JOURNAL OF TEXTILES AND POLYMERS, VOL. 6, NO. 1, JANUARY

Size: px
Start display at page:

Download "JOURNAL OF TEXTILES AND POLYMERS, VOL. 6, NO. 1, JANUARY"

Transcription

1 JOURNAL OF TEXTILES AND POLYMERS, VOL. 6, NO., JANUARY 08 9 Visoelasi Modeling o he Reovery Behavior o Cu Pile Carpe Aer Sai Loading: A Comparison Beween Linear and Nonlinear Models Sahar Jaari * and Mohammad Ghane Absra- In his work, he reovery propery o mahinemade arpe was invesigaed using he visoelasi models. Visoelasi modeling o exile maerials are usually perormed wih presening dieren ombinaion o spring and dashpo. Two dieren mehanial models inluding linear and nonlinear Jeery s mehanial model were analyzed and ompared. Sai loading was applied o he samples or a erain ime. The load was hen removed and reovery behavior was invesigaed. The experimenal daa were hen adaped o he heoreial daa using urve iing based on leas square mehod. The resuls showed ha here was a reasonably good agreemen beween he Jerey s models and experimenal daa. The reason is ha hese wo models are no ompleely elasi showing seondary reep. No signiian dierene was observed beween linear and nonlinear model. The speed o reovery a he removal o he sai loading was also analyzed. The resuls show ha he nonlinear Jeery s model indiaes less value o speed o reovery a zero ime in omparison o he linear model. The reovery o u pile arpers shows some permanen reep and is explained by nonlinear and linear Jeery s model aepably. Keywords: u pile arpe, sai loading, reovery, visoelasi models, hikness loss I. INTRODUCTION Sanding and walking are dieren oresand deormaions ha applied o Carpe piles during suh human daily aiviies. Axial ompression, bending, laening, and exension and also sai and dynami pressure are some examples o hese deormaions []. Furhermore, he ompression behavior and mehanial reaion inluene on he piles hikness lossin he arpe. The reovery behavior o he pile arpe aer sai loading S. Jaari and M. Ghane Deparmen o Texile Engineering, Isahan Universiy o Tehnology, Isahan 83, Iran. Correspondene should be addressed o Sahar Jaari ???? is imporan or he qualiy, perormane and lieime o he piled arpe aer sai loading []. The abiliy o arpe pile o reurn o is original sae aer deormaion is denoed as Reovery or Resilieny. For modeling he mehanial behavior o he exile maerials, Dieren ombinaions o spring and dashpo sysems are usually onsidered. The visoelasi models are usually onsised o wo elemens i.e. visous dashpos whih obey Newon s law and springs whih obey Hooke s law [3]. However Non-Newonian dashpos or nonlinear springs are also involved o explain he dieren aspes o he maerials properies. Meng and Wu [4] sudied he sress relaxaion o membrane sruures in he pre-sress sae by onsidering visoelasi properies o oaed abris. The validiy o he suggesed analyial mehod is examined by omparing he numerial resuls wih experimenal daa o model ess. Shim e al. [5] sudied dynami mehanial properies o abri armor. The resuls show ha he proposed onsiuive equaion, based on a linear visoelasi model is able o desribe reasonably auraely he experimenal sress-srain response over a range o srain raes.vangheluwe [6] applied sandard nonlinear model o haraerize he relaxaion and inverse relaxaion o yarns aer dynami loading. The resuls show ha he model an alulae he residual ore a ininie ime in a relaxaion es or he ensile urve o spun yams. There seems o be good orrelaion wih he resuls o ess made using his mehod. Manih e al. [7] sudied he Ee o proessing and wearing on visoelasi modeling o polylaide/wool and polyeser/wool woven abris subjeed o bursing. The visoelasi behavior o he abris when mulidireional exended was simulaed and modeled using a modiied nonlinear Maxwell model. Asayesh e al. [8, 9] esimaed he reep and aigue behaviors o plain woven abris. They used he Eyring s model and he sandard linear model o desribe he abri behavior. Hashemi e al. [0] and Ardakani e al. [] sudied he inluene o wo bar warp-knied sruure on he abri

