SPLICING OF TIME OPTIMAL CONTROLS
|
|
- Jason Rudolph Wright
- 5 years ago
- Views:
Transcription
1 Dynamic Sysems and Applicaions 21 (212) SPLICING OF TIME OPTIMAL CONTROLS H. O. FATTORINI Deparmen of Mahemaics, Universiy of California Los Angeles, California , USA ABSTRACT. Two conrols u 1 () and u 2 () are spliced (in symbols (u 1 u 2 )()) if u 2 () is applied afer u 1 (); boh are defined in finie inervals. We seek condiions under which ime opimaliy of u 1, u 2 imply ime opimaliy of u 1 u 2, and eend he resuls o a finie or infinie number of conrols. The heorems (or raher eamples, since hey are resriced o he righ ranslaion semigroup in L 2 (, )) are used o consruc ime opimal conrols ha do no saisfy Ponryagin s maimum principle. AMS (MOS) Subjec Classificaion. 93E2, 93E25 1. PRELIMINARIES The sysem is (1.1) y () = Ay() + u(), y() = ζ wih conrols u( ) L (, T; E). The operaor A generaes a srongly coninuous semigroup S() in a Banach space E, called he sae space of (1.1). The soluion of (1.1) is he coninuous funcion (1.2) y() = y(, ζ, u) = S()ζ + A conrol is admissible if S( σ)u(σ)dσ. (1.3) u( ) L (,T;E) 1. The conrol is ime opimal if i drives he iniial poin ζ o a poin arge (1.4) y(t, ζ, u) = ȳ in opimal ime T, ha is, no oher admissible conrol does he drive in less ime. Under resricions on ζ, ȳ, necessary and sufficien condiions for opimaliy can be given in erms of Ponryagin s maimum principle (1.6) below. The principle requires mulipliers [4], [6] Secion 2.3 whose consrucion we ouline. When A has a bounded inverse, E 1 is he compleion of he dual E in he norm y E 1 = (A 1 ) y E. Received November 15, $15. c Dynamic Publishers, Inc.
2 17 H. O. FATTORINI The adjoin semigroup S() can be eended o an operaor S() : E 1 E 1. If S() is srongly coninuous, Z(T) E 1 consiss of all z E 1 such ha S() z E ( > ) and (1.5) z Z(T) = T S() z E d <. The norm (1.5) makes Z(T) a Banach space. All Z(T) coincide and all norms Z(T) are equivalen for T >. Z(T) is an eample of a muliplier space, a linear space Z E o which S() can be eended in such a way ha S() Z E for > and ha he semigroup equaion S(s + ) ζ = S(s) S() ζ is valid for ζ Z and s, >. When A does no have a bounded inverse, E 1 is he compleion of E in any of he equivalen norms y E 1,λ = ((λi A) 1 ) y E (λ large enough). The definiion of Z(T) (and of muliplier spaces) doesn change. An admissible conrol ū( ) L (, T; E) saisfies Ponryagin s maimum principle if (1.6) S(T ) η, ū() = ma u 1 S(T ) η, u a. e. in < T,, he dualiy of he spaces E and E, η in some muliplier space Z. We call η he muliplier and z() = S(T ) η E he cosae corresponding o (or associaed wih) he conrol ū(). We assume ha (1.6) is nonrivial, ha is, ha S(T ) z is no idenically zero in he inerval < T, alhough i may be zero in par of he inerval (where (1.6) gives no informaion on ū()). When E is a Hilber space (1.6) reduces o (1.7) ū() = S(T ) η S(T ) η (T δ < T), where (T δ, T] is he maimal inerval where S(T ) η ; if δ = T he inerval is < T. We say ha ū() is regular if i saisfies (1.6) wih η = z Z(T). Theorem 1.1. Assume ū() drives ζ E o ȳ = y(t, ζ, ū) ime opimally in he inerval T and ha (1.8) ȳ S(T)ζ D(A). Then ū() is regular. Theorem 1.2. Le ū() be a regular conrol wih (a) ȳ = y(t, ζ, ū) D(A), Aȳ < 1,or (b) ζ D(A), Aζ < 1, S(T ) z ( < T). Then ū() drives ζ E o ȳ = y(t, ζ, ū) ime opimally in he inerval T.
3 SPLICING OF TIME OPTIMAL CONTROLS 171 Theorem 1.1 is [6] Theorem I does no guaranee ha S() z in he whole inerval (see Remark 4.4). Theorem 1.2 is [6] Theorem We only use i here when ζ = (which fis ino (b), wih no assumpions on ȳ). We say ha ȳ E is reachable if here eiss an admissible conrol driving o ȳ. Theorem 1.3 (eisence of opimal conrols). Le E be a Hilber space. If ȳ is reachable hen here eiss an opimal conrol, ha is, an admissible conrol ū( ) driving o ȳ in opimal ime. Alhough sufficien for his paper, he resul is rue in spaces much more general han Hilber; see [6] Secion 3.1. The following resul is [6] Theorem and is oally independen of he maimum principle (1.6). Theorem 1.4. Le ū( ) be ime opimal. 1 Then (1.9) ū() = 1. Theorem 1.4 implies uniqueness of opimal conrols in a Hilber space. In fac, if wo conrols ū 1 () and ū 2 () drive o ȳ in opimal ime T so does ū() = (ū 1 () + ū 2 ())/2; since (1.9) is mandaory, ū 1 () = ū 2 (). The resul is valid in sricly conve spaces; see [6] Theorem We don know wheher sric conveiy is necessary for uniqueness, alhough nonuniqueness eamples in spaces no sricly conve eis (see [6], Secions 1.2 and 5.5). Theorem 1.1 says nohing abou ime opimal conrols driving ζ o ȳ no saisfying (1.8), in paricular abou conrols driving o ȳ / D(A). In fac, he main purpose of his paper is o consruc ime opimal conrols ha do no saisfy he maimum principle (1.6). For hese, y(t,, ū) / D(A). 2. SPLICING Le u 1 ( ) L (, T 1 ; E), u 2 ( ) L (, T 2 ; E). The splice u 1 u 2 of u 1 and u 2 is u 1 () ( < T 1 ) (2.1) u() = (u 1 u 2 )() = u 2 ( T 1 ) (T 1 < T 1 + T 2 ) and belongs o L (, T 1 +T 2 ; E). Splicing of n conrols u j ( ) L (, T j ; E) is defined direcly, or inducively by (2.2) u = u 1 u 2 u n = (u 1 u 2 u n 1 ) u n 1 Saemens like (1.9) should be qualified by almos everywhere. We don boher wih his.
