Archive

Experimental Study on Shape and Rise Velocity of Small Bubbles in Stagnant Water

Authors:

A Mitra, P Bhattacharya, S Mukhopadhyay, K K Dhar

DOI NO:

https://doi.org/10.26782/jmcms.2015.01.00004

Abstract:

This paper presents the results of an experimental study on the shape andrise velocityof small bubbles risingin stagnant water. Bubbles, generated at the bottom of the chamberholding water, rise through it.A high speed camera (1000 fps, Kodak, Model 1000 HRC)together with a 90 mm Macro lens is placed at a height of 60 cm from the bottom of thechamber. It is linked with a PC. The commercial software Sigma Scan Pro 5.0 and AdobePhotoshop are used for image capturing and processing.Bubbles(diametersin the range0.0245-5.903 cm)aregenerated at the bottom of the chamber holding the water. We find thatbubbles have threesteady shapes, a sphere,an ellipsoidandspherical capin this diameterrange.The experimentally determined rise velocity of bubble in the present investigationagrees well with the data available in the literature

Keywords:

Bubble,Rise Velocity,Stagnant Water,Shape,

Refference:

I.Arnold, K. and M. Stewart, Surface production operations. 3rd ed. Vol. 1. 2008,Amsterdam: Elsevier.768p.

II.Speight, J.G., The chemistry and technology of petroleum. 1999, New York:Marcel Dekker. xiv, 918 p.

III.Haugan, J.A., Challenges in heavy crude oil-Grane, an overview, Journal ofpetroleum technology, 2006. 58(6): p. 53-54.

IV.Bybee, K., Production of heavy crude oil: Topside experiences on Grane, Journalof petroleum technology, 2007. 59(4): p. 86-89.

V.Abdel-Aal, H.K., M. Aggour, and M.A. Fahim, Petroleum and gas field processing.2003, New York: Marcel Dekker. XII, 364 p.

VI.Shoham,O. and G.E. Kouba, State of the art of gas/liquid cylindrical-cyclonecompact-separator technology, Journal of petroleum technology, 1998. 50(7): p. 58-65.

VII.Baker, A.C. and J.H. Entress, The VASPS subsea separation and pumpingsystem.Chemical engineering research & design, 1992. 70(1): p. 9-16.

VIII.Cohen, D.M. and P.A. Fischer, Production systems hit the seafloor running, WorldOil, 2008. 229(1): p. 71-8.

IX.CDS engineering and FMC Technologies, CDS StatoilHydro Degasser. [cited 2009March 23]; Available from: http://www.fmctechnologies.com/upload/factsheet_cds_degasser.pdf.

X.Schinkelshoek, P. and H.D. Epsom, Supersonic gas conditioning-Commercialisation of Twister technology, in GPA conference. 2008: Grapevine,Texas, USA.

XI.Gjerdseth, A.C., A. Faanes, and R. Ramberg. The Tordis IOR Project, in Offshoretechnology conference, 2007. Houston.

XII.Clift, R., J.R. Grace, and M.E. Weber, Bubbles, drops, and particles. 1978, NewYork: Academic Press, xiii, 380 p.

XIII.Grace, J.R., Shapes and velocities of bubbles rising in infinite liquids,Transactions of the Institution of Chemical Engineers, 1973. 51(2): p. 116-20.

XIV.Grace, J.R., Shapes and velocities of single drops and bubbles moving freelythrough immiscible liquids, Transactions of the Institution of Chemical Engineers,1976. 54(3): p. 167-173.

XV.A. Mitra, T K Dutta & D N Ghosh,Natural Convective Heat Transfer in WaterEnclosed Between Pairs of Differentially Heated VerticalPlates, Heat and MassTransfer, 45, 2008, 187-192.

XVI.A. Mitra, T K Dutta & D N Ghosh,Augmentation of Heat Transfer in a Bubble-agitated Vertical Rectangular Cavity, Heat and Mass Transfer, 48, 2012, 695-704.

XVII.Mitra A, Bhattacharya P, MukhopadhyayS,Dhar K K, “Experimental Study onShape and Path of Small Bubbles using Video-Image Analysis,”2015 ThirdInternational Conf. On Computer, Communication, Control And InformationTechnology, 7–8 February 2015, Academy of Technology, Hooghly, West Bengal,India

XVIII.S.Mukhopadhyay,N.K.Das,A.Pradhan,N.Ghosh,P.K.Panigrahi,”Wavelet andmulti-fractal based analysis on DIC images in epithelium region to detect anddiagnose the cancer progress among different grades of tissues”,SPIE PhotonicsEurope-2014, Belgium.

XIX.S.Mukhopadhyay,N.K.Das,A.Pradhan,N.Ghosh,P.K.Panigrahi,”Pre-cancerDetection by Wavelet Transform and Multi-fractality in various grades of DICStromal Images”, SPIE West Photonics-2014, USA.

XX.Lima Ochoterena, R. and Zenit, R., 2003, Visualization of the flow around abubble moving in a low viscosity liquid, Revista Mexicana De Fisica 49, 348-352.

XXI.R. C. Clift, J. R. Grace and M. E. Weber, Bubbles, Drops, and Particles,Academic, NewYork, 1978.

XXII.Zheng, Li and Yapa, P.D., Buoyant Velocity of Spherical and Non sphericalBubbles/Droplets, Journal of Hydraulic Engineering, Vol. 126, No. 11, 2000.

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Numerical study and CFD Simulations of Incompressible Newtonian Flow by Solving steady Navier-stokes equations using Newton’s method

Authors:

K. M.Helal

DOI NO:

https://doi.org/10.26782/jmcms.2015.01.00005

Abstract:

Inthis paper, incompressible Newtonian flow is numerically studied byapproximatingthesolutionof the steady Navier-Stokes equationsin two dimensional case.Computational Fluid Dynamics (CFD)simulationsare carriedout byusing thefiniteelement method.Newton’smethodis applied to solvetheNavier-Stokes equationswherethe finite element solutions of Stokes equations is considered as the initial guess to obtainthe convergenceof Newton’s sequence.The numericalsimulations are presentedin termsofthe contours ofvelocity, pressure and streamline. All themeshes andsimulations areimplementedonthegeneralfinite element solver FreeFem++.Atwo-dimensionalbenchmark flow was computedwith posteriori estimates.It hasalsobeen established thatthe free accesssolverFreeFem++ can provide a reasonable good numerical simulationsof complicated flow behavior.

