Estimating a Bounded Normal Mean Under the LINEX Loss Function

Size: px
Start display at page:

Download "Estimating a Bounded Normal Mean Under the LINEX Loss Function"

Transcription

1 Journl of Sciences, Islic Republic of Irn 4(): (03) University of Tehrn, ISSN Estiting Bounded Norl Men Under the LINEX Loss Function A. Krinezhd * Deprtent of Sttistics, Fculty of Mthetics, Sttistics nd Coputer Science, University of Tehrn, Tehrn, Islic Republic of Irn Received: 8 Jnury 03 / Revised: 3 My 03 / Accepted: July 03 Abstrct Let X be rndo vrible fro norl distribution with unknown en θ nd known vrince σ. In ny prcticl situtions, θ is known in dvnce to lie in n intervl, sy [,], for soe > 0. As the usul estitor of θ, i.e., X under the LINEX loss function is indissible, finding soe copetitors for X becoes worthwhile. The only study in the literture considered the proble of inix estition of θ In this pper, by constructing dointing clss of estitors, we show tht the xiu likelihood estitor is indissible. Then, s copetitor, the Byes estitor ssocited with unifor prior on the intervl [,] is proposed. Finlly, considering risk perfornce s coprison criterion, the estitors re copred nd depending on the vlues tken by θ in the intervl [,], the pproprite estitor is suggested. Keywords: Adissibility; Byes estitor; LINEX loss function; Mxiu likelihood estitor; Norl distribution Introduction In the sttisticl literture it is often ssued tht the preter spce is unbounded which sees to be never fulfilled in prctice. In vrious physicl, industril nd biologicl experients, the experienter hs often soe prior knowledge bout the preter(s) of the underlying popultion. The verge per cpit incoe of developing country is likely to lie between those of n underdeveloped nd developed country. The verge fuel efficiency of new odel of pssenger cr will lie between those of n old odel nd forul one rcing cr. Exples of siilr nture where en of rel phenoen lies in bounded intervl bound in prctice (e.g., physicl ttributes such s height or weight of people, verge life of nils), [4]. Therefore there is prcticl interest to include such dditionl infortion into sttisticl procedures. Surprisingly, while the ssuption of boundedness cn be useful in prctice, it introduces soe chllenging probles in theory. Such probles first rose with the prcticl proble in 950 in which two probbilities nd known to stisfy the restriction, needed to be estited. Mxiu likelihood estition ws used for this purpose. Lter Mxiu Likelihood Estitors (s) were shown to be indissible under Squred Error Loss (SEL) function L ) (, ) (, * Corresponding uthor, Tel.: +98()664, Fx: +98()66478, E-il:.krinezhd@khy.ut.c.ir 57

2 Vol. 4 No. Spring 03 Krinezhd J. Sci. I. R. Irn tht is, it ws shown tht there exist estitors which re better thn the in the sense tht their expected loss, i.e., R(, ) E[ L(, )], s function of the preter to be estited, is nowhere lrger nd soewhere sller thn tht of the. This then led to the serch for dointors for these indissible estitors s well s for dissible estitors with good properties. One such property is tht of inixity where n estitor is inix when there does not exist n estitor with sller xiu expected loss. Exples of probles ddressed in the restricted preter spces, cn be found in [], [7], [6] nd the recent tretise by ven Eeden [7] for detiled discussion. Let X ~ N (, ) denote rndo vrible hving norl distribution with the probbility density function ( ) x f ( x, ) e, x, where, it is supposed tht the vrince is known nd the unknown en, lies in n intervl of the for [, ], for soe known > 0. The first study in estiting the bounded norl en under the SEL function dtes bck to 98. Csell nd Strwdern [4] showed tht, when , there exists unique dissible nd inix estitor of, ssocited with syetric two-point prior on, nd proved tht it dointes the of, when 0. They lso gve clss of dissible nd inix estitors for the cse when.4.6. These estitors re inix w.r.t. syetric three-point prior on,0,. Bickel [] presented n estitor which is syptoticlly inix s, nd showed tht the wek liit of the lest fvourble prior (rescled to [,] ) hs the density cos, nd the inix risk is o( ). After these initil works, severl uthors considered the estition proble in restricted preter spces under the SEL function. Moors [8, 9] ssued bounded estition proble is invrint w.r.t. finite group of trnsfortions nd constructed dointors of boundry estitor. He then pplied his results into the estition proble of bounded norl en. Gtsonis et l. [0] considered the Byes estitor w.r.t. the unifor prior on the intervl [, ], s copetitor for the sple en X, nd showed tht it dointes X. They further nuericlly copred risk perfornce of their Byes estitor, the, the inix estitor, nd the Byes estitor w.r.t. the Bickel s prior, nd finlly recoended the use of their proposed estitor. In ddition to [8, 9], the estition in restricted preter spces under the SEL function, in very generl setting, ws considered in [5, 6, 7]. DsGupt [7] in estiting vector h ( ) when is restricted to sll bounded convex subset k of derived sufficient conditions under which the Byes estitor w.r.t. lest fvourble prior on the boundry of is inix. He then pplied his results in soe distributions including the norl distribution nd showed tht the Byes estitor w.r.t. the two-point prior considered in [4] is inix when Conditions for either indissibility or ethods of constructing dointors within given clss of estitors were presented in [5, 6]. Kur nd Tripthi [4], on the bsis of, proposed nother estitor nd copred the risk perfornce of it with the boveentioned estitors. Dou nd vn Eeden [8], showed the indissibility conditions in [5, 6] re stisfied for the bounded norl en proble nd hence, by giving n explicit for of dointing estitor, derived indissibility of of the en. Ltely, the generl theory of estiting preters of syetric distribution which is subject to n intervl constrint, under the SEL function developed in [6]. See lso [5] for siilr developent. It is worth entioning tht the proble of estiting norl en in the cse where is bounded below, i.e.,, for soe constnt, lso received considerble ttention in the literture. Estition of positive norl en ws first considered in Ktz [3]. Ktz proposed the generlized Byes estitor of w.r.t. the unifor prior on [0, ) nd proved its dissibility nd inixity under the SEL function. He lso proved tht the restricted, is inix. The results of Ktz were independently proved in [] nd generlized in [9] to generl loction preter fily under certin conditions. Therefter, the proble of estiting positive norl en hs developed in the literture, see for exples [5,6] nd references there in. All the bove-entioned studies re bsed on the SEL function which penlizes eqully overestition nd underestition of desired preter, while it does not occur in prctice. For exple, in food processing industries, if the continers re underfilled, it is possible to incur uch ore severe penlty rising fro isrepresenttion of the products ctul weight or volue, see []. As nother exple, in d construction, n underestition of the pek wter level is usully uch ore serious thn n overestition, see [9]. 58

