We are IntechOpen, the world s leading publisher of Open Access books Built by scientists, for scientists. International authors and editors
|
|
- Lesley Sherman
- 5 years ago
- Views:
Transcription
1 W r InchOpn, h world s lding publishr of Opn Accss books Buil b sciniss, for sciniss 3,500 08,000.7 M Opn ccss books vilbl Inrnionl uhors nd diors Downlods Our uhors r mong h 5 Counris dlivrd o TOP % mos cid sciniss.% Conribuors from op 500 univrsiis Slcion of our books indd in h Book Ciion Ind in Wb of Scinc Cor Collcion (BKCI) Inrsd in publishing wih us? Conc book.dprmn@inchopn.com Numbrs displd bov r bsd on ls d collcd. For mor informion visi
2 Chpr Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw José Simão Anuns do Crmo Addiionl informion is vilbl h nd of h chpr hp://d.doi.org/0.577/6866 Absrc Numricl modls r usful insrumn for suding compl suprposiion of wv wv nd wv currn inrcions in cosl nd surin rgions nd o invsig h inrcion of wvs wih compl bhmris or srucurs buil in nrshor rs. Morovr, sinc hir pplicions r significnl lss pnsiv nd mor flibl hn h consrucion of phsicl modls, h r convnin ool o suppor dsign. Th bili of h sndrd oussinsq nd Srr or Grn nd Nghdi quions o rproduc hs nonlinr procsss is wll known. Howvr, hs modls r rsricd o shllow wr condiions, nd ddiion of ohr rms of disprsiv origin hs bn considrd sinc h 990s, priculrl for pproimions of h oussinsq-p. To llow pplicions in grr rng of ν 0 / λ, ohr hn shllow wrs, whr ν 0 is h wr dph rs nd λ is h wvlngh, nw s of Srr-p quions, wih ddiionl rms of disprsiv origin, is dvlopd nd sd wih h vilbl d nd wih numricl soluion of oussinsq-p modl, lso improvd wih disprsiv chrcrisics. Δplici nd implici mhods of fini diffrnc r implmnd o solv boh pproimions of oussinsq nd Srr ps wih improvd disprsiv chrcrisics. fini lmn mhod is lso implmnd o solv n nsion of oussinsq-p modl h ks ino ccoun wv currn inrcions. pplicion mpls o solv rl-world problms r shown nd discussd. Th prformncs of boh HΓ modls r comprd wih primnl d of vr dmnding pplicions, nml: (ξ) highl nonlinr solir wv propging up slop nd rflcing from vricl wll nd (ξξ) priodic wv propging in inrmdidph wrs upsrm rpzoidl br, followd b vr shllow wrs ovr h br, nd gin in inrmdi-dph wr condiions downsrm. Kwords: Δndd oussinsq quions, Δndd Srr quions, Γisprsiv chrcrisics, Inrmdi wrs, Numricl mhods 05 Th Auhor(s). Licns InTch. This chpr is disribud undr h rms of h Criv Commons Aribuion Licns (hp://crivcommons.org/licnss/b/3.0), which prmis unrsricd us, disribuion, nd rproducion in n mdium, providd h originl work is proprl cid.
3 4 Nw Prspcivs in Fluid Dnmics. Inroducion In rcn dcds, significn dvncs hv bn md in dvloping mhmicl nd numricl modls o dscrib h nir phnomn obsrvd in shllow wr condiions. Indd, no onl our undrsnding of h phnomn hs significnl improvd bu lso h compuionl cpbiliis h r vilbl hv lso incrsd considrbl. In his con, w cn now us mor powrful nd mor rlibl ools in h dsign of srucurs commonl usd in cosl nvironmns. h nd of h 970s, du o h lck of sufficinl dp knowldg, bu bov ll for lck of compuing powr, h us of h linr wv hor for h simulion of phnomn, such s rfrcion nd diffrcion of wvs, ws common prcic. In h 980s, ohr modls h k ino ccoun no onl h rfrcion bu lso h diffrcion procss hv bn proposd nd commonl usd b [] rkhoff ζρ., 98, [] Kirb nd Γlrmpl, 983, [3] ooij, 983, [0] Kirb, 984, nd [5] Γlrmpl, 988, mong mn ohrs. Howvr, s h r bsd on h linr hor, hos modls should no b uilizd in shllow wr condiions. s nod in [6], vn h im modls bsd on h Sin-Vnn quions (s lso [3] Sin-Vnn, 87) wr λrquρ usd ξ prζcξcζρ ζppρξcζξτs. Hτwvr, ζs νζs η wξdρ dmτsrζd, ξ sνζρρτw wζr cτdξξτs ζd λτr sτm ps τλ wζvs, mτdρs ηζsd τ ζ τ-dξsprsξv ντr, τλ wνξcν ν Sζξ-Vζ mτdρ ξs ζ ζmpρ, ζr ρξmξd ζd ζr τ usuζρρ ζηρ τ cτmpu sζξsλζcτr rsuρs τvr ρτμ prξτds τλ ζζρsξs (s lso [33]). Nowds, i is gnrll ccpd h for prcicl pplicions h combind grvi wv ffcs in shllow wr condiions mus b kn ino ccoun. In ddiion, h rfrcion nd diffrcion procsss, h swlling, rflcion nd brking wvs, ll hv o b considrd. lso ccording o [6] ζ umηr τλ λζcτrs νζv mζd ξ pτssξηρ τ mpρτ ξcrζsξμρ cτmpρ mζνmζξcζρ mτdρs. Indd, no onl hs hr bn gr improvmn in our horicl knowldg of h phnomn involvd bu lso h numricl mhods hv bn usd mor fficinl. Th gr dvncs md in compur chnolog, spcill sinc h 980s, improving informion procssing nd nbling lrg mouns of d o b sord, hv md possibl h us of mor mhmicl modls, of grr compli nd wih fwr rsricions. Indd, onl modls of ordr ( =ν 0 / λ, whr ν 0 nd λ rprsn, rspcivl, dph nd wvlngh chrcrisics) or grr, of h oussinsq or Srr ps [4, 35], r bl o dscrib h nir disprsiv nd nonlinr inrcion procss of gnrion, propgion nd run-up of wvs rsuling from wv wv nd wv currn inrcions. I is lso worh o poin ou h in mor compl problms, such s wv gnrion b sfloor movmn, propgion ovr unvn booms, nd ddd brking ffcs, high-frqunc wvs cn ris s consqunc of nonlinr inrcion. In h ps fw rs, h possibili of using mor powrful compuionl fciliis, nd h chnologicl voluion nd sophisicion of conrol ssms hv rquird horough horicl nd primnl rsrch dsignd o improv h knowldg of cosl hdrodnmics. Numricl mhods imd for h pplicions in nginring filds h r mor sophisicd nd wih highr dgr of compli hv lso bn dvlopd.
4 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ In Scion, h gnrl shllow wr wv hor is usd o dvlop diffrn mhmicl pprochs, which r nowds h bsis of h mos sophisicd modls in hdrodnmics nd sdimnr dnmics. Δnsions of h quions for inrmdi wr of h mor gnrl pprochs (ordr ) r prsnd in Scion 3. Numricl formulions of h modls nd ppropri pplicion mpls r prsnd in Scion 4. Firsl, submrgd dissipion plform o proc h ugio lighhous, siud h Tgus sur mouh, Lisbon, is dsignd nd sd numricll. Th scond pplicion is rl-world problm concrning cosl procion, using submrgd srucur o forc h brking wvs offshor. Th hird mpl shows h giions sblishd in h por of Figuir d Foz, Porugl, for diffrn s ss, wih h objciv of dsigning nw prociv jis, or nd h ising ons. Finll, h fourh mpl shows h prformnc of h ndd Srr quions for h propgion of wv in vr dmnding condiions. Conclusions nd fuur dvlopmns r givn in Scion 5.. Mhmicl formulions W sr from h fundmnl quions of h Fluid Mchnics, wrin in Δulr s vribls, rling o hr-dimnsionl nd quζsξ-irroionl flow of prfc fluid [Δulr quions, or Nvir-Soks quions wih h ssumpions of non-comprssibili (dρ / d =dξvv =0), irroionli (rτv =0) nd prfc fluid (dnmic viscosi, µ =0)]: u + v + w = 0 z u + uu + vu + wu = - p z v + uv + vv + wv = - p z w + uw + vw + ww = - p r - μ z z u = w ; v = w ; v = u z z r r () wih p =0 z =η(,, ), w =η + uη + vη z =η(,, ), nd w =ξ + uξ + vξ z = ν 0 + ξ(,, ). In hs quions ρ is dnsi, is im, μ is grviionl cclrion, p is prssur, η is fr surfc lvion, ξ is boom, nd u, v, w r vloci componns. Γfining h dimnsionlss quniis ε =ζ / ν 0 nd =ν 0 / λ, in which ζ is chrcrisic wv mpliud, ν 0 rprsns wr dph, nd λ is chrcrisic wvlngh, w procd wih suibl nondimnsionl vribls: ( ) ' = l, ' = l, z' = z ν, h' = h ζ, ' = ν, ' = μν l = c l, p' = p rμν, ( ) ( ) ( ) ( ) l ( ) l ( 0 ) u' = u ζ μ ν = uν ζc, v' = v ζ μ ν = vν ζc, w' = w ζν μ ν = w ζc, whr c 0 rprsns criicl clri, givn b c 0 =(μν 0 ) /, nd, s bov,η is fr surfc lvion, ξ rprsns bhmr, u, v nd w r vloci componns, nd p is prssur. In
5 6 Nw Prspcivs in Fluid Dnmics dimnsionlss vribls, wihou h lin ovr h vribls, h fundmnl quions nd h boundr condiions r wrin [5]:. Fundmnl quions u + v + w = 0 z εu + ε uu + ε vu + ε wu = -p z εv + ε uv + ε vv + ε wv = -p z ε w + ε uw + ε vw + ε ww = -p - d z z u = s w ; v = s w ; v = u z z b c () b. oundr condiions ( ) w = + u + v, z = - + w = h + uh + vh, z = h b p = 0, z = h c (3) Ingring h firs quion () bwn h bd + ξ nd h fr surfc εη, king ino ccoun 3() nd 3(b), ilds h coninui quion (4): ( ) ( ) ( ) éη ε ξ é ξ εη u é ξ εη v = 0 (4) whr h br ovr h vribls rprsns h vrg vlu long h vricl. Thn, ccping h fundmnl hpohsis of h shllow wr hor, =ν 0 / λ < <, nd dvloping h dpndn vribls in powr sris of h smll prmr, h is ξ= 0 ξ ( s ), for ξ ( h ) λ = å λ λ = u,v,w,p,,,a (5) whr A=u + v, from coninui (), nd wih 3() nd 3(b), h following quions r obind: ( ) w = - z + - A + w (6) * ( h ) w = A + w (7) ** *
