Box-Particle Labeled Multi-Bernoulli Filter for Multiple Extended Target Tracking

Size: px
Start display at page:

Download "Box-Particle Labeled Multi-Bernoulli Filter for Multiple Extended Target Tracking"

Transcription

1 RADIOENGINEERING, VOL. 5, NO. 3, SEPTEBER Bo-Patcle Labeled ult-benoull Flte fo ultle Etended Taget Tacng ao LI, Zang LIN, We AN, Yyu ZHOU ollege of Electonc Scence and Engneeng, Natonal Unvesty of Defense Technology, No. 09, Deya Road, hangsha, P. R. hna anusct eceved anuay, 06 Abstact. Ths ae focuses on eal-tme tacng of multle etended tagets n clutte based on labeled mult- Benoull flte. To addess ths oblem, a novel aoach s oosed wthn the ecently esented bo-atcle famewo. Unle the tadtonal ont-atcle aoach, the measuements of etended tagets ae modeled as nteval measuements n ths wo, and the coesondng lelhood functon s gven based on nteval analyss. Then, labeled mult-benoull ecuson fo etended tagets s mlemented by bo atcles, efeed to as BP-LB flte. Futhemoe, BP--LB flte s oosed to bette accommodate the uncetanty of taget dynamcs by ntegatng the BP-LB flte wth nteactng multle models (I) algothm. Smulatons demonstate that the oosed aoach can sgnfcantly educe the numbe of atcles and well tac multle etended tagets wth less untme. Keywods Bo atcle, labeled mult-benoull, mult-taget tacng, etended taget, nteactng multle models.. Intoducton Standad tacng algothms assume that one taget geneates at most one ont measuement. Howeve, n many actcal stuatons ths assumton s not aoate [], []. Due to the nceasng esoluton of ada and otcal sensos, one taget may oduce multle ont measuements. Such taget s efeed to as etended taget. Etended taget tacng s a evalent tas. Recently, the andom-fnte-set (RFS) based mult-taget tacng algothms have attacted etensve attenton [3]. Based on RFS famewo, the obablty hyothess densty (PHD), adnalzed PHD (PHD) and mult-taget mult-benoull (ebe) fltes have been oosed [4 6]. Howeve, these fltes only ovde unlabeled estmates at each tme, and addtonal ost-ocessng s needed to fom taget tacs. To ovecome the ssue, the labeled RFS s ntoduced n [7] by augmentng the state of each taget wth a tac label. Subsequently, the Genealzed Labeled ult-benoull (GLB) and the δ-glb RFS wee oosed as the secfc subclasses of labeled RFS [8]. As an accuate and comutatonally effcent aomaton of the δ-glb flte, the labeled ult-benoull (LB) flte has been oosed n [9]. Both Gaussan tues (G) and sequental onte alo (S) technques have been mlemented fo these RFS based fltes [6], [0]. The tadtonal S s caed out by ont atcles (PP). The G mlementaton s constaned to lnea Gaussan scenaos, and the S mlementaton can be aled to some nonlnea non-gaussan scenaos. Howeve, n many actcal alcatons, the tagets usually ehbt stong maneuve, and the combnaton of nteactng multle models (I) algothm and RFS based flte s adoted to coe wth such adly maneuveng tagets []. In the I algothm, multle sngle-model fltes ae needed. onsequently, the tadtonal S mlementaton s comutatonally eensve, esecally when the numbe of tagets s lage o the I algothm s adoted. Ths motvates us to seach fo comutatonally cheae altenatves. Fo nteval measuements, the bo-atcle (BP) aoach has a otental to sgnfcantly educe comutatonal cost []. Thus, we focus on tacng multle etended tagets by bo-atcle aoach n ths wo. In tacng alcatons, the measuements may be affected by thee souces of uncetanty: stochastc, data assocaton and settheoetc uncetanty [3], [4]. The uncetanty ognatng fom andom nose s efeed to as statstcal uncetanty. The data assocaton uncetanty s the uncetanty as to whch measuements ae coesondng to the taget. Tadtonal tacng algothms, such as PHD flte and LB flte, have been desgned based on both stochastc and assocaton uncetanty. Howeve, they gnoe the effect bought by set-theoetc uncetanty. Because of unnown bases and othe easons, nteval measuements, athe than tadtonal ont measuements, can be usually obtaned. The bo-atcle aoach based on the nteval analyss famewo can well accommodate above tle uncetanty. In the Bayesan esectve, bo atcles can be nteeted as suots of unfom obablty densty functons (PDF). DOI: 0.364/e SIGNALS

2 58. LI, Z. LIN, W. AN, ET AL., BOX-PARTILE LABELED ULTI-BERNOULLI FILTER FOR ULTIPLE EXTENDED TARGET In fact, the nteval measuements ae common fo etended tagets. An etended taget can geneate seveal ont measuements based on Posson model, and they andomly dstbute aound the cente of taget etent []. onsequently, the unambguous oston coodnates of taget cente cannot be etacted. On the contay, the nteval measuements o ambguous taget egons ae avalable. In ths ae, we aly bo-atcle aoach to mlement the LB ecuson fo etended tagets. Fstly, the nteval measuement model of etended taget s modeled, and the lelhood functon wthn nteval analyss famewo s gven. Secondly, the bo-atcle mlementaton of LB flte fo lnea etended tagets (BP-LB flte) s deved. Then, to bette accommodate maneuveng etended tagets, the BP-LB flte and nteactng multle models (I) algothm ae combned, and BP--LB flte s oosed. Smulatons demonstate that the oosed aoach can each smla accuacy wth consdeably less comutatonal costs n comason wth ont-atcle aoach. The emande of the ae s oganzed as follows: Secton evews the theoes of Posson model of etended taget, LB flte and nteval analyss. Secton 3 ooses the BP-LB flte and BP--LB flte. The esults and analyss of the eements ae manly esented n Secton 4. Secton 5 daws conclusons.. Bacgound Ths secton ovdes a bef evew of Posson model of etended taget, LB flte and nteval analyss. oe detals can be found n [], [9], [].. Posson odel of Etended Taget In the mult-taget tacng scenao, the tacng s often efomed on ont measuements afte theshold segmentaton. The taget measuement set of etended taget s usually modeled by Posson model. The cadnalty dstbuton s [] n n e () n! whee s the mean numbe of ont measuements. The ont measuements ognatng fom the etended taget can be andomly dawn fom Gauss satal dstbuton aound taget cente.. LB Flte A mult-benoull RFS X can be seen as a unon of some ndeendent Benoull RFSs,.e. X,. Hee, and eesent the estence obablty and satal dstbuton of sngle taget, esectvely. In LB flte, a label s aended to sngle-taget state to enable the estmaton of a taget tac. Labeled sngle-taget state and mult-taget state ae denoted by and X, esectvely. The ecuson of LB flte s caed out on as follows [9]. ) Pedcton: Assume that the aamete set of osteo mult-taget densty at tme s gven by π,. The state sace and label sace. The edcted mult- ae eesented by and taget LB RFS aamete set s gven as + +P, +P, B B π,,. () The fst tem n () eesents suvvng tagets and the second one denotes bth tagets. s the label sace of bth tagets. The estence obabltes and satal dstbutons of suvvng tagets ae calculated as +P, P +P, S,,, P, (3) f, (4) P S,, (5) whee the suvval obablty of the tac s eesented by S (, ), and f, denotes the sngle-taget aov tanston densty. The aamete set of bth tagets s gven by bth model [9]. ) Udate: The label sace afte edcton ncludes two ats: suvvng tagets and bth tagets, so. The edcted LB aamete set s ewtten as a unfom LB aamete set as followng π,. (6) The LB flte s an aomaton of the δ-glb flte, and ts measuement udate s stll caed out n the aoach of δ-glb. To facltate the δ-glb udate, the edcted LB RFS s conveted nto an equvalent δ-glb fom,.e. X X X, (7) X L L, (8), (9) whee eesents the oecton fom the labeled state sace to the label sace, and X X. Befoe udate, measuement set attonng s needed fo etended taget tacng, whch attons ont measuement set nto multle subsets. A well-nown atton- X