3 Estiting Bounded Norl Men Under the LINEX Loss Function Soe uthors hve considered n estition proble under n syetric LINEX (LINer EXponentil) loss function L s e () ( ) s, (, ) { ( ) }, where 0 nd s 0 re fixed rel nubers. This loss function which ws first introduced by Vrin [8], rises exponentilly on one side nd pproxitely linerly on the other side, nd is useful when overestition is perceived s ore serious thn underestition or vice-vers. For ore infortion on point estition under LINEX loss function, see [0, 9]. In the norl en estition proble with no restriction on, Zellner [9] showed tht the usul estitor X under the LINEX loss function is indissible nd dointed by * ( X ) X. () Hence, X is neither dissible nor inix. Also, Rojo [] nd Sdooghi-Alvndi nd Netollhi [3] proved tht in the clss of estitors of the for * cx d, is the only inix nd dissible estitor of. In the bounded norl cse under the LINEX loss function (), the only study dtes bck to 995. Bischoff et l. [3] considered inix estition of nd showed tht the Byes estitor w.r.t. the two-point prior i.e., ( ) ( ), g( X ) ( X ) ln g ( X ) x x where g ( x ) e ( ) e, is inix when 0, nd (0, 0], 0 in 3, ln 3 In this pper, we consider the LINEX loss function () nd with no loss of generlity, we tke s, i.e., L (, ) e, 0. (3) We then propose soe estitors of the bounded norl en nd copre risk perfornce of the proposed ones with the inix estitor derived in [3]. To this end, first, we obtin conditions under which the of, i.e., X ( X ) X X X. is indissible nd hence, we derive clss of dointing estitors. We then propose the Byes estitor of the en w.r.t. unifor prior s copetitor for. Finlly, we wish to copre risk perfornce of the derived estitors. Notice tht the concept of dissibility, Byesinity, invrince nd inixity highly depends on the choice of loss function. It is worth noting tht there exist soe other works relted to restricted preter estition proble, considering other losses. For brief history nd soe relted references, see the recent work done by Krinezhd [] which considered the bounded norl en estition proble reltive to the SEL function. Indissibility of In this section, we construct dointing clss of estitors of bsed on the work done by Chrrs [5] nd Chrrs nd vn Eeden [6] (reders y refer to [8] s convenience version of [5, 6]). Let Ch be shrinkge estitor of the following for X Ch ( X ) X X X, (4) where (0, ]. Due to the entioned i, we first provide soe required terils below. Le. Let x ux ( ) e x ( x) e ( x ) ( x), 0, x v( x) e x ( x) e ( x ) ( x), 0, (5) (6) where (.) nd (.) denote the distribution nd density function of stndrd norl rndo vrible. Then ux ( ), v( x ) nd their first nd second derivtives hve 59

4 Vol. 4 No. Spring 03 Krinezhd J. Sci. I. R. Irn the following properties: () ux ( ) nd v( x ) re decresing for x 0 nd incresing for x 0. (b) ( ) x u x e ( x ) nd hs the se sign s x. x (c) u ( x) e ( x) for x 0. (d) ( ) x v x e ( x ) nd hs the se sign s x. x (e) v ( x ) e ( x) for x 0. Proof. The proof is strightforwrd nd oitted. Le. Let hx (, ) u( x) v( x) where ux ( ) nd v( x ) re given by (5) nd (6). Further suppose is positive, then () For fixed (0, ) nd for (, ], h (, ) is decresing function of. x [0, ], (b) For let ( x ) h ( x, ) u( x) v( x). (7) Then (0) 0 nd ( ) 0. Furtherore, if 0 stisfy one of the following conditions: 0 (8) or where 0 x ( ), ( ) 0 nd w w (9) w e (0) ( ) nd w ( ) e ( ) () ( e ) e ( ), then ( x ) 0, for x (0, ). Hence, there exists unique root (0, ) of the eqution ( x ) 0 such tht under conditions (8) or (9), for x [0, ), ( x ) 0, nd for x (, ], ( x ) 0. Proof. () Differentiting h (, ) w.r.t., we hve h (, ) u( ) () v ( ). Now using Le (c) nd (e), the reinder is esily obtined. (b) Differentiting ( x ) w.r.t. x, we hve ( x ) u ( x ) v ( x). On the other side, for x [0, ] u ( x) v ( x) ( x) Now let w x e e e ( x ) x x ( ). (3) We discuss the sign of w( x ). Due to condition (8), nd hence w( x ) is positive. Moreover under condition (9), it cn be esily seen tht w( x ) is n incresing function. So using eqution (0), for x [0, ], w ( x ) w (0) e w ( ). Further, using the following inequlities ( x ) e x e ( x ) x e x e ( ) ( ), ( x) e ( ) e, x ( x) e 0, ( ) (0), And equtions () nd (3), we conclude tht u ( x ) v ( x) w ( ). Hence, if 0 nd e ( x ) x e ( x) ( ) x x e () x () x e x e ( x) ( ) x x e () x () x e x e ( x) ( ) x ( x) e e x w( ), w ( ) 0, u ( x) v ( x) will be positive nd the proof is copleted. The in result of this section is s follows. Theore. Let X ~ N(,) when, 0. Then under conditions (8) nd (9), :0 Ch is clss of dointing estitors of w.r.t. the LINEX loss function (3), where is the unique root of eqution (0). x ( x) e e e ( x) x x 60

5 Estiting Bounded Norl Men Under the LINEX Loss Function Proof. Due to equtions (5) nd (6), it cn be esily verify tht the risk function of nd Ch hve the following for nd R(, ) u( ) v( ) Let (, ;, ) R(, ) R(, ). Ch Ch (4) (5) Now, we discuss the sign of (, Ch ;, ) in two cses. (i) when [, ), using Le () the desired result follows. (ii) when (, ], differentiting (, Ch ;, ) w.r.t., ccording to Le (), we hve () 0, 0 (, Ch ;, ) h (, ) ( ) 0,. Consequently, for [0, ] nd (, ], (, ;, ) (, ;,0) 0 Ch Ch And this copletes the proof. The next le which is siilr to the work done by Moors [8, 9] nd Bischoff et l. [3], provides useful extension of the in result. Le 3. Suppose n estition proble is invrint w.r.t. the finite group of trnsfortions G e, g, where for x, ex ( ) x is n identity trnsfortion nd g ( x) x. Further suppose for x, i( x ) i( x ), i,. Then, in the fily of norl distributions N (,), nd under the LINEX function (3), for given 0 nd [, ], dointes if nd only if for 0 nd [, ],.. dointe. R(, ) u( ) v( ). Ch Proof. The following reltion is held ssuing the entioned ssuptions E L, i ( X ) E L, i( X ), i, nd becuse of tht,, ( ), ( ) E L X E L X E L, ( X ) E L, ( X ). This gives the desired result. Now, using Theore nd Le 3, the next theore is ieditely derived. Theore. Let X ~ N(,) when, 0. Then under conditions or 0 nd x w ( ), w ( ) 0 where w () nd w () re given in equtions (0) nd () respectively, for 0 nd [, ], is indissible nd :0 Ch is clss of dointing estitors of, where Ch is given in (4) nd is the unique root stisfying Theore. In Tble, vlues of w(), w () (given by equtions (0) nd ()) for different vlues of nd hve been tbulted. As it cn be seen, when is positive, t lest on of w () nd w () is positive nd the condition x w( ), w ( ) 0 is not liiting one. In the se wy, it cn be inferred tht when is negtive, the condition x w( ), w ( ) 0 is not n encubrnce condition. In Tble, vlues of the unique root of eqution (7) for vrious vlues of nd hve been clculted. Notice tht under conditions entioned in Theore, for (0, ] nd [, ], Ch dointes but becuse of the theticl difficult coputtions, it is not esy to prove this property explicitly. This subject in Theore for (0, ] nd [, ] holds but becuse of the se reson, we cnnot prove tht. This desired property is obviously seen fro Fig. Tble. Vlues of (w(),w()) for different vlues of nd (0.0896,0.0997) (0.408,0.79) (0.488,0.0305) 0.50 (0.087,0.056) (0.065,0.043) (0.493,0.33) 0.80 ( ,0.038) ( ,0.004) (0.0780,0.004).00 (-0.97,0.005) (-0.3,0.009) (0.009, ).00 ( ,0.0373) ( ,0.0453) (-0.59,0.090) 5.00 ( ,0.0368) ( ,0.005) (-0.997,0.0073) 0.00 (-0.787,0.035) ( ,0.007) (-0.000,0.007) 6

