Characteristics of a Terrain-Following Sigma Coordinate
|
|
- Eugene Tucker
- 5 years ago
- Views:
Transcription
1 ATMOSPERIC AND OCEANIC SCIENCE LETTERS, 0, VOL. 4, NO., 576 Caractristics of a Trrain-Following Sigma Coordinat LI Yi-Yuan, WANG Bin,, WANG Dong-ai Stat K Laborator of Numrical Modling for Atmospric Scincs Gopsical Fluid Dnamics, Institut of Atmospric Psics, Cins Acadm of Scincs, Bing 0009, Cina Cntr for Eart Sstm Scinc, Tsingua Univrsit, Bing 00084, Cina Stat K Laborator of Svr Watr, Cins Acadm of Mtorological Scincs, Bing 0008, Cina Rcivd Januar 0; rvisd 7 Marc 0; accptd 7 Marc 0; publisd 6 Ma 0 Abstract Tis stud quantifis t main caractristics of a trrain-following, -coordinat troug matmatical analss of its covariant contravariant basis vctors as wll as t vrtical coordinat of. A -D scmatic of t -coordinat in a curvilinar coordinat sstm is providd in tis stud. T caractristics of t basis vctors wr brokn down into tir local vctor caractristics spatial distribution caractristics, t act prssions of t covariant; in addition, t contravariant basis vctors of t -coordinat usd to lucidat tir dtaild caractristics wr proprl solvd. Troug rwriting t prssion of t vrtical coordinat of, a matmatical prssion of all t -coordinat surfacs was found, trb quantifing t socalld trrain-following caractristics lack of flibilit to adjust t slop variation of -coordinat surfacs for t classic dfinition of. Finall, an analsis on t rang valu of t vrtical coordinat dmonstratd tat t gnral valu rang of could b obtaind b liminating t -coordinat surfacs blow t Eart s surfac. All ts quantitativ dscriptions of t caractristics of -coordinat wr t foundation for improving t -coordinat or crating a nw on. Kwords: quantitativ dscription, sigma coordinat, -D scmatic, basis vctors, non-ortogonal Citation: Li, Y.-Y., B. Wang, D.-. Wang, 0: Caractristics of a trrain-following sigma coordinat, Atmos. Ocanic Sci. Ltt., 4, Introduction A trrain-following, -coordinat initiatd b Pillips (957) is widl applid to numrical modls bcaus of its advantag in implmnting boundar conditions. owvr, som caractristics of σ-coordinat, spciall bcaus it is non-ortogonal curvilinar, ar likl to rsult in computational problms in a modl. Clark (977) proposd tat t Cristoffl smbols in t tird momntum quation of t -coordinat aris from t non-ortogonal caractristics, wic brougt about t non-consrvativ problm in a modl. It as bn rportd tat t curvilinar -coordinat surfacs could caus computational rrors in oriontal gradint trms abov stp topograp (Corb t al., 97; Lin, 997; Klmp Skamarock, 00). Stpplr t al. (00) notd tat Corrsponding autor: WANG Bin, wab@lasg.iap.ac.cn t -coordinat was non-ortogonal strongl dformd ovr stp trrain, wic can rsult in a sris of potntial problms, suc as spurious flows. Mor rcntl, Ji t al. (005) pointd out tat analss on problms associatd wit t non-ortogonal caractristic of -coordinat wr still lacking. Altoug t main caractristics of -coordinat would caus a sris of problms in a modl, t wr usuall dscribd in a qualitativ wa, suc as a twodimnsional (-D) scmatic of -coordinat surfacs drawn b Pilk (00) basis vctors at crtain location illustratd b Zdundowski Bott (00b). Morovr, fw studis providd a complt -D scmatic of t -coordinat, littl was don to quantif tos caractristics. W rvisit t main caractristics of t -coordinat in dtail troug a comprnsiv matmatical analsis of spcific prssions of t covariant contravariant basis vctors t vrtical coordinat of. Basd on ts quantitativ analss, fasibl approacs ar proposd in tis stud to improv t trrain-following coordinat to ovrcom its disadvantags. In tis stud, a complt -D scmatic of t -coordinat in a viw of a curvilinar coordinat sstm is prsntd. T caractristics of t basis vctors wr brokn down into two aspcts in addition, matmatical prssions of t covariant contravariant basis vctors of t -coordinat t -coordinat surfacs wr solvd. Basd on ts computations, t dtaild caractristics of t basis vctors wr dtrmind, t caractristics of t -coordinat surfacs wr quantifid, a gnral rang of was validatd. Caractristics of t -coordinat in a -D viw A coordinat sstm is composd of an origin, coordinat as, coordinat lins, coordinat surfacs. Coordinat surfacs ar t surfacs on wic coordinats ar constant, coordinat lins ar t curvs wr two coordinat surfacs intrsct, coordinat as ar tangntial lins of t coordinat lins. Figur provids a -D viw of ts caractristics for t -coordinat, Tabl summaris t caractristics. Basis vctors ar anotr important lmnt of a coordinat sstm wit two dfinitions: t on is tat covariant basis vctors ar tangnt to coordinat lins; t otr
2 58 ATMOSPERIC AND OCEANIC SCIENCE LETTERS VOL. 4 Figur A -D scmatic of coordinat surfacs, coordinat lins, coordinat as of a -coordinat. Rd, ligt-blu, grn ms surfacs rprsnt -, -, -coordinat surfacs, rspctivl. Dark-blu lins ar -, -, -coordinat lins, black arrows rprsnt -, -, -coordinat as. is tat contravariant basis vctors ar normal to t coordinat surfacs (Dutton, 976a). In a -coordinat, t oriontal covariant basis vctors t vrtical contravariant basis vctors var in t oriontal vrtical, rspctivl, wil t covariant contravariant basis vctors ar non-ortogonal wn t igt slop of trrain do not qual ro (Fig. ). Quantifing t caractristics of t -coordinat T covariant contravariant basis vctors of t -coordinat wr solvd t prssion of t vrtical coordinat of was rwrittn in a spcific form to quantif t caractristics of t basis vctors