6 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ whr h simpl nd doubl srisk rprsn h vribls vlus h boom nd h surfc, rspcivl. Of () w obin, succssivl [34]: ( ) ( ) u = u,, v = v,, ( )( ) ( )( ) ( )( ) ( )( ) u = - z + - A + z + - A + w + u * * v = - z + - A + z + - A + w + v * * (8) (9) so h h vrg vlus of h horizonl componns of h vloci, on h vricl, r givn b: ( 6)( ) * s s h u = u + u A * 4 ( s )( h 0 0 )( A w ) O( s ) ( 6)( ) * s s h v = v + v A * 4 ( s )( h 0 0 )( A w ) O( s ) (0) On h ohr hnd, king ino ccoun h, from (5) nd (9) w obin: * ( s ) ( h ) λ = λ + O for λ = u, v,,, w 0 () ( s 3)( h ) ** u = u A * 4 ( s )( h )( A w ) O( s ) ( s 3)( h ) ** v = v A * 4 ( s )( h )( A w ) O( s ) () Rprsning b Γ=w + εuw + εvw + εww z h vricl cclrion of h pricls, w g Γ=w 0 + εu 0 w 0 + εv 0 w 0 + εw 0 w 0z + O( ), nd from (6), (7) nd () h following pproch is obind: ( ) G = - z + - éa ua va A * * * + éw uw vw + + O + ( s ) (3)
7 8 Nw Prspcivs in Fluid Dnmics in which h rms wihin h firs prnhsis (srigh prnhsis) rprsn h vricl cclrion whn h boom is horizonl, nd h rms wihin h scond prnhsis (srigh prnhsis) rprsn h vricl cclrion long h rl boom. I should b nod h quion (d) cn b wrin s: s G = -p z - (4) whr, b vricl ingrion bwn h boom nd h surfc, h prssur p on h surfc is obind s: p p ( s ) ( s ) = h G + ** ** = h G + ** ** (5) which, long wih (b) nd (c), llow us o obin [34]: ** ( u uu vu wu ) h z ( s ** ) ** ( v uv vv wv z ) h ( s ** ) G = G = 0 (6) or vn, givn h ( λ s ) ** = λ s ** ε( λ z ) ** η s, whr λ =(u, v) nd s =(,, ): ( ) ( ) u + u u + v u + h + s G = 0 ** ** ** ** ** ** v + u v + v v + h + s G = 0 ** ** ** ** ** ** (7) dvloping prssions (7) in scond pproch (ordr in ), h following quions of moion (8) r obind (for dils s [34]): u + uu + vu + h { é( 3)( ) ( ) ( 3)( ) P P } é Q ( )( ) Q s h h 4 + s h + + h - s + = v + uv + vv + h s é { ( 3)( h ) ( ) ê P ( 3)( h ) P ú } 4 s éh Q ( )( h ) Q s 0 ( h ) A = ( ) P = + - A - ua - va - Q = w + uw + vw ( ) w = + u + v A = u + v (8)
8 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ whr, likwis, h br ovr h vribls rprsns h vrg vlu long h vricl. In dimnsionl vribls nd wih solid/fid boom (ξ =0), h compl s of quions is wrin, in scond pproch: ( ) ( ) ν + νu + νv = 0 u + uu + vu + μh ( ) ( ) ( ) ( ) + é 3 ν + P 3 νp ν Q νq = v + uv + vv + μh ( ) ( ) ( ) ( ) + é 3 ν + P 3 νp ν Q νq = ( ) P = ν A - ua - va - A Q = w + uw + vw w = u + v A = u + v (9) whr ν =ν 0 ξ + η is ol wr dph. Th on-dimnsionl form (HΓ) of h quion ssm (9) is wrin, lso wih fid boom: ( uν) ν + = 0 ( ) ( ) ( ) ( ) νu + νuu + μνh + éν P 3 + Q + ν P + Q = 0 P = - ν u + uu - u Q = u + uu + u (0) ssuming ddiionll rliv lvion of h surfc du o h wvs (ε =ζ / ν 0 ) hving vlu clos o h squr of h rliv dph ( =ν 0 / λ), i.. O(ε) = O( ), from h ssm of quions (8), nd h sm ordr of pproimion, h following pproch is obind, in dimnsionl vribls: ( ) ( ) ν + νu + νv = 0 ( ) ( ) ( ) ( ) ( ) ( ) u + uu + vu + μh - é P + ν P + ν Q = r r v + uv + vv + μh - é 6 P 3 ν P ν Q = r r () whr ν r =ν 0 ξ is h wr column high rs, P nd Q r givn b P = (ν 0 ξ)(ū + v ) nd Q =(ūξ + v ξ ). Th momnum quions r wrin s:
9 30 Nw Prspcivs in Fluid Dnmics h ( 6) ( ) ( 3) ( ) ( 3) ν ( u v ) ( ) ν ( u v ) 0 r r u + uu + vu + μ + ν u + v - ν u + v r r = h ( 6) ( ) ( 3) ( ) ( 3) ν ( u v ) ( ) ν ( u v ) 0 r r v + uv + vv + μ + ν u + v - ν u + v r r = () (3) wih ξ =0, h compl ssm of quions (4) is obind: ( ) ( ) ν + νu + νv = 0 h ( 3) ( ) ( ) ν ( u v v v r ) h ( 3) ( ) ( ) νr ( v u u u ) u + uu + vu + μ - ν u + v + ν u r r = 0 v + uv + vv + μ - ν u + v + ν v r r = 0 (4) Furhr simplifing h quions of moion (8), rining onl rms up o ordr in, i.., nglcing ll rms of disprsiv origin, his ssm of quions is wrin in dimnsionl vribls: ( ) ( ) 0 ν + νu + νv = u + uu + vu + μh = 0 v + uv + vv + μh = 0 (5) pprochs (9), (4) nd (5) r known s Srr quions, or Grn & Nghdi, oussinsq nd Sin-Vnn, rspcivl, in wo horizonl dimnsions (HΓ modls). Th clssicl Srr quions (9) [7] r full nonlinr nd wkl disprsiv. oussinsq quions (4) onl incorpor wk disprsion nd wk nonlinri nd r vlid onl for long wvs in shllow wrs. s for h oussinsq-p modls, lso Srr s quions r vlid onl for shllow wr condiions. 3. Drivion of highr-ordr quions 3.. Wkl nonlinr pprochs wih improvd disprsiv prformnc 3... Nwτμu s ζpprτζcν To llow pplicions in grr rng of ν 0 / λ, ohr hn shllow wrs, [7] inroducd highr-ordr disprsiv rms ino h govrning quions o improv linr disprsion
10 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ propris. rdfining h dpndn vribl, [30] chivd h sm improvmn wihou h nd o dd such rms o h quions. Following [36], h ndd ussinsq quions obind b [30] r drivd in his scion, using h nondimnsionlisd scld quion ssm () (3) s h sring poin, rhr hn h procdur prsnd b Nwogu. For simplici rsons, nd wihou loss of gnrli, h on-dimnsionl ndd oussinsq quion ssm is drivd. For consisnc wih h prvious work (Scion ), h coninui quion () in wo vricl dimnsions (, z) is ingrd hrough h dph: z z ò w dz = - z ò u dz (6) - + ξ - + ξ æ ö w - w = - udz + u - u z z z - + ç ò è - + ξ ø - + z (7) Γnoing w z b w, wih ξ =0 nd using Libniz rul, h boundr condiion 3() z = + ξ givs: z æ ö w = -ç udz ç ò (8) è - + ξ ø Subsiuing (8) in h irroionli quion (), u z = w, ilds: æ z ö u = s w = -s udz z ç ò (9) è - + ø Considring Tlor sris pnsion (30) of u(, z, ), bou z = z α, whr h horizonl vloci u α (, ) dnos h vloci dph z α, u (, z α, ), his Tlor pnsion is ingrd hrough h dph from + ξ o z, ilding (3) (for dils s [36]): ( ) ( z - z ) α u = u + z - z u + u +L α α z z= z zz (30) α z= zα z ò - + ξ ( z - z ) ( - + z ) é udz = ( z + - ) u + ê - úu ê ú ( z - z ) ( - + z ) 3 3 é + ê + úu + L zz ê 6 6 ú z= z z z= z (3)
11 3 Nw Prspcivs in Fluid Dnmics Subsiuing (3) in quion (9) givs: ì é( z z ) ( z ) ü u = - s ( z z í + - ) u + ê - úu + L z ý (3) ê ú î z= z þ Γiffrniing quion (3) wih rspc o z, noing from (9) h u z =O( ) : ( s ) 4 ( z - z ) ì ü u = - s zz íu + ( z - z ) u + u + L z z= z zz ý z= z î þ = - s u + O (33) Γiffrniing quion (33) wih rspc o z nd noing h boh u z nd u zz r O( ) : { ( ) } ( s ) z= z z= z u = - s u + z - z u + L = O (34) 4 zzz z zz Rpd diffrniion of his prssion will produc prssions for h highr drivivs of u wih rspc o z nd show hm o b of O( 4) ordr or grr. Subsiuing quions (33) nd (34) bck in quion (3): ì ( - + z ) u = -s ( - + z z ) u - u + O s î z= z ( z ) u O ( ) ( ) í z 4 = -s é s ü ý þ (35) Subsiuing quions (33), (34) nd (35) in h Tlor sris pnsion (30) producs n prssion for h horizonl vloci componn u: ( z - z ) ü ( ) ý ( ) ì u = u -s ( z - z ) é( - + z ) u + u + O s î þ 4 α í α α α (36) Subsiuing h horizonl vloci (36) in quion (8) lds o n prssion for h vricl vloci componn w:
12 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ {( ) w = z u 3 ( z ) ( z ) éæ ö ç z u ( u ) é ü s ê ú ê 6 ú þ è ø - ý + O 4 ( s ) (37) Using h vlociis u (36) nd w (37) in h vricl momnum, quion (d) ilds: { é( ) α ( )} z ( ) ε - z + - ξ u + O + p + + O ε = 0 (38) This cn b rrrngd o giv n prssion for h prssur p: ( ) ( ) 4 - p = - s é z + - u + O s, s z (39) Ingring hrough h dph from z o h fr surfc εη: ìé z ü - p + p = h - z + s í + - z u + O s, s h z ê î þ 4 ( ) ú ý ( ) (40) Using h fr surfc boundr condiion 3(c) for h prssur, nd dnoing p z simpl s p givs: ìé z ü p = h - z + s íê + - z u + O s, s î þ 4 ( ) ú ý ( ) (4) Subsiuing h quions for h horizonl vloci componn (36), h vricl vloci componn (37) nd h prssur (4) in h horizonl momnum quion (b) givs h oussinsq momnum quion: ( z - z ) ( ) ì ü -s ( - ) é( - + ) + ý î þ ìé z ü + u u + h + s + - z u = O s, s î þ u z z z u u í 4 íê ( ) ú ý ( ) (4)
13 34 Nw Prspcivs in Fluid Dnmics or ì ü u + u u + h + s z é - u + u = O s, s z ( ) ( ) ý ( ) 4 í î þ (43) Th scond quion of h oussinsq ssm is dvlopd b firs ingring h coninui quion () hrough h dph + ξ: h æ ö udz - u h u w w 0 h h = ç ò è - + ø (44) Using Libniz Rul nd h kinmic boundr condiions h bd z = + ξ 3() nd h fr surfc z = εη 3(b) givs: h æ ö h + udz 0 = ç ò (45) è - + ø From h prssion (36) for h horizonl vloci u: h ò - + h ì é ( z z ) - udz = ( - + h ) u -s ( z ) u í ê ú é - + ê ú î - + εη 3 é ü ( z - z ) 4 + ê ú u O ý + ( s ) ê 6 ú - + þ (46) or h ò - + ( - + z ) ìé z udz = ( - + h ) u -s ( z ) u í ê - ú é - + ê ú î 3 é 3 z ( - + z ) ü 4 + ê- + úu O ( s, s ý + ) ê 6 6 ú þ (47) ilding:
14 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ h ò - + ( - ) ìé udz = ( - + h ) u -s ( ) z ( z ) u í ê ú é - + ê ú î 3 é ( - ) ( - ) z ( - ) z ü 4 + ê + + ú( u ) O ( s, s ý + ) ê 6 ú þ (48) nd hus h ò - + ìé - udz = ( - + h ) u + s z ( ) ( ) u íê + ú - é - î é z ( - ) ü 4 + ê - ú( - )( u ) O ( s, s ý + ) ê 6 ú þ (49) Subsiuing quion (49) in h fr surfc quion (45) givs h oussinsq coninui quion: ìæ - ö h + é( h ) u s z ( ) é( ) u íç è î ø æ z ( - ) ö ü 4 + ç - ( - )( u ) O( s, s ý = ) ç 6 è ø þ (50) Rurning o dimnsionl vribls, unscld form, quions (43) nd (50) r wrin: z u + u u + μh + z ( ν u ) + ( u ) = 0 (5) r h éæ ν ö æ z ν r r + é( ν h 0 ) u ( ) ( ) 0 + z ν ν u ν u + êç + + r r - = r ú ê ç 6 è ø è ø ú ö (5) Sing h rbirr dph z α =αν 0, whr α 0, h ssm (5) (5) is rwrin: u u u μ ν ν ( u + + h + é ) ( ) 0 r r ν u + = r (53)