4 172 H. O. FATTORINI and u( ) L (, T 1 + T T n ; E). The definiion eends o infinie sequences u n ( ) L (, T n ; E); n = 1, 2,... }. If u n ( ) L (,T n;e) C hen he splice ( (2.3) u() = u n )() n=1 belongs o L (, T; E), T = n=1 T n. We only use his case when T <. Obviously, he finie or infinie splice of admissible conrols is admissible. Splicing is associaive bu no commuaive. In general, splicing opimal conrols does no preserve opimaliy; for he simples one-dimensional sysem y () = u() he only ime opimal conrols in [, T] are u 1 () = 1 and u 1 () = 1 and no nonrivial splicing is opimal. One can only hope for eamples where splicing preserves opimaliy, and he resuls are only for he conrol sysem (2.4) y(, ) y(, ) = + u(, ), y(, ) = ζ(), y(, ) = (, < ). This sysem can be wrien as (1.1) in he space E = L 2 (, ) wih (2.5) Ay() = y (), domain D(A) = all y( ) L 2 (, ) wih y ( ) in L 2 (, ) and y() = }. This operaor generaes he (isomeric) righ ranslaion semigroup y( ) ( ) (2.6) S()y() = ( < ). We show below ha here eiss classes SP(T) of opimal conrols 2 such ha if u 2 ( ) SP(T 2 ) and u 1 ( ) is an arbirary opimal conrol in [, T 1 ] hen he splice (u 1 u 2 )() is opimal (Theorem 4.1). The resul is easily eended o finie splicings (Theorem 4.2). Infinie splicings are no as simple; all we can show (Theorem 5.3) is ha here eis inducively defined sequences of opimal conrols ū j ( )} (ū 1 ( ) ime opimal, u j ( ) SP(T j ) for j = 2, 3,...) whose splice is ime opimal. Since he resuls are resriced o he sysem (2.4) splicing seems lile more han a curiosiy. However, i can be used o produce ime opimal conrols no saisfying Ponryagin s maimum principle (1.6). The resuls are generalizaions of he resuls in [5] and [6] Secion 2.7 (where splicing was used in paricular cases bu no eplicily defined) and we are able o produce ime opimal conrols rougher han he ones herein. 2 Each conrol u() is defined in is own inerval [, T], possibly differen for differen conrols. Tha u() is opimal in [, T] means i drives ime opimally o he arge ȳ = y(t,, ū), ha is, he arge is no fied beforehand. Opimaliy has he same meaning: no oher admissible conrol u( ) can drive o y(t,, ū) in less ime. Someimes we abbreviae opimal in [, T] o simply opimal.
5 SPLICING OF TIME OPTIMAL CONTROLS 173 Splicing (alhough no of opimal conrols) is known in conrol heory; i has been especially used in conrollabiliy of sysems in Euclidean spaces and Lie groups. For references see [6], Secion THE RIGHT TRANSLATION SEMIGROUP The adjoin of (2.6) is he lef ranslaion (and chop-off) semigroup (3.1) S() y( + ) ( ) y() = ( < ). We have (3.2) S() S() = I, S()S() y() = χ ()y(), χ () he characerisic funcion of [, ). Formula (1.2) for he conrol u()() = u(, ) is (3.3) y(,, ζ, u) = y(, ζ, u)() = = ζ( ) + ( ) S()ζ + S( σ)u(σ)dσ () u(σ, ( σ))dσ, hus he conribuion of he conrol u(σ, ) o y(,, ζ, u) is he inegral of u(σ, ) over he inersecion of he posiive quadran, wih he line (σ, ( σ)) joining (, ) wih (, ) as shown in Figure 1. The space Z of all mulipliers consiss of all measurable z() defined in > and such ha κ(, z) = S() z( ) = z( + ) 2 d = z() 2 d <, for >, while Z(T) consiss of all z( ) Z saisfying he inegrabiliy condiion (1.5), T S(σ) z( ) dσ = T κ(σ, z)dσ <. Since we are in a Hilber space, (1.7) applies, and any conrol ha saisfies (1.6) is given by (3.4) ū(, ) = S(T ) z() S(T ) z( ) z( + (T )) = χ () κ(t, z) (T δ < T),
6 174 H. O. FATTORINI Figure 1. Inegraion lines in formula (3.3). T T s(ȳ) R s(ȳ) K T R s(ȳ) K Figure 2. Opimal ime and opimal conrol when s(ȳ) <. where (T δ, T] is he maimal inerval where S(T ) z ; if δ = T, he inerval in (3.4) is < T. Using he second equaliy (3.2) (3.5) S(T σ)ū(σ, ) = S(T σ)s(t σ) z() S(T σ) z( ) = χ T σ()z() κ(t σ, z) (T δ < T). Consequenly, if κ(t σ) in < σ T, y(t,,, u) is he inegral in σ T of he righ side of (3.5). This leads o a simple eplici formula for y(t,,, u) in erms of z() ([6] formula (2.6.25)) which we don need o use here. Le ϕ() be measurable in >. Define s(ϕ( )) as he minimum s such ha suppor ϕ( ) [, s] (suppor defined modulo null ses). If he suppor of ϕ( ) is no conained in any inerval [, s] we se s(ϕ( )) =. Lemma 3.1. Assume ha ȳ( ) L 2 (, ) is reachable and s(ȳ( )) <. Then (a) if T is he opimal driving ime from o ȳ() we have T s(ȳ), (b) if ū(, ) is he opimal conrol doing he drive, he suppor of ū(, ) is conained in he region R in Figure 2 righ.
7 SPLICING OF TIME OPTIMAL CONTROLS 175 Proof. Assume T > s(ȳ) so ha we have he configuraion in Figure 2 lef. If he ime opimal conrol ū(, ) is no zero in K we may modify is definiion o ū(, ) = here. This doesn affec he arge and, if anyhing, improves each norm ū(, ) L 2 (, ). The modified conrol is admissible, hus ime opimal; by uniqueness i is equal o ū(, ). If T > s(ȳ) hen ū(, ) L 2 (, ) = in T s(ȳ). However, Theorem 1.4 says ha a ime opimal conrol mus saisfy u() = 1, hus we have a conradicion. (b) If he opimal conrol ū(, ) is no zero in K we modify is definiion o ū(, ) = here and argue as in (a). Lemma 3.2. Assume ȳ() is reachable wih a conrol of he form (3.4). Then (3.6) s(z( )) = s(ȳ( )). Proof. Equaliy (3.6) follows from he far more precise saemen (3.7) z() = ȳ() =. To see ha (3.7) holds we look a formula (3.5). The arge ȳ() is obained inegraing in σ T he funcion on he righ side, hus z() = ȳ() =. On he oher hand, he funcion χ T σ () (as a funcion of ) is nonzero for T σ hus ȳ() = z() = and we are done. Lemma 3.1 and Lemma 3.2 have oally differen scopes. In Lemma 3.1 ȳ() is jus reachable by an admissible conrol (hus by an opimal conrol in view of Theorem 1.3). In Lemma 3.2, ȳ() is reachable by a conrol of he form (3.4), his conrol being auomaically opimal by Theorem 1.2. The aim of his paper is o produce opimal conrols no of he form (3.4). 