DYNAMICS. Systems of Particles VECTOR MECHANICS FOR ENGINEERS: Seventh Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.

Size: px
Start display at page:

Download "DYNAMICS. Systems of Particles VECTOR MECHANICS FOR ENGINEERS: Seventh Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr."

Transcription

1 Seeth Edto CHPTER 4 VECTOR MECHNICS FOR ENINEERS: DYNMICS Ferdad P. eer E. Russell Johsto, Jr. Systes of Partcles Lecture Notes: J. Walt Oler Texas Tech Uersty 003 The Mcraw-Hll Copaes, Ic. ll rghts resered.

2 Seeth Edto Vector Mechacs for Egeers: Dyacs Cotets Itroducto pplcato of Newto s Laws: Effecte Forces Lear ad gular Moetu Moto of Mass Ceter of Syste of Partcles gular Moetu bout Mass Ceter Coserato of Moetu Saple Proble 4. Ketc Eergy Work-Eergy Prcple. Coserato of Eergy Prcple of Ipulse ad Moetu Saple Proble 4.4 Saple Proble 4.5 Varable Systes of Partcles Steady Strea of Partcles Steady Strea of Partcles. pplcatos Streas ag or Losg Mass Saple Proble The Mcraw-Hll Copaes, Ic. ll rghts resered. 4 -

3 Seeth Edto Vector Mechacs for Egeers: Dyacs Itroducto I the curret chapter, you wll study the oto of systes of partcles. The effecte force of a partcle s defed as the product of t ass ad accelerato. It wll be show that the syste of exteral forces actg o a syste of partcles s equpollet wth the syste of effecte forces of the syste. The ass ceter of a syste of partcles wll be defed ad ts oto descrbed. pplcato of the work-eergy prcple ad the pulseoetu prcple to a syste of partcles wll be descrbed. Result obtaed are also applcable to a syste of rgdly coected partcles,.e., a rgd body. alyss ethods wll be preseted for arable systes of partcles,.e., systes whch the partcles cluded the syste chage. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-3

4 Seeth Edto Vector Mechacs for Egeers: Dyacs pplcato of Newto s Laws. Effecte Forces Newto s secod law for each partcle P syste of partcles, F r j j ( r f ) F exteral force a effecte force F f j a j r a f j teral forces a The syste of exteral ad teral forces o a partcle s equalet to the effecte force of the partcle. The syste of exteral ad teral forces actg o the etre syste of partcles s equalet to the syste of effecte forces. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-4

5 Seeth Edto Vector Mechacs for Egeers: Dyacs pplcato of Newto s Laws. Effecte Forces Sug oer all the eleets, F f a j ( ) ( ) r F r f ( r a ) j j j Sce the teral forces occur equal ad opposte collear pars, the resultat force ad couple due to the teral forces are zero, F a r F r a ( ) ( ) The syste of exteral forces ad the syste of effecte forces are equpollet by ot equalet. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-5

6 Seeth Edto Vector Mechacs for Egeers: Dyacs Lear & gular Moetu Lear oetu of the syste of partcles, L L a Resultat of the exteral forces s equal to rate of chage of lear oetu of the syste of partcles, F L gular oetu about fxed pot O of syste of partcles, H r H O O ( ) ( r ) ( r ) ( r a ) Moet resultat about fxed pot O of the exteral forces s equal to the rate of chage of agular oetu of the syste of partcles, M O H O 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-6

7 Seeth Edto Vector Mechacs for Egeers: Dyacs Moto of the Mass Ceter of a Syste of Partcles Mass ceter of syste of partcles s defed by posto ector whch r satsfes r r Dfferetatg twce, r r a L F L The ass ceter oes as f the etre ass ad all of the exteral forces were cocetrated at that pot. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-7

8 Seeth Edto Vector Mechacs for Egeers: Dyacs gular Moetu bout the Mass Ceter a a a Cosder the cetrodal frae of referece x y z, whch traslates wth respect to the Newtoa frae Oxyz. The agular oetu of the syste of partcles about the ass ceter, H H ( r ) ( r a ) ( r ( a a )) ( r a ) ( r a ) ( r F ) M r a The cetrodal frae s ot, geeral, a Newtoa frae. The oet resultat about of the exteral forces s equal to the rate of chage of agular oetu about of the syste of partcles. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-8

9 Seeth Edto Vector Mechacs for Egeers: Dyacs gular Moetu bout the Mass Ceter gular oetu about of the partcles ther oto relate to the cetrodal x y z frae of referece, H ( r ) gular oetu about of partcles ther absolute oto relate to the Newtoa Oxyz frae of referece. H H ( r ) ( r ( )) H r M ( r ) gular oetu about of the partcle oeta ca be calculated wth respect to ether the Newtoa or cetrodal fraes of referece. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-9

10 Seeth Edto Vector Mechacs for Egeers: Dyacs Coserato of Moetu If o exteral forces act o the partcles of a syste, the the lear oetu ad agular oetu about the fxed pot O are cosered. L F 0 H O M O 0 L costat H costat O Cocept of coserato of oetu also apples to the aalyss of the ass ceter oto, L F 0 H M 0 L costat costat H costat I soe applcatos, such as probles olg cetral forces, L F 0 H O M O 0 L costat H costat O 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-0

11 Seeth Edto Vector Mechacs for Egeers: Dyacs Saple Proble 4. SOLUTION: Sce there are o exteral forces, the lear oetu of the syste s cosered. Wrte separate copoet equatos for the coserato of lear oetu. 0 kg projectle s og wth a elocty of 30 /s whe t explodes to.5 ad 7.5 kg fragets. Iedately after the exploso, the fragets trael the drectos θ 45 o ad θ 30 o. Detere the elocty of each fraget. Sole the equatos sultaeously for the fraget eloctes. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4 -

12 Seeth Edto Vector Mechacs for Egeers: Dyacs Saple Proble 4. SOLUTION: Sce there are o exteral forces, the lear oetu of the syste s cosered. Wrte separate copoet equatos for the coserato of lear oetu. (.5) ( 7.5) ( 0) 0 0 y x x copoets:.5 cos cos30 y copoets:.5 s s ( 30) Sole the equatos sultaeously for the fraget eloctes. 6./s 9.3 s 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4 -

13 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. Vector Mechacs for Egeers: Dyacs Seeth Edto 4-3 Ketc Eergy Ketc eergy of a syste of partcles, ( ) T Expressg the elocty ters of the cetrodal referece frae, ( ) ( ) [ ] T Ketc eergy s equal to ketc eergy of ass ceter plus ketc eergy relate to the cetrodal frae.