6 Vol. 4 No. Spring 03 Krinezhd J. Sci. I. R. Irn to Fig. 6. Moreover when tends to, the difference between risk functions of Ch nd becoes significnt. This desired property is obvious fro Fig.. Besides in Fig., risk functions of Ch nd cut ech other in [, ]. This is due to the vlue of. In fct the vlues 0.4 nd 0.7 is out of the intervl (0, ) (see Tble ) nd hence ccording to Theore there is no reson for the doinnce of Ch on. The se thing hppens in Fig. 3. Additionlly, copring Fig. nd Fig. 3 revels the iportnt of selection for vlues of (difference between overestition nd underestition). Underlying the iportnt of overestition nd underestition, it cn be seen tht in Fig. ll the risk functions, between nd, tke their iniu t the point nd in Fig. 3 this issue hppens conversely. Byes Estitor Associted with the Unifor Prior In this section we propose nother copetitor for. This copetitor is the Byes estitor ssocited with the unifor prior u ( ), [, ]. The Byes estitor w.r.t. the LINEX loss function (3) is given by, ( X ) lne e X h,0( X ) X ln, h ( X ), where h, ( X ) ( X ) ( X ). Copring, with * (given by ()), we re interested in the behviour of risk function of,. In the next section, we crry out siultion study to see the perfornce of,. Coprisons of Risk Perfornce In this section we coproise the risk function of ll the estitors, nely *,,,, Ch nd,. * The risk function of is constnt ( /) nd the risk of nd Ch hve been given in (4) nd (5),, respectively. The risk function of nd, hs not n nlyticl for nd hence, it is ipossible to copre their risks explicitly. So, we hve coputed their estited risks nd figured the in Fig. 4 to Fig. 6. Since Bischoff et l. [3] hve proved inixity of, for 0, we hve chosen soe positive vlues for. Further, we hve considered two-point prior used in this pper, is syetric one, i.e., /. Notice tht our coprisons re on the bsis of crefully nlysis nd here, we hve just figured the risk functions for soe selected vlues of nd. Our conclusion is s follows: * () Risk function of is constnt ( /) but s it cn be seen especilly fro Fig. 4, other the estitors hve sller risk vlues. Moreover * is not rngepreserving. So, becuse of these resons, we prefer not to use it ny longer., (b) under the inixity condition, i.e., (0, 0], where 0 in{ ( 3 ), ln 3}, hs quite good risk perfornce when is close to. (c) Ch hs good risk perfornce w.r.t.. The risk difference of these two estitors for sll vlues of nd is stisfctory. In ddition, nd Ch hs sller risk vlues when is close to. (d), for oderte vlues of in [, ], hs rerkble risk perfornce. It lso is less sensitive to, chnges in vlues of nd. Moreover, tkes the xiu vlue its risk function t point which is close to the risk function of the inix estitor,. These desirble behviours of the risk function of cn be observed siplicity fro Fig. 4 to Fig. 6., Results The proble considered in this pper is tht of estiting the en of norl distribution under the dditionl infortion tht the en lies in bounded intervl [, ] under the LINEX loss function (3). Soe estitors for the en were proposed, nely, X, *,,,, Ch nd,. It ws first shown tht, under ild conditions, Ch dointes. Then, considering risk perfornce s coprison criterion, the estitors were copred. We do not recoend the use of the usul estitor X nd *, which re not rnge preserving. We then bsed on our nuericl, results, recoend the use of when is close to, nd or Ch when is close to. The use of, is recoended when hs oderte vlues in [, ]. 6

7 Estiting Bounded Norl Men Under the LINEX Loss Function Figure. Risk functions of δ nd δch for = = 0.5 nd different vlues of. Figure. Risk functions of δ nd δch for = = 0.75 nd different vlues of. Figure 3. Risk functions of δ nd δch for = = 0.75 nd different vlues of. Figure 4. The risk functions for = = Figure 5. The risk functions for = 0.5 nd =. Figure 6. The risk functions for = nd =.5. 63

8 Vol. 4 No. Spring 03 Krinezhd J. Sci. I. R. Irn Tble. Vlues of the unique root of eqution (7) for vrious vlues of tken by estitors when, Tble. Continued Acknowledgents The uthor pprecites Prof. Ahd Prsin nd Dr. Nder Netollhi for their vluble rerks. The uthor lso would like to thnk Dr. J. J. A. Moors for sending copy of his thesis. References. Bder G. nd Bischoff W. Old nd new spects of inix estition of bounded preter. IMS Lecture Notes-Monogrph Series, 4: 5-30, Institute of theticl sttistics, Hywrd, Cliforni, USA (003).. Bickel P.J. Minix estition of the en of norl distribution when the preter spce is restricted. Ann. Sttist., 9: (98). 3. Bischoff W., Fieger W. nd Wulfert S. Minix nd Γ- inix estition of bounded norl en under LINEX loss. Sttist. Decisions, 3: (995). 4. Csell G. nd Strwdern W.E. Estiting bounded norl en. Ann. Sttist., 9: (98). 5. Chrrs A. Propriete Bysienne et dissibilite p destiteurs dns in sousenseble convex de, Ph.D. Thesis, Universite de Montrel, Montrel, Cnd, (979). 6. Chrrs A. nd vn Eeden C. Byes nd dissibility properties of estitors in truncted preter spces. Cnd. J. Sttist., 9: 34 (99). 7. DsGupt A. Byes inix estition in ultipreter filies when the preter spce is restricted to bounded convex set. Snkhy Ser. A, 47: (985). 8. Dou Y. nd vn Eeden, C. Coprisons of the perfornces of estitors of bounded norl en under squred-error loss. REVSTAT, 7: 03-6 (009). 9. Frrell R.H. Estitors of loction preter in the bsolutely continuous cse. Ann. Mth. Sttist., 35: (964). 0. Gtsonis C., McGibbon B. nd Strdern, W.E. On the estition of restricted norl en. Sttist. Prob. Lett., 3: -30 (987).. Hrris T.J. Optil controliers of nonsyetric nd nonqudrtic loss functions. Technoetrics, 34: (99).. Krinezhd A. Estiting bounded norl en reltive to squred error loss function. J. Sci., I.R. Irn, (3): (0). 3. Ktz M.W. Adissible nd inix estites of preters in truncted spces. Ann. Mth. Sttist., 3: 36 4 (96). 4. Kur S. nd Tripthi Y.M. Estiting restricted norl en. Metrik, 68: 7-88 (008). 5. Mrchnd E., Oussou I., Pyndeh A.T. nd Perron F. On the estition of restricted loction preter for syetric distributions. J. Jpn Sttist. Soc., 38: (008). 6. Mrchnd E. nd Perron F. Estiting bounded preter for syetric distributions. Ann. Inst. Sttist. Mth. 6: 5-34 (009). 7. Mrchnd E. nd Strwdern, W. E. Estition on restricted preter spces: A review, IMS Lecture Notes- Monogrph Series, 45: -4, Institute of theticl sttistics, Hywrd, Cliforni, USA (004). 8. Moors J.J.A. Indissibility of linerly invrint estitors in truncted preter spces. J. Aer. Sttist. Assoc., 76: (98). 9. Moors J.J.A. Estition in truncted preter spces, Ph.D. Thesis, Tilburg University, The Netherlnds (985). 0. Prsin A. nd Kirni S.N.U.A. Estition under LINEX function. In: An Ullh, Wn A.T.K. nd Chturvedi A. (Eds.), hndbook of pplied econoics nd sttisticsl inference, pp (00).. Rojo J. On the dissibility of cx d w.r.t. the LINEX loss function, Co. Sttist. - Theory Methods, 6: (987).. Scks J. Generlized Byes solutions in estition probles, The Ann. Mth. Sttist., 34: (963). 3. Sdooghi-Alvndi. S.M. nd Netollhi N. On the dissibility of cx d reltive to LINEX loss function. Co. Sttist. - Theory Methods, : (989). 4. Sho P. Y-S. nd Strwdern W. E. Iproving on the of positive norl en, Sttist. Sinic, 6: (996). 5. Tripthi Y.M. nd Kur S. Estiting positive norl en, Sttist. Ppers, 48: (007). 6. vn Eeden C. Estition in restricted preter spcesoe history nd soe recent developents. CWI Qurterly, 9: (996). 7. vn Eeden C. Restricted preter spce estition probles: dissibility nd inixity properties. Springer, New York (006). 8. Vrin A. Byesin pproch to rel stte ssessent. In studies in Byesin Econoetrics nd sttistics in honour of Leonrd J. Svge, Eds. Stephn E., Fienberg nd Arnold Zellner, Asterd: North-Holnd, (975). 9. Zellner A. Byesin estition nd prediction using ssyetric loss function. J. Aer. Sttist. Assoc., 8: (986). 64

