Bulk Viscous Fluid Bianchi Type - I String Cosmological Model in General Relativity

Size: px
Start display at page:

Download "Bulk Viscous Fluid Bianchi Type - I String Cosmological Model in General Relativity"

Transcription

1 IOSR Joural o athematcs (IOSR-J) e-issn: , p-issn: 39-75X. Volume, Issue Ver. IV (ar. - pr. 0), PP -5 Bulk Vscous Flud Bach ype - I Strg Cosmologcal odel Geeral Relatvty Varu Humad, Harsh Nagar, Sapa Shrmal 3 Research Scholar o ewar Uversty, Chttorgarh (Rajastha), Ida. Departmet o athematcs, ewar Uversty, Chttorgarh (Rajastha), Ida. 3 Departmet o athematcs, Pacc cademy o Hgher Educato & Research Uversty, Udapur (Rajastha), Ida. bstract: I ths paper we have vestgated Bulk vscous lud Bach ype - I strg cosmologcal model geeral relatvty. o get a determstc model, t s assumed that ξθ = (costat), where ξ s the coecet o bulk vscosty s, θ s the scalar o expaso ad a relato betwee metrc potetal B =.he physcal ad geometrcal aspects o the model are also cussed. Key wor: Bach ype-i models, bulk vscosty, scalar o expaso. I. Itroducto It s a challegg problem to determe the exact physcal stuato at the very early stages o the ormato o our uverse. Strg cosmologcal models are wdely studed recet tmes because o ther prme role the descrpto o the evoluto o the early phase o uverse. hese arse durg the phase trasto ater the bg bag exploso as the temperature goes dow below some crtcal temperature as predcted by grad ued theores [,, 3]. It s beleved that cosmc strgs may act as gravtatoal leses ad these objects are cosdered as possble see or ormato o galaxes. he geeral relatvstc treatmet o strg was tated by Leteler[4] ad Stachel [5]. Leteler [4] has obtaed the soluto o Este s eld equato or a cloud strg wth sphercal, plae ad cyldrcal symmetry. he 983, he solved Este s eld equato or cloud massve strg ad obtas cosmologcal models Bach ype-i ad Katowsk-Sachs sphase tme. kekar ad patel [,7]. Bal ad yag [8] have obtaed a cyldrcally symmetrc homogeeous cosmologcal model wth electromagetc eld or perect lud trbuto. Beerjee et al. [9] have vestgated a axally symmetrc Bach ype I strg dust cosmologcal model presece ad absece o magetc eld. Bal et al.[0,,] have vestgated Bach ype I magetzed strg cosmologcal models. pawar et al. [3] have vestgated about deret aspects o plae symmetrc Bulk vscous lud strg dust magetzed cosmologcal model geeral relatvty. Saha et al. [4] ad Saha [5] have studed Bach ype I cosmologcal model presece o magetc lux deret cotexts. Recetly yag et al. [] vestgated Bulk vscous lud plae symmetrc strg dust magetzed cosmologcal model geeral relatvty. I ths paper, we have vestgated Bulk vscous lud Bach ype - I Strg cosmologcal model geeral relatvty. equatoξθ = (costat), where ξ s the coecet o bulk vscosty, θ s the scalar o expaso ad a relato betwee metrc potetals B = are assumed. he physcal ad geometrcal aspects o the model are also cussed. etrc d Feld Equato We cosder Bach ype - I metrc o the orm dt ( dx dy ) B dz... () where ad B are ucto o tme oly. he eergy mometum tesor or a cloud o strg wth bulk vscosty s u u x x u u g )... () j j ( j where s the rest eergy desty o the cloud o strg wth partcles attached to them wth s the rest eergy desty o partcle ad s the teso desty o the cloud o strgs, u ; s the scalar o expaso ad s the coecet o bulk vscosty. he vector u descrbes the low velocty vector ad x represet a drecto o asotropy.e. the drecto o strgs, satsy the stadard relato. u u x x,u x 0... (3) he expresso or scalar o expaso ad shear scalar are DOI: / Page

2 Bulk Vscous Flud Bach ype - I Strg Cosmologcal odel I Geeral Relatvty B u ; B... (4) B B... (5) he Este's eld equato ( gravtatoal uts c =, 8G = ) or a system o strg R Rg... () For the metrc (), Este's eld equato's ca be wrtte as B B B B B B... (7)... (8)... (9) Where a over dot sta or the rst ad double dot or the secod dervatve wth respect to cosmc tme t. Soluto O he Feld Equatos he eld equatos (7) to (9) are three equatos ve ukows parameters, B,, ad. I order to obta a determate soluto, we have assumed two codtos: ξθ = (costat) (0).e. the coecet o bulk vscosty s versely proportoal to expaso (θ). () B = () relato betwee metrc potetals ad B, Where s costat. From equato (7), (0) ad (), we get hs lea to Let us assume () d d /,... () / d d Usg (3) ad (4) equato (), we get d d ter tegrato, we get K Where K s the costat o tegrato. (4) (3)... (5) DOI: / Page