14 Seeth Edto Vector Mechacs for Egeers: Dyacs Work-Eergy Prcple. Coserato of Eergy Prcple of work ad eergy ca be appled to each partcle P, T U T where U represets the work doe by the teral forces ad f j the resultat exteral force actg F o P. Prcple of work ad eergy ca be appled to the etre syste by addg the ketc eerges of all partcles ad cosderg the work doe by all exteral ad teral forces. lthough f j ad f jare equal ad opposte, the work of these forces wll ot, geeral, cacel out. If the forces actg o the partcles are coserate, the work s equal to the chage potetal eergy ad T V T V whch expresses the prcple of coserato of eergy for the syste of partcles. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-4

15 Seeth Edto Vector Mechacs for Egeers: Dyacs Prcple of Ipulse ad Moetu L F t t L Fdt t t L Fdt L L H M t t M O H O t dt t M O H O dt H H The oeta of the partcles at te t ad the pulse of the forces fro t to t for a syste of ectors equpollet to the syste of oeta of the partcles at te t. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-5

16 Seeth Edto Vector Mechacs for Egeers: Dyacs Saple Proble 4.4 SOLUTION: all, of ass,s suspeded fro a cord, of legth l, attached to cart, of ass, whch ca roll freely o a frctoless horzotal tract. Whle the cart s at rest, the ball s ge a tal elocty 0 gl. Detere (a) the elocty of as t reaches t axu eleato, ad (b) the axu ertcal dstace h through whch wll rse. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. Wth o exteral horzotal forces, t follows fro the pulse-oetu prcple that the horzotal copoet of oetu s cosered. Ths relato ca be soled for the elocty of at ts axu eleato. The coserato of eergy prcple ca be appled to relate the tal ketc eergy to the axu potetal eergy. The axu ertcal dstace s detered fro ths relato. 4-6

17 Seeth Edto Vector Mechacs for Egeers: Dyacs Saple Proble 4.4 y x SOLUTION: Wth o exteral horzotal forces, t follows fro the pulse-oetu prcple that the horzotal copoet of oetu s cosered. Ths relato ca be soled for the elocty of at ts axu eleato. t L Fdt L, x copoet equato: t, 0 Veloctes at postos ad are,,,,,, 0, ( ) 0,, (elocty of relate to s zero at posto ),, The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-7

18 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. Vector Mechacs for Egeers: Dyacs Seeth Edto 4-8 Saple Proble 4.4 The coserato of eergy prcple ca be appled to relate the tal ketc eergy to the axu potetal eergy. V T V T Posto - Potetal Eergy: Ketc Eergy: Posto - Potetal Eergy: Ketc Eergy: gl V 0 T gh gl V ( ), T ( ) gh gl gl, 0 g h 0 0 0, 0 g g g g h g g h 0 0

19 Seeth Edto Vector Mechacs for Egeers: Dyacs Saple Proble 4.5 all has tal elocty 0 3 /s parallel to the axs of the table. It hts ball ad the ball C whch are both at rest. alls ad C ht the sdes of the table squarely at ad C ad ball hts oblquely at. ssug perfectly elastc collsos, detere eloctes,, ad C wth whch the balls ht the sdes of the table. SOLUTION: There are four ukows:,,x,,y, ad C. Soluto requres four equatos: coserato prcples for lear oetu (two copoet equatos), agular oetu, ad eergy. Wrte the coserato equatos ters of the ukow eloctes ad sole sultaeously. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-9

20 Seeth Edto Vector Mechacs for Egeers: Dyacs Saple Proble 4.5 SOLUTION: There are four ukows:,,x,,y, ad C. j, x, y j C C The coserato of oetu ad eergy equatos, L Fdt L H T O, V 0 0 M dt H T O V, x O, C 0 ( ), x, y C, y ( 0.6 ) 0 (.4 ) (.), y ( 0.9 ) C y x Solg the frst three equatos ters of C, 3, y 3 C 6, x Substtutg to the eergy equato, ( 6) ( 3 ) 3 0 C C 78 C C C 7 0. s 4 j C 9 ( ) s.34 s C.4 s 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-0

21 Seeth Edto Vector Mechacs for Egeers: Dyacs Varable Systes of Partcles Ketcs prcples establshed so far were dered for costat systes of partcles,.e., systes whch ether ga or lose partcles. large uber of egeerg applcatos requre the cosderato of arable systes of partcles, e.g., hydraulc turbe, rocket ege, etc. For aalyses, cosder auxlary systes whch cosst of the partcles stataeously wth the syste plus the partcles that eter or leae the syste durg a short te teral. The auxlary systes, thus defed, are costat systes of partcles. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4 -

22 Seeth Edto Vector Mechacs for Egeers: Dyacs Steady Strea of Partcles Syste cossts of a steady strea of partcles agast a ae or through a duct. Defe auxlary syste whch cludes partcles whch flow ad out oer t. The auxlary syste s a costat syste of partcles oer t. L [ ( ) ] F t [ ( ) ] t t Fdt L F d dt ( ) 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4 -

23 Seeth Edto Vector Mechacs for Egeers: Dyacs Steady Strea of Partcles. pplcatos Flud Strea Derted by Vae or Duct Fa Flud Flowg Through a Ppe Jet Ege Helcopter 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-3

24 Seeth Edto Vector Mechacs for Egeers: Dyacs Streas ag or Losg Mass Defe auxlary syste to clude partcles of ass wth syste at te t plus the partcles of ass whch eter the syste oer te teral t. The auxlary syste s a costat syste of partcles. L t t Fdt L d d F u dt dt d a F u dt [ ( ) a ] F t ( )( ) F t ( ) ( ) a 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-4

25 Seeth Edto Vector Mechacs for Egeers: Dyacs Saple Proble 4.6 ra falls oto a chute at the rate of 0 kg/s. It hts the chute wth a elocty of 6 /s ad leaes wth a elocty of 4.5 /s. The cobed weght of the chute ad the gra t carres s 3 kn wth the ceter of graty at. Detere the reactos at C ad. SOLUTION: Defe a syste cosstg of the ass of gra o the chute plus the ass that s added ad reoed durg the te teral t. pply the prcples of coserato of lear ad agular oetu for three equatos for the three ukow reactos. 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-5

26 Seeth Edto Vector Mechacs for Egeers: Dyacs Saple Proble 4.6 SOLUTION: Defe a syste cosstg of the ass of gra o the chute plus the ass that s added ad reoed durg the te teral t. pply the prcples of coserato of lear ad agular oetu for three equatos for the three ukow reactos. H L C, C x 0.9 t Fdt ( ) cos0 ( ) ( C W ) t ( ) s0 M C dt L y H C, ( ) (.W 3.6) t.8( ) cos0 3.6( ) s0 Sole for C x, C y, ad wth t 0kg s 3. ft s 7.45slug s 0 N C j ( ) N 003 The Mcraw-Hll Copaes, Ic. ll rghts resered. 4-6

DYNAMICS. Systems of Particles VECTOR MECHANICS FOR ENGINEERS: Tenth Edition CHAPTER

DYNAMICS. Systems of Particles VECTOR MECHANICS FOR ENGINEERS: Tenth Edition CHAPTER Teth Edto CHPTER 4 VECTOR MECHNICS FOR ENINEERS: DYNMICS Ferdad P. eer E. Russell Johsto, Jr. Phllp J. Corwell Lecture Notes: ra P. Self Calfora Polytechc State Uersty Systes of Partcles 03 The Mcraw-Hll

More information

VECTOR MECHANICS FOR ENGINEERS: Vector Mechanics for Engineers: Dynamics. In the current chapter, you will study the motion of systems of particles.