2 0 JOURNAL OF TEXTILES AND POLYMERS, VOL. 6, NO., JANUARY 08 ensile sress relaxaion. They examined dieren abri sruure and analyzed dieren visoelasi models. The experimenal resuls showed ha he abri sruure aes he ensile sress relaxaion signiianly. They also onluded ha he hree-omponen model wih he parallel-onne nonlinear spring shoed he bes agreemen wih he experimenal relaxaion o he analyzed abris. Khavari and Ghane [] sudied he ompression and reovery behavior o u pile arpes under onsan rae o ompression by mehanial models. Maxwell mehanial model, he sandard linear and nonlinear models were employed or simulaing he ompression behavior and reovery o he arpe samples. The resuls showed ha he sandard nonlinear models an desribe he ompression behavior o more signiianly in ompression o Maxwell and sandard linear models. Jaari and Ghane [3] sudied he reovery behavior o u pile arpe aer sai loading by mehanial models. Jeery s model and sandard linear model was used or simulaing he reovery behavior. The sandard linear model showed poor regression or he reovery properies o u pile arpes aer sai loading. The reason was ha he sandard linear model was ompleely elasi. Jaari and Ghane [4] also sudied he ee o UV radiaion on he reovery properies o pile arpe aer sai loading hrough analyial and visoelasi modeling. They ound ha he hikness loss and he maximum ompression were boh higher a longer UV exposure imes. The aim o his work is o invesigae he he oreial and experimenal reovery behavior o he u pile arpes. In his sudy, wo well-known mehanial models i.e. he linear and nonlinear Jeery s model were analyzed. To ind he bes model semi empirial urve iing mehod based on he leas square mehod was used. II. MECHANICAL MODELING Dieren mehanisms are involved when a u pile arpe is exposed o ompressive ore. The irs one is avisoelasi deormaion. The deormaion is reoverable wih a reardaionime. The seond mehanism involves a plasi or non-reoverable deormaion. This is due o dispassion o energy beween he pile yarns and plasi deormaion o he onsiuen ibers. I seems ha mehanial models onsising o dieren ombinaion o spring and dashpo an be used o represen he elaso-plasi behavior o he arpe under ompressive sai load. The aim o his paper is o analyze and ompare dieren visoelasi models in order o explain he mehanial behavior o arpe piles aer a shor-erm sai loading. For his purpose, wo models were presened or simulaion Fig.. Visoelasi models or he reovery behavior o u pile arpe: (a) linear Jeery s model and (b) nonlinear Jeery s model. o reovery behaviors o arpe pile yarns inluding; a) linear Jeery s model [5], b) quadrai nonlinear Jeery s model. Shemai diagrams o wo models are presened in Fig.. The ompressive ore is applied o he model. Erepresens he spring onsan or linear model (N/m) and b is he spring onsan or nonlinear model and η is he dashpo onsan (N.s/m). The governing dierenial equaion or he linear visoelasi model is ound o be: In his modeling a onsan load ( ) is applied o he model. Thus, o ind he x- equaion or he nonlinear model, we an separae wo par o exension. () x = x + x We an alulae plasi deormaion x p and elasi deormaion x e separaely and hen add hem ogeher. In plasi par we have: = η dx d p In he ase o onsan load ( ), we have: x η E a) + + (Ex +η x) = 0 η η p e = η The governing deerenial equaion in elasi par is: = bx x +ηx e e e In he ase o onsan load i beomes: bx x +η x = 0 p e e e For he elasi par we have he ollowing boundary () (3) (4) (5) (6)