3 Bulk Vscous Flud Bach ype - I Strg Cosmologcal odel I Geeral Relatvty DOI: / Page K... () K... (7) Equato (7) lea to d K dt Hece the model () s reduce to dz dy dx d K... (8) ter usg a sutable trasormato o coordates the model (8) reduce to dz dy dx d K... (9) Where =, x = X, y = Y, z = Z Some Physcal d Geometrcal spects O he odel For the model o equato (9), the other physcal ad geometrcal parameters ca be easly obtaed. he eergy desty, the strg teso desty, the scalar o expaso, the coecet o bulk vscosty, ad the shear scalar are respectvely gve by K... (0) k... () K... () K... (3) K... (4)

4 Bulk Vscous Flud Bach ype - I Strg Cosmologcal odel I Geeral Relatvty DOI: / Page cosat... (5) I the absece o bulk vscosty.e. whe 0,the le elemet () reduce to dz dy dx d K () he eergy desty, the strg teso desty, the scalar o expaso, the coecet o bulk vscosty, ad the shear scalar are respectvely gve by K... (7) k... (8) K... (9) 0 (30) K... (3) cosat... (3) II. Cocluso he eergy codto ρ 0 the presece o bulk vscous lud lea to 0 K (33) hus the model (9) exsts durg the tme spa gve by (33). Whe, ad due to presece o bulk vscous lud. Sce 0 Lm Hece model does ot sotropze or large value o. s 0 the ρ, θ, the model starts wth a bg bag at =0. he eergy codto ρ 0 or the model () lea to

5 Bulk Vscous Flud Bach ype - I Strg Cosmologcal odel I Geeral Relatvty K 0 (34) hus the model () exsts durg the tme spa gve by (34). he model starts bg bag at =0 ad the Lm 0 expaso the model decreases as tme creases,hece model does ot sotropze or large value o. Reereces []. Kbble,.W.B., Some mplcatos a cosmologcal phase-trasto, Phys. Rep. 7, 83 (980). []. Zel sdovch, Ya. B., Kokzarev, I. Yu ad Oku. L. B. Cosmologcal cosequeces o a spotaeous breakdow o a crete symmetry, Z.Sov.phys. JEP.40, -5 (975). [3]. Vlek,.,Cosmc strgs Phys. Rev. D 4, 08 (983). [4]. Leteler, P.S., Strg cosmologes, Phys. Rev. D 0, 94 (979). [5]. Stachel, J., hckeg the strg I the strg perect dust, Phys. Rev. D, 7 (980). []. kekar, R. ad Patel, L.K., Some exact solutos o strg cosmology Bach III space tme, Ge. Rel. Grav. 4, 397 (99). [7]. kekar, R. ad Patel, L.K.,: Some exact solutos Bach VIo strg cosmology, Pramaa. J. Phys. 4, 483 (994). [8]. Bal, R. ad yag,., Some exact solutos Bach VIo strg cosmology, Ge. Re. Grav., (989). [9]. Baerjee,., Sayal,.K. ad Chakraborty, S., Strg cosmology Bach I space tme, Pramaa-J. Phys. 34, (990). [0]. Bal, R. ad Upadhaya, R.D., LRS Bach type I strg dust magetzed cosmologcal model geeral relatvty, strophys. Space Sc. 83, 97 (003). []. Bal, R. ad jal,: Bach type I magetzed strg cosmologcal model geeral relatvty, strophys. Space Sc. 30, 0 (00). []. Bal, R., Pareek, U.K. ad Pradha,., Bach type I massve strg magetzed barotropc perect cosmologcal model geeral relatvty,ch. Phys. Lett. 4, 585 (007). [3]. Pawar, D.D., Bhaware, S.W. ad Deshmukh,.G., Bulk Vscous Flud plae symmetrc strg dust magetzed cosmologcal model geeral relatvty, It. J. heor. Phys. 47, 599 (008). [4]. Saha, B. ad Vsescu,., Strg cosmologcal model the presece o a magetc lux, strophys. Space Sc. 35, 99, (008). [5]. Saha, B., strophys. Iteractg scalar ad Spor el Bach type I uverse eld wth mageto- lud, Space Sc. 99, 49, (005). []. yag,. ad Sharma, K., Bulk Vscous lud plae symmetrc strg dust magetzed cosmologcal model geeral relatvty, Id. cad. o athematcs. 3,, (00). DOI: / Page

Bianchi Type I Bulk Viscous Fluid String Dust Cosmological Model with Magnetic Field in Bimetric Theory of Gravitation

Bianchi Type I Bulk Viscous Fluid String Dust Cosmological Model with Magnetic Field in Bimetric Theory of Gravitation valable at http://pvamu.edu/aam ppl. ppl. Math. ISSN: 9-966 Vol. 5, Issue (Jue 00) pp. 96-09 (Prevously, Vol. 5, No. ) pplcatos ad ppled Mathematcs: Iteratoal Joural (M) ach ype I ulk Vscous Flud Strg

More information

Expanding & Shearing Biachi Type-I Non-Static Cosmological Model in General Relativity

Expanding & Shearing Biachi Type-I Non-Static Cosmological Model in General Relativity 769 Expadg & Shearg ach ype-i No-Statc osmologcal Model Geeral Relatvty Reea Mathur, Gaedra P. Sgh * & tul yag Departmet of Mathematcs ad Statstcs, MohaLal Suhada Uversty, Udapur Departmet of Mathematcs,

More information

Bianchi Type-III String Cosmological Models in The Presence of Magnetic Field in General Relativity