ECONOMETRIC THEORY. MODULE IV Lecture - 16 Predictions in Linear Regression Model

ECONOMETRIC THEORY. MODULE IV Lecture - 16 Predictions in Linear Regression Model ECONOMETRIC THEORY MODULE IV Lecture - 16 Predictions in Liner Regression Model Dr. Shlbh Deprtent of Mthetics nd Sttistics Indin Institute of Technology Knpur Prediction of vlues of study vrible An iportnt

More information

UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH HÖLDER CONTINUITY

UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH HÖLDER CONTINUITY UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH HÖLDER CONTINUITY YIFEI PAN, MEI WANG, AND YU YAN ABSTRACT We estblish soe uniqueness results ner 0 for ordinry differentil equtions of the

More information

UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH HÖLDER CONTINUITY

UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH HÖLDER CONTINUITY UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH HÖLDER CONTINUITY YIFEI PAN, MEI WANG, AND YU YAN ABSTRACT We study ordinry differentil equtions of the type u n t = fut with initil conditions

More information

New Expansion and Infinite Series

New Expansion and Infinite Series Interntionl Mthemticl Forum, Vol. 9, 204, no. 22, 06-073 HIKARI Ltd, www.m-hikri.com http://dx.doi.org/0.2988/imf.204.4502 New Expnsion nd Infinite Series Diyun Zhng College of Computer Nnjing University

More information

Contact Analysis on Large Negative Clearance Four-point Contact Ball Bearing

Contact Analysis on Large Negative Clearance Four-point Contact Ball Bearing Avilble online t www.sciencedirect.co rocedi ngineering 7 0 74 78 The Second SR Conference on ngineering Modelling nd Siultion CMS 0 Contct Anlysis on Lrge Negtive Clernce Four-point Contct Bll Bering

More information

The Regulated and Riemann Integrals

The Regulated and Riemann Integrals Chpter 1 The Regulted nd Riemnn Integrls 1.1 Introduction We will consider severl different pproches to defining the definite integrl f(x) dx of function f(x). These definitions will ll ssign the sme vlue

More information

Exponents and Powers

Exponents and Powers EXPONENTS AND POWERS 9 Exponents nd Powers CHAPTER. Introduction Do you know? Mss of erth is 5,970,000,000,000, 000, 000, 000, 000 kg. We hve lredy lernt in erlier clss how to write such lrge nubers ore

More information

Second degree generalized gauss-seidel iteration method for solving linear system of equations. ABSTRACT

Second degree generalized gauss-seidel iteration method for solving linear system of equations. ABSTRACT Ethiop. J. Sci. & Technol. 7( 5-, 0 5 Second degree generlized guss-seidel itertion ethod for solving liner syste of equtions Tesfye Keede Bhir Dr University, College of Science, Deprtent of Mthetics tk_ke@yhoo.co

More information

Lecture 1. Functional series. Pointwise and uniform convergence.

Lecture 1. Functional series. Pointwise and uniform convergence. 1 Introduction. Lecture 1. Functionl series. Pointwise nd uniform convergence. In this course we study mongst other things Fourier series. The Fourier series for periodic function f(x) with period 2π is

More information

Continuous Random Variables

Continuous Random Variables STAT/MATH 395 A - PROBABILITY II UW Winter Qurter 217 Néhémy Lim Continuous Rndom Vribles Nottion. The indictor function of set S is rel-vlued function defined by : { 1 if x S 1 S (x) if x S Suppose tht

More information

Lyapunov-type inequalities for Laplacian systems and applications to boundary value problems

Lyapunov-type inequalities for Laplacian systems and applications to boundary value problems Avilble online t www.isr-publictions.co/jns J. Nonliner Sci. Appl. 11 2018 8 16 Reserch Article Journl Hoepge: www.isr-publictions.co/jns Lypunov-type inequlities for Lplcin systes nd pplictions to boundry

More information

Unit #9 : Definite Integral Properties; Fundamental Theorem of Calculus

Unit #9 : Definite Integral Properties; Fundamental Theorem of Calculus Unit #9 : Definite Integrl Properties; Fundmentl Theorem of Clculus Gols: Identify properties of definite integrls Define odd nd even functions, nd reltionship to integrl vlues Introduce the Fundmentl

More information

Math 31S. Rumbos Fall Solutions to Assignment #16

Math 31S. Rumbos Fall Solutions to Assignment #16 Mth 31S. Rumbos Fll 2016 1 Solutions to Assignment #16 1. Logistic Growth 1. Suppose tht the growth of certin niml popultion is governed by the differentil eqution 1000 dn N dt = 100 N, (1) where N(t)

More information

NUMERICAL INTEGRATION. The inverse process to differentiation in calculus is integration. Mathematically, integration is represented by.

NUMERICAL INTEGRATION. The inverse process to differentiation in calculus is integration. Mathematically, integration is represented by. NUMERICAL INTEGRATION 1 Introduction The inverse process to differentition in clculus is integrtion. Mthemticlly, integrtion is represented by f(x) dx which stnds for the integrl of the function f(x) with

More information

r = cos θ + 1. dt ) dt. (1)

r = cos θ + 1. dt ) dt. (1) MTHE 7 Proble Set 5 Solutions (A Crdioid). Let C be the closed curve in R whose polr coordintes (r, θ) stisfy () Sketch the curve C. r = cos θ +. (b) Find pretriztion t (r(t), θ(t)), t [, b], of C in polr

More information

5.7 Improper Integrals

5.7 Improper Integrals 458 pplictions of definite integrls 5.7 Improper Integrls In Section 5.4, we computed the work required to lift pylod of mss m from the surfce of moon of mss nd rdius R to height H bove the surfce of the

More information

Estimation of Binomial Distribution in the Light of Future Data

Estimation of Binomial Distribution in the Light of Future Data British Journl of Mthemtics & Computer Science 102: 1-7, 2015, Article no.bjmcs.19191 ISSN: 2231-0851 SCIENCEDOMAIN interntionl www.sciencedomin.org Estimtion of Binomil Distribution in the Light of Future

More information

AQA Further Pure 2. Hyperbolic Functions. Section 2: The inverse hyperbolic functions

AQA Further Pure 2. Hyperbolic Functions. Section 2: The inverse hyperbolic functions Hperbolic Functions Section : The inverse hperbolic functions Notes nd Emples These notes contin subsections on The inverse hperbolic functions Integrtion using the inverse hperbolic functions Logrithmic

More information

MIXED MODELS (Sections ) I) In the unrestricted model, interactions are treated as in the random effects model:

MIXED MODELS (Sections ) I) In the unrestricted model, interactions are treated as in the random effects model: 1 2 MIXED MODELS (Sections 17.7 17.8) Exmple: Suppose tht in the fiber breking strength exmple, the four mchines used were the only ones of interest, but the interest ws over wide rnge of opertors, nd

More information

MAC-solutions of the nonexistent solutions of mathematical physics

MAC-solutions of the nonexistent solutions of mathematical physics Proceedings of the 4th WSEAS Interntionl Conference on Finite Differences - Finite Elements - Finite Volumes - Boundry Elements MAC-solutions of the nonexistent solutions of mthemticl physics IGO NEYGEBAUE

More information

7.2 The Definite Integral

7.2 The Definite Integral 7.2 The Definite Integrl the definite integrl In the previous section, it ws found tht if function f is continuous nd nonnegtive, then the re under the grph of f on [, b] is given by F (b) F (), where

More information

OXFORD H i g h e r E d u c a t i o n Oxford University Press, All rights reserved.

