On interval-valued optimization problems with generalized invex functions

Size: px
Start display at page:

Download "On interval-valued optimization problems with generalized invex functions"

Transcription

1 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 htt:// R E S E A R C H On Accss On intval-valud otimization oblms with gnalizd inv functions Izha Ahmad,2*, Anuag Jayswal 3 and Jonaki Banj 3 * Cosondnc: dizha@kfum.du.sa Datmnt of Mathmatics and Statistics, King Fahd Univsity of Ptolum and Minals, Dhahan, 326, Saudi Aabia 2 Pmannt addss: Datmnt of Mathmatics, Aligah Muslim Univsity, Aligah, , India Full list of autho infomation is availabl at th nd of th aticl Abstact This a is dvotd to study intval-valud otimization oblms. Sufficint otimality conditions a stablishd fo LU otimal solution conct und gnalizd (, ) ρ (η, θ)-invity. Wak, stong and stict convs duality thoms fo Wolf and Mond-Wi ty duals a divd in od to lat th LU otimal solutions of imal and dual oblms. MSC: 90C46; 90C26; 90C30 Kywods: nonlina ogamming; intval-valud functions; (, ) ρ (η, θ)-invity; LU-otimal; sufficincy; duality Intoduction Many al wold dcision-making oblms nd to accomlish many objctivs: minimiz cost, maimiz liability, minimiz dviations fom dsi lvls, minimiz isk, tc. In ths cass otimization oblms hav a lag numb of alications. Th main goal of singl objctiv otimization is to find th bst solution which cosonds to th minimum o maimum valu of a singl objctiv function. In many sach filds and al wold oblms, th mthodology fo solving otimization oblms has bn usd. Th a th kinds of mthodology that a usd fo solving otimization oblms, namly dtministic otimization oblm, stochastic otimization oblm and intval-valud otimization oblm. Th otimization oblms with intval cofficints a tmd an intval-valud otimization oblm. In this oblm, th cofficint is takn as closd intvals. Th solution conct imosd uon th objctiv function is th main diffnc btwn th abov said th kinds of oblms. Intval ogamming mthods hav bn usd to tackl scific issus in multil objctiv lina ogamming: som dal with unctainty in th objctiv functions, oths handl unctainty both in th objctiv functions and in th RHS of th constaints and oths dal with unctainty in all th cofficints of th modl. Chans t al. [] oosd an ida fo solving th lina ogamming oblms in which th constaints w assumd as closd intvals. Lat, Stu [2] dvlod an algoithm to solv th lina ogamming oblm with intval objctiv functions. Uli and Nadau [3] sntd a ocss to solv th multi-objctiv lina ogamming oblms with intval cofficints. Chanas and Kuchta [4]gnalizd th solution concts of th lina ogamming oblm with intval cofficints in th objctiv function basd on fnc lations btwn intvals. By imosing a atial oding 203 Ahmad t al.; licns Sing. This is an On Accss aticl distibutd und th tms of th Cativ Commons Attibution Licns (htt://cativcommons.og/licnss/by/2.0), which mits unstictd us, distibution, and oduction in any mdium, ovidd th oiginal wok is oly citd.

2 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 2 of 4 htt:// on th st of all closd intvals, Wu [5] intoducd a solution conct in otimization oblms with intval-valud objctiv functions. Th a sval aoachs to modl unctainty in otimization oblms such as stochastic otimization and fuzzy otimization. H w consid an otimization oblm with intval-valud objctiv function. Stancu-Minasian and Tigan [6, 7]invstigatd this kind of otimization oblm. Wu [8] fomulatd Kaush-Kuhn-Tuck otimality conditions fo an intval-valud objctiv function. Lat, Wu [9, 0] fomulatd a Wolf-ty dual oblm latd to th intval-valud otimization oblm and stablishd duality thoms by using th conct of nondominatd solution mloyd in vcto otimization oblms. Zhou and Wang [] stablishd a sufficint otimality condition and discussd mid-ty duality fo a class of nonlina intval-valud otimization oblms. Rcntly, Bhuj and Panda [2] dvlod amthodologytostudy thistncofthsolutionsofanintval otimization oblm.vy cntly,zhangt al. [3] discussd th otimality conditions and duality sults fo intval-valud otimization oblms und gnalizd invity. Convity lays an imotant ol in oving th istnc of a solution of a gnal otimization oblm. Hnc th is a nd to study th conv oty of intval otimization oblms. On of th most usful gnalizations of convity was intoducd by Hanson [4]. Fo dtails, ads a advisd to s [5]. Aft th conct of ρ (η, θ)- inv function and (, )-inv function had bn intoducd by Zalmai [6] and Antczak [7], sctivly, Mandal and Nahak[8] oosd a nw conct of (, ) ρ (η, θ)- inv function and stablishd som symmtic duality sults. Rcntly, Jayswal t al. [9] divd sufficint otimality conditions and duality thoms fo intval-valud otimization oblms involving gnalizd conv functions. In this a, w consid an intval-valud otimization oblm in which th objctiv function is an intval-valud function and th constaint functions a alvalud, and div sufficint otimality conditions and duality thoms und gnalizd (, ) ρ (η, θ)-invity. Th oganization of th a is as follows. In Sction 2,w call som dfinitions and som basic otis latd to intval-valud otimization oblms. In Sction3, som sufficint otimality conditions fo a class of intval-valud ogamming oblms a discussd. Wolf and Mond-Wi ty duality thoms a obtaind in Sctions 4 and 5, sctivly. Conclusion and futu wok a oosd in Sction 6. 2 Notation and liminais Lt I b a class of all closd and boundd intvals in R. Thoughout this a, whn w say that A is a closd intval, w man that A is also boundd in R.IfAis a closd intval, w us th notation A =[a L, a U ], wh a L and a U man th low and u bounds of A, sctivly.ifa L = a U = a, thna =[a, a] =a is a al numb. Lt A =[a L, a U ], B =[b L, b U ] I,wdfin (i) A + B = a + b : a A and b B} =[a L + b L, a U + b U ], (ii) A = a : a A} =[ a U, a L ]. Thfo w s that A B = A +( B)=[a L b U, a U b L ]. W also hav (i) k + A = k + a : a A} =[k + a L, k + a U ],

3 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 3 of 4 htt:// [ka L, ka U ] if k 0, (ii) ka = ka : a A} = wh k is a al numb. [ka U, ka L ] if k <0, Lt R n dnot an n-dimnsional Euclidan sac. Th function F : R n I is calld an intval-valud function, i.., F()=F(, 2,..., n ) is a closd intval in R fo ach R n. Th intval-valud function F can also b wittn as F()=[F L (), F U ()], wh F L (), F U () a al-valud functions dfind on R n and satisfy th condition F L () F U ()fo ach R n.wnotthat[f()] L = F L ()and[f()] U = F U (). In intval mathmatics, an od lation is oftn usd to ank intval numbs and it imlis that an intval numb is btt than anoth but not that on is lag than anoth. Fo A =[a L, a U ]andb =[b L, b U ], w wit A LU B if and only if a L b L and a U b U.Itisasytosthat LU is a atial oding on I.Also,wcanwitA < LU B if and only if A LU B and A B. Equivalntly, A < LU B if and only if a L < b L, a U b U o a L b L, a U < b U o a L < b L, a U < b U. Dfinition 2. [8] Ltf : R n R b a diffntiabl function and lt, b abitay al numbs. If th ist η : R n R n R n, θ : R n R n R n and ρ R such that th lations ( (f () f (y)) ) (>) f (y)( η(,y) ) + ρ θ(, y) 2 fo 0, 0, ( (f () f (y)) ) (>) f (y)η(, y)+ρ θ(, y) 2 fo =0, 0, f () f (y)(>) f (y)( η(,y) ) + ρ θ(, y) 2 fo 0, =0, f () f (y)(>) f (y)η(, y)+ρ θ(, y) 2 fo =0, =0 hold, thn f is said to b (stictly) (, ) ρ (η, θ)-inv at th oint y on R n with sct to η, θ. Dfinition 2.2 Lt f : R n R b a diffntiabl function and lt, b abitay al numbs. If th ist η : R n R n R n, θ : R n R n R n and ρ R such that th lations f (y)( η(,y) ) + ρ θ(, y) 2 0 ( (f () f (y)) ) (>) 0 fo 0, 0, f (y)η(, y)+ρ θ(, y) 2 ( 0 (f () f (y)) ) (>) 0 fo =0, 0, f (y)( η(,y) ) + ρ θ(, y) 2 0 f () f(y)(>) 0 fo 0, =0, f (y)η(, y)+ρ θ(, y) 2 0 f () f(y)(>) 0 fo =0, =0 hold, thn f is said to b (stictly) (, ) ρ (η, θ)-sudo-inv at th oint y on R n with sct to η, θ.