15 36 Nw Prspcivs in Fluid Dnmics é æ ö æ ö 3 h + é( ν h ) u ν ( ν u ) ν ( u ) 0 + r + êç = r r ç 6 r ú ê è ø è ø ú (54) In wo dimnsions, h quion ssm (53) (54) is wrin:. ( ν h ) h + Ñ é + u r ì æ ö æ ö 3 ü + Ñ íç + ν Ñ éñ.( ν ) + ν (. ) 0 r r - Ñ Ñ = r ý u ç 6 u î è ø è ø þ (55)... r r r ( ) μ h ν é ( ν ) ν ( ) u + u Ñ u + Ñ + Ñ Ñ u + Ñ Ñ = 0 u (56) whr rprsns h wo-dimnsionl grdin opror wih rspc o h horizonl coordins (, ) ( = /, / ), nd h vloci vcor u(,, )=(u, v) rprsns h wodimnsionl vloci fild dph z =αν Bjξ ζd Nζdζτπζ s, ζd Lξu ζd Su s ζpprτζcνs Sring from h sndrd oussinsq quions nd doping h mhodolog inroducd b [7] [] prsnd nw pproch h llows for pplicions unil vlus of ν 0 / λ o h ordr of 0.5, nd sill wih ccpbl rrors in mpliud nd phs vloci up o vlus of ν 0 / λ nr n ddiion nd subrcion procss, using h pproimion u = μ η nd considring disprsion prmr β in h momnum quion of h HΓ ssm (4), ji nd Ndok obind n improvd s of oussinsq quions for vribl dph, wih β vlu obind b comprison of h disprsion rlion of h linrizd form of h rsuling quion wih scond-ordr Pdé pnsion of h linr disprsion rlion ω / μπ =nh(πν r ). In ordr o improv disprsion nd linr sholing chrcrisics in h ji nd Ndok s quions, [3] inroducd wo uning prmrs, α nd γ, so h β =.5α 0.5γ. Th nonlinri in h prvious oussinsq-p modls ws improvd b Liu nd Sun dding highr-ordr rms ccur o h ordr of O( ε ). Th HΓ sndrd oussinsq quions nd h pprochs of ji nd Ndok nd Liu nd Sun r idnifid wihin h following ssm of quions (57) for wr of vribl dph: ν ( νu) 0 h {( ) ( g ) 6} ( 6) ( ) + = u + uu + μ ν u r - - g μν h + + ν u + μν h r r r ( ) h r r ( s ) ν u μν = O (57)
16 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ fr linrizion of h quions ssm (57), [3] obind h following disprsion rlion (58): πν é ( 6 r + - g ) ( ) ( g ) w π ν r = (58) μπ + + π ν / - + π ν / 6 r r Compring quion (58), wrin in rms of h phs spd (59) C + ( - g 6 )( πνr ) ( )( ) ( g )( ) w é = = μν ê ú r π ê πν / πν / 6 ú r r (59) wih h linr disprsion rlion ω / μπ =nh(πν r ), using h pproch (60) ( πνr ) ( πν ) w é C = = ( μν ) nh Aξr r ( πνr ) = μν ê ú + O é r ( πν) π ê ê ú 5ú + r (60) llows o obin h bs vlus for h prmrs α nd γ: α =0.308 nd γ = Considring ppropri vlus for h uning prmrs α nd γ, w cn idnif wihin h quion ssm (57): Th sndrd oussinsq quions b sing α =γ =0 Th ji nd Ndok quions considring α =γ =0.0 Th Liu nd Sun quions wih α =0.308 nd γ = visul comprison of numricl rsuls of h ndd oussinsq pproimion (57), wih α =0.308 nd γ = ), shown in [, ] nd [3], wih similr sud prformd b [37], using h ndd oussinsq (53) (54) modl (Nwogu s pproch, wih α = 0.53) shows no rlvn diffrncs in h grphs. In his rgrd, i is worh rmmbring [4] ζρντuμν ν mντds τλ drξvζξτ ζr dξλλr, ν rsuρξμ dξsprsξτ rρζξτs τλ νs dd Bτussξsq quζξτs ζr sξmξρζr, ζd mζ η ντuμν τλ ζs ζ sρξμν mτdξλξcζξτ τλ ν scτd-τrdr Pζdé ζpprτξmζ τλ ν λuρρ dξsprsξτ rρζξτ. 3.. Full nonlinr pprochs wih improvd disprsiv prformnc Insd of using h horizonl vloci crin dph, ohr nsions of h oussinsq quions hv bn md b using h vloci ponil on n rbirr dph, lso wih uning prmr. Wi ζρ. (995) [39] usd h Nwogu s pproch o driv oussinsqp modl which rins full nonlinri b including O( ε ) rms no considrd in h
17 38 Nw Prspcivs in Fluid Dnmics Nwogu s (53) (54) ssm, nd hus improving h nonlinri o O(ε)=. Wi ζρ., nd lr [6] Gobbi ζρ., drivd fourh-ordr oussinsq modl in which h vloci ponil is pproimd b fourh-ordr polnomil in z. In rms of non-dimnsionl vribls, boh considr h boundr vlu problm for ponil flow, givn b: 0, j + m Ñ j = - + h zz j + m Ñν. Ñ j = 0, z = - + z - é h + j + ( ) ( ) 0, ê Ñ j + j z z ú = = h m h + Ñj. Ñh - j = 0, z = h z m z (6) whr, s bov, z is h vricl coordin sring h sill wr lvl ν 0 (, ) nd poining upwrds, scld b picl dph ν 0, nd η is h wr surfc displcmn scld b rprsniv mpliud ζ. Th wo dimnsionlss prmrs ε nd µ r dfind s ε =ζ / ν 0 nd µ =(π 0 ν 0 ), wih rprsniv wv numbr π 0 =π / λ, so µ =(π). Tim is scld b π 0 (μν 0 ) /, nd φ, h vloci ponil, is scld b εν 0 (μν 0 ) /. W us h nondimnsionl wr lvl ν ξ insd of ξ. Ingring h firs quion of (6) ovr h wr column, nd using h ppropri boundr condiions, h coninui quion is obind: h + Ñ. M = 0 (6) εη whr M = +ξ φdz. Rining rms o O ( µ ), nd dnoing φα s h vlu of φ z = z α (, ), n pproim vloci ponil is givn b:. ( ) m, ( z z) ( ν ) ( z z ) O( 4 - ) j = j + m - Ñ Ñ j + - Ñ j + m (63) Subsiuing quion (63) ino (6), mss flu consrvion quion is obind [39]:.. ì æ ö ì ì é z h + Ñ íç ν + h z ( ν j m j ) j è - ø íñ + íñ ê Ñ Ñ + Ñ - ú î î î ê ú é ( ν h ) ν hν ( h ) üüü ê - - ú + Ñ éñ. ( ν Ñj ) - Ñ Ñ j = 0 - ýýý 6 þþþ (64)
18 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ Similrl, subsiuing (63) ino h hird quion of (6), momnum quion is obind in rms of h vloci ponil. Thn, givn h z = z α, u α = φ α, full nonlinr vrsion of oussinsq p modl in rms of η nd u α is wrin:.. ( ( ) ) ú ( u ) ì ì ìé z h + Ñ í + h í + m í - - h + h Ñ Ñ 6 î î î ê ú é üüü + êz + ν - Ñ Ñ. ν = O ú þ þþ æ ö ç ν ν ν u - ê è ø ( h ) é ( u ) ( m - - ýýý ) (65). ( ) O( 4 ) u + u Ñ u + Ñ h + m R + m S = m (66) whr.... é R = z Ñ( Ñ u ) + z Ñ éñ ( ν u ) - Ñ ( h ) Ñ + hñ ( ν - - ) ê u u ú (67) ì S = Ñ í - u. Ñ Ñ. u + - u. Ñ Ñ. u î ( z h )( ) é ( ν ) éz ( h ) - ( )( ) ê ú + Ñ é { Ñ.( ν u ) + hñ. u - } ü ý þ (68) I should b nod h Nwogu s pproimion is rcovrd b nglcing highr-ordr rms. Numricl compuions show h his modl grs wll wih soluions of h full ponil problm ovr h rng of rlvn wr dphs. high-ordr, prdicor corrcor, fini diffrnc numricl lgorihm o solv his modl ws dvlopd nd is prsnd in [5] for h on- nd wo-lr modls (s Scions 3.. nd 3..). Considring on lr onl, h corrsponding numricl modl h is h bsis of h COULW VΔ modl is prsnd lr, in Scions 4..3 nd To improv h ccurc of numricl modls, i hs bn common prcic h us of highordr polnomils o pproim h vricl vloci dpndnc. Howvr, his rquirs vr lbor nd pnsiv numricl clculion procdurs. diffrn pproch is suggsd b [6], which consiss of using qudric polnomils, mchd inrfcs h divid h wr column ino lrs. In his rgrd, i is worh mnioning [6] "νξs ζpprτζcν ρζds τ ζ s τλ mτdρ quζξτs wξντu ν νξμν-τrdr spζξζρ drξvζξvs ζssτcξζd wξν νξμν-τrdr pτρτmξζρ ζpprτξmζξτs".
19 40 Nw Prspcivs in Fluid Dnmics 3... Mζνmζξcζρ mτdρ λτr τ-ρζr Γfining h prmrs S =.u nd T =. ( ξ) u + ( / ε)( ν ξ / ), h modl uss h following pproch for h coninui quion (o compu η vlus), in nondimnsionl vribls:. ν- h + + Ñ é( h + ν ) u - ìé ( h + ν ) π -. í ê 6 ú î é h - ν ü + ê - + úñ ý = ê ú þ h + ν- - m Ñ ê - ú ÑS - 4 ( h ν ) π T O ( m - ) (69) whr u = horizonl vloci vcor, π =α ν + β η, α nd β r cofficins o b dfind b h usr. Th ind mns on-lr modl. To compu h vloci componns (u, v), h following pproch of h momnum quion is solvd, in nondimnsionl vribls:. u ì π ü + u Ñ u + Ñ h + m í Ñ S + π ÑT ý î þ é ( u. π ) T π ( u. T ) π ( u. π ) S π é æ T ö + Ñ( u. Ñ S ) ú + m êt ÑT - Ñ h ç ú ú è ø æ h S ö + m Ñ ç hs T - -h u. ÑT è ø é h 4 + m ( ) ( ) S. S Ñ ê - u Ñ ú = O m + m Ñ Ñ + Ñ Ñ + Ñ Ñ (70) Th horizonl vloci vcor is givn s: U ìz - π 4 = u - m S z π T O í Ñ + - Ñ + î ü ( ) ý ( m ) þ (7) This on-lr modl, ofn rfrrd o s h full nonlinr, ndd oussinsq quions in h lirur (.g. [38]), hs bn mind nd pplid o significn n. Th wkl nonlinr vrsion of (69) (7) (i.., ssuming O(ε)=O( µ ), hrb nglcing ll nonlinr disprsiv rms) ws firs drivd b [30]. Through linr nd firs-ordr nonlinr nlsis of h modl quions, Nwogu rcommndd h z = 0.53ν, nd h vlu hs bn
20 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ rcommndd nd dopd b mos rsrchrs who us hs quions. Rfs. [] nd lr [38] usd h Nwogu s pproch o driv high-ordr modl which rins "full nonlinri" b including rms no considrd in h Nwogu s pproch. Compring Liu's nd Wi nd Kirb's quions, hr r som diffrncs h cn b ribud o h bsnc of som nonlinr disprsiv rms in Wi nd Kirb [9]. Th bov on-lr quions (69) nd (70) r idnicl o hos drivd b [] Mζνmζξcζρ mτdρ λτr wτ-ρζrs Γils bou h wo-lr mhmicl modl r prsnd in [5] nd [4]. Th modl consiss of coninui quion, momnum quion for h uppr lr nd mching quion for h vloci in h lowr lr. Ths quions r solvd using n ppropri numricl mhod o compu vlus for h fr surfc lvion η nd h vloci componns (u, v). In dimnsionl vribls, his s of quions is wrin ([4]):. η + Ñ é( h z ) ( z ν ) r - u + + u ì 3 3 éz + ν ( z + νr ) π é r z - ν ü r - Ñ. íê - úñ S + ê - ( z + νr ) π T úñ ý 6 îê ú ê ú þ 3 3 ìéh - z ( h - z ) π éh - z ü - Ñ. íê - úñ S + ê - ( h - z ) π Ñ T = 0 ú ý ê 6 ú î þ. u + Ñ ( u u ) + μñh é π æ h ö + ê Ñ S + π ÑT - Ñ S - Ñ( ht ) ú ç ê è ø ú é h + Ñ ê ( T + hs ) + ( π -h )( u. Ñ ) T + ( π -h )( u. Ñ) S + ( T + hs ) R R n S η λ T ú é Ñ - Ñ u æ π ö h -Ñ Ñ S + π Ñ T + Ñ Ñ S + hñ ç æ T ö 0 ç ú = è ø è øú (7) (73) u π - z π - z + Ñ S + ( π - z ) Ñ T = u + Ñ S + ( π - z ) ÑT (74) whr S =.u, T =ζ(s S ) + T, S =.u, nd T =.(ν r u ). R η = brking-rld dissipion rm, R λ = λ / (ν r + η) u η u η ccouns for boom fricion, whr u η = vloci vlud h