Bianchi Type-III String Cosmological Models in The Presence of Magnetic Field in General Relativity Iteratoal Joural of Scetfc & Egeerg Research, Volume, Issue, November-0 Bach ye-iii Strg Cosmologcal odels he Presece of agetc Feld Geeral Relatvty adalkar S.P., Samdurkar S.W. ad Gawade S.P. Deartmet

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

BULK VISCOUS BIANCHI TYPE IX STRING DUST COSMOLOGICAL MODEL WITH TIME DEPENDENT TERM SWATI PARIKH Department of Mathematics and Statistics,

BULK VISCOUS BIANCHI TYPE IX STRING DUST COSMOLOGICAL MODEL WITH TIME DEPENDENT TERM SWATI PARIKH Department of Mathematics and Statistics, UL VISCOUS INCHI YPE IX SRING DUS COSMOLOGICL MODEL WIH IME DEPENDEN ERM SWI PRIH Department of Mathematcs and Statstcs, Unversty College of Scence, MLSU, Udapur, 3300, Inda UL YGI Department of Mathematcs

More information

Kantowski-Sachs Cosmological Model in f(r,t) Theory of Gravity

Kantowski-Sachs Cosmological Model in f(r,t) Theory of Gravity he Afrca Revew of Physcs (05 0:009 9 Katows-Sachs Cosologcal Model f(r, heory of Gravty V. U. M. Rao,* ad G. Suryaarayaa Deartet of Aled Matheatcs, Adhra Uversty, Vsahaata, Ida Deartet of Matheatcs, ANIS,

More information

Bianchi Type II Stiff Fluid Tilted Cosmological Model in General Relativity

Bianchi Type II Stiff Fluid Tilted Cosmological Model in General Relativity Ieraoal Joural of Mahemacs esearch. IN 0976-50 Volume 6, Number (0), pp. 6-7 Ieraoal esearch Publcao House hp://www.rphouse.com Bach ype II ff Flud led Cosmologcal Model Geeral elay B. L. Meea Deparme

More information

Estimation of Stress- Strength Reliability model using finite mixture of exponential distributions

Estimation of Stress- Strength Reliability model using finite mixture of exponential distributions Iteratoal Joural of Computatoal Egeerg Research Vol, 0 Issue, Estmato of Stress- Stregth Relablty model usg fte mxture of expoetal dstrbutos K.Sadhya, T.S.Umamaheswar Departmet of Mathematcs, Lal Bhadur

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

Perfect Fluid Cosmological Model in the Frame Work Lyra s Manifold

Perfect Fluid Cosmological Model in the Frame Work Lyra s Manifold Prespacetme Journal December 06 Volume 7 Issue 6 pp. 095-099 Pund, A. M. & Avachar, G.., Perfect Flud Cosmologcal Model n the Frame Work Lyra s Manfold Perfect Flud Cosmologcal Model n the Frame Work Lyra

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

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

4 Inner Product Spaces

4 Inner Product Spaces 11.MH1 LINEAR ALGEBRA Summary Notes 4 Ier Product Spaces Ier product s the abstracto to geeral vector spaces of the famlar dea of the scalar product of two vectors or 3. I what follows, keep these key

More information

Generalized Ideal Gas Equations for Structureful Universe

Generalized Ideal Gas Equations for Structureful Universe Etropy, 2006, 8,175-181 Etropy ISSN 1099-4300 www.mdp.org/etropy/ Full paper Geeralzed Ideal Gas Equatos for Structureful Uverse Shahd N. Afrd 1 ad Khald Kha 2 Departmet of Physcs, Quad--Azam Uversty,

More information

Carbonyl Groups. University of Chemical Technology, Beijing , PR China;

Carbonyl Groups. University of Chemical Technology, Beijing , PR China; Electroc Supplemetary Materal (ESI) for Physcal Chemstry Chemcal Physcs Ths joural s The Ower Socetes 0 Supportg Iformato A Theoretcal Study of Structure-Solublty Correlatos of Carbo Doxde Polymers Cotag

More information

EVALUATION OF FUNCTIONAL INTEGRALS BY MEANS OF A SERIES AND THE METHOD OF BOREL TRANSFORM

EVALUATION OF FUNCTIONAL INTEGRALS BY MEANS OF A SERIES AND THE METHOD OF BOREL TRANSFORM EVALUATION OF FUNCTIONAL INTEGRALS BY MEANS OF A SERIES AND THE METHOD OF BOREL TRANSFORM Jose Javer Garca Moreta Ph. D research studet at the UPV/EHU (Uversty of Basque coutry) Departmet of Theoretcal

More information

Numerical Simulations of the Complex Modied Korteweg-de Vries Equation. Thiab R. Taha. The University of Georgia. Abstract

Numerical Simulations of the Complex Modied Korteweg-de Vries Equation. Thiab R. Taha. The University of Georgia. Abstract Numercal Smulatos of the Complex Moded Korteweg-de Vres Equato Thab R. Taha Computer Scece Departmet The Uversty of Georga Athes, GA 002 USA Tel 0-542-2911 e-mal thab@cs.uga.edu Abstract I ths paper mplemetatos

More information

On Submanifolds of an Almost r-paracontact Riemannian Manifold Endowed with a Quarter Symmetric Metric Connection

On Submanifolds of an Almost r-paracontact Riemannian Manifold Endowed with a Quarter Symmetric Metric Connection Theoretcal Mathematcs & Applcatos vol. 4 o. 4 04-7 ISS: 79-9687 prt 79-9709 ole Scepress Ltd 04 O Submafolds of a Almost r-paracotact emaa Mafold Edowed wth a Quarter Symmetrc Metrc Coecto Mob Ahmad Abdullah.