3 RADIOENGINEERING, VOL. 5, NO. 3, SEPTEBER ng method s the dstance atton. It s caed out based on the fundamental nsght that measuements fom the same etended taget ae satally close to each othe [5]. In atcle alcatons, the dstance theshold can be set based on o nowledge, and then the most lely ones among all of the ossble attons ae adoted n measuement udate. Aftewads, the udated estence obabltes and satal dstbutons can be comuted by: I, ZI I, I I,, (0) I,, ZI I () whee I eesents the sace of mangs fom tac label to measuement, and : I 0,,, Z. Y X s nclude ndcato functon [9]..3 Inteval Analyss easuements wth bounded eos can be convenently modeled as nteval measuements. To facltate the ocessng of nteval measuements, the tool of nteval analyss has been develoed []. A eal nteval s defned as a closed and connected subset,.e.,. The and eesent esectvely the lowe bound and ue bound. Fo the case wth mult-dmensonal states, the nteval s egaded as a bo. Bo s defned as a atesan oduct of multle ntevals,.e. d, whee d s the numbe of dmensons. Afte a nonlnea oagaton, the esult of the oagaton may not be a bo. To coe wth ths ssue, ncluson functons ae necessay. Let f be a functon fom n m n m to. An nteval functon f fom to s sad to be an ncluson functon fo f, f f f, functon s usually adoted [], [6]. n. In the contet of tacng, natual ncluson The contacton s anothe motant concet fo boatcle aoach, whch s used n the calculaton of lelhood functon as gven n Sec. 3.. A onstant Satsfacton Poblem (SP) can be denoted by g =0,. () In shot, equaton () means fndng the smallest bo to elace ognal unde the constant. The onstant Poagaton (P) has bette sutablty n comason wth othe methods. Thus, the P method has been wdely used n many tacng alcatons [4], [6]. 3. Bo-Patcle Imlementatons 3. Inteval easuement odel and Lelhood Functon Fo a two-dmensonal case, the sngle-taget state can be descbed by nteval state vecto as,, y, y, and (3) whee y ae the oston ntevals of the taget cente, and y ae the coesondng velocty ntevals. Fo an etended taget, some ont measuements aound taget cente can be obtaned afte theshold segmentaton,.e. Z, y. Hee, the tem ee- sents the numbe of ont measuements ognatng fom the etended taget, and and y ae the oston coodnates of the th ont measuement. As ntoduced n Sec.., the s subect to Posson dstbuton. Obvously, the ecse cente of taget etent cannot be dectly obtaned. Howeve, the nteval at whch the taget cente z z, z z and locates s avalable,.e.. The z y ae nteval measuements of taget cente n -decton and y-decton, esectvely. In ths wo, they ae comuted by z, y, (4) z y y y, y (5) whee and y ae the estmated oston coodnates of taget cente, and y descbe the sze of nteval. They ae comuted by: y mean, (6) mean y, (7) ma, (8) ma y y y. (9) Fo convenence, the above ocessng, fom ont measuement set to one nteval measuement, s denoted z I Z. by The measuement lelhood functon g (z) s equed by Bayes-le fltes. Ths s also tue fo bo-at- T

4 530. LI, Z. LIN, W. AN, ET AL., BOX-PARTILE LABELED ULTI-BERNOULLI FILTER FOR ULTIPLE EXTENDED TARGET cle flte. In the contet of ths ae, the measuement lelhood fo nteval measuement z s gven as z, z hp g (0) whee the functon hp, z etuns a contacted veson of. In ths wo, the dectly measued comonents ae contacted based on nteval measuements,.e. z, y y z y. The unmeasued comonents, and y, ae contacted based on o nowledge. = y y whee denotes the volume of nteval. 3. BP-LB Flte In ths subsecton, the bo-atcle mlement of LB flte s deved n detal, whch s efeed to as BP-LB flte n ths ae. In classcal LB flte, the satal dstbuton () s aomated usng a set of weghted ont atcles as () whee denotes the Dac delta functon concentated at, s the numbe of ont atcles, and eesents the weght of the th ont atcle. In bo atcle aoach, bo atcles ae nteeted as suots of unfom PDF, then equaton () s ewtten as: U () whee U eesents the unfom PDF ove the bo. The detals about BP-LB ecuson ae esented as followng. ) Pedcton: Suose that the osteo mult-taget densty at s an LB RFS wth aamete set π,, s aomated by a set of weghted bo atcles,,,, U,,.e. (3) whee s the numbe of bo atcles of tac at tme. The edcted LB densty conssts of suvvng etended tagets and bth etended tagets n (). In the BP-LB flte, the aamete set of suvvng etended tagets can be calculated by whee,, P S,, P, P U,, P =, (4), (5),, +, P f, (6),,,, P S S =. (7) The suvval obablty S s assumed to be state ndeendent. The outut of f s a bo contanng f. The aamete set of bth etended tagets ae gven by bth model n Sec. 4.. ) Udate: Afte edcton, the unfom mult-taget densty π, s gven, and each s aomated by a set of bo atcles, U,,,,,.e.. (8) Then, the equvalent δ-glb fom s obtaned by (7 to 9). Based on dstance atton as ntoduced n Sec.., the ont measuement set s dvded nto dsonted subsets, N n n.e. Z Z, sub. Z sub, eesents the nth subset and t n n conssts of some ont measuements,.e. Z n,m n,m, y n m sub,. The dstance theshold Th a used n dstance atton s secfed a o. Then, subsets ae conveted nto nteval measuements usng the method n- N n toduced n Sec. 3.,.e. Z z whee z n n I Z, sub. The udate usng the nteval measuement set s gven by I, I, I I, I ZI I I n,, Z, (9) Z. (30) The weghts and the satal dstbutons ae calculated by I, I Z Z I, (3)

5 RADIOENGINEERING, VOL. 5, NO. 3, SEPTEBER Z,, U, (3),,, h P, z, (33) Z,,, Z Z ;, (34),, Z ;, (35), Dg z, ;,f 0 (36) qd, f 0 whee g z s the nteval measuement lelhood and has been gven as (0). denotes the clutte densty, and the clutte s modeled as Posson model [9]. D eesents the detecton obablty, t s state ndeendent, and q. D D 3) Resamlng: Smla to the tadtonal ont-atcle aoach, the esamlng ste s necessay fo the boatcle aoach to event degeneacy of bo atcles. Howeve, nstead of elcatng bo atcles wth lage osteo weghts, we atton them nto multle sub boes. These sub boes ae equally weghted. onsequently, the esoluton n the egons of state sace can be efned, and taget state ntevals can be contacted. In ths wo, we andomly c a dmenson to be dvded fo the selected bo-atcle []. In addton, the unng, megng and state etacton ae smla to those n [4]. Punng of hyotheszed tacs means that the tacs wth estence obabltes below the theshold Th del wll be deleted. Two tacs wthn a dstance theshold Th me wll be meged. A taget s declaed esent only f the estence obablty s geate than theshold Th Ta. Fnally, the mult-taget state can be etacted by whee atcle.,, md (37) md eesents fndng the cente of the bo 3.3 BP--LB Flte To bette accommodate maneuveng etended tagets, BP--LB flte s oosed by ntegatng the BP- LB flte wth I algothm. To deve the BP--LB flte, s ntoduced to denote sngle moton model. The state of sngle etended taget s consequently eesented by,. The moton model of the taget s usually egaded as a aov chan wth tanston obablty mat H h st [7]. Fo eamle, hst t s denotes the obablty that a taget swtches fom model s to model t, whee st, and h t st. The tem s the numbe of moton models. In essence, the BP--LB flte conssts of a fnte numbe of sngle-model BP-LB fltes coesondng to dffeent moton models. In addton to those stes n BP- LB flte, mng ste s addtonally equed [8]. The othe stes ae smla to BP-LB flte, and the mng ste of BP--LB flte s gven as follows. Assume that at tme the mult-taget osteo densty s π,,, and each s aomated by a set of augmented bo atcles,,,,,.e., U,,. (38), Then, the med LB aamete set can be eessed by: π,,. (39) Snce the model tanston s only decded by model tanston obablty and s ndeendent of the state tanston,, t can be comuted by, s s s t,, t s,, t s s st h Theefoe,, s. τ t, s aomated by (40),,, h,,,, t t. (4) It can be found that much moe atcles ae needed and the numbe of atcles afte mng fo tac s nceased to. Thus, comutatonally cheae mlementaton s motant fo maneuveng taget tacng. Subsequently, the edcton and udate ae caed out based on augmented bo atcles. Note that the augmented sngle-taget state tanston densty s f,, h f.

