A novel analytic potential function applied to neutral diatomic molecules and charged lons
|
|
- Griselda Hicks
- 5 years ago
- Views:
Transcription
1 Vol., No., (00 Natual Scic A ovl aalytic pottial fuctio applid to utal diatomic molculs ad chad los Cha-F Yu, Cha-Ju Zhu, Cho-Hui Zha, Li-Xu So, Qiu-Pi Wa Dpatmt of physics, School of Scic, Xi a Polytchic Uivsity, Xi a, Chia; yuh55@6.com Rcivd 4 Novmb 009; visd 8 Jauay 00; accptd 0 Jauay 00. ABSTRACT I this pap, a w mthod o costucti aalytical pottial y fuctios is pstd, ad fom this a aalytical pottial y fuctio applid to both utal diatomic molculs ad chad diatomic molcula ios is obtaid. This pottial y fuctio icluds th dimsiolss udtmid paamts which ca b dtmid uiquly by solvi lia quatios with th xpimtal spctoscopic paamts of molculs. Th solutios of th dimsiolss udtmid paamts a al umbs ath tha complx umbs, this sus that th aalytical pottial y fuctio has xtsiv uivsality. Fially, th pottial y fuctio is xamid with fou kids of diatomic molculs o ios homoucla utal diatomic molcul H(X, K(B u ad Li (B u, homoucla chad diatomic molcula io H (X u, N (X ad O (X, htucla utal diatomic Molcul AlB(A, PuO(X ad NaLi(X, htucla ch- ad diatomic Molcula io BC (X, MH (X ad i,as a cosquc, ood sults a obtaid. Kywods: Diatomic Molculs Ad Ios; Pottial Ey Fuctio; Foc Costats; Spctoscopic Paamts; Phas Facto. INTRODUCTION Aalytical pottial y fuctios a of at siificac i th study of matial scic, molcula spctum, actio dyamics of atoms ad molculs, vibatioal ad otatioal y-lvl stuctus of molculs, itactios btw las ad matt, photoioizatio tc. [-] Du to th impotac ad xtsiv applicatios of th pottial y fuctio, th cospodi sach woks hav b caid o all alo [4-6]. So fa, th pstativ aalytical pottial y fuctio poposd hav Mos pottial [7], Rydb pottial [8], Mull-Sobi pottial (M-S [9] ad Huxly-Mull-Sobi pottial (HMS [0] tc. Rctly, Su Wiuo t al hav poposd a y cosistt mthod (ECM ad costuctd a w physically wll bhavd aalytical pottial fuctio of a diatomic systm calld ECM pottial []. Ths pottial fuctios abov hav mits ad dfcts spctivly, thy a valid i dscibi th bhavios of som idividual o classificatoy diatoms ad molculs. But o of thm ca dscib both utal diatomic molculs ad chad diatomic molcula ios ad dscib pcisly th bhavios of pottial y fuctio ov th whol a of itucla distac. S fom xpssioal foms, most of ths pottial y fuctios adopt th foms of ployomial ad xpotial. I this pap, a cosi fuctio with a phas facto is usd as basic pottial y fuctio ad, thouh omalizatio to th phas facto, a uivsal pottial y fuctio applid to fou kids of diatomic molculs o ios homoucla utal diatomic molculs, homoucla chad diatomic molcula ios, htucla utal diatomic molculs ad htucla chad diatomic molcula ios is iv. Fially, th pottial y fuctio is xamid with twlv difft kids of diatomic molculs ad ios tc., as a cosquc, ood sults a obtaid.. FUNDAMENTAL SUPPOSITIONS, AND DERIVATION OF A UNIVERSAL ANALYTIC POTENTIAL FUNCTION Suppos that th pottial fuctio of diatomic molcula satisfis th followi latio V( Acos ( B ( wh, wh ( accos( / ( A, B a udtmid costats, ( is a Copyiht 00 SciRs.
2 C. F. Yu t al. / Natual Scic ( phas facto latd to, ad th itucla distac, h is quivalt phas diffc btw two itacti atoms, is quilibium itucla distac. Substituti Eq. ito Eq., yilds V( Acos accos( / B A ( / cos / si B ( Eq. is a basic aalytical pottial y fuctio. I od to obtai th uivsal aalytical pottial fuctio of diatomic molculs ad ios, omalizatio should b dd fo th tm i Eq., so as to su that th divativs of ach od of th Eq. a cotiuous ad fiit at quilibium distac. Thus w ca xpad th tm ito biomial sis (i! i ( (4 i i0 4 ( i! (i H, Eq.4 is a ifiit sis, it d to b tucatd ito fiit tms ad its followi ifiit tms should b absobd ito th udtmid cofficits a, b, c, so fom Eq.4, w hav i0 H( i( wh i i0 (i! ( i 4 ( i! (i a( b( 4 (i! H ( i i 4 ( i! (i i a( c( 6 (5 (6 Gally, th pottial y fuctio satisfis asymptotic coditio lim V( 0,so fom Eq. w hav B Asi (7 Substituti Eq.5 ad Eq.7 ito Eq., ad otic H ( 0, yilds A i V ( cos Asi H ( i( i (8 4 6 a( b( c( I Eq.8, th udtmid costat A ca b dtmid accodi to th poptis of pottial y fuctio. At th quilibium distac, th pottial valu is qual to th ativ valu of dissociatio y D, i.. V ( D, ad th fist divativs of V ( with spct to is zo. So fom Eq.8, w obtai V ( Acos Asi H i a b c ( D (9 i dv d A A cos si{ H ( i(i i a ( b( 4 c( 6 0 (0 Fom Eq.9 ad Eq.0, th solutios of A ad cos ca b iv as follows D A si i H( i(i a( b( c( 5 ( cos si{ i H ( i(i a( b ( 4 c( 6} ( Substituti Eq. ad Eq. ito Eq.8, yilds V ( i 4 D H ( i( / a( / b( / i c( 6 c( 6 H ( i(i a( b( 4 i i H ( i(i a( b ( c( 5 ( Eq. is th uivsal aalytical pottial y fuctio that is quid. Th udtmid paamts a, b, c ca b dtmid with th xpimtal spctoscopic paamts (,, B of molculs o fitti mthod usi silpoit pottial y scai. Wh,,, fom Eq.,w hav 4 D ( V a 6a 0b 4c 6 8 b c 4a6b8 c, ( 4 8D ( V 7 40a 56b 7c 8 ( a b c 6 a 8 b 0 c ( (5 Copyiht 00 SciRs.