t -coordinat surfacs as wll as to anal t rang valus of. T classic prssions of t -coordinat dfind b Gal-Cn Somrvill (975) av bn usd b man numrical modls, suc as t Rgional Atmospric Modling Sstm (Pilk t al., 99), t Coupld Ocan/Atmospr Msoscal Prdiction Sstm (odur, 997), t Advancd Rgional Prdiction Sstm (Xu t al., 000). T dfinitions of ts classic -coordinat ar usd in t following computation as an ampl:, (), (), () wr ar two oriontal coordinats of t -coordinat, is t vrtical coordinat, is t top of t modl, =(, ) rprsnts t trrain.. Covariant contravariant basis vctors To obtain dtaild caractristics of ts vctors, tir caractristics wr brokn down into two aspcts: () t local vctor caractristics comprising t magnitud dirction of vr basis vctor at crtain location () t spatial distribution caractristics comprising t variation of all t basis vctors according to t oriontal vrtical. Dutton (976b) Pilk (00) solvd basis vctors of a gnralid vrtical coordinat; owvr, t did not prsnt t act prssions in t -coordinat. rin, Eqs. ()() wr usd to solv t covariant contravariant basis vctors of t -coordinat, illustratd b t vrtical coordinat trrain. T dfinitions of covariant contravariant basis vctors ar givn b t following: j i i i j, (4) q i j i j, (5) q wr i =,, or, j is a sum from to, i j ar basis vctors of t Cartsian coordinat, i i ar covariant contravariant basis vctors of t σ-coordinat, rspctivl, j q i ar coordinats in t Cartsian coordinat σ-coordinat, rspctivl. T valus of j i i j q q wr calculatd according to Eqs. ()() pd t summation; t covariant contravariant basis vctors of -coordinat wr tn obtaind as follows: i k, (6) j k, (7) k, (8) =i, (9) =j, (0) i j k, () T rigt- sid (RS) of Eqs. (6)() dmonstratd t spatial distribution caractristics of t basis vctors (Tabls ). Spcificall, wn t vrtical coordinat incrasd, t scond trm on t RS of Eq. (6) Eq. (7) dcrasd, t first trm stad constant; t vrtical componnts of t covariant basis vctors,, dcrasd, wil tir oriontal componnts wr constant, wit t rsult tat bcam flat, according to t igt (Fig. ). In addition, i Tabl Caractristics of t coordinat surfacs, lins, as in a -coordinat. Coordinat surfacs Coordinat lins Coordinat as Vrtical plans Curvilinar surfacs following t trrain Curvilinar lins following t trrain Vrtical lins Tangnt to t trrain at t ground Alwas vrtical
3 NO. LI ET AL.: CARACTERISTICS OF A TERRAIN-FOLLOWING SIGMA COORDINATE 59 Figur A -D scmatic of t basis vctors in a vrtical cross sction of a -coordinat. Growt lins rprsnt -coordinat surfacs, wil blu grn arrows ar covariant contravariant basis vctors of t -coordinat, rspctivl. T black arrows indicat t basis vctors of t Cartsian coordinat. wn t igt incrasd, t first scond trms on t RS of Eq. () dcrasd t tird trm rmaind constant; t oriontal componnt of t contravariant basis vctor dcrasd wil its vrtical componnt was constant; trfor, bcam stp according to t igt (Fig. ). T mtric tnsors of t -coordinat wr usd to dmonstrat t local vctor caractristics of t basis vctors. T dfinitions of t covariant contravariant mtric tnsors wr givn b Zdunkowski Bott (00a) as follows: g, () g. () Componnts on t diagonal of g g rprsntd t innr products of t covariant contravariant basis vctors, rspctivl; t otrs wr t mutual innr products of t two. Substituting Eqs. (6)() into Eq. () Eq. (), g g of t -coordinat wr obtaind: g 0 0 g In Eq. (4) Eq. (5), g =g =, g =0, onl two oriontal contravariant basis vctors ar unit vctors ortogonal to ac otr (Tabls ). Tus, t co- Tabl Caractristics of t covariant basis vctors in t -coordinat, wn t igt slop of t trrain did not qual ro. Spatial distribution caractristics Local vctor caractristics In t oriontal In t vrtical i Not unit vctors, non-ortogonal Tangnt to t trrain at t ground Alwas vrtical wit its magnitud linarl dcrasing, according to t trrain igt Bcom flat wit t igt incrass Tabl Caractristics of t contravariant basis vctors in t -coordinat, wn t igt slop of t trrain did not qual ro. Spatial distribution caractristics Local vctor caractristics In t oriontal In t vrtical Unit vctors, ortogonal to ac otr Not unit vctor, not ortogonal to t otr two Normal to t trrain at t ground Bcoms stp wn t igt incrass, (4). (5)
4 60 ATMOSPERIC AND OCEANIC SCIENCE LETTERS VOL. 4 variant basis vctors of t -coordinat wr nonortogonal t contravariant basis vctors could b dscribd as alf-ortogonal, wn t igt slop of trrain did not qual ro (Fig. ). Not tat t oriontal (vrtical) covariant basis vctors ar alwas ortogonal to t vrtical (oriontal) contravariant basis vctors (Fig. ), watvr t prssion of, according to t dfinition of covariant contravariant basis vctors. Tus, using t oriontal (vrtical) covariant basis vctor t vrtical (oriontal) contravariant basis vctor of -coordinat as t basis vctors of a coordinat, an ortogonal trrain-following coordinat can b obtaind, upon wic t quations will b as simpl as tos in t Cartsian coordinat, wic can potntiall avoid t associatd computational problms. Finall, substituting 0, 0, =0 into Eqs. (6)(), Eq. (4) Eq. (5), rspctivl, t following wr obtaind: = =i, (6) = =j, (7) = =k, (8) 0 0 g g 0 0. (9) 0 0 Eqs. (6)(9) sowd tat bot t covariant contravariant basis vctors wr idntical to tos of t Cartsian coordinat, wn t igt slop of t trrain quald ro (Fig. ). Tis was anotr important caractristic of t -coordinat, wic must b complid b an trrain-following coordinat.. -coordinat surfacs First, Eq. () was rwrittn as t following:. (0) Eq. (0) was