Keywords:

Navier-Stokesequations,CFD simulation,finite elementmethod,Newton-Raphsonmethod,

Refference:

I.Adams, R.A.,and Fournier,J.F.(2003).Sobolev Spaces,Second Edition,Academic Press, New York.

II.Becker, E., Carey, G. and Oden, J.(1981).Finite Elements. AnIntroduction,Vol.1,Prentice Hall, Inc., Englewood Cliffs, New Jersey.

III.Borges, L. (2006). Domain Decomposition Methods for Non-NewtonianFluids, PhD Thesis, IST, Lisbon.

IV.Brezis,H.(2011).Functional Analysis,Sobolev Spaces and Partial Differential Equations,Springer

V.Carey, G. F.and Oden,J.T.(1986).Finite elements. Vol.VI. Fluidmechanics,TheTexasFinite Element Series,VI. Prentice Hall, Inc.,Englewood Cliffs,NewJersey.

VI.Galdi, G. P. (1994). An Introduction to the Mathematical Theory of theNavier-Stokes Equations: Linearized Steady Problems, SpringerTracts inNatural Philosophy, Vol. 38,Springer, New York.

VII.Ghia, U., Ghia, K. N. and Shin, C. T. (1982). High-resolutionsforincom pressible flowsusingthe Navier-Stokes equations and a multigridmethod, J. Comput. Phys. 48, 387-411.

VIII.Hecht,F. (2012). FreeFem++, Version 3.23,http://www.freefem.org/ff++.Kim,S. D., Lee,Y. H. and Shin,B. C.(2006).Newton’s Method for theNavier-StokesEquations with Finite-Element Initial Guess of Stokes Equation,Computers and Mathematics with applications,51, 805-816.

IX.Quarteroni, A. and Valli, A.(1994).Numerical Approximation of Partial Differential Equations, Springer-Verlag.

X.Girault,V. and Raviart, P. A.(1986).Finite Element Approximation of theNavier-stokes Equations,Computational Mathematics,Springer-Verlag,Berlin.

XI.Temam, R.(1984).Navier-Stokes Equations. Theory and Numerical Analysis,3rded.,North-Holland, Amsterdam.

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A Direct Analytical Method for Finding an Optimal Solution for Transportation Problems

Authors:

M. Wali Ullah, Rizwana Kawser, M. Alhaz Uddin

DOI NO:

https://doi.org/10.26782/jmcms.2015.01.00006

Abstract:

In this paper a direct analytical method is proposed for finding an optimalsolution for a wide range of transportation problems. A numerical illustration isestablished and the optimality of the result yielded by this method is also checked. Themost attractive feature of this method is that it requires very simple arithmetical andlogical calculations. Themethod will be very worthwhile for those decision makers whoare dealing with logistics and supply chain related issues.One canalsoeasily adopt theproposed method among the existing methods for simplicity of the presented method.

Keywords:

TP=Transportation problem,SS=Stepping Stone ,MODI= Modified Distribution,NCM= North-West Corner Method , LCM= Least Cost Method,VAM= Vogel’sApproximation Method,Numerical Example,

Refference:

I.Goyal, S.K.-Improving VAM for the Unbalanced Transportation Problem,J.Opl.Res.Soc.35, 1113-1114(1984).

II.Ramakrishna, C. S.-An Improvement to Goyal’s Modified VAM for theUnbalanced Transportaion Problem, J Opl.Res.Soc. Vol.39, 609-610(1988).

III.Sultan, A.-Heuristic for Finding an Initial B. F. S. in TransportationProblems,OpsearchVol.25, 197-199(1988).

IV.Sultan, A. andGoyal, S.K.-Resolution of Degeneracy in TransportationProblems, J.Opl.Res.Soc. Vol.39, 411-413(1988).

V.Adlakha, V. andKowalski, K.-An Alternative Solution Algorithm forCertainTransportation Problems, IJMEST 30, 719-728(1999).

VI.Adlakha, V., Kowalski, K. andLev,B.-Solving Transportation Problem withMixed Constraints, JMSEM 1, 47-52(2006).

VII.Ji Ping & Chu, K. F.-A dual matrix approach to the transportationproblem.Asia-Pacafic Journal ofOperations Research,Vol.19, 35-45(2002).

VIII.Pandian,P.and Natarajan,G.-A New Method for Finding an OptimalSolution for Transportation Problems,International J. of Math.Sci. & Engg.Appls.Vol.4 59-65(2010).

IX.Sudhakar,V. J.,Arunsankar, N.and Karpagam,T.-A New approach forfinding an Optimal Solution forTransportation Problems,European Journal ofScientific Research, vol.68, 254-257(2012).

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GLIVENKO CONGRUENCE ON A 0-DISTRIBUTIVE MEET SEMILATTICE

Authors:

Momtaz Begum

DOI NO:

https://doi.org/10.26782/jmcms.2015.01.00007

Abstract:

In This paper the author studiesthe Glivenko congruence R in a0-distributive meet semilattice. It isprovedthata meet semilattice S with 0 is0-distributive if and only if the quotient semilattice RS is distributive. Hence S is0-distributive if and only if (0] is the Kernel of some homomorphism ofS onto adistributive meet semilattice with 0.

Keywords:

Glivenko congruence,0-distributive semilattice ,distributive meetsemilattice,

Refference:

I.P. Balasubramani and P. V. Venkatanarasimhan,Characterizations of the 0-Distributive Lattices,Indian J. Pure appl.Math. 32(3) 315-324, (2001).