3 86 C. F. Yu t al. / Natual Scic ( D V ( 9 a 44b 76c a b c 6 5 /8 8a 0b c ( ( a4b60c f X 740a56b7c D 4 400a896b680c f Y 740a56b7c 6D a576b5640c f4 Z 740a56b7c 4D (, ad 98X Y 4Z 80 0 (0. USING EXPERIMENTAL SPECTROSCOPIC PARAMETERS TO DETERMINE a,b,c Th udtmid paamts a, b, c ca b dtmid with th xpimtal spctoscopic paamts (,, B of diatomic molculs o ios. Th picipl of this mthod is, accodi to th latioship btw udtmid paamts ad foc costats, to obtai a, b, c by solvi lia quatios. Fom Eq., th al xpssio of foc costats at th quilibium itucla distac ca b iv as follows [ m m m d V ( V 0 fm [ ( ( ] m m Hi i j d i j 0 ( m! ( m! (5 m! a b c (! (! (5! i wh V 0 H ( i(i a( b( 4 c( 6] i m! ( m,, 4 (7 D H ( i(i a( b( c( 5 (8 Fom Eq.7 ad Eq.8, wh,,, th followi lia quatios ca b obtaid a0b56c f X 6a 0b 4c D a 00b 4c f Y 6a0b4c 6D 4 6a 40b 644c f4 Z 6a0b4c 4D (, ad 6X 5Y 4Z 0 ( a70b056c f X 9 a44b76c D 98 79a60b56c f Y 9 a44b76c 6D a80b648c f4 Z 9 a44b76c 4D (, ad 4X 7Y 4Z 60 0 ( I Eqs.9-, th latioships btw foc costats ad spctoscopic paamts a as follows f f 4 c ( f ( ( 6B f 8 f4 5( (4 6B B Th Eqs.9- abov a all lia quatios, wh th coditios of 6X 5Y 4Z 0, 98X Y 4Z 800ad4X 7Y 4Z 60 0 a satisfid with spct to Eqs.9-, thy hav uiqu al umb solutios fo th udtmid paamts a, b, c. Calculatios show that th coditios abov a always tabl i al. This sus that th aalytical pottial fuctio Eq. has xtsiv uivsality, which ca dscib ay of diatomic molculs ad ios spcially th bhavios of molculs a quilibium itucla distac. So fa, th most xtsivly usd aalytical pottial y fuctio is Mul-Sobi (M-S pottial. Th udtmid paamts i Mul-sobi pottial which a dtmid by xpimtal spctoscopic paamts hav o uiqu solutios ad cotai complx umb solutios. Thus, th M-S pottial is xtmly limitd i applicatios to som diatomic molculs ad ios. [] 4. APPLIED EXAMPLES OF THE UNIVERSAL ANALYTICAL POTENTIAL ENERGY FUNCTION Fo xamii pottial y fuctio Eq., fifty kids of utal diatomic molculs ad chad diatomic Copyiht 00 SciRs.
4 C. F. Yu t al. / Natual Scic ( Tabl. Expimtal spctoscopic paamts of diatomic molculs ad ios. stats / cm / cm B / cm / cm / m D / V Rfs. H(X [] K(B u [4] Li(B u [5] H (X u [6] N (X [4] O (X [7] AlB(A [4] PuO(X [8] NaLi(X [] BC (X [9] MH (X [4] [4] i Tabl. Pottial paamts ad foc costats of diatomic molculs ad ios. stats 4 4 D / V / m. a b c f /0 aj m f /0 aj m f4 /0 aj m H(X K(B u Li(B u H ( X u N (X O (X AlB(A PuO(X NaLi(X BC (X MH (X i Tabl. Pottial paamts of Mul-Sobi pottial of diatomic molculs ad ios. stats a / m a / m a / m / m D / V H(X K(B u Li(B u H ( X u N (X O (X AlB(A PuO(X NaLi(X BC (X MH (X i Copyiht 00 SciRs.
5 88 C. F. Yu t al. / Natual Scic ( Fiu. Pottial cuv of H X. Fiu 4. Pottial cuv of BC (X. u Fiu. Pottial cuv of H ( X Fiu. Pottial cuv of AlB A. molcula ios hav v b ivstiatd ad ood sults a obtaid. Calculatios show that two commo pottial y cuvs, i.. stadystat ad mtastabl stat ca b iv by usi th pottial y fuctio dtmid with xpimtal spctoscopic paamts. Th xpimtal spctoscopic paamts of H(X, H (X u, AlB(A ad BC (X tc. a listd i Tabl. Accodi to Eqs.-4, th cospodi foc costats ca b obtaid by usi th xpimtal spctoscopic paamts abov, ad substituti ths foc costats ito Eq.9 o Eq., th th udtmid paamts a, b, c ca b calculatd by solvi th lia quatios. Th calculatio valus a listd i Tabl. Th pottial y cuvs (to b calculatd ad plottd by usi Eq.4 ad Eq.6 dictly with Oii 7.0 softwa plottd by Eq.4 ad Eq.6 of H(X, H (X u, AlB(A ad BC (X a illustatd i Fius -4. As compaiso, i th Fis., th dot lis a th pottial cuvs which a plottd by usi th most xtsivly usd Mul-Sobi Pottial. Th M-S pottial xpssio is as follows V( D a a xp a a (5 Th latioships btw udtmid paamts of M-S pottial ad foc costats a as follows ( a a f (6 D D D (a a a a 4 a a a 4aa f (7 ( f (8 5.CONCLUSIONS I this pap, w fist itoduc th phas cocpt to th studis of aalytical pottial y fuctios ad t 4 Copyiht 00 SciRs.
