFirst Lecture of Machine Learning. Hung-yi Lee
Firs Lcur of Machin Larning Hung-yi L Larning o say ys/no Binary Classificaion Larning o say ys/no Sam filring Is an -mail sam or no? Rcommndaion sysms rcommnd h roduc o h cusomr or no? Malwar dcion Is
More informationWave Equation (2 Week)
Rfrnc Wav quaion ( Wk 6.5 Tim-armonic filds 7. Ovrviw 7. Plan Wavs in Losslss Mdia 7.3 Plan Wavs in Loss Mdia 7.5 Flow of lcromagnic Powr and h Poning Vcor 7.6 Normal Incidnc of Plan Wavs a Plan Boundaris
More informationOption Pricing When Changes of the Underlying Asset Prices Are Restricted
Journal of Mahmaial Finan 8-33 doi:.436/jmf..4 Publishd Onlin Augus (hp://www.sirp.org/journal/jmf) Opion Priing Whn Changs of h Undrling Ass Pris Ar Rsrid Absra Gorg J. Jiang Guanzhong Pan Li Shi 3 Univrsi
More information2. The Laplace Transform
Th aac Tranorm Inroucion Th aac ranorm i a unamna an vry uu oo or uying many nginring robm To in h aac ranorm w conir a comx variab σ, whr σ i h ra ar an i h imaginary ar or ix vau o σ an w viw a a oin
More informationCHAPTER CHAPTER14. Expectations: The Basic Tools. Prepared by: Fernando Quijano and Yvonn Quijano
Expcaions: Th Basic Prpard by: Frnando Quijano and Yvonn Quijano CHAPTER CHAPTER14 2006 Prnic Hall Businss Publishing Macroconomics, 4/ Olivir Blanchard 14-1 Today s Lcur Chapr 14:Expcaions: Th Basic Th
More informationLet s look again at the first order linear differential equation we are attempting to solve, in its standard form:
Th Ingraing Facor Mhod In h prvious xampls of simpl firs ordr ODEs, w found h soluions by algbraically spara h dpndn variabl- and h indpndn variabl- rms, and wri h wo sids of a givn quaion as drivaivs,
More informationMath 3301 Homework Set 6 Solutions 10 Points. = +. The guess for the particular P ( ) ( ) ( ) ( ) ( ) ( ) ( ) cos 2 t : 4D= 2
Mah 0 Homwork S 6 Soluions 0 oins. ( ps) I ll lav i o you o vrify ha y os sin = +. Th guss for h pariular soluion and is drivaivs is blow. Noi ha w ndd o add s ono h las wo rms sin hos ar xaly h omplimnary
More informationLecture 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 informationBoyce/DiPrima 9 th ed, Ch 2.1: Linear Equations; Method of Integrating Factors
Boc/DiPrima 9 h d, Ch.: Linar Equaions; Mhod of Ingraing Facors Elmnar Diffrnial Equaions and Boundar Valu Problms, 9 h diion, b William E. Boc and Richard C. DiPrima, 009 b John Wil & Sons, Inc. A linar
More informationwhereby we can express the phase by any one of the formulas cos ( 3 whereby we can express the phase by any one of the formulas
Third In-Class Exam Soluions Mah 6, Profssor David Lvrmor Tusday, 5 April 07 [0] Th vrical displacmn of an unforcd mass on a spring is givn by h 5 3 cos 3 sin a [] Is his sysm undampd, undr dampd, criically
More informationN. G. Mensah Department of Mathematics and Statistics, University of Cape Coast, Ghana
AMPFCAON OF ACOUSC WAE N GaN N HE PRESENCE OF SOWY CHANGNG PEROC EECRC FE N. G. Mnsah armn of Mahmais and Saisis, Univrsiy of Ca Coas, Ghana Absra: Aousi wav roagaion in bulk GaN Smionduor in h rsn of
More information10. If p and q are the lengths of the perpendiculars from the origin on the tangent and the normal to the curve
0. If p and q ar h lnghs of h prpndiculars from h origin on h angn and h normal o h curv + Mahmaics y = a, hn 4p + q = a a (C) a (D) 5a 6. Wha is h diffrnial quaion of h family of circls having hir cnrs
More informationUNSTEADY FLOW OF A FLUID PARTICLE SUSPENSION BETWEEN TWO PARALLEL PLATES SUDDENLY SET IN MOTION WITH SAME SPEED
006-0 Asian Rsarch Publishing work (ARP). All righs rsrvd. USTEADY FLOW OF A FLUID PARTICLE SUSPESIO BETWEE TWO PARALLEL PLATES SUDDELY SET I MOTIO WITH SAME SPEED M. suniha, B. Shankr and G. Shanha 3