4. FINITE SPLICING A conrol u(, ) in L (, T; L 2 (, )) belongs o he class SP(T) if and only if i is admissible and drives in opimal ime T o a arge ȳ() wih s(ȳ( )) = T. Eamples of conrols in SP(T) are easy o produce wih he help of Theorem 1.2 and (3.4): if z( ) Z(T) wih s(z( )) = T hen he conrol ū(, ) in (3.4) drives o a arge ȳ() = y(t,,, ū) in opimal ime T and hus is in SP(T). Since Z(T) L 2 (, ) we may ake z( ) L 2 (, ) for he purposes of his paper. Any conrol in SP(T) mus be zero in he region K in Figure 3; if no, we can modify is definiion o ū(, ) = here and argue as in he proof of Lemma 3.1 The condiion s(z( )) = s(ȳ( )) = T alone does no guaranee ha T is he opimal ime o reach ȳ( ); if s(z( )) = T and T < T he conrol ū(, ) = S(T ) z() S(T ) z( ) = χ () z( + (T )) κ(t, z) drives o a arge ȳ( ) wih s(ȳ( )) = T in ime T < T. ( < T )
8 176 H. O. FATTORINI T s(ȳ) = T K Figure 3. Conrols in he class SP(T). T 2 ȳ 2 () T 2 ȳ 2 () T 2 ȳ 1 ( T 2 ) T 1 + T 2 R ū 2 ( T 1, ) K R ū 2 (, ) K T 1 ȳ 1 () ū 1 (, ) Figure 4. Splicing of ū 1 (, ) and ū 2 (, ). Theorem 4.1. Le he admissible conrol ū 1 (, ) L (, T 1 ; L 2 (, )) be opimal in [, T 1 ] and le u 2 (, ) SP(T 2 ). Then he splice (u 1 u 2 )(, ) L (, T 1 + T 2 ; L 2 (, )) is opimal in [, T 1 + T 2 ]. Proof. ū 2 (, ) is zero in he complemen K of he riangle R in Figure 4 lef, hus he splice ū(, ) = (ū 1 ū 2 )(, ) is zero in he corresponding region K of Figure 4 righ. If ū 2 (, ) drives o he arge ȳ 2 () in ime T 2 and ū 1 (, ) drives o he arge ȳ 1 () in ime T 1, formula (3.3) shows ha ū(, ) drives o he arge ȳ 2 () ( T 2 ) (4.1) ȳ() = ȳ 1 ( T 2 ) (T 2 < ) in ime T = T 1 + T 2. I remains o show ha his drive is opimal. Since ū(, ) is admissible he arge (4.1) is reachable and Theorem 1.3 says ha a ime opimal conrol ũ(, ) eiss. Le T be he opimal driving ime, and assume firs ha T < T 2. The conrol ũ(, ) (, ) u(, ) = R (, ) K
9 SPLICING OF TIME OPTIMAL CONTROLS 177 ȳ 2 () T 2 ȳ 1 ( T 2 ) T 1 + T 2 T ȳ 2 () T 2 R K R K T 1 δ Figure 5. Time opimaliy of he splice. ( R, K he wo regions in Figure 5 lef) is admissible and drives o ȳ2 () in ime T < T 2, which conradics he opimaliy of ū 2 (, ). Accordingly, T T2. If T < T 1 + T 2, le δ = T 1 + T 2 T. The admissible conrol does he drive The conrol u δ (, ) = ũ( δ, ) (δ T 1 + T 2 ) y(δ,,, u δ ) =, y(t 1 + T 2,,, u δ ) = ȳ(). v(, ) = u δ (, ) (, ) R (, ) K (T 1 T 1 + T 2 ) (R, K he regions in Figure 5 righ) is admissible and does he drive y(t 1,,, v) =, y(t 1 + T 2,,, v) = ȳ 2 () while ū 2 ( T 1, ) does he same drive opimally; i follows ha v(, ) is also opimal and, by uniqueness of opimal conrols, 3 (4.2) v(, ) = u δ (, ) = ū 2 ( T 1, ) (T 1 T 1 + T 2 ) which shows ha u δ (, ) = in K. By Formula (3.3) (Figure 1) we mus have (4.3) y(t 1,,, u δ ) = ȳ 1 (). Accordingly, u δ ( + δ, ) = ũ(, ) drives o ȳ 1 () in ime T 1 δ, which conradics he opimaliy of ū 1 (, ). Theorem 4.2. Le ū 1 (, ) L (, T 1 ; L 2 (, )) be opimal in [, T 1 ] and le ū j (, ) SP(T j ), j = 2,..., n. Then he splice v n (, ) = (ū 1 ū 2 ū n )(, ) L (, T 1 + T T n ; L 2 (, )) is opimal in [, T 1 + T T n ]. 3 Time opimaliy can be defined for an arbirary inerval [a, b]. Resuls are he same.
10 178 H. O. FATTORINI Proof. Theorem 4.1 and inducion: use formula (2.2). Remark 4.3. We can figure ou he arge hi by v n (, ) arguing as in Theorem 4.1. Le ȳ j () = y(t j,,, ū j ) be he arge hi by he conrol ū j (, ) in opimal ime T j, and define S j = T T j (j = 1,...n 1), T = T 1 + T T n. Then (4.4) y(t,,, v n ) ȳ 1 ( (T S 1 )) (T S 1 < ) = ȳ j ( (T S j )) (T S j < T S j 1, j = 2,...,n 1) ȳ n () ( < T n ). This formula reads from righ o lef as j increases. We can pu i in able form: Inerval Targe ȳ() [, T n ) ȳ n () [T n, T n + T n 1 ) ȳ n 1 ( T n ) [T n + T n 1, T n + T n 1 + T n 2 ) ȳ n 2 ( T n T n 1 )..... T n + + T 3, T n + + T 2 ) ȳ 2 ( T n T 3 ) [T n + + T 2, ) ȳ 1 ( T n T 2 ) Remark 4.4. The finie splices of opimal conrols in Theorem 4.2 have a seemingly conflicual relaionship wih Theorem 1.1. Assume he opimal conrols ū j (, ) in he splice are produced from formula (3.4) and le z j () be he muliplier for each conrol. I is proved in [6] Secion 2.6 ha z j () can be chosen in such a way ha ȳ j () = (T j,,, ū j ) is coninuously differeniable in [, T j ] wih ȳ j () = ȳ j() = ȳ j (T j ) = = ȳ j (T j) =. In view of he definiion (2.5) of he infiniesimal generaor A and of formula (4.4) he arge ȳ(t,,, v n ) belongs o D(A). In fac, he differen pieces of he arge are smooh and mach (ogeher wih heir derivaives) a he divisory poins of (4.4) and he arge is zero for =. Theorem 1.1 applies and v(, ) saisfies he maimum principle (1.6) in is Hilber space version (1.7), which seems o clash wih he disconinuous naure of v n (, ). The eplanaion lies in he fac ha Theorem 1.1 does no guaranee ha he cosae z() = S(T ) z in (1.6) is nonzero in he enire conrol inerval [, T], jus in an inerval (T δ, T]. The muliplier provided by Theorem 1.1 for he conrol v(, ) is he muliplier z n ( ) (eended = for T n ) for he las piece ū n (, ) of he splice v n (, ), and he cosae z() = S(T ) z n vanishes ouside of he inerval (T T n, T]. In fac, he conrol v n (, ) swiches cosaes every ime crosses one of he divisory poins S j = T T j in he inerval [, T]. For more deails on his see [6] Secion 2.7.