VECTOR MECHANICS FOR ENGINEERS: Vector Mechanics for Engineers: Dynamics. In the current chapter, you will study the motion of systems of particles. Seeth Edto CHPTER 4 VECTOR MECHNICS FOR ENINEERS: DYNMICS Fedad P. ee E. Russell Johsto, J. Systems of Patcles Lectue Notes: J. Walt Ole Texas Tech Uesty 003 The Mcaw-Hll Compaes, Ic. ll ghts eseed. Seeth

More information

Chapter 4: Linear Momentum and Collisions

Chapter 4: Linear Momentum and Collisions Chater 4: Lear oetu ad Collsos 4.. The Ceter o ass, Newto s Secod Law or a Syste o artcles 4.. Lear oetu ad Its Coserato 4.3. Collso ad Iulse 4.4. oetu ad Ketc Eergy Collsos 4.. The Ceter o ass. Newto

More information

PHYS Look over. examples 2, 3, 4, 6, 7, 8,9, 10 and 11. How To Make Physics Pay PHYS Look over. Examples: 1, 4, 5, 6, 7, 8, 9, 10,

PHYS Look over. examples 2, 3, 4, 6, 7, 8,9, 10 and 11. How To Make Physics Pay PHYS Look over. Examples: 1, 4, 5, 6, 7, 8, 9, 10, PHYS Look over Chapter 9 Sectos - Eamples:, 4, 5, 6, 7, 8, 9, 0, PHYS Look over Chapter 7 Sectos -8 8, 0 eamples, 3, 4, 6, 7, 8,9, 0 ad How To ake Phscs Pa We wll ow look at a wa of calculatg where the

More information

Stationary states of atoms and molecules

Stationary states of atoms and molecules Statoary states of atos ad olecules I followg wees the geeral aspects of the eergy level structure of atos ad olecules that are essetal for the terpretato ad the aalyss of spectral postos the rotatoal

More information

MOLECULAR VIBRATIONS

MOLECULAR VIBRATIONS MOLECULAR VIBRATIONS Here we wsh to vestgate molecular vbratos ad draw a smlarty betwee the theory of molecular vbratos ad Hückel theory. 1. Smple Harmoc Oscllator Recall that the eergy of a oe-dmesoal

More information

Manipulator Dynamics. Amirkabir University of Technology Computer Engineering & Information Technology Department

Manipulator Dynamics. Amirkabir University of Technology Computer Engineering & Information Technology Department Mapulator Dyamcs mrkabr Uversty of echology omputer Egeerg formato echology Departmet troducto obot arm dyamcs deals wth the mathematcal formulatos of the equatos of robot arm moto. hey are useful as:

More information

DIFFERENTIAL GEOMETRIC APPROACH TO HAMILTONIAN MECHANICS

DIFFERENTIAL GEOMETRIC APPROACH TO HAMILTONIAN MECHANICS DIFFERENTIAL GEOMETRIC APPROACH TO HAMILTONIAN MECHANICS Course Project: Classcal Mechacs (PHY 40) Suja Dabholkar (Y430) Sul Yeshwath (Y444). Itroducto Hamltoa mechacs s geometry phase space. It deals

More information

2/20/2013. Topics. Power Flow Part 1 Text: Power Transmission. Power Transmission. Power Transmission. Power Transmission

2/20/2013. Topics. Power Flow Part 1 Text: Power Transmission. Power Transmission. Power Transmission. Power Transmission /0/0 Topcs Power Flow Part Text: 0-0. Power Trassso Revsted Power Flow Equatos Power Flow Proble Stateet ECEGR 45 Power Systes Power Trassso Power Trassso Recall that for a short trassso le, the power

More information

7.0 Equality Contraints: Lagrange Multipliers

7.0 Equality Contraints: Lagrange Multipliers Systes Optzato 7.0 Equalty Cotrats: Lagrage Multplers Cosder the zato of a o-lear fucto subject to equalty costrats: g f() R ( ) 0 ( ) (7.) where the g ( ) are possbly also olear fuctos, ad < otherwse

More information

Physics 114 Exam 2 Fall Name:

Physics 114 Exam 2 Fall Name: Physcs 114 Exam Fall 015 Name: For gradg purposes (do ot wrte here): Questo 1. 1... 3. 3. Problem Aswer each of the followg questos. Pots for each questo are dcated red. Uless otherwse dcated, the amout

More information

PRACTICAL CONSIDERATIONS IN HUMAN-INDUCED VIBRATION

PRACTICAL CONSIDERATIONS IN HUMAN-INDUCED VIBRATION PRACTICAL CONSIDERATIONS IN HUMAN-INDUCED VIBRATION Bars Erkus, 4 March 007 Itroducto Ths docuet provdes a revew of fudaetal cocepts structural dyacs ad soe applcatos hua-duced vbrato aalyss ad tgato of

More information

VIII Dynamics of Systems of Particles

VIII Dynamics of Systems of Particles VIII Dyacs of Systes of Patcles Cete of ass: Cete of ass Lea oetu of a Syste Agula oetu of a syste Ketc & Potetal Eegy of a Syste oto of Two Iteactg Bodes: The Reduced ass Collsos: o Elastc Collsos R whee:

More information

A New Method for Solving Fuzzy Linear. Programming by Solving Linear Programming

A New Method for Solving Fuzzy Linear. Programming by Solving Linear Programming ppled Matheatcal Sceces Vol 008 o 50 7-80 New Method for Solvg Fuzzy Lear Prograg by Solvg Lear Prograg S H Nasser a Departet of Matheatcs Faculty of Basc Sceces Mazadara Uversty Babolsar Ira b The Research

More information

Long blade vibration model for turbine-generator shafts torsional vibration analysis

Long blade vibration model for turbine-generator shafts torsional vibration analysis Avalable ole www.ocpr.co Joural of Checal ad Pharaceutcal Research, 05, 7(3):39-333 Research Artcle ISSN : 0975-7384 CODEN(USA) : JCPRC5 Log blade vbrato odel for turbe-geerator shafts torsoal vbrato aalyss

More information

Consider two masses m 1 at x = x 1 and m 2 at x 2.

Consider two masses m 1 at x = x 1 and m 2 at x 2. Chapte 09 Syste of Patcles Cete of ass: The cete of ass of a body o a syste of bodes s the pot that oes as f all of the ass ae cocetated thee ad all exteal foces ae appled thee. Note that HRW uses co but

More information

How does the momentum before an elastic and an inelastic collision compare to the momentum after the collision?