More information( ) ( ) + = ( ) + ( )
Mah 0 Homwork S 6 Soluions 0 oins. ( ps I ll lav i o you vrify ha h omplimnary soluion is : y ( os( sin ( Th guss for h pariular soluion and is drivaivs ar, +. ( os( sin ( ( os( ( sin ( Y ( D 6B os( +
More informationI) Title: Rational Expectations and Adaptive Learning. II) Contents: Introduction to Adaptive Learning
I) Til: Raional Expcaions and Adapiv Larning II) Conns: Inroducion o Adapiv Larning III) Documnaion: - Basdvan, Olivir. (2003). Larning procss and raional xpcaions: an analysis using a small macroconomic
More informationLecture 14 (Oct. 30, 2017)
Ltur 14 8.31 Quantum Thory I, Fall 017 69 Ltur 14 (Ot. 30, 017) 14.1 Magnti Monopols Last tim, w onsidrd a magnti fild with a magnti monopol onfiguration, and bgan to approah dsribing th quantum mhanis
More informationElementary Differential Equations and Boundary Value Problems
Elmnar Diffrnial Equaions and Boundar Valu Problms Boc. & DiPrima 9 h Ediion Chapr : Firs Ordr Diffrnial Equaions 00600 คณ ตศาสตร ว ศวกรรม สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา /55 ผศ.ดร.อร ญญา ผศ.ดร.สมศ
More information1. Inverse Matrix 4[(3 7) (02)] 1[(0 7) (3 2)] Recall that the inverse of A is equal to:
Rfrncs Brnank, B. and I. Mihov (1998). Masuring monary policy, Quarrly Journal of Economics CXIII, 315-34. Blanchard, O. R. Proi (00). An mpirical characrizaion of h dynamic ffcs of changs in govrnmn spnding
More informationDEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018
DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS Aoc. Prof. Dr. Burak Kllci Spring 08 OUTLINE Th Laplac Tranform Rgion of convrgnc for Laplac ranform Invr Laplac ranform Gomric valuaion
More information2. Transfer function. Kanazawa University Microelectronics Research Lab. Akio Kitagawa
. ransfr funion Kanazawa Univrsiy Mirolronis Rsarh Lab. Akio Kiagawa . Wavforms in mix-signal iruis Configuraion of mix-signal sysm x Digial o Analog Analog o Digial Anialiasing Digial moohing Filr Prossor
More informationLogistic equation of Human population growth (generalization to the case of reactive environment).
Logisic quaion of Human populaion growh gnralizaion o h cas of raciv nvironmn. Srg V. Ershkov Insiu for Tim aur Exploraions M.V. Lomonosov's Moscow Sa Univrsi Lninski gor - Moscow 999 ussia -mail: srgj-rshkov@andx.ru
More information= x. I (x,y ) Example: Translation. Operations depend on pixel s Coordinates. Context free. Independent of pixel values. I(x,y) Forward mapping:
Gomric Transormaion Oraions dnd on il s Coordinas. Con r. Indndn o il valus. (, ) ' (, ) ' I (, ) I ' ( (, ), ( ) ), (,) (, ) I(,) I (, ) Eaml: Translaion (, ) (, ) (, ) I(, ) I ' Forward Maing Forward
More informationPoisson process Markov process
E2200 Quuing hory and lraffic 2nd lcur oion proc Markov proc Vikoria Fodor KTH Laboraory for Communicaion nwork, School of Elcrical Enginring 1 Cour oulin Sochaic proc bhind quuing hory L2-L3 oion proc
More information16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 7: Convective Heat Transfer: Reynolds Analogy
6.5, ok Propulsion Prof. Manul Marinz-Sanhz Lur 7: Conviv Ha Transfr: ynolds Analogy Ha Transfr in ok Nozzls Gnral Ha ransfr o alls an aff a rok in a las o ays: (a) duing h prforman. This nds o b a -3%
More informationChapter 5 The Laplace Transform. x(t) input y(t) output Dynamic System
EE 422G No: Chapr 5 Inrucor: Chung Chapr 5 Th Laplac Tranform 5- Inroducion () Sym analyi inpu oupu Dynamic Sym Linar Dynamic ym: A procor which proc h inpu ignal o produc h oupu dy ( n) ( n dy ( n) +