6 C. F. Yu t al. / Natual Scic ( ood sults. This shows that th mthod of costucti aalytical pottial y fuctio by mas of phas is ffctiv ad liabl. Compad with oth pottial y fuctios, th pottial y fuctio iv i this pap has two mits: Th udtmid paamt quatios dtmid by xpimtal spctoscopic paamts a lia quatios. Bcaus ths lia quatios hav uiqu al umb solutios, so this pottial y fuctio has a xtsiv uivsality; This pottial y fuctio ca dscib fou difft kids of diatomic molculs o ios homoucla utal diatomic molculs, homoucla chad diatomic molcula ios, htucla utal diatomic molculs ad htucla chad diatomic molcula ios; I additio, This pottial y fuctio ca also dscib accuatly th bhavios of pottial cuvs ov a faily wid a of itucla distac. Pottial y fuctios of diatomic molculs a th basis to th studis of multi-atomic molculs, ios ad clusts, which hav xtmly siificacs ad applid valus i th study of matial scic, molcula spctum chmical actio tc. Chmical actio, molcula collisio ad may oth poblms d pcis aalytical pottial y fuctios. Thus, th studis of aalytical pottial y fuctio will still b impotat subjct i atomic ad molcula physics. REFERENCES [] Yiaopoulou, A., Ju, G.-H., Su, J.P., t al. (999 Pottial-y cuvs fo hihly xcitd lctoic stats i diatomic molculs latd to th atomic obital udulatios [J]. Physical Rviw A, 59(, [] Liu, G.Y., Su, W.G. ad F, H. (004 Studis o th aalytical pottial y fuctio of diatomic molcula Io XY + usi vaiatioal mthod [J]. Scic i Chia (Sis G, 47(, [] Maio, M. ad Acioli, P.H. Full cofiuatio itactio psudopottial dtmiatio of th oud-stat pottial y cuvs of Li ad LiH [J]. Itatioal Joual of Quatum Chmisty, 0(5, [4] Xi, R.H. ad Go, J.B. (005 A Simpl Th- paamt modl pottial fo diatomic systms: Fom wakly ad sto to mtastabl molcula ios [J]. Physical Rviw Ltts, 95, 60. [5] Yu, C.f., Ya, K. ad Liu, D.Z. (006 A uivsal aalytic pottial-y fuctio basd o a phas facto [J]. Acta Mtalluica Sica (Elish Ltts, 9(6, [6] Estvs, C.S., d Olivia, H.C.B., Ribio, L., t al. (006 Modli diatomic pottial y cuvs thouh th alizd xpotial fuctio [J]. Chmical Physics Ltts, 47(, 0-. [7] Mos, P.M. (99 Diatomic molculs accodi to th wav mchaics. Ⅱ. Vibatioal lvls [J]. Physical Rviw Ltts, 4: [8] Rydb, R. (9 Gaphisch Dastllu ii Badsp-ktoskopisch Ebiss [J]. Z Physics, 7: [9] Mul, J.N. ad Sobi, K.S. (974 Nw aalytic fom fo th pottial y cuvs of stabl diatomic stat [J]. Joual of th Chmical Socity, Faaday Tas, II, 70, [0] Huxly, P. ad Mul, J.N. (98 Goud-stat diatomic pottial [J]. Joual of th Chmical Socity, Faaday Tas Ⅱ, 79, -8. [] Su, W.G. ad F, H. (999 A y-cosistt mthod fo pottial y cuvs of diatomic molculs [J]. Joual of Physics B: Atomic, Molcula ad Optical Physics, (, [] Zhu, Z.H. ad Yu, H.G. (997 Molcula stuctu ad molcula pottial y fuctio [M]. Scic Pss, Biji, 8-. [] G, Z.D., Fa, X.W. ad Zha, Y.S. (006 Stuctu ad pottial y fuctio of th oud stat of XY (H, Li, Na.[J] Acta Physica Siica, 55(05, [4] Hzb, G. (98 Molcula spcta ad molcula stuctu (i. spcta of diatomic molculs [M]. Scic Pss, Biji, [5] Yu, B.H., Shi, D.H., Su, J.F., Zhu, Z.L., Liu, Y.F. ad Ya, X.D. (007 Ab iitio Calculatio o Accuat Aalytic Pottial Ey Fuctios ad Hamoic Fqucis of c ad B u Stats of Dim 7Li [J]. Chis Physics, 6(8, [6] Hablad, H., Issdoff, B.V., Fochticht, R., t al. (995 Absoptio Spctoscopy ad Photodissociatio Dyamics of Small Hlium Clust Ios [J] Joual of Chmical Physics, 0(, [7] Savpt, K. ad Mahaja, C.G. (999 Wi hua s fou-paamt pottial commts ad computatio of molcula costats_ ad [J]. Pamaa joual of physics, 5(4, [8] Gao, T., Wa, H.Y., Yi, Y.-G., Ta, M.-L., Zhu, Z.-H., Su, Y., Wa, X.-L. ad Fu, Y.-B. (999 Ab itio calculatio of th pottial y fuctio ad thmodyamic fuctios fo oud stat X of PuO [J]. 5 Acta. Physica Siica, 48(, -7. [9] Tzli, D. ad Mavidis, A. (00 Cotiui ou study o th lctoic stuctu of th cabids BC ad AlC [J]. Joual of Physical Chmisty, A05, Copyiht 00 SciRs.
ENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles
ENGG 03 Tutoial Systms ad Cotol 9 Apil Laig Obctivs Z tasfom Complx pols Fdbac cotol systms Ac: MIT OCW 60, 6003 Diffc Equatios Cosid th systm pstd by th followig diffc quatio y[ ] x[ ] (5y[ ] 3y[ ]) wh
More informationGalaxy Photometry. Recalling the relationship between flux and luminosity, Flux = brightness becomes
Galaxy Photomty Fo galaxis, w masu a sufac flux, that is, th couts i ach pixl. Though calibatio, this is covtd to flux dsity i Jaskys ( Jy -6 W/m/Hz). Fo a galaxy at som distac, d, a pixl of sid D subtds
More informationToday s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom
Today s topic Sttig up th Hydog Ato pobl Hydog ato pobl & Agula Motu Objctiv: to solv Schödig quatio. st Stp: to dfi th pottial fuctio Schatic of Hydog Ato Coulob s aw - Z 4ε 4ε fo H ato Nuclus Z What
More informationCh. 6 Free Electron Fermi Gas
Ch. 6 lcto i Gas Coductio lctos i a tal ov fl without scattig b io cos so it ca b cosidd as if walitactig o f paticls followig idiac statistics. hfo th coductio lctos a fqutl calld as f lcto i gas. Coductio
More informationOn Jackson's Theorem
It. J. Cotm. Math. Scics, Vol. 7, 0, o. 4, 49 54 O Jackso's Thom Ema Sami Bhaya Datmt o Mathmatics, Collg o Educatio Babylo Uivsity, Babil, Iaq mabhaya@yahoo.com Abstact W ov that o a uctio W [, ], 0
More informationELEC9721: Digital Signal Processing Theory and Applications
ELEC97: Digital Sigal Pocssig Thoy ad Applicatios Tutoial ad solutios Not: som of th solutios may hav som typos. Q a Show that oth digital filts giv low hav th sam magitud spos: i [] [ ] m m i i i x c
More informationPhysics 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 informationInstrumentation for Characterization of Nanomaterials (v11) 11. Crystal Potential
Istumtatio o Chaactizatio o Naomatials (v). Cystal Pottial Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio om cystal. Idal cystals a iiit this, so th will b som iiitis lii
More informationand integrated over all, the result is f ( 0) ] //Fourier transform ] //inverse Fourier transform
NANO 70-Nots Chapt -Diactd bams Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio. Idal cystals a iiit this, so th will b som iiitis lii about. Usually, th iiit quatity oly ists
More informationDESIGN AND ANALYSIS OF HORN ANTENNA AND ITS ARRAYS AT C BAND
Itatioal Joual of lctoics, Commuicatio & Istumtatio giig Rsach ad Dvlopmt (IJCIRD) ISS(P): 49-684X; ISS(): 49-795 Vol. 5, Issu 5, Oct 5, -4 TJPRC Pvt. Ltd. DSIG AD AALYSIS OF HOR ATA AD ITS ARRAYS AT C
More informationBayesian Estimations on the Burr Type XII Distribution Using Grouped and Un-grouped Data
Austalia Joual of Basic ad Applid Scics, 5(6: 525-53, 20 ISSN 99-878 Baysia Estimatios o th Bu Typ XII Distibutio Usig Goupd ad U-goupd Data Ima Mahdoom ad Amollah Jafai Statistics Dpatmt, Uivsity of Payam
More informationChapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is
Chapt Solutios. Th wavlgth of th pak is pic 3.898 K T 3.898 K 373K 885 This cospods to ifad adiatio.. Th tpatu is foud with 3.898 K pic T 3 9.898 K 50 T T 5773K 3. Th pow is 4 4 ( 0 ) P σ A T T ( ) ( )
More informationChaos and Correlation
Chaos ad Colatio May, Chaos ad Colatio Itatioal Joual, Mayl, Ядерные оболочки и периодический закон Менделеева Nucli shlls ad piodic tds Alxad P. Tuv (Tooto, Caada) Alxad P. Tuv На основе теории ядерных
More informationThe Hydrogen Atom. Chapter 7
Th Hyog Ato Chapt 7 Hyog ato Th vy fist pobl that Schöig hislf tackl with his w wav quatio Poucig th oh s gy lvls a o! lctic pottial gy still plays a ol i a subatoic lvl btw poto a lcto V 4 Schöig q. fo
More informationRelation between wavefunctions and vectors: In the previous lecture we noted that:
Rlatio tw wavuctios a vctos: I th pvious lctu w ot that: * Ψm ( x) Ψ ( x) x Ψ m Ψ m which claly mas that th commo ovlap itgal o th lt must a i pouct o two vctos. I what ss is ca w thi o th itgal as th
More informationz 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z
Sris Expasio of Rciprocal of Gamma Fuctio. Fuctios with Itgrs as Roots Fuctio f with gativ itgrs as roots ca b dscribd as follows. f() Howvr, this ifiit product divrgs. That is, such a fuctio caot xist
More information2011 HSC Mathematics Extension 1 Solutions
0 HSC Mathmatics Etsio Solutios Qustio, (a) A B 9, (b) : 9, P 5 0, 5 5 7, si cos si d d by th quotit ul si (c) 0 si cos si si cos si 0 0 () I u du d u cos d u.du cos (f) f l Now 0 fo all l l fo all Rag
More informationA New Method of Estimating Wave Energy from Ground Vibrations