4 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 4 of 4 htt:// Dfinition 2.3 Lt f : R n R b a diffntiabl function and lt, b abitay al numbs. If th ist η : R n R n R n, θ : R n R n R n and ρ R such that th lations ( (f () f (y)) ) 0 f (y)( η(,y) ) ρ θ(, y) 2 fo 0, 0, ( (f () f (y)) ) 0 f (y)η(, y) ρ θ(, y) 2 fo =0, 0, f () f (y) 0 f (y)( η(,y) ) ρ θ(, y) 2 fo 0, =0, f () f (y) 0 f (y)η(, y) ρ θ(, y) 2 fo =0, =0 hold, thn f is said to b (, ) ρ (η, θ)-quasi-inv at th oint y on R n with sct to η, θ. Rmak 2. It should b notd that th onntials aaing on th ight-hand sids of inqualitis abov a undstood to b takn comonntwis and =(,,...,) R n. Rmak 2.2 All thoms in this a will b ovd only in th cas whn 0, 0 (oth cass can b dalt with likwis sinc th only changs ais in a fom of inquality). Moov, without loss of gnality, w shall assum that >0, >0(inthcaswhn <0, < 0, th diction of som of th inqualitis in th oof of th thoms should b changd to th oosit on). In this a, w consid th following imal otimization oblm with intvalvalud objctiv function: (IVP) min F()= [ F L (), F U () ] subjct to g j () 0, j =,2,...,m, wh F : R n I is an intval-valud function and g j : R n R is a al-valud function. Lt = R n : g j () 0, j =,2,...,m} b th st of all fasibl solutions of (IVP). W also dnot by Obj(F, )=F(): } th st of all objctiv valus of imal oblm (IVP). Dfinition 2.4 [20] Lt * b a fasibl solution of th imal oblm (IVP). W say that * is a LU otimal solution of oblm (IVP) if th ists no 0 such that F( 0 )< LU F( * ). Thom 2. (Kaush-Kuhn-Tuck ty conditions [9]) Assum that * is a LU otimal solution of imal oblm (IVP) and F, g j, j =,2,...,m, a diffntiabl at *. Suos that th constaint function g j, j =,2,...,m, satisfis th suitabl Kuhn-Tuck constaint qualification [9] at *. Thn th ist multilis 0<ξ L, ξ U Rand0 μ j R, j =,2,...,m, such that ξ L F L( *) + ξ U F U( *) + ( μ j g j * ) =0, () μ j g j ( * ) =0, j =,2,...,m. (2)

5 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 5 of 4 htt:// 3 Sufficint otimality conditions In this sction, w shall stablish th following sufficint otimality conditions fo (IVP). Thom 3. (Sufficincy) Lt * b a fasibl solution of (IVP). Suos that th objctiv function F and th constaint function g j, j =,2,...,m, a diffntiabl at *. Assum that F L and F U a (, ) ρ (η, θ)-inv and (, ) ρ 2 (η, θ)-inv, sctivly, with sct to η, θ and m μ jg j is (, ) ρ 3 (η, θ)-inv with sct to η, θ at * with (ξ L ρ + ξ U ρ 2 + ρ 3 ) 0. If th ist (Lagang) multilis 0<ξ L, ξ U Rand μ =(μ, μ 2,...,μ m ), 0 μ j R, j =,2,...,m, such that ( *, ξ L, ξ U, μ) satisfis () and (2), thn * is a LU otimal solution to oblm (IVP). Poof Lt * b not a LU otimal solution of (IVP). Thn th ists a fasibl solution 0 such that F( 0 )< LU F ( *). That is, F L ( 0 )<F L ( * ), F U ( 0 )<F U ( * ), o F L ( 0 ) F L ( * ), F U ( 0 )<F U ( * ), o F L ( 0 )<F L ( * ), F U ( 0 ) F U ( * ). Sinc > 0, using th oty of an onntial function, w obtain [FL ( 0 ) F L ( * )} ]<0, [FU ( 0 ) F U ( *)} ]<0, [FL ( 0 ) F L ( *)} ]<0, o [FL ( 0 ) F L ( *)} ] 0, [FU ( 0 ) F U ( *)} ]<0, o [FU ( 0 ) F U ( * )} ] 0. Using th abov inqualitis and th (, ) ρ (η, θ)-invity of F L and th (, ) ρ 2 (η, θ)-invity of F U at *,wgt FL ( * )}( η( 0, *) )+ρ θ( 0, * ) 2 <0, FU ( * )}( η( 0, *) )+ρ 2 θ( 0, * ) 2 <0, FL ( * )}( η( 0, *) )+ρ θ( 0, * ) 2 0, FU ( * )}( η( 0, *) )+ρ 2 θ( 0, * ) 2 <0, o o FL ( * )}( η( 0, *) )+ρ θ( 0, * ) 2 <0, FU ( * )}( η( 0, *) )+ρ 2 θ( 0, * ) 2 0. Sinc ξ L >0andξ U > 0, fom th abov inqualitis, w gt ξ L F L( *) + ξ U F U( *)}( η( 0, *) ) + ξ L ρ θ ( 0, *) 2 + ξ U ρ 2 θ ( 0, *) 2 <0. (3)

6 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 6 of 4 htt:// On th oth hand, fom th fasibility of 0 to (IVP), w hav g j ( 0 ) 0, j =,2,...,m. Sinc μ j 0, j =,2,...,m, th abov inquality togth with (2)yilds μ j g j ( 0 ) ( μ j g j * ). As > 0, using th oty of an onntial function, w gt [ m μ j g j ( 0 ) m μ j g j ( *)} ] 0, which togth with th assumtion that m μ jg j is (, ) ρ 3 (η, θ)-inv at * givs ( μ j g j * )( η( 0, *) ) + ρ 3 θ ( 0, *) 2 0. (4) On adding (3)and(4), w gt ( η( 0, *) )[ ξ L F L( *) + ξ U F U( *) + + ( ξ L ρ + ξ U ρ 2 + ρ 3 ) θ ( 0, *) 2 <0. ( μ j g j * )] Thfo, fom th hyothsis that (ξ L ρ + ξ U ρ 2 + ρ 3 ) 0 and th abov inquality, w gt ( η( 0, *) )[ ξ L F L( *) + ξ U F U( *) + ( μ j g j * )] <0, which contadicts (). Thfo * is a LU otimal solution of (IVP). This comlts th oof. Thom 3.2 (Sufficincy) Lt * b a fasibl solution of (IVP). Suos that th objctiv function F and th constaint function g j, j =,2,...,m, a diffntiabl at *. Assum that (ξ L F L + ξ U F U ) is (, ) ρ (η, θ)-sudo-inv with sct to η, θ and m μ jg j is (, ) ρ 2 (η, θ)-quasi-inv with sct to η, θ at * with (ρ + ρ 2 ) 0. If th ist (Lagang) multilis 0<ξ L, ξ U Randμ =(μ, μ 2,...,μ m ), 0 μ j R, j =,2,...,m, such that ( *, ξ L, ξ U, μ) satisfis () and (2), thn * is a LU otimal solution to oblm (IVP). Poof Lt * b not a LU otimal solution of (IVP). Thn th ists a fasibl solution 0 such that F( 0 )< LU F ( *).