II.Momtaz Begum and A.S.A. Noor,Semi prime ideals in meet semilattices,Indian J. Pure appl.Math.Vol.1, No.2, 2012, 149-157.

III.H.S.Chakraborty and M.R.Talukder,Some characterizations of 0-distributivesemilattices,Accepted in the Bulletin of Malaysian Math. Sci.Soc.

IV.Azmal Hossain, Title: A study on meet semilattices directed above, Ph.D.Thesis, RU (2004).

V.Y. S. Powar and N. K. Thakare,0-Distributivesemilattices, Canad. Math. Bull.Vol. 21(4) (1978), 469-475.

VI.Rhodes, J.B. Modular and distributive semilattices. Trans. Amer. Math. Society.Vol.201(1975), P.31-41.

VII.J. C. Varlet,A generalization of the notion of pseudo-complementedness,Bull.Soc.Sci.Liege, 37(1968), 149-158.

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ON THE SOLVABILITY OF A CLASS OF NONLINEAR FUNCTIONAL EQUATIONS

Authors:

D. C. Sanyal

DOI NO:

https://doi.org/10.26782/jmcms.2015.10.00001

Abstract:

It is proposed to introduce some simple criteria regarding the existence of unique solutions of a class of nonlinear functional equations in supermetric and metric spaces followed by suitable examples. The results obtained may be of much useful to many physical problems arising nonlinear equations.

Keywords:

Supermetric space,metric space,functional equation,Hammerstein equation. ,

Refference:

1) Sen, R. N. : Approximate Iterative Process in a Supermetric Space. Bull Cal. Math Soc., Vol. 63 (1971) p. 121-123.
2) Sen, R. N. & Mukherjee, S. : On Iterative Solution of Nonlinear Functional
Equations. Int J. Math. & Math. Sc. Vol. 6 (1983) p. 161-170
3) Sen, R. N. & Mukherjee, S. : A Note on a Unique Solvability of a Class of Nonlinear Equations. Int J. Math. & Math. Sc. Vol. 11 (1988) p. 201-204.
4) Collatz, L. : Functional Analysis and Numerical Mathematics. Academic Press, New York (1966).
5) Kannan, R. : Some Results on Fixed Points. Bull Cal. Math Soc., Vol 60 (1968)
p. 71-76.

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OPTIMUM LOCATION OF DISTRIBUTED ENERGY RESOURCES IN DISTRIBUTED NETWORK

Authors:

Nabanita Das, Sudipta Ghosh, Shilpi Samajpati, Balaram Kar4, Debasish Kundu

DOI NO:

https://doi.org/10.26782/jmcms.2015.10.00002

Abstract:

With ever increasing energy consumption, rising public awareness of environmentalprotection, steady progress inpower deregulation and revolution of environment,transmission line obstruction is quite regular. For maximum benefit and improvement ofobstruction, proper position of distributed generators is very necessary. This proposed workidentifies the optimum location to connect distribution energy resources in distributednetwork to minimize the total reactive power loss. Here use a simple conventional iterativesearch technique by matlab software. Gauss-Seidel method of load flow study is implementedon IEEE 6bus and IEEE 30 bus systems.

Keywords:

Distributedgeneration(DG),Gauss-Seidel(GS),Objective function(OF),

Refference:

I.W. El-Khattam, M.M.A. Salama.Distributed generation technologies, definitions andbenefitsDepartment of Electrical and Computer Engineering,.[ Received 15 August 2002;accepted 14 January 2004]

II.N.Hatziargyriou*,G. Kariniotakis N.Jenkins,J. PecasLopes,J.Oyarzabal,F. Kanellos, X.LePivert,N. JayawarnaN. Gil, C. MoreiraZ. Larrabe.Modelling of Micro-Sources forSecurity Studies.

III.D.H. Popovic ́a,*,1, J.A. Greatbanksb,1, M. Begovic ́c, A. Pregeljd,2. School of Electricaland Computer Engineering, Placement of distributed generators and reclosers for distributionnetwork security and reliability. Received 19 August 2003; revised 25 November 2004;accepted 2 February 2005

IV.SudiptaGhosh *, S.P. Ghoshal, SaradinduGhosh.Optimal sizing and placement ofdistributed generation in a network system. Department of Electrical Engineering, NationalInstitute of Technology, Received 28 March 2009 Received in revised form 22 December2009 Accepted 28 January 2010.

V.S.G.BharathiDasan,S.SelviRamalakshmiDr.R.P.Kumudinidevi.Department of EEE.Optimal Siting and Sizing of Hybrid Distributed Generation using EP. 2009 ThirdInternational Conference on Power Systems, Kharagpur, INDIA December 27-29.

VI.A.Kazemi, and M.Sadeghi. A Load Flow Based Method For Optimal Location OfDispersed Generation Units.

VII.G.N. Koutroumpezis, A.S. SafigianniOptimum allocation of the maximum possibledistributed generation penetration in a distribution network.Electrical and ComputerEngineering Department, Received 9 November 2009 Received inrevised form 21 April 2010Accepted 8 June 2010 Available online 15 July 2010.

VIII.Hasham Khan, Mohammad Ahmad Choudhry Implementation of Distributed Generation(IDG) algorithm for performance enhancement of distribution feeder under extreme loadgrowth.Department of Electrical Engineering, University of Engineering and Technology,Taxila, Pakistan,[ Received 19 September 2007 Received in revised form 27 October 2009Accepted 23 February 2010.]

IX.H. Kakigano, Y. Miura and T. Ise,Member, IEEE,T. Momoseand H. Hayakawa,Non-memberFundamental Characteristics of DC Microgrid for Residential Houses withCogeneration System in Each House.

X.D. Feng Z. Chen ,The Institute of Energy Engineering, Aalborg University, Denmark,System Control of Power Electronics Interfaced Distribution Generation Units.

XI.KarthickThyagarajanAsadDavariAliFeliachi ECE Dept, WW Tech ECE Dept, WWTechMontgomery,WV-25136Montgomery,WV-25136 Morgantown,Load Sharing Controlin Distributed Generation System.