3 JAFARI AND GHANE: VISCOELASTIC MODELING OF THE RECOVERY BEHAVIOR OF... ondiions: = = = = b xe 0 a 0 and xe a Solving he dierenial Eq. (6) and applying he boundary ondiion as in Eq. (7) he deormaion o he elasi par under he onsan load is ound o be: b. = xe an h. b η For he nonlinear model he oal exension under he onsan load an be ound by summing Eqs. (4) and (8). The x- equaions or he linear (model a) and quadrai nonlinear model (model b) are shown in Eq. (9): = + + E η η a)x e b. = + η b) x an h. The onsan load,, is applied o he proposed model. The se is ompressed o he exen o x a he ime. The value o x is ound o be as in Eqs. (0): a)x e η = + E η b) x = an h b.. + η (7) (8) (9) (0) I is lear ha he ompression o he whole se is equal o he ompression o boh elasi (x e ) and plasi pars (x p ) i.e. x =x e +x p. Thus, he amoun o ompression or elasi and plasi pars an be deermined separaely as in Eqs. (): a) x e and x η e = p = E η b) x = an h b.. and x = e p η () Aer removing he applied onsan load rom he se, reovery equaions ould be obained. By onsidering he general equaion o he models as well as our ondiion (aer load removal; =0, =0) he reovery dierenial equaions or boh models are ahieved as ollows: dx d x a)e +η = 0 d d dxr d xr r b) bx +η = 0 d d () Solving hese dierenial equaions need boundary ondiions. The ondiions an be provided rom he displaemen equaion where x=x a =0, as well as x = x p a =. For he nonlinear model we onsider x r =0 a =0 and x r =x e a =. Thus, hikness loss-ime equaions obained as in Eqs. (3) or (4): η a) x = xee + xp b) x = x b.x an h. and x = x x e r e r η (3) Or; replaing he boundary values orm Eqs. 0 and gives: η η a)x = e e + E η b. = + b) x an h. η b b. b. x e an h. an h. η η III. MATERIALS AND EXPERIMENT (4) A. Maerials In his work, he 700-reeds mahine woven arpe samples wih densiies o knos were produed. The arpe samples onsis o he oon/polyeser blended yarns wih densiy o 700 per meer as he warp yarns, he jue yarns wih densiy o 800 per meer as he we yarns. Aryli yarn was used as he pile yarn and he pile heigh was adjused o be 0 mm. B. Experimens Digial hikness gauge was used o measure he sample hikness. Iniial hikness o he sample was measured and denoed by x 0. A laboraory saled sai loading apparaus was used o simulae he applying o he sai loading. The appropriae weigh was hanged on he end o he arm o he apparaus so ha he onsan pressure o 700 kpa was applied o he arpe sample. The load was hen removed aer he ime. Two levels o sai loading ( ) were esed i.e. min and h. The hikness o he arpe is measured a his ime (x ) whih is onsidered as zero ime or he

4 JOURNAL OF TEXTILES AND POLYMERS, VOL. 6, NO., JANUARY 08 reovery mode. The ompression o he arpe a he ime (x ) is denoed by x =x 0 -x. The reovery proess was hen moniored and in every min inervals he hikness o he arpe (x ) is measured. This oninues up o 30 min. The hikness loss o he samples a he ime is hen onsidered as x=x 0 -x. IV. RESULTS AND DISCUSSION In his paper, he reovery propery o he pile arpes aer sai loading was invesigaed by presening wo visoelasi models. Analyial approah was used and he reovery-ime equaions were derived. The heoreial equaions were hen adaped o he experimenal daa using bes urve iing based on he leas square mehod. Deerminaion o he bes i equaion allows he exraing he disree visoelasi parameers o he models. The reovery behavior o he pile arpe was invesigaed in wo dieren sai load ime i.e. min and h. In eah level o sai loading, he values o hikness loss (x) were measured in he inerval imes o every min. Fig. shows he experimenal daa and he ied urves or reovery behavior o he arpe pile yarns aer applying min and h sai loading. Fig. reveals ha here is a good orrelaion beween he ied and he experimenal daa or wo Jeery s model. The ied urves show very high R-square o This an provide a suiable explanaion or he reovery behaviors o he arpe. The model is able o explain he non-reoverable deormaion o he arpe piles due o sai loading. The model is also desribes he ee o he ime o he onsan sai loading (See Table I). Eqs. (5a) and (5b) represenhe equaions o he ied urve wih linear Jeery s model and nonlinear Jeery s model respeively mod el (a) hours : x = 0.9e +.66 min ues : x.49e = + mod el (b) hours : x = an h (0.5.) min ues : x = an h (0.9.) (5a) (5b) (a) (b) Fig.. Fied urves vs. experimenal daa or reovery aer h and min sai loading: (a) linear Jeery s model and (b) nonlinear Jeery s model. To alulae he model parameers he onsan load,, is needed. This was alulaed rom he pile densiies and pressure load applied by he laboraory-saled sai loading apparaus. The onsan load,, applied o eah pile was alulaed as.4 N/pile. The model parameers were deermined using ied Eqs. (5a) and (5b) in aordane o Eq. (4). The resuls are shown in Table I. The good agreemen beween he ied urve and he experimenal daa suggess ha wo Jerey s model an predi well he reovery behavior o arpe piles aer sai loading. Analysis and omparison beween wo models revealed ha here was no signiian dierene beween he linear and quadrai nonlinear models in order o jusiy he reovery properies o he u-pile arpe aer removing o he sai loading. I an be onluded ha he Jeery s linear model shows signiian auray and an be proposed o explain he reovery properies o he upile arpes. Anoher ouome o he resuls is ha boh spring onsan and dashpo onsan show less values in longer sai loading. This shows learly ha he ime aes he ine sruure o he ibres. In oher words, he ime auses deerioraion in he rysal regions as well as he amorphous regions. This suggesion needs more ine sruural analysis. VI. SPEED OF RECOVERY The speed o reovery a he sar o reovery proess an