11 SPLICING OF TIME OPTIMAL CONTROLS INFINITE SPLICING If y E = sae space of (1.1) we denoe by T (y) he opimal driving ime from o y. If y is reachable and E is a Hilber space, Theorem 1.3 says ha T (y) eiss and is finie. If y is no reachable, ha is, if canno be driven o y by any admissible conrol in any ime we define T (y) =. The firs resul below is in [4], [6] Lemma 2.7.3; he second resul is specific o he sysem (2.4). Lemma 5.1. Le E be a Hilber space and le y n } E be a sequence wih y n y E. Then (5.1) T (y) lim inf n T (y n). Lemma 5.2. Assume y 1 () y 2 (). Then (5.2) T (y 1 ( )) T (y 2 ( )). Proof. We may assume ha T (y 2 ( )) <. If ū 2 (, ) is he conrol driving o y 2 () opimally we define a new conrol u 1 (, ) muliplying ū 2 (, ) by he quoien y 1 ()/y 2 () over each inegraion line (σ, (T σ)) in Formula (3.3) (Figure 1); precisely u 1 (σ, (T σ)) = φ()ū 2 (σ, (T σ)) ( <, σ T, + (T σ) ) where φ() = if y 2 () =, φ() = y 1 ()/y 2 () if y 2 (). We have φ() 1, hus u 1 (σ, ) ū 2 (σ, ) and i follows ha u 1 (σ, ) is admissible. Formula (3.3) shows ha y(t,,, u 1 ) = y 1 (), so ha y 1 () is reachable in ime T = T (y 2 ( )). The opimal driving ime is T, hus inequaliy (5.2) holds and we are done. The infinie sequence o be spliced is ū n (, )}, where he firs conrol ū 1 (, ) L (, T 1 ; L 2 (, )) is ime opimal in [, T 1 ] and u n (, ) SP(T n ) (n = 2, 3,...). The sequence is far from arbirary; in fac i will be consruced inducively, each ū n (, ) (or, raher, is suppor) depending on he choice of he preceding erms ū 1 (, ),...,ū n 1 (, ). The procedure implies T = n=1 T n <, hus he splice is defined in a finie inerval [, T]. The primary objecs are no he T n bu wo sequences S n ; n =, 1, 2,... } and S n ; n =, 1, 2,... } such ha (5.3) < S < S 1 < S 2 <... S > S 1 > S 2 >... S n < S n (n =, 1, 2,...). In addiion, he sequences S n } and S n } saisfy (5.4) S n+1 S n α n, S n S n α n (n =, 1, 2,...),
12 18 H. O. FATTORINI S n+1 y(τ,,, w n ) y(s n,,, v n ) S n S n 1 Figure 6. Choice of S n+1 from v n (, ). where he summable posiive series α n ; n =, 1,... } is given in advance and oally arbirary. The T n are obained from he S n by (5.5) T n = S n S n 1 (n = 1, 2,...), hence (5.6) T = T n = (S n S n 1 ) n=1 n=1 α n 1 = α n = α. n=1 n= The sequences begin wih S = and S > saisfying he second condiion (5.4) for n =, ha is, S S α. For he inducive sep, we assume ha he S j, he S j and he ū j (, ) have been consruced for j n. Define v n (, ) as he finie splice (5.7) v n (, ) = (ū 1 ū 2 ū n )(, ). By Theorem 4.2 i drives in opimal ime S n o he arge y(s n,,, v n ). If we define (5.8) w n (, ) = v n (, ) ( S n ) (S n < ) we have (Figure 6) (5.9) y(τ,,, w n ) = ( < τ S n ) y(s n, (τ S n )),, v n ) (τ S n ) for τ > S n, so ha y(τ,,, w n ) y(s n,,, v n ) L 2 (, ) as τ S n. Accordingly, Lemma 5.1 can be applied and we can selec S n+1 > S n wih (5.1) T (y(τ,,, w n )) T (y(s n,,, v n )) 1 n (S n τ S n+1 ).
13 SPLICING OF TIME OPTIMAL CONTROLS 181 In fac, if his choice is no possible here eiss a sequence τ k }, τ k S n such ha T (y(s n,,, v n )) lim inf k T (y(τ k,,, w n )) + 1 n conradicing (5.1). Since T (y(s n,,, v n )) = S n, (5.1) becomes (5.11) T (y(τ,,, w n )) S n 1 n (S n τ S n+1 ). Moving S n+1 o he lef if necessary we may assume ha (5.12) S n+1 S n α n+1 and hen selec S n+1 wih (5.13) S n < S n+1 < S n+1 which, in view of (5.12) gives he second condiion (5.4). The conrol ū n+1 (, ) added a his sep o he splice is an arbirary conrol in SP(T n+1 ), where T n+1 = S n+1 S n. This conrol eiss, since formula (3.4) applied o z( ) wih s(z( )) = T (T arbirary) produces a conrol in SP(T). The sequences S n } and S n } consruced by repeaed applicaion of his inducive sep saisfy he hree condiions (5.3) and he wo condiions (5.4). We hen define and splice he chosen sequence ū n (, ), T = sup S n = lim S n = lim S n+1 = inf n n n n Sn+1 ū = n=1 obaining an admissible conrol ū(, ) L (, T; L 2 (, )). This conrol drives o he arge ū n (5.14) ȳ() = y(t,,, ū) ȳ 1 ( (T S 1 )) (T S 1 < ) = ȳ j ( (T S j )) (T S j < T S j 1, j = 2, 3,...) where ȳ j () = y(t j,,, ū j ) has suppor in [, T j ] for j 2; he suppor of ȳ 1 () is unresriced. (This formula is he generalizaion of (4.4) o infinie splices.) Consider now a second splice where each ū j (, ) (j n + 1) is replaced by ξ j (, ) = in he same inerval [, T j ], ( n ) ( w n = ū n j=1 j=n+1 ξ j ). This conrol is he same defined in (5.8). I drives o a arge y(t,,, w n ) which can be described by (5.14) wih he only difference ha ȳ j () = for j n+1;
14 182 H. O. FATTORINI precisely (5.15) ȳ() = y(t,,, ū) ȳ 1 ( (T S 1 )) (T S 1 ) = ȳ j ( (T S j )) (T S j < T S j 1, j = 2, 3,..., n) ( < T S n ) which can be wrien in he form (5.16) y(t,,, w n ) = χ()y(t,,, ū) where χ() is he characerisic funcion of he inerval [, T S n ]. I follows from (5.16) ha y(t,,, w n ) y(t,,, ū) hence, using Lemma 5.2 in he firs inequaliy and aking (5.11) ino accoun in he second, (5.17) T (ȳ( )) T (y(t,,, w n )) S n 1 n T as n. Taking limis, we deduce ha T (ȳ( )) T. Since ū(, ) drives o ȳ() in ime T, i follows ha T (ȳ( )) = T and ha ū(, ) is opimal. We have proved Theorem 5.3. The infinie splice (2.3) of he conrols ū n (, ); n = 1, 2,... } is ime opimal. Remark 5.4. The funcion T (y) is a version of he value funcion used in he Hamilon-Jacobi approach o opimal conrol, alhough he usual value funcion is defined as he ime needed o drive a arge y E o (see [1], [2], [3]). Lemma 5.1 is relaed o eising resuls on smoohness of he value funcion. 6. APPLICATIONS: STRONGLY SINGULAR TIME OPTIMAL CONTROLS A conrol is called singular if does no saisfy he maimum principle (1.6) wih any muliplier z Z(T). If a singular conrol saisfies (1.6) wih a muliplier η Z i is called weakly singular; if i does no saisfy (1.6) wih any muliplier η, i is called srongly singular. The conrol ū(, ) consruced in Theorem 5.3 using conrols ū n (, ) SP(T n ) of he form (3.4) as building blocks is srongly singular, ha is, i does no saisfy he maimum principle (1.6) wih any muliplier η. In fac, if i did, i would have iself he form (3.4) wih z( ) Z = space of all mulipliers (Secion 3) in some inerval [T δ, T]. This is impossible; conrols of he form (3.4) are eiher = or on lines + (T ) = c, a qualiy ha ū(, ) conspicuously lacks. However,
15 SPLICING OF TIME OPTIMAL CONTROLS 183 ū(, ) is ime opimal in any subinerval 4 [, T ], T < T and is regular in each of hese subinervals. This is he class of conrols consruced in [5] [6] Theorem We can apply he same idea o consruc opimal conrols ha are more singular han he ones in [5], [6]. We prove firs an addendum o Theorem 5.3 having o do wih he assumpions on ū 1 (, ). In Theorem 5.3 ū 1 (, ) is jus assumed o be an opimal conrol in [, T 1 ] (he oher conrols ū n (, ) are in SP(T n )). We assume now ha u 1 (, ) belongs o he class SP(T 1 ) as well. Theorem 6.1. Assume ha all conrols ū n (, ); n = 1, 2,... } in Theorem 5.3 belong o SP(T n ). Then he infinie splice ū(, ) belongs o SP(T). Proof. We know from Theorem 5.3 ha ū(, ) drives in opimal ime T o a arge ȳ() described by formula (5.14); all we have o show is ha (6.1) s(ȳ( )) = T. By he assumpion on ū 1 (, ) we have s(ȳ 1 ( )) = s(y(t 1,,, ū 1 )) = T 1, in paricular, suppor ȳ 1 ( ) [, T 1 ]. This means he suppor of y 1 ( (T S 1 )) in he firs line of (5.14) is conained in [T S 1, T] = [T T 1, T], so ha suppor ȳ( ) [, T]. If suppor ȳ( ) [, T ǫ] for ǫ > we reverse his implicaion and deduce ha s(ȳ 1 ( ))) T ǫ, a conradicion. We call SP (T) SP(T) he se of all conrols of he form (3.4) wih s(z( )) = T. The se SP 1 (T) SP(T) consiss of all infinie splices produced under he auspices of Theorem 6.1 wih building blocks ū n (, ) SP (T n ). Lemma 6.2. SP 1 (T) for all T >. Proof. A resul like his is needed because he opimal ime T in Theorems 5.3 and 6.1 is no chosen in advance; i is a byproduc of he heorem, precisely, i depends on he choice of he S n. Given T > arbirary we consruc firs a conrol v 1 (, ) SP 1 (T ) for some T T. This is possible since he series α n } and is sum α in (5.6) are compleely arbirary; we may ake α = T. If T = T we are done. Oherwise, we ake a conrol v (, ) SP (T) wih opimal ime T T and define ū = v v 1, ha is, we add he building block v a he beginning of he splice. By Theorem 6.1 he conrol ū belongs o SP 1 ((T T ) + T ) = SP 1 (T). 4 The opimaliy principle says ha if ū( ) is ime opimal in [, T] hen i is ime opimal in any subinerval [a, b] [, T]. The proof is immediae; if we can improve he driving ime in [a, b] hen (via a ime ranslaion) we can improve he driving ime in [, T]. The ime ranslaion works because he sysem (1.1) does no depend eplicily on ime.