XII.H. Kakigano, Y. Miura and T. Ise,Member, IEEE,Configuration andControl of a DC MicrogridforResidential Houses.

XIII.Nikhil K. Ardeshna,Member,IEEE, and Badrul H. Chowdhury,Senior Member, IEEE,Optimizing Micro-grid Operations in thePresence of Wind Generation.

XIV.Caisheng Wang,Modeling and Control of HybrideWind/Photovoltaic/Full CellDistributed Generation Systems.

XV.AtefehPourshafie, Mohsen. Saniei, S. S. Mortazavi, and A. Saeedian, OptimalCompensation of Reactive Power in theRestructured Distribution Network.

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ON THE FLOW OF TWO IMMISCIBLE VISCO-ELASTIC FLUIDS THROUGH A RECTANGULAR CHANNEL

Authors:

Goutam Chakraborty , Supriya Panja

DOI NO:

https://doi.org/10.26782/jmcms.2015.10.00003

Abstract:

This paper is concerned with the flow of two immiscible visco-elastic fluidsthrough a rectangular channel. The flow takes place due to a time-variantpressuregradient whichis transient in character. The visco-elastic fluids are of Oldroyd type. Infinding solutions of the problem variable separation technique appropriate to theboundary conditions and pressure gradient is applied. In the bulk of the paper, someinterestingresults such as interface velocity, flux, skin-friction and mean velocity arepresented.

Keywords:

,

Refference:

I.BAGCHI, K. C.–Rev. Roum. Sci. Tech. Mech. Appl., 11, 3, 603, (1966).

II.KAPUR, J. N. and SUKHLA, J. B.–ZAMM, 44, 6, 268, (1962).

III.DAS, K. K.–Ind. Jour. Theo. Phys., 37, 2, 141, (1989).

IV.SENGUPTA, P. R. and RAY MAHAPATRA, J.–Rev. Roum. Sci. Tech. Mech.Appl., 16, 5,1023, (1971).

V.OLDROYD, J. G.–Proc. Roy. Soc., A 200, 523, (1950)

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NUMERICAL SIMULATION OF LAMINAR CONVECTION FLOW AND HEAT TRANSFER AT THE LOWER STAGNATION POINT OF A SOLID SPHERE.

Authors:

Asish Mitra

DOI NO:

https://doi.org/10.26782/jmcms.2015.10.00004

Abstract:

A numerical algorithm is presented for studyinglaminar convection flow andheat transferat the lower stagnation point of a solid sphere.By means of similaritytransformation, the original nonlinear partial differential equations of flow aretransformed to a pair of nonlinear ordinary differential equations. Subsequently theyare reduced to a first order system and integrated using Newton Raphson andadaptiveRunge-Kutta methods.The computer codes are developedfor this numerical analysis inMatlab environment. Velocity and temperature profiles for various values of Prandtlnumber and at a fixed conjugate parameter are illustrated graphically. The results ofthe present simulation are then compared with previousresults available in literaturewith good agreement.

Keywords:

Free Convection,Fluid Flow,Heat Transfer,Matlab,Numerical Simulation,Solid Sphere,Stagnant Point,

Refference:

I.Chen T and Mucoglu A 1977 Int. J. Heat. Mass. Transfer20867.

II.Nazar R, Amin N, Grosan T and Pop I 2002a Int.Comm. Heat. Mass. Transfer29377.

III.Nazar R, Amin N, Grosan T and Pop I 2002b Int.Comm. Heat. Mass. Transfer291129.

IV.Nazar R, Amin N and Pop I 2002c Arab. J. Sci. Eng27117.

V.Cheng C Y 2008 Int.Comm. Heat. Mass. Transfer35750.

VI.Mitra A, Numerical simulation on Unsteady Heat Transfer of a Sphere, InternationalJournal on Emerging Technology and Applied Sciences, 03, 2014, 355-365.

VII.Mitra A, Numerical Simulation on Laminar Free-Convection Flow and HeatTransfer Over an Isothermal Vertical Plate,International Journal of Research inEngineering & Technology, 04, 2015, 488-494.

VIII.Mitra A, Numerical simulation on laminar convection flow and heat transfer over anon-isothermal horizontal plate,International Journal of Research in Engineering &Technology,accepted.

IX.Salleh M Z, Nazar R and Pop I 2010 Acta Applic Math 112 263.

X.AlkasasbehH T, Salleh M Z, Tahar R M, Nazar R,Numerical Solutions of FreeConvection Boundary Layer Flow on a Solid Sphere with Convective BoundaryConditions, Journal of Physics: Conference Series 495 (2014).

XII.Cebeci T and Bradshaw P 1984 Physical and computational aspects of convectiveheat transfer Springer, New York.

XIII.Na T Y 1979 Computational methods in engineering boundary valueproblem New York: Academic Press.

XIII.. I. Pop, D.B. Ingham, Convective Heat Transfer: Mathematical and Computational Modelling of Viscous Fluids and Porous Media, Oxford, Pergamon, 2001.

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PRESENT VALUE CALCULATION WITH DISIMILARITY IN EXPECTED RATE AND DISCOUNTING RATE

Authors:

Debashish Dutta, Sudipta Ghosh, Arpan Dutta, BalaramKar, Debasish Kundu

DOI NO:

https://doi.org/10.26782/jmcms.2015.10.00005

Abstract:

The sole aim of this paper is to calculate present value of periodical cash flows(fixed time interval)from an investmentconsideringthe effect of inflation,where cashflowis fixed (anordinaryannuity),orin a constant growth, or in a random nature.Incommon practice the discountingrateis equal to the expected rate of return of theinvestorfor calculating present value, but in reality this is not equal.The reason is thatthe expected rate of return is affected by the change of price level, that’s inflation,andthat’s whythisdirectlyaffectsthe purchasing power of moneyof the investor.Toprevent the purchasing power from the inflation, some adjustment is required forcalculating actual discounting rate. This paper providesthemethod of calculatinginflation adjusted discounting rateandc alculating adjusted present value of future cashflows. It also providesthecorrect investment decisions from various investment opportunities.