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

Statistical modelling and latent variables (2)

Statistical modelling and latent variables (2) Statstcal modellg ad latet varables (2 Mxg latet varables ad parameters statstcal erece Trod Reta (Dvso o statstcs ad surace mathematcs, Departmet o Mathematcs, Uversty o Oslo State spaces We typcally

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

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

The Primitive Idempotents in

The Primitive Idempotents in Iteratoal Joural of Algebra, Vol, 00, o 5, 3 - The Prmtve Idempotets FC - I Kulvr gh Departmet of Mathematcs, H College r Jwa Nagar (rsa)-5075, Ida kulvrsheora@yahoocom K Arora Departmet of Mathematcs,

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

ESS Line Fitting

ESS Line Fitting ESS 5 014 17. Le Fttg A very commo problem data aalyss s lookg for relatoshpetwee dfferet parameters ad fttg les or surfaces to data. The smplest example s fttg a straght le ad we wll dscuss that here

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

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

Analysis of Variance with Weibull Data

Analysis of Variance with Weibull Data Aalyss of Varace wth Webull Data Lahaa Watthaacheewaul Abstract I statstcal data aalyss by aalyss of varace, the usual basc assumptos are that the model s addtve ad the errors are radomly, depedetly, ad

More information

Bivariate Vieta-Fibonacci and Bivariate Vieta-Lucas Polynomials

Bivariate Vieta-Fibonacci and Bivariate Vieta-Lucas Polynomials IOSR Joural of Mathematcs (IOSR-JM) e-issn: 78-78, p-issn: 19-76X. Volume 1, Issue Ver. II (Jul. - Aug.016), PP -0 www.osrjourals.org Bvarate Veta-Fboacc ad Bvarate Veta-Lucas Polomals E. Gokce KOCER 1

More information

Bianchi Type I Magnetized Cosmological Model in Bimetric Theory of Gravitation

Bianchi Type I Magnetized Cosmological Model in Bimetric Theory of Gravitation Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 93-966 Vol. 05 Issue (December 00) pp. 563 57 (Prevously Vol. 05 Issue 0 pp. 660 67) Applcatons and Appled Mathematcs: An Internatonal Journal (AAM)

More information

A Class of Deformed Hyperbolic Secant Distributions Using Two Parametric Functions. S. A. El-Shehawy

A Class of Deformed Hyperbolic Secant Distributions Using Two Parametric Functions. S. A. El-Shehawy A Class o Deormed Hyperbolc Secat Dstrbutos Usg Two Parametrc Fuctos S. A. El-Shehawy Departmet o Mathematcs Faculty o Scece Meoua Uversty Sheb El-om Egypt shshehawy6@yahoo.com Abstract: Ths paper presets

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

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

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

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

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

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

Solving Constrained Flow-Shop Scheduling. Problems with Three Machines

Solving Constrained Flow-Shop Scheduling. Problems with Three Machines It J Cotemp Math Sceces, Vol 5, 2010, o 19, 921-929 Solvg Costraed Flow-Shop Schedulg Problems wth Three Maches P Pada ad P Rajedra Departmet of Mathematcs, School of Advaced Sceces, VIT Uversty, Vellore-632

More information

Reflection of Plane Waves from a Free Surface of an Initially Stressed Transversely Isotropic Dissipative Medium

Reflection of Plane Waves from a Free Surface of an Initially Stressed Transversely Isotropic Dissipative Medium ppled Mathematcs 0 9- do:0.6/am.0.956 Publshed Ole September 0 (http://www.scrp.org/joural/am) Reflecto of Plae Waves from a Free Surface of a Itally Stressed Trasversely Isotropc Dsspatve Medum bstract

More information

ICS141: Discrete Mathematics for Computer Science I

ICS141: Discrete Mathematics for Computer Science I Uversty o Hw ICS: Dscrete Mthemtcs or Computer Scece I Dept. Iormto & Computer Sc., Uversty o Hw J Stelovsy bsed o sldes by Dr. Be d Dr. Stll Orgls by Dr. M. P. Fr d Dr. J.L. Gross Provded by McGrw-Hll

More information

THE ROYAL STATISTICAL SOCIETY GRADUATE DIPLOMA

THE ROYAL STATISTICAL SOCIETY GRADUATE DIPLOMA THE ROYAL STATISTICAL SOCIETY 3 EXAMINATIONS SOLUTIONS GRADUATE DIPLOMA PAPER I STATISTICAL THEORY & METHODS The Socety provdes these solutos to assst caddates preparg for the examatos future years ad

More information

Answer key to problem set # 2 ECON 342 J. Marcelo Ochoa Spring, 2009

Answer key to problem set # 2 ECON 342 J. Marcelo Ochoa Spring, 2009 Aswer key to problem set # ECON 34 J. Marcelo Ochoa Sprg, 009 Problem. For T cosder the stadard pael data model: y t x t β + α + ǫ t a Numercally compare the fxed effect ad frst dfferece estmates. b Compare