t act matmatical prssion of all t -coordinat surfacs in a viw of t Cartsian coordinat. Mor prcisl, wn quald a constant, Eq. (0) rprsntd t sap of t crtain -coordinat surfac. T RS of Eq. (0) bcam a linar combination of trrain, trfor, vr -coordinat surfac was trrain-following. Scond, t partial drivativ wit rspct to in Eq. (0) is givn b t following:. () T trm rprsnting t slops of -coordinat surfacs in t -dirction is proportional to /. Tus, t slop of t -coordinat surfac was consistnt wit t slop of trrain dcrasd wit incrasing igt. Tn, = was dfind its partial drivativ was solvd wit rspct to in Eq. ():. () T trm, rprsnting t slop variation of t -coordinat surfacs in t vrtical dirction, dpndd on t. Tus, t valu can b adjustd b onl canging t top igt of a modl or t trrain function. owvr, ts two variabls ar alwas fid in a modl. Man mtods av bn dsignd to crat smoot σ-coordinat surfacs, suc as t smoot lvl vrtical coordinat dvlopd b Scär t al. (00), wic modifid t trrain igt to rduc t slop of σ-coordinat surfac in igr lvls. Furtrmor, a trrain-following coordinat can b dsignd via Eq. () variabls could b addd to mak t valu dcras wit t igt.. Rang of t vrtical coordinat Substituting t rang 0, into Eq. (), t following was obtaind:,. () owvr, tis was diffrnt from t gnral on, wic was 0,. Furtrmor, t valu of monotonousl incrasd according to t igt, t -coordinat surfac coincidd wit t ground surfac wn =0 (=). As a rsult, wn t igt was lss ), t corrsponding -coordinat surfacs wr curvilinar surfacs blow t Eart surfac (Fig. ). Basd on tis analsis, 0, was substitutd into Eq. () to obtain t following:, 0. (4) In practical applications, -coordinat surfacs blow t Eart surfac wr liminatd b taking t valus ranging from Eq. (4) out of Eq. (), tn obtain t gnral valu rang of. tan t valu of t trrain ( 0, 0. (5), Not tat t dfinition of σ is actuall a binar function of variabls. Bcaus of t uslssnss of t Figur A cross-sction of t -coordinat surfacs blow t Eart surfac, vrticall. T black lin rprsnts trrain, wil colord lins rprsnt t -coordinat surfacs. T dirctions of t Cartsian coordinat ar indicatd at t lowr lft cornr.
5 NO. LI ET AL.: CARACTERISTICS OF A TERRAIN-FOLLOWING SIGMA COORDINATE 6 -coordinat surfacs blow t Eart surfac, onl t prssion of tis function abov t trrain was considrd wn dsigning t trrain-following coordinat. 4 Summar T main caractristics of a -coordinat wr dscribd in a mor quantitativ wa tan in prvious studis to quantif t known caractristics to lucidat som dtaild caractristics. Spcificall, a -D scmatic of t coordinat surfacs, lins, as of a -coordinat was providd in viw of a curvilinar coordinat sstm. T spatial variation of t covariant contravariant basis vctors of t -coordinat wr obtaind b braking down t caractristics of t basis vctors into t local vctor caractristics spatial distribution caractristics analing tir matmatical prssions. Particularl, a matmatical prssion of all t -coordinat surfacs was found as viwd in t Cartsian coordinat framwork to quantif t so-calld trrain-following caractristic lack of flibilit to adjust t slop variation of -coordinat surfacs in t classic dfinition of. In addition, t -coordinat surfacs blow t Eart surfac wr found, trb validating t gnral rang valu of t vrtical coordinat. T quantitativ dscriptions of t caractristics of t -coordinat providd dtaild suggstions to improv t classic -coordinat or crat a nw on, tus potntiall rsolving its associatd computational problms. First, t local vctor caractristics spatial distribution caractristics of basis vctors manifst t possibilit to crat an ortogonal trrain-following coordinat; scond, t matmatical prssion of -coordinat surfacs tir slop variation can b usd to gnrat a smoot -coordinat surfac in ig lvls, wil prsrving t trrain-following caractristic; tird, t analsis of t valu rang of allowd for t focus to b placd primaril on t dfinition of abov t trrain. Incidntall, improvmnts of t classic -coordinat, wic complid wit t quantitativ dscriptions, nd to b invstigatd via furtr numrical primnts. Acknowldgmnts. T two anonmous rviwrs lpd us to aciv t prsnt rsults. Tis work was jointl supportd b t National Natural Scinc Foundation of Cina undr Grant Nos , 40606, Rfrncs Clark, T. L., 977: A small-scal dnamic modl using a trrain-following coordinat transformation, J. Comp. Ps., 4, 865. Corb, G. A., A. Gilcrist, R. L. Nwson, 97: A gnral circulation modl of t atmospr suitabl for long priod intgrations, Quart. J. Ro. Mtor. Soc., 98, Dutton, J. A., 976a: Vctor tnsor analsis fundamntal kinmatics of fluid flow, in: T Caslss Wind: An Introduction to T Tor of Atmospric Motion, McGraw-ill, NwYork, 90. Dutton, J. A., 976b: Mtorological quations of motion, in: T Caslss Wind: An Introduction to T Tor of Atmospric Motion, McGraw-ill, NwYork, Gal-Cn, T., R. C. J. Somrvill, 975: On t us of a coordinat transformation for t solution of t Navir-stoks quations, J. Comp. Ps., 7, 098. odur, R. M., 997: T naval rsarc laborator s coupld ocan/atmospr msoscal prdiction sstm (COAMPS), Mon. Wa. Rv., 5, Ji, L., J. Cn, D. Zang, t al., 005: Rviw of som numrical aspcts of t dnamic framwork of NWP modl, Cins J. Atoms. Sci. (in Cins), 9, 00. Klmp, J. B., W. C. Skamarock, 00: Numrical consistnc of mtric trms in trrain-following coordinats, Mon. Wa. Rv.,, 99. Lin, S., 997: A finit-volum intgration mtod for computing prssur gradint forc in gnral vrtical coordinats, Quart. J. Ro. Mtor. Soc.,, Pillips, N. A., 957: A