More informationLecture 1: Growth and decay of current in RL circuit. Growth of current in LR Circuit. D.K.Pandey
cur : Growh and dcay of currn in circui Growh of currn in Circui us considr an inducor of slf inducanc is conncd o a DC sourc of.m.f. E hrough a rsisr of rsisanc and a ky K in sris. Whn h ky K is swichd
More informationPhysics 160 Lecture 3. R. Johnson April 6, 2015
Physics 6 Lcur 3 R. Johnson April 6, 5 RC Circui (Low-Pass Filr This is h sam RC circui w lookd a arlir h im doma, bu hr w ar rsd h frquncy rspons. So w pu a s wav sad of a sp funcion. whr R C RC Complx
More informationA MATHEMATICAL MODEL FOR NATURAL COOLING OF A CUP OF TEA
MTHEMTICL MODEL FOR NTURL COOLING OF CUP OF TE 1 Mrs.D.Kalpana, 2 Mr.S.Dhvarajan 1 Snior Lcurr, Dparmn of Chmisry, PSB Polychnic Collg, Chnnai, India. 2 ssisan Profssor, Dparmn of Mahmaics, Dr.M.G.R Educaional
More informationUtilizing exact and Monte Carlo methods to investigate properties of the Blume Capel Model applied to a nine site lattice.
Utilizing xat and Mont Carlo mthods to invstigat proprtis of th Blum Capl Modl applid to a nin sit latti Nik Franios Writing various xat and Mont Carlo omputr algorithms in C languag, I usd th Blum Capl
More informationA THREE COMPARTMENT MATHEMATICAL MODEL OF LIVER
A THREE COPARTENT ATHEATICAL ODEL OF LIVER V. An N. Ch. Paabhi Ramacharyulu Faculy of ahmaics, R D collgs, Hanamonda, Warangal, India Dparmn of ahmaics, Naional Insiu of Tchnology, Warangal, India E-ail:
More informationVoltage v(z) ~ E(z)D. We can actually get to this wave behavior by using circuit theory, w/o going into details of the EM fields!
Considr a pair of wirs idal wirs ngh >, say, infinily long olag along a cabl can vary! D olag v( E(D W can acually g o his wav bhavior by using circui hory, w/o going ino dails of h EM filds! Thr
More informationCHAPTER 9 Compressible Flow
CHPTER 9 Comrssibl Flow Char 9 / Comrssibl Flow Inroducion 9. c c cv + R. c kcv. c + R or c R k k Rk c k Sd of Sound 9.4 Subsiu Eq. 4.5.8 ino Eq. 4.5.7 and nglc onial nrgy chang: Q WS + + u~ u~. m ρ ρ
More information16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 3: Ideal Nozzle Fluid Mechanics
6.5, Rok ropulsion rof. nul rinz-snhz Lur 3: Idl Nozzl luid hnis Idl Nozzl low wih No Sprion (-D) - Qusi -D (slndr) pproximion - Idl gs ssumd ( ) mu + Opimum xpnsion: - or lss, >, ould driv mor forwrd
More informationCopyright 2012 Pearson Education, Inc. Publishing as Prentice Hall.
Chapr Rviw 0 6. ( a a ln a. This will qual a if an onl if ln a, or a. + k an (ln + c. Thrfor, a an valu of, whr h wo curvs inrsc, h wo angn lins will b prpnicular. 6. (a Sinc h lin passs hrough h origin
More informationChapter 9 Cross-checks on design of tail surfaces ( Lectures 34 to 37)
hapr-9 hapr 9 ross-hks on dsign of ail surfas ( Lurs 34 o 37 Kywords : ross-hks for dsign of ail surfas; loaion of sik-fr nural poin ; lvaor rquird for rim a Lma nar ground and nos whl lif-off ; dsirabl
More informationRecommendation ITU-R S.1857 (01/2010)
Rommndaion TU-R S.857 (0/00 Mhodologis o sima h off-axis.i.r.. dnsiy lvls and o assss h inrfrn owards adjan sallis rsuling from oining rrors of vhil-mound arh saions in h 4 Hz frquny band S Sris Fixd-salli
More informationEconomics 302 (Sec. 001) Intermediate Macroeconomic Theory and Policy (Spring 2011) 4/25/2011. UW Madison
conomics 302 (Sc. 001) Inrmdia Macroconomic Thory and Policy (Spring 2011) 4/25/2011 Insrucor: Prof. Mnzi Chinn Insrucor: Prof. Mnzi Chinn UW Madison 21 1 Th Mdium Run ε = P * P Thr ar wo ways in which
More informationInverse Fourier Transform. Properties of Continuous time Fourier Transform. Review. Linearity. Reading Assignment Oppenheim Sec pp.289.