Keywords:

Present value of cash flows,Expected rate ofreturn ,Value of money,Inflation,Purchasingpower of money, Discounting rate, Annuity,

Refference:

I.Taylor, RichardW., “Future Value of a Growing Annuity: A Note.”Journal ofFinancialEducation (Fall 1986), 17-21.

II.Albert L. Auxier and John M. Wachowicz, Jr.Associate Professor and Professor, TheUniversity of Tennessee-“GROWING ANNUITIES”

III.G. A.Hawawini and A. Vora, The History of Interest Approximations,Arno Press,USA, 1980, ISBN 0-405-13480-0

IV.C. S. Park, R. Pelot, K. C. Porteous, M.J. Zuo, ContemporaryEngineeringEconomics, Addison Wesley Longman, Toronto, 2001,ISBN 0-201-61390-5

V.Myron Gordon, The Investment,Financing, and Valuation of the Corporation,Homewood, Ill.: Irwin,1962.

VI.Chicago Board of Trade, “Interest Rate Futuresfor Institutional Investors”–Chicago: 1987

VII.Figlewski, S., “Hedging with Financial Futures for Institutional Investors.”Cambridge, Mass.: Ballinger, 1986.

VIII.Gay, G. D. R. W. Kolb, and R. Chiang, “Interest Rate Hedging: An Empirical Test ofAlternative Strategies,”–Journal of Financial Research, 6 (Fall 1983), 187-97.

IX.Kolb, R. W., “Interest Rate Futures: A Comprehensive Introduction.”–Richmond,Va.: R. F. Dame, 1982.

X.Kolb, R. W., and R. Chiang, “Improving HedgingPerformance Using Interest RateFutures,”–Financial Management, 10 (Autumn 1981), 72-79.

XI.Veit, W. T., and W. W. Reiff, “Commercial Banks and Interest Rate Futures: AHedging Survey,”–Journal of Futures Markets, 3 (1983), 283-93.

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NUMERICAL SIMULATION ON LAMINAR FREE-CONVECTION FLOW AND HEAT TRANSFER OVER A VERTICAL PLATE WITH CONSTANT HEAT FLUX

Authors:

Asish Mitra

DOI NO:

https://doi.org/10.26782/jmcms.2016.01.00001

Abstract:

In the present numerical study,laminar free-convection flow and heat transfer over avertical plate with constant heat flux is presented. By means of similarity transformation, the original nonlinear coupled partial differential equations of flow are transformed to a pair of simultaneous nonlinear ordinary differential equations. Then, they are reduced to first order system. Finally, Newton-Raphson method and adaptive Runge-Kutta methodare use dfortheir integration.The computer codes are developed for this numerical analysis in Matlab environment. Velocity and temperature profiles for various Prandtl number are illustrated graphically. Flow and heat transfer parameters are derived as functionsof  Prandtl  numberalone. The results of the present simulation are then compared with experimental data published in literature and find a good agreement.

Keywords:

Constant Heat Flux,Free Convection,Heat Transfer,Matlab,Numerical Simulation,Vertical Plate,

Refference:

I. Sparrow, E. M., Gregg, J. L., “Similar Solutions for Laminar Free Convection from aNon isothermal Vertical Plate”,Trans. ASME, Journal of Heat Transfer,80, pp. 379387, 1958.

II. Pohlhausen, E., “Der Wنrmeaustausch zwischen festen Kِrpern und Flüssigkeiten mitKleiner Reibung und kleiner Wنrmeleitung“,Z. Angew. Math.Mech.1, 235-252,1921.

III. Dotson, J. P., “Heat Transfer from a Vertical Plate by Free Convection” MS Thesis,Purdue University, W. Lafayette. Ind., May 1954.

IV. Goldstien R. J., Eckert E. R. G., “The Steady and Transient Free Convection BoundaryLayerson a Uniformly Heated Vertical Plate,” Int. Journal of Heat and Mass Transfer,1, 208 218, 1960.

V. Fujii T., Fuji M., “The Dependence of Local Nusselt number on Prandtl number incase of Free Convection along a VerticalSurface with Uniform Heat Flux, ”Int.Journal ofHeat andMass Transfer, 19, 121-122, 1976.

VI. Pittman J. F. T., Richardson J. F., Sherrad C. P., “An Experimental Study of HeatTransfer by Laminar Natural Convection between an Electrically-Heated Vertical Plateand both Newtonian and Non-Newtonian Fluids,” Int. Journal of Heat and MassTransfer, 42, 657-671, 1999.

VII. Aydin O., Guessous L., “Fundamental Correlations for Laminar and Turbulent FreeConvection from an uniformly Heated Vertical Plate,”Int. Journal of Heat and MassTransfer, 44, 4605-4611, 2001.

VIII. Bejan, A.,Heat Transfer, John Wiley, New York, 1993.

IX. Incropera, F. P., DeWitt D. P.,Introduction to Heat Transfer, Fourth edition, JohnWiley, New York, 2002.

X. Çengel, Y. A.,Heat Transfer,Second edition, McGraw–Hill, New York, 2003.

XI. Lienhard IV, J. H., Lienhard V, J. H.,A Heat Transfer Textbook, Phlogiston Press,Cambridge, MA, 2003.

XII. Nellis, G., Klein, S.,Heat Transfer, Cambridge UniversityPress, London, UK, 2008.

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A COMPARATIVE STUDY OF FORECASTING AGRICULTURAL TIME SERIES: SOME SELECTED FOOD GRAIN IN BANGLADESH

Authors:

Md. Salauddin Khan, Masudul Islam, Md. Rasel Kabir, Lasker Ershad Ali

DOI NO:

https://doi.org/10.26782/jmcms.2016.01.00002

Abstract:

Bangladesh bureau of statistics (BBS) publish a statistical year book in every year where comprehensive and systematic summary of basic statistical information of Bangladesh covering wide range of fields. BBS also forecast different sectors such aseconomics, weather, agriculture etc in different time in this country. In this paper we mainly concern on the wheat, rice and maize food grain which plays a vital role in economic development of Bangladesh. The main purposes of this paper as to compare which techniques are better BBS’s or statistical techniques for forecasting. There are different forecasting models are available in statistics among these we used Auto regressive (AR), Moving Average(MA), Auto regressive Moving Average (ARMA)and Auto regressive Integrated Moving Average (ARIMA) models. For this reason, we clarify the stationary and non-stationary series by graphical method. On the basis of that,the stationary model is being set up asthe forecasting purpose. After analyze, we compare the forecasting result of our selective foodgrain and find that for ecasted valu esusing statistical techniques are nearest to the actual values compare to BBS’s project edvalues.