How does the momentum before an elastic and an inelastic collision compare to the momentum after the collision? Experent 9 Conseraton o Lnear Moentu - Collsons In ths experent you wll be ntroduced to the denton o lnear oentu. You wll learn the derence between an elastc and an nelastc collson. You wll explore how

More information

Debabrata Dey and Atanu Lahiri

Debabrata Dey and Atanu Lahiri RESEARCH ARTICLE QUALITY COMPETITION AND MARKET SEGMENTATION IN THE SECURITY SOFTWARE MARKET Debabrata Dey ad Atau Lahr Mchael G. Foster School of Busess, Uersty of Washgto, Seattle, Seattle, WA 9895 U.S.A.

More information

Centroids & Moments of Inertia of Beam Sections

Centroids & Moments of Inertia of Beam Sections RCH 614 Note Set 8 S017ab Cetrods & Momets of erta of Beam Sectos Notato: b C d d d Fz h c Jo L O Q Q = ame for area = ame for a (base) wdth = desgato for chael secto = ame for cetrod = calculus smbol

More information

Simple Linear Regression

Simple Linear Regression Statstcal Methods I (EST 75) Page 139 Smple Lear Regresso Smple regresso applcatos are used to ft a model descrbg a lear relatoshp betwee two varables. The aspects of least squares regresso ad correlato

More information

Applying the condition for equilibrium to this equilibrium, we get (1) n i i =, r G and 5 i

Applying the condition for equilibrium to this equilibrium, we get (1) n i i =, r G and 5 i CHEMICAL EQUILIBRIA The Thermodyamc Equlbrum Costat Cosder a reversble reacto of the type 1 A 1 + 2 A 2 + W m A m + m+1 A m+1 + Assgg postve values to the stochometrc coeffcets o the rght had sde ad egatve

More information

Module 1 : The equation of continuity. Lecture 5: Conservation of Mass for each species. & Fick s Law

Module 1 : The equation of continuity. Lecture 5: Conservation of Mass for each species. & Fick s Law Module : The equato of cotuty Lecture 5: Coservato of Mass for each speces & Fck s Law NPTEL, IIT Kharagpur, Prof. Sakat Chakraborty, Departmet of Chemcal Egeerg 2 Basc Deftos I Mass Trasfer, we usually

More information

The theoretical background of

The theoretical background of he theoretcal backgroud of -echologes he theoretcal backgroud of FactSage he followg sldes gve a abrdged overvew of the ajor uderlyg prcples of the calculatoal odules of FactSage. -echologes he bbs Eergy

More information

Construction of generalized coordinates basis functions in Lagrangian dynamics of flat manipulators

Construction of generalized coordinates basis functions in Lagrangian dynamics of flat manipulators Appled ad Coputatoal Matheatcs 4; (: 86-9 Publshed ole Septeber 4 (http://www.scecepublshggroup.co//ac) do:.648/.ac.44. ISSN: 8-565 (Prt); ISSN: 8-56 (Ole) Costructo of geeralzed coordates bass fuctos

More information

RECURSIVE FORMULATION FOR MULTIBODY DYNAMICS

RECURSIVE FORMULATION FOR MULTIBODY DYNAMICS ultbody Dyamcs Lecture Uversty of okyo, Japa Dec. 8, 25 RECURSIVE FORULAION FOR ULIODY DYNAICS Lecturer: Sug-Soo m Professor, Dept. of echatrocs Egeerg, orea Vstg Professor, Ceter for Collaboratve Research

More information

Chapter 2 - Free Vibration of Multi-Degree-of-Freedom Systems - II

Chapter 2 - Free Vibration of Multi-Degree-of-Freedom Systems - II CEE49b Chapter - Free Vbrato of Mult-Degree-of-Freedom Systems - II We ca obta a approxmate soluto to the fudametal atural frequecy through a approxmate formula developed usg eergy prcples by Lord Raylegh

More information

+ve 10 N. Note we must be careful about writing If mass is not constant: dt dt dt

+ve 10 N. Note we must be careful about writing If mass is not constant: dt dt dt Force /N Moet is defied as the prodct of ass ad elocity. It is therefore a ector qatity. A ore geeral ersio of Newto s Secod Law is that force is the rate of chage of oet. I the absece of ay exteral force,

More information

GENERALIZATIONS OF CEVA S THEOREM AND APPLICATIONS

GENERALIZATIONS OF CEVA S THEOREM AND APPLICATIONS GENERLIZTIONS OF CEV S THEOREM ND PPLICTIONS Floret Smaradache Uversty of New Mexco 200 College Road Gallup, NM 87301, US E-mal: smarad@um.edu I these paragraphs oe presets three geeralzatos of the famous

More information

UNIT 2 SOLUTION OF ALGEBRAIC AND TRANSCENDENTAL EQUATIONS

UNIT 2 SOLUTION OF ALGEBRAIC AND TRANSCENDENTAL EQUATIONS Numercal Computg -I UNIT SOLUTION OF ALGEBRAIC AND TRANSCENDENTAL EQUATIONS Structure Page Nos..0 Itroducto 6. Objectves 7. Ital Approxmato to a Root 7. Bsecto Method 8.. Error Aalyss 9.4 Regula Fals Method

More information

Some Different Perspectives on Linear Least Squares

Some Different Perspectives on Linear Least Squares Soe Dfferet Perspectves o Lear Least Squares A stadard proble statstcs s to easure a respose or depedet varable, y, at fed values of oe or ore depedet varables. Soetes there ests a deterstc odel y f (,,

More information

ON THE MOTION OF PLANAR BARS SYSTEMS WITH CLEARANCES IN JOINTS

ON THE MOTION OF PLANAR BARS SYSTEMS WITH CLEARANCES IN JOINTS ON THE MOTION OF PLANAR BARS SYSTEMS WITH CLEARANCES IN JOINTS Şl uv dr g Ja-Crsta GRIGORE, Uverstatea d Pteşt, strtîrgu dvale Nr Prof uv dr g Ncolae PANDREA, Uverstatea d Pteşt, strtîrgu dvale Nr Cof

More information

Introduction. Free Electron Fermi Gas. Energy Levels in One Dimension

Introduction. Free Electron Fermi Gas. Energy Levels in One Dimension ree Electro er Gas Eergy Levels Oe Deso Effect of eperature o the er-drac Dstrbuto ree Electro Gas hree Desos Heat Capacty of the Electro Gas Electrcal Coductvty ad Oh s Law Moto Magetc elds heral Coductvty

More information

Coherent Potential Approximation

Coherent Potential Approximation Coheret Potetal Approxato Noveber 29, 2009 Gree-fucto atrces the TB forals I the tght bdg TB pcture the atrx of a Haltoa H s the for H = { H j}, where H j = δ j ε + γ j. 2 Sgle ad double uderles deote

More information

Chapter 9 Jordan Block Matrices

Chapter 9 Jordan Block Matrices Chapter 9 Jorda Block atrces I ths chapter we wll solve the followg problem. Gve a lear operator T fd a bass R of F such that the matrx R (T) s as smple as possble. f course smple s a matter of taste.