21 4 Nw Prspcivs in Fluid Dnmics sfloor, nd λ = boom fricion cofficin, picll in h rng of 0 3 0, ν T = consn dd viscosi, =( /, / ), π = 0.7ν r = vluion lvl for h vloci u, ζ = 0.66ν r = lr inrfc lvion, s = vluion lvl for h vloci u, nd η = fr surfc lvion HD Srr s quions wih improvd disprsiv prformnc To llow pplicions in grr rng of ν 0 / λ, ohr hn shllow wrs, nw s of ndd Srr quions, wih ddiionl rms of disprsiv origin, is dvlopd nd sd in [] nd [] b comprisons wih h vilbl s d. Th quions r solvd using n fficin fini diffrnc mhod, whos consisnc nd sbili r sd in h work b comprison wih closd-form solir wv soluion of h Srr quions. From h quion ssm (0), b dding nd subrcing rms of disprsiv origin, using h pproimion u = μ η nd considring h prmrs α, β nd γ, wih β =.5α 0.5γ, llows o obin nw ssm of quions wih improvd linr disprsion chrcrisics: ( uν) ν + = 0 ν u + uu + μ( ν + ) + ( + )( W u - νν u ) - ( + b ) u 3 ν + μw ( ν + ) - μνν ( ν + ) - b μ ( ν + ) - νν uu 3 ν u u uu ν u ν u ν ( ) ( ) ( ) ( ) ν + ( W + ν ) uu + u = 0 (75) fr linrizion of h quion ssm (75), h disprsion rlion (58) is obind. s for h oussinsq pproch obind b Liu nd Sun, quing quion (58) wih h linr disprsion rlion ω / μπ =nh(πν r ), using h pproch (60), vlus of α =0.308 nd γ = r obind, so h β =0.0. I should b nod h h Srr s quion ssm (0) is rcovrd b sing α =β =0. 4. Numricl formulions nd pplicions 4.. HD Boussinsq-p pprochs 4... WACUP umrξcζρ mτdρ n nsion of h oussinsq modl (4) o k ino ccoun wv currn inrcions hs bn drivd nd prsnd in [5]. This modl is nmd W CUP (ζ HD WAv Pρus CUrr
22 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ Bτussξsq-p mτdρ). Wih dimnsionl vribls, king mn quniis of h horizonl vloci componns U =(u + u c ) nd V =(v + v c ), whr ind c rprsns currn nd u =U - u c nd v =V - v c, h finl s of hs quions r wrin s follows: ( ) ( ) 0 ν + νu + νv = (76) νr ( ) ( ) U + UU + VU + μ ν + - U + V 3 νr æ ö - éuc ( U + V ) + vc ( U + V ) + ν + u + v r c c 3 ç è ø τ τ s η - ν ( U + U ) - + = 0 ρ ρν ρν (77) νr ( ) ( ) V + UV + VV + μ ν + - U + V 3 νr æ ö - éuc ( U + V ) + vc ( U + V ) + ν + u + v r c c 3 ç è ø τ τ s η - ν ( V + V ) - + = 0 ρ ρν ρν (78) whr τ s nd τ η rprsn srsss on surfc nd boom, rspcivl. Th sndrd oussinsq modl (4) nd h ndd ssm of quions (76) (78) r solvd in [8] nd [5], rspcivl, using n fficin fini lmn mhod for spil discrizion of h pril diffrnil quions. Firsl, h (U, V) drivivs in im nd hird spil drivivs r groupd in wo quions. This mns h n quivln ssm of fiv quions is solvd insd of h originl quion ssm (76) (78). Th finl quion ssm ks h following form: ν + νu + Uν + νv + Vν = 0 (79) ( ) r + u r + v r = -uu - vu - μ ν + c c νr æ ö + é u U + U + v V + V - ν + u + v c c r c c 3 ç è ø é s η + ên + ν ( + u + v ) ( U U ) 0 ρ r c c 3 ú = rν rν ( ) ( ) ( ) ( ) (80)
23 44 Nw Prspcivs in Fluid Dnmics ( ) s + u s + v s = -uv - vv - μ ν + c c νr æ ö + é u U U v V V ν u v c c r c c 3 ê ç + + ú è ø ( ) ( ) ( ) ( ) é s η + ên + ν ( + u + v ) ( V V ) 0 ρ r c c 3 ú = rν rν (8) ( ) νr U - U + U = r (8) 3 ( ) νr V - V + V = s (83) 3 I should b nod h wkl vricl roionl flows wr ssumd, which sricl corrspond o limiion of h numricl mhod. s h vlus of vribls ν, U, V, r nd s r known im, w cn us numricl procdur bsd on h following sps o compu h corrsponding vlus im + (for dils s [5]):. Th quion (79) llows us o prdic h vlus of vribl ν(ν p + ), considring h known vlus of h, U nd V im in h whol domin.. Δquions (80) nd (8) mk i possibl o prdic h vlus of vribls r (r p + ) nd s (s p + ), king ino ccoun h vlus of U, V, r, s nd ν + =0.5ν + 0.5ν p + known for h whol domin. 3. Soluions of quions (8) nd (83) giv us h vlus of h mn-vrgd vloci componns U nd V (U + nd V + ), king ino ccoun h prdicd vlus of r nd s (r p + nd s p +, rspcivl). 4. Δquion (79) llows us o compu h dph ν im + (vlus of ν + ) considring h vlus of vribls ν, U +05 =0.5U + 0.5U + nd V +05 =0.5V + 0.5V + known for h whol domin. 5. Δquions (80) nd (8) llow us o compu h vlus of vribls r nd s im + (vlus of r + nd s + ), king ino ccoun h vlus of r, s ν +05 =0.5ν + 0.5ν +, U +05 =0.5U + 0.5U + nd V +05 =0.5V + 0.5V + known for h whol domin. Th Prov-Glrkin procdur is uilizd o chiv soluions for h unknowns ν, r nd s. ccording o h wighd rsidul chniqu, minimizion rquirs h orhogonli of h rsidul R J o s of wighing funcions W ξ,j, i..,
24 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ ò W R dd = 0, ξ =, L, ξ, J J (84) D whr h gnrl form of h wighing funcions pplid o hs quions is dfind s: ( ) d ( ) W = N + d N + N, ξ =, L, ξ, J ξ uξ vξ (85) ξ ξ nd whr h cofficins δ uξ, nd δ vξ r funcions of: (ξ) h locl vlociis U nd V; (ξξ) h rio of h wv mpliud o h wr dph, nd (ξξξ) h lmn lngh. To illusr his procdur, compl soluion of quions (79) (80) nd (8) is prsnd hr in dil. Inroducing in quion (79), h pproimd vlus r givn b: p» pˆ = å N p (86) = ξ ξ h following rsidul R 79 is obind: R = νˆ + νu ˆ ˆ + Uν ˆ ˆ + νv ˆ ˆ + Vν ˆ ˆ (87) 79 Th R 79 rror minimizion lds o h following quion: ò D ò ˆ ˆ ( ˆ ˆ ˆ ˆ ˆ ˆ ˆ ) W R dd = W ν + νu + Uν + νv + Vν dd ξ,79 79 D ξ,79 é = ò W êå N ( ν ) + å( N ) U å N ν + å N U å( N ) ν D ê dd = ξ,79 j j π π j j π π j j j= π= j= π= j= ( ) ( ) + N V N ν + N V N ν π π j j π π j j ú π= j= π= j= ú å å å å 0 (88) In h mri form, his quion m b wrin s: Aν + Bν = 0 (89) whr
25 46 Nw Prspcivs in Fluid Dnmics ò ζ = W N dd ; ξ, j =, L, ξ, j D ξ,79 j ò ( ) ( ) j ò å π η = W N U N dd + W N U N dd ξ, j D ξ,79 π π D ξ,79 π j π= π= ò ( ) å ( ) + W N V N dd + W N V N dd ; ξ, j =, L, D å å ξ,79 π j ξ,79 π π π D j π= π= ò (90) Th rsidul R 80 is wrin s: R = rˆ + uˆ rˆ + vˆ rˆ + uu ˆ ˆ + vu ˆ ˆ 80 c c ˆ ˆ ( ˆ νr + μ ν + ) - é( uˆ ) ( Uˆ + Uˆ ) + ( vˆ ) ( Vˆ + Vˆ c c ) 3 ˆ é + ν ˆ ˆ ˆ ˆ ˆ r ê + u + u + v + v c c c c ( ˆ ˆ s η - n U + U ρ ) - + rν rν ( ) ( ˆ ) ( ) ˆ ( ) ( ˆ ) ( ) ˆ ( ) ú (9) I should b nod h h rm 3 ν r(ξ + u c ξ + v c ξ )(V + V ) of quion (80) is of ordr 4 or grr. For his rson, i is no considrd in h numricl dvlopmns. Similrl, nd for h sm rson, considring λ =ν r / 3, ll rms involving λ in h numricl dvlopmns r omid. Th Grn s horm is usd o solv h scond drivivs prsn in quion (80) (rsidul w obin: R 80 ), nd in quions (8) o (83), i.., considring p^ =(U^, V^ ), from p^ + p^ n ( ˆ ˆ é ) ( ) ( ) å ò W p + p d D = W N N p d D ξ, ρ ò + D D ξ, ρ ê j j j ú (9) j= nd so n W ξ,ρ j= (N ) j + (N ) j p j d = (W ) ξ,ρ (N ) j p j d j= (W ) ξ,ρ j= (N ) j p j d + W Γ ξ,ρ (N ) j p j dγ ; p =(U, V ) j= (93) Rining rms up o ordr 3, h R 80 rror minimizion lds o:
26 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ ò D ì é W R d W N r N u N r î ê D = ξ,80 80 ò í ξ,80 êå ( ) + j π ( c ) ( ) j å D πå j j j= π= j= ( ) ( ) ( ) ( ) å å å å å å + N v N r + N u N U + N v N U π c π j π π j π π j j j j π= j= π= j= π= j= ( ν ) r ρ + μå( N ) ( ν + ) ú - ρ ( ) ( c ) ( c ) j j å N å N é u U + v V π π π j= ú ρ= 3 π= é + W ê N N + N ν N u N ê ( ν ) r π å å( ) ( ) å ( ) å( ) ( ) å( ) ( ) ξ,80 π j j ρ r ρ π c π j j π= j= ρ= π= j= + å N ( ν ρ r ) ( ) ( c ) ( ) ( ) ρå N v π π å N ú j j ρ= π= j= ú é + N ( ν ) N ( u ) ( % ρ r π c ) + Nπ ( vc ) ( % å ) ρ êå π å n π ú - U ρ ρ= π= π= ü -W N é,80 ( ) ( ) 0 ξ å π ê - N ν dd = s η j j π π ú å ý π= j= ν þ (94) whr ( % ) = -( W ) ( N ) ( ), ( % ) = -( W ) ( N ) ( ) å ξ,80 j j ξ,80 j j j= j= å (95) nd é p = - ê W N + W N p p = U V ξ, J j ξ, J j j ê j= j= ú ( ) ( ) ( ) ( ) ú, (, ) å å (96) In h mri form, his quion m b wrin s: Ar + Br = C (97) whr ζ =,,,, ξ, j ò W N dd ξ j = L ξ,80 j (98) D é η =,,,, ξ, j ò W N u N N v N d ξ j D ξ,80 êå + π c π j π c π ú D = L (99) j π= π= ( ) ( ) å ( ) ( )