6 53. LI, Z. LIN, W. AN, ET AL., BOX-PARTILE LABELED ULTI-BERNOULLI FILTER FOR ULTIPLE EXTENDED TARGET 4. Numecal Studes 4. Smulaton Setu The smulaton esults ae dvded nto two ats: Fstly, multle lnea etended tagets ae taced by the oosed BP-LB flte and the tadtonal ont-atcle LB flte (PP-LB flte) [], [9]. Secondly, the BP- -LB flte s comaed wth the sngle-model BP- LB flte (BP-V-LB flte) and mult-model PP-LB flte (PP--LB flte) n the scenao contanng multle adly maneuveng etended tagets. onsde a D suvellance egon n the atesan coodnates, secfed by the lowe-left cone (, ) and ue-ght cone (5, 5). Each sequence has 30 fames and eod s T = s. Thee ae thee etended tagets n each sequence, and they ae embedded nto each sequence as Posson model. The aveage numbe of taget ont measuements s 8. The aveage numbe of clutte measuements s 0 n each fame. In the fst eement, thee tagets all move at a constant velocty (V) model n the suvellance egon. Howeve, the tagets may move at a constant velocty model o a coodnated tun (T) model n the second eement. Smla to classcal LB flte, the bth ocess s modeled as a mult Benoull RFS [9],.e. π,, 0.06, U. 3 B B B B B B Tang the Taget as an eamle, and the ntal taget state vecto s 385, 399,[ B 5,5],[55,69],[ 5,5]. (4) The velocty vecto s contacted based on o dstbuton. In ths wo, t follows a unfom PDF,.e. 5, 5 5,5 y 5, 5 5,5. and The state tanston functons of V model and T model ae descbed by (43) and (44) [8]. The tun ate of T model n the second eement s set to Ω = 0.8 ad. f T f V T T sn T cos 0 0 cost 0 snt cost snt 0 0 snt 0 cost T (43) (44) The statstcal efomance of the algothm s evaluated usng the Otmal Sub-Patten Assgnment (OSPA) metc [9], because t ontly catues dffeences n cadnalty and ndvdual elements between two fnte sets n a mathematcally consstent yet ntutvely meanngful way. Then, fo, c 0, X,, m and Y y,, yn, f m n, d If m > n, c c X, Y mn n n c m c d, y. (45) c c nm d X, Y d Y, X. If m = n =0, d X, Y 0. We use the aametes c = 50 and = n ths wo. Some aametes used n LB ecuson ae lsted n Tab.. Tha Vaable S D Th me Th del ThTa Value Tab.. Paametes of LB ecuson. 4. Tacng ultle Lnea Etended Tagets In ths eement, thee ae thee etended tagets n ths scenao, and they all move at a V model. The tycal ont measuements ognatng fom the Taget ae gven n Fg.. The tue taget tacs ae shown n Fg.. Taget, Taget and Taget 3 ae bon at s, 0 s and 0 s, esectvely. The tacng esults obtaned fom PP-LB flte and the oosed BP-LB flte fo a sngle un s also gven n Fg.. It can be seen that two fltes can successfully tac thee lnea etended tagets. To ovde a efomance comason n sense of statstcal evaluaton, the aveage cadnalty and aveage OPSA dstance ove 50 onte alo uns ae shown n Fg. 3 and Fg. 4, esectvely (a) Fame (c) Fame (b) Fame (d) Fame5 Fg.. The ont measuements of Taget at dffeent fames n the fst eement.

7 RADIOENGINEERING, VOL. 5, NO. 3, SEPTEBER Taget Taget Taget3 tue tacs PP-LB BP-LB Fo RFS based algothms, the cadnalty means the numbe of estmated tagets. The OSPA dstance s a oe metc, whch enalzes both the cadnalty eo and the eo n the state sace. As shown n Fg. 3, both PP-LB flte and BP-LB flte can accuately estmate cadnalty. Howeve, the oosed BP-LB flte can acheve moe accuate state estmaton. The OSPA ea aeas at about 0 s, because of bth tagets. As shown n Tab., 40 bo atcles ae enough fo each tac n the oosed BP-LB flte. Howeve, PP-LB flte eques 000 ont atcles. The numbe of atcles needed fo BP-LB flte s much smalle than that of PP-LB flte. As a esult, the aveage untme of BP-LB flte s much less than that of PP-LB flte. It oves the oosed BP- LB flte can emaably deceases the untme fo multle lnea etended tagets Fg.. The tue tacs and tacng esults n the fst eement. adnalty 4 3 eal numbe PP-LB BP-LB Tme Fg. 3. adnalty statstcs fo PP-LB and BP-LB fltes n the fst eement. OSPA 6 4 PP-LB BP-LB Tme Fg. 4. Aveage OSPA dstances fo PP-LB and BP-LB fltes n the fst eement. Flte Paamete PP-LB BP-LB Suvvng atcle numbe Newbon atcle numbe 000 Runtme (sec) Tab.. Aveage untme and the numbe of atcles fo PP-LB and BP-LB fltes n the fst eement. 4.3 Tacng ultle aneuveng Etended Tagets In ths eement, tue taget tacs ae shown n Fg. 5. Thee ae two hghly maneuveng etended tagets and one lnea etended taget n ths scenao. Fo eamle, Taget s bon at s and des at 30 s. It fstly moves at V model fom s to 9 s, then eecutes T model fom the 0 s to s, and fnally moves at V model fom 3 s to end. The motons of the tagets ae summazed n Tab. 3. Let denote the V model and denote the T model. The ntal moton models ae set to V. The model tanston mat s set to H (46) The tacng esults obtaned fom PP--LB, BP-V-LB and BP--LB fltes fo a sngle un ae also shown n Fg. 5. When the moton model swtch occus, the sngle-model flte fals to catue the tagets. Howeve, the PP--LB flte and BP--LB flte can well accommodate taget maneuve. The aveage cadnalty and the aveage OPSA dstance ove 50 onte alo uns ae dected n Fg. 6 and 7. BP-V-LB flte yelds lage cadnalty eo at 0 s to 0 s and 6 s-30 s due to taget maneuve. Futhemoe, thee ae hgh eas n OSPA metc whee the estmated cadnalty s ncoect. It oves that sngle-model flte s not enough to tac adly maneuveng etended tagets. Taget Bon tme De tme Taget s 30 s Taget 0 s 30 s V moton s-9 s, 3 s-30 s s-5 s, 9 s-30 s Taget 3 0 s 30 s s-30 s T moton 0 s- s 6 s-8 s Tab. 3. The moton of etended tagets n the second eement.

8 534. LI, Z. LIN, W. AN, ET AL., BOX-PARTILE LABELED ULTI-BERNOULLI FILTER FOR ULTIPLE EXTENDED TARGET Taget tue tacs BP-V-LB PP--LB BP--LB Flte Paamete PP- -LB BP- V-LB BP- -LB Suvvng atcle numbe Newbon atcle umbe 000 Runtme(sec) Taget Tab. 4. Aveage untme and the numbe of atcles n the second eement s, and t s about ten tmes less than that of PP-- LB flte. It oves that BP--LB flte s moe comutatonally effcent than PP--LB flte. Theefoe, the oosed aoach s moe aoate fo ealtme tacng. 00 Taget Fg. 5. The tue tacs and tacng esults n the second eement. adnalty 4 3 eal numbe BP-V-LB PP--LB BP--LB 5. onclusons Ths ae esents a novel aoach to tac multle etended tagets wthn the bo-atcle famewo. BP- LB and BP--LB fltes ae oosed to tac lnea etended tagets and adly maneuveng etended tagets, esectvely. In ou aoach, the measuements of etended taget ae modeled as nteval measuements, and the ont samles ae elaced by egon samles n LB ecuson. omaed wth tadtonal ont-atcle aoach, the oosed aoach needs fewe atcles to guaantee a smla accuacy. onsequently, multle etended tagets can be taced usng less untme, whch s motant fo eal-tme alcatons Tme Fg. 6. adnalty statstcs fo BP-V-LB, PP--LB and BP--LB fltes n the second eement. OSPA BP-V-LB PP--LB BP--LB Tme Fg. 7. Aveage OSPA dstances fo BP-V-LB, PP-- LB and BP--LB fltes n the second eement. As ndcated by Fg. 7, both PP--LB flte and BP--LB flte efom comaably well. Howeve, much fewe atcles ae needed by the BP--LB flte. The aveage untmes of these thee fltes ae lsted n Tab. 4. The aveage untme of BP--LB flte s Refeences [] AI, F., FAN, H., FU, Q. Benoull flte fo etended taget n clutte usng Posson models. hnese ounal of Electoncs, 05, vol. 4, no., DOI: 0.049/ce [] GILHOL, K., GODSILL, S., ASKELL, S., et al. Posson models fo etended taget and gou tacng. In SPIE Poc alfona (USA), 005,. 5930R 5930R. DOI: 0.7/ [3] AHLER, R. P. S. Statstcal ultsouce ulttaget Infomaton Fuson. London (UK): Atech House, 007. [4] AHLER, R. P. S. ulttaget Bayes flteng va fst-ode multtaget moments. IEEE Tansactons on Aeosace and Electonc Systems, 003, vol. 39, no. 4, DOI: 0.09/TAES [5] AHLER, P. R. S. PHD fltes of hghe ode n taget numbe. IEEE Tansactons on Aeosace and Electonc Systems, 007, vol. 43, no. 4, DOI: 0.09/TAES [6] VO, B. T., VO, B. N., ANTONI, A. The cadnalty balanced mult-taget mult-benoull flte and ts mlementatons. IEEE Tansactons on Sgnal Pocessng, 009, vol. 57, no.,. 409 to 43. DOI: 0.09/TSP [7] VO, B. N., VO, B. T., PHUNG, D. Labeled andom fnte sets and the Bayes mult-taget tacng flte. IEEE Tansactons on Sgnal Pocessng, 04, vol. 6, no. 4, DOI: 0.09/TSP [8] VO, B. T., VO, B. N. Labeled andom fnte sets and mult-obect