More information

Non-degenerate Perturbation Theory

Non-degenerate Perturbation Theory No-degeerate Perturbato Theory Proble : H E ca't solve exactly. But wth H H H' H" L H E Uperturbed egevalue proble. Ca solve exactly. E Therefore, kow ad. H ' H" called perturbatos Copyrght Mchael D. Fayer,

More information

C-1: Aerodynamics of Airfoils 1 C-2: Aerodynamics of Airfoils 2 C-3: Panel Methods C-4: Thin Airfoil Theory

C-1: Aerodynamics of Airfoils 1 C-2: Aerodynamics of Airfoils 2 C-3: Panel Methods C-4: Thin Airfoil Theory ROAD MAP... AE301 Aerodyamcs I UNIT C: 2-D Arfols C-1: Aerodyamcs of Arfols 1 C-2: Aerodyamcs of Arfols 2 C-3: Pael Methods C-4: Th Arfol Theory AE301 Aerodyamcs I Ut C-3: Lst of Subects Problem Solutos?

More information

Solutions to problem set ); (, ) (

Solutions to problem set ); (, ) ( Solutos to proble set.. L = ( yp p ); L = ( p p ); y y L, L = yp p, p p = yp p, + p [, p ] y y y = yp + p = L y Here we use for eaple that yp, p = yp p p yp = yp, p = yp : factors that coute ca be treated

More information

Some results and conjectures about recurrence relations for certain sequences of binomial sums.

Some results and conjectures about recurrence relations for certain sequences of binomial sums. Soe results ad coectures about recurrece relatos for certa sequeces of boal sus Joha Cgler Faultät für Matheat Uverstät We A-9 We Nordbergstraße 5 Joha Cgler@uveacat Abstract I a prevous paper [] I have

More information

Functions of Random Variables

Functions of Random Variables Fuctos of Radom Varables Chapter Fve Fuctos of Radom Varables 5. Itroducto A geeral egeerg aalyss model s show Fg. 5.. The model output (respose) cotas the performaces of a system or product, such as weght,

More information

d dt d d dt dt Also recall that by Taylor series, / 2 (enables use of sin instead of cos-see p.27 of A&F) dsin

d dt d d dt dt Also recall that by Taylor series, / 2 (enables use of sin instead of cos-see p.27 of A&F) dsin Learzato of the Swg Equato We wll cover sectos.5.-.6 ad begg of Secto 3.3 these otes. 1. Sgle mache-fte bus case Cosder a sgle mache coected to a fte bus, as show Fg. 1 below. E y1 V=1./_ Fg. 1 The admttace

More information

PGE 310: Formulation and Solution in Geosystems Engineering. Dr. Balhoff. Interpolation

PGE 310: Formulation and Solution in Geosystems Engineering. Dr. Balhoff. Interpolation PGE 30: Formulato ad Soluto Geosystems Egeerg Dr. Balhoff Iterpolato Numercal Methods wth MATLAB, Recktewald, Chapter 0 ad Numercal Methods for Egeers, Chapra ad Caale, 5 th Ed., Part Fve, Chapter 8 ad

More information

A Conventional Approach for the Solution of the Fifth Order Boundary Value Problems Using Sixth Degree Spline Functions

A Conventional Approach for the Solution of the Fifth Order Boundary Value Problems Using Sixth Degree Spline Functions Appled Matheatcs, 1, 4, 8-88 http://d.do.org/1.4/a.1.448 Publshed Ole Aprl 1 (http://www.scrp.org/joural/a) A Covetoal Approach for the Soluto of the Ffth Order Boudary Value Probles Usg Sth Degree Sple

More information

2.28 The Wall Street Journal is probably referring to the average number of cubes used per glass measured for some population that they have chosen.

2.28 The Wall Street Journal is probably referring to the average number of cubes used per glass measured for some population that they have chosen. .5 x 54.5 a. x 7. 786 7 b. The raked observatos are: 7.4, 7.5, 7.7, 7.8, 7.9, 8.0, 8.. Sce the sample sze 7 s odd, the meda s the (+)/ 4 th raked observato, or meda 7.8 c. The cosumer would more lkely

More information

Standard Deviation for PDG Mass Data

Standard Deviation for PDG Mass Data 4 Dec 06 Stadard Devato for PDG Mass Data M. J. Gerusa Retred, 47 Clfde Road, Worghall, HP8 9JR, UK. gerusa@aol.co, phoe: +(44) 844 339754 Abstract Ths paper aalyses the data for the asses of eleetary

More information

,...R) where r = H (1.4) + Tn + Vof. etic energy terms are: here. ZA ZB Vee = & Vnn = (1.6) (1.4) H = Te + Tn + Ven + Vee + Vnn. i A r i.

,...R) where r = H (1.4) + Tn + Vof. etic energy terms are: here. ZA ZB Vee = & Vnn = (1.6) (1.4) H = Te + Tn + Ven + Vee + Vnn. i A r i. where r H r, r (r,,...r), r, RE R (r, RR),.., R represet theelectros. electro (.3) ad uclear coor,all,.ucle ates of ad all Itutvely, ollowgdates, SE: respectvely, ad H (r, R) E (r, R), we feel t are very

More information

The Geometric Least Squares Fitting Of Ellipses

The Geometric Least Squares Fitting Of Ellipses IOSR Joural of Matheatcs (IOSR-JM) e-issn: 78-578, p-issn: 39-765X. Volue 4, Issue 3 Ver.I (May - Jue 8), PP -8 www.osrourals.org Abdellatf Bettayeb Departet of Geeral Studes, Jubal Idustral College, Jubal

More information

1 Onto functions and bijections Applications to Counting

1 Onto functions and bijections Applications to Counting 1 Oto fuctos ad bectos Applcatos to Coutg Now we move o to a ew topc. Defto 1.1 (Surecto. A fucto f : A B s sad to be surectve or oto f for each b B there s some a A so that f(a B. What are examples of

More information

Hamilton s principle for non-holonomic systems

Hamilton s principle for non-holonomic systems Das Hamltosche Przp be chtholoome Systeme, Math. A. (935), pp. 94-97. Hamlto s prcple for o-holoomc systems by Georg Hamel Berl Traslate by: D. H. Delphech I the paper Le prcpe e Hamlto et l holoomsme,

More information

b) Choose one o f the graphs in part a that did b) is the atomic number o f

b) Choose one o f the graphs in part a that did b) is the atomic number o f REVIEW ad f^l^h^s. Ths table shows soe Northwest Coast artsts ad ther cultural hertage. Artst Hertage Bob Depse Tlgt Doroth Grat Hada Bll Hel Tssha Joh Joseph Squash Judth P. Morga Gtxsa Bll Red Hada a)