5 JAFARI AND GHANE: VISCOELASTIC MODELING OF THE RECOVERY BEHAVIOR OF... 3 TABLE I ESTIMATED VISCOELASTIC PARAMETERS Model Time R Spring onsan η min N. mm η min N. mm a) linear Jeery s model b) nonlinear Jeery s model min 0.96 E=0.37 (N/mm) h E=.54 (N/mm) min b =0. (N/mm ) h 0.97 b =.75 (N/mm ) be a good rierion o evaluae he ompression properies o he pile arpes. To ind he speed o reovery, he irs derivaion o reovery-ime equaion (Eq. 4) an be alulaed as shown below: η η a)x = e e η b. b. b.x e b) x = xe an h. se h. η η η (6) Applying he values o he parameers in o Eq. (6) he speed o reovery a zero ime or boh linear and nonlinear model were alulaed as an be seen in Table II. The experimenal values o he speed o reovery a zero ime were alulaed orm he slope o angen o he displaemen-ime urves (Fig. ) a zero ime (=0). The resuls o he heoreial and experimenal values o he speed o reovery a zero ime are shown in Table II. As seen in Table II, he speed o reovery a he sar o reovery (zero ime) is less in longer sai loading. The reason may be explained by he deerioraion or degradaion o he ine sruure o he ibers in longer ime o sai loading. The nonlinear model also shows lower reovery speed in min as well as h sai loading. Comparison o he heoreial and experimenal values o he speed o reovery a zero ime reveals ha wo values are reasonably lose o eah oher. Furhermore, he resuls o heoreial values by he nonlinear model are loser o he experimenal values. I an be onluded ha he nonlinear model is more reliable o predi he speed o reovery in omparison o he linear model. The reovery properies o he u pile arpes is aeed by dieren aors inluding he ype and mehanial properies o pile yarn and weigh and duraion o sai load. Finding an appropriae mehanial model and alulaing he visoelasi parameers allows invesigaing on he ee o dieren eeive aors on he reovery properies o he u pile arpes. Finally, we may be able o propose he sruure and maerials o gain opimum reovery properies. VI. CONCLUSIONS The aim o his paper was o ompare wo visoelasi models o desribe he reovery behavior o he pile arpe aer sai loading. Using analyial proedure reovery-ime equaions were derived and ompared o he experimenal daa. Bes ied urves based on he leas square mehod were deermined. The models were analyzed and a omparison was made beween he linear and quadrai nonlinear Jery s models. Using he analyial mehods he reovery equaions were derived and he disri visoelasi parameers were deermined and presened. The resul o urve iing proedure showed ha boh linear and nonlinear models i he experimenal daa signiianly. However, no signiian dierene was observed beween wo models. The nonlinear model provided less speed o reovery a he sar o he reovery TABLE II SPEED OF RECOVERY AT ZERO TIME FOR LINEAR AND NONLINEAR MODEL FOR RECOVERY a) linear Model Time Speed o reovery (mm/min) Speed o reoverya =0 (mm/min) Theoreial Experimenal min x = 0.38e Jeery s model b) nonlinear Jeery s model h x = 0.7e min x = 0.8seh (0.9) h x = 0.0seh (0.5)