Keywords:

ARIMA,ARMA,Forecast,Foodgrain,

Refference:

I.  Abdullah, L. (2012),ARIMA Model for Gold Bullion Coin Selling PricesForecasting,International Journal of Advances in Applied Sciences. Vol. 1, No.4, pp. 153-158.

II. Anderson, T.W. (1984),An Introduction to Multivariate Statistical Analysis, 2nded.New York:John Wiley and Sons Inc.

III. Arumugan, P. and Anithakumari, V. (2013),Fuzzy Time SeriesMethod forForecastingTaiwanExport Data,International Journal of Engineering trendsandTechnology. Vol.8,pp. 3342-3347.

IV. Box, G. E. P. and Jenkins, G. M. (1976),Time Series Analysis: Forecasting andControl,SanFrancisco: Holden-Day.

V. Brokwell, P.J. and Davis, R.A. (1997),Introduction to Time Series andForecasting, Springer,New York

VI.Clements, M. and Hendry, D. (1998),Forecasting Economic Time Series,United UniversityPress, Cambridge.

VII. Deepak, P., et al. (2015), A Comparison of forecasting methods: Fundamentals,Polling, Prediction Markets, and Experts,A Journal of Prediction Markets,Vol.23, No.2, pp.1-31.

VIII. Diebold, F. (2004),Elements of Forecasting, 3rded. Thomsos sourth-westrn,India.

IX. Ediger, S.A, (2006),ARIMAForecasting of Primary Energy Demand by Fuel inTurkey,Energypolicy, Vol. 35, pp.1-8.

X. Gouriroux, C. and Monfort, A. (1997),Time Series and Dynammic Models,Giampiero,M.Gallo Cambridge.

XI. Gujarati, D.N. (2004),Basic Econometrics, 4thed.,McGraw Hill, New York.

XII. Hannan, E.J. (1994),Multiple Time Series,New York: John Wiley & Sons Inc.

XIII. Kumar, et al. (2009),Surface flux modelingusing ARIMA technique in humansubtropicalmonsoon area,Journal of Atmospheric and Solar-TerrestrialPhysics. Vol. 71, pp. 1293-1298.

XIV. Lloret, et al. (2000),Time Series Modeling of Landings in NorthMediterranean Sea,ICESJournal of Marine Science: Journal du Conseil. Vol.57, pp. 171-184.

XV. Mitrea, C. A., Lee, C. K.M. and Wu,Z. (2009), A Comparison betweenNeural Networks and Traditional Forecasting Methods: A Case Study,International Journal of Engineering Business Management, Vol. 1, No. 2, pp.19-24.

XVI. Mucuk, M. and Uysal, D. (2009),Turkey’s Energy Demand,Current ResearchJournal of SocialSciences, Vol.1(3), pp. 123-128.

XVII.Pingfan, H. and Zhibo, T. (2014), A comparison study of the forecasingperformance of three international organizations,JEL codes: C30, C80.

XVIII. Prindyck,R.S. and Rubinfeld, D.L. (1981),Economic Models and EconomicForecasts,3rded.McGraw-Hill, Inc.

XIX. Slvanathan, E. A. (1991),A Note on the Accuracy of Business Economists GoldPrice Forecasts,Australian Journal of Management. Vol. 16, pp. 91-94.

XX. Tseng, et al. (2001),Fuzzy ARIMA model for forecasting the foreign exchangemarket,FuzzySets and Systems. Vol. 118, pp. 1-11.

XXI. Wood, et al. (1996), Classifying Trend Movements in the MSCI U.S.A.Capitalmarket Index-A,Comparison of Regressions, ARIMA and Neural Network Method.Computers &Operation Research. Vol. 23, pp. 611-622.

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EXPANSION OF A SPHERICAL CAVITY AT THE CENTRE OF A NON-HOMOGENEOUS SPHERE OF DUCTILE METAL WITH EFFECT OF WORK-HARDENING UNDER INTERNAL AND EXTERNAL PRESSURES

Authors:

L.K. Roy

DOI NO:

https://doi.org/10.26782/jmcms.2016.01.00003

Abstract:

The aim of this paper is to investigate the distribution of stresses due to expansion of a spherical cavity at the centre of a non-homogeneous  metallic sphere of finite radius for an elasto-plastic solid with effect of work-hardening under an increasing internal pressure, the external pressure remaining constant. The non-homogenecity of the elastic material is characterised by supposing that the Lame constrants very exponentially as the function of radial distance. The case of ideal plastic solid has also been deduced from this general case.  

Keywords:

Refference:

1. R. Hill (1950), : Theory of Plasticity, Oxford University Press, p-317

2. A.E.H.Love (1952),: The Mathematical Theory of Elasticity, Dover
Publication, P-164, Landon.

3. Saint-Venant (1865), : Jour, De-Math, Primes at appl, (Lonvilla) t-10.

4. S.G.Lekhnitskii (1963), : Theory of Elasticity of an Anisotropic Elastic
Body, Holden-Day, INC, p-390.

5. H.G.Hopkins (1960), : Progress in solid Mechanics, Vol-I, p-80, Edited by I.N.Sneddon and R.Hill, North Holland Publishing Company, Amsterdem.