9 RADIOENGINEERING, VOL. 5, NO. 3, SEPTEBER conugate os. IEEE Tansactons on Sgnal Pocessng, 03, vol. 6, no. 3, DOI: 0.09/TSP [9] REUTER, S., VO, B. T., VO, B. N., et al. The labeled mult- Benoull flte. IEEE Tansactons on Sgnal Pocessng, 04, vol. 6, no., DOI: 0.09/TSP [0] VO, B. N., A, W. K. The Gaussan mtue obablty hyothess densty flte. IEEE Tansactons on Sgnal Pocessng, 006, vol. 54, no., DOI: 0.09/TSP [] REUTER, S., SHEEL, A., DIETAYER, K. The multle model labeled mult-benoull flte. In 8 th Intenatonal onfeence on Infomaton Fuson. Washngton, D (USA), 05, [] GNING, A., RISTI, B., IHAYLOVA, L., et al. An ntoducton to bo atcle flteng. IEEE Sgnal Pocessng agazne, 03, vol. 30, no. 4, DOI: 0.09/SP [3] SHIKORA,., GNING, A., IHAYLOVA, L., et al. Boatcle obablty hyothess densty flteng. IEEE Tansactons on Aeosace and Electonc Systems, 04, vol. 50, no. 3, DOI: 0.09/TAES [4] SONG, L., ZHAO, X. Bo-atcle cadnalty balanced multtaget mult-benoull flte. Radoengneeng, 04, vol. 3, no., [5] GRANSTRÖ, K., LUNDQUIST,., ORGUNER, U. A Gaussan mtue PHD flte fo etended taget tacng. In 3 th onfeence on Infomaton Fuson. Ednbugh (UK), 00,. 8. DOI: 0.09/IIF [6] GNING, A., RISTI, B., IHAYLOVA, L. Benoull atcle/bo-atcle fltes fo detecton and tacng n the esence of tle measuement uncetanty. IEEE Tansactons on Sgnal Pocessng, 0, vol. 60, no. 5, DOI: 0.09/TSP [7] LONG, Y. L., XU, H., AN, W., et al. Tac-befoe-detect fo nfaed maneuveng dm mult-taget va -PHD. hnese ounal of Aeonautcs, 0, vol. 5, no., DOI: 0.06/S () [8] LI, X. R., ILKOV, V. P. Suvey of maneuveng taget tacngat V: multle-model methods. IEEE Tansactons on Aeosace and Electonc Systems, 005, vol. 4, no. 4, DOI: 0.09/TAES [9] SHUHAHER, D., VO, B. T., VO, B. N. A consstent metc fo efomance evaluaton of mult-obect fltes. IEEE Tansactons on Sgnal Pocessng, 008, vol. 56, no. 8, DOI: 0.09/TSP About the Authos... ao LI was bon n 988. He eceved hs.sc. n Electonc Scence and Technology fom Natonal Unvesty of Defense Technology n 0. He s cuently wong towad the Ph.D. degee and nteested n sgnal ocessng, small taget detecton and tacng. Zang LIN was bon n 98. He eceved hs Ph.D. degees n ommuncaton and Infomaton System fom Natonal Unvesty of Defense Technology n 0. Hs eseach nteests nclude sgnal ocessng and nfomaton fuson. We AN s bon n969. She s cuently a Pofesso n Natonal Unvesty of Defense Technology. He eseach s focused on sace nfomaton acquston and ocessng. Yyu ZHOU was bon n 948. He s cuently a Pofesso n Natonal Unvesty of Defense Technology. Hs eseach s focused on ada sgnal ocessng, assve locaton technology.

INTERVAL ESTIMATION FOR THE QUANTILE OF A TWO-PARAMETER EXPONENTIAL DISTRIBUTION

INTERVAL ESTIMATION FOR THE QUANTILE OF A TWO-PARAMETER EXPONENTIAL DISTRIBUTION Intenatonal Jounal of Innovatve Management, Infomaton & Poducton ISME Intenatonalc0 ISSN 85-5439 Volume, Numbe, June 0 PP. 78-8 INTERVAL ESTIMATION FOR THE QUANTILE OF A TWO-PARAMETER EXPONENTIAL DISTRIBUTION

More information

Multistage Median Ranked Set Sampling for Estimating the Population Median

Multistage Median Ranked Set Sampling for Estimating the Population Median Jounal of Mathematcs and Statstcs 3 (: 58-64 007 ISSN 549-3644 007 Scence Publcatons Multstage Medan Ranked Set Samplng fo Estmatng the Populaton Medan Abdul Azz Jeman Ame Al-Oma and Kamaulzaman Ibahm

More information

On Maneuvering Target Tracking with Online Observed Colored Glint Noise Parameter Estimation

On Maneuvering Target Tracking with Online Observed Colored Glint Noise Parameter Estimation Wold Academy of Scence, Engneeng and Technology 6 7 On Maneuveng Taget Tacng wth Onlne Obseved Coloed Glnt Nose Paamete Estmaton M. A. Masnad-Sha, and S. A. Banan Abstact In ths pape a compehensve algothm

More information

Generalized Loss Variance Bounds

Generalized Loss Variance Bounds Int. J. Contem. ath. Scences Vol. 7 0 no. 3 559-567 Genealzed Loss Vaance Bounds Wene Hülmann FRSGlobal Swtzeland Seefeldstasse 69 CH-8008 Züch Swtzeland wene.huelmann@fsglobal.com whulmann@bluewn.ch Abstact

More information

A NOVEL DWELLING TIME DESIGN METHOD FOR LOW PROBABILITY OF INTERCEPT IN A COMPLEX RADAR NETWORK

A NOVEL DWELLING TIME DESIGN METHOD FOR LOW PROBABILITY OF INTERCEPT IN A COMPLEX RADAR NETWORK Z. Zhang et al., Int. J. of Desgn & Natue and Ecodynamcs. Vol. 0, No. 4 (205) 30 39 A NOVEL DWELLING TIME DESIGN METHOD FOR LOW PROBABILITY OF INTERCEPT IN A COMPLEX RADAR NETWORK Z. ZHANG,2,3, J. ZHU

More information

Concept of Game Equilibrium. Game theory. Normal- Form Representation. Game definition. Lecture Notes II-1 Static Games of Complete Information

Concept of Game Equilibrium. Game theory. Normal- Form Representation. Game definition. Lecture Notes II-1 Static Games of Complete Information Game theoy he study of multeson decsons Fou tyes of games Statc games of comlete nfomaton ynamc games of comlete nfomaton Statc games of ncomlete nfomaton ynamc games of ncomlete nfomaton Statc v. dynamc

More information

iclicker Quiz a) True b) False Theoretical physics: the eternal quest for a missing minus sign and/or a factor of two. Which will be an issue today?

iclicker Quiz a) True b) False Theoretical physics: the eternal quest for a missing minus sign and/or a factor of two. Which will be an issue today? Clce Quz I egsteed my quz tansmtte va the couse webste (not on the clce.com webste. I ealze that untl I do so, my quz scoes wll not be ecoded. a Tue b False Theoetcal hyscs: the etenal quest fo a mssng

More information

Rigid Bodies: Equivalent Systems of Forces

Rigid Bodies: Equivalent Systems of Forces Engneeng Statcs, ENGR 2301 Chapte 3 Rgd Bodes: Equvalent Sstems of oces Intoducton Teatment of a bod as a sngle patcle s not alwas possble. In geneal, the se of the bod and the specfc ponts of applcaton

More information

CSE-571 Robotics. Ball Tracking in RoboCup. Tracking Techniques. Rao-Blackwelized Particle Filters for State Estimation

CSE-571 Robotics. Ball Tracking in RoboCup. Tracking Techniques. Rao-Blackwelized Particle Filters for State Estimation CSE-571 Rootcs Rao-Blacwelzed Patcle Fltes fo State Estaton Ball Tacng n RooCup Exteely nosy nonlnea oton of oseve Inaccuate sensng lted pocessng powe Inteactons etween taget and Goal: envonent Unfed faewo

More information

A. Thicknesses and Densities

A. Thicknesses and Densities 10 Lab0 The Eath s Shells A. Thcknesses and Denstes Any theoy of the nteo of the Eath must be consstent wth the fact that ts aggegate densty s 5.5 g/cm (ecall we calculated ths densty last tme). In othe

More information

8 Baire Category Theorem and Uniform Boundedness

8 Baire Category Theorem and Uniform Boundedness 8 Bae Categoy Theoem and Unfom Boundedness Pncple 8.1 Bae s Categoy Theoem Valdty of many esults n analyss depends on the completeness popety. Ths popety addesses the nadequacy of the system of atonal

More information

ORBIT uncertainty propagation plays an important role in

ORBIT uncertainty propagation plays an important role in JOURNAL OF GUIDANCE, CONTROL, AND DYNAMICS Vol. 3, No. 6, Novembe Decembe 27 Nonlnea Sem-Analytc Metods fo Tajectoy Estmaton Ryan S. Pa and Danel J. Sceees Unvesty of Mcgan, Ann Abo, Mcgan 489 DOI:.254/.296