27 48 Nw Prspcivs in Fluid Dnmics ì é c = - ò íw êå N u å( N ) U + å N v å( N ) U î ê ξ D ξ,80 π π j j π π j j π= j= π= j= ( ν ) r ρ + μå( N ) ( ν + ) ú - å Nρ å( N ) ú 3 é( uc ) U + ( vc ) V é N u N + W ê ê N N + N ν + å N ( ν ρ r ) ( ) ( ) ( ) ( ) ρå N v π c π å N ú j j ρ= π= j= ú é + N ( ν ) N ( u ρ r π c ) ( % ) + Nπ ( vc ) ( % å ) ρ ρ êå π å π ú -n U ρ= π= π= ü -W N é,80 ( ) ( ) N ν d 0, ξ,. ξ å π ê - D = = s η j j ý π π ú å K π= j= ν þ j j π π π j= ρ= π= ( ν ) r π å å( ) ( ) å ( ) å( ) ( ) å ( ) ( ) ξ,80 π j j ρ r ρ π c π j π= j= ρ= π= j= j (00) Th rsidul R 8 is wrin s: ˆ ˆ ˆ ˆ ν æ r U U 8 ö R = U rˆ 3 ç è ø (0) ccording o Glrkin s procdur, fr using ingrion b prs (or Grn's horm) o rduc h scond drivivs, h R 8 rror minimizion lds o h following quion: W ξ,8 R 8 = d {W ξ,8 N j U j j= (ν + r ) π N π π= 3 (W ) ξ,8 j= (N ) j + (W ) ξ,8 (N ) j U j j= W ξ,8 N j r j }d N (ν r ) π j= Γ π W 3 ξ,8 (N ) j U j dγ (0) Th ls rm of (0) cn b wrin s: Γ N π (ν r ) π 3 (ν W ξ,8 (N ) j U j dγ = r ) p Γξ N p W 3 q,8 (N ) r U r dγ ξ (ν + r ) p Γ N p W 3 q,8 U dγ (03)
28 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ whr p, q =,,, bing h numbr of nods in h corrsponding lmn sid coincidn wih h boundr domin, Γ ξ rprsns h lmn sids wihin h domin, wih h corrsponding ingrl null bcus h rsuling lmn conribuions r qul, bu wih opposi signls, nd Γ rprsns h lmn sids coincidn wih h boundr domin. ccordingl, n quivln form of quion (0) m b wrin s follows: W ξ,8 R 8 = d {W ξ,8 N j j= ν ( + r ) π N π π= 3 (W ) ξ,8 j= (N ) j + (W ) ξ,8 (N ) j }U j d j= = W ξ,8 N j r j d + N (ν r ) p j= Γ p W 3 q,8 U dγ p, q =,, (04) In h mri form, his quion m b wrin s: AU = B (05) whr ( νr ) ì é,,8 ( ) ( ),8 ( ) ( ) ü π ζ = ξ j ò íwξ å N + j å Nπ ê W ξ å N + W N d D j å,8 úý D 3 ξ j î j= π= ê j= j= ú þ (06) η ξ = W ξ,8 N j r j d + N (ν r ) p j= Γ p W 3 q,8 U dγ p, q =,,. (07) s rcommndd in [5] ζ suξζηρ μrξd ξs τrmζρρ crucξζρ τ ν succss τλ ζ λξξ ρm mτdρ. I τur cζs, ν λτρρτwξμ ruρs mus η λuρλξρρd λτr ξs μrζξτ.. Eρm sξd ρτwr νζ ν ρτcζρ dpν. b. Mξξmum τλ 0 τ 5 ρms pr wζv ρμν. c. Cτurζ umηr ζρwζs ρτwr νζ τ ξ ν wντρ dτmζξ Rζρ cζs sud usξμ ν WACUP mτdρ Th forificion of S. Lournço d Cbç Sc (lighhous of ugio) Tgus sur (Porugl) hs ndurd ovr h cours of four cnuris h coninuous cion of wvs nd currns,
29 50 Nw Prspcivs in Fluid Dnmics s wll s bhmric modificions rsuling from h movmn of significn quniis of snd in h r whr i is locd. Wih h innion of prvning h dsrucion of his forificion, svrl sudis wr conducd o vlu h bs procion srucur. Th sudis hv ld o prociv srucur which consiss of circulr dissipion plform, wih lvl of m (HZ) nd bou 80 m rdius (Figur ). Figur. Submrgd dissipion plform o proc h ugio lighhous, siud h mouh of h Tgus sur. Th wv currn oussinsq-p modl W CUP ws usd o obin h im-dpndn hdrodnmic chrcrisics of h join cion of rlivl common wv ovr h high flow id currn. Th wv chrcrisics r: wv high, H = 3.5 m, priod T = s nd dircion = 80. Figur shows h fr surfc lvl whn h wv pprochs h plform nd is cion on h ugio lighhous. Figur 3 shows fr surfc wr lvl, in qusisionr s. s cn b sn, h wv cion on h forificion ws drsicll rducd s consqunc of h wv brking, rfrcion nd diffrcion on h dissipion plform consrucd round h forificion. Figur. Prspciv of h fr surfc obind b simulion round h ugio lighhous, siud in h Tgus sur, Porugl, in rnsin condiion.
30 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ Figur 3. Procion of h ugio lighhous siud h mouh of h Tgus sur. Prspciv of h fr surfc obind wih numricl simulion, in qusi-sd s COULWAVE τ-ρζr mτdρ numricl schm similr o h of [38] nd [39] is uilizd b [5], wih h inclusion of r nonlinr rms. sicll using h sm high-ordr prdicor corrcor schm, [5] dvlopd numricl cod (COULW VΔ) bsd on Nwogu s quions for on nd wo lrs. Prmrizions of boom fricion nd wv brking hv bn includd in h cod, s wll s moving boundr schm o simul wv runup nd rundown. fini diffrnc lgorihm is usd for h gnrl on- nd wo-lr modl quions. ccording o [9], ν quζξτs ζr sτρvd usξμ ζ νξμν-τrdr prdξcτr-cτrrcτr scνm, mpρτξμ ζ νξrd τrdr ξ ξm pρξcξ Adζms-Bζsνλτrν prdξcτr sp, ζd ζ λτurν τrdr ξ ξm Adζms-Mτuρτ ξmpρξcξ cτrrcτr sp [3]. lso in ccordnc wih [9], h implici corrcor sp mus b ird unil convrgnc cririon is sisfid. In ordr o solv numricll h nondimnsionl quions (69) (7), hs r prviousl rwrin in dimnsionl vribls. Thn, o simplif h prdicor corrcor quions, h vloci im drivivs in h momnum quions r groupd ino h dimnsionl form (for dils s [5]): π -h U = u + u + π - ν u - u + ν u r r ( h )( ) h éh ( ) π -h V = v + v + ( π -h )( ν v r ) - h éh v + ( ν v r ) ê ú (08) (09) whr subscrips dno pril drivivs. For rsons of sbili nd lss irions rquird in h procss of convrgnc, h nonlinr im drivivs, risn from h nonlinr disprsion rms η(.(ν r u α ) + ν r / ε ) nd ( η / ).uα, cn b rformuld using h rlions:
31 5 Nw Prspcivs in Fluid Dnmics... é æ ν ö é æ ν ö é æ ν ö Ñ h ç Ñ ( ν u ) + = Ñ h ç Ñ ( ν u ) + - Ñ h ç Ñ ( ν u ) + ê è øú ê è øú ê è øú r r r r r r... æ ö æ ö h h Ñ ç Ñ u u u = Ñ Ñ - Ñ Ñ ç è ø è ø ( hh ) (0) () Th plici prdicor quions r: ( ) + Δ - - η = η + E - E + E ξ,j ξ,j ξ,j ξ,j ξ,j () ( ) ( ) 3( ) ( ) + Δ U = U + F - F + F + F - F + F ξ,j ξ,j ξ,j ξ,j ξ,j (3) ξ,j ξ,j ξ,j ( ) ( ) 3 ( ) ( ) + Δ V = V + G - G + G + G - G + G ξ,j ξ,j ξ,j ξ,j ξ,j (4) ξ,j ξ,j ξ,j whr ( h ) ( h ) E = -ν - é + ν u - é + ν v r r r ì éæ ö æ ö ü + í( h + νr ) êç ( h - hν + ν r r ) - π S + ç ( h - νr ) - π T úý î è 6 ø è ø þ ì éæ ö æ ö ü + í( h + νr ) êç ( h - hν + ν r r ) - π S + ç ( h - νr ) - π T úý î è 6 ø è ø þ (5) ( ) ( ) h ( h ) F = - é u + v - μ - πν - π ν + Eν + ν é - ée( hs T ) + - ( π h )( us vs ) ê - + ú - é( π - h )( ut + vt ) - é( T + hs) ê ú r r r r (6) h - π F = v - ( π - h )( ν v r ) + h éh v + ( ν v r ) ê ú (7)
32 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ ( ) ( ) h ( h ) G = - é u + v - μ - πν - π ν + Eν + ν ê ú é - ée( hs T ) + - ( π - h )( us + vs ) ê ú r r r r - é( π - h )( ut + vt ) - é( T + hs) ê ú (8) h - π G = u - π - ν u + u + ν u r r ( h )( ) h éh ( ) (9) nd ( ) ( ) S = u + v ; T = ν + ν u + ν v (0) r r r ll firs-ordr spil drivivs r diffrncd wih fourh-ordr ( 4 = 4 ) ccur quions, which r fiv-poin diffrncs. Scond-ordr spil drivivs r pproimd wih hr-poin cnrd fini-diffrnc quions, which r scond-ordr ccur. Th fourh-ordr implici corrcor prssions for h fr surfc lvion, η, nd h horizonl vlociis, u nd v, r: ( ) + Δ η = η + E + E - E + E ξ,j ξ,j ξ,j ξ,j ξ,j ξ,j () 4 + ( ) ( ) ( ) + Δ U = U + F + F - F + F + F - F ξ,j ξ,j ξ,j ξ,j ξ,j ξ,j () ξ,j ξ,j 4 + ( ) ( ) ( ) + Δ V = V + G + G - G + G + G - G ξ,j ξ,j ξ,j ξ,j ξ,j ξ,j (3) ξ,j ξ,j 4 s nod in [5], ν ssm ξs sτρvd η λξrs vζρuζξμ ν prdξcτr quζξτs, ν u ζd v ζr sτρvd vξζ (08) ζd (09), rspcξvρ. Bτν (08) ζd (09) ξρd ζ dξζμτζρ mζrξ ζλr λξξ dξλλrcξμ. Tν mζrξcs ζr dξζμτζρ, wξν ζ ηζdwξdν τλ νr (du τ νr-pτξ λξξ dξλλrcξμ), ζd ν λλξcξ Tντmζs ζρμτrξνm cζ η uξρξzd. A νξs pτξ ξ ν umrξcζρ ssm, w νζv prdξcτrs λτr η, u ζd v. N, h corrcor prssions r vlud, nd gin u nd v r drmind from (08) nd (09). lso in ccordnc wih [5], ν rrτr ξs cζρcuρζd, ξ τrdr τ drmξ ξλ ν ξmpρξcξ cτrrcτrs d τ η rξrζd. Tν rrτr crξrξζ mpρτd ξs ζ duζρ cζρcuρζξτ, ζd rquξrs νζ ξνr
33 54 Nw Prspcivs in Fluid Dnmics å å w - w* ε w - w* m < or < ε + + w 00 w (4) In hs prssions, w rprsns n of h vribls η, u nd v, nd w is h prvious irions vlu. Th vlu of h rror is s o 0 6. Linr sbili nlsis prformd b [38, 8] nd [40] show h < / ( c) o nsur sbili, whr c is h clri Rsζrcν sud usξμ COULWAVE mτdρ For h nlsis concrning cosl procion, h mn currns round submrgd srucur (rificil rf) r nlsd. Th oupu of h COULW VΔ modl corrsponds o h vloci vlus dph 0.53 ν r blow h wr surfc. Th vloci his dph is usd o drmin h vloci clls nr h shorlin h could giv n indicion of h sdimn rnspor. Γivrgn clls indic rosion nr b h shorlin nd convrgn clls indic sdimnion. Th numricl simulions o sud h HΓ bhvior of h hdrodnmics round h rf hv bn don for four css: wo rf gomris, vring h rf ngl (45 o nd 66 o ), nd wo wv condiions. Th chrcrisics of h simulions for h diffrn css r dscribd in Tbl. Rf ngl ( ) H (m) T (s) Numbr of grid poins pr wvlngh Grid siz (m) Tim sp (s) C C C C Tbl. Min chrcrisics of h simulions prformd. s rcordd in [8], ν cτmpuζξτζρ dτmζξ ξs ζrτud 870 m ξ ν ρτμ-sντr ζd 670 m ξ ν crτss-sντr dξrcξτ wξν ζ cτsζ τd spζcξμ τλ ζrτud = =.0 m ζd ζ Cτurζ umηr τλ 0.5. Tν τζρ sξmuρζξτ ξm wζs 800 s. A λρζ ηττm ξs pρζcd ξ λrτ τλ ν sρτp wνr wζvs ζr μrζd usξμ ν sτurc λucξτ mντd ([39] Wξ ζρ., 995). Tν sτurc λucξτ ξs ρτcζd ζ =80 m ζρτμ ν dξrcξτ (Figur 4). Two spong lrs r usd, on in fron of h offshor boundr o bsorb h ougoing wv nrg, nd h ohr on h bch, boh wih widh of 0.5 ims h wvlngh of h incidn wv. Th numricl rsuls obind b h modl r h im sris of h fr surfc lvion, h wo vloci componns, u nd v, nd h wv brking rs (Figur 5).