More information

Chapter 5. Curve fitting

Chapter 5. Curve fitting Chapter 5 Curve ttg Assgmet please use ecell Gve the data elow use least squares regresso to t a a straght le a power equato c a saturato-growthrate equato ad d a paraola. Fd the r value ad justy whch

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

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

CS475 Parallel Programming

CS475 Parallel Programming CS475 Parallel Programmg Deretato ad Itegrato Wm Bohm Colorado State Uversty Ecept as otherwse oted, the cotet o ths presetato s lcesed uder the Creatve Commos Attrbuto.5 lcese. Pheomea Physcs: heat, low,

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

On Signed Product Cordial Labeling

On Signed Product Cordial Labeling Appled Mathematcs 55-53 do:.436/am..6 Publshed Ole December (http://www.scrp.or/joural/am) O Sed Product Cordal Label Abstract Jayapal Baskar Babujee Shobaa Loaatha Departmet o Mathematcs Aa Uversty Chea

More information

Homework Assignment Number Eight Solutions

Homework Assignment Number Eight Solutions D Keer MSE 0 Dept o Materals Scece & Egeerg Uversty o Teessee Kovlle Homework Assgmet Number Eght Solutos Problem Fd the soluto to the ollowg system o olear algebrac equatos ear () Soluto: s Sce ths s

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

Analysis of a Repairable (n-1)-out-of-n: G System with Failure and Repair Times Arbitrarily Distributed

Analysis of a Repairable (n-1)-out-of-n: G System with Failure and Repair Times Arbitrarily Distributed Amerca Joural of Mathematcs ad Statstcs. ; (: -8 DOI:.593/j.ajms.. Aalyss of a Reparable (--out-of-: G System wth Falure ad Repar Tmes Arbtrarly Dstrbuted M. Gherda, M. Boushaba, Departmet of Mathematcs,

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

Coding Theorems on New Fuzzy Information Theory of Order α and Type β

Coding Theorems on New Fuzzy Information Theory of Order α and Type β Progress Noear yamcs ad Chaos Vo 6, No, 28, -9 ISSN: 232 9238 oe Pubshed o 8 February 28 wwwresearchmathscorg OI: http://ddoorg/22457/pdacv6a Progress Codg Theorems o New Fuzzy Iormato Theory o Order ad

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

Fractional Order Finite Difference Scheme For Soil Moisture Diffusion Equation And Its Applications

Fractional Order Finite Difference Scheme For Soil Moisture Diffusion Equation And Its Applications IOS Joural of Mathematcs (IOS-JM e-iss: 78-578. Volume 5, Issue 4 (Ja. - Feb. 3, PP -8 www.osrourals.org Fractoal Order Fte Dfferece Scheme For Sol Mosture Dffuso quato Ad Its Applcatos S.M.Jogdad, K.C.Takale,

More information

Bayesian Inferences for Two Parameter Weibull Distribution Kipkoech W. Cheruiyot 1, Abel Ouko 2, Emily Kirimi 3

Bayesian Inferences for Two Parameter Weibull Distribution Kipkoech W. Cheruiyot 1, Abel Ouko 2, Emily Kirimi 3 IOSR Joural of Mathematcs IOSR-JM e-issn: 78-578, p-issn: 9-765X. Volume, Issue Ver. II Ja - Feb. 05, PP 4- www.osrjourals.org Bayesa Ifereces for Two Parameter Webull Dstrbuto Kpkoech W. Cheruyot, Abel

More information

A Characterization of Jacobson Radical in Γ-Banach Algebras

A Characterization of Jacobson Radical in Γ-Banach Algebras Advaces Pure Matheatcs 43-48 http://dxdoorg/436/ap66 Publshed Ole Noveber (http://wwwscrporg/joural/ap) A Characterzato of Jacobso Radcal Γ-Baach Algebras Nlash Goswa Departet of Matheatcs Gauhat Uversty

More information

Generalization of the Dissimilarity Measure of Fuzzy Sets

Generalization of the Dissimilarity Measure of Fuzzy Sets Iteratoal Mathematcal Forum 2 2007 o. 68 3395-3400 Geeralzato of the Dssmlarty Measure of Fuzzy Sets Faramarz Faghh Boformatcs Laboratory Naobotechology Research Ceter vesa Research Isttute CECR Tehra

More information

The E vs k diagrams are in general a function of the k -space direction in a crystal

The E vs k diagrams are in general a function of the k -space direction in a crystal vs dagram p m m he parameter s called the crystal mometum ad s a parameter that results from applyg Schrödger wave equato to a sgle-crystal lattce. lectros travelg dfferet drectos ecouter dfferet potetal

More information

The Power Series Solution of Fingering Phenomenon Arising in Fluid Flow through Homogeneous Porous Media

The Power Series Solution of Fingering Phenomenon Arising in Fluid Flow through Homogeneous Porous Media Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 6, Issue 2 (December 2011), pp. 497 509 Applcatos ad Appled Mathematcs: A Iteratoal Joural (AAM) he Power Seres Soluto of Fgerg Pheomeo