16 184 H. O. FATTORINI Theorem 6.3. The conrols ū n (, ) making up he infinie splice in Theorem 6.1 can be aken in SP 1 (T n ). Proof. We go over he proof of Theorem 5.3 as modified in Theorem 6.1, especially over he inducive choice of ū n+1 (, ) in he paragraph following (5.11). The only qualificaion on ū n+1 (, ) is an arbirary conrol in SP(T n+1 ) wih T n+1 = S n+1 S n where S n+1 has been chosen on he basis of (5.11). By Lemma 6.2 we can selec ū(, ) in SP 1 (T n+1 ) for arbirary T n+1. The res of he proof of Theorem 5.3 remains he same. The se of all splices produced by Theorem 6.1 wih building blocks ū n (, ) SP 1 (T n ) is SP 2 (T) SP(T). Conrols in his class are srongly singular no only in he whole inerval [, T] bu in each subinerval [, S n, ] S n } he sequence in Theorem 5.3 wih S n T. Eploiing he same idea we prove firs ha SP 2 (T) for all T > and hen use Theorem 6.1 o consruc conrols whose building blocks are in SP 2 (T n ). This is he class SP 3 (T); he inervals where he conrols are srongly singular are [, S mn ] where S mn S n as m and S n T. The classes SP n (T) are inducively defined in a similar way for all n and conain opimal conrols which are srongly singular in more and more subinervals of [, T]. A ime opimal conrol ū( ) for (1.1) is called hypersingular in [, T] if i is srongly singular in any inerval [a, b] [, T] (for an eample, see [7]). Obviously, he conrols in any class SP n (T) fall shor of hypersingular. To produce a hypersingular conrol aking ū n (, ) SP n (T) and hen aking limis as n won work since he conrols in he sequence would have suppor in a shrinking band T, ǫ n. We don know if he consrucion in his paper can be modified o give hypersingular conrols, in fac we don know if hypersingular conrols for (2.4) eis a all. The oy conrol sysem (2.4) (one of he simples involving parial differenial equaions) is he carrier of a number of ineresing conrol heory eamples and counereamples; for informaion on his see [6], [9], [1]. For a recen survey on regular, singular and srongly singular conrols for he sysem (1.1) and relaed opics see [1]. REFERENCES [1] P. Cannarsa and O. Cǎrjâ, On he Bellman equaion for he minimum ime problem in infinie dimensions, SIAM J. Conrol & Opimizaion, 43: , 24. [2] O. Cǎrjâ, On he minimum ime funcion and he minimum energy problem; a nonlinear case. Sysems & Conrol Leers, 55: , 26. [3] O. Cǎrjâ and A. Lazu, On he minimal ime null conrollabiliy of he hea equaion. Discree Conin. Dyn. Sys, Proc. 7h AIMS Conference on Dynamical Sysems, Differenial Equaions and Applicaions, , 29.
17 SPLICING OF TIME OPTIMAL CONTROLS 185 [4] H. O. Faorini, Eisence of singular eremals and singular funcionals in reachable spaces, Jour. Evoluion Equaions, 1: , 21. [5] H. O. Faorini, Vanishing of he cosae in Ponryagin s maimum principle and singular ime opimal conrols, Jour. Evoluion Equaions, 4:99 123, 24. [6] H. O. Faorini, Infinie Dimensional Linear Conrol Sysems, Norh-Holland Mahemaical Sudies 21, Elsevier, Amserdam 25. [7] H. O. Faorini, Linear conrol sysems in sequence spaces, Funcional Analysis and Evoluion Equaions. The Güner Lumer Volume , 27. [8] H. O. Faorini, Time and norm opimaliy of weakly singular conrols, Progress in Nonlinear Differenial Equaions and Their Applicaions 8: Springer Basel AG [9] H. O. Faorini, Srongly regular ime and norm opimal conrols, o appear in Dynamics of Coninuous, Discree and Impulsive Sysems Series B: Applicaions and Algorihms 18: , 211. [1] H. O. Faorini, Time and norm opimal conrols: a survey of recen resuls and open problems, Aca Mahemaica Scienia 31B: , 211.
4 Sequences of measurable functions
4 Sequences of measurable funcions 1. Le (Ω, A, µ) be a measure space (complee, afer a possible applicaion of he compleion heorem). In his chaper we invesigae relaions beween various (nonequivalen) convergences
More informationThe Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales
Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions
More informationHamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation:
M ah 5 7 Fall 9 L ecure O c. 4, 9 ) Hamilon- J acobi Equaion: Weak S oluion We coninue he sudy of he Hamilon-Jacobi equaion: We have shown ha u + H D u) = R n, ) ; u = g R n { = }. ). In general we canno
More informationLecture Notes 2. The Hilbert Space Approach to Time Series
Time Series Seven N. Durlauf Universiy of Wisconsin. Basic ideas Lecure Noes. The Hilber Space Approach o Time Series The Hilber space framework provides a very powerful language for discussing he relaionship
More informationMath 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:
Mah 4 Eam Review Problems Problem. Calculae he 3rd Taylor polynomial for arcsin a =. Soluion. Le f() = arcsin. For his problem, we use he formula f() + f () + f ()! + f () 3! for he 3rd Taylor polynomial
More informationSection 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients
Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous
More informationConvergence of the Neumann series in higher norms
Convergence of he Neumann series in higher norms Charles L. Epsein Deparmen of Mahemaics, Universiy of Pennsylvania Version 1.0 Augus 1, 003 Absrac Naural condiions on an operaor A are given so ha he Neumann
More informationt dt t SCLP Bellman (1953) CLP (Dantzig, Tyndall, Grinold, Perold, Anstreicher 60's-80's) Anderson (1978) SCLP
Coninuous Linear Programming. Separaed Coninuous Linear Programming Bellman (1953) max c () u() d H () u () + Gsusds (,) () a () u (), < < CLP (Danzig, yndall, Grinold, Perold, Ansreicher 6's-8's) Anderson
More informationFinish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!