Convrgnc of ourir Trnsform Rding Assignmn Oppnhim Sc 42 pp289 Propris of Coninuous im ourir Trnsform Rviw Rviw or coninuous-im priodic signl x, j x j d Invrs ourir Trnsform 2 j j x d ourir Trnsform Linriy
More information3(8 ) (8 x x ) 3x x (8 )
Scion - CHATER -. a d.. b. d.86 c d 8 d d.9997 f g 6. d. d. Thn, = ln. =. =.. d Thn, = ln.9 =.7 8 -. a d.6 6 6 6 6 8 8 8 b 9 d 6 6 6 8 c d.8 6 6 6 6 8 8 7 7 d 6 d.6 6 6 6 6 6 6 8 u u u u du.9 6 6 6 6 6
More informationCoherence and interactions in diffusive systems. Cours 4. Diffusion + e-e interations
Cohrnc and inracions in diffusiv sysms G. Monambaux Cours 4 iffusion + - inraions nsiy of sas anomaly phasing du o lcron-lcron inracions Why ar h flucuaions univrsal and wak localizaion is no? ΔG G cl
More information( ) is the stretch factor, and x the
(Lecures 7-8) Liddle, Chaper 5 Simple cosmological models (i) Hubble s Law revisied Self-similar srech of he universe All universe models have his characerisic v r ; v = Hr since only his conserves homogeneiy
More informationPrimordial Hot Evolving Black Holes and the Evolved Primordial Cold Black Hole Universe
Froniers of Asronomy, Asrophysis and Cosmology, 5, Vol., No., 6- Available online a hp://pubs.siepub.om/faa/// Siene and duaion ublishing DOI:.69/faa--- rimordial Ho volving lak Holes and he volved rimordial
More informationPaper Code:MICW-004 I. INTRODUCTION
Par Cod:ICW-4 Oral ANALYSIS OF A LONGITUDINAL RCTANGULAR WAVGUID POWR COBINR FOR TWO DINSIONAL PASD ARRAY APPLICATIONS USING ULTIPL CAVITY ODLING TCNIQU Dbndra Kumar Panda 1 and Aa Chakrabor Darmn of lronis
More informationNon-linear mathematical models for the jets penetrating liquid pool of different density under diverse physical conditions and their simulation
Ian V Kazahko Olxandr V Konoal Non-linar mahmaial modls for h js pnraing liquid pool of diffrn dnsiy undr dirs physial ondiions and hir simulaion IVAN V KAZACHKOV ( ( and OLEXANDER V KONOVAL ( ( Dparmn
More informationShear Wave Propagation in Piezoelectric-Piezoelectric Composite layered structure
483 Shar Wav Propagaion in PizolriPizolri Composi layrd sruur Absra Th propagaion bhavior of ar wav in pizolri omposi sruur is invsigad by wo layr modl prsnd in his approah. Th omposi sruur ompriss of
More informationRobust Control of the Aircraft Attitude
Robus Conrol of h Airraf Aiu F X Wu 1, an W J Zhang Darmn of Mhanial Enginring Univrsiy of Sasahan, Sasaoon, SK S7N 5A9, Canaa Chris_Zhang@EngrUsasCa 1 On h sial laving from Norhsrn Ployhnial Univrsiy,
More information4.3 Design of Sections for Flexure (Part II)
Prsrssd Concr Srucurs Dr. Amlan K Sngupa and Prof. Dvdas Mnon 4. Dsign of Scions for Flxur (Par II) This scion covrs h following opics Final Dsign for Typ Mmrs Th sps for Typ 1 mmrs ar xplaind in Scion
More informationReview Lecture 5. The source-free R-C/R-L circuit Step response of an RC/RL circuit. The time constant = RC The final capacitor voltage v( )
Rviw Lcur 5 Firs-ordr circui Th sourc-fr R-C/R-L circui Sp rspons of an RC/RL circui v( ) v( ) [ v( 0) v( )] 0 Th i consan = RC Th final capacior volag v() Th iniial capacior volag v( 0 ) Volag/currn-division
More information