coordinat sstm aving som spcial advantags for numrical forcasting, J. Mtor., 4, Pilk, R. A., 00: Coordinat transformations, in: Msoscal Mtorological Modling, nd (d.), Acadmic Prss, San Digo, 09. Pilk, R. A., W. R. Cotton, R. L. Walko, t al., 99: A comprnsiv mtorological modling sstm RAMS, Mtor. Atmos. Ps., 49, 699. Scär, C., D. Lunbrgr, O. Furr, t al., 00: A nw trrain-following vrtical coordinat formulation for atmospric prdiction modls, Mon. Wa. Rv., 0, Stpplr, J., R. ss, U. Scättlr, t al., 00: Rviw of numrical mtods for nondrostatic watr prdiction modls, Mtor. Atmos. Ps., 8, 870. Xu, M., K. K. Drogmir, V. Wong, 000: T advancd rgional prdiction sstm (ARPS) A multi-scal nondrostatic atmospric simulation prdiction modl. Part I: modl dnamics vrification, Mtor. Atmos. Ps., 75, 69. Zdunkowski, W., A. Bott, 00a: Rciprocal coordinat sstms, in: Dnamics of t Atmospr: A Cours in Tortical Mtorolog, Cambridg Univrsit Prss, Cambridg, 56. Zdunkowski, W., A. Bott, 00b: Orograp-following coordinat sstms, in: Dnamics of t Atmospr: A Cours in Tortical Mtorolog, Cambridg Univrsit Prss, Cambridg,
3-2-1 ANN Architecture
ARTIFICIAL NEURAL NETWORKS (ANNs) Profssor Tom Fomby Dpartmnt of Economics Soutrn Mtodist Univrsity Marc 008 Artificial Nural Ntworks (raftr ANNs) can b usd for itr prdiction or classification problms.
More informationu x A j Stress in the Ocean
Strss in t Ocan T tratmnt of strss and strain in fluids is comlicatd and somwat bond t sco of tis class. Tos rall intrstd sould look into tis rtr in Batclor Introduction to luid Dnamics givn as a rfrnc
More informationTrigonometric functions
Robrto s Nots on Diffrntial Calculus Captr 5: Drivativs of transcndntal functions Sction 5 Drivativs of Trigonomtric functions Wat you nd to know alrady: Basic trigonomtric limits, t dfinition of drivativ,
More informationPhysics 43 HW #9 Chapter 40 Key
Pysics 43 HW #9 Captr 4 Ky Captr 4 1 Aftr many ours of dilignt rsarc, you obtain t following data on t potolctric ffct for a crtain matrial: Wavlngt of Ligt (nm) Stopping Potntial (V) 36 3 4 14 31 a) Plot
More informationCharacteristics of Gliding Arc Discharge Plasma
Caractristics of Gliding Arc Discarg Plasma Lin Li( ), Wu Bin(, Yang Ci(, Wu Cngkang ( Institut of Mcanics, Cins Acadmy of Scincs, Bijing 8, Cina E-mail: linli@imc.ac.cn Abstract A gliding arc discarg
More informationdy 1. If fx ( ) is continuous at x = 3, then 13. If y x ) for x 0, then f (g(x)) = g (f (x)) when x = a. ½ b. ½ c. 1 b. 4x a. 3 b. 3 c.
AP CALCULUS BC SUMMER ASSIGNMENT DO NOT SHOW YOUR WORK ON THIS! Complt ts problms during t last two wks of August. SHOW ALL WORK. Know ow to do ALL of ts problms, so do tm wll. Itms markd wit a * dnot
More informationDIFFERENTIAL EQUATION
MD DIFFERENTIAL EQUATION Sllabus : Ordinar diffrntial quations, thir ordr and dgr. Formation of diffrntial quations. Solution of diffrntial quations b th mthod of sparation of variabls, solution of homognous
More informationu 3 = u 3 (x 1, x 2, x 3 )
Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.
More information2008 AP Calculus BC Multiple Choice Exam
008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl
More informationThat is, we start with a general matrix: And end with a simpler matrix:
DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss
More informationImproved Dual to Ratio Cum Dual to Product Estimator in the Stratified Random Sampling
Amrican Journal of Oprational Rsarc 05 5(3): 57-63 DOI: 0593/jajor0505030 Improvd Dual to Ratio Cum Dual to Product Eimator in t Stratifid Random Sampling Subas Kumar adav S S Misra Cm Kadilar Alok Kumar
More informationEinstein Equations for Tetrad Fields
Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for
More informationis an appropriate single phase forced convection heat transfer coefficient (e.g. Weisman), and h
For t BWR oprating paramtrs givn blow, comput and plot: a) T clad surfac tmpratur assuming t Jns-Lotts Corrlation b) T clad surfac tmpratur assuming t Tom Corrlation c) T clad surfac tmpratur assuming
More informationAvailable online at ScienceDirect. Procedia Engineering 126 (2015 )
Availabl onlin at www.scincdirct.com ScincDirct Procdia Enginring 26 (25 ) 628 632 7t Intrnational Confrnc on Fluid Mcanics, ICFM7 Applications of ig ordr ybrid DG/FV scms for twodimnsional RAS simulations
More informationAP Calculus BC AP Exam Problems Chapters 1 3
AP Eam Problms Captrs Prcalculus Rviw. If f is a continuous function dfind for all ral numbrs and if t maimum valu of f() is 5 and t minimum valu of f() is 7, tn wic of t following must b tru? I. T maimum
More informationHomotopy perturbation technique
Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,
More informationSection 11.6: Directional Derivatives and the Gradient Vector
Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th
More informationChapter Taylor Theorem Revisited
Captr 0.07 Taylor Torm Rvisitd Atr radig tis captr, you sould b abl to. udrstad t basics o Taylor s torm,. writ trascdtal ad trigoomtric uctios as Taylor s polyomial,. us Taylor s torm to id t valus o
More informationThe graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the
Copyright itutcom 005 Fr download & print from wwwitutcom Do not rproduc by othr mans Functions and graphs Powr functions Th graph of n y, for n Q (st of rational numbrs) y is a straight lin through th
More informationCOHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.
MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function
More informationFourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.
Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform
More informationHigher order derivatives
Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of
More informationSystems of Equations
CHAPTER 4 Sstms of Equations 4. Solving Sstms of Linar Equations in Two Variabls 4. Solving Sstms of Linar Equations in Thr Variabls 4. Sstms of Linar Equations and Problm Solving Intgratd Rviw Sstms of
More information4037 ADDITIONAL MATHEMATICS
CAMBRIDGE INTERNATIONAL EXAMINATIONS GCE Ordinary Lvl MARK SCHEME for th Octobr/Novmbr 0 sris 40 ADDITIONAL MATHEMATICS 40/ Papr, maimum raw mark 80 This mark schm is publishd as an aid to tachrs and candidats,
More information1 General boundary conditions in diffusion
Gnral boundary conditions in diffusion Πρόβλημα 4.8 : Δίνεται μονοδιάτατη πλάκα πάχους, που το ένα άκρο της κρατιέται ε θερμοκραία T t και το άλλο ε θερμοκραία T 2 t. Αν η αρχική θερμοκραία της πλάκας
More informationMAT 270 Test 3 Review (Spring 2012) Test on April 11 in PSA 21 Section 3.7 Implicit Derivative
MAT 7 Tst Rviw (Spring ) Tst on April in PSA Sction.7 Implicit Drivativ Rmmbr: Equation of t tangnt lin troug t point ( ab, ) aving slop m is y b m( a ). dy Find t drivativ y d. y y. y y y. y 4. y sin(
More informationExponential Functions
Eponntial Functions Dinition: An Eponntial Function is an unction tat as t orm a, wr a > 0. T numbr a is calld t bas. Eampl: Lt i.. at intgrs. It is clar wat t unction mans or som valus o. 0 0,,, 8,,.,.
More informationText: WMM, Chapter 5. Sections , ,
Lcturs 6 - Continuous Probabilit Distributions Tt: WMM, Chaptr 5. Sctions 6.-6.4, 6.6-6.8, 7.-7. In th prvious sction, w introduc som of th common probabilit distribution functions (PDFs) for discrt sampl
More informationCHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle
CHPTER 1 Introductory Concpts Elmnts of Vctor nalysis Nwton s Laws Units Th basis of Nwtonian Mchanics D lmbrt s Principl 1 Scinc of Mchanics: It is concrnd with th motion of matrial bodis. odis hav diffrnt
More informationAP Calculus Multiple-Choice Question Collection
AP Calculus Multipl-Coic Qustion Collction 985 998 . f is a continuous function dfind for all ral numbrs and if t maimum valu of f () is 5 and t minimum valu of f () is 7, tn wic of t following must b
More informationBroadband All-Angle Negative Refraction by Phononic Crystals
Supplmntar Information Broadband All-Angl Ngativ Rfraction b Phononic Crstals Yang Fan Li, Fi Mng, Shiwi Zhou, Ming-Hui Lu and Xiaodong Huang 1 Optimization algorithm and procss Bfor th optimization procss,
More informationDual Nature of Matter and Radiation
Higr Ordr Tinking Skill Qustions Dual Natur of Mattr and Radiation 1. Two bas on of rd ligt and otr of blu ligt of t sa intnsity ar incidnt on a tallic surfac to it otolctrons wic on of t two bas its lctrons
More informationSelf-Adjointness and Its Relationship to Quantum Mechanics. Ronald I. Frank 2016
Ronald I. Frank 06 Adjoint https://n.wikipdia.org/wiki/adjoint In gnral thr is an oprator and a procss that dfin its adjoint *. It is thn slf-adjoint if *. Innr product spac https://n.wikipdia.org/wiki/innr_product_spac
More informationAtomic Physics. Final Mon. May 12, 12:25-2:25, Ingraham B10 Get prepared for the Final!
# SCORES 50 40 30 0 10 MTE 3 Rsults P08 Exam 3 0 30 40 50 60 70 80 90 100 SCORE Avrag 79.75/100 std 1.30/100 A 19.9% AB 0.8% B 6.3% BC 17.4% C 13.1% D.1% F 0.4% Final Mon. Ma 1, 1:5-:5, Ingraam B10 Gt
More informationFull Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient
Full Wavform Invrsion Using an Enrgy-Basd Objctiv Function with Efficint Calculation of th Gradint Itm yp Confrnc Papr Authors Choi, Yun Sok; Alkhalifah, ariq Ali Citation Choi Y, Alkhalifah (217) Full
More informationSTRESSES FROM LOADING ON RIGID PAVEMENT COURSES
bartosova.qxd 16.8.004 14:34 StrÆnka 3 003/1 PAGES 3 37 RECEIVED 5. 6. 00 ACCEPTED 15. 11. 00 ¼. BARTOŠOVÁ STRESSES FROM LOADING ON RIGID PAVEMENT COURSES ¼udmila Bartošová, Ing., PD. Assistant lcturr
More informationHydrogen Atom and One Electron Ions
Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial
More informationare given in the table below. t (hours)
CALCULUS WORKSHEET ON INTEGRATION WITH DATA Work th following on notbook papr. Giv dcimal answrs corrct to thr dcimal placs.. A tank contains gallons of oil at tim t = hours. Oil is bing pumpd into th
More informationA Propagating Wave Packet Group Velocity Dispersion
Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to
More informationEffects of Couple Stress Lubricants on Pressure and Load Capacity of Infinitely Wide Exponentially Shaped Slider Bearing
Procdings of t World Congrss on Enginring and Computr Scinc 200 Vol II, Octobr 20-22, 200, San Francisco, USA Effcts of Coupl Strss Lubricants on Prssur and Load Capacity of Infinitly Wid Eponntially Sapd
More informationDifferentiation of Exponential Functions
Calculus Modul C Diffrntiation of Eponntial Functions Copyright This publication Th Northrn Albrta Institut of Tchnology 007. All Rights Rsrvd. LAST REVISED March, 009 Introduction to Diffrntiation of