Gomatials, 215, 5, 45-55 Publishd Oli Apil 215 i SciRs. http://www.scip.o/joual/m http://dx.doi.o/1.4236/m.215.525 A Nw Mthod of stimati Wav fom Goud Vibatios K. Ram Chada *, V. R. Sast Dpatmt of Mii ii,
More informationA A A. p mu E mc K mc E p c m c. = d /dk. c = 3.00 x 10 8 m/s e = 1.60 x C 1 ev = 1.60 x J 1 Å = m M Sun = 2 x kg
Physics 9HE-Mod Physics Fial Examiatio Mach 1, 14 (1 poits total) You may ta off this sht. ---------------------------------------------------------------------------------------------- Miscllaous data
More informationRADIO-FREQUENCY WALL CONDITIONING FOR STEADY-STATE STELLARATORS
RAIO-FREQUENCY WALL CONIIONING FOR SEAY-SAE SELLARAORS Yu. S. Kulyk, V.E.Moisko,. Wauts, A.I.Lyssoiva Istitut of Plasma Physics, Natioal Scic Ct Khakiv Istitut of Physics ad chology, 68 Khakiv, Ukai Laboatoy
More informationMagnetic effects and the peculiarity of the electron spin in Atoms
Magtic ffcts ad t pculiaity of t lcto spi i Atos Pit Za Hdik otz Nobl Piz 90 Otto t Nobl 9 Wolfgag Pauli Nobl 95 ctu Nots tuctu of Matt: Atos ad Molculs; W. Ubacs T obital agula otu of a lcto i obit iclassical
More informationGRAVITATION. (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 information5.61 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 informationSession : Plasmas in Equilibrium
Sssio : Plasmas i Equilibrium Ioizatio ad Coductio i a High-prssur Plasma A ormal gas at T < 3000 K is a good lctrical isulator, bcaus thr ar almost o fr lctros i it. For prssurs > 0.1 atm, collisio amog
More informationDiscrete Fourier Transform (DFT)
Discrt Fourir Trasorm DFT Major: All Egirig Majors Authors: Duc guy http://umricalmthods.g.us.du umrical Mthods or STEM udrgraduats 8/3/29 http://umricalmthods.g.us.du Discrt Fourir Trasorm Rcalld th xpotial
More informationCHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method
CHAPTER 5 : SERIES 5.1 Seies 5. The Sum of a Seies 5..1 Sum of Powe of Positive Iteges 5.. Sum of Seies of Patial Factio 5..3 Diffeece Method 5.3 Test of covegece 5.3.1 Divegece Test 5.3. Itegal Test 5.3.3
More informationInfinite Series and Improper Integrals
8 Special Fuctios Ifiite Series ad Improper Itegrals Ifiite series are importat i almost all areas of mathematics ad egieerig I additio to umerous other uses, they are used to defie certai fuctios ad to
More informationMolecules 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 informationCMF Signal Processing Method Based on Feedback Corrected ANF and Hilbert Transformation
.478/ms-4-7 MESUREMENT SCIENCE REVIEW, Volum 4, No., 4 CMF Sigal Pocssig Mthod Basd o Fdbac Coctd NF ad Hilbt Tasfomatio Yaqig Tu, Huiyu Yag, Haitao Zhag, Xiagyu Liu Logistical Egiig Uivsity, Chogqig 43,
More informationThe tight-binding method
Th tight-idig thod Wa ottial aoach: tat lcto a a ga of aly f coductio lcto. ow aout iulato? ow aout d-lcto? d Tight-idig thod: gad a olid a a collctio of wa itactig utal ato. Ovla of atoic wav fuctio i
More informationStudy of the Balance for the DHS Distribution
Itatioal Mathmatical Foum, Vol. 7, 01, o. 3, 1553-1565 Study of th Balac fo th Distibutio S. A. El-Shhawy Datmt of Mathmatics, Faculty of scic Moufiya Uivsity, Shbi El-Kom, Egyt Cut addss: Datmt of Mathmatics,
More informationE 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 informationPotential Energy of the Electron in a Hydrogen Atom and a Model of a Virtual Particle Pair Constituting the Vacuum
Applid Physics Rsach; Vol 1, No 4; 18 ISSN 1916-9639 -ISSN 1916-9647 Publishd by Caadia Ct of Scic ad ducatio Pottial gy of th lcto i a Hydog Atom ad a Modl of a Vitual Paticl Pai Costitutig th Vacuum
More informationSUPPLEMENTARY 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 informationShor 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 informationAakash. 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 informationChapter 11.00C Physical Problem for Fast Fourier Transform Civil Engineering
haptr. Physical Problm for Fast Fourir Trasform ivil Egirig Itroductio I this chaptr, applicatios of FFT algorithms [-5] for solvig ral-lif problms such as computig th dyamical (displacmt rspos [6-7] of
More informationSTATISTICAL 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 informationOn the approximation of the constant of Napier
Stud. Uiv. Babş-Bolyai Math. 560, No., 609 64 O th approximatio of th costat of Napir Adri Vrscu Abstract. Startig from som oldr idas of [] ad [6], w show w facts cocrig th approximatio of th costat of
More information( ) L = D e. e e. Example:
xapl: A Si p juctio diod av acoss sctioal aa of, a accpto coctatio of 5 0 8 c -3 o t p-sid ad a doo coctatio of 0 6 c -3 o t -sid. T lif ti of ols i -gio is 47 s ad t lif ti of lctos i t p-gio is 5 s.