7 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 7 of 4 htt:// That is, F L ( 0 )<F L ( * ), F U ( 0 )<F U ( * ), o F L ( 0 ) F L ( * ), F U ( 0 )<F U ( * ), o F L ( 0 )<F L ( * ), F U ( 0 ) F U ( * ). Sinc ξ L >0andξ U > 0, fom th abov inqualitis, w hav ξ L F L ( 0 )+ξ U F U ( 0 )<ξ L F L( *) + ξ U F U( *). As > 0, using th oty of an onntial function, w gt [ (ξ L F L ( 0 )+ξ U F U ( 0 )) (ξ L F L ( * )+ξ U F U ( *))} ] <0, which togth with th assumtion that ξ L F L + ξ U F U is (, ) ρ (η, θ)-sudo-inv at * givs ξ L F L( *) + ξ U F U( *)}( η( 0, *) ) + ρ θ ( 0, *) 2 <0. (5) On th oth hand, fom th fasibility of 0 to (IVP), w hav g j ( 0 ) 0, j =,2,...,m. Sinc μ j 0, j =,2,...,m, th abov inquality togth with (2)yilds μ j g j ( 0 ) ( μ j g j * ). As > 0, using th oty of an onntial function, w gt [ m μ j g j ( 0 ) m μ j g j ( *)} ] 0, which togth with th assumtion that m μ jg j is (, ) ρ 2 (η, θ)-quasi-inv at * givs ( μ j g j * )( η( 0, *) ) ( + ρ 2 θ 0, *) 2 0. (6) On adding (5)and(6), w gt ( η( 0, *) )[ ξ L F L( *) + ξ U F U( *) + +(ρ + ρ 2 ) θ ( 0, *) 2 <0. Sinc (ρ + ρ 2 ) 0, w hav ( η( 0, *) )[ ξ L F L( *) + ξ U F U( *) + ( μ j g j * )] ( μ j g j * )] <0,

8 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 8 of 4 htt:// which contadicts (). Thfo * is a LU otimal solution of (IVP). This comlts th oof. 4 Wolf-tyduality In this sction, w consid th following Wolf-ty dual oblm: (WD) ma F(y)+ subjct to μ j g j (y) ξ L F L (y)+ξ U F U (y)+ μ j g j (y)=0, (7) ξ L >0,ξ U >0,μ j 0, j =,2,...,m, (8) wh F(y)+ m μ jg j (y)=[f L (y)+ m μ jg j (y), F U (y)+ m μ jg j (y)] is an intval-valud function. Dfinition 4. Lt (y *, ξ *L, ξ *U, μ * ) b a fasibl solution of dual oblm (WD). W say that (y *, ξ *L, ξ *U, μ * ) is a LU otimal solution of dual oblm (WD) if th ists no (y, ξ *L, ξ *U, μ * )suchthatf(y * )+ m μ* j g j(y * )< LU F(y)+ m μ* j g j(y). Thom 4. (Wak duality) Lt X 0 b an on subst of R n. Lt F and g j, j =,2,...,m, b diffntiabl on X 0. Suos that and (y, ξ L, ξ U, μ) a th fasibl solutions to (IVP) and (WD), sctivly. Futh assum that ξ L >0,ξ U >0and μ j 0, j =,2,...,m, such that ξ L F L + ξ U F U + m μ jg j is (, ) ρ (η, θ)-inv with sct to η, θ at y with ξ L + ξ U = and ρ 0. Thn F() LU F(y)+ μ j g j (y). Poof Suos contay to th sult that F()< LU F(y)+ μ j g j (y). That is, F L ()<F L (y)+ m μ jg j (y), F U ()<F U (y)+ m μ jg j (y), F L ()<F L (y)+ m μ jg j (y), F U () F U (y)+ m μ jg j (y). o F L () F L (y)+ m μ jg j (y), F U ()<F U (y)+ m μ jg j (y), o Sinc ξ L >0,ξ U >0andξ L + ξ U =, th abov inqualitis togth with th fasibility of to (IVP) bcom ξ L F L ()+ξ U F U ()+ μ j g j ()<ξ L F L (y)+ξ U F U (y)+ μ j g j (y). (9)

9 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 9 of 4 htt:// Fom th assumtion that ξ L F L + ξ U F U + m μ jg j is (, ) ρ (η, θ)-inv at y,whav [ (ξ L F L ()+ξ U F U ()+ m μ j g j ()) (ξ L F L (y)+ξ U F U (y)+ m μ j g j (y))} ] [ ( ξ L F L (y)+ξ U F U (y)+ μ j g j (y)] η(,y) ) + ρ θ(, y) 2. Th abov inquality togth with (7)andρ 0yilds [ (ξ L F L ()+ξ U F U ()+ m μ j g j ()) (ξ L F L (y)+ξ U F U (y)+ m μ j g j (y))} ] 0. Sinc > 0, using th oty of an onntial function, w gt ξ L F L ()+ξ U F U ()+ μ j g j () ξ L F L (y)+ξ U F U (y)+ μ j g j (y), which contadicts th inquality (9). This comlts th oof. Thom 4.2 (Stong duality) Lt * b a LU otimal solution to (IVP) at which Kuhn- Tuck constaints qualification a satisfid. Thn th ist ξ *L >0,ξ *U >0and μ * 0 such that ( *, ξ *L, ξ *U, μ * ) is fasibl fo (WD) and th two objctivs hav th sam valu. Futh, if th hyothsis of wak duality Thom 4. holds fo all fasibl solutions (y *, ξ *L, ξ *U, μ * ), thn ( *, ξ *L, ξ *U, μ * ) is a LU otimal solution to (WD). Poof Sinc * is a LU otimal solution to (IVP) and th Kuhn-Tuck constaints qualification a satisfid at *, thn by Thom 2.,thistmultilisξ *L >0,ξ *U >0and μ * j 0, j =,2,...,m,suchthat ξ *L F L( *) + ξ *U F U( *) + μ * j g j( * ) =0, * ) =0, which yilds that ( *, ξ *L, ξ *U, μ * ) is a fasibl solution fo (WD) and cosonding objctiv valus a th sam. Futh, if ( *, ξ *L, ξ *U, μ * ) is not a LU otimal solution of (WD), thn th ists a fasibl solution (y *, ξ *L, ξ *U, μ * )fo(wd)suchthat F ( *) < LU F ( y *) + y * ), which contadicts wak duality Thom 4..Hnc( *, ξ *L, ξ *U, μ * ) is a LU otimal solution to (WD). Thom 4.3 (Stict convs duality) Lt X 0 b an on subst of R n. Lt F and g j, j =,2,...,m, b diffntiabl on X 0. Suos that * and (y *, ξ *L, ξ *U, μ * ) a th fasibl solutions to (IVP) and (WD), sctivly. Assum that ξ *L F L + ξ *U F U + m μ* j g j is

10 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 0 of 4 htt:// stictly (, ) ρ (η, θ)-inv with sct to η, θ at y * with ρ 0 and ξ *L F L( *) + ξ *U F U( *) + * ) ξ *L F L( y *) + ξ *U F U( y *) + y * ). (0) Thn * = y *. Poof Now w assum that * y * and hibit a contadiction. Fom th assumtion that ξ *L F L + ξ *U F U + m μ* j g j is stictly (, ) ρ (η, θ)-inv at y *,whav [ (ξ *L F L ( * )+ξ *U F U ( * )+ m * )) (ξ *L F L (y * )+ξ *U F U (y * )+ m y *))} ] [ > ξ *L F L( y *) + ξ *U F U( y *) + μ * j g j( y * )] ( η( *,y *) ) + ρ ( θ *, y *) 2. Fom th fasibility of (y *, ξ *L, ξ *U, μ * ) to (WD), th abov inquality togth with th hyothsis ρ 0yilds [ (ξ *L F L ( * )+ξ *U F U ( * )+ m * )) (ξ *L F L (y * )+ξ *U F U (y * )+ m y *))} ] >0. Sinc > 0, using th oty of an onntial function, w gt ξ *L F L( *) + ξ *U F U( *) + * ) > ξ *L F L( y *) + ξ *U F U( y *) + y * ), which contadicts (0). This comltsth oof. 5 Mond-Wi ty duality In this sction, w consid th following Mond-Wi ty dual oblm fo (IVP): (MWD) ma F(y)= [ F L (y), F U (y) ] subjct to ξ L F L (y)+ξ U F U (y)+ μ j g j (y)=0, () μ j g j (y) 0, j =,2,...,m, (2) ξ L >0,ξ U >0,μ j 0, j =,2,...,m. (3) Dfinition 5. Lt (y *, ξ *L, ξ *U, μ * ) b a fasibl solution of dual oblm (MWD). W say that (y *, ξ *L, ξ *U, μ * ) is a LU otimal solution of dual oblm (MWD) if th ists no (y, ξ *L, ξ *U, μ * )suchthatf(y * )< LU F(y). Thom 5. (Wak duality) Lt X 0 b an on subst of R n. Lt F and g j, j =,2,...,m, b diffntiabl on X 0. Suos that and (y, ξ L, ξ U, μ) a th fasibl solutions to (IVP) and (MWD), sctivly. Futh assum that th ist ξ L >0and ξ U >0and μ j 0, j =