6. P. R. Sengupta (1969), Ind. Jour, Mech and Math., Special issue, Part-II,
p-80, Prof. B. Sen, D.Sc., F.N.I., 70th’Birth Anniversary Volume
7. L. K. Roy (1992), Proc. Nat. Acad. Sci. India, 62(A), III p-445

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NUMERICAL SIMULATION ON LAMINAR CONVECTION FLOW AND HEAT TRANSFER OVER AN ISOTHERMAL HORIZONTAL PLATE

Authors:

Asish Mitra

DOI NO:

https://doi.org/10.26782/jmcms.2016.01.00004

Abstract:

A numerical algorithm is presented for studyinglaminar convection flow andheat transfer over an isothermal horizontal plate. By means of similarity transformation,the original nonlinear coupled partial differential equations of flow are transformed to apair of simultaneous nonlinear ordinary differential equations. Subsequently they arereduced to a first order system and integrated using Newton RaphsonandadaptiveRunge-Kutta methods.The computer codes are developed for this numerical analysis inMatlab environment. Velocity, and temperature profiles for various Prandtl number areillustrated graphically. Flow, and heat transfer parameters are derivedas functions of Prandtl number alone. The results of the present simulation are then compared withexperimental data in literature with good agreement.

Keywords:

Free Convection, Heat Transfer ,Isothermal Horizontal Plate, Matlab,Numerical Simulation,

Refference:

I.Blasius, H., “Grenzschichten in Flussikeiten mitkleiner Reibung”, Z. Angew,Math.Phys., vol. 56, pp. 1-37, 1908 [English translation in NACA Technical Memo. 1256].

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III.Rosenhead, L. (ED), “Laminar Boundary Layers”, Oxford Univ. Press, London, 1963.

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V.Bejan, A.,Heat Transfer, John Wiley, New York, 1993.

VI.Sachdev, P. L., “Self-Similarity and Beyond: Exact Solutions of NonlinearProblems”, CRC Press, Boca Ratton, Fla, 2000

VII.Incropera, F.P. and DeWitt D.P.,Introduction to Heat Transfer, Fourthedition, JohnWiley, New York, 2002.

VIII.Çengel, Y.A.,Heat Transfer,Second edition, McGraw–Hill, New York, 2003.

IX.Lienhard IV, J.H. and Lienhard V, J.H.,A Heat Transfer Textbook, Phlogiston Press,Cambridge, MA, 2003.

X.Nellis, G. and Klein, S.,Heat Transfer, Cambridge University Press, London, UK,2008.

XI.Mitra A., “Numerical Simulation on Laminar Free-Convection Flow and HeatTransfer OveranIsothermal Vertical Plate,”International Journal of Research inEngineering & Technology, 04, 2015, pp 488-494.

XII.Leipmann, H. W., “Investigation on Laminar Boundary-Layer Stabilty andTransition on Carved Boundaries,“ NACAWartime Report W107 (ACR3H30),1943 [see also NACA Technical Memo. 1196 (1947) and NACA Report 890 (1947)].

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A CREDIT POLICY APPROACH OF AN INVENTORY MODEL FOR DETERIORATING ITEM WITH PRICE AND TIME DEPENDENT DEMAND

Authors:

Md. Abdul Hakim, Mohammad Anwar Hossen, M Sharif Uddin

DOI NO:

https://doi.org/10.26782/jmcms.2016.01.00005

Abstract:

In this paper, we have developed an inventory model for deteriorating items withprice and time dependentdemand considering inflation effect on the system. Shortages ifany are allowed and partially backlogged with a variable rate dependent on the durationof waiting time up to the arrival of next lot. The corresponding problem has beenformulated as a nonlinear constrained optimization problem, all the cost parameters arecrisp valued and solved. A numerical example has been considered to illustrate the modeland the significant features of the results are discussed. Finally, based on these examples,a sensitivity analyses have been studied by taking one parameter at a time keeping theother parameters as same.

Keywords:

Inventory,deterioration,partially backlogged shortages ,permissible delay in payment,

Refference:

I.C.W. Haley, H.C. Higgins, Inventory policy and trade credit financing, Manage.Sci. 20 (1973) 464-471.

II.S.K. Goyal, Economic order quantity under conditions of permissible delay inpayments, J. Oper. Res. Soc. 36 (1985) 35–38.

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VII.P.L. Abad, C.K.Jaggi, A joint approach for setting unit price and the length of thecredit period for a seller when end demand is price sensitive, Int. J. Prod. Econ. 83(2003) 115–122.

VIII.L.Y. Ouyang, K.S. Wu, C.T. Yang, A study on an inventory model for noninstantaneous deteriorating items with permissible delay in payments, Comp. Ind.Eng. 51 (2006) 637–651.

IX.Y.F. Huang, An inventory model under two levels of trade credit and limitedstorage space derived without derivatives, Appl. Math. Model. 30 (2006) 418–436.

X.Y.F. Huang, Economic order quantity under conditionally permissible delay inpayments, Euro.J.Oper.Res.176 (2007) 911–924.

XI.Y.F. Huang, Optimal retailer’s replenishment decisions in the EPQ model undertwolevels of trade credit policy, Euro.J.Oper.Res.176 (2007) 1577–1591.

XII.B. Das, K. Maity, M. Maiti, A two warehouse supply-chain model underpossibility/necessity/credibility measures, Math. Comp. Model. 46 (2007) 398–409.

XIII.B. Niu, J.X. Xie, A note on Two-warehouse inventory model with deteriorationunder FIFO dispatch policy, Euro. J. Oper. Res. 190 (2008) 571-577.

XIV.M. Rong, N.K. Mahapatra, M. Maiti, A twowarehouse inventory model for adeteriorating item with partially/fully backlogged shortage and fuzzy lead time,Euro. J. Oper. Res. 189 (2008) 59–75.

XV.J.K. Dey, S.K. Mondal, M. Maiti, Two storage inventory problem with dynamicdemandand interval valued lead-time over finite time horizon under inflation andtime-value of money, Euro. J. Oper. Res. 185 (2008) 170–194.