More informationAdvanced Higher Formula List
Advaced Highe Fomula List Note: o fomulae give i eam emembe eveythig! Uit Biomial Theoem Factoial! ( ) ( ) Biomial Coefficiet C!! ( )! Symmety Idetity Khayyam-Pascal Idetity Biomial Theoem ( y) C y 0 0
More informationThe Real Hydrogen Atom
T Ra Hydog Ato ov ad i fist od gt iddt of :.6V a us tubatio toy to dti: agti ffts si-obit ad yfi -A ativisti otios Aso av ab sift du to to sfitatio. Nd QD Dia q. ad dds o H wavfutio at sou of ti fid. Vy
More informationDielectric Waveguide 1
Dilctic Wavgui Total Ital Rflctio i c si c t si si t i i i c i Total Ital Rflctio i c i cos si Wh i t i si c si cos t j o cos t t o si i si bcoms pul imagia pul imagia i, al Total Ital Rflctio 3 i c i
More informationLow-Frequency Full-Wave Finite Element Modeling Using the LU Recombination Method
33 CES JOURNL, OL. 23, NO. 4, DECEMBER 28 Low-Fqucy Fu-Wav Fiit Elmt Modlig Usig th LU Rcombiatio Mthod H. K ad T. H. Hubig Dpatmt of Elctical ad Comput Egiig Clmso Uivsity Clmso, SC 29634 bstact I this
More information(Reference: sections in Silberberg 5 th ed.)
ALE. Atomic Structur Nam HEM K. Marr Tam No. Sctio What is a atom? What is th structur of a atom? Th Modl th structur of a atom (Rfrc: sctios.4 -. i Silbrbrg 5 th d.) Th subatomic articls that chmists
More informationFI 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 informationQ 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 information1985 AP Calculus BC: Section I
985 AP Calculus BC: Sctio I 9 Miuts No Calculator Nots: () I this amiatio, l dots th atural logarithm of (that is, logarithm to th bas ). () Ulss othrwis spcifid, th domai of a fuctio f is assumd to b
More informationThe Simplest Proofs of Both Arbitrarily Long. Arithmetic Progressions of primes. Abstract
The Simplest Proofs of Both Arbitrarily Lo Arithmetic Proressios of primes Chu-Xua Jia P. O. Box 94, Beiji 00854 P. R. Chia cxjia@mail.bcf.et.c Abstract Usi Jia fuctios J ( ω ), J ( ω ) ad J ( ) 4 ω we
More informationBohr 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 informationPH672 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 informationChapter 2 Reciprocal Lattice. An important concept for analyzing periodic structures
Chpt Rcpocl Lttc A mpott cocpt o lyzg podc stuctus Rsos o toducg cpocl lttc Thoy o cystl dcto o x-ys, utos, d lctos. Wh th dcto mxmum? Wht s th tsty? Abstct study o uctos wth th podcty o Bvs lttc Fou tsomto.
More informationExtinction 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 informationComparing convolution-integral models with analytical pipe- flow solutions
Joual of Physics: Cofc Sis PAPE OPEN ACCESS Compaig covolutio-itgal modls with aalytical pip- flow solutios To cit this aticl: K Ubaowicz t al 6 J. Phys.: Cof. S. 76 6 Viw th aticl oli fo updats ad hacmts.
More informationCDS 101: Lecture 5.1 Reachability and State Space Feedback
CDS, Lctur 5. CDS : Lctur 5. Rachability ad Stat Spac Fdback Richard M. Murray ad Hido Mabuchi 5 Octobr 4 Goals: Di rachability o a cotrol systm Giv tsts or rachability o liar systms ad apply to ampls
More informationPURE MATHEMATICS A-LEVEL PAPER 1
-AL P MATH PAPER HONG KONG EXAMINATIONS AUTHORITY HONG KONG ADVANCED LEVEL EXAMINATION PURE MATHEMATICS A-LEVEL PAPER 8 am am ( hours) This papr must b aswrd i Eglish This papr cosists of Sctio A ad Sctio
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More information( ) 1 Comparison Functions. α is strictly increasing since ( r) ( r ) α = for any positive real number c. = 0. It is said to belong to
Compaiso Fuctios I this lesso, we study stability popeties of the oautoomous system = f t, x The difficulty is that ay solutio of this system statig at x( t ) depeds o both t ad t = x Thee ae thee special
More informationLECTURE 13 Filling the bands. Occupancy of Available Energy Levels
LUR 3 illig th bads Occupacy o Availabl rgy Lvls W hav dtrmid ad a dsity o stats. W also d a way o dtrmiig i a stat is illd or ot at a giv tmpratur. h distributio o th rgis o a larg umbr o particls ad
More informationConditional Convergence of Infinite Products
Coditioal Covegece of Ifiite Poducts William F. Tech Ameica Mathematical Mothly 106 1999), 646-651 I this aticle we evisit the classical subject of ifiite poducts. Fo stadad defiitios ad theoems o this
More informationphysicsandmathstutor.com
physicsadmathstuto.com physicsadmathstuto.com Jue 005 5x 3 3. (a) Expess i patial factios. (x 3)( x ) (3) (b) Hece fid the exact value of logaithm. 6 5x 3 dx, givig you aswe as a sigle (x 3)( x ) (5) blak
More informationWorksheet: Taylor Series, Lagrange Error Bound ilearnmath.net
Taylor s Thorm & Lagrag Error Bouds Actual Error This is th ral amout o rror, ot th rror boud (worst cas scario). It is th dirc btw th actual () ad th polyomial. Stps:. Plug -valu ito () to gt a valu.