OXFORD H i g h e r E d u c a t i o n Oxford University Press, All rights reserved. Renshw: Mths for Econoics nswers to dditionl exercises Exercise.. Given: nd B 5 Find: () + B + B 7 8 (b) (c) (d) (e) B B B + B T B (where 8 B 6 B 6 8 B + B T denotes the trnspose of ) T 8 B 5 (f) (g) B

More information

Exam 2, Mathematics 4701, Section ETY6 6:05 pm 7:40 pm, March 31, 2016, IH-1105 Instructor: Attila Máté 1

Exam 2, Mathematics 4701, Section ETY6 6:05 pm 7:40 pm, March 31, 2016, IH-1105 Instructor: Attila Máté 1 Exm, Mthemtics 471, Section ETY6 6:5 pm 7:4 pm, Mrch 1, 16, IH-115 Instructor: Attil Máté 1 17 copies 1. ) Stte the usul sufficient condition for the fixed-point itertion to converge when solving the eqution

More information

Lecture 1: Introduction to integration theory and bounded variation

Lecture 1: Introduction to integration theory and bounded variation Lecture 1: Introduction to integrtion theory nd bounded vrition Wht is this course bout? Integrtion theory. The first question you might hve is why there is nything you need to lern bout integrtion. You

More information

UNIT 1 FUNCTIONS AND THEIR INVERSES Lesson 1.4: Logarithmic Functions as Inverses Instruction

UNIT 1 FUNCTIONS AND THEIR INVERSES Lesson 1.4: Logarithmic Functions as Inverses Instruction Lesson : Logrithmic Functions s Inverses Prerequisite Skills This lesson requires the use of the following skills: determining the dependent nd independent vribles in n exponentil function bsed on dt from

More information

20 MATHEMATICS POLYNOMIALS

20 MATHEMATICS POLYNOMIALS 0 MATHEMATICS POLYNOMIALS.1 Introduction In Clss IX, you hve studied polynomils in one vrible nd their degrees. Recll tht if p(x) is polynomil in x, the highest power of x in p(x) is clled the degree of

More information

V E L O C I T Y a n d V E L O C I T Y P R E S S U R E I n A I R S Y S T E M S

V E L O C I T Y a n d V E L O C I T Y P R E S S U R E I n A I R S Y S T E M S V E L O C I T Y n d V E L O C I T Y R E S S U R E I n A I R S Y S T E M S A nlysis of fluid systes using ir re usully done voluetric bsis so the pressure version of the Bernoulli eqution is used. This

More information

MUHAMMAD MUDDASSAR AND AHSAN ALI

MUHAMMAD MUDDASSAR AND AHSAN ALI NEW INTEGRAL INEQUALITIES THROUGH GENERALIZED CONVEX FUNCTIONS WITH APPLICATION rxiv:138.3954v1 [th.ca] 19 Aug 213 MUHAMMAD MUDDASSAR AND AHSAN ALI Abstrct. In this pper, we estblish vrious inequlities

More information

On Some Classes of Breather Lattice Solutions to the sinh-gordon Equation

On Some Classes of Breather Lattice Solutions to the sinh-gordon Equation On Soe Clsses of Brether Lttice Solutions to the sinh-gordon Eqution Zunto Fu,b nd Shiuo Liu School of Physics & Lbortory for Severe Stor nd Flood Disster, Peing University, Beijing, 0087, Chin b Stte

More information

Improper Integrals, and Differential Equations

Improper Integrals, and Differential Equations Improper Integrls, nd Differentil Equtions October 22, 204 5.3 Improper Integrls Previously, we discussed how integrls correspond to res. More specificlly, we sid tht for function f(x), the region creted

More information

Review of Calculus, cont d

Review of Calculus, cont d Jim Lmbers MAT 460 Fll Semester 2009-10 Lecture 3 Notes These notes correspond to Section 1.1 in the text. Review of Clculus, cont d Riemnn Sums nd the Definite Integrl There re mny cses in which some

More information

UNIFORM CONVERGENCE. Contents 1. Uniform Convergence 1 2. Properties of uniform convergence 3

UNIFORM CONVERGENCE. Contents 1. Uniform Convergence 1 2. Properties of uniform convergence 3 UNIFORM CONVERGENCE Contents 1. Uniform Convergence 1 2. Properties of uniform convergence 3 Suppose f n : Ω R or f n : Ω C is sequence of rel or complex functions, nd f n f s n in some sense. Furthermore,

More information

Main topics for the Second Midterm

Main topics for the Second Midterm Min topics for the Second Midterm The Midterm will cover Sections 5.4-5.9, Sections 6.1-6.3, nd Sections 7.1-7.7 (essentilly ll of the mteril covered in clss from the First Midterm). Be sure to know the

More information

CS667 Lecture 6: Monte Carlo Integration 02/10/05

CS667 Lecture 6: Monte Carlo Integration 02/10/05 CS667 Lecture 6: Monte Crlo Integrtion 02/10/05 Venkt Krishnrj Lecturer: Steve Mrschner 1 Ide The min ide of Monte Crlo Integrtion is tht we cn estimte the vlue of n integrl by looking t lrge number of

More information

Duality # Second iteration for HW problem. Recall our LP example problem we have been working on, in equality form, is given below.

Duality # Second iteration for HW problem. Recall our LP example problem we have been working on, in equality form, is given below. Dulity #. Second itertion for HW problem Recll our LP emple problem we hve been working on, in equlity form, is given below.,,,, 8 m F which, when written in slightly different form, is 8 F Recll tht we

More information

Properties of Integrals, Indefinite Integrals. Goals: Definition of the Definite Integral Integral Calculations using Antiderivatives

Properties of Integrals, Indefinite Integrals. Goals: Definition of the Definite Integral Integral Calculations using Antiderivatives Block #6: Properties of Integrls, Indefinite Integrls Gols: Definition of the Definite Integrl Integrl Clcultions using Antiderivtives Properties of Integrls The Indefinite Integrl 1 Riemnn Sums - 1 Riemnn

More information

The final exam will take place on Friday May 11th from 8am 11am in Evans room 60.

The final exam will take place on Friday May 11th from 8am 11am in Evans room 60. Mth 104: finl informtion The finl exm will tke plce on Fridy My 11th from 8m 11m in Evns room 60. The exm will cover ll prts of the course with equl weighting. It will cover Chpters 1 5, 7 15, 17 21, 23

More information

Chapter 0. What is the Lebesgue integral about?

Chapter 0. What is the Lebesgue integral about? Chpter 0. Wht is the Lebesgue integrl bout? The pln is to hve tutoril sheet ech week, most often on Fridy, (to be done during the clss) where you will try to get used to the ides introduced in the previous

More information

How do we solve these things, especially when they get complicated? How do we know when a system has a solution, and when is it unique?

How do we solve these things, especially when they get complicated? How do we know when a system has a solution, and when is it unique? XII. LINEAR ALGEBRA: SOLVING SYSTEMS OF EQUATIONS Tody we re going to tlk bout solving systems of liner equtions. These re problems tht give couple of equtions with couple of unknowns, like: 6 2 3 7 4

More information

Proc. of the 8th WSEAS Int. Conf. on Mathematical Methods and Computational Techniques in Electrical Engineering, Bucharest, October 16-17,

Proc. of the 8th WSEAS Int. Conf. on Mathematical Methods and Computational Techniques in Electrical Engineering, Bucharest, October 16-17, Proc. of the 8th WSEAS Int. Conf. on Mtheticl Methods nd Coputtionl Techniques in Electricl Engineering, Buchrest, October 6-7, 006 Guss-Legendre Qudrture Forul in Runge-utt Method with Modified Model

More information

different methods (left endpoint, right endpoint, midpoint, trapezoid, Simpson s).

different methods (left endpoint, right endpoint, midpoint, trapezoid, Simpson s). Mth 1A with Professor Stnkov Worksheet, Discussion #41; Wednesdy, 12/6/217 GSI nme: Roy Zho Problems 1. Write the integrl 3 dx s limit of Riemnn sums. Write it using 2 intervls using the 1 x different