6 4 JOURNAL OF TEXTILES AND POLYMERS, VOL. 6, NO., JANUARY 08 mode in omparison o he linear model. The resuls o he analysis also revealed ha he model parameers i.e. he spring onsens as well as he dashpo onsans are signiianly less in longer sai loading ime. I may be onluded ha he erm o sai loading aes he inernal sruure o iber. Deerioraion o he inernal sruure an lead o less value o model parameers. More ine sruure analysis is needed o veriy his onlusion. VII. ACKNOWLEDGMENT The auhors would like o express heir sinere hanks o he researh depuy o Isahan Universiy o Tehnology or he inanial suppor. REFERENCES [] Y. Korkmaz and S. DaliKoer, Resiliene behaviors o woven aryli arpes under shor- and long-erm sai loading, J. Tex. Ins., vol. 0, pp. 36-4, 00. [] S.M. Tabaabaei, M. Ghane, A. ZeinalHamadani, and H. Hasani, Modeling he unional ompression properies o hand-knoed arpes using aorial design and response surae mehodology, Fiber. Polym., vol. 5, pp , 04. [3] J.D. Ferry, Visoelasi properies o polymers, 3rd ed. New York: John Wiley & Sons, 980. [4] L. Meng and M. Wu, Sudy on sress relaxaion o membrane sruures in he presress sae by onsidering visoelasi properies o oaed abris, Thin. Wall. Sru., vol. 06, pp. 8-7, 06. [5] V.P.W. Shim, C.T. Lim, and K.J. Foo, Dynami mehanial properies o abri armour, In. J. Impa Eng., vol. 5, pp. -5, 00. [6] L. Vangheluwe, Relaxaion and inverse relaxaion o yarns aer dynami loading, Tex. Res. J., vol. 63, pp , 993. [7] A.M. Manih, R. Miguel, M.J.d.S. Silva, J. Luas, M. Marí, and D. Cayuela, Ee o proessing and wearing on visoelasi modeling o polylaide/ wool and polyeser/wool woven abris subjeed o bursing, Tex. Res. J., vol. 84, pp , 04. [8] A. Asayesh, A.A.A. Jeddi, and P. Ghadimi, Modeling he aigue behavior o plain woven abris Consrued rom exured polyeser yarn, Tex. Res. J., vol. 79, pp.3-, 009. [9] A. Asayesh and A.A.A. Jeddi, Modeling he reep behavior o plain woven abris onsrued rom exured polyeser yarn, Tex. Res. J., vol. 80, pp , 00. [0] N. Hashemi, A. Asayesh, Ali A.A. Jeddi, and T. Ardakani, The inluene o wo bar warp-knied sruure on he abri ensile sress relaxaion par I: (reverse lokni, sharkskin, queens ord), J. Tex. Ins., vol. 07, pp. 5 54, 06. [] T. Ardakani, A. Asayesh, and Ali A.A. Jeddi, The inluene o wo bar warp-knied sruure on he abri ensile sress relaxaion par II: (lokni, sain, loop raised), J. Tex. Ins., vol. 07, No., pp , 06. [] S. Khavari and M. Ghane, An analyial approah or he ompression and reovery behavior o u pile arpes under onsan rae o ompression by mehanial models, Fiber. Polym., vol. 8, pp , 07. [3] S. Jaari and M. Ghane, An analyial approah or he reovery behavior o u pile arpe aer sai loading by mehanial models, Fiber. Polym., vol.7, pp , 06. [4] S. Jaari and M. Ghane, Analysis o he ee o UV radiaion on he reovery properies o pile arpe aer sai loading hrough analyial and visoelasi modeling, J. Tex. Ins., vol. 08, pp , 07. [5] F. Mainardi and G. Spada, Creep, relaxaion and visosiy properies or basi raional models in rheology, European Physial J., vol. 93, pp , 0.

Concrete damaged plasticity model

Concrete damaged plasticity model Conree damaged asiiy model Conree damaged asiiy model is a maerial model for he analysis of onree sruures mainly under dynami loads suh as earhquakes(only aes an be analyzed under he dynami loads like

More information

5.2 Design for Shear (Part I)

5.2 Design for Shear (Part I) 5. Design or Shear (Par I) This seion overs he ollowing opis. General Commens Limi Sae o Collapse or Shear 5..1 General Commens Calulaion o Shear Demand The objeive o design is o provide ulimae resisane

More information

Linear Quadratic Regulator (LQR) - State Feedback Design

Linear Quadratic Regulator (LQR) - State Feedback Design Linear Quadrai Regulaor (LQR) - Sae Feedbak Design A sysem is expressed in sae variable form as x = Ax + Bu n m wih x( ) R, u( ) R and he iniial ondiion x() = x A he sabilizaion problem using sae variable

More information

Nonlinear Finite Element Analysis of Shotcrete Lining Reinforced with Steel Fibre and Steel Sets

Nonlinear Finite Element Analysis of Shotcrete Lining Reinforced with Steel Fibre and Steel Sets IACSIT Inernaional Journal of Engineering and Tehnology, Vol. 5, No. 6, Deember 2013 Nonlinear Finie Elemen Analysis of Shoree Lining Reinfored wih Seel Fibre and Seel Ses Jeong Soo Kim, Moon Kyum Kim,