More information

Distinct 8-QAM+ Perfect Arrays Fanxin Zeng 1, a, Zhenyu Zhang 2,1, b, Linjie Qian 1, c

Distinct 8-QAM+ Perfect Arrays Fanxin Zeng 1, a, Zhenyu Zhang 2,1, b, Linjie Qian 1, c nd Intenatonal Confeence on Electcal Compute Engneeng and Electoncs (ICECEE 15) Dstnct 8-QAM+ Pefect Aays Fanxn Zeng 1 a Zhenyu Zhang 1 b Lnje Qan 1 c 1 Chongqng Key Laboatoy of Emegency Communcaton Chongqng

More information

P 365. r r r )...(1 365

P 365. r r r )...(1 365 SCIENCE WORLD JOURNAL VOL (NO4) 008 www.scecncewoldounal.og ISSN 597-64 SHORT COMMUNICATION ANALYSING THE APPROXIMATION MODEL TO BIRTHDAY PROBLEM *CHOJI, D.N. & DEME, A.C. Depatment of Mathematcs Unvesty

More information

Parameter Estimation Method in Ridge Regression

Parameter Estimation Method in Ridge Regression Paamete Estmaton Method n dge egesson Dougade.V. Det. of tatstcs, hvaj Unvesty Kolhau-46004. nda. adougade@edff.com Kashd D.N. Det. of tatstcs, hvaj Unvesty Kolhau-46004. nda. dnkashd_n@yahoo.com bstact

More information

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law Physcs 11b Lectue # Electc Feld Electc Flux Gauss s Law What We Dd Last Tme Electc chage = How object esponds to electc foce Comes n postve and negatve flavos Conseved Electc foce Coulomb s Law F Same

More information

Scalars and Vectors Scalar

Scalars and Vectors Scalar Scalas and ectos Scala A phscal quantt that s completel chaacteed b a eal numbe (o b ts numecal value) s called a scala. In othe wods a scala possesses onl a magntude. Mass denst volume tempeatue tme eneg

More information

Tian Zheng Department of Statistics Columbia University

Tian Zheng Department of Statistics Columbia University Haplotype Tansmsson Assocaton (HTA) An "Impotance" Measue fo Selectng Genetc Makes Tan Zheng Depatment of Statstcs Columba Unvesty Ths s a jont wok wth Pofesso Shaw-Hwa Lo n the Depatment of Statstcs at

More information

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering Themodynamcs of solds 4. Statstcal themodynamcs and the 3 d law Kwangheon Pak Kyung Hee Unvesty Depatment of Nuclea Engneeng 4.1. Intoducton to statstcal themodynamcs Classcal themodynamcs Statstcal themodynamcs

More information

VOL. 5, NO. 12, December 2015 ISSN ARPN Journal of Science and Technology All rights reserved.

VOL. 5, NO. 12, December 2015 ISSN ARPN Journal of Science and Technology All rights reserved. Moded Thomson and Tau based Imulse Nose Detecto G. Maagatham S. Md Mansoo Room 3 A. Sasthadev Assstant Pofesso Deatment of Electoncs and Communcaton Unvesty College of Engneeng Dndgul Inda Assstant Pofesso

More information

A Brief Guide to Recognizing and Coping With Failures of the Classical Regression Assumptions

A Brief Guide to Recognizing and Coping With Failures of the Classical Regression Assumptions A Bef Gude to Recognzng and Copng Wth Falues of the Classcal Regesson Assumptons Model: Y 1 k X 1 X fxed n epeated samples IID 0, I. Specfcaton Poblems A. Unnecessay explanatoy vaables 1. OLS s no longe

More information

3. A Review of Some Existing AW (BT, CT) Algorithms

3. A Review of Some Existing AW (BT, CT) Algorithms 3. A Revew of Some Exstng AW (BT, CT) Algothms In ths secton, some typcal ant-wndp algothms wll be descbed. As the soltons fo bmpless and condtoned tansfe ae smla to those fo ant-wndp, the pesented algothms

More information

CS649 Sensor Networks IP Track Lecture 3: Target/Source Localization in Sensor Networks

CS649 Sensor Networks IP Track Lecture 3: Target/Source Localization in Sensor Networks C649 enso etwoks IP Tack Lectue 3: Taget/ouce Localaton n enso etwoks I-Jeng Wang http://hng.cs.jhu.edu/wsn06/ png 006 C 649 Taget/ouce Localaton n Weless enso etwoks Basc Poblem tatement: Collaboatve

More information

Analysis of the chemical equilibrium of combustion at constant volume

Analysis of the chemical equilibrium of combustion at constant volume Analyss of the chemcal equlbum of combuston at constant volume Maus BEBENEL* *Coesondng autho LIEHNICA Unvesty of Buchaest Faculty of Aeosace Engneeng h. olzu Steet -5 6 Buchaest omana mausbeb@yahoo.com

More information

Stochastic Orders Comparisons of Negative Binomial Distribution with Negative Binomial Lindley Distribution

Stochastic Orders Comparisons of Negative Binomial Distribution with Negative Binomial Lindley Distribution Oen Jounal of Statcs 8- htt://dxdoog/46/os5 Publshed Onlne Al (htt://wwwscrpog/ounal/os) Stochac Odes Comasons of Negatve Bnomal Dbuton wth Negatve Bnomal Lndley Dbuton Chooat Pudommaat Wna Bodhsuwan Deatment

More information

COMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS

COMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS ultscence - XXX. mcocd Intenatonal ultdscplnay Scentfc Confeence Unvesty of skolc Hungay - pl 06 ISBN 978-963-358-3- COPLEENTRY ENERGY ETHOD FOR CURVED COPOSITE BES Ákos József Lengyel István Ecsed ssstant

More information

Energy in Closed Systems

Energy in Closed Systems Enegy n Closed Systems Anamta Palt palt.anamta@gmal.com Abstact The wtng ndcates a beakdown of the classcal laws. We consde consevaton of enegy wth a many body system n elaton to the nvese squae law and

More information

PHYS 705: Classical Mechanics. Derivation of Lagrange Equations from D Alembert s Principle

PHYS 705: Classical Mechanics. Derivation of Lagrange Equations from D Alembert s Principle 1 PHYS 705: Classcal Mechancs Devaton of Lagange Equatons fom D Alembet s Pncple 2 D Alembet s Pncple Followng a smla agument fo the vtual dsplacement to be consstent wth constants,.e, (no vtual wok fo

More information

Set of square-integrable function 2 L : function space F

Set of square-integrable function 2 L : function space F Set of squae-ntegable functon L : functon space F Motvaton: In ou pevous dscussons we have seen that fo fee patcles wave equatons (Helmholt o Schödnge) can be expessed n tems of egenvalue equatons. H E,

More information

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems Engneeng echancs oce esultants, Toques, Scala oducts, Equvalent oce sstems Tata cgaw-hll Companes, 008 Resultant of Two oces foce: acton of one bod on anothe; chaacteed b ts pont of applcaton, magntude,

More information

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints.

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints. Mathematcal Foundatons -1- Constaned Optmzaton Constaned Optmzaton Ma{ f ( ) X} whee X {, h ( ), 1,, m} Necessay condtons fo to be a soluton to ths mamzaton poblem Mathematcally, f ag Ma{ f ( ) X}, then

More information

Chapter Fifiteen. Surfaces Revisited

Chapter Fifiteen. Surfaces Revisited Chapte Ffteen ufaces Revsted 15.1 Vecto Descpton of ufaces We look now at the vey specal case of functons : D R 3, whee D R s a nce subset of the plane. We suppose s a nce functon. As the pont ( s, t)

More information

Optimal System for Warm Standby Components in the Presence of Standby Switching Failures, Two Types of Failures and General Repair Time

Optimal System for Warm Standby Components in the Presence of Standby Switching Failures, Two Types of Failures and General Repair Time Intenatonal Jounal of ompute Applcatons (5 ) Volume 44 No, Apl Optmal System fo Wam Standby omponents n the esence of Standby Swtchng Falues, Two Types of Falues and Geneal Repa Tme Mohamed Salah EL-Shebeny

More information

(8) Gain Stage and Simple Output Stage

(8) Gain Stage and Simple Output Stage EEEB23 Electoncs Analyss & Desgn (8) Gan Stage and Smple Output Stage Leanng Outcome Able to: Analyze an example of a gan stage and output stage of a multstage amplfe. efeence: Neamen, Chapte 11 8.0) ntoducton

More information

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1 Rotatonal Knematcs Rgd Object about a Fxed Axs Westen HS AP Physcs 1 Leanng Objectes What we know Unfom Ccula Moton q s Centpetal Acceleaton : Centpetal Foce: Non-unfom a F c c m F F F t m ma t What we