34 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ Figur 4. Schmic rprsnion of h simuld gomr (no scl) [8]. C: H = 4.0 m, T = 5 s, 45º C: H = 4.0 m, T = 5 s, 66º C3: H =.5 m, T = 9 s, 45º C4: H =.5 m, T = 9 s, 66º Figur 5. Vloci prns of css C o C4 [8].
35 56 Nw Prspcivs in Fluid Dnmics Rsuls of his simulion r dscribd in [9], including h obsrvd phnomn, such s ζρτμ ν rλ, ζ ξcrζs τλ ν wζv νξμν ξs τηsrvd, ξ τppτsξξτ τ ν sξuζξτ wξντu ν rλ, τwξμ τ ν dcrζs τλ ν dpν ξ ν rλ zτ. Mτrτvr, τwξμ τ ν ξcrζs ξ wζv νξμνs, ν wζv ηrζπξμ τccurs ζrρξr (ζd ξ μrζρ τvr ν rλ) ξ cτmpζrξsτ wξν ν sξuζξτ wξντu ζ rλ. Frτm Fξμur 5, ξ ξs cρζr νζ ν prsc τλ ν rλ sξμξλξcζρ ζρrs ν wζv νξμνs, wξν ν wζv νξμν ξcrζsξμ ζρτμ ν rλ ζs ζ cτsquc τλ dcrζsξμ wζr dpν. Figur 5 lso shows for ll css h convrgn clls ppr, indicing possibl sdimnion nr h shorlin, suggsing h h chosn gomris (Figur 4) r dvngous for boh cosl procion nd improving surf condiions. nw, s rfrrd in [8], morphologicl sud should b don in ordr o confirm hs rsuls. 4.. HD Srr s sndrd modl 4... Numrξcζρ λτrmuρζξτ Th quion ssm (9) is solvd in [7] using n plici fini diffrnc mhod bsd on h McCormck im-spliing schm. For his purpos, h quions r wrin in h following form: ν + P + Q = 0 (5) { } ( ) ( ) é( b ) 3 = -( μ + b + ) ν - + Rdξv( ν μrζdu) P + up + vp + μ + + ν ( ) ( ) é( b ) 3 = -( μ + b + ) ν - + Rdξv( ν μrζdv) η { } Q + uq + vq + μ + + ν η (6) (7) whr P =νu, Q =νv, α =d ν / d ; β=d ξ / d nd h boom fricion rms, τ η nd τ η, r obind hrough (8): η P P Q Q P Q = μ + nd = μ + (8) 7 3 η 7 3 K ν K ν In ordr o ppl h McCormck s mhod, quions (5) (7) r spli ino wo ssms of hr quions hroughou h O nd O dircions. Th corrsponding oprors L nd L k h following form [7]:
36 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ Opror L Opror L ( ) é( ) ν + P = 0 (9) { 3 } ( ) P + up + μ + b + ν = - μ + b + ν - + R P (30) η ( ) é( ) ( ) Q + uq = RQ (3) ν + Q = 0 (3) ( ) P + vp = RP (33) { 3 } ( ) η Q + vq + μ + b + ν = - μ + b + ν - + RQ (34) Considring h gnric vribl F, h soluion im ( + ), for h compuionl poin (ξ, j), is obind from h known soluion F ξ, j hrough h following smmric pplicion: + æ D ö æ D ö æ D ö æ D ö æ D ö æ D ö æ D ö æ D ö F = Lç Lç Lç Lç Lç Lç Lç Lç F è 4 ø è 4 ø è 4 ø è 4 ø è 4 ø è 4 ø è 4 ø è 4 ø ξ, j ξ, j (35) whr ch opror, L nd L, is composd of prdicor corrcor squnc nd rprsns gnric im. In h pplicion (35) of igh prdicor corrcor squncs, lrnl bckwrd nd forwrd spc diffrncs r usd. fr ch prdicor nd ch corrcor of h pplicion F, h vlus of h vlociis (u, v) r updd nd h vlus of h vricl cclrions, α nd β, r rclculd (for dils s [7]) Rζρ cζs sud This modl ws pplid o compu h giion sblishd in h por of Figuir d Foz, Porugl, for diffrn s ss. This por is,50 m long nd 400 m wid, pproiml. Is vrg dph is of h ordr of 7 m, wih pproiml m hroughou h our por bsin. Two simulions wr prformd, considring h s of rs s iniil condiion in boh css, lhough for diffrn idl highs. Th firs cs corrsponds o h nrnc of sinusoidl wv in h opn s (inpu boundr), wih mn wv high H = 3.90 m, priod T = 5 s, wvlngh λ = 47 m, nd dircion Φ = 60 W. Th scond cs corrsponds o mn wv high H = 4.80 m, priod T = 7.5 s, wvlngh λ = 73 m, nd dircion Φ = 58. W. Figurs 6 nd 7 show prspciv viws of h fr surfc compud in h bsin 69. s nd 360 s fr ciion. s cn b sn, zon wih srongr giion is obsrvd in h our hrbor in h scond cs.
37 58 Nw Prspcivs in Fluid Dnmics Figur 6. Por of Figuir d Foz. Prspciv viw of h fr surfc compud 69. s fr ciion, for mn wv high, H = 3.90 m, priod T = 5 s, wvlngh λ = 47 m nd dircion Φ = 83 W. Tid high, 3.35 m (HZ). Figur 7. Por of Figuir d Foz. Prspciv viw of h fr surfc compud 360 s fr ciion, for mn wv high H = 4.80 m, priod T = 7.5 s, wvlngh λ = 73 m nd dircion Φ = 58. W. Tid high,.65 m (HZ) HD Srr s nsion modl Numrξcζρ sτρuξτ Th quion ssm (75) is solvd using n fficin fini diffrnc mhod, whos consisnc nd sbili wr sd in [] nd [] b comprison wih closd-form solir wv soluion of h Srr quions. For his purpos, h rms conining drivivs in im of u r groupd. Th finl ssm of hr quions is rwrin ccording o h following quivln form (SΔRIMP modl) [, 3]: ( uν) ν + = 0 ì q + uq - éu + + ν u + + u - ν u î ê ν uu ( ) ( ) ( )( ) ( ) í ν + éμ( ) νuu + W + b h - μνν h - b μ h 3 æ b ö - é( ν u ) + ν u - ν uu + - ν u u ç è 3 ø ( ν ) + b 3 + η r = 0 ν é + ( ) + W u - ( + ) ν ν u - ( + b ) u = q 3 c W = h + ν + ( ) d ü úý þ (36)
38 Modling of Wv Propgion from Arbirr Dphs o Shllow Wrs A Rviw hp://d.doi.org/0.577/ To compu h soluion of quion ssm (75) (vlus of h vribls ν nd u im + ), w us numricl procdur bsd on h following schm, islf bsd on h ls quion ssm (36), for vribls ν, q nd u. Knowing ll vlus of ν ξ nd u ξ, ξ =, N, in h whol domin im, h quions (36c) nd (36d) r usd o obin h firs vlus of q ξ nd Ω ξ in h whol domin. Thn, w coninu wih h following sps, in which h ind p mns prdicd vlus (s lso [, ] nd [3]):. Th firs quion (36) is usd o prdic h vribl vlus ν pξ im + (ν + pξ ), in h whol domin.. Th scond quion (36b) mks i possibl o prdic h vribl vlus q pξ im + (q + pξ ), king ino ccoun h vlus ν ξ+ =0.5(ν + ξ + ν pξ ), nml for Ω ξ in h whol domin. 3. Th hird quion (36c) mks i possibl o compu h mn-vrgd vlociis u ξ + + im +, king ino ccoun h prdicd vlus ν pξ nd q + pξ, nml for Ω ξ in h whol domin. 4. Th firs oprion (sp ) is rpd in ordr o improv h ccurc of h vribl vlus ν ξ im + (ν ξ + ), using h vlus ū ξ + =0.5 (u ξ + u ξ + ) in h whol domin. 5. Finll, h scond oprion (sp ) is rpd in ordr o improv h ccurc of h vribl vlus q ξ im + (q + ξ ), king ino ccoun h vlus ν + ξ =0.5(ν + ξ + ν ξ ) nd ū ξ + =0.5 (u ξ + u ξ + ) in h whol domin. ch inrior poin i, h firs, scond nd hird-ordr spil drivivs r pproimd hrough cnrd diffrncs nd h im drivivs r pproimd using forwrd diffrncs. Th convciv rms (uν ) nd (uq) in quions (36) nd 36b) r pproimd hrough cnrd schms in spc nd im for vribls h nd q. ch im, hs rms r wrin in h following form: æ ν - ν + ν - ν ö æ u - u ξ+ ξ- ξ+ ξ- ξ+ ξ- ö ç 4D ç D è ø è ø +D +D +D ( uν) = u + ξ ( ν + ν ξ ξ ) æ q - q + q - q ö æ u - u ξ+ ξ- ξ+ ξ- ξ+ ξ- ö ç 4D ç D è ø è ø +D +D +D ( uq) = u + ξ ( q + q ξ ξ ) (37) (38) ll fini diffrnc quions r implici. Thrfor, h soluion of ssm (36) rquirs, in ch im sp, h compuion of fiv hr-digonl ssms of N- quions (sps o 5), which r sil compud using h hr-digonl mri lgorihm (TΓM ), lso known s h Thoms lgorihm. Th sbili condiion o b obsrvd cn b prssd in rms of h Courn/CFL numbr, nd is givn b:
39 60 Nw Prspcivs in Fluid Dnmics D C = μν <.0 R D (39) Bτudζr cτdξξτs W ofn prscrib n influ on h lf boundr, usull mono- or bi-chromic wv flow. Th iniil condiion for his (mono-chromic) influ is: ζ ì æ p ö cos( w) é æ p öü h ( 0,) = ísin( w) nhç - + sin( w) - ê - nh ç - úý î è w ø w è w øþ ζ μ é æ p ö u ( 0,) = cos( w) ênhç - + ú w è w ø (40) (4) whr ζ is h wv mpliud nd h ζν is usd s rmp funcion. I incrss smoohl from 0 o, o cr smooh sr. For lrg, h boundr condiion rducs o: ζ η ( 0,) = sin( ω) (4) μ u ( 0,) = cos( w) (43) w If w wn o void rflcions h righ boundr (oupu), h domin is ndd wih dmping rgion of lngh L dζmp. In his cs, rms lik m() η nd m() u m b ddd o h coninui (36) nd momnum (36b) quions, rspcivl. Th lngh of h dmpd rgion is chosn such h w do no s n significn rflcions Sτρξζr wζv rζvρρξμ up ζ sρτp ζd rλρcξτ τ ζ vrξcζρ wζρρ Δprimnl d nd numricl rsuls r vilbl for solir wv propging on h bhmr shown in Figur 8 [, ]. I shows consn dph bfor = 55 m nd slop :50 bwn = 55 m nd = 75 m. n imprmbl vricl wll is plcd = 75 m, corrsponding o full rflcing boundr condiions. solir wv of mpliud 0. m is iniill cnrd = 5 m. Th compuionl domin ws uniforml discrizd wih spil sp = 0.05 m. zro fricion fcor hs bn considrd. Compuions wr crrid ou wih im sp =0.00 s. Figur 9 comprs numricl im sris of surfc lvion nd s d = 7.75 m. Figur 9 shows wo pks; h firs on corrsponding o h incidn wv, nd h scond o h rflcd wv. Th ndd Srr modl prdicions for boh pks gr wll wih h msurmns. RMSE vlus qul o m nd 0.07 m wr found in firs nd scond pks, rspcivl, for h wv high. Rgrding h phs, hr is loss of pproiml 0.05 s nd of 0.0 s in hos pks (for dils s [] nd []).