More information

Time Truncated Two Stage Group Sampling Plan For Various Distributions

Time Truncated Two Stage Group Sampling Plan For Various Distributions Time Truncted Two Stge Group Smpling Pln For Vrious Distributions Dr. A. R. Sudmni Rmswmy, S.Jysri Associte Professor, Deprtment of Mthemtics, Avinshilingm University, Coimbtore Assistnt professor, Deprtment

More information

1.9 C 2 inner variations

1.9 C 2 inner variations 46 CHAPTER 1. INDIRECT METHODS 1.9 C 2 inner vritions So fr, we hve restricted ttention to liner vritions. These re vritions of the form vx; ǫ = ux + ǫφx where φ is in some liner perturbtion clss P, for

More information

A SHORT NOTE ON THE MONOTONICITY OF THE ERLANG C FORMULA IN THE HALFIN-WHITT REGIME. Bernardo D Auria 1

A SHORT NOTE ON THE MONOTONICITY OF THE ERLANG C FORMULA IN THE HALFIN-WHITT REGIME. Bernardo D Auria 1 Working Pper 11-42 (31) Sttistics nd Econometrics Series December, 2011 Deprtmento de Estdístic Universidd Crlos III de Mdrid Clle Mdrid, 126 28903 Getfe (Spin) Fx (34) 91 624-98-49 A SHORT NOTE ON THE

More information

Chapter 5 : Continuous Random Variables

Chapter 5 : Continuous Random Variables STAT/MATH 395 A - PROBABILITY II UW Winter Qurter 216 Néhémy Lim Chpter 5 : Continuous Rndom Vribles Nottions. N {, 1, 2,...}, set of nturl numbers (i.e. ll nonnegtive integers); N {1, 2,...}, set of ll

More information

The First Fundamental Theorem of Calculus. If f(x) is continuous on [a, b] and F (x) is any antiderivative. f(x) dx = F (b) F (a).

The First Fundamental Theorem of Calculus. If f(x) is continuous on [a, b] and F (x) is any antiderivative. f(x) dx = F (b) F (a). The Fundmentl Theorems of Clculus Mth 4, Section 0, Spring 009 We now know enough bout definite integrls to give precise formultions of the Fundmentl Theorems of Clculus. We will lso look t some bsic emples

More information

IN GAUSSIAN INTEGERS X 3 + Y 3 = Z 3 HAS ONLY TRIVIAL SOLUTIONS A NEW APPROACH

IN GAUSSIAN INTEGERS X 3 + Y 3 = Z 3 HAS ONLY TRIVIAL SOLUTIONS A NEW APPROACH INTEGERS: ELECTRONIC JOURNAL OF COMBINATORIAL NUMBER THEORY 8 (2008), #A2 IN GAUSSIAN INTEGERS X + Y = Z HAS ONLY TRIVIAL SOLUTIONS A NEW APPROACH Elis Lmpkis Lmpropoulou (Term), Kiprissi, T.K: 24500,

More information

KRASNOSEL SKII TYPE FIXED POINT THEOREM FOR NONLINEAR EXPANSION

KRASNOSEL SKII TYPE FIXED POINT THEOREM FOR NONLINEAR EXPANSION Fixed Point Theory, 13(2012), No. 1, 285-291 http://www.mth.ubbcluj.ro/ nodecj/sfptcj.html KRASNOSEL SKII TYPE FIXED POINT THEOREM FOR NONLINEAR EXPANSION FULI WANG AND FENG WANG School of Mthemtics nd

More information

Theoretical foundations of Gaussian quadrature

Theoretical foundations of Gaussian quadrature Theoreticl foundtions of Gussin qudrture 1 Inner product vector spce Definition 1. A vector spce (or liner spce) is set V = {u, v, w,...} in which the following two opertions re defined: (A) Addition of

More information

Advanced Calculus: MATH 410 Notes on Integrals and Integrability Professor David Levermore 17 October 2004

Advanced Calculus: MATH 410 Notes on Integrals and Integrability Professor David Levermore 17 October 2004 Advnced Clculus: MATH 410 Notes on Integrls nd Integrbility Professor Dvid Levermore 17 October 2004 1. Definite Integrls In this section we revisit the definite integrl tht you were introduced to when

More information

ADVANCEMENT OF THE CLOSELY COUPLED PROBES POTENTIAL DROP TECHNIQUE FOR NDE OF SURFACE CRACKS

ADVANCEMENT OF THE CLOSELY COUPLED PROBES POTENTIAL DROP TECHNIQUE FOR NDE OF SURFACE CRACKS ADVANCEMENT OF THE CLOSELY COUPLED PROBES POTENTIAL DROP TECHNIQUE FOR NDE OF SURFACE CRACKS F. Tkeo 1 nd M. Sk 1 Hchinohe Ntionl College of Technology, Hchinohe, Jpn; Tohoku University, Sendi, Jpn Abstrct:

More information

Name Solutions to Test 3 November 8, 2017

Name Solutions to Test 3 November 8, 2017 Nme Solutions to Test 3 November 8, 07 This test consists of three prts. Plese note tht in prts II nd III, you cn skip one question of those offered. Some possibly useful formuls cn be found below. Brrier

More information

MATH34032: Green s Functions, Integral Equations and the Calculus of Variations 1

MATH34032: Green s Functions, Integral Equations and the Calculus of Variations 1 MATH34032: Green s Functions, Integrl Equtions nd the Clculus of Vritions 1 Section 1 Function spces nd opertors Here we gives some brief detils nd definitions, prticulrly relting to opertors. For further

More information

ODE: Existence and Uniqueness of a Solution

ODE: Existence and Uniqueness of a Solution Mth 22 Fll 213 Jerry Kzdn ODE: Existence nd Uniqueness of Solution The Fundmentl Theorem of Clculus tells us how to solve the ordinry differentil eqution (ODE) du = f(t) dt with initil condition u() =

More information

PHYS 601 HW3 Solution

PHYS 601 HW3 Solution 3.1 Norl force using Lgrnge ultiplier Using the center of the hoop s origin, we will describe the position of the prticle with conventionl polr coordintes. The Lgrngin is therefore L = 1 2 ṙ2 + 1 2 r2

More information

Recitation 3: More Applications of the Derivative

Recitation 3: More Applications of the Derivative Mth 1c TA: Pdric Brtlett Recittion 3: More Applictions of the Derivtive Week 3 Cltech 2012 1 Rndom Question Question 1 A grph consists of the following: A set V of vertices. A set E of edges where ech

More information

Definition of Continuity: The function f(x) is continuous at x = a if f(a) exists and lim

Definition of Continuity: The function f(x) is continuous at x = a if f(a) exists and lim Mth 9 Course Summry/Study Guide Fll, 2005 [1] Limits Definition of Limit: We sy tht L is the limit of f(x) s x pproches if f(x) gets closer nd closer to L s x gets closer nd closer to. We write lim f(x)

More information

Euler, Ioachimescu and the trapezium rule. G.J.O. Jameson (Math. Gazette 96 (2012), )

Euler, Ioachimescu and the trapezium rule. G.J.O. Jameson (Math. Gazette 96 (2012), ) Euler, Iochimescu nd the trpezium rule G.J.O. Jmeson (Mth. Gzette 96 (0), 36 4) The following results were estblished in recent Gzette rticle [, Theorems, 3, 4]. Given > 0 nd 0 < s

More information

Physics 116C Solution of inhomogeneous ordinary differential equations using Green s functions

Physics 116C Solution of inhomogeneous ordinary differential equations using Green s functions Physics 6C Solution of inhomogeneous ordinry differentil equtions using Green s functions Peter Young November 5, 29 Homogeneous Equtions We hve studied, especilly in long HW problem, second order liner