More information

An Expansion of the Derivation of the Spline Smoothing Theory Alan Kaylor Cline

An Expansion of the Derivation of the Spline Smoothing Theory Alan Kaylor Cline A Epaso of the Derato of the Sple Smoothg heory Ala Kaylor Cle he classc paper "Smoothg by Sple Fctos", Nmersche Mathematk 0, 77-83 967) by Chrsta Resch showed that atral cbc sples were the soltos to a

More information

Beam Warming Second-Order Upwind Method

Beam Warming Second-Order Upwind Method Beam Warmg Secod-Order Upwd Method Petr Valeta Jauary 6, 015 Ths documet s a part of the assessmet work for the subject 1DRP Dfferetal Equatos o Computer lectured o FNSPE CTU Prague. Abstract Ths documet

More information

A NEW FINITE ELEMENT CONSIDERING SHEAR LAG

A NEW FINITE ELEMENT CONSIDERING SHEAR LAG Bullet of the raslvaa Uversty of Braşov CIBv 204 Vol. 7 (56) Specal Issue No. - 204 A NEW FINIE EEMEN CONSIDERING SHEAR AG A. PROIC M. VOJNIC PURCAR D. UIC Abstract: A ew model of descrbg the shear lag

More information

Chapt. 9 Systems of Particles and Conservation of Linear Momentum

Chapt. 9 Systems of Particles and Conservation of Linear Momentum Chapt. 9 Systes o Patcles ad Coseato o Lea oetu 9. Lea oetu ad Its Coseato 9. Isolated Syste lea oetu: P F dp d( d a solated syste F ext 0 dp dp F F dp dp d F F 0 0 ( P P P tot cost p p p p the law o coseato

More information

Mu Sequences/Series Solutions National Convention 2014

Mu Sequences/Series Solutions National Convention 2014 Mu Sequeces/Seres Solutos Natoal Coveto 04 C 6 E A 6C A 6 B B 7 A D 7 D C 7 A B 8 A B 8 A C 8 E 4 B 9 B 4 E 9 B 4 C 9 E C 0 A A 0 D B 0 C C Usg basc propertes of arthmetc sequeces, we fd a ad bm m We eed

More information

1 Lyapunov Stability Theory

1 Lyapunov Stability Theory Lyapuov Stablty heory I ths secto we cosder proofs of stablty of equlbra of autoomous systems. hs s stadard theory for olear systems, ad oe of the most mportat tools the aalyss of olear systems. It may

More information

Mechanics of Materials CIVL 3322 / MECH 3322

Mechanics of Materials CIVL 3322 / MECH 3322 Mechacs of Materals CVL / MECH Cetrods ad Momet of erta Calculatos Cetrods = A = = = A = = Cetrod ad Momet of erta Calculatos z= z A = = Parallel As Theorem f ou kow the momet of erta about a cetrodal

More information

Basic Concepts in Numerical Analysis November 6, 2017

Basic Concepts in Numerical Analysis November 6, 2017 Basc Cocepts Nuercal Aalyss Noveber 6, 7 Basc Cocepts Nuercal Aalyss Larry Caretto Mecacal Egeerg 5AB Sear Egeerg Aalyss Noveber 6, 7 Outle Revew last class Mdter Exa Noveber 5 covers ateral o deretal

More information

The Mathematical Appendix

The Mathematical Appendix The Mathematcal Appedx Defto A: If ( Λ, Ω, where ( λ λ λ whch the probablty dstrbutos,,..., Defto A. uppose that ( Λ,,..., s a expermet type, the σ-algebra o λ λ λ are defed s deoted by ( (,,...,, σ Ω.

More information

On the Modeling and Simulation of Collision and Collision-Free Motion for Planar Robotic Arm Galia V. Tzvetkova

On the Modeling and Simulation of Collision and Collision-Free Motion for Planar Robotic Arm Galia V. Tzvetkova Iteratoal Joural of Egeerg Research & Scece (IJOER [Vol-, Issue-9, December- 25] O the Modelg ad Smulato of Collso ad Collso-Free Moto for Plaar Robotc Arm Gala V. Tzvetova Isttute of mechacs, Bulgara

More information

THE TRUNCATED RANDIĆ-TYPE INDICES

THE TRUNCATED RANDIĆ-TYPE INDICES Kragujeac J Sc 3 (00 47-5 UDC 547:54 THE TUNCATED ANDIĆ-TYPE INDICES odjtaba horba, a ohaad Al Hossezadeh, b Ia uta c a Departet of atheatcs, Faculty of Scece, Shahd ajae Teacher Trag Uersty, Tehra, 785-3,

More information

Computational Geometry

Computational Geometry Problem efto omputatoal eometry hapter 6 Pot Locato Preprocess a plaar map S. ve a query pot p, report the face of S cotag p. oal: O()-sze data structure that eables O(log ) query tme. pplcato: Whch state

More information

The internal structure of natural numbers, one method for the definition of large prime numbers, and a factorization test

The internal structure of natural numbers, one method for the definition of large prime numbers, and a factorization test Fal verso The teral structure of atural umbers oe method for the defto of large prme umbers ad a factorzato test Emmaul Maousos APM Isttute for the Advacemet of Physcs ad Mathematcs 3 Poulou str. 53 Athes

More information

1 0, x? x x. 1 Root finding. 1.1 Introduction. Solve[x^2-1 0,x] {{x -1},{x 1}} Plot[x^2-1,{x,-2,2}] 3

1 0, x? x x. 1 Root finding. 1.1 Introduction. Solve[x^2-1 0,x] {{x -1},{x 1}} Plot[x^2-1,{x,-2,2}] 3 Adrew Powuk - http://www.powuk.com- Math 49 (Numercal Aalyss) Root fdg. Itroducto f ( ),?,? Solve[^-,] {{-},{}} Plot[^-,{,-,}] Cubc equato https://e.wkpeda.org/wk/cubc_fucto Quartc equato https://e.wkpeda.org/wk/quartc_fucto

More information

Third handout: On the Gini Index

Third handout: On the Gini Index Thrd hadout: O the dex Corrado, a tala statstca, proposed (, 9, 96) to measure absolute equalt va the mea dfferece whch s defed as ( / ) where refers to the total umber of dvduals socet. Assume that. The

More information

Centroids Method of Composite Areas

Centroids Method of Composite Areas Cetrods Method of Composte reas small boy swallowed some cos ad was take to a hosptal. Whe hs gradmother telephoed to ask how he was a urse sad 'No chage yet'. Cetrods Prevously, we developed a geeral

More information

Solving the fuzzy shortest path problem on networks by a new algorithm

Solving the fuzzy shortest path problem on networks by a new algorithm Proceedgs of the 0th WSEAS Iteratoal Coferece o FUZZY SYSTEMS Solvg the fuzzy shortest path proble o etworks by a ew algorth SADOAH EBRAHIMNEJAD a, ad REZA TAVAKOI-MOGHADDAM b a Departet of Idustral Egeerg,

More information

Maps on Triangular Matrix Algebras

Maps on Triangular Matrix Algebras Maps o ragular Matrx lgebras HMED RMZI SOUROUR Departmet of Mathematcs ad Statstcs Uversty of Vctora Vctora, BC V8W 3P4 CND sourour@mathuvcca bstract We surveys results about somorphsms, Jorda somorphsms,

More information

Projectile Motion. Parabolic Motion curved motion in the shape of a parabola. In the y direction, the equation of motion has a t 2.