Fourier Series and Parseval s Relation Çağatay Candan Dec. 22, 2013
Fourir Sris nd Prsvl s Rlion Çğy Cndn Dc., 3 W sudy h m problm EE 3 M, Fll3- in som dil o illusr som conncions bwn Fourir sris, Prsvl s rlion nd RMS vlus. Q. ps h signl sin is h inpu o hlf-wv rcifir circui
More information3.4 Repeated Roots; Reduction of Order
3.4 Rpd Roos; Rducion of Ordr Rcll our nd ordr linr homognous ODE b c 0 whr, b nd c r consns. Assuming n xponnil soluion lds o chrcrisic quion: r r br c 0 Qudric formul or fcoring ilds wo soluions, r &
More informationRevisiting what you have learned in Advanced Mathematical Analysis
Fourir sris Rvisiing wh you hv lrnd in Advncd Mhmicl Anlysis L f x b priodic funcion of priod nd is ingrbl ovr priod. f x cn b rprsnd by rigonomric sris, f x n cos nx bn sin nx n cos x b sin x cosx b whr
More informationLecture 21 : Graphene Bandstructure
Fundmnls of Nnolcronics Prof. Suprio D C 45 Purdu Univrsi Lcur : Grpn Bndsrucur Rf. Cpr 6. Nwor for Compuionl Nnocnolog Rviw of Rciprocl Lic :5 In ls clss w lrnd ow o consruc rciprocl lic. For D w v: Rl-Spc:
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 informationMath 266, Practice Midterm Exam 2
Mh 66, Prcic Midrm Exm Nm: Ground Rul. Clculor i NOT llowd.. Show your work for vry problm unl ohrwi d (pril crdi r vilbl). 3. You my u on 4-by-6 indx crd, boh id. 4. Th bl of Lplc rnform i vilbl h l pg.
More informationSection 2: The Z-Transform
Scion : h -rnsform Digil Conrol Scion : h -rnsform In linr discr-im conrol sysm linr diffrnc quion chrcriss h dynmics of h sysm. In ordr o drmin h sysm s rspons o givn inpu, such diffrnc quion mus b solvd.
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 information1 Finite Automata and Regular Expressions
1 Fini Auom nd Rgulr Exprion Moivion: Givn prn (rgulr xprion) for ring rching, w migh wn o convr i ino drminiic fini uomon or nondrminiic fini uomon o mk ring rching mor fficin; drminiic uomon only h o
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 informationThe model proposed by Vasicek in 1977 is a yield-based one-factor equilibrium model given by the dynamic
h Vsick modl h modl roosd by Vsick in 977 is yild-bsd on-fcor quilibrium modl givn by h dynmic dr = b r d + dw his modl ssums h h shor r is norml nd hs so-clld "mn rvring rocss" (undr Q. If w u r = b/,
More informationEngine Thrust. From momentum conservation
Airbrhing Propulsion -1 Airbrhing School o Arospc Enginring Propulsion Ovrviw w will b xmining numbr o irbrhing propulsion sysms rmjs, urbojs, urbons, urboprops Prormnc prmrs o compr hm, usul o din som
More informationUNSTEADY HEAT TRANSFER
UNSADY HA RANSFR Mny h rnsfr problms rquir h undrsnding of h ompl im hisory of h mprur vriion. For mpl, in mllurgy, h h ring pross n b onrolld o dirly ff h hrrisis of h prossd mrils. Annling (slo ool)
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 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 informationLaplace Transform. National Chiao Tung University Chun-Jen Tsai 10/19/2011
plc Trnorm Nionl Chio Tung Univriy Chun-Jn Ti /9/ Trnorm o Funcion Som opror rnorm uncion ino nohr uncion: d Dirniion: x x, or Dx x dx x Indini Ingrion: x dx c Dini Ingrion: x dx 9 A uncion my hv nicr
More informationSingle Correct Type. cos z + k, then the value of k equals. dx = 2 dz. (a) 1 (b) 0 (c)1 (d) 2 (code-v2t3paq10) l (c) ( l ) x.
IIT JEE/AIEEE MATHS y SUHAAG SIR Bhopl, Ph. (755)3 www.kolsss.om Qusion. & Soluion. In. Cl. Pg: of 6 TOPIC = INTEGRAL CALCULUS Singl Corr Typ 3 3 3 Qu.. L f () = sin + sin + + sin + hn h primiiv of f()
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 informationSystems of First Order Linear Differential Equations
Sysms of Firs Ordr Linr Diffrnil Equions W will now urn our nion o solving sysms of simulnous homognous firs ordr linr diffrnil quions Th soluions of such sysms rquir much linr lgbr (Mh Bu sinc i is no
More information2 T. or T. DSP First, 2/e. This Lecture: Lecture 7C Fourier Series Examples: Appendix C, Section C-2 Various Fourier Series
DSP Firs, Lcur 7C Fourir Sris Empls: Common Priodic Signls READIG ASSIGMES his Lcur: Appndi C, Scion C- Vrious Fourir Sris Puls Wvs ringulr Wv Rcifid Sinusoids lso in Ch. 3, Sc. 3-5 Aug 6 3-6, JH McCllln
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 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 informationThe Laplace Transform
Th Lplc Trnform Dfiniion nd propri of Lplc Trnform, picwi coninuou funcion, h Lplc Trnform mhod of olving iniil vlu problm Th mhod of Lplc rnform i ym h rli on lgbr rhr hn clculu-bd mhod o olv linr diffrnil
More informationFourier. Continuous time. Review. with period T, x t. Inverse Fourier F Transform. x t. Transform. j t
Coninuous im ourir rnsform Rviw. or coninuous-im priodic signl x h ourir sris rprsnion is x x j, j 2 d wih priod, ourir rnsform Wh bou priodic signls? W willl considr n priodic signl s priodic signl wih
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 informationELECTRIC VELOCITY SERVO REGULATION
ELECIC VELOCIY SEVO EGULAION Gorg W. Younkin, P.E. Lif FELLOW IEEE Indusril Conrols Consuling, Di. Bulls Ey Mrking, Inc. Fond du Lc, Wisconsin h prformnc of n lcricl lociy sro is msur of how wll h sro
More informationVIBRATION ANALYSIS OF CURVED SINGLE-WALLED CARBON NANOTUBES EMBEDDED IN AN ELASTIC MEDIUM BASED ON NONLOCAL ELASTICITY
VIBRATION ANASIS OF CURVED SINGE-AED CARBON NANOTUBES EMBEDDED IN AN EASTIC MEDIUM BASED ON NONOCA EASTICIT Pym Solni Amir Kssi Dprmn of Mchnicl Enginring Islmic Azd Univrsiy-Smnn Brnch Smnm Irn -mil:
More informationSystems of First Order Linear Differential Equations
Sysms of Firs Ordr Linr Diffrnil Equions W will now urn our nion o solving sysms of simulnous homognous firs ordr linr diffrnil quions Th soluions of such sysms rquir much linr lgbr (Mh Bu sinc i is no
More informationRelation between Fourier Series and Transform
EE 37-3 8 Ch. II: Inro. o Sinls Lcur 5 Dr. Wih Abu-Al-Su Rlion bwn ourir Sris n Trnsform Th ourir Trnsform T is riv from h finiion of h ourir Sris S. Consir, for xmpl, h prioic complx sinl To wih prio
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 informationEEE 303: Signals and Linear Systems
33: Sigls d Lir Sysms Orhogoliy bw wo sigls L us pproim fucio f () by fucio () ovr irvl : f ( ) = c( ); h rror i pproimio is, () = f() c () h rgy of rror sigl ovr h irvl [, ] is, { }{ } = f () c () d =
More informationLGOVNATDEFUSAAD
ECONOMETRIC PROBLEMS WITH TIME-SERIES DATA Sionriy: A sris is sid o covrinc sionry if is mn nd covrincs r unffcd y chng of im origin Qusion : Do you hink h following sris r sionry? Log Rl Nionl Dfnc Expndiurs
More informationLecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9
Lctur contnts Bloch thorm -vctor Brillouin zon Almost fr-lctron modl Bnds ffctiv mss Hols Trnsltionl symmtry: Bloch thorm On-lctron Schrödingr qution ch stt cn ccommo up to lctrons: If Vr is priodic function:
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 informationSE1CY15 Differentiation and Integration Part B
SECY5 Diffrniion nd Ingrion Pr B Diffrniion nd Ingrion 6 Prof Richrd Michll Tody w will sr o look mor ypicl signls including ponnils, logrihms nd hyprbolics Som of his cn b found in h rcommndd books Crof
More informationK x,y f x dx is called the integral transform of f(x). The function
APACE TRANSFORMS Ingrl rnform i priculr kind of mhmicl opror which ri in h nlyi of om boundry vlu nd iniil vlu problm of clicl Phyic. A funcion g dfind by b rlion of h form gy) = K x,y f x dx i clld h
More informationControl Systems. Modelling Physical Systems. Assoc.Prof. Haluk Görgün. Gears DC Motors. Lecture #5. Control Systems. 10 March 2013
Lcur #5 Conrol Sy Modlling Phyicl Sy Gr DC Moor Aoc.Prof. Hluk Görgün 0 Mrch 03 Conrol Sy Aoc. Prof. Hluk Görgün rnfr Funcion for Sy wih Gr Gr provid chnicl dvng o roionl y. Anyon who h riddn 0-pd bicycl
More informationBicomplex Version of Laplace Transform
Annd Kumr l. / Inrnionl Journl of Enginring nd Tchnology Vol.,, 5- Bicomplx Vrsion of Lplc Trnsform * Mr. Annd Kumr, Mr. Prvindr Kumr *Dprmn of Applid Scinc, Roork Enginring Mngmn Tchnology Insiu, Shmli
More informationCIVL 8/ D Boundary Value Problems - Rectangular Elements 1/7
CIVL / -D Boundr Vlu Prolms - Rctngulr Elmnts / RECANGULAR ELEMENS - In som pplictions, it m mor dsirl to us n lmntl rprsnttion of th domin tht hs four sids, ithr rctngulr or qudriltrl in shp. Considr
More informationDigital Signal Processing. Digital Signal Processing READING ASSIGNMENTS. License Info for SPFirst Slides. Fourier Transform LECTURE OBJECTIVES
Digil Signl Procssing Digil Signl Procssing Prof. Nizmin AYDIN nydin@yildiz.du.r hp:www.yildiz.du.r~nydin Lcur Fourir rnsform Propris Licns Info for SPFirs Slids READING ASSIGNMENS his work rlsd undr Criv
More informationName:... Batch:... TOPIC: II (C) 1 sec 3 2x - 3 sec 2x. 6 é ë. logtan x (A) log (tan x) (B) cot (log x) (C) log log (tan x) (D) tan (log x) cos x (C)
Nm:... Bch:... TOPIC: II. ( + ) d cos ( ) co( ) n( ) ( ) n (D) non of hs. n sc d sc + sc é ësc sc ù û sc sc é ë ù û (D) non of hs. sc cosc d logn log (n ) co (log ) log log (n ) (D) n (log ). cos log(
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 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 informationA Tutorial of The Context Tree Weighting Method: Basic Properties
A uoril of h on r Wighing Mhod: Bic ropri Zijun Wu Novmbr 9, 005 Abrc In hi uoril, ry o giv uoril ovrvi of h on r Wighing Mhod. W confin our dicuion o binry boundd mmory r ourc nd dcrib qunil univrl d
More informationMore on FT. Lecture 10 4CT.5 3CT.3-5,7,8. BME 333 Biomedical Signals and Systems - J.Schesser
Mr n FT Lcur 4CT.5 3CT.3-5,7,8 BME 333 Bimdicl Signls nd Sysms - J.Schssr 43 Highr Ordr Diffrniin d y d x, m b Y b X N n M m N M n n n m m n m n d m d n m Y n d f n [ n ] F d M m bm m X N n n n n n m p
More informationImproved Computation of Electric Field in. Rectangular Waveguide. Based Microwave Components Using. Modal Expansion
Journl of Innoviv Tchnolog n Eucion, Vol. 3, 6, no., 3 - HIKARI L, www.-hikri.co hp://.oi.org/.988/ji.6.59 Iprov Copuion of Elcric Fil in Rcngulr Wvgui Bs icrowv Coponns Ug ol Epnsion Rj Ro Dprn of lcronics
More informationChapter 3: Fourier Representation of Signals and LTI Systems. Chih-Wei Liu
Chapr 3: Fourir Rprsnaion of Signals and LTI Sysms Chih-Wi Liu Oulin Inroducion Complx Sinusoids and Frquncy Rspons Fourir Rprsnaions for Four Classs of Signals Discr-im Priodic Signals Fourir Sris Coninuous-im
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 informationThe Procedure Abstraction Part II: Symbol Tables and Activation Records
Th Produr Absrion Pr II: Symbol Tbls nd Aivion Rords Th Produr s Nm Sp Why inrodu lxil soping? Provids ompil-im mhnism for binding vribls Ls h progrmmr inrodu lol nms How n h ompilr kp rk of ll hos nms?