More informationSTABILITY ANALYSIS OF FUZZY CONTROLLERS USING THE MODIFIED POPOV CRITERION
SABILIY ANALYSIS OF FUZZY CONROLLERS USING HE MODIFIED POPOV CRIERION Mauricio Gonçalvs Santana Junior Instituto cnológico d Aronáutica Pça Mal Eduardo Goms, 50 Vila das Acácias - CEP 2228-900 São José
More informationElements of Statistical Thermodynamics
24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,
More informationSolution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:
APPM 6 Final 5 pts) Spring 4. 6 pts total) Th following parts ar not rlatd, justify your answrs: a) Considr th curv rprsntd by th paramtric quations, t and y t + for t. i) 6 pts) Writ down th corrsponding
More informationDynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA *
17 nd Intrnational Confrnc on Mchanical Control and Automation (ICMCA 17) ISBN: 978-1-6595-46-8 Dynamic Modlling of Hoisting Stl Wir Rop Da-zhi CAO, Wn-zhng DU, Bao-zhu MA * and Su-bing LIU Xi an High
More information10. The Discrete-Time Fourier Transform (DTFT)
Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w
More informationNEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA
NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals
More information3 Finite Element Parametric Geometry
3 Finit Elmnt Paramtric Gomtry 3. Introduction Th intgral of a matrix is th matrix containing th intgral of ach and vry on of its original componnts. Practical finit lmnt analysis rquirs intgrating matrics,
More informationInstantaneous Cutting Force Model in High-Speed Milling Process with Gyroscopic Effect
Advancd Matrials sarch Onlin: -8-6 ISS: 66-8985, Vols. 34-36, pp 389-39 doi:.48/www.scintific.nt/am.34-36.389 rans ch Publications, Switzrland Instantanous Cutting Forc Modl in High-Spd Milling Procss
More informationStudies of Turbulence and Transport in Alcator C-Mod Ohmic Plasmas with Phase Contrast Imaging and Comparisons with GYRO*
Studis of Turbulnc and Transport in Ohmic Plasmas with Phas Contrast Imaging and Comparisons with GYRO* L. Lin 1, M. Porkolab 1, E.M. Edlund 1, J.C. Rost 1, M. Grnwald 1, D.R. Mikklsn 2, N. Tsujii 1 1
More informationExam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.
Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r
More informationSectrix Curves on the Sphere
riginal scintific papr Accptd 22. 2. 205. LÁSZLÓ NÉMETH Sctri Curvs on th Sphr Sctri Curvs on th Sphr ABSTRACT In this papr w introduc a class of curvs drivd from a gomtrical construction. Ths planar curvs
More informationFinite Element Models for Steady Flows of Viscous Incompressible Fluids
Finit Elmnt Modls for Stad Flows of Viscous Incomprssibl Fluids Rad: Chaptr 10 JN Rdd CONTENTS Govrning Equations of Flows of Incomprssibl Fluids Mid (Vlocit-Prssur) Finit Elmnt Modl Pnalt Function Mthod
More informationDifferential Equations
UNIT I Diffrntial Equations.0 INTRODUCTION W li in a world of intrrlatd changing ntitis. Th locit of a falling bod changs with distanc, th position of th arth changs with tim, th ara of a circl changs
More informationME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002
3.4 Forc Analysis of Linkas An undrstandin of forc analysis of linkas is rquird to: Dtrmin th raction forcs on pins, tc. as a consqunc of a spcifid motion (don t undrstimat th sinificanc of dynamic or
More informationThinking outside the (Edgeworth) Box
Tinking outsid t (dgwort) ox by Jon G. Rily Dartmnt of conomics UCL 0 Novmbr 008 To dvlo an undrstanding of Walrasian quilibrium allocations, conomists tyically start wit t two rson, two-commodity xcang
More informationDirect Approach for Discrete Systems One-Dimensional Elements
CONTINUUM & FINITE ELEMENT METHOD Dirct Approach or Discrt Systms On-Dimnsional Elmnts Pro. Song Jin Par Mchanical Enginring, POSTECH Dirct Approach or Discrt Systms Dirct approach has th ollowing aturs:
More informationExercise 1. Sketch the graph of the following function. (x 2
Writtn tst: Fbruary 9th, 06 Exrcis. Sktch th graph of th following function fx = x + x, spcifying: domain, possibl asymptots, monotonicity, continuity, local and global maxima or minima, and non-drivability
More information1973 AP Calculus AB: Section I
97 AP Calculus AB: Sction I 9 Minuts No Calculator Not: In this amination, ln dnots th natural logarithm of (that is, logarithm to th bas ).. ( ) d= + C 6 + C + C + C + C. If f ( ) = + + + and ( ), g=
More informationPartial Derivatives: Suppose that z = f(x, y) is a function of two variables.
Chaptr Functions o Two Variabls Applid Calculus 61 Sction : Calculus o Functions o Two Variabls Now that ou hav som amiliarit with unctions o two variabls it s tim to start appling calculus to hlp us solv
More informationu x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula
7. Intgration by Parts Each drivativ formula givs ris to a corrsponding intgral formula, as w v sn many tims. Th drivativ product rul yilds a vry usful intgration tchniqu calld intgration by parts. Starting
More informationarxiv: v1 [physics.comp-ph] 30 Jun 2016
On anisotropy function in crystal growth simulations using Lattic Boltzmann quation AMINA YOUNSI a,1, ALAIN CARTALADE a, a Dn DM2S, STMF, LMSF, CEA, Univrsité d Paris-Saclay, F-91191, Gif-sur-Yvtt, Franc.