More information

Math 520 Final Exam Topic Outline Sections 1 3 (Xiao/Dumas/Liaw) Spring 2008

Math 520 Final Exam Topic Outline Sections 1 3 (Xiao/Dumas/Liaw) Spring 2008 Mth 520 Finl Exm Topic Outline Sections 1 3 (Xio/Dums/Liw) Spring 2008 The finl exm will be held on Tuesdy, My 13, 2-5pm in 117 McMilln Wht will be covered The finl exm will cover the mteril from ll of

More information

Frobenius numbers of generalized Fibonacci semigroups

Frobenius numbers of generalized Fibonacci semigroups Frobenius numbers of generlized Fiboncci semigroups Gretchen L. Mtthews 1 Deprtment of Mthemticl Sciences, Clemson University, Clemson, SC 29634-0975, USA gmtthe@clemson.edu Received:, Accepted:, Published:

More information

1 Probability Density Functions

1 Probability Density Functions Lis Yn CS 9 Continuous Distributions Lecture Notes #9 July 6, 28 Bsed on chpter by Chris Piech So fr, ll rndom vribles we hve seen hve been discrete. In ll the cses we hve seen in CS 9, this ment tht our

More information

MATH 144: Business Calculus Final Review

MATH 144: Business Calculus Final Review MATH 144: Business Clculus Finl Review 1 Skills 1. Clculte severl limits. 2. Find verticl nd horizontl symptotes for given rtionl function. 3. Clculte derivtive by definition. 4. Clculte severl derivtives

More information

NOTE ON TRACES OF MATRIX PRODUCTS INVOLVING INVERSES OF POSITIVE DEFINITE ONES

NOTE ON TRACES OF MATRIX PRODUCTS INVOLVING INVERSES OF POSITIVE DEFINITE ONES Journl of pplied themtics nd Computtionl echnics 208, 7(), 29-36.mcm.pcz.pl p-issn 2299-9965 DOI: 0.752/jmcm.208..03 e-issn 2353-0588 NOE ON RCES OF RIX PRODUCS INVOLVING INVERSES OF POSIIVE DEFINIE ONES

More information

TANDEM QUEUE WITH THREE MULTISERVER UNITS AND BULK SERVICE WITH ACCESSIBLE AND NON ACCESSBLE BATCH IN UNIT III WITH VACATION

TANDEM QUEUE WITH THREE MULTISERVER UNITS AND BULK SERVICE WITH ACCESSIBLE AND NON ACCESSBLE BATCH IN UNIT III WITH VACATION Indin Journl of Mthemtics nd Mthemticl Sciences Vol. 7, No., (June ) : 9-38 TANDEM QUEUE WITH THREE MULTISERVER UNITS AND BULK SERVICE WITH ACCESSIBLE AND NON ACCESSBLE BATCH IN UNIT III WITH VACATION

More information

Math 360: A primitive integral and elementary functions

Math 360: A primitive integral and elementary functions Mth 360: A primitive integrl nd elementry functions D. DeTurck University of Pennsylvni October 16, 2017 D. DeTurck Mth 360 001 2017C: Integrl/functions 1 / 32 Setup for the integrl prtitions Definition:

More information

State space systems analysis (continued) Stability. A. Definitions A system is said to be Asymptotically Stable (AS) when it satisfies

State space systems analysis (continued) Stability. A. Definitions A system is said to be Asymptotically Stable (AS) when it satisfies Stte spce systems nlysis (continued) Stbility A. Definitions A system is sid to be Asymptoticlly Stble (AS) when it stisfies ut () = 0, t > 0 lim xt () 0. t A system is AS if nd only if the impulse response

More information

Lecture 13 - Linking E, ϕ, and ρ

Lecture 13 - Linking E, ϕ, and ρ Lecture 13 - Linking E, ϕ, nd ρ A Puzzle... Inner-Surfce Chrge Density A positive point chrge q is locted off-center inside neutrl conducting sphericl shell. We know from Guss s lw tht the totl chrge on

More information

Chapters 4 & 5 Integrals & Applications

Chapters 4 & 5 Integrals & Applications Contents Chpters 4 & 5 Integrls & Applictions Motivtion to Chpters 4 & 5 2 Chpter 4 3 Ares nd Distnces 3. VIDEO - Ares Under Functions............................................ 3.2 VIDEO - Applictions

More information

ARITHMETIC OPERATIONS. The real numbers have the following properties: a b c ab ac

ARITHMETIC OPERATIONS. The real numbers have the following properties: a b c ab ac REVIEW OF ALGEBRA Here we review the bsic rules nd procedures of lgebr tht you need to know in order to be successful in clculus. ARITHMETIC OPERATIONS The rel numbers hve the following properties: b b

More information

Math Calculus with Analytic Geometry II

Math Calculus with Analytic Geometry II orem of definite Mth 5.0 with Anlytic Geometry II Jnury 4, 0 orem of definite If < b then b f (x) dx = ( under f bove x-xis) ( bove f under x-xis) Exmple 8 0 3 9 x dx = π 3 4 = 9π 4 orem of definite Problem

More information

Main topics for the First Midterm

Main topics for the First Midterm Min topics for the First Midterm The Midterm will cover Section 1.8, Chpters 2-3, Sections 4.1-4.8, nd Sections 5.1-5.3 (essentilly ll of the mteril covered in clss). Be sure to know the results of the

More information

Credibility Hypothesis Testing of Fuzzy Triangular Distributions

Credibility Hypothesis Testing of Fuzzy Triangular Distributions 666663 Journl of Uncertin Systems Vol.9, No., pp.6-74, 5 Online t: www.jus.org.uk Credibility Hypothesis Testing of Fuzzy Tringulr Distributions S. Smpth, B. Rmy Received April 3; Revised 4 April 4 Abstrct

More information

arxiv: v1 [math.st] 26 Apr 2018

arxiv: v1 [math.st] 26 Apr 2018 On Mesuring the Vribility of Sll Are Estitors in Multivrite Fy-Herriot Model rxiv:1804.09941v1 th.st 26 Apr 2018 Tsubs Ito nd Ttsuy Kubokw Abstrct This pper is concerned with the sll re estition in the

More information

1 The Lagrange interpolation formula

1 The Lagrange interpolation formula Notes on Qudrture 1 The Lgrnge interpoltion formul We briefly recll the Lgrnge interpoltion formul. The strting point is collection of N + 1 rel points (x 0, y 0 ), (x 1, y 1 ),..., (x N, y N ), with x

More information

Riemann Sums and Riemann Integrals

Riemann Sums and Riemann Integrals Riemnn Sums nd Riemnn Integrls Jmes K. Peterson Deprtment of Biologicl Sciences nd Deprtment of Mthemticl Sciences Clemson University August 26, 203 Outline Riemnn Sums Riemnn Integrls Properties Abstrct

More information

Tests for the Ratio of Two Poisson Rates

Tests for the Ratio of Two Poisson Rates Chpter 437 Tests for the Rtio of Two Poisson Rtes Introduction The Poisson probbility lw gives the probbility distribution of the number of events occurring in specified intervl of time or spce. The Poisson

More information

A REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H. Thomas Shores Department of Mathematics University of Nebraska Spring 2007

A REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H. Thomas Shores Department of Mathematics University of Nebraska Spring 2007 A REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H Thoms Shores Deprtment of Mthemtics University of Nebrsk Spring 2007 Contents Rtes of Chnge nd Derivtives 1 Dierentils 4 Are nd Integrls 5 Multivrite Clculus

More information

AN ORIGINAL METHOD FOR URBAN TRAFFIC NOISE PREDICTION

AN ORIGINAL METHOD FOR URBAN TRAFFIC NOISE PREDICTION AN ORIGINA METHOD FOR URBAN TRAFFIC NOISE REDICTION Federico Rossi 1, Uberto Di Mtteo, Sofi Sioni 3 1 University of erugi Industril Engineering Deprtent oc. enti Bss 1, 05100, Terni, Itly frossi@unipg.it

More information

approaches as n becomes larger and larger. Since e > 1, the graph of the natural exponential function is as below

approaches as n becomes larger and larger. Since e > 1, the graph of the natural exponential function is as below . Eponentil nd rithmic functions.1 Eponentil Functions A function of the form f() =, > 0, 1 is clled n eponentil function. Its domin is the set of ll rel f ( 1) numbers. For n eponentil function f we hve.