More informationLectures 9 IIR Systems: First Order System
EE3054 Sigals ad Systms Lcturs 9 IIR Systms: First Ordr Systm Yao Wag Polytchic Uivrsity Som slids icludd ar xtractd from lctur prstatios prpard by McCllla ad Schafr Lics Ifo for SPFirst Slids This work
More informationCHAPTER 5. Theory and Solution Using Matrix Techniques
A SERIES OF CLASS NOTES FOR 2005-2006 TO INTRODUCE LINEAR AND NONLINEAR PROBLEMS TO ENGINEERS, SCIENTISTS, AND APPLIED MATHEMATICIANS DE CLASS NOTES 3 A COLLECTION OF HANDOUTS ON SYSTEMS OF ORDINARY DIFFERENTIAL
More informationWhat Makes Production System Design Hard?
What Maks Poduction Systm Dsign Had? 1. Things not always wh you want thm whn you want thm wh tanspot and location logistics whn invntoy schduling and poduction planning 2. Rsoucs a lumpy minimum ffctiv
More informationThe calculation method for SNE
Elctroic Supplmtary Matrial (ESI) for RSC Advacs. This joural is Th Royal Socity of Chmistry 015 Th ulatio mthod for SNE (1) Slct o isothrm ad o rror fuctio (for xampl, th ERRSQ rror fuctio) ad gt th solvr
More information07 - SEQUENCES AND SERIES Page 1 ( Answers at he end of all questions ) b, z = n
07 - SEQUENCES AND SERIES Pag ( Aswrs at h d of all qustios ) ( ) If = a, y = b, z = c, whr a, b, c ar i A.P. ad = 0 = 0 = 0 l a l
More informationQ 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 informationProgression. CATsyllabus.com. CATsyllabus.com. Sequence & Series. Arithmetic Progression (A.P.) n th term of an A.P.
Pogessio Sequece & Seies A set of umbes whose domai is a eal umbe is called a SEQUENCE ad sum of the sequece is called a SERIES. If a, a, a, a 4,., a, is a sequece, the the expessio a + a + a + a 4 + a
More informationON EUCLID S AND EULER S PROOF THAT THE NUMBER OF PRIMES IS INFINITE AND SOME APPLICATIONS
Joual of Pue ad Alied Mathematics: Advaces ad Alicatios Volume 0 Numbe 03 Pages 5-58 ON EUCLID S AND EULER S PROOF THAT THE NUMBER OF PRIMES IS INFINITE AND SOME APPLICATIONS ALI H HAKAMI Deatmet of Mathematics
More informationThomas J. Osler. 1. INTRODUCTION. This paper gives another proof for the remarkable simple
5/24/5 A PROOF OF THE CONTINUED FRACTION EXPANSION OF / Thomas J Oslr INTRODUCTION This ar givs aothr roof for th rmarkabl siml cotiud fractio = 3 5 / Hr is ay ositiv umbr W us th otatio x= [ a; a, a2,
More informationStatistics 3858 : Likelihood Ratio for Exponential Distribution
Statistics 3858 : Liklihood Ratio for Expotial Distributio I ths two xampl th rjctio rjctio rgio is of th form {x : 2 log (Λ(x)) > c} for a appropriat costat c. For a siz α tst, usig Thorm 9.5A w obtai
More informationNEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES
Digst Joural of Naomatrials ad Biostructurs Vol 4, No, March 009, p 67-76 NEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES A IRANMANESH a*, O KHORMALI b, I NAJAFI KHALILSARAEE c, B SOLEIMANI
More informationFIXED POINT AND HYERS-ULAM-RASSIAS STABILITY OF A QUADRATIC FUNCTIONAL EQUATION IN BANACH SPACES
IJRRAS 6 () July 0 www.apapess.com/volumes/vol6issue/ijrras_6.pdf FIXED POINT AND HYERS-UAM-RASSIAS STABIITY OF A QUADRATIC FUNCTIONA EQUATION IN BANACH SPACES E. Movahedia Behbaha Khatam Al-Abia Uivesity
More informationPrevious knowlegde required. Spherical harmonics and some of their properties. Angular momentum. References. Angular momentum operators
// vious owg ui phica haoics a so o thi poptis Goup thoy Quatu chaics pctoscopy H. Haga 8 phica haoics Rcs Bia. iv «Iucib Tso thos A Itouctio o chists» Acaic ss D.A. c Quai.D. io «hii hysiu Appoch oécuai»
More informationUNIT # 12 (PART - I)
JEE-Pysics od-6\e:\data\\kota\jee-dvacd\smp\py\solutio\uit-9 & \5.Mod Pysics.p65 MODER PHYSICS (tomic ad ucla pysics) EXERCISE I c 6V c. V c. P(D) t /. T, T B ; T +B 6. so, fist alf livs (by ) xt alf livs
More information(5x 7) is. 63(5x 7) 42(5x 7) 50(5x 7) BUSINESS MATHEMATICS (Three hours and a quarter)
BUSINESS MATHEMATICS (Three hours ad a quarter) (The first 5 miutes of the examiatio are for readig the paper oly. Cadidate must NOT start writig durig this time). ------------------------------------------------------------------------------------------------------------------------
More informationSIMULTANEOUS METHODS FOR FINDING ALL ZEROS OF A POLYNOMIAL
Joual of athmatcal Sccs: Advacs ad Applcatos Volum, 05, ags 5-8 SIULTANEUS ETHDS FR FINDING ALL ZERS F A LYNIAL JUN-SE SNG ollg of dc Yos Uvsty Soul Rpublc of Koa -mal: usopsog@yos.ac. Abstact Th pupos
More informationHydrogen 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 informationStudy 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 informationLecture 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 informationStatics. Consider the free body diagram of link i, which is connected to link i-1 and link i+1 by joint i and joint i-1, respectively. = r r r.