More informationOn the Hamiltonian of a Multi-Electron Atom
On th Hamiltonian of a Multi-Elctron Atom Austn Gronr Drxl Univrsity Philadlphia, PA Octobr 29, 2010 1 Introduction In this papr, w will xhibit th procss of achiving th Hamiltonian for an lctron gas. Making
More informationA General Thermal Equilibrium Discharge Flow Model
Journal of Enrgy and Powr Enginring 1 (216) 392-399 doi: 1.17265/1934-8975/216.7.2 D DAVID PUBLISHING A Gnral Thrmal Equilibrium Discharg Flow Modl Minfu Zhao, Dongxu Zhang and Yufng Lv Dpartmnt of Ractor
More informationScattering States of l-wave Schrödinger Equation with Modified Rosen Morse Potential
Commun. Thor. Phys. 66 06 96 00 Vol. 66, No., August, 06 Scattring Stats of l-wav Schrödingr Equation with Modifid Rosn Mors Potntial Wn-Li Chn í,, Yan-Wi Shi á, and Gao-Fng Wi Ôô, Gnral Education Cntr,
More informationChapter 1. Chapter 10. Chapter 2. Chapter 11. Chapter 3. Chapter 12. Chapter 4. Chapter 13. Chapter 5. Chapter 14. Chapter 6. Chapter 7.
Chaptr Binomial Epansion Chaptr 0 Furthr Probability Chaptr Limits and Drivativs Chaptr Discrt Random Variabls Chaptr Diffrntiation Chaptr Discrt Probability Distributions Chaptr Applications of Diffrntiation
More informationEinstein Rosen inflationary Universe in general relativity
PRAMANA c Indian Acadmy of Scincs Vol. 74, No. 4 journal of April 2010 physics pp. 669 673 Einstin Rosn inflationary Univrs in gnral rlativity S D KATORE 1, R S RANE 2, K S WANKHADE 2, and N K SARKATE
More informationCalculus Revision A2 Level
alculus Rvision A Lvl Tabl of drivativs a n sin cos tan d an sc n cos sin Fro AS * NB sc cos sc cos hain rul othrwis known as th function of a function or coposit rul. d d Eapl (i) (ii) Obtain th drivativ
More informationDetermination of Vibrational and Electronic Parameters From an Electronic Spectrum of I 2 and a Birge-Sponer Plot
5 J. Phys. Chm G Dtrmination of Vibrational and Elctronic Paramtrs From an Elctronic Spctrum of I 2 and a Birg-Sponr Plot 1 15 2 25 3 35 4 45 Dpartmnt of Chmistry, Gustavus Adolphus Collg. 8 Wst Collg
More informationJournal of Computational and Applied Mathematics. An adaptive discontinuous finite volume method for elliptic problems
Journal of Computational and Applid Matmatics 235 (2011) 5422 5431 Contnts lists availabl at ScincDirct Journal of Computational and Applid Matmatics journal ompag: www.lsvir.com/locat/cam An adaptiv discontinuous
More informationUniformly stable discontinuous Galerkin discretization and robust iterative solution methods for the Brinkman problem
www.oaw.ac.at Uniformly stabl discontinuous Galrin discrtization and robust itrativ solution mtods for t Brinman problm Q. Hong, J. Kraus RICAM-Rport 2014-36 www.ricam.oaw.ac.at UNIFORMLY STABLE DISCONTINUOUS
More informationA Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes
Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical
More informationPrelab Lecture Chmy 374 Thur., March 22, 2018 Edited 22mar18, 21mar18
Prlab Lctur Cmy 374 Tur., Marc, 08 Editd mar8, mar8 LA REPORT:From t ClassicalTrmoISub-7.pdf andout: Was not a dry lab A partially complt spradst was postd on wb Not ruird 3 If solid is pur X Partial
More informationPrelim Examination 2011 / 2012 (Assessing Units 1 & 2) MATHEMATICS. Advanced Higher Grade. Time allowed - 2 hours
Prlim Eamination / (Assssing Units & ) MATHEMATICS Advancd Highr Grad Tim allowd - hours Rad Carfull. Calculators ma b usd in this papr.. Candidats should answr all qustions. Full crdit will onl b givn
More information16. Electromagnetics and vector elements (draft, under construction)
16. Elctromagntics (draft)... 1 16.1 Introduction... 1 16.2 Paramtric coordinats... 2 16.3 Edg Basd (Vctor) Finit Elmnts... 4 16.4 Whitny vctor lmnts... 5 16.5 Wak Form... 8 16.6 Vctor lmnt matrics...
More informationMathematics. Complex Number rectangular form. Quadratic equation. Quadratic equation. Complex number Functions: sinusoids. Differentiation Integration
Mathmatics Compl numbr Functions: sinusoids Sin function, cosin function Diffrntiation Intgration Quadratic quation Quadratic quations: a b c 0 Solution: b b 4ac a Eampl: 1 0 a= b=- c=1 4 1 1or 1 1 Quadratic
More informationApplication of Vague Soft Sets in students evaluation
Availabl onlin at www.plagiarsarchlibrary.com Advancs in Applid Scinc Rsarch, 0, (6):48-43 ISSN: 0976-860 CODEN (USA): AASRFC Application of Vagu Soft Sts in studnts valuation B. Chtia*and P. K. Das Dpartmnt
More informationMA 262, Spring 2018, Final exam Version 01 (Green)
MA 262, Spring 218, Final xam Vrsion 1 (Grn) INSTRUCTIONS 1. Switch off your phon upon ntring th xam room. 2. Do not opn th xam booklt until you ar instructd to do so. 3. Bfor you opn th booklt, fill in
More informationUNIFIED ERROR ANALYSIS
UNIFIED ERROR ANALYSIS LONG CHEN CONTENTS 1. Lax Equivalnc Torm 1 2. Abstract Error Analysis 2 3. Application: Finit Diffrnc Mtods 4 4. Application: Finit Elmnt Mtods 4 5. Application: Conforming Discrtization
More informationLagrangian Analysis of a Class of Quadratic Liénard-Type Oscillator Equations with Exponential-Type Restoring Force function
agrangian Analysis of a Class of Quadratic iénard-ty Oscillator Equations wit Eonntial-Ty Rstoring Forc function J. Akand, D. K. K. Adjaï,.. Koudaoun,Y. J. F. Komaou,. D. onsia. Dartmnt of Pysics, Univrsity
More informationJOHNSON COUNTY COMMUNITY COLLEGE Calculus I (MATH 241) Final Review Fall 2016