MAT 257, Handou 6: Ocober 7-2, 20. I. Assignmen. Finish reading Chaper 2 of Spiva, rereading earlier secions as necessary. handou and fill in some missing deails! II. Higher derivaives. Also, read his
More informationAn Introduction to Malliavin calculus and its applications
An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214
More information( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is
UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires
More informationAn Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance.
1 An Inroducion o Backward Sochasic Differenial Equaions (BSDEs) PIMS Summer School 2016 in Mahemaical Finance June 25, 2016 Chrisoph Frei cfrei@ualbera.ca This inroducion is based on Touzi [14], Bouchard
More informationt is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...
Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger
More informationSolutions from Chapter 9.1 and 9.2
Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is
More informationLecture 20: Riccati Equations and Least Squares Feedback Control
34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he
More informationHamilton Jacobi equations
Hamilon Jacobi equaions Inoducion o PDE The rigorous suff from Evans, mosly. We discuss firs u + H( u = 0, (1 where H(p is convex, and superlinear a infiniy, H(p lim p p = + This by comes by inegraion
More informationOn Gronwall s Type Integral Inequalities with Singular Kernels
Filoma 31:4 (217), 141 149 DOI 1.2298/FIL17441A Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Gronwall s Type Inegral Inequaliies
More informationDISCRETE GRONWALL LEMMA AND APPLICATIONS
DISCRETE GRONWALL LEMMA AND APPLICATIONS JOHN M. HOLTE MAA NORTH CENTRAL SECTION MEETING AT UND 24 OCTOBER 29 Gronwall s lemma saes an inequaliy ha is useful in he heory of differenial equaions. Here is
More informationChapter 2. First Order Scalar Equations
Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.
More informationOn Oscillation of a Generalized Logistic Equation with Several Delays
Journal of Mahemaical Analysis and Applicaions 253, 389 45 (21) doi:1.16/jmaa.2.714, available online a hp://www.idealibrary.com on On Oscillaion of a Generalized Logisic Equaion wih Several Delays Leonid
More informationOscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson
PROCEEDINGS OF THE FOURTH INTERNATIONAL CONFERENCE ON DYNAMICAL SYSTEMS AND DIFFERENTIAL EQUATIONS May 4 7, 00, Wilmingon, NC, USA pp 0 Oscillaion of an Euler Cauchy Dynamic Equaion S Huff, G Olumolode,
More information3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon
3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of
More informationAnn. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:
Ann. Func. Anal. 2 2011, no. 2, 34 41 A nnals of F uncional A nalysis ISSN: 2008-8752 elecronic URL: www.emis.de/journals/afa/ CLASSIFICAION OF POSIIVE SOLUIONS OF NONLINEAR SYSEMS OF VOLERRA INEGRAL EQUAIONS
More informationProperties Of Solutions To A Generalized Liénard Equation With Forcing Term
Applied Mahemaics E-Noes, 8(28), 4-44 c ISSN 67-25 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Properies Of Soluions To A Generalized Liénard Equaion Wih Forcing Term Allan Kroopnick
More informationOptimality Conditions for Unconstrained Problems
62 CHAPTER 6 Opimaliy Condiions for Unconsrained Problems 1 Unconsrained Opimizaion 11 Exisence Consider he problem of minimizing he funcion f : R n R where f is coninuous on all of R n : P min f(x) x
More informationEXERCISES FOR SECTION 1.5
1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler
More informationOptimizing heat exchangers
Opimizing hea echangers Jean-Luc Thiffeaul Deparmen of Mahemaics, Universiy of Wisconsin Madison, 48 Lincoln Dr., Madison, WI 5376, USA wih: Florence Marcoe, Charles R. Doering, William R. Young (Daed:
More informationFEEDBACK NULL CONTROLLABILITY OF THE SEMILINEAR HEAT EQUATION
Differenial and Inegral Equaions Volume 5, Number, January 2002, Pages 5 28 FEEDBACK NULL CONTROLLABILITY OF THE SEMILINEAR HEAT EQUATION Mihai Sîrbu Deparmen of Mahemaical Sciences, Carnegie Mellon Universiy
More informationContinuous Time. Time-Domain System Analysis. Impulse Response. Impulse Response. Impulse Response. Impulse Response. ( t) + b 0.
Time-Domain Sysem Analysis Coninuous Time. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 1. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 2 Le a sysem be described by a 2 y ( ) + a 1
More informationSome Ramsey results for the n-cube
Some Ramsey resuls for he n-cube Ron Graham Universiy of California, San Diego Jozsef Solymosi Universiy of Briish Columbia, Vancouver, Canada Absrac In his noe we esablish a Ramsey-ype resul for cerain
More informationMatrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality
Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]
More informationThis document was generated at 1:04 PM, 09/10/13 Copyright 2013 Richard T. Woodward. 4. End points and transversality conditions AGEC
his documen was generaed a 1:4 PM, 9/1/13 Copyrigh 213 Richard. Woodward 4. End poins and ransversaliy condiions AGEC 637-213 F z d Recall from Lecure 3 ha a ypical opimal conrol problem is o maimize (,,
More informationAn introduction to the theory of SDDP algorithm
An inroducion o he heory of SDDP algorihm V. Leclère (ENPC) Augus 1, 2014 V. Leclère Inroducion o SDDP Augus 1, 2014 1 / 21 Inroducion Large scale sochasic problem are hard o solve. Two ways of aacking
More information2. Nonlinear Conservation Law Equations
. Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear
More informationMATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence
MATH 433/533, Fourier Analysis Secion 6, Proof of Fourier s Theorem for Poinwise Convergence Firs, some commens abou inegraing periodic funcions. If g is a periodic funcion, g(x + ) g(x) for all real x,
More informationPredator - Prey Model Trajectories and the nonlinear conservation law
Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories
More information23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes
Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion
More informationAsymptotic instability of nonlinear differential equations
Elecronic Journal of Differenial Equaions, Vol. 1997(1997), No. 16, pp. 1 7. ISSN: 172-6691. URL: hp://ejde.mah.sw.edu or hp://ejde.mah.un.edu fp (login: fp) 147.26.13.11 or 129.12.3.113 Asympoic insabiliy
More informationPositive continuous solution of a quadratic integral equation of fractional orders
Mah. Sci. Le., No., 9-7 (3) 9 Mahemaical Sciences Leers An Inernaional Journal @ 3 NSP Naural Sciences Publishing Cor. Posiive coninuous soluion of a quadraic inegral equaion of fracional orders A. M.
More informationû s L u t 0 s a ; i.e., û s 0
Te Hille-Yosida Teorem We ave seen a wen e absrac IVP is uniquely solvable en e soluion operaor defines a semigroup of bounded operaors. We ave no ye discussed e condiions under wic e IVP is uniquely solvable.
More informationPOSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION
Novi Sad J. Mah. Vol. 32, No. 2, 2002, 95-108 95 POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION Hajnalka Péics 1, János Karsai 2 Absrac. We consider he scalar nonauonomous neural delay differenial
More informationExistence of positive solution for a third-order three-point BVP with sign-changing Green s function
Elecronic Journal of Qualiaive Theory of Differenial Equaions 13, No. 3, 1-11; hp://www.mah.u-szeged.hu/ejqde/ Exisence of posiive soluion for a hird-order hree-poin BVP wih sign-changing Green s funcion
More informationSMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15.