Projectile Motion. Parabolic Motion curved motion in the shape of a parabola. In the y direction, the equation of motion has a t 2. Projectle Moton Phc Inentor Parabolc Moton cured oton n the hape of a parabola. In the drecton, the equaton of oton ha a t ter Projectle Moton the parabolc oton of an object, where the horzontal coponent

More information

{ }{ ( )} (, ) = ( ) ( ) ( ) Chapter 14 Exercises in Sampling Theory. Exercise 1 (Simple random sampling): Solution:

{ }{ ( )} (, ) = ( ) ( ) ( ) Chapter 14 Exercises in Sampling Theory. Exercise 1 (Simple random sampling): Solution: Chapter 4 Exercses Samplg Theory Exercse (Smple radom samplg: Let there be two correlated radom varables X ad A sample of sze s draw from a populato by smple radom samplg wthout replacemet The observed

More information

ONE GENERALIZED INEQUALITY FOR CONVEX FUNCTIONS ON THE TRIANGLE

ONE GENERALIZED INEQUALITY FOR CONVEX FUNCTIONS ON THE TRIANGLE Joural of Pure ad Appled Mathematcs: Advaces ad Applcatos Volume 4 Number 205 Pages 77-87 Avalable at http://scetfcadvaces.co. DOI: http://.do.org/0.8642/jpamaa_7002534 ONE GENERALIZED INEQUALITY FOR CONVEX

More information

Centers of Gravity - Centroids

Centers of Gravity - Centroids RCH Note Set 9. S205ab Ceters of Gravt - Cetrods Notato: C Fz L O Q Q t tw = ame for area = desgato for chael secto = ame for cetrod = force compoet the z drecto = ame for legth = ame for referece org

More information

Camera calibration & radiometry

Camera calibration & radiometry Caera calbrato & radoetr Readg: Chapter 2, ad secto 5.4, Forsth & oce Chapter, Hor Optoal readg: Chapter 4, Forsth & oce Sept. 2, 22 MI 6.8/6.866 rofs. Freea ad Darrell Req: F 2, 5.4, H Opt: F 4 Req: F

More information

VŠB Technical University of Ostrava Faculty of Mechanical Engineering STATICS

VŠB Technical University of Ostrava Faculty of Mechanical Engineering STATICS VŠB Techcal Uverst of Ostrava acult of echacal Egeerg STATICS Ostrava 0 Geeral Prcples VSB-Techcal Uverst of Ostrava has take part several teratoal programs focused o studet echages The umber of teratoal

More information

CURVE FITTING LEAST SQUARES METHOD

CURVE FITTING LEAST SQUARES METHOD Nuercl Alss for Egeers Ger Jord Uverst CURVE FITTING Although, the for of fucto represetg phscl sste s kow, the fucto tself ot be kow. Therefore, t s frequetl desred to ft curve to set of dt pots the ssued

More information

Physic 231 Lecture 14

Physic 231 Lecture 14 Physc 3 Lecture 4 Man ponts o last lecture: Ipulses: orces that last only a short te Moentu p Ipulse-Moentu theore F t p ( ) Ipulse-Moentu theore ptot, p, p, p, p, ptot, Moentu and external orces F p ext

More information

Derivation of 3-Point Block Method Formula for Solving First Order Stiff Ordinary Differential Equations

Derivation of 3-Point Block Method Formula for Solving First Order Stiff Ordinary Differential Equations Dervato of -Pot Block Method Formula for Solvg Frst Order Stff Ordary Dfferetal Equatos Kharul Hamd Kharul Auar, Kharl Iskadar Othma, Zara Bb Ibrahm Abstract Dervato of pot block method formula wth costat

More information

1.3 Hence, calculate a formula for the force required to break the bond (i.e. the maximum value of F)

1.3 Hence, calculate a formula for the force required to break the bond (i.e. the maximum value of F) EN40: Dynacs and Vbratons Hoework 4: Work, Energy and Lnear Moentu Due Frday March 6 th School of Engneerng Brown Unversty 1. The Rydberg potental s a sple odel of atoc nteractons. It specfes the potental

More information

3.1 Introduction to Multinomial Logit and Probit

3.1 Introduction to Multinomial Logit and Probit ES3008 Ecooetrcs Lecture 3 robt ad Logt - Multoal 3. Itroducto to Multoal Logt ad robt 3. Estato of β 3. Itroducto to Multoal Logt ad robt The ultoal Logt odel s used whe there are several optos (ad therefore

More information

Lecture 07: Poles and Zeros

Lecture 07: Poles and Zeros Lecture 07: Poles ad Zeros Defto of poles ad zeros The trasfer fucto provdes a bass for determg mportat system respose characterstcs wthout solvg the complete dfferetal equato. As defed, the trasfer fucto

More information

Introduction to local (nonparametric) density estimation. methods

Introduction to local (nonparametric) density estimation. methods Itroducto to local (oparametrc) desty estmato methods A slecture by Yu Lu for ECE 66 Sprg 014 1. Itroducto Ths slecture troduces two local desty estmato methods whch are Parze desty estmato ad k-earest

More information

Algorithms Theory, Solution for Assignment 2

Algorithms Theory, Solution for Assignment 2 Juor-Prof. Dr. Robert Elsässer, Marco Muñz, Phllp Hedegger WS 2009/200 Algorthms Theory, Soluto for Assgmet 2 http://lak.formatk.u-freburg.de/lak_teachg/ws09_0/algo090.php Exercse 2. - Fast Fourer Trasform

More information

Engineering Mechanics Dynamics & Vibrations. Engineering Mechanics Dynamics & Vibrations Plane Motion of a Rigid Body: Equations of Motion

Engineering Mechanics Dynamics & Vibrations. Engineering Mechanics Dynamics & Vibrations Plane Motion of a Rigid Body: Equations of Motion 1/5/013 Egieerig Mechaics Dyaics ad Vibratios Egieerig Mechaics Dyaics & Vibratios Egieerig Mechaics Dyaics & Vibratios Plae Motio of a Rigid Body: Equatios of Motio Motio of a rigid body i plae otio is

More information

L5 Polynomial / Spline Curves

L5 Polynomial / Spline Curves L5 Polyomal / Sple Curves Cotets Coc sectos Polyomal Curves Hermte Curves Bezer Curves B-Sples No-Uform Ratoal B-Sples (NURBS) Mapulato ad Represetato of Curves Types of Curve Equatos Implct: Descrbe a