11 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag of 4 htt:// such that (ξ L F L +ξ U F U ) is (, ) ρ (η, θ)-sudo-inv with sct to η, θ and m μ jg j is (, ) ρ 2 (η, θ)-quasi-inv with sct to η, θ at y with (ρ + ρ 2 ) 0. Thn F() LU F(y). Poof Suos contay to th sult that F()< LU F(y). That is, F L ()<F L (y), F U ()<F U (y), o F L () F L (y), F U ()<F U (y), o F L ()<F L (y), F U () F U (y). Sinc ξ L >0andξ U > 0, fom th abov inqualitis, w hav ξ L F L ()+ξ U F U ()<ξ L F L (y)+ξ U F U (y). (4) On th oth hand, sinc μ j 0, j =,2,...,m, fom th fasibility of and (y, ξ L, ξ U, μ)to (IVP) and (MWD), sctivly, w obtain μ j g j () μ j g j (y). Sinc > 0, using th oty of an onntial function, w gt [ m μ j g j () m μ j g j (y)} ] 0, which togth with th assumtion that m μ jg j is (, ) ρ 2 (η, θ)-quasi-inv at y, givs μ j g j (y) ( η(,y) ) + ρ 2 θ(, y) 2 0. Thfo, fom () and th hyothsis that (ρ + ρ 2 ) 0, th abov inquality yilds ( η(,y) )[ ξ L F L (y)+ξ U F U (y) ] + ρ θ(, y) 2 0, which togth with th assumtion that ξ L F L + ξ U F U is (, ) ρ (η, θ)-sudo-inv at y givs [ (ξ L F L ()+ξ U F U ()) (ξ L F L (y)+ξ U F U (y))} ] 0. Sinc > 0, using th oty of an onntial function, w gt ξ L F L ()+ξ U F U () ξ L F L (y)+ξ U F U (y), which contadicts (4). This comlts th oof.

12 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 2 of 4 htt:// Thom 5.2 (Stong duality) Lt * b a LU otimal solution to (IVP) at which Kuhn- Tuck constaints qualification a satisfid. Thn th ist ξ *L >0,ξ *U >0and μ * 0 such that ( *, ξ *L, ξ *U, μ * ) is fasibl fo (MWD) and th two objctivs hav th sam valu. Futh, if th hyothsis of wak duality Thom 5. holds fo all fasibl solutions (y *, ξ *L, ξ *U, μ * ), thn ( *, ξ *L, ξ *U, μ * ) is a LU otimal solution to (MWD). Poof Sinc * is a LU otimal solution to (IVP) and th Kuhn-Tuck constaints qualification a satisfid at *, thn by Thom 2., thistmultilisξ *L >0,ξ *U >0, μ * j 0, j =,2,...,m,suchthat ξ *L F L( *) + ξ *U F U( *) + μ * j g j( * ) =0, * ) =0, which yilds that ( *, ξ *L, ξ *U, μ * ) is a fasibl solution fo (MWD) and cosonding objctiv valus a sam. Futh, if ( *, ξ *L, ξ *U, μ * ) is not a LU otimal solution of (MWD), thn th ists a fasibl solution (y *, ξ *L, ξ *U, μ * )fo(mwd)suchthat F ( *) < LU F ( y *), which contadicts wak duality Thom 5..Hnc( *, ξ *L, ξ *U, μ * ) is a LU otimal solution to (MWD). Thom 5.3 (Stict convs duality) Lt X 0 b an on subst of R n. Lt F and g j, j =,2,...,m, b diffntiabl on X 0. Suos that * and (y *, ξ *L, ξ *U, μ * ) a th fasibl solutions to (IVP) and (MWD), sctivly. Assum that ξ *L F L + ξ *U F U is stictly (, ) ρ (η, θ)-sudo-inv and m μ* j g j is (, ) ρ 2 (η, θ)-quasi-inv with sct to η, θ at y * with (ρ + ρ 2 ) 0 and ξ *L F L( *) + ξ *U F U( *) ξ *L F L( y *) + ξ *U F U( y *). (5) Thn * = y *. Poof Now w assum that * y * and hibit a contadiction. Fom th assumtion that (y *, ξ *L, ξ *U, μ * ) is a fasibl solution fo (MWD), w gt ξ *L F L( y *) + ξ *U F U( y *) + μ * j g j( y * ) =0. (6) Sinc μ * j 0, j =,2,...,m, fom th fasibility of * and (y *, ξ *L, ξ *U, μ * )to(ivp)and (MWD), sctivly, w obtain * ) y * ).

13 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 3 of 4 htt:// As > 0, using th oty of an onntial function, w gt [ m * ) m y *)} ] 0, which togth with th assumtion that m μ* j g j is (, ) ρ 2 (η, θ)-quasi-inv at y * givs μ * j g j( y * )( η(*,y *) ) ( + ρ 2 θ *, y *) 2 0. Thfo, fom (6) and th hyothsis that (ρ + ρ 2 ) 0, th abov inquality yilds ( η( *,y *) )[ ξ *L F L( y *) + ξ *U F U( y *)] ( + ρ θ *, y *) 2 0, which togth with th assumtion that ξ *L F L +ξ *U F U is stictly (, ) ρ (η, θ)-sudoinv at y * givs [ (ξ *L F L ( * )+ξ *U F U ( * )) (ξ *L F L (y * )+ξ *U F U (y *))} ] >0. Sinc > 0, using th oty of an onntial function, w gt ξ *L F L( *) + ξ *U F U( *) > ξ *L F L( y *) + ξ *U F U( y *), which contadicts (5). This comltsth oof. 6 Conclusion In this a, w hav divd sufficint otimality conditions fo a class of intval-valud otimization oblms und gnalizd inv functions. Wak, stong and stict convs duality thoms a discussd fo two tys of th dual modls. It will b intsting to obtain th otimality and duality thom fo a class of intval-valud ogamming und gnalizd invity assumtions in which th involvd functions a non-smooth. Moov, it will also b intsting to s whth th scond-od duality sults fo a class of intval-valud ogamming oblm hold o not. This will oint th futu sach of th authos. Comting intsts Th authos dcla that thy hav no comting intsts. Authos contibutions All authos caid out th oof. All authos concivd of th study, and aticiatd in its dsign and coodination. All authos ad and aovd th final manuscit. Autho dtails Datmnt of Mathmatics and Statistics, King Fahd Univsity of Ptolum and Minals, Dhahan, 326, Saudi Aabia. 2 Pmannt addss: Datmnt of Mathmatics, Aligah Muslim Univsity, Aligah, , India. 3 Datmnt of Alid Mathmatics, Indian School of Mins, Jhakhand, Dhanbad , India. Acknowldgmnts Izha Ahmad thanks th King Fahd Univsity of Ptolum and Minals, Dhahan-326, Saudi Aabia fo th suot und th Intnal Pojct No. IN037. Th authos wish to thank th fs fo thi sval valuabl suggstions which hav considably imovd th sntation of this aticl. Rcivd: 27 Mach 203 Acctd: 3 Jun 203 Publishd: 3 July 203

14 Ahmad t al. Jounal of Inqualitis and Alications 203, 203:33 Pag 4 of 4 htt:// Rfncs. Chans, A, Ganot, F, Phillis, F: An algoithm fo solving intval lina ogamming oblms. O. Rs. 25, (977) 2. Stu, RE: Algoithms fo lina ogamming oblms with intval objctiv function cofficints. Math. O. Rs. 6, (98) 3. Uli, B, Nadau, R: An intactiv mthod to multiobjctiv lina ogamming oblms with intval cofficints. INFOR 30, (992) 4. Chanas, S, Kuchta, D: Multiobjctiv ogamming in otimization of intval objctiv functions-a gnalizd aoach. Eu. J. O. Rs. 94, (996) 5. Wu, H-C: Duality thoy fo otimization oblms with intval-valud objctiv functions. J. Otim. Thoy Al. 44, (200) 6. Stancu-Minasian, IM, Tigan, S: Multiobjctiv mathmatical ogamming with inact data. In: Slowiński, R, Tghm, J (ds.) Stochastic vsus Fuzzy Aoachs to Multiobjctiv Mathmatical Pogamming und Unctainty, Kluw Acadmic, Boston (990) 7. Stancu-Minasian, IM: Stochastic Pogamming with Multil Objctiv Function. Ridl, Dodcht (984) 8. Wu, H-C: Th Kaush-Kuhn-Tuck otimality conditions in an otimization oblm with intval-valud objctiv function. Eu. J. O. Rs. 76, (2007) 9. Wu, H-C: On intval-valud nonlina ogamming oblms. J. Math. Anal. Al. 338, (2008) 0. Wu, H-C: Wolf duality fo intval-valud otimization. J. Otim. Thoy Al. 38, (2008). Zhou, HC, Wang, YJ: Otimality condition and mid duality fo intval-valud otimization. In: Fuzzy Infomation and Engining, Volum 2. Pocdings of th Thid Intnational Confnc on Fuzzy Infomation and Engining (ICFIE 2009). Advancs in Intllignt and Soft Comuting, vol. 62, Sing, Blin (2009) 2. Bhuj, AK, Panda, G: Efficint solution of intval otimization oblm. Math. Mthods O. Rs. 76, (202) 3. Zhang, J, Liu, S, Li, L, Fng, Q: Th KKT otimality conditions in a class of gnalizd conv otimization oblms with an intval-valud objctiv function. Otim. Ltt. (202). doi:0.007/s Hanson, MA: On sufficincy of th Kuhn-Tuck conditions. J. Math. Anal. Al. 80, (98) 5. Aana, M, Ruiz, G, Rufián, A (ds.): Otimality Conditions in Vcto Otimization. Bntham Scinc Publishs, Bussum (200) 6. Zalmai, GJ: Gnalizd sufficincy citia in continuous-tim ogamming with alication to a class of vaiational-ty inqualitis. J. Math. Anal. Al. 53, (990) 7. Antczak, T: (, )-Inv sts and functions. J. Math. Anal. Al. 263, (200) 8. Mandal, P, Nahak, C: Symmtic duality with (, ) ρ (η, θ)-invity. Al. Math. Comut. 27, (20) 9. Jayswal, A, Stancu-Minasian, IM, Ahmad, I: On sufficincy and duality fo a class of intval-valud ogamming oblms. Al. Math. Comut. 28, (20) 20. Sun, Y, Wang, L: Otimality conditions and duality in nondiffntiabl intval-valud ogamming. J. Ind. Manag. Otim. 9, 3-42 (203) doi:0.86/ x Cit this aticl as: Ahmad t al.: On intval-valud otimization oblms with gnalizd inv functions. Jounal of Inqualitis and Alications :33.

ADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS. Ghiocel Groza*, S. M. Ali Khan** 1. Introduction

ADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS. Ghiocel Groza*, S. M. Ali Khan** 1. Introduction ADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS Ghiocl Goza*, S. M. Ali Khan** Abstact Th additiv intgal functions with th cofficints in a comlt non-achimdan algbaically closd fild of chaactistic 0 a studid.

More information

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

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

More information

E F. and H v. or A r and F r are dual of each other.

E F. and H v. or A r and F r are dual of each other. A Duality Thom: Consid th following quations as an xampl = A = F μ ε H A E A = jωa j ωμε A + β A = μ J μ A x y, z = J, y, z 4π E F ( A = jω F j ( F j β H F ωμε F + β F = ε M jβ ε F x, y, z = M, y, z 4π

More information

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

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

More information

A STUDY OF PROPERTIES OF SOFT SET AND ITS APPLICATIONS

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

More information

An Elementary Approach to a Model Problem of Lagerstrom

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

More information

Extinction Ratio and Power Penalty

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

More information

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

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

More information

Overview. 1 Recall: continuous-time Markov chains. 2 Transient distribution. 3 Uniformization. 4 Strong and weak bisimulation

Overview. 1 Recall: continuous-time Markov chains. 2 Transient distribution. 3 Uniformization. 4 Strong and weak bisimulation Rcall: continuous-tim Makov chains Modling and Vification of Pobabilistic Systms Joost-Pit Katon Lhstuhl fü Infomatik 2 Softwa Modling and Vification Goup http://movs.wth-aachn.d/taching/ws-89/movp8/ Dcmb

More information

PH672 WINTER Problem Set #1. Hint: The tight-binding band function for an fcc crystal is [ ] (a) The tight-binding Hamiltonian (8.

PH672 WINTER Problem Set #1. Hint: The tight-binding band function for an fcc crystal is [ ] (a) The tight-binding Hamiltonian (8. PH67 WINTER 5 Poblm St # Mad, hapt, poblm # 6 Hint: Th tight-binding band function fo an fcc cstal is ( U t cos( a / cos( a / cos( a / cos( a / cos( a / cos( a / ε [ ] (a Th tight-binding Hamiltonian (85

More information

Mid Year Examination F.4 Mathematics Module 1 (Calculus & Statistics) Suggested Solutions

Mid Year Examination F.4 Mathematics Module 1 (Calculus & Statistics) Suggested Solutions Mid Ya Eamination 3 F. Matmatics Modul (Calculus & Statistics) Suggstd Solutions Ma pp-: 3 maks - Ma pp- fo ac qustion: mak. - Sam typ of pp- would not b countd twic fom wol pap. - In any cas, no pp maks

More information

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

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

More information

Chapter 9. Optimization: One Choice Variable. 9.1 Optimum Values and Extreme Values

Chapter 9. Optimization: One Choice Variable. 9.1 Optimum Values and Extreme Values RS - Ch 9 - Optimization: On Vaiabl Chapt 9 Optimization: On Choic Vaiabl Léon Walas 8-9 Vildo Fdico D. Pato 88 9 9. Optimum Valus and Etm Valus Goal vs. non-goal quilibium In th optimization pocss, w

More information

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

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

More information

Einstein Equations for Tetrad Fields

Einstein 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 information

An Axisymmetric Inverse Approach for Cold Forging Modeling

An Axisymmetric Inverse Approach for Cold Forging Modeling An Axisymmtic Invs Aoach fo Cold Foging Modling Ali Halouani, uming Li, Boussad Abbès, ing-qiao Guo Abstact his a snts th fomulation of an axi-symmtic lmnt basd on an fficint mthod calld th Invs Aoach

More information

Supplementary Materials

Supplementary Materials 6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic

More information

Derangements and Applications

Derangements and Applications 2 3 47 6 23 Journal of Intgr Squncs, Vol. 6 (2003), Articl 03..2 Drangmnts and Applications Mhdi Hassani Dpartmnt of Mathmatics Institut for Advancd Studis in Basic Scincs Zanjan, Iran mhassani@iasbs.ac.ir

More information

On Jackson's Theorem

On Jackson's Theorem It. J. Cotm. Math. Scics, Vol. 7, 0, o. 4, 49 54 O Jackso's Thom Ema Sami Bhaya Datmt o Mathmatics, Collg o Educatio Babylo Uivsity, Babil, Iaq mabhaya@yahoo.com Abstact W ov that o a uctio W [, ], 0

More information

New bounds on Poisson approximation to the distribution of a sum of negative binomial random variables

New bounds on Poisson approximation to the distribution of a sum of negative binomial random variables Sogklaaka J. Sc. Tchol. 4 () 4-48 Ma. -. 8 Ogal tcl Nw bouds o Posso aomato to th dstbuto of a sum of gatv bomal adom vaabls * Kat Taabola Datmt of Mathmatcs Faculty of Scc Buaha Uvsty Muag Chobu 3 Thalad

More information

Logical Topology Design for WDM Networks Using Survivable Routing

Logical Topology Design for WDM Networks Using Survivable Routing Logical Toology Dsign fo WDM Ntwoks Using Suvivabl Routing A. Jakl, S. Bandyoadhyay and Y. Ana Univsity of Windso Windso, Canada N9B 3P4 {aunita, subi, ana@uwindso.ca Abstact Suvivabl outing of a logical

More information

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM Elctronic Journal of Diffrntial Equations, Vol. 2003(2003), No. 92, pp. 1 6. ISSN: 1072-6691. URL: http://jd.math.swt.du or http://jd.math.unt.du ftp jd.math.swt.du (login: ftp) LINEAR DELAY DIFFERENTIAL

More information

Basic Polyhedral theory

Basic Polyhedral theory Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist

More information

A NEW SOLUTION FOR SHALLOW AND DEEP TUNNELS BY CONSIDERING THE GRAVITATIONAL LOADS

A NEW SOLUTION FOR SHALLOW AND DEEP TUNNELS BY CONSIDERING THE GRAVITATIONAL LOADS A NEW SOLUTION FOR SHALLOW AND DEEP TUNNELS BY CONSIDERING THE GRAVITATIONAL LOADS MOHAMMAD REZA ZAREIFARD and AHMAD FAHIMIFAR about th authos Mohammad Rza Zaifad Amikabi Univsity of Tchnology Than, Ian

More information

SCHUR S THEOREM REU SUMMER 2005

SCHUR S THEOREM REU SUMMER 2005 SCHUR S THEOREM REU SUMMER 2005 1. Combinatorial aroach Prhas th first rsult in th subjct blongs to I. Schur and dats back to 1916. On of his motivation was to study th local vrsion of th famous quation

More information

Centralized Multi-Node Repair in Distributed Storage

Centralized Multi-Node Repair in Distributed Storage Cntalizd ulti-nod Rpai in Distibutd Stoag awn Zogui, and Zhiying Wang Cnt fo Pvasiv Communications and Computing (CPCC) Univsity of Califonia, Ivin, USA {mzogui,zhiying}@uci.du Abstact In distibutd stoag