Statcs Th cotact btw a mapulato ad ts vomt sults tactv ocs ad momts at th mapulato/vomt tac. Statcs ams at aalyzg th latoshp btw th actuato dv tous ad th sultat oc ad momt appld at th mapulato dpot wh
More informationChapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series
Chatr Ifiit Sris Pag of Sctio F Itgral Tst Chatr : Ifiit Sris By th d of this sctio you will b abl to valuat imror itgrals tst a sris for covrgc by alyig th itgral tst aly th itgral tst to rov th -sris
More informationOn a Problem of Littlewood
Ž. JOURAL OF MATHEMATICAL AALYSIS AD APPLICATIOS 199, 403 408 1996 ARTICLE O. 0149 O a Poblem of Littlewood Host Alze Mosbache Stasse 10, 51545 Waldbol, Gemay Submitted by J. L. Bee Received May 19, 1995
More information15/03/1439. Lectures on Signals & systems Engineering
Lcturs o Sigals & syms Egirig Dsigd ad Prd by Dr. Ayma Elshawy Elsfy Dpt. of Syms & Computr Eg. Al-Azhar Uivrsity Email : aymalshawy@yahoo.com A sigal ca b rprd as a liar combiatio of basic sigals. Th
More informationProblem Session (3) for Chapter 4 Signal Modeling
Pobm Sssio fo Cht Sig Modig Soutios to Pobms....5. d... Fid th Pdé oimtio of scod-od to sig tht is giv by [... ] T i.. d so o. I oth wods usig oimtio of th fom b b b H fid th cofficits b b b d. Soutio
More informationSums of Involving the Harmonic Numbers and the Binomial Coefficients
Ameica Joual of Computatioal Mathematics 5 5 96-5 Published Olie Jue 5 i SciRes. http://www.scip.og/oual/acm http://dx.doi.og/.46/acm.5.58 Sums of Ivolvig the amoic Numbes ad the Biomial Coefficiets Wuyugaowa
More informationJ. Stat. Appl. Pro. Lett. 2, No. 1, (2015) 15
J. Stat. Appl. Pro. Lett. 2, No. 1, 15-22 2015 15 Joural of Statistics Applicatios & Probability Letters A Iteratioal Joural http://dx.doi.org/10.12785/jsapl/020102 Martigale Method for Rui Probabilityi
More information6.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 informationToday s topics. How did we solve the H atom problem? CMF Office Hours
CMF Offc ous Wd. Nov. 4 oo-p Mo. Nov. 9 oo-p Mo. Nov. 6-3p Wd. Nov. 8 :30-3:30 p Wd. Dc. 5 oo-p F. Dc. 7 4:30-5:30 Mo. Dc. 0 oo-p Wd. Dc. 4:30-5:30 p ouly xa o Th. Dc. 3 Today s topcs Bf vw of slctd sults
More informationEE 232 Lightwave Devices Lecture 3: Basic Semiconductor Physics and Optical Processes. Optical Properties of Semiconductors
3 Lightwav Dvics Lctur 3: Basic Smicoductor Physics ad Optical Procsss Istructor: Mig C. Wu Uivrsity of Califoria, Brly lctrical girig ad Computr Scics Dpt. 3 Lctur 3- Optical Proprtis of Smicoductors
More informationDTFT Properties. Example - Determine the DTFT Y ( e ) of n. Let. We can therefore write. From Table 3.1, the DTFT of x[n] is given by 1
DTFT Proprtis Exampl - Dtrmi th DTFT Y of y α µ, α < Lt x α µ, α < W ca thrfor writ y x x From Tabl 3., th DTFT of x is giv by ω X ω α ω Copyright, S. K. Mitra Copyright, S. K. Mitra DTFT Proprtis DTFT
More informationCOMPSCI 230 Discrete Math Trees March 21, / 22
COMPSCI 230 Dict Math Mach 21, 2017 COMPSCI 230 Dict Math Mach 21, 2017 1 / 22 Ovviw 1 A Simpl Splling Chck Nomnclatu 2 aval Od Dpth-it aval Od Badth-it aval Od COMPSCI 230 Dict Math Mach 21, 2017 2 /
More informationSolid 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 informationLecture 24: Observability and Constructibility
ectue 24: Obsevability ad Costuctibility 7 Obsevability ad Costuctibility Motivatio: State feedback laws deped o a kowledge of the cuet state. I some systems, xt () ca be measued diectly, e.g., positio
More informationphysicsandmathstutor.com
physicsadmathstuto.com physicsadmathstuto.com Jue 005. A cuve has equatio blak x + xy 3y + 16 = 0. dy Fid the coodiates of the poits o the cuve whee 0. dx = (7) Q (Total 7 maks) *N03B034* 3 Tu ove physicsadmathstuto.com
More informationDiscrete Fourier Transform. Discrete Fourier Transform. Discrete Fourier Transform. Discrete Fourier Transform. Discrete Fourier Transform
Discrt Fourir Trasform Dfiitio - T simplst rlatio btw a lt- squc x dfid for ω ad its DTFT X ( ) is ω obtaid by uiformly sampli X ( ) o t ω-axis btw ω < at ω From t dfiitio of t DTFT w tus av X X( ω ) ω
More informationImproving the Predictive Capability of Popular SWCCs by Incorporating Maximum Possible Suction
Itatioal Joual of Gocic, 2011, 2, 468-475 doi:10.4236/ijg.2011.24049 Publihd Oli Novb 2011 (http://www.scirp.og/joual/ijg) Ipovig th Pdictiv Capabilit of Popula SWCC b Icopoatig Maxiu Poibl Suctio Abtact
More informationMATH 312 Midterm I(Spring 2015)
MATH 3 Midterm I(Sprig 05) Istructor: Xiaowei Wag Feb 3rd, :30pm-3:50pm, 05 Problem (0 poits). Test for covergece:.. 3.. p, p 0. (coverges for p < ad diverges for p by ratio test.). ( coverges, sice (log
More informationGAUSS 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