More information

Log1 Contest Round 2 Theta Complex Numbers. 4 points each. 5 points each

Log1 Contest Round 2 Theta Complex Numbers. 4 points each. 5 points each 01 Log1 Cotest Roud Theta Complex Numbers 1 Wrte a b Wrte a b form: 1 5 form: 1 5 4 pots each Wrte a b form: 65 4 4 Evaluate: 65 5 Determe f the followg statemet s always, sometmes, or ever true (you may

More information

On Eccentricity Sum Eigenvalue and Eccentricity Sum Energy of a Graph

On Eccentricity Sum Eigenvalue and Eccentricity Sum Energy of a Graph Aals of Pure ad Appled Mathematcs Vol. 3, No., 7, -3 ISSN: 79-87X (P, 79-888(ole Publshed o 3 March 7 www.researchmathsc.org DOI: http://dx.do.org/.7/apam.3a Aals of O Eccetrcty Sum Egealue ad Eccetrcty

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

STA 108 Applied Linear Models: Regression Analysis Spring Solution for Homework #1

STA 108 Applied Linear Models: Regression Analysis Spring Solution for Homework #1 STA 08 Appled Lear Models: Regresso Aalyss Sprg 0 Soluto for Homework #. Let Y the dollar cost per year, X the umber of vsts per year. The the mathematcal relato betwee X ad Y s: Y 300 + X. Ths s a fuctoal

More information

. The set of these sums. be a partition of [ ab, ]. Consider the sum f( x) f( x 1)

. The set of these sums. be a partition of [ ab, ]. Consider the sum f( x) f( x 1) Chapter 7 Fuctos o Bouded Varato. Subject: Real Aalyss Level: M.Sc. Source: Syed Gul Shah (Charma, Departmet o Mathematcs, US Sargodha Collected & Composed by: Atq ur Rehma (atq@mathcty.org, http://www.mathcty.org

More information

1 Solution to Problem 6.40

1 Solution to Problem 6.40 1 Soluto to Problem 6.40 (a We wll wrte T τ (X 1,...,X where the X s are..d. wth PDF f(x µ, σ 1 ( x µ σ g, σ where the locato parameter µ s ay real umber ad the scale parameter σ s > 0. Lettg Z X µ σ we

More information

Assignment 7/MATH 247/Winter, 2010 Due: Friday, March 19. Powers of a square matrix

Assignment 7/MATH 247/Winter, 2010 Due: Friday, March 19. Powers of a square matrix Assgmet 7/MATH 47/Wter, 00 Due: Frday, March 9 Powers o a square matrx Gve a square matrx A, ts powers A or large, or eve arbtrary, teger expoets ca be calculated by dagoalzg A -- that s possble (!) Namely,

More information

STRING COSMOLOGICAL MODEL IN PRESENCE OF MASSLESS SCALAR FIELD IN MODIFIED THEORY OF GENERAL RELATIVITY

STRING COSMOLOGICAL MODEL IN PRESENCE OF MASSLESS SCALAR FIELD IN MODIFIED THEORY OF GENERAL RELATIVITY ASROPHYSICS SRING COSMOLOGICAL MODEL IN PRESENCE OF MASSLESS SCALAR FIELD IN MODIFIED HEORY OF GENERAL RELAIVIY D.D. PAWAR, S.N. BAYASKAR, A.G. DESHMUKH 3 Departet of Matheatc, Govt. Vdarbha Ittute of

More information

Evolution Operators and Boundary Conditions for Propagation and Reflection Methods

Evolution Operators and Boundary Conditions for Propagation and Reflection Methods voluto Operators ad for Propagato ad Reflecto Methods Davd Yevck Departmet of Physcs Uversty of Waterloo Physcs 5/3/9 Collaborators Frak Schmdt ZIB Tlma Frese ZIB Uversty of Waterloo] atem l-refae Nortel

More information

Lecture 7: Linear and quadratic classifiers

Lecture 7: Linear and quadratic classifiers Lecture 7: Lear ad quadratc classfers Bayes classfers for ormally dstrbuted classes Case : Σ σ I Case : Σ Σ (Σ daoal Case : Σ Σ (Σ o-daoal Case 4: Σ σ I Case 5: Σ Σ j eeral case Lear ad quadratc classfers:

More information

Integral Equation Methods. Jacob White. Thanks to Deepak Ramaswamy, Michal Rewienski, Xin Wang and Karen Veroy

Integral Equation Methods. Jacob White. Thanks to Deepak Ramaswamy, Michal Rewienski, Xin Wang and Karen Veroy Itroducto to Smulato - Lecture 22 Itegral Equato ethods Jacob Whte Thaks to Deepak Ramaswamy, chal Rewesk, X Wag ad Kare Veroy Outle Itegral Equato ethods Exteror versus teror problems Start wth usg pot

More information

Plane Wave Propagation in a Rotating Polygonal Cross-sectional Plate Immersed in Fluid

Plane Wave Propagation in a Rotating Polygonal Cross-sectional Plate Immersed in Fluid Amerca Joural o Materals Scece 4, 4(: 45-55 DOI:.59/.materals.44. Plae Wave Propagato a Rotatg Polygoal Cross-sectoal Plate Immersed Flud P. Pousamy Departmet o Mathematcs, Govermet Arts College (Autoomous,