More information

8 - GRAVITATION Page 1

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

More information

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation Pof. D. I. Nass Phys57 (T-3) Sptmb 8, 03 Foui_Tansf_phys57_T3 Foui tansfoms (Chapt 5) Foui intgals a gnalizations of Foui sis. Th sis psntation a0 nπx nπx f ( x) = + [ an cos + bn sin ] n = of a function

More information

u 3 = u 3 (x 1, x 2, x 3 )

u 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 information

2008 AP Calculus BC Multiple Choice Exam

2008 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 information

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

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

More information

International Journal of Industrial Engineering Computations

International Journal of Industrial Engineering Computations Intnational Jounal of Industial Engining Computations 5 (4 65 74 Contnts lists availabl at GowingScinc Intnational Jounal of Industial Engining Computations hompag: www.gowingscinc.com/ijic A nw modl fo

More information

Two-Wheeled Welding Mobile Robot for Tracking a Smooth Curved Welding Path Using Adaptive Sliding-Mode Control Technique

Two-Wheeled Welding Mobile Robot for Tracking a Smooth Curved Welding Path Using Adaptive Sliding-Mode Control Technique Intnational wo-whld Jounal Wlding of Contol, Mobil Automation, Robot fo acking and Systms, a Smooth vol. Cuvd, no. 3, Wlding pp. 83-94, Path Using Jun Adaptiv 7 Sliding-Mod 83 wo-whld Wlding Mobil Robot

More information

Estimation of a Random Variable

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

More information

On the Kinematics of Robotic-assisted Minimally Invasive Surgery

On the Kinematics of Robotic-assisted Minimally Invasive Surgery , Vol. 34, No. 2, 203,. 69 82, ISSN 890 328 On Kinmatics of Robotic-assistd Minimally Invasiv Sugy Pål Johan Fom Datmnt of Mamatical Scincs and Tchnology, Nogian Univsity of Lif Scincs, 432 Ås, Noay. E-mail:

More information

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals Hydogn atom Engy lvls and wav functions Obital momntum, lcton spin and nucla spin Fin and hypfin intaction Hydogn obitals Hydogn atom A finmnt of th Rydbg constant: R ~ 109 737.3156841 cm -1 A hydogn mas

More information

Network Congestion Games

Network Congestion Games Ntwork Congstion Gams Assistant Profssor Tas A&M Univrsity Collg Station, TX TX Dallas Collg Station Austin Houston Bst rout dpnds on othrs Ntwork Congstion Gams Travl tim incrass with congstion Highway

More information

Shor s Algorithm. Motivation. Why build a classical computer? Why build a quantum computer? Quantum Algorithms. Overview. Shor s factoring algorithm

Shor s Algorithm. Motivation. Why build a classical computer? Why build a quantum computer? Quantum Algorithms. Overview. Shor s factoring algorithm Motivation Sho s Algoith It appas that th univs in which w liv is govnd by quantu chanics Quantu infoation thoy givs us a nw avnu to study & tst quantu chanics Why do w want to build a quantu coput? Pt

More information

Midterm Exam. CS/ECE 181B Intro to Computer Vision. February 13, :30-4:45pm

Midterm Exam. CS/ECE 181B Intro to Computer Vision. February 13, :30-4:45pm Nam: Midtm am CS/C 8B Into to Comput Vision Fbua, 7 :-4:45pm las spa ouslvs to th dg possibl so that studnts a vnl distibutd thoughout th oom. his is a losd-boo tst. h a also a fw pags of quations, t.

More information

School of Electrical Engineering. Lecture 2: Wire Antennas

School of Electrical Engineering. Lecture 2: Wire Antennas School of lctical ngining Lctu : Wi Antnnas Wi antnna It is an antnna which mak us of mtallic wis to poduc a adiation. KT School of lctical ngining www..kth.s Dipol λ/ Th most common adiato: λ Dipol 3λ/

More information

SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH.

SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH. SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH. K VASUDEVAN, K. SWATHY AND K. MANIKANDAN 1 Dpartmnt of Mathmatics, Prsidncy Collg, Chnnai-05, India. E-Mail:vasu k dvan@yahoo.com. 2,

More information

ON RIGHT(LEFT) DUO PO-SEMIGROUPS. S. K. Lee and K. Y. Park

ON RIGHT(LEFT) DUO PO-SEMIGROUPS. S. K. Lee and K. Y. Park Kangwon-Kyungki Math. Jour. 11 (2003), No. 2, pp. 147 153 ON RIGHT(LEFT) DUO PO-SEMIGROUPS S. K. L and K. Y. Park Abstract. W invstigat som proprtis on right(rsp. lft) duo po-smigroups. 1. Introduction

More information

Spectral Synthesis in the Heisenberg Group

Spectral Synthesis in the Heisenberg Group Intrnational Journal of Mathmatical Analysis Vol. 13, 19, no. 1, 1-5 HIKARI Ltd, www.m-hikari.com https://doi.org/1.1988/ijma.19.81179 Spctral Synthsis in th Hisnbrg Group Yitzhak Wit Dpartmnt of Mathmatics,

More information

217Plus TM Integrated Circuit Failure Rate Models

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

More information

INTEGRATION BY PARTS

INTEGRATION BY PARTS Mathmatics Rvision Guids Intgration by Parts Pag of 7 MK HOME TUITION Mathmatics Rvision Guids Lvl: AS / A Lvl AQA : C Edcl: C OCR: C OCR MEI: C INTEGRATION BY PARTS Vrsion : Dat: --5 Eampls - 6 ar copyrightd

More information

CBSE-XII-2013 EXAMINATION (MATHEMATICS) The value of determinant of skew symmetric matrix of odd order is always equal to zero.

CBSE-XII-2013 EXAMINATION (MATHEMATICS) The value of determinant of skew symmetric matrix of odd order is always equal to zero. CBSE-XII- EXAMINATION (MATHEMATICS) Cod : 6/ Gnal Instuctions : (i) All qustions a compulso. (ii) Th qustion pap consists of 9 qustions dividd into th sctions A, B and C. Sction A compiss of qustions of

More information

GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL

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

More information

INCOMPLETE KLOOSTERMAN SUMS AND MULTIPLICATIVE INVERSES IN SHORT INTERVALS. xy 1 (mod p), (x, y) I (j)

INCOMPLETE KLOOSTERMAN SUMS AND MULTIPLICATIVE INVERSES IN SHORT INTERVALS. xy 1 (mod p), (x, y) I (j) INCOMPLETE KLOOSTERMAN SUMS AND MULTIPLICATIVE INVERSES IN SHORT INTERVALS T D BROWNING AND A HAYNES Abstract W invstigat th solubility of th congrunc xy (mod ), whr is a rim and x, y ar rstrictd to li

More information

Geometrical Analysis of the Worm-Spiral Wheel Frontal Gear

Geometrical Analysis of the Worm-Spiral Wheel Frontal Gear Gomtical Analysis of th Wom-Spial Whl Fontal Ga SOFIA TOTOLICI, ICOLAE OACEA, VIRGIL TEODOR, GABRIEL FRUMUSAU Manufactuing Scinc and Engining Dpatmnt, Dunaa d Jos Univsity of Galati, Domnasca st., 8000,

More information

A Study of Generalized Thermoelastic Interaction in an Infinite Fibre-Reinforced Anisotropic Plate Containing a Circular Hole

A Study of Generalized Thermoelastic Interaction in an Infinite Fibre-Reinforced Anisotropic Plate Containing a Circular Hole Vol. 9 0 ACTA PHYSICA POLONICA A No. 6 A Study of Gnalizd Thmolastic Intaction in an Infinit Fib-Rinfocd Anisotopic Plat Containing a Cicula Hol Ibahim A. Abbas a,b, and Abo-l-nou N. Abd-alla a,b a Dpatmnt

More information

cycle that does not cross any edges (including its own), then it has at least

cycle that does not cross any edges (including its own), then it has at least W prov th following thorm: Thorm If a K n is drawn in th plan in such a way that it has a hamiltonian cycl that dos not cross any dgs (including its own, thn it has at last n ( 4 48 π + O(n crossings Th

More information

Extensive Form Games with Incomplete Information. Microeconomics II Signaling. Signaling Examples. Signaling Games

Extensive Form Games with Incomplete Information. Microeconomics II Signaling. Signaling Examples. Signaling Games Extnsiv Fom Gams ith Incomplt Inomation Micoconomics II Signaling vnt Koçksn Koç Univsity o impotant classs o xtnsiv o gams ith incomplt inomation Signaling Scning oth a to play gams ith to stags On play