More information

On the Distribution of the Weighted Sum of L Independent Rician and Nakagami Envelopes in the Presence of AWGN

On the Distribution of the Weighted Sum of L Independent Rician and Nakagami Envelopes in the Presence of AWGN On the Dstbuton of the Weghted Sum of L Indeendent Rcan and Naagam Enveloes n the Pesence of AWN eoge K Kaagannds and Stavos A Kotsooulos Abstact: An altenatve, unfed, sem-analytcal aoach fo the evaluaton

More information

an application to HRQoL

an application to HRQoL AlmaMate Studoum Unvesty of Bologna A flexle IRT Model fo health questonnae: an applcaton to HRQoL Seena Boccol Gula Cavn Depatment of Statstcal Scence, Unvesty of Bologna 9 th Intenatonal Confeence on

More information

PHY126 Summer Session I, 2008

PHY126 Summer Session I, 2008 PHY6 Summe Sesson I, 8 Most of nfomaton s avalable at: http://nngoup.phscs.sunsb.edu/~chak/phy6-8 ncludng the sllabus and lectue sldes. Read sllabus and watch fo mpotant announcements. Homewok assgnment

More information

Khintchine-Type Inequalities and Their Applications in Optimization

Khintchine-Type Inequalities and Their Applications in Optimization Khntchne-Type Inequaltes and The Applcatons n Optmzaton Anthony Man-Cho So Depatment of Systems Engneeng & Engneeng Management The Chnese Unvesty of Hong Kong ISDS-Kolloquum Unvestaet Wen 29 June 2009

More information

PARAMETRIC FAULT LOCATION OF ELECTRICAL CIRCUIT USING SUPPORT VECTOR MACHINE

PARAMETRIC FAULT LOCATION OF ELECTRICAL CIRCUIT USING SUPPORT VECTOR MACHINE XVIII IMEKO WORLD CONGRESS Metology fo a Sustanable Develoment Setembe, 7 22, 2006, Ro de Janeo, Bazl PARAMETRIC FAULT LOCATION OF ELECTRICAL CIRCUIT USING SUPPORT VECTOR MACHINE S. Osowsk,2, T. Makewcz,

More information

Event Shape Update. T. Doyle S. Hanlon I. Skillicorn. A. Everett A. Savin. Event Shapes, A. Everett, U. Wisconsin ZEUS Meeting, October 15,

Event Shape Update. T. Doyle S. Hanlon I. Skillicorn. A. Everett A. Savin. Event Shapes, A. Everett, U. Wisconsin ZEUS Meeting, October 15, Event Shape Update A. Eveett A. Savn T. Doyle S. Hanlon I. Skllcon Event Shapes, A. Eveett, U. Wsconsn ZEUS Meetng, Octobe 15, 2003-1 Outlne Pogess of Event Shapes n DIS Smla to publshed pape: Powe Coecton

More information

Chapter 8. Linear Momentum, Impulse, and Collisions

Chapter 8. Linear Momentum, Impulse, and Collisions Chapte 8 Lnea oentu, Ipulse, and Collsons 8. Lnea oentu and Ipulse The lnea oentu p of a patcle of ass ovng wth velocty v s defned as: p " v ote that p s a vecto that ponts n the sae decton as the velocty

More information

Vibration Input Identification using Dynamic Strain Measurement

Vibration Input Identification using Dynamic Strain Measurement Vbaton Input Identfcaton usng Dynamc Stan Measuement Takum ITOFUJI 1 ;TakuyaYOSHIMURA ; 1, Tokyo Metopoltan Unvesty, Japan ABSTRACT Tansfe Path Analyss (TPA) has been conducted n ode to mpove the nose

More information

APPLICATIONS OF SEMIGENERALIZED -CLOSED SETS

APPLICATIONS OF SEMIGENERALIZED -CLOSED SETS Intenatonal Jounal of Mathematcal Engneeng Scence ISSN : 22776982 Volume Issue 4 (Apl 202) http://www.mes.com/ https://stes.google.com/ste/mesounal/ APPLICATIONS OF SEMIGENERALIZED CLOSED SETS G.SHANMUGAM,

More information

Part V: Velocity and Acceleration Analysis of Mechanisms

Part V: Velocity and Acceleration Analysis of Mechanisms Pat V: Velocty an Acceleaton Analyss of Mechansms Ths secton wll evew the most common an cuently pactce methos fo completng the knematcs analyss of mechansms; escbng moton though velocty an acceleaton.

More information

A Study about One-Dimensional Steady State. Heat Transfer in Cylindrical and. Spherical Coordinates

A Study about One-Dimensional Steady State. Heat Transfer in Cylindrical and. Spherical Coordinates Appled Mathematcal Scences, Vol. 7, 03, no. 5, 67-633 HIKARI Ltd, www.m-hka.com http://dx.do.og/0.988/ams.03.38448 A Study about One-Dmensonal Steady State Heat ansfe n ylndcal and Sphecal oodnates Lesson

More information

Physics Exam II Chapters 25-29

Physics Exam II Chapters 25-29 Physcs 114 1 Exam II Chaptes 5-9 Answe 8 of the followng 9 questons o poblems. Each one s weghted equally. Clealy mak on you blue book whch numbe you do not want gaded. If you ae not sue whch one you do

More information

Transport Coefficients For A GaAs Hydro dynamic Model Extracted From Inhomogeneous Monte Carlo Calculations

Transport Coefficients For A GaAs Hydro dynamic Model Extracted From Inhomogeneous Monte Carlo Calculations Tanspot Coeffcents Fo A GaAs Hydo dynamc Model Extacted Fom Inhomogeneous Monte Calo Calculatons MeKe Ieong and Tngwe Tang Depatment of Electcal and Compute Engneeng Unvesty of Massachusetts, Amhest MA

More information

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o?

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o? Test 1 phy 0 1. a) What s the pupose of measuement? b) Wte all fou condtons, whch must be satsfed by a scala poduct. (Use dffeent symbols to dstngush opeatons on ectos fom opeatons on numbes.) c) What

More information

Machine Learning. Spectral Clustering. Lecture 23, April 14, Reading: Eric Xing 1

Machine Learning. Spectral Clustering. Lecture 23, April 14, Reading: Eric Xing 1 Machne Leanng -7/5 7/5-78, 78, Spng 8 Spectal Clusteng Ec Xng Lectue 3, pl 4, 8 Readng: Ec Xng Data Clusteng wo dffeent ctea Compactness, e.g., k-means, mxtue models Connectvty, e.g., spectal clusteng

More information

The Greatest Deviation Correlation Coefficient and its Geometrical Interpretation

The Greatest Deviation Correlation Coefficient and its Geometrical Interpretation By Rudy A. Gdeon The Unvesty of Montana The Geatest Devaton Coelaton Coeffcent and ts Geometcal Intepetaton The Geatest Devaton Coelaton Coeffcent (GDCC) was ntoduced by Gdeon and Hollste (987). The GDCC

More information

Time Warp Edit Distance

Time Warp Edit Distance Tme Wa Edt Dstance PIERRE-FRNÇOIS MRTEU ee-fancos.mateau@unv-ubs.f VLORI UNIVERSITE EUROPEENNE DE RETGNE CMPUS DE TONNIC T. YVES COPPENS P 573 567 VNNES CEDEX FRNCE FERURY 28 TECNICL REPORT N : VLORI.28.V5

More information

Detection and Estimation Theory

Detection and Estimation Theory ESE 54 Detecton and Etmaton Theoy Joeph A. O Sullvan Samuel C. Sach Pofeo Electonc Sytem and Sgnal Reeach Laboatoy Electcal and Sytem Engneeng Wahngton Unvety 411 Jolley Hall 314-935-4173 (Lnda anwe) jao@wutl.edu

More information

Physics 2A Chapter 11 - Universal Gravitation Fall 2017

Physics 2A Chapter 11 - Universal Gravitation Fall 2017 Physcs A Chapte - Unvesal Gavtaton Fall 07 hese notes ae ve pages. A quck summay: he text boxes n the notes contan the esults that wll compse the toolbox o Chapte. hee ae thee sectons: the law o gavtaton,

More information

Capítulo. Three Dimensions

Capítulo. Three Dimensions Capítulo Knematcs of Rgd Bodes n Thee Dmensons Mecánca Contents ntoducton Rgd Bod Angula Momentum n Thee Dmensons Pncple of mpulse and Momentum Knetc Eneg Sample Poblem 8. Sample Poblem 8. Moton of a Rgd

More information

Recursive Least-Squares Estimation in Case of Interval Observation Data

Recursive Least-Squares Estimation in Case of Interval Observation Data Recusve Least-Squaes Estmaton n Case of Inteval Obsevaton Data H. Kuttee ), and I. Neumann 2) ) Geodetc Insttute, Lebnz Unvesty Hannove, D-3067 Hannove, Gemany, kuttee@gh.un-hannove.de 2) Insttute of Geodesy