More information

Bianchi Type V String Cosmological Model with Variable Deceleration Parameter

Bianchi Type V String Cosmological Model with Variable Deceleration Parameter September 013 Volume 4 Issue 8 pp. 79-800 79 Banch Type V Strng Cosmologcal Model wth Varable Deceleraton Parameter Kanka Das * &Tazmn Sultana Department of Mathematcs, Gauhat Unversty, Guwahat-781014,

More information

Entropy ISSN by MDPI

Entropy ISSN by MDPI Etropy 2003, 5, 233-238 Etropy ISSN 1099-4300 2003 by MDPI www.mdp.org/etropy O the Measure Etropy of Addtve Cellular Automata Hasa Aı Arts ad Sceces Faculty, Departmet of Mathematcs, Harra Uversty; 63100,

More information

Periodic Table of Elements. EE105 - Spring 2007 Microelectronic Devices and Circuits. The Diamond Structure. Electronic Properties of Silicon

Periodic Table of Elements. EE105 - Spring 2007 Microelectronic Devices and Circuits. The Diamond Structure. Electronic Properties of Silicon EE105 - Srg 007 Mcroelectroc Devces ad Crcuts Perodc Table of Elemets Lecture Semcoductor Bascs Electroc Proertes of Slco Slco s Grou IV (atomc umber 14) Atom electroc structure: 1s s 6 3s 3 Crystal electroc

More information

( q Modal Analysis. Eigenvectors = Mode Shapes? Eigenproblem (cont) = x x 2 u 2. u 1. x 1 (4.55) vector and M and K are matrices.

( q Modal Analysis. Eigenvectors = Mode Shapes? Eigenproblem (cont) = x x 2 u 2. u 1. x 1 (4.55) vector and M and K are matrices. 4.3 - Modal Aalyss Physcal coordates are ot always the easest to work Egevectors provde a coveet trasformato to modal coordates Modal coordates are lear combato of physcal coordates Say we have physcal

More information

Stress Wave propagation in Electro-Magneto-Elastic plate of arbitrary cross-sections

Stress Wave propagation in Electro-Magneto-Elastic plate of arbitrary cross-sections Iteratoal Joural of Scetfc & Egeerg Research Volume 3, Issue 8, August-1 1 ISSN 9-5518 Stress Wave propagato Electro-Mageto-Elastc plate of arbtrary cross-sectos P. Pousamy Departmet of Mathematcs Govermet

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

Locally Rotationally Symmetric Bianchi Type I Massive String Cosmological Models with Bulk Viscosity and Decaying Vacuum Energy Density

Locally Rotationally Symmetric Bianchi Type I Massive String Cosmological Models with Bulk Viscosity and Decaying Vacuum Energy Density Advances n Astrophyscs, Vol., No., August 06 Locally otatonally Symmetrc Banch Type I Massve Strng Cosmologcal Models wth Bulk Vscosty and Decayng Vacuum Energy Densty aj Bal * and Swat Sngh States Professor

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

,...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

A unified matrix representation for degree reduction of Bézier curves

A unified matrix representation for degree reduction of Bézier curves Computer Aded Geometrc Desg 21 2004 151 164 wwwelsevercom/locate/cagd A ufed matrx represetato for degree reducto of Bézer curves Hask Suwoo a,,1, Namyog Lee b a Departmet of Mathematcs, Kokuk Uversty,

More information

Ellipsometry Overview

Ellipsometry Overview llpsometry Overvew ~ R Δ p ρ = ta( Ψ) e = ~ Rs ñ(λ) = (λ) + k(λ) ε = ñ 2 p-plae s-plae p-plae plae of cdece s-plae llpsometry buldg-blocks Lght ad Polarzato Materals / Optcal Costats Iteracto of Lght wth

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

PTAS for Bin-Packing

PTAS for Bin-Packing CS 663: Patter Matchg Algorthms Scrbe: Che Jag /9/00. Itroducto PTAS for B-Packg The B-Packg problem s NP-hard. If we use approxmato algorthms, the B-Packg problem could be solved polyomal tme. For example,

More information

1 Mixed Quantum State. 2 Density Matrix. CS Density Matrices, von Neumann Entropy 3/7/07 Spring 2007 Lecture 13. ψ = α x x. ρ = p i ψ i ψ i.

1 Mixed Quantum State. 2 Density Matrix. CS Density Matrices, von Neumann Entropy 3/7/07 Spring 2007 Lecture 13. ψ = α x x. ρ = p i ψ i ψ i. CS 94- Desty Matrces, vo Neuma Etropy 3/7/07 Sprg 007 Lecture 3 I ths lecture, we wll dscuss the bascs of quatum formato theory I partcular, we wll dscuss mxed quatum states, desty matrces, vo Neuma etropy

More information

IS 709/809: Computational Methods in IS Research. Simple Markovian Queueing Model

IS 709/809: Computational Methods in IS Research. Simple Markovian Queueing Model IS 79/89: Comutatoal Methods IS Research Smle Marova Queueg Model Nrmalya Roy Deartmet of Iformato Systems Uversty of Marylad Baltmore Couty www.umbc.edu Queueg Theory Software QtsPlus software The software

More information

A Family of Non-Self Maps Satisfying i -Contractive Condition and Having Unique Common Fixed Point in Metrically Convex Spaces *