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 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 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 informationSOLUTIONS. 1. Consider two continuous random variables X and Y with joint p.d.f. f ( x, y ) = = = 15. Stepanov Dalpiaz
STAT UIUC Pracic Problms #7 SOLUTIONS Spanov Dalpiaz Th following ar a numbr of pracic problms ha ma b hlpful for compling h homwor, and will lil b vr usful for suding for ams.. Considr wo coninuous random
More informationLecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture:
Lctur 11 Wvs in Priodic Potntils Tody: 1. Invrs lttic dfinition in 1D.. rphicl rprsnttion of priodic nd -priodic functions using th -xis nd invrs lttic vctors. 3. Sris solutions to th priodic potntil Hmiltonin
More informationA modified hyperbolic secant distribution
Songklnkrin J Sci Tchnol 39 (1 11-18 Jn - Fb 2017 hp://wwwsjspsuch Originl Aricl A modifid hyprbolic scn disribuion Pnu Thongchn nd Wini Bodhisuwn * Dprmn of Sisics Fculy of Scinc Kssr Univrsiy Chuchk
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 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 informationDiscussion 06 Solutions
STAT Discussion Soluions Spring 8. Th wigh of fish in La Paradis follows a normal disribuion wih man of 8. lbs and sandard dviaion of. lbs. a) Wha proporion of fish ar bwn 9 lbs and lbs? æ 9-8. - 8. P
More informationFREE VIBRATION AND BENDING ANALYSES OF CANTILEVER MICROTUBULES BASED ON NONLOCAL CONTINUUM MODEL
Mhmicl nd Compuionl Applicions Vol. 15 o. pp. 89-98 1. Associion for Scinific Rsrch FREE VIBRATIO AD BEDIG AALYSES OF CATILEVER MICROTUBULES BASED O OLOCAL COTIUUM MODEL Ömr Civlk Çiğdm Dmir nd Bkir Akgöz
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 informationModelling of three dimensional liquid steel flow in continuous casting process
AMME 2003 12h Modlling of hr dimnsional liquid sl flow in coninuous casing procss M. Jani, H. Dyja, G. Banasz, S. Brsi Insiu of Modlling and Auomaion of Plasic Woring Procsss, Faculy of Marial procssing
More informationChapter 4 Circular and Curvilinear Motions
Chp 4 Cicul n Cuilin Moions H w consi picls moing no long sigh lin h cuilin moion. W fis su h cicul moion, spcil cs of cuilin moion. Anoh mpl w h l sui li is h pojcil..1 Cicul Moion Unifom Cicul Moion
More informationWeek 06 Discussion Suppose a discrete random variable X has the following probability distribution: f ( 0 ) = 8
STAT W 6 Discussion Fll 7..-.- If h momn-gnring funcion of X is M X ( ), Find h mn, vrinc, nd pmf of X.. Suppos discr rndom vribl X hs h following probbiliy disribuion: f ( ) 8 7, f ( ),,, 6, 8,. ( possibl
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 informationPHA Final Exam Fall On my honor, I have neither given nor received unauthorized aid in doing this assignment.
Nm: UFI#: PHA 527 Finl Exm Fll 2008 On my honor, I hv nihr givn nor rcivd unuhorizd id in doing his ssignmn. Nm Pls rnsfr h nswrs ono h bubbl sh. Pls fill in ll h informion ncssry o idnify yourslf. h procors
More informationAn Optimal Ordering Policy for Inventory Model with. Non-Instantaneous Deteriorating Items and. Stock-Dependent Demand
Applid Mhmicl Scincs, Vol. 7, 0, no. 8, 407-4080 KA Ld, www.m-hikri.com hp://dx.doi.org/0.988/ms.0.56 An piml rdring Policy for nvnory Modl wih Non-nsnnous rioring ms nd Sock-pndn mnd Jsvindr Kur, jndr
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 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 informationMidterm. Answer Key. 1. Give a short explanation of the following terms.
ECO 33-00: on nd Bnking Souhrn hodis Univrsi Spring 008 Tol Poins 00 0 poins for h pr idrm Answr K. Giv shor xplnion of h following rms. Fi mon Fi mon is nrl oslssl produd ommodi h n oslssl sord, oslssl
More informationPHA Second Exam. Fall On my honor, I have neither given nor received unauthorized aid in doing this assignment.
Nm: UFI #: PHA 527 Scond Exm Fll 20 On my honor, I hv nihr givn nor rcivd unuhorizd id in doing his ssignmn. Nm Pu ll nswrs on h bubbl sh OAL /200 ps Nm: UFI #: Qusion S I (ru or Fls) (5 poins) ru (A)
More informationA Kalman filtering simulation
A Klmn filering simulion The performnce of Klmn filering hs been esed on he bsis of wo differen dynmicl models, ssuming eiher moion wih consn elociy or wih consn ccelerion. The former is epeced o beer
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 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 informationUNSTEADY STATE HEAT CONDUCTION
MODUL 5 UNADY A HA CONDUCION 5. Inroduion o his poin, hv onsidrd onduiv h rnsfr problms in hih h mprurs r indpndn of im. In mny ppliions, hovr, h mprurs r vrying ih im, nd rquir h undrsnding of h ompl
More informationA Study on the Nature of an Additive Outlier in ARMA(1,1) Models
Europn Journl of Scinific Rsrch SSN 45-6X Vol3 No3 9, pp36-368 EuroJournls Publishing, nc 9 hp://wwwuroournlscom/srhm A Sudy on h Nur of n Addiiv Oulir in ARMA, Modls Azmi Zhrim Cnr for Enginring Rsrch
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 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 informationMulti-Section Coupled Line Couplers
/0/009 MultiSction Coupld Lin Couplrs /8 Multi-Sction Coupld Lin Couplrs W cn dd multipl coupld lins in sris to incrs couplr ndwidth. Figur 7.5 (p. 6) An N-sction coupld lin l W typiclly dsign th couplr
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 informationErrata for Second Edition, First Printing
Errt for Scond Edition, First Printing pg 68, lin 1: z=.67 should b z=.44 pg 1: Eqution (.63) should rd B( R) = x= R = θ ( x R) p( x) R 1 x= [1 G( x)] = θp( R) + ( θ R)[1 G( R)] pg 15, problm 6: dmnd of
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 informationCS 688 Pattern Recognition. Linear Models for Classification
//6 S 688 Pr Rcogiio Lir Modls for lssificio Ø Probbilisic griv modls Ø Probbilisic discrimiiv modls Probbilisic Griv Modls Ø W o ur o robbilisic roch o clssificio Ø W ll s ho modls ih lir dcisio boudris
More informationCanadian Journal of Physics. Kantowski-Sachs modified holographic Ricci dark energy model in Saez-Ballester theory of gravitation
Cndin Journl of Physics Knowsi-Schs modifid hologrphic Ricci dr nrgy modl in Sz-Bllsr hory of grviion Journl: Cndin Journl of Physics Mnuscrip ID cjp--7.r Mnuscrip Typ: Aricl D Submid by h Auhor: -Jul-7
More informationDE Dr. M. Sakalli
DE-0 Dr. M. Sakalli DE 55 M. Sakalli a n n 0 a Lh.: an Linar g Equaions Hr if g 0 homognous non-homognous ohrwis driving b a forc. You know h quaions blow alrad. A linar firs ordr ODE has h gnral form
More informationMajor: All Engineering Majors. Authors: Autar Kaw, Luke Snyder
Nolr Rgrsso Mjor: All Egrg Mjors Auhors: Aur Kw, Luk Sydr hp://urclhodsgusfdu Trsforg Nurcl Mhods Educo for STEM Udrgrdus 3/9/5 hp://urclhodsgusfdu Nolr Rgrsso hp://urclhodsgusfdu Nolr Rgrsso So populr
More informationFeedback Control and Synchronization of Chaos for the Coupled Dynamos Dynamical System *
ISSN 746-7659 England UK Jornal of Informaion and Comping Scinc Vol. No. 6 pp. 9- Fdbac Conrol and Snchroniaion of Chaos for h Copld Dnamos Dnamical Ssm * Xdi Wang Liin Tian Shmin Jiang Liqin Y Nonlinar
More informationJonathan Turner Exam 2-10/28/03
CS Algorihm n Progrm Prolm Exm Soluion S Soluion Jonhn Turnr Exm //. ( poin) In h Fioni hp ruur, u wn vrx u n i prn v u ing u v i v h lry lo hil in i l m hil o om ohr vrx. Suppo w hng hi, o h ing u i prorm
More informationControl System Engineering (EE301T) Assignment: 2
Conrol Sysm Enginring (EE0T) Assignmn: PART-A (Tim Domain Analysis: Transin Rspons Analysis). Oain h rspons of a uniy fdack sysm whos opn-loop ransfr funcion is (s) s ( s 4) for a uni sp inpu and also
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 informationMASTER CLASS PROGRAM UNIT 4 SPECIALIST MATHEMATICS SEMESTER TWO 2014 WEEK 11 WRITTEN EXAMINATION 1 SOLUTIONS
MASTER CLASS PROGRAM UNIT SPECIALIST MATHEMATICS SEMESTER TWO WEEK WRITTEN EXAMINATION SOLUTIONS FOR ERRORS AND UPDATES, PLEASE VISIT WWW.TSFX.COM.AU/MC-UPDATES QUESTION () Lt p ( z) z z z If z i z ( is
More informationPhysics 2A HW #3 Solutions
Chper 3 Focus on Conceps: 3, 4, 6, 9 Problems: 9, 9, 3, 41, 66, 7, 75, 77 Phsics A HW #3 Soluions Focus On Conceps 3-3 (c) The ccelerion due o grvi is he sme for boh blls, despie he fc h he hve differen
More informationStability of time-varying linear system
KNWS 39 Sbiliy of im-vrying linr sysm An Szyd Absrc: In his ppr w considr sufficin condiions for h ponnil sbiliy of linr im-vrying sysms wih coninuous nd discr im Sbiliy gurning uppr bounds for diffrn
More informationFL/VAL ~RA1::1. Professor INTERVI of. Professor It Fr recru. sor Social,, first of all, was. Sys SDC? Yes, as a. was a. assumee.
B Pror NTERV FL/VAL ~RA1::1 1 21,, 1989 i n or Socil,, fir ll, Pror Fr rcru Sy Ar you lir SDC? Y, om um SM: corr n 'd m vry ummr yr. Now, y n y, f pr my ry for ummr my 1 yr Un So vr ummr cour d rr o l
More informationT h e C S E T I P r o j e c t
T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T
More informationAdvanced Engineering Mathematics, K.A. Stroud, Dexter J. Booth Engineering Mathematics, H.K. Dass Higher Engineering Mathematics, Dr. B.S.
Rfrc: (i) (ii) (iii) Advcd Egirig Mhmic, K.A. Sroud, Dxr J. Booh Egirig Mhmic, H.K. D Highr Egirig Mhmic, Dr. B.S. Grwl Th mhod of m Thi coi of h followig xm wih h giv coribuio o h ol. () Mid-rm xm : 3%
More informationChapter4 Time Domain Analysis of Control System
Chpr4 im Domi Alyi of Corol Sym Rouh biliy cririo Sdy rror ri rpo of h fir-ordr ym ri rpo of h cod-ordr ym im domi prformc pcificio h rliohip bw h prformc pcificio d ym prmr ri rpo of highr-ordr ym Dfiiio
More informationErrata for Second Edition, First Printing
Errt for Scond Edition, First Printing pg 68, lin 1: z=.67 should b z=.44 pg 71: Eqution (.3) should rd B( R) = θ R 1 x= [1 G( x)] pg 1: Eqution (.63) should rd B( R) = x= R = θ ( x R) p( x) R 1 x= [1
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 informationEE 529 Remote Sensing Techniques. Review
59 Rmo Snsing Tchniqus Rviw Oulin Annna array Annna paramrs RCS Polariaion Signals CFT DFT Array Annna Shor Dipol l λ r, R[ r ω ] r H φ ηk Ilsin 4πr η µ - Prmiiviy ε - Prmabiliy
More informationTOPIC 5: INTEGRATION
TOPIC 5: INTEGRATION. Th indfinit intgrl In mny rspcts, th oprtion of intgrtion tht w r studying hr is th invrs oprtion of drivtion. Dfinition.. Th function F is n ntidrivtiv (or primitiv) of th function
More information