More information

4 Recursive Linear Predictor

4 Recursive Linear Predictor 4 Recusve Lnea Pedcto The man objectve of ths chapte s to desgn a lnea pedcto wthout havng a po knowledge about the coelaton popetes of the nput sgnal. In the conventonal lnea pedcto the known coelaton

More information

Correspondence Analysis & Related Methods

Correspondence Analysis & Related Methods Coespondence Analyss & Related Methods Ineta contbutons n weghted PCA PCA s a method of data vsualzaton whch epesents the tue postons of ponts n a map whch comes closest to all the ponts, closest n sense

More information

19 The Born-Oppenheimer Approximation

19 The Born-Oppenheimer Approximation 9 The Bon-Oppenheme Appoxmaton The full nonelatvstc Hamltonan fo a molecule s gven by (n a.u.) Ĥ = A M A A A, Z A + A + >j j (883) Lets ewte the Hamltonan to emphasze the goal as Ĥ = + A A A, >j j M A

More information

Combining IMM Method with Particle Filters for 3D Maneuvering Target Tracking

Combining IMM Method with Particle Filters for 3D Maneuvering Target Tracking Combnng IMM Method wth Patcle Fltes fo D Maneuveng Taget Tacng Pe Hu Foo Depatment of Physcs Natonal Unvesty of Sngapoe Sngapoe g657@nus.edu.sg Abstact - The Inteactng Multple Model (IMM) algothm s a wdely

More information

N = N t ; t 0. N is the number of claims paid by the

N = N t ; t 0. N is the number of claims paid by the Iulan MICEA, Ph Mhaela COVIG, Ph Canddate epatment of Mathematcs The Buchaest Academy of Economc Studes an CECHIN-CISTA Uncedt Tac Bank, Lugoj SOME APPOXIMATIONS USE IN THE ISK POCESS OF INSUANCE COMPANY

More information

Dirichlet Mixture Priors: Inference and Adjustment

Dirichlet Mixture Priors: Inference and Adjustment Dchlet Mxtue Pos: Infeence and Adustment Xugang Ye (Wokng wth Stephen Altschul and Y Kuo Yu) Natonal Cante fo Botechnology Infomaton Motvaton Real-wold obects Independent obsevatons Categocal data () (2)

More information

A Micro-Doppler Modulation of Spin Projectile on CW Radar

A Micro-Doppler Modulation of Spin Projectile on CW Radar ITM Web of Confeences 11, 08005 (2017) DOI: 10.1051/ tmconf/20171108005 A Mco-Dopple Modulaton of Spn Pojectle on CW Rada Zh-Xue LIU a Bacheng Odnance Test Cente of Chna, Bacheng 137001, P. R. Chna Abstact.

More information

Probabilistic number theory : A report on work done. What is the probability that a randomly chosen integer has no square factors?

Probabilistic number theory : A report on work done. What is the probability that a randomly chosen integer has no square factors? Pobabilistic numbe theoy : A eot on wo done What is the obability that a andomly chosen intege has no squae factos? We can constuct an initial fomula to give us this value as follows: If a numbe is to

More information

LASER ABLATION ICP-MS: DATA REDUCTION

LASER ABLATION ICP-MS: DATA REDUCTION Lee, C-T A Lase Ablaton Data educton 2006 LASE ABLATON CP-MS: DATA EDUCTON Cn-Ty A. Lee 24 Septembe 2006 Analyss and calculaton of concentatons Lase ablaton analyses ae done n tme-esolved mode. A ~30 s

More information

Generating Functions, Weighted and Non-Weighted Sums for Powers of Second-Order Recurrence Sequences

Generating Functions, Weighted and Non-Weighted Sums for Powers of Second-Order Recurrence Sequences Geneatng Functons, Weghted and Non-Weghted Sums fo Powes of Second-Ode Recuence Sequences Pantelmon Stăncă Aubun Unvesty Montgomey, Depatment of Mathematcs Montgomey, AL 3614-403, USA e-mal: stanca@studel.aum.edu

More information

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M Dola Bagayoko (0) Integal Vecto Opeatons and elated Theoems Applcatons n Mechancs and E&M Ι Basc Defnton Please efe to you calculus evewed below. Ι, ΙΙ, andιιι notes and textbooks fo detals on the concepts

More information

A. P. Sakis Meliopoulos Power System Modeling, Analysis and Control. Chapter 7 3 Operating State Estimation 3

A. P. Sakis Meliopoulos Power System Modeling, Analysis and Control. Chapter 7 3 Operating State Estimation 3 DRAF and INCOMPLEE able of Contents fom A. P. Saks Melopoulos Powe System Modelng, Analyss and Contol Chapte 7 3 Opeatng State Estmaton 3 7. Intoducton 3 7. SCADA System 4 7.3 System Netwok Confguato 7

More information

UNIT10 PLANE OF REGRESSION

UNIT10 PLANE OF REGRESSION UIT0 PLAE OF REGRESSIO Plane of Regesson Stuctue 0. Intoducton Ojectves 0. Yule s otaton 0. Plane of Regesson fo thee Vaales 0.4 Popetes of Resduals 0.5 Vaance of the Resduals 0.6 Summay 0.7 Solutons /

More information

Chapter 13 - Universal Gravitation

Chapter 13 - Universal Gravitation Chapte 3 - Unesal Gataton In Chapte 5 we studed Newton s thee laws of moton. In addton to these laws, Newton fomulated the law of unesal gataton. Ths law states that two masses ae attacted by a foce gen

More information

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution oden Appled Scence The Fomn Theoy and the NC achnn fo The Rotay us wth the Spectal Ede Dstbuton Huan Lu Depatment of echancal Enneen, Zhejan Unvesty of Scence and Technoloy Hanzhou, c.y. chan, 310023,

More information

Dynamics of Rigid Bodies

Dynamics of Rigid Bodies Dynamcs of Rgd Bodes A gd body s one n whch the dstances between consttuent patcles s constant thoughout the moton of the body,.e. t keeps ts shape. Thee ae two knds of gd body moton: 1. Tanslatonal Rectlnea

More information

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles /4/04 Chapte 7 Lnea oentu Lnea oentu of a Sngle Patcle Lnea oentu: p υ It s a easue of the patcle s oton It s a vecto, sla to the veloct p υ p υ p υ z z p It also depends on the ass of the object, sla

More information

Efficiency of the principal component Liu-type estimator in logistic

Efficiency of the principal component Liu-type estimator in logistic Effcency of the pncpal component Lu-type estmato n logstc egesson model Jbo Wu and Yasn Asa 2 School of Mathematcs and Fnance, Chongqng Unvesty of Ats and Scences, Chongqng, Chna 2 Depatment of Mathematcs-Compute

More information

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER Edton CAPTER 8 VECTOR MECANCS FOR ENGNEERS: DYNAMCS Fednand P. Bee E. Russell Johnston, J. Lectue Notes: J. Walt Ole Teas Tech Unvest Knematcs of Rgd Bodes n Thee Dmensons 003 The McGaw-ll Companes, nc.

More information

Backward Haplotype Transmission Association (BHTA) Algorithm. Tian Zheng Department of Statistics Columbia University. February 5 th, 2002

Backward Haplotype Transmission Association (BHTA) Algorithm. Tian Zheng Department of Statistics Columbia University. February 5 th, 2002 Backwad Haplotype Tansmsson Assocaton (BHTA) Algothm A Fast ult-pont Sceenng ethod fo Complex Tats Tan Zheng Depatment of Statstcs Columba Unvesty Febuay 5 th, 2002 Ths s a jont wok wth Pofesso Shaw-Hwa

More information

Chapter 23: Electric Potential

Chapter 23: Electric Potential Chapte 23: Electc Potental Electc Potental Enegy It tuns out (won t show ths) that the tostatc foce, qq 1 2 F ˆ = k, s consevatve. 2 Recall, fo any consevatve foce, t s always possble to wte the wok done

More information

A Branch and Bound Method for Sum of Completion Permutation Flow Shop

A Branch and Bound Method for Sum of Completion Permutation Flow Shop UNLV Theses, Dssetatons, Pofessonal Paes, and Castones 5--04 A Banch and Bound ethod fo Sum of Comleton Pemutaton Flow Sho Swana Kodmala Unvesty of Nevada, Las Vegas, swanakodmala@gmal.com Follow ths and

More information

Variance estimation in multi-phase calibration

Variance estimation in multi-phase calibration Catalogue no. -00-X ISSN 49-09 Suvey Methodology Vaance estmaton n mult-hase calbaton by Noam Cohen, Dan Ben-Hu and Lusa Buck Release date: June, 07 How to obtan moe nfomaton Fo nfomaton about ths oduct

More information

Exact Simplification of Support Vector Solutions

Exact Simplification of Support Vector Solutions Jounal of Machne Leanng Reseach 2 (200) 293-297 Submtted 3/0; Publshed 2/0 Exact Smplfcaton of Suppot Vecto Solutons Tom Downs TD@ITEE.UQ.EDU.AU School of Infomaton Technology and Electcal Engneeng Unvesty