More information

Math Lecture 23

Math Lecture 23 Mth 8 - Lecture 3 Dyln Zwick Fll 3 In our lst lecture we delt with solutions to the system: x = Ax where A is n n n mtrix with n distinct eigenvlues. As promised, tody we will del with the question of

More information

8 Laplace s Method and Local Limit Theorems

8 Laplace s Method and Local Limit Theorems 8 Lplce s Method nd Locl Limit Theorems 8. Fourier Anlysis in Higher DImensions Most of the theorems of Fourier nlysis tht we hve proved hve nturl generliztions to higher dimensions, nd these cn be proved

More information

Riemann Sums and Riemann Integrals

Riemann Sums and Riemann Integrals Riemnn Sums nd Riemnn Integrls Jmes K. Peterson Deprtment of Biologicl Sciences nd Deprtment of Mthemticl Sciences Clemson University August 26, 2013 Outline 1 Riemnn Sums 2 Riemnn Integrls 3 Properties

More information

Research Article Moment Inequalities and Complete Moment Convergence

Research Article Moment Inequalities and Complete Moment Convergence Hindwi Publishing Corportion Journl of Inequlities nd Applictions Volume 2009, Article ID 271265, 14 pges doi:10.1155/2009/271265 Reserch Article Moment Inequlities nd Complete Moment Convergence Soo Hk

More information

Before we can begin Ch. 3 on Radicals, we need to be familiar with perfect squares, cubes, etc. Try and do as many as you can without a calculator!!!

Before we can begin Ch. 3 on Radicals, we need to be familiar with perfect squares, cubes, etc. Try and do as many as you can without a calculator!!! Nme: Algebr II Honors Pre-Chpter Homework Before we cn begin Ch on Rdicls, we need to be fmilir with perfect squres, cubes, etc Try nd do s mny s you cn without clcultor!!! n The nth root of n n Be ble

More information

Infinite Geometric Series

Infinite Geometric Series Infinite Geometric Series Finite Geometric Series ( finite SUM) Let 0 < r < 1, nd let n be positive integer. Consider the finite sum It turns out there is simple lgebric expression tht is equivlent to

More information

Best Approximation in the 2-norm

Best Approximation in the 2-norm Jim Lmbers MAT 77 Fll Semester 1-11 Lecture 1 Notes These notes correspond to Sections 9. nd 9.3 in the text. Best Approximtion in the -norm Suppose tht we wish to obtin function f n (x) tht is liner combintion

More information

LYAPUNOV-TYPE INEQUALITIES FOR THIRD-ORDER LINEAR DIFFERENTIAL EQUATIONS

LYAPUNOV-TYPE INEQUALITIES FOR THIRD-ORDER LINEAR DIFFERENTIAL EQUATIONS Electronic Journl of Differentil Equtions, Vol. 2017 (2017), No. 139, pp. 1 14. ISSN: 1072-6691. URL: http://ejde.mth.txstte.edu or http://ejde.mth.unt.edu LYAPUNOV-TYPE INEQUALITIES FOR THIRD-ORDER LINEAR

More information

THE EXISTENCE-UNIQUENESS THEOREM FOR FIRST-ORDER DIFFERENTIAL EQUATIONS.

THE EXISTENCE-UNIQUENESS THEOREM FOR FIRST-ORDER DIFFERENTIAL EQUATIONS. THE EXISTENCE-UNIQUENESS THEOREM FOR FIRST-ORDER DIFFERENTIAL EQUATIONS RADON ROSBOROUGH https://intuitiveexplntionscom/picrd-lindelof-theorem/ This document is proof of the existence-uniqueness theorem

More information

How can we approximate the area of a region in the plane? What is an interpretation of the area under the graph of a velocity function?

How can we approximate the area of a region in the plane? What is an interpretation of the area under the graph of a velocity function? Mth 125 Summry Here re some thoughts I ws hving while considering wht to put on the first midterm. The core of your studying should be the ssigned homework problems: mke sure you relly understnd those

More information

Math 113 Exam 1-Review

Math 113 Exam 1-Review Mth 113 Exm 1-Review September 26, 2016 Exm 1 covers 6.1-7.3 in the textbook. It is dvisble to lso review the mteril from 5.3 nd 5.5 s this will be helpful in solving some of the problems. 6.1 Are Between

More information

The steps of the hypothesis test

The steps of the hypothesis test ttisticl Methods I (EXT 7005) Pge 78 Mosquito species Time of dy A B C Mid morning 0.0088 5.4900 5.5000 Mid Afternoon.3400 0.0300 0.8700 Dusk 0.600 5.400 3.000 The Chi squre test sttistic is the sum of

More information

NONLINEAR CONSTANT LIFE MODEL FOR FATIGUE LIFE PREDICTION OF COMPOSITE MATERIALS

NONLINEAR CONSTANT LIFE MODEL FOR FATIGUE LIFE PREDICTION OF COMPOSITE MATERIALS 18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS NONLINEAR CONSTANT LIFE MODEL FOR FATIGUE LIFE PREDICTION OF COMPOSITE MATERIALS T. Prk 1, M. Ki 1, B. Jng 1, J. Lee 2, J. Prk 3 * 1 Grdute School,

More information

AQA Further Pure 1. Complex Numbers. Section 1: Introduction to Complex Numbers. The number system

AQA Further Pure 1. Complex Numbers. Section 1: Introduction to Complex Numbers. The number system Complex Numbers Section 1: Introduction to Complex Numbers Notes nd Exmples These notes contin subsections on The number system Adding nd subtrcting complex numbers Multiplying complex numbers Complex

More information

Formulae For. Standard Formulae Of Integrals: x dx k, n 1. log. a dx a k. cosec x.cot xdx cosec. e dx e k. sec. ax dx ax k. 1 1 a x.

Formulae For. Standard Formulae Of Integrals: x dx k, n 1. log. a dx a k. cosec x.cot xdx cosec. e dx e k. sec. ax dx ax k. 1 1 a x. Forule For Stndrd Forule Of Integrls: u Integrl Clculus By OP Gupt [Indir Awrd Winner, +9-965 35 48] A B C D n n k, n n log k k log e e k k E sin cos k F cos sin G tn log sec k OR log cos k H cot log sin

More information

Math 1B, lecture 4: Error bounds for numerical methods

Math 1B, lecture 4: Error bounds for numerical methods Mth B, lecture 4: Error bounds for numericl methods Nthn Pflueger 4 September 0 Introduction The five numericl methods descried in the previous lecture ll operte by the sme principle: they pproximte the

More information

Families of Solutions to Bernoulli ODEs

Families of Solutions to Bernoulli ODEs In the fmily of solutions to the differentil eqution y ry dx + = it is shown tht vrition of the initil condition y( 0 = cuses horizontl shift in the solution curve y = f ( x, rther thn the verticl shift

More information

Title: Robust statistics from multiple pings improves noise tolerance in sonar.

Title: Robust statistics from multiple pings improves noise tolerance in sonar. Title: Robust sttistics fro ultiple pings iproves noise tolernce in sonr. Authors: Nicol Neretti*, Nthn Intrtor, Leon N Cooper This work ws supported in prt by ARO (DAAD 9---43), nd ONR (N--C- 96). N.

More information

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER /2019

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER /2019 ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS MATH00030 SEMESTER 208/209 DR. ANTHONY BROWN 7.. Introduction to Integrtion. 7. Integrl Clculus As ws the cse with the chpter on differentil

More information

Review of Riemann Integral

Review of Riemann Integral 1 Review of Riemnn Integrl In this chpter we review the definition of Riemnn integrl of bounded function f : [, b] R, nd point out its limittions so s to be convinced of the necessity of more generl integrl.

More information