JOHNSON COUNTY COMMUNITY COLLEGE Calculus I (MATH ) Final Rviw Fall 06 Th Final Rviw is a starting point as you study for th final am. You should also study your ams and homwork. All topics listd in th
More informationTwo Products Manufacturer s Production Decisions with Carbon Constraint
Managmnt Scinc and Enginring Vol 7 No 3 pp 3-34 DOI:3968/jms9335X374 ISSN 93-34 [Print] ISSN 93-35X [Onlin] wwwcscanadant wwwcscanadaorg Two Products Manufacturr s Production Dcisions with Carbon Constraint
More informationIntroduction to Condensed Matter Physics
Introduction to Condnsd Mattr Physics pcific hat M.P. Vaughan Ovrviw Ovrviw of spcific hat Hat capacity Dulong-Ptit Law Einstin modl Dby modl h Hat Capacity Hat capacity h hat capacity of a systm hld at
More informationMor Tutorial at www.dumblittldoctor.com Work th problms without a calculator, but us a calculator to chck rsults. And try diffrntiating your answrs in part III as a usful chck. I. Applications of Intgration
More informationMassachusetts Institute of Technology Department of Mechanical Engineering
Massachustts Institut of Tchnolog Dpartmnt of Mchanical Enginring. Introduction to Robotics Mid-Trm Eamination Novmbr, 005 :0 pm 4:0 pm Clos-Book. Two shts of nots ar allowd. Show how ou arrivd at our
More informationFinite element discretization of Laplace and Poisson equations
Finit lmnt discrtization of Laplac and Poisson quations Yashwanth Tummala Tutor: Prof S.Mittal 1 Outlin Finit Elmnt Mthod for 1D Introduction to Poisson s and Laplac s Equations Finit Elmnt Mthod for 2D-Discrtization
More informationperm4 A cnt 0 for for if A i 1 A i cnt cnt 1 cnt i j. j k. k l. i k. j l. i l
h 4D, 4th Rank, Antisytric nsor and th 4D Equivalnt to th Cross Product or Mor Fun with nsors!!! Richard R Shiffan Digital Graphics Assoc 8 Dunkirk Av LA, Ca 95 rrs@isidu his docunt dscribs th four dinsional
More informationThermodynamical insight on the role of additives in shifting the equilibrium between white and grey tin
hrmodynamical insight on th rol of additivs in shifting th quilibrium btwn whit and gry tin Nikolay Dmntv Dpartmnt of Chmistry, mpl Univrsity, Philadlphia, PA 19122 Abstract In this study mthods of statistical
More informationPrinciples of Humidity Dalton s law
Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid
More informationSCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott
SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER J. C. Sprott PLP 821 Novmbr 1979 Plasma Studis Univrsity of Wisconsin Ths PLP Rports ar informal and prliminary and as such may contain rrors not yt
More informationELECTRON-MUON SCATTERING
ELECTRON-MUON SCATTERING ABSTRACT Th lctron charg is considrd to b distributd or xtndd in spac. Th diffrntial of th lctron charg is st qual to a function of lctron charg coordinats multiplid by a four-dimnsional
More information1997 AP Calculus AB: Section I, Part A
997 AP Calculus AB: Sction I, Part A 50 Minuts No Calculator Not: Unlss othrwis spcifid, th domain of a function f is assumd to b th st of all ral numbrs for which f () is a ral numbr.. (4 6 ) d= 4 6 6
More informationDirectivity effect of the 2016 Kumamoto Earthquake on both the ground motion and the damage of wooden house
Dirctivit ffct of th 216 Kumamoto Earthquak on both th ground motion and th damag of woodn hous *Haato Nishikawa 1) and Tomia Takatani 2) 1), 2) Nat l Institut of Tchnolog, Maizuru Collg, Maizuru, Koto
More informationA UNIFIED A POSTERIORI ERROR ESTIMATOR FOR FINITE VOLUME METHODS FOR THE STOKES EQUATIONS
A UNIFIED A POSTERIORI ERROR ESTIMATOR FOR FINITE VOLUME METHODS FOR THE STOKES EQUATIONS JUNPING WANG, YANQIU WANG, AND XIU YE Abstract. In tis papr, t autors stablisd a unifid framwork for driving and
More informationGEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES. Eduard N. Klenov* Rostov-on-Don, Russia
GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES Eduard N. Klnov* Rostov-on-Don, Russia Th articl considrs phnomnal gomtry figurs bing th carrirs of valu spctra for th pairs of th rmaining additiv
More informationVSMN30 FINITA ELEMENTMETODEN - DUGGA
VSMN3 FINITA ELEMENTMETODEN - DUGGA 1-11-6 kl. 8.-1. Maximum points: 4, Rquird points to pass: Assistanc: CALFEM manual and calculator Problm 1 ( 8p ) 8 7 6 5 y 4 1. m x 1 3 1. m Th isotropic two-dimnsional
More informationBackground: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.
Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby
More informationGH. Rahimi & AR. Davoodinik
US ntrnational Journal of nginring Scinc Vol 9 No5-8 Pag 5- HRMAL BHAVOR ANALYSS OF H FUNONALLY GRADD MOSHNKO'S BAM GH Raimi & AR Davoodinik Abstract: intntion of tis stud is t analsis of trmal bavior
More informationDynamic analysis of a Timoshenko beam subjected to moving concentrated forces using the finite element method
Shock and Vibration 4 27) 459 468 459 IOS Prss Dynamic analysis of a Timoshnko bam subjctd to moving concntratd forcs using th finit lmnt mthod Ping Lou, Gong-lian Dai and Qing-yuan Zng School of Civil
More informationSpace-Time Discontinuous Galerkin Method for Maxwell s Equations
Commun. Comput. Pys. doi: 0.4208/cicp.23042.2722a Vol. 4, No. 4, pp. 96-939 Octobr 203 Spac-Tim Discontinuous Galrkin Mtod for Maxwll s Equations Ziqing Xi,2, Bo Wang 3,4, and Zimin Zang 5,6 Scool of Matmatics
More information