SMT Calculus Tes Soluions February 5,. Le f() = and le g() =. Compue f ()g (). Answer: 5 Soluion: We noe ha f () = and g () = 6. Then f ()g () =. Plugging in = we ge f ()g () = 6 = 3 5 = 5.. There is a
More informationarxiv:math/ v1 [math.nt] 3 Nov 2005
arxiv:mah/0511092v1 [mah.nt] 3 Nov 2005 A NOTE ON S AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION D. A. GOLDSTON AND S. M. GONEK Absrac. Le πs denoe he argumen of he Riemann zea-funcion a he poin 1 + i. Assuming
More informationCorrespondence should be addressed to Nguyen Buong,
Hindawi Publishing Corporaion Fixed Poin Theory and Applicaions Volume 011, Aricle ID 76859, 10 pages doi:101155/011/76859 Research Aricle An Implici Ieraion Mehod for Variaional Inequaliies over he Se
More informationTwo Coupled Oscillators / Normal Modes
Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own
More informationarxiv: v1 [math.ca] 15 Nov 2016
arxiv:6.599v [mah.ca] 5 Nov 26 Counerexamples on Jumarie s hree basic fracional calculus formulae for non-differeniable coninuous funcions Cheng-shi Liu Deparmen of Mahemaics Norheas Peroleum Universiy
More informationChallenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k
Challenge Problems DIS 03 and 0 March 6, 05 Choose one of he following problems, and work on i in your group. Your goal is o convince me ha your answer is correc. Even if your answer isn compleely correc,
More information4.6 One Dimensional Kinematics and Integration
4.6 One Dimensional Kinemaics and Inegraion When he acceleraion a( of an objec is a non-consan funcion of ime, we would like o deermine he ime dependence of he posiion funcion x( and he x -componen of
More informationThe Contradiction within Equations of Motion with Constant Acceleration
The Conradicion wihin Equaions of Moion wih Consan Acceleraion Louai Hassan Elzein Basheir (Daed: July 7, 0 This paper is prepared o demonsrae he violaion of rules of mahemaics in he algebraic derivaion
More informationThe expectation value of the field operator.
The expecaion value of he field operaor. Dan Solomon Universiy of Illinois Chicago, IL dsolom@uic.edu June, 04 Absrac. Much of he mahemaical developmen of quanum field heory has been in suppor of deermining
More informationLecture 10: The Poincaré Inequality in Euclidean space
Deparmens of Mahemaics Monana Sae Universiy Fall 215 Prof. Kevin Wildrick n inroducion o non-smooh analysis and geomery Lecure 1: The Poincaré Inequaliy in Euclidean space 1. Wha is he Poincaré inequaliy?
More informationKEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow
1 KEY Mah 4 Miderm I Fall 8 secions 1 and Insrucor: Sco Glasgow Please do NOT wrie on his eam. No credi will be given for such work. Raher wrie in a blue book, or on our own paper, preferabl engineering
More informationExample on p. 157
Example 2.5.3. Le where BV [, 1] = Example 2.5.3. on p. 157 { g : [, 1] C g() =, g() = g( + ) [, 1), var (g) = sup g( j+1 ) g( j ) he supremum is aken over all he pariions of [, 1] (1) : = < 1 < < n =
More informationAppendix 14.1 The optimal control problem and its solution using
1 Appendix 14.1 he opimal conrol problem and is soluion using he maximum principle NOE: Many occurrences of f, x, u, and in his file (in equaions or as whole words in ex) are purposefully in bold in order
More information10. State Space Methods
. Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he
More informationGuest Lectures for Dr. MacFarlane s EE3350 Part Deux
Gues Lecures for Dr. MacFarlane s EE3350 Par Deux Michael Plane Mon., 08-30-2010 Wrie name in corner. Poin ou his is a review, so I will go faser. Remind hem o go lisen o online lecure abou geing an A
More informationt 2 B F x,t n dsdt t u x,t dxdt
Evoluion Equaions For 0, fixed, le U U0, where U denoes a bounded open se in R n.suppose ha U is filled wih a maerial in which a conaminan is being ranspored by various means including diffusion and convecion.
More informationChapter 6. Systems of First Order Linear Differential Equations
Chaper 6 Sysems of Firs Order Linear Differenial Equaions We will only discuss firs order sysems However higher order sysems may be made ino firs order sysems by a rick shown below We will have a sligh
More informationSZG Macro 2011 Lecture 3: Dynamic Programming. SZG macro 2011 lecture 3 1
SZG Macro 2011 Lecure 3: Dynamic Programming SZG macro 2011 lecure 3 1 Background Our previous discussion of opimal consumpion over ime and of opimal capial accumulaion sugges sudying he general decision
More information1 Review of Zero-Sum Games
COS 5: heoreical Machine Learning Lecurer: Rob Schapire Lecure #23 Scribe: Eugene Brevdo April 30, 2008 Review of Zero-Sum Games Las ime we inroduced a mahemaical model for wo player zero-sum games. Any
More informationOrthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind
Proceedings of he World Congress on Engineering 2008 Vol II Orhogonal Raional Funcions, Associaed Raional Funcions And Funcions Of The Second Kind Karl Deckers and Adhemar Bulheel Absrac Consider he sequence
More informationMATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018
MATH 5720: Gradien Mehods Hung Phan, UMass Lowell Ocober 4, 208 Descen Direcion Mehods Consider he problem min { f(x) x R n}. The general descen direcions mehod is x k+ = x k + k d k where x k is he curren
More informationSOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM
SOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM FRANCISCO JAVIER GARCÍA-PACHECO, DANIELE PUGLISI, AND GUSTI VAN ZYL Absrac We give a new proof of he fac ha equivalen norms on subspaces can be exended
More information8. Basic RL and RC Circuits
8. Basic L and C Circuis This chaper deals wih he soluions of he responses of L and C circuis The analysis of C and L circuis leads o a linear differenial equaion This chaper covers he following opics
More informationarxiv: v2 [math.ap] 16 Oct 2017
Unspecified Journal Volume 00, Number 0, Pages 000 000 S????-????XX0000-0 MINIMIZATION SOLUTIONS TO CONSERVATION LAWS WITH NON-SMOOTH AND NON-STRICTLY CONVEX FLUX CAREY CAGINALP arxiv:1708.02339v2 [mah.ap]
More informationEssential Microeconomics : OPTIMAL CONTROL 1. Consider the following class of optimization problems
Essenial Microeconomics -- 6.5: OPIMAL CONROL Consider he following class of opimizaion problems Max{ U( k, x) + U+ ( k+ ) k+ k F( k, x)}. { x, k+ } = In he language of conrol heory, he vecor k is he vecor
More informationTHE WAVE EQUATION. part hand-in for week 9 b. Any dilation v(x, t) = u(λx, λt) of u(x, t) is also a solution (where λ is constant).
THE WAVE EQUATION 43. (S) Le u(x, ) be a soluion of he wave equaion u u xx = 0. Show ha Q43(a) (c) is a. Any ranslaion v(x, ) = u(x + x 0, + 0 ) of u(x, ) is also a soluion (where x 0, 0 are consans).