More information

CDS 110b: Lecture 8-1 Robust Stability

CDS 110b: Lecture 8-1 Robust Stability DS 0b: Lct 8- Robst Stabilit Richad M. Ma 3 Fba 006 Goals: Dscib mthods fo psnting nmodld dnamics Div conditions fo obst stabilit Rading: DFT, Sctions 4.-4.3 3 Fb 06 R. M. Ma, altch Gam lan: Robst fomanc

More information

COMPSCI 230 Discrete Math Trees March 21, / 22

COMPSCI 230 Discrete Math Trees March 21, / 22 COMPSCI 230 Dict Math Mach 21, 2017 COMPSCI 230 Dict Math Mach 21, 2017 1 / 22 Ovviw 1 A Simpl Splling Chck Nomnclatu 2 aval Od Dpth-it aval Od Badth-it aval Od COMPSCI 230 Dict Math Mach 21, 2017 2 /

More information

Two Products Manufacturer s Production Decisions with Carbon Constraint

Two 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 information

ON A SECOND ORDER RATIONAL DIFFERENCE EQUATION

ON A SECOND ORDER RATIONAL DIFFERENCE EQUATION Hacttp Journal of Mathmatics and Statistics Volum 41(6) (2012), 867 874 ON A SECOND ORDER RATIONAL DIFFERENCE EQUATION Nourssadat Touafk Rcivd 06:07:2011 : Accptd 26:12:2011 Abstract In this papr, w invstigat

More information

Theoretical Study of Electromagnetic Wave Propagation: Gaussian Bean Method

Theoretical Study of Electromagnetic Wave Propagation: Gaussian Bean Method Applid Mathmatics, 3, 4, 466-47 http://d.doi.og/.436/am.3.498 Publishd Onlin Octob 3 (http://www.scip.og/jounal/am) Thotical Study of Elctomagntic Wav Popagation: Gaussian Ban Mthod E. I. Ugwu, J. E. Ekp,

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!

More information

ESCI 341 Atmospheric Thermodynamics Lesson 16 Pseudoadiabatic Processes Dr. DeCaria

ESCI 341 Atmospheric Thermodynamics Lesson 16 Pseudoadiabatic Processes Dr. DeCaria ESCI 34 Atmohi hmoynami on 6 Puoaiabati Po D DCaia fn: Man, A an FE obitaill, 97: A omaion of th uialnt otntial tmatu an th tati ngy, J Atmo Si, 7, 37-39 Btt, AK, 974: Futh ommnt on A omaion of th uialnt

More information

GRAVITATION. (d) If a spring balance having frequency f is taken on moon (having g = g / 6) it will have a frequency of (a) 6f (b) f / 6

GRAVITATION. (d) If a spring balance having frequency f is taken on moon (having g = g / 6) it will have a frequency of (a) 6f (b) f / 6 GVITTION 1. Two satllits and o ound a plant P in cicula obits havin adii 4 and spctivly. If th spd of th satllit is V, th spd of th satllit will b 1 V 6 V 4V V. Th scap vlocity on th sufac of th ath is

More information

Loss factor for a clamped edge circular plate subjected to an eccentric loading

Loss factor for a clamped edge circular plate subjected to an eccentric loading ndian ounal of Engining & Matials Scincs Vol., Apil 4, pp. 79-84 Loss facto fo a clapd dg cicula plat subjctd to an ccntic loading M K Gupta a & S P Niga b a Mchanical Engining Dpatnt, National nstitut

More information

Aakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics

Aakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics Aakash A UNIQUE PPRTUNITY T HELP YU FULFIL YUR DREAMS Fo Class XII Studying / Passd Studnts Physics, Chmisty & Mathmatics Rgistd ffic: Aakash Tow, 8, Pusa Road, Nw Dlhi-0005. Ph.: (0) 4763456 Fax: (0)

More information

2 MARTIN GAVALE, GÜNTER ROTE R Ψ 2 3 I 4 6 R Ψ 5 Figu I ff R Ψ lcm(3; 4; 6) = 12. Th componnts a non-compaabl, in th sns of th o

2 MARTIN GAVALE, GÜNTER ROTE R Ψ 2 3 I 4 6 R Ψ 5 Figu I ff R Ψ lcm(3; 4; 6) = 12. Th componnts a non-compaabl, in th sns of th o REAHABILITY OF FUZZY MATRIX PERIOD MARTIN GAVALE, GÜNTER ROTE Abstact. Th computational complxity of th matix piod achability (MPR) poblm in a fuzzy algba B is studid. Givn an n n matix A with lmnts in

More information

(Upside-Down o Direct Rotation) β - Numbers

(Upside-Down o Direct Rotation) β - Numbers Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

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

More information

10. The Discrete-Time Fourier Transform (DTFT)

10. 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 information

Exactness Property of the Exact Absolute Value Penalty Function Method for Solving Convex Nondifferentiable Interval-Valued Optimization Problems

Exactness Property of the Exact Absolute Value Penalty Function Method for Solving Convex Nondifferentiable Interval-Valued Optimization Problems J Optim Theory Appl (2018) 176:205 224 https://doi.org/10.1007/s10957-017-1204-2 Exactness Property of the Exact Absolute Value Penalty Function Method for Solving Convex Nondifferentiable Interval-Valued

More information

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming CPSC 665 : An Algorithmist s Toolkit Lctur 4 : 21 Jan 2015 Lcturr: Sushant Sachdva Linar Programming Scrib: Rasmus Kyng 1. Introduction An optimization problm rquirs us to find th minimum or maximum) of

More information

Chapter 4: Algebra and group presentations

Chapter 4: Algebra and group presentations Chapt 4: Algba and goup psntations Matthw Macauly Dpatmnt of Mathmatical Scincs Clmson Univsity http://www.math.clmson.du/~macaul/ Math 4120, Sping 2014 M. Macauly (Clmson) Chapt 4: Algba and goup psntations

More information

Higher order derivatives

Higher 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 information

Research Article Norm and Essential Norm of an Integral-Type Operator from the Dirichlet Space to the Bloch-Type Space on the Unit Ball

Research Article Norm and Essential Norm of an Integral-Type Operator from the Dirichlet Space to the Bloch-Type Space on the Unit Ball Hindawi Publishing Corporation Abstract and Applid Analysis Volum 2010, Articl ID 134969, 9 pags doi:10.1155/2010/134969 Rsarch Articl Norm and Essntial Norm of an Intgral-Typ Oprator from th Dirichlt

More information

Calculus concepts derivatives

Calculus concepts derivatives All rasonabl fforts hav bn mad to mak sur th nots ar accurat. Th author cannot b hld rsponsibl for any damags arising from th us of ths nots in any fashion. Calculus concpts drivativs Concpts involving

More information

θ θ φ EN2210: Continuum Mechanics Homework 2: Polar and Curvilinear Coordinates, Kinematics Solutions 1. The for the vector i , calculate:

θ θ φ EN2210: Continuum Mechanics Homework 2: Polar and Curvilinear Coordinates, Kinematics Solutions 1. The for the vector i , calculate: EN0: Continm Mchanics Homwok : Pola and Cvilina Coodinats, Kinmatics Soltions School of Engining Bown Univsity x δ. Th fo th vcto i ij xx i j vi = and tnso S ij = + 5 = xk xk, calclat: a. Thi componnts

More information

u r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C

u r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C Tchniqus of Intgration c Donald Kridr and Dwight Lahr In this sction w ar going to introduc th first approachs to valuating an indfinit intgral whos intgrand dos not hav an immdiat antidrivativ. W bgin

More information

Mechanism Analysis of Dynamic Compaction based on Large Deformation

Mechanism Analysis of Dynamic Compaction based on Large Deformation Th Opn Civil Engining Jounal,,, - Opn Accss Mchanism Analysis of Dynamic Compaction basd on Lag Dfomation Xi Nnggang *, Chn Yun, Y Y and Wang Lu Anhui Univsity of Tchnology, Maanshan, Anhui Povinc, China,

More information

Investigation Effect of Outage Line on the Transmission Line for Karbalaa-132Kv Zone in Iraqi Network

Investigation Effect of Outage Line on the Transmission Line for Karbalaa-132Kv Zone in Iraqi Network Intnational Rsach Jounal of Engining and Tchnology (IRJET) -ISSN: - Volum: Issu: Jun - www.ijt.nt p-issn: - Invstigation Effct of Outag on th Tansmission fo Kabalaa-Kv Zon in Iaqi Ntwok Rashid H. AL-Rubayi

More information

APPENDIX II Electrical Engineering (Archiv fur Elektrotechnik).