More information

C.11 Bang-bang Control

C.11 Bang-bang Control Itroucto to Cotrol heory Iclug Optmal Cotrol Nguye a e -.5 C. Bag-bag Cotrol. Itroucto hs chapter eals wth the cotrol wth restrctos: s boue a mght well be possble to have scotutes. o llustrate some of

More information

best estimate (mean) for X uncertainty or error in the measurement (systematic, random or statistical) best

best estimate (mean) for X uncertainty or error in the measurement (systematic, random or statistical) best Error Aalyss Preamble Wheever a measuremet s made, the result followg from that measuremet s always subject to ucertaty The ucertaty ca be reduced by makg several measuremets of the same quatty or by mprovg

More information

Quantization in Dynamic Smarandache Multi-Space

Quantization in Dynamic Smarandache Multi-Space Quatzato Dyamc Smaradache Mult-Space Fu Yuhua Cha Offshore Ol Research Ceter, Beg, 7, Cha (E-mal: fuyh@cooc.com.c ) Abstract: Dscussg the applcatos of Dyamc Smaradache Mult-Space (DSMS) Theory. Supposg

More information

Chapter 8. Momentum Impulse and Collisions. Analysis of motion: 2 key ideas. Newton s laws of motion. Conservation of Energy

Chapter 8. Momentum Impulse and Collisions. Analysis of motion: 2 key ideas. Newton s laws of motion. Conservation of Energy Chapter 8 Moentu Ipulse and Collsons Analyss o oton: key deas Newton s laws o oton Conseraton o Energy Newton s Laws st Law: An object at rest or traelng n unor oton wll rean at rest or traelng n unor

More information

Analysis of Lagrange Interpolation Formula

Analysis of Lagrange Interpolation Formula P IJISET - Iteratoal Joural of Iovatve Scece, Egeerg & Techology, Vol. Issue, December 4. www.jset.com ISS 348 7968 Aalyss of Lagrage Iterpolato Formula Vjay Dahya PDepartmet of MathematcsMaharaja Surajmal

More information

The Mathematics of Portfolio Theory

The Mathematics of Portfolio Theory The Matheatcs of Portfolo Theory The rates of retur of stocks, ad are as follows Market odtos state / scearo) earsh Neutral ullsh Probablty 0. 0.5 0.3 % 5% 9% -3% 3% % 5% % -% Notato: R The retur of stock

More information

Block-Based Compact Thermal Modeling of Semiconductor Integrated Circuits

Block-Based Compact Thermal Modeling of Semiconductor Integrated Circuits Block-Based Compact hermal Modelg of Semcoductor Itegrated Crcuts Master s hess Defese Caddate: Jg Ba Commttee Members: Dr. Mg-Cheg Cheg Dr. Daqg Hou Dr. Robert Schllg July 27, 2009 Outle Itroducto Backgroud

More information

COMPROMISE HYPERSPHERE FOR STOCHASTIC DOMINANCE MODEL

COMPROMISE HYPERSPHERE FOR STOCHASTIC DOMINANCE MODEL Sebasta Starz COMPROMISE HYPERSPHERE FOR STOCHASTIC DOMINANCE MODEL Abstract The am of the work s to preset a method of rakg a fte set of dscrete radom varables. The proposed method s based o two approaches:

More information

MA 524 Homework 6 Solutions

MA 524 Homework 6 Solutions MA 524 Homework 6 Solutos. Sce S(, s the umber of ways to partto [] to k oempty blocks, ad c(, s the umber of ways to partto to k oempty blocks ad also the arrage each block to a cycle, we must have S(,

More information

Arithmetic Mean and Geometric Mean

Arithmetic Mean and Geometric Mean Acta Mathematca Ntresa Vol, No, p 43 48 ISSN 453-6083 Arthmetc Mea ad Geometrc Mea Mare Varga a * Peter Mchalča b a Departmet of Mathematcs, Faculty of Natural Sceces, Costate the Phlosopher Uversty Ntra,

More information

Investigation of Partially Conditional RP Model with Response Error. Ed Stanek

Investigation of Partially Conditional RP Model with Response Error. Ed Stanek Partally Codtoal Radom Permutato Model 7- vestgato of Partally Codtoal RP Model wth Respose Error TRODUCTO Ed Staek We explore the predctor that wll result a smple radom sample wth respose error whe a

More information

Rademacher Complexity. Examples

Rademacher Complexity. Examples Algorthmc Foudatos of Learg Lecture 3 Rademacher Complexty. Examples Lecturer: Patrck Rebesch Verso: October 16th 018 3.1 Itroducto I the last lecture we troduced the oto of Rademacher complexty ad showed

More information

We have already referred to a certain reaction, which takes place at high temperature after rich combustion.

We have already referred to a certain reaction, which takes place at high temperature after rich combustion. ME 41 Day 13 Topcs Chemcal Equlbrum - Theory Chemcal Equlbrum Example #1 Equlbrum Costats Chemcal Equlbrum Example #2 Chemcal Equlbrum of Hot Bured Gas 1. Chemcal Equlbrum We have already referred to a

More information

Cubic Nonpolynomial Spline Approach to the Solution of a Second Order Two-Point Boundary Value Problem

Cubic Nonpolynomial Spline Approach to the Solution of a Second Order Two-Point Boundary Value Problem Joural of Amerca Scece ;6( Cubc Nopolyomal Sple Approach to the Soluto of a Secod Order Two-Pot Boudary Value Problem W.K. Zahra, F.A. Abd El-Salam, A.A. El-Sabbagh ad Z.A. ZAk * Departmet of Egeerg athematcs

More information

Dynamic Analysis of Axially Beam on Visco - Elastic Foundation with Elastic Supports under Moving Load

Dynamic Analysis of Axially Beam on Visco - Elastic Foundation with Elastic Supports under Moving Load Dyamc Aalyss of Axally Beam o Vsco - Elastc Foudato wth Elastc Supports uder Movg oad Saeed Mohammadzadeh, Seyed Al Mosayeb * Abstract: For dyamc aalyses of ralway track structures, the algorthm of soluto

More information

A Remark on the Uniform Convergence of Some Sequences of Functions

A Remark on the Uniform Convergence of Some Sequences of Functions Advaces Pure Mathematcs 05 5 57-533 Publshed Ole July 05 ScRes. http://www.scrp.org/joural/apm http://dx.do.org/0.436/apm.05.59048 A Remark o the Uform Covergece of Some Sequeces of Fuctos Guy Degla Isttut

More information

Department of Mechanical Engineering ME 322 Mechanical Engineering Thermodynamics. Ideal Gas Mixtures. Lecture 31

Department of Mechanical Engineering ME 322 Mechanical Engineering Thermodynamics. Ideal Gas Mixtures. Lecture 31 Departet of echacal Egeerg E 322 echacal Egeerg Therodyacs Ideal Gas xtures Lecture 31 xtures Egeerg Applcatos atural gas ethae, ethae, propae, butae, troge, hydroge, carbo doxde, ad others Refrgerats

More information