A Family of Non-Self Maps Satisfying i -Contractive Condition and Having Unique Common Fixed Point in Metrically Convex Spaces * Advaces Pure Matheatcs 0 80-84 htt://dxdoorg/0436/a04036 Publshed Ole July 0 (htt://wwwscrporg/oural/a) A Faly of No-Self Mas Satsfyg -Cotractve Codto ad Havg Uque Coo Fxed Pot Metrcally Covex Saces *

More information

Fourth Order Four-Stage Diagonally Implicit Runge-Kutta Method for Linear Ordinary Differential Equations ABSTRACT INTRODUCTION

Fourth Order Four-Stage Diagonally Implicit Runge-Kutta Method for Linear Ordinary Differential Equations ABSTRACT INTRODUCTION Malasa Joural of Mathematcal Sceces (): 95-05 (00) Fourth Order Four-Stage Dagoall Implct Ruge-Kutta Method for Lear Ordar Dfferetal Equatos Nur Izzat Che Jawas, Fudzah Ismal, Mohamed Sulema, 3 Azm Jaafar

More information

MAX-MIN AND MIN-MAX VALUES OF VARIOUS MEASURES OF FUZZY DIVERGENCE

MAX-MIN AND MIN-MAX VALUES OF VARIOUS MEASURES OF FUZZY DIVERGENCE merca Jr of Mathematcs ad Sceces Vol, No,(Jauary 0) Copyrght Md Reader Publcatos wwwjouralshubcom MX-MIN ND MIN-MX VLUES OF VRIOUS MESURES OF FUZZY DIVERGENCE RKTul Departmet of Mathematcs SSM College

More information

Semiconductor Device Physics

Semiconductor Device Physics 1 Semcoductor evce Physcs Lecture 7 htt://ztomul.wordress.com 0 1 3 Semcoductor evce Physcs Chater 6 Jucto odes: I-V Characterstcs 3 Chater 6 Jucto odes: I-V Characterstcs Qualtatve ervato Majorty carrers

More information

THE PROBABILISTIC STABILITY FOR THE GAMMA FUNCTIONAL EQUATION

THE PROBABILISTIC STABILITY FOR THE GAMMA FUNCTIONAL EQUATION Joural of Scece ad Arts Year 12, No. 3(2), pp. 297-32, 212 ORIGINAL AER THE ROBABILISTIC STABILITY FOR THE GAMMA FUNCTIONAL EQUATION DOREL MIHET 1, CLAUDIA ZAHARIA 1 Mauscrpt receved: 3.6.212; Accepted

More information

On Face Bimagic Labeling of Graphs

On Face Bimagic Labeling of Graphs IOSR Joural of Mathematcs (IOSR-JM) e-issn: 78-578, p-issn: 319-765X Volume 1, Issue 6 Ver VI (Nov - Dec016), PP 01-07 wwwosrouralsor O Face Bmac Label of Graphs Mohammed Al Ahmed 1,, J Baskar Babuee 1

More information

Comparison of Parameters of Lognormal Distribution Based On the Classical and Posterior Estimates

Comparison of Parameters of Lognormal Distribution Based On the Classical and Posterior Estimates Joural of Moder Appled Statstcal Methods Volume Issue Artcle 8 --03 Comparso of Parameters of Logormal Dstrbuto Based O the Classcal ad Posteror Estmates Raja Sulta Uversty of Kashmr, Sragar, Ida, hamzasulta8@yahoo.com

More information

Lower Bounds of the Kirchhoff and Degree Kirchhoff Indices

Lower Bounds of the Kirchhoff and Degree Kirchhoff Indices SCIENTIFIC PUBLICATIONS OF THE STATE UNIVERSITY OF NOVI PAZAR SER. A: APPL. MATH. INFORM. AND MECH. vol. 7, (205), 25-3. Lower Bouds of the Krchhoff ad Degree Krchhoff Idces I. Ž. Mlovaovć, E. I. Mlovaovć,

More information

CHAPTER VI Statistical Analysis of Experimental Data

CHAPTER VI Statistical Analysis of Experimental Data Chapter VI Statstcal Aalyss of Expermetal Data CHAPTER VI Statstcal Aalyss of Expermetal Data Measuremets do ot lead to a uque value. Ths s a result of the multtude of errors (maly radom errors) that ca

More information

FREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM

FREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM Joural of Appled Matematcs ad Computatoal Mecacs 04, 3(4), 7-34 FREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM Ata Cekot, Stasław Kukla Isttute of Matematcs, Czestocowa Uversty of Tecology Częstocowa,

More information

Midterm Exam 1, section 1 (Solution) Thursday, February hour, 15 minutes

Midterm Exam 1, section 1 (Solution) Thursday, February hour, 15 minutes coometrcs, CON Sa Fracsco State Uversty Mchael Bar Sprg 5 Mdterm am, secto Soluto Thursday, February 6 hour, 5 mutes Name: Istructos. Ths s closed book, closed otes eam.. No calculators of ay kd are allowed..

More information

Solutions to Homework Problems for the Complexity Explorer Course on Random Walks

Solutions to Homework Problems for the Complexity Explorer Course on Random Walks Solutos to Homework Problems for the Complexty Explorer Course o Radom Walks. Dsplacemet of a radom walk. Cosder the Pearso radom walk ay spatal dmeso whch the legth of each step has the fxed value a,

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