APPENDIX II Electrical Engineering (Archiv fur Elektrotechnik). Rintd with mission fom th ublish. APPENDIX II Elctical Engining (Achiv fu Elktotchnik). Publication P2 ISSN: 948-792 (Pint), 432-487 (Onlin) DOI:.7/s22-6-327-5 Th oiginal ublication is availabl at www.singlink.com

More information

Self-interaction mass formula that relates all leptons and quarks to the electron

Self-interaction mass formula that relates all leptons and quarks to the electron Slf-intraction mass formula that rlats all lptons and quarks to th lctron GERALD ROSEN (a) Dpartmnt of Physics, Drxl Univrsity Philadlphia, PA 19104, USA PACS. 12.15. Ff Quark and lpton modls spcific thoris

More information

Inference Methods for Stochastic Volatility Models

Inference Methods for Stochastic Volatility Models Intrnational Mathmatical Forum, Vol 8, 03, no 8, 369-375 Infrnc Mthods for Stochastic Volatility Modls Maddalna Cavicchioli Cá Foscari Univrsity of Vnic Advancd School of Economics Cannargio 3, Vnic, Italy

More information

ON A GENERALIZED PROBABILITY DISTRIBUTION IN ASSOCIATION WITH ALEPH ( ) - FUNCTION

ON A GENERALIZED PROBABILITY DISTRIBUTION IN ASSOCIATION WITH ALEPH ( ) - FUNCTION Intnational Jounal of Engining, Scinc and athmatic Vol. 8, Iu, Januay 8, ISSN: 3-94 Impact Facto: 6.765 Jounal Hompag: http://www.ijm.co.in, Email: ijmj@gmail.com Doubl-Blind P Riwd Rfd Opn Acc Intnational

More information

What Makes Production System Design Hard?

What Makes Production System Design Hard? What Maks Poduction Systm Dsign Had? 1. Things not always wh you want thm whn you want thm wh tanspot and location logistics whn invntoy schduling and poduction planning 2. Rsoucs a lumpy minimum ffctiv

More information

Knowledge Creation with Parallel Teams: Design of Incentives and the Role of Collaboration

Knowledge Creation with Parallel Teams: Design of Incentives and the Role of Collaboration Association fo nfomation Systms AS Elctonic Libay (ASL) AMCS 2009 Pocdings Amicas Confnc on nfomation Systms (AMCS) 2009 Knowldg Cation with Paalll Tams: Dsign of ncntivs and th Rol of Collaboation Shanka

More information

Analysis and experimental validation of a sensor-based event-driven controller 1

Analysis and experimental validation of a sensor-based event-driven controller 1 Analysis and ximntal validation of a snso-basd vnt-divn contoll 1 J.H. Sand Eindhovn Univsity of Tchnology Dt. of Elct. Eng. Contol Systms gou W.P.M.H. Hmls Eindhovn Univsity of Tchnology Dt. of Mch. Eng.

More information

Path (space curve) Osculating plane

Path (space curve) Osculating plane Fo th cuilin motion of pticl in spc th fomuls did fo pln cuilin motion still lid. But th my b n infinit numb of nomls fo tngnt dwn to spc cu. Whn th t nd t ' unit ctos mod to sm oigin by kping thi ointtions

More information

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

NEW 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 information

ECE602 Exam 1 April 5, You must show ALL of your work for full credit.

ECE602 Exam 1 April 5, You must show ALL of your work for full credit. ECE62 Exam April 5, 27 Nam: Solution Scor: / This xam is closd-book. You must show ALL of your work for full crdit. Plas rad th qustions carfully. Plas chck your answrs carfully. Calculators may NOT b

More information

GRAVITATION 4) R. max. 2 ..(1) ...(2)

GRAVITATION 4) R. max. 2 ..(1) ...(2) GAVITATION PVIOUS AMCT QUSTIONS NGINING. A body is pojctd vtically upwads fom th sufac of th ath with a vlocity qual to half th scap vlocity. If is th adius of th ath, maximum hight attaind by th body

More information

Partial Fraction Expansion

Partial Fraction Expansion Paial Facion Expanion Whn ying o find h inv Laplac anfom o inv z anfom i i hlpfl o b abl o bak a complicad aio of wo polynomial ino fom ha a on h Laplac Tanfom o z anfom abl. W will illa h ing Laplac anfom.

More information

PARTITION HOLE DESIGN FOR MAXIMIZING OR MINIMIZING THE FUNDAMENTAL EIGENFREQUENCY OF A DOUBLE CAVITY BY TOPOLOGY OPTIMIZATION

PARTITION HOLE DESIGN FOR MAXIMIZING OR MINIMIZING THE FUNDAMENTAL EIGENFREQUENCY OF A DOUBLE CAVITY BY TOPOLOGY OPTIMIZATION ICSV4 Cns Australia 9- July, 007 PARTITION HOLE DESIGN FOR MAXIMIZING OR MINIMIZING THE FUNDAMENTAL EIGENFREQUENCY OF A DOUBLE CAVITY BY TOPOLOGY OPTIMIZATION Jin Woo L and Yoon Young Kim National Crativ

More information

ON SEMANTIC CONCEPT SIMILARITY METHODS

ON SEMANTIC CONCEPT SIMILARITY METHODS 4 ON SEMANTIC CONCEPT SIMILARITY METHODS Lu Yang*, Vinda Bhavsa* and Haold Boly** *Faculty of Comput Scinc, Univsity of Nw Bunswick Fdicton, NB, E3B 5A3, Canada **Institut fo Infomation Tchnology, National

More information

Application of Vague Soft Sets in students evaluation

Application 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 information

BEST CONSTANTS FOR UNCENTERED MAXIMAL FUNCTIONS. Loukas Grafakos and Stephen Montgomery-Smith University of Missouri, Columbia

BEST CONSTANTS FOR UNCENTERED MAXIMAL FUNCTIONS. Loukas Grafakos and Stephen Montgomery-Smith University of Missouri, Columbia BEST CONSTANTS FOR UNCENTERED MAXIMAL FUNCTIONS Loukas Gafakos and Stehen Montgomey-Smith Univesity of Missoui, Columbia Abstact. We ecisely evaluate the oeato nom of the uncenteed Hady-Littlewood maximal

More information

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

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

More information

Validation of an elastoplastic model to predict secant shear modulus of natural soils by experimental results

Validation of an elastoplastic model to predict secant shear modulus of natural soils by experimental results Validation of an lastolastic modl to dict scant sha modulus of natual soils by ximntal sults J.A.Santos & A.Goms Coia Tchnical Univsity of Lisbon, Potugal A.Modassi & F.Loz-Caballo Ecol Cntal Pais LMSS-Mat,

More information

International Journal of Mathematical Archive-5(1), 2014, Available online through ISSN

International Journal of Mathematical Archive-5(1), 2014, Available online through   ISSN ntrnational Journal of Mathmatical rchiv-51 2014 263-272 vailabl onlin through www.ijma.info SSN 2229 5046 ON -CU UZZY NEUROSOPHC SO SES. rockiarani* &. R. Sumathi* *Dpartmnt of Mathmatics Nirmala Collg

More information

Some Results on E - Cordial Graphs

Some Results on E - Cordial Graphs Intrnational Journal of Mathmatics Trnds and Tchnology Volum 7 Numbr 2 March 24 Som Rsults on E - Cordial Graphs S.Vnkatsh, Jamal Salah 2, G.Sthuraman 3 Corrsponding author, Dpartmnt of Basic Scincs, Collg

More information

Construction of asymmetric orthogonal arrays of strength three via a replacement method

Construction of asymmetric orthogonal arrays of strength three via a replacement method isid/ms/26/2 Fbruary, 26 http://www.isid.ac.in/ statmath/indx.php?modul=prprint Construction of asymmtric orthogonal arrays of strngth thr via a rplacmnt mthod Tian-fang Zhang, Qiaoling Dng and Alok Dy

More information

The angle between L and the z-axis is found from

The angle between L and the z-axis is found from Poblm 6 This is not a ifficult poblm but it is a al pain to tansf it fom pap into Mathca I won't giv it to you on th quiz, but know how to o it fo th xam Poblm 6 S Figu 6 Th magnitu of L is L an th z-componnt

More information

Physics 240: Worksheet 15 Name

Physics 240: Worksheet 15 Name Physics 40: Woksht 15 Nam Each of ths poblms inol physics in an acclatd fam of fnc Althouh you mind wants to ty to foc you to wok ths poblms insid th acclatd fnc fam (i.. th so-calld "won way" by som popl),

More information