More informationNEW APPROACH TO DIFFERENTIAL EQUATIONS WITH COUNTABLE IMPULSES
1 9 NEW APPROACH TO DIFFERENTIAL EQUATIONS WITH COUNTABLE IMPULSES Hong-Kun ZHANG Jin-Guo LIAN Jiong SUN Received: 1 January 2007 c 2006 Springer Science + Business Media, Inc. Absrac This paper provides
More informationRANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY
ECO 504 Spring 2006 Chris Sims RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY 1. INTRODUCTION Lagrange muliplier mehods are sandard fare in elemenary calculus courses, and hey play a cenral role in economic
More informationA Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero
JOURNAL OF MAEMAICAL ANALYSIS AND APPLICAIONS 24, 7887 1997 ARICLE NO. AY965143 A Necessary and Sufficien Condiion for he Soluions of a Funcional Differenial Equaion o Be Oscillaory or end o Zero Piambar
More information11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu
ON EQUATIONS WITH SETS AS UNKNOWNS BY PAUL ERDŐS AND S. ULAM DEPARTMENT OF MATHEMATICS, UNIVERSITY OF COLORADO, BOULDER Communicaed May 27, 1968 We shall presen here a number of resuls in se heory concerning
More information4. Advanced Stability Theory
Applied Nonlinear Conrol Nguyen an ien - 4 4 Advanced Sabiliy heory he objecive of his chaper is o presen sabiliy analysis for non-auonomous sysems 41 Conceps of Sabiliy for Non-Auonomous Sysems Equilibrium
More informationBasic Circuit Elements Professor J R Lucas November 2001
Basic Circui Elemens - J ucas An elecrical circui is an inerconnecion of circui elemens. These circui elemens can be caegorised ino wo ypes, namely acive and passive elemens. Some Definiions/explanaions
More informationMODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE
Topics MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES 2-6 3. FUNCTION OF A RANDOM VARIABLE 3.2 PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE 3.3 EXPECTATION AND MOMENTS
More informationTHE BELLMAN PRINCIPLE OF OPTIMALITY
THE BELLMAN PRINCIPLE OF OPTIMALITY IOANID ROSU As I undersand, here are wo approaches o dynamic opimizaion: he Ponrjagin Hamilonian) approach, and he Bellman approach. I saw several clear discussions
More informationAn Invariance for (2+1)-Extension of Burgers Equation and Formulae to Obtain Solutions of KP Equation
Commun Theor Phys Beijing, China 43 2005 pp 591 596 c Inernaional Academic Publishers Vol 43, No 4, April 15, 2005 An Invariance for 2+1-Eension of Burgers Equaion Formulae o Obain Soluions of KP Equaion
More informationExpert Advice for Amateurs
Exper Advice for Amaeurs Ernes K. Lai Online Appendix - Exisence of Equilibria The analysis in his secion is performed under more general payoff funcions. Wihou aking an explici form, he payoffs of he
More informationSPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F. Trench. SIAM J. Matrix Anal. Appl. 11 (1990),
SPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F Trench SIAM J Marix Anal Appl 11 (1990), 601-611 Absrac Le T n = ( i j ) n i,j=1 (n 3) be a real symmeric
More informationd 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3
and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or
More informationClass Meeting # 10: Introduction to the Wave Equation
MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion
More informationEchocardiography Project and Finite Fourier Series
Echocardiography Projec and Finie Fourier Series 1 U M An echocardiagram is a plo of how a porion of he hear moves as he funcion of ime over he one or more hearbea cycles If he hearbea repeas iself every
More informationStability and Bifurcation in a Neural Network Model with Two Delays
Inernaional Mahemaical Forum, Vol. 6, 11, no. 35, 175-1731 Sabiliy and Bifurcaion in a Neural Nework Model wih Two Delays GuangPing Hu and XiaoLing Li School of Mahemaics and Physics, Nanjing Universiy
More informationExistence Theory of Second Order Random Differential Equations
Global Journal of Mahemaical Sciences: Theory and Pracical. ISSN 974-32 Volume 4, Number 3 (22), pp. 33-3 Inernaional Research Publicaion House hp://www.irphouse.com Exisence Theory of Second Order Random
More informationUndetermined coefficients for local fractional differential equations
Available online a www.isr-publicaions.com/jmcs J. Mah. Compuer Sci. 16 (2016), 140 146 Research Aricle Undeermined coefficiens for local fracional differenial equaions Roshdi Khalil a,, Mohammed Al Horani
More informationMorning Time: 1 hour 30 minutes Additional materials (enclosed):
ADVANCED GCE 78/0 MATHEMATICS (MEI) Differenial Equaions THURSDAY JANUARY 008 Morning Time: hour 30 minues Addiional maerials (enclosed): None Addiional maerials (required): Answer Bookle (8 pages) Graph
More informationCHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR
Annales Academiæ Scieniarum Fennicæ Mahemaica Volumen 31, 2006, 39 46 CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR Joaquim Marín and Javier
More informationCONTRIBUTION TO IMPULSIVE EQUATIONS
European Scienific Journal Sepember 214 /SPECIAL/ ediion Vol.3 ISSN: 1857 7881 (Prin) e - ISSN 1857-7431 CONTRIBUTION TO IMPULSIVE EQUATIONS Berrabah Faima Zohra, MA Universiy of sidi bel abbes/ Algeria
More informationSOLUTIONS TO ECE 3084
SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no
More informationT L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB
Elecronic Companion EC.1. Proofs of Technical Lemmas and Theorems LEMMA 1. Le C(RB) be he oal cos incurred by he RB policy. Then we have, T L E[C(RB)] 3 E[Z RB ]. (EC.1) Proof of Lemma 1. Using he marginal
More informationThe Arcsine Distribution
The Arcsine Disribuion Chris H. Rycrof Ocober 6, 006 A common heme of he class has been ha he saisics of single walker are ofen very differen from hose of an ensemble of walkers. On he firs homework, we
More informationA remark on the H -calculus
A remark on he H -calculus Nigel J. Kalon Absrac If A, B are secorial operaors on a Hilber space wih he same domain range, if Ax Bx A 1 x B 1 x, hen i is a resul of Auscher, McInosh Nahmod ha if A has
More informationCHAPTER 2 Signals And Spectra
CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par
More informationMath 334 Fall 2011 Homework 11 Solutions
Dec. 2, 2 Mah 334 Fall 2 Homework Soluions Basic Problem. Transform he following iniial value problem ino an iniial value problem for a sysem: u + p()u + q() u g(), u() u, u () v. () Soluion. Le v u. Then
More informationdt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3.
Mah Rahman Exam Review Soluions () Consider he IVP: ( 4)y 3y + 4y = ; y(3) = 0, y (3) =. (a) Please deermine he longes inerval for which he IVP is guaraneed o have a unique soluion. Soluion: The disconinuiies
More informationIMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013
IMPLICI AND INVERSE FUNCION HEOREMS PAUL SCHRIMPF 1 OCOBER 25, 213 UNIVERSIY OF BRIISH COLUMBIA ECONOMICS 526 We have exensively sudied how o solve sysems of linear equaions. We know how o check wheher
More informationSupplementary Material
Dynamic Global Games of Regime Change: Learning, Mulipliciy and iming of Aacks Supplemenary Maerial George-Marios Angeleos MI and NBER Chrisian Hellwig UCLA Alessandro Pavan Norhwesern Universiy Ocober
More informationLAPLACE TRANSFORM AND TRANSFER FUNCTION
CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions
More informationBU Macro BU Macro Fall 2008, Lecture 4
Dynamic Programming BU Macro 2008 Lecure 4 1 Ouline 1. Cerainy opimizaion problem used o illusrae: a. Resricions on exogenous variables b. Value funcion c. Policy funcion d. The Bellman equaion and an
More informationVariational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations
IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial
More information