More information

gravity r2,1 r2 r1 by m 2,1

gravity r2,1 r2 r1 by m 2,1 Gavtaton Many of the foundatons of classcal echancs wee fst dscoveed when phlosophes (ealy scentsts and atheatcans) ted to explan the oton of planets and stas. Newton s ost faous fo unfyng the oton of

More information

Cooperative and Active Sensing in Mobile Sensor Networks for Scalar Field Mapping

Cooperative and Active Sensing in Mobile Sensor Networks for Scalar Field Mapping 3 IEEE Intenatonal Confeence on Automaton Scence and Engneeng (CASE) TuBT. Coopeatve and Actve Sensng n Moble Senso Netwos fo Scala Feld Mappng Hung Manh La, Wehua Sheng and Jmng Chen Abstact Scala feld

More information

Parallel Algorithms for Residue Scaling and Error Correction in Residue Arithmetic

Parallel Algorithms for Residue Scaling and Error Correction in Residue Arithmetic Weless Engneeng Technology 8- htt://ddoog/6/wet Publshed Onlne Octobe (htt://wwwscog/ounal/wet) Paallel Algoths fo Resdue Scalng Eo Coecton n Resdue Athetc Hao-Yung Lo Tng-We Ln Deatent of Electcal Engneeng

More information

A Queuing Model for an Automated Workstation Receiving Jobs from an Automated Workstation

A Queuing Model for an Automated Workstation Receiving Jobs from an Automated Workstation Intenatonal Jounal of Opeatons Reseach Intenatonal Jounal of Opeatons Reseach Vol. 7, o. 4, 918 (1 A Queung Model fo an Automated Wokstaton Recevng Jobs fom an Automated Wokstaton Davd S. Km School of

More information

H5 Gas meter calibration

H5 Gas meter calibration H5 Gas mete calibation Calibation: detemination of the elation between the hysical aamete to be detemined and the signal of a measuement device. Duing the calibation ocess the measuement equiment is comaed

More information

Large scale magnetic field generation by accelerated particles in galactic medium

Large scale magnetic field generation by accelerated particles in galactic medium Lage scale magnetc feld geneaton by acceleated patcles n galactc medum I.N.Toptygn Sant Petesbug State Polytechncal Unvesty, depatment of Theoetcal Physcs, Sant Petesbug, Russa 2.Reason explonatons The

More information

Remember: When an object falls due to gravity its potential energy decreases.

Remember: When an object falls due to gravity its potential energy decreases. Chapte 5: lectc Potental As mentoned seveal tmes dung the uate Newton s law o gavty and Coulomb s law ae dentcal n the mathematcal om. So, most thngs that ae tue o gavty ae also tue o electostatcs! Hee

More information

A NOTE ON ELASTICITY ESTIMATION OF CENSORED DEMAND

A NOTE ON ELASTICITY ESTIMATION OF CENSORED DEMAND Octobe 003 B 003-09 A NOT ON ASTICITY STIATION OF CNSOD DAND Dansheng Dong an Hay. Kase Conell nvesty Depatment of Apple conomcs an anagement College of Agcultue an fe Scences Conell nvesty Ithaca New

More information

VParC: A Compression Scheme for Numeric Data in Column-Oriented Databases

VParC: A Compression Scheme for Numeric Data in Column-Oriented Databases The Intenatonal Aab Jounal of Infomaton Technology VPaC: A Compesson Scheme fo Numec Data n Column-Oented Databases Ke Yan, Hong Zhu, and Kevn Lü School of Compute Scence and Technology, Huazhong Unvesty

More information

VISUALIZATION OF THE ABSTRACT THEORIES IN DSP COURSE BASED ON CDIO CONCEPT

VISUALIZATION OF THE ABSTRACT THEORIES IN DSP COURSE BASED ON CDIO CONCEPT VISUALIZATION OF THE ABSTRACT THEORIES IN DSP COURSE BASED ON CDIO CONCEPT Wang L-uan, L Jan, Zhen Xao-qong Chengdu Unvesty of Infomaton Technology ABSTRACT The pape analyzes the chaactestcs of many fomulas

More information

Location-Aware Cross-Tier Coordinated Multipoint Transmission in Two-Tier Cellular Networks

Location-Aware Cross-Tier Coordinated Multipoint Transmission in Two-Tier Cellular Networks Locaton-Awae Coss-Te Coodnated Multpont Tansmsson n Two-Te Cellula Netwoks Ahmed Hamd Sak and Ekam Hossan axv:45.876v cs.ni] 8 Sep 4 Abstact Mult-te cellula netwoks ae consdeed as an effectve soluton to

More information

SOME NEW SELF-DUAL [96, 48, 16] CODES WITH AN AUTOMORPHISM OF ORDER 15. KEYWORDS: automorphisms, construction, self-dual codes

SOME NEW SELF-DUAL [96, 48, 16] CODES WITH AN AUTOMORPHISM OF ORDER 15. KEYWORDS: automorphisms, construction, self-dual codes Факултет по математика и информатика, том ХVІ С, 014 SOME NEW SELF-DUAL [96, 48, 16] CODES WITH AN AUTOMORPHISM OF ORDER 15 NIKOLAY I. YANKOV ABSTRACT: A new method fo constuctng bnay self-dual codes wth

More information

Competition from Product Line in a Consumer Search Model 1

Competition from Product Line in a Consumer Search Model 1 Cometton fom Poduct Lne n a Consume Seach Model Kuson Leawsakul July 3, 03 Abstact Ths study ams to nvestgate the cometton fom oduct lne when consumes seach among two multoduct fms fo dffeentated oducts

More information

c( 1) c(0) c(1) Note z 1 represents a unit interval delay Figure 85 3 Transmit equalizer functional model

c( 1) c(0) c(1) Note z 1 represents a unit interval delay Figure 85 3 Transmit equalizer functional model Relace 85.8.3.2 with the following: 85.8.3.2 Tansmitted outut wavefom The 40GBASE-CR4 and 100GBASE-CR10 tansmit function includes ogammable equalization to comensate fo the fequency-deendent loss of the

More information

On a New Definition of a Stochastic-based Accuracy Concept of Data Reconciliation-Based Estimators

On a New Definition of a Stochastic-based Accuracy Concept of Data Reconciliation-Based Estimators On a New Defnton of a Stochastc-based Accuacy Concept of Data Reconclaton-Based Estmatos M. Bagajewcz Unesty of Olahoma 100 E. Boyd St., Noman OK 73019, USA Abstact Tadtonally, accuacy of an nstument s

More information

Multi-element based on proxy re-encryption scheme for mobile cloud computing

Multi-element based on proxy re-encryption scheme for mobile cloud computing 36 11 Vol.36 No.11 015 11 Jounal on Communcatons Novembe 015 do:10.11959/.ssn.1000-436x.01517 1 1 1. 10094. 100070 TP309. A Mult-element based on poxy e-encypton scheme fo moble cloud computng SU Mang

More information

PARAMETER ESTIMATION FOR TWO WEIBULL POPULATIONS UNDER JOINT TYPE II CENSORED SCHEME

PARAMETER ESTIMATION FOR TWO WEIBULL POPULATIONS UNDER JOINT TYPE II CENSORED SCHEME Sept 04 Vol 5 No 04 Intenatonal Jounal of Engneeng Appled Scences 0-04 EAAS & ARF All ghts eseed wwweaas-ounalog ISSN305-869 PARAMETER ESTIMATION FOR TWO WEIBULL POPULATIONS UNDER JOINT TYPE II CENSORED

More information

Stellar Astrophysics. dt dr. GM r. The current model for treating convection in stellar interiors is called mixing length theory:

Stellar Astrophysics. dt dr. GM r. The current model for treating convection in stellar interiors is called mixing length theory: Stella Astophyscs Ovevew of last lectue: We connected the mean molecula weght to the mass factons X, Y and Z: 1 1 1 = X + Y + μ 1 4 n 1 (1 + 1) = X μ 1 1 A n Z (1 + ) + Y + 4 1+ z A Z We ntoduced the pessue

More information

Web Page Ranking based on Fuzzy and Learning Automata

Web Page Ranking based on Fuzzy and Learning Automata Web Page Ranng based on Fuzzy and Leanng Autoata Zoheh Ana Deatent of Coute ngneeng Shabesta Azad Unvesty Shabesta,Ian +98(47)53 zoheh_ana@aushab.ac. Mohaad Reza Meybod Deatent of Coute ngneeng Aab Unvesty

More information

Physics 201 Lecture 4

Physics 201 Lecture 4 Phscs 1 Lectue 4 ltoda: hapte 3 Lectue 4 v Intoduce scalas and vectos v Peom basc vecto aleba (addton and subtacton) v Inteconvet between atesan & Pola coodnates Stat n nteestn 1D moton poblem: ace 9.8

More information