More information

1.054/1.541 Mechanics and Design of Concrete Structures (3-0-9) Outline 5 Creep and Shrinkage Deformation

1.054/1.541 Mechanics and Design of Concrete Structures (3-0-9) Outline 5 Creep and Shrinkage Deformation 1.54/1.541 Mehanis and Design of Conree ruures pring 24 Prof. Oral Buyukozurk Massahuses Insiue of Tehnology Ouline 5 1.54/1.541 Mehanis and Design of Conree ruures (3--9 Ouline 5 and hrinkage Deformaion

More information

An Inventory Model for Weibull Time-Dependence. Demand Rate with Completely Backlogged. Shortages

An Inventory Model for Weibull Time-Dependence. Demand Rate with Completely Backlogged. Shortages Inernaional Mahemaial Forum, 5, 00, no. 5, 675-687 An Invenory Model for Weibull Time-Dependene Demand Rae wih Compleely Baklogged Shorages C. K. Tripahy and U. Mishra Deparmen of Saisis, Sambalpur Universiy

More information

Polymer Engineering (MM3POE)

Polymer Engineering (MM3POE) Polymer Engineering (MM3POE) VISCOELASTICITY hp://www.noingham.ac.uk/~eazacl/mm3poe Viscoelasiciy 1 Conens Wha is viscoelasiciy? Fundamenals Creep & creep recovery Sress relaxaion Modelling viscoelasic

More information

Hybrid probabilistic interval dynamic analysis of vehicle-bridge interaction system with uncertainties

Hybrid probabilistic interval dynamic analysis of vehicle-bridge interaction system with uncertainties 1 APCOM & SCM 11-14 h Deember, 13, Singapore Hybrid probabilisi inerval dynami analysis of vehile-bridge ineraion sysem wih unerainies Nengguang iu 1, * Wei Gao 1, Chongmin Song 1 and Nong Zhang 1 Shool

More information

Derivation of longitudinal Doppler shift equation between two moving bodies in reference frame at rest

Derivation of longitudinal Doppler shift equation between two moving bodies in reference frame at rest Deriaion o longiudinal Doppler shi equaion beween wo moing bodies in reerene rame a res Masanori Sao Honda Eleronis Co., d., Oyamazuka, Oiwa-ho, Toyohashi, ihi 44-393, Japan E-mail: msao@honda-el.o.jp

More information

Theory of! Partial Differential Equations-I!

Theory of! Partial Differential Equations-I! hp://users.wpi.edu/~grear/me61.hml! Ouline! Theory o! Parial Dierenial Equaions-I! Gréar Tryggvason! Spring 010! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and

More information

Navneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi

Navneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi Creep in Viscoelasic Subsances Numerical mehods o calculae he coefficiens of he Prony equaion using creep es daa and Herediary Inegrals Mehod Navnee Saini, Mayank Goyal, Vishal Bansal (23); Term Projec

More information

Theory of! Partial Differential Equations!

Theory of! Partial Differential Equations! hp://www.nd.edu/~gryggva/cfd-course/! Ouline! Theory o! Parial Dierenial Equaions! Gréar Tryggvason! Spring 011! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and

More information

ON UNITARY RHEOLOGICAL APPROACH OF VIBRATION ISOLATION PASSIVE DEVICES

ON UNITARY RHEOLOGICAL APPROACH OF VIBRATION ISOLATION PASSIVE DEVICES 8h Inernaional DAAAM Bali Conferene "INDUTRIAL ENGINEERING - 9- April, Tallinn, Esonia ON UNITARY RHEOLOGICAL APPROACH O VIBRATION IOLATION PAIVE DEVICE Poirnihe, A.; Nasa,.; Leopa, A.; Debelea, C. & Capaana,

More information

Analysis of Tubular Linear Permanent Magnet Motor for Drilling Application

Analysis of Tubular Linear Permanent Magnet Motor for Drilling Application Analysis of Tubular Linear Permanen Magne Moor for Drilling Appliaion Shujun Zhang, Lars Norum, Rober Nilssen Deparmen of Eleri Power Engineering Norwegian Universiy of Siene and Tehnology, Trondheim 7491

More information

The Nottingham eprints service makes this work by researchers of the University of Nottingham available open access under the following conditions.