XIV.T.P. Hsieh, C.Y. Dye, L.Y. Ouyang, Determining optimal lot size for a twowarehouse system with deterioration and shortagesusing net present value, Euro.J. Oper. Res. 191 (2008) 182-192.

XVII.M.K. Maiti, Fuzzy inventory model with two warehouses under possibilitymeasure on fuzzy goal, Euro. J. Oper. Res. 188 (2008) 746–774.

XVIII.C. K. Jaggi, and P. Verma,Joint optimization of price and order quantity withshortages for a two-warehouse system,Top (Spain),16 (2008) 195-213.

XIX.S.S. Sana, K.S. Chaudhuri, A deterministic EOQ model with delays in paymentsand price-discountoffers, Euro. J. Oper. Res.184 (2008) 509–533.

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XXII.C.C. Lee, S.L. Hsu, A two-warehouse production model for deterioratinginventory items withtime-dependent demands,Euro. J. Oper. Res. 194 (2009)700–710.

XXIII.C.K. Jaggi, K.K. Aggarwal, P. Verma, Inventory and pricing strategies fordeteriorating items with limited capacity and timeproportional backlogging rate,Int. J. Oper. Res. 8(3) (2010) 331-354.

XXIV.C.K. Jaggi, A. Khanna, Supply chain models fordeteriorating items with stockdependent consumption rate and shortages underinflation and permissible delayin payment,Int. J. Math. Opera. Res. 2(4) (2010) 491-514.

XXV.C.K. Jaggi, A. Kausar, Retailer’s ordering policy in a supply chain when demandis price and credit period dependent,Int. J. Strat. Dec. Sci. 2(4) (2011) 61-74.

XXVI.A.K. Bhunia, A.A. Shaikh,A two warehouse inventory model for deteriorating itemswith time dependent partial backlogging and variable demand dependent on marketingstrategy and time,International Journal of Inventory Control and Management, 1 (2011),95-110.

XXVII.A.K. Bhunia,P. Pal, S. Chattopadhyay, B. K.Medya, An inventory model oftwo-warehouse system with variable demand dependent on instantaneousdisplayed stock and marketing decisions via hybrid RCGA,Int. J. Ind. Eng.Comput. 2(2) (2011) 351-368.
XXVIII.C.K. Jaggi, A. Khanna, P. Verma,Two-warehouse partially backlogginginventory model for deteriorating items with linear trend in demand underinflationary conditions,Int. J. Syst.Sci. 42(7) (2011) 1185-1196.
XXIX.C.K. Jaggi, M. Mittal, Retailer’s ordering policy for deteriorating items withinitial inspection and allowable shortages under the condition of permissibledelay in payments,Int. J. Appl. Ind. Eng. 1(1) (2012) 64-79.
XXX.H.L. Yang, (2012), ‘Two-warehouse partial backlogging inventory models with threeparameter weibull .distribution deterioration under inflation’International Journal ofProduction Economics,138, 107-116.
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XXXII.A.K. Bhunia, A.A. Shaikh,R.K. Gupta, A study on two-warehouse partiallybacklogged deteriorating inventory models under inflation via particle swarmoptimization,International Journal of System Science.(to appear) 2013.
XXXIII.H.L. Yang, C.T. Chang, A two-warehouse partialbacklogging inventory model fordeteriorating items with permissible delay in payment under inflation’,AppliedMathematical Modelling,37(2013), 2717-2726.
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XXXVII. N.H. Shah, A.R. Patel, K.R. Lou, Optimal ordering and pricing policy for pricesensitive stock-dependent demand under progressive payment scheme,International Journal Industrial Engineering Computations, 2(2011), 523-532
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A NEW APPROACH TO IMPROVE THE PERFORMANCE OF POSITION CONTROL OF DC SERVO MOTOR BY USING FUZZY LOGIC CONTROLLER

Authors:

Abhishek Kumar Kashyap, Binanda Kishore Mondal, Souvik Chatterjeeand, Sudipta Ghosh

DOI NO:

https://doi.org/10.26782/jmcms.2016.01.00006

Abstract:

The position control system is one of the interesting term in control systemengineering. Now a days several control system algorithm have been applied in thatapplication. PID controller is a well known controller and widely used infeedbackcontrol in industrial processes. For position control system sometime pid controller is notaccurate for this application because of non linear properties. Therefore e in thisresearch the fuzzy logic controller is proposed to overcome the problemof pid controller.Fuzzy logic controller has a ability to overcome the problem of pid controller. Fuzzylogic controller has ability to control the non linear systems also because the algorithmused is concentrated by emulating the expert and implementedin language based on theexperimental result , the fuzzy logic controller designed, is able to improve theperformance of the position control system compare to the pid controller, in terms of risetime (Tr) is 50%, settling time Ts is 80% and maximum overshoot (M%) is 98%, and thatcan be reduced.

Keywords:

uzzy logic controller,PID controller, position control,DC servo motor,

Refference:

I. Nagrath, I.J. and M. Gopal,Control Systems Engineering, 3rdedition, New AgePublishers, 2000

II.Driankov, D., H. Hellendoorn and M. Reinfrank,An Introduction to FuzzyControl,2ndedition, Springer International Student Edition, 2001

III.Klir, G.J. and Bo Yuan,FuzzySets and Fuzzy Logic: Theory and Applications,Prentice Hall International, 1995

IV.Chen, G. and T.T. Pham,Introduction to, Fuzzy Sets, Fuzzy Logic and Fuzzy]Control System,CRC Press, 2001

V.Beucher, O. and M. Weeks,INTRODUCTION TO MATLAB® & SIMULINK AProject Approach,3rdedition, Infinity Science Press LLC, 2008

VI.Rajoriya, A. and H. Ahmed(2014)Performance Assessment of Tuning Methodsfor PID Controller Parameter used for Position Control of DC Motor,InternationalJournal , Electrical Engg., 9, 139-148

VII. http://www.mathworks.com/matlabcentral

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