The Nottingham eprints service makes this work by researchers of the University of Nottingham available open access under the following conditions. Hyde, Chrisopher J. and Hyde, T.H. and Sun, Wei and Beker, A.A. () Damage mehanis based prediions of reep rak growh in 36 sainless seel. Engineering Fraure Mehanis, 77 (). pp. 385-4. ISSN 3-7944 Aess from

More information

Shear failure of plain concrete in strain localized area

Shear failure of plain concrete in strain localized area Shear failure of plain onree in srain loalized area Y. Kaneko & H. Mihashi Tohoku Universiy, Sendai, Miyagi, Japan S. Ishihara Asanuma Corporaion, Takasuki, Osaka, Japan ABSTRACT: The objeive of his paper

More information

Mass Transfer Coefficients (MTC) and Correlations I

Mass Transfer Coefficients (MTC) and Correlations I Mass Transfer Mass Transfer Coeffiiens (MTC) and Correlaions I 7- Mass Transfer Coeffiiens and Correlaions I Diffusion an be desribed in wo ways:. Deailed physial desripion based on Fik s laws and he diffusion

More information

AN INVENTORY MODEL FOR DETERIORATING ITEMS WITH EXPONENTIAL DECLINING DEMAND AND PARTIAL BACKLOGGING

AN INVENTORY MODEL FOR DETERIORATING ITEMS WITH EXPONENTIAL DECLINING DEMAND AND PARTIAL BACKLOGGING Yugoslav Journal of Operaions Researh 5 (005) Number 77-88 AN INVENTORY MODEL FOR DETERIORATING ITEMS WITH EXPONENTIAL DECLINING DEMAND AND PARTIAL BACKLOGGING Liang-Yuh OUYANG Deparmen of Managemen Sienes

More information

Numerical simulation of damage in glass subjected to static indentation

Numerical simulation of damage in glass subjected to static indentation 8 ème Congrès Français de Méanique Grenoble, 7- aoû 007 Numerial simulaion of damage in glass subjeed o sai indenaion Jewan Ismail, Fahmi Zaïri, Moussa Naï-Abdelaziz & Ziouni Azari Laboraoire de Méanique

More information

Tensile and Compressive Damage Coupling for Fully-reversed Bending Fatigue of Fibre-reinforced Composites

Tensile and Compressive Damage Coupling for Fully-reversed Bending Fatigue of Fibre-reinforced Composites Van Paepegem, W. and Degriek, J. (00. Tensile and Compressive Damage Coupling for Fully-reversed Bending Faigue of Fibrereinfored Composies. Faigue and Fraure of Engineering Maerials & Sruures, 5(6, 547-56.

More information

Calculation of Initial Stiffness of Semirigid Connections with Consideration of Rotational Constraint on Angle from Beam Contact Surface

Calculation of Initial Stiffness of Semirigid Connections with Consideration of Rotational Constraint on Angle from Beam Contact Surface Calulaion of Iniial Siffness of Semirigid Conneions wih Consideraion of Roaional Consrain on Angle from Beam Cona Surfae X.G. Lin Osaka Insiue of Tehnology, Japan K. Asada Oayashi Corporaion, Japan SUMMARY:

More information

mywbut.com Lesson 11 Study of DC transients in R-L-C Circuits

mywbut.com Lesson 11 Study of DC transients in R-L-C Circuits mywbu.om esson Sudy of DC ransiens in R--C Ciruis mywbu.om Objeives Be able o wrie differenial equaion for a d iruis onaining wo sorage elemens in presene of a resisane. To develop a horough undersanding

More information

COSC 3361 Numerical Analysis I Ordinary Differential Equations (I) - Introduction

COSC 3361 Numerical Analysis I Ordinary Differential Equations (I) - Introduction COSC 336 Numerial Analsis I Ordinar Dierenial Equaions I - Inroduion Edgar Gabriel Fall 5 COSC 336 Numerial Analsis I Edgar Gabriel Terminolog Dierenial equaions: equaions onaining e derivaive o a union

More information

Boyce/DiPrima 9 th ed, Ch 6.1: Definition of. Laplace Transform. In this chapter we use the Laplace transform to convert a

Boyce/DiPrima 9 th ed, Ch 6.1: Definition of. Laplace Transform. In this chapter we use the Laplace transform to convert a Boye/DiPrima 9 h ed, Ch 6.: Definiion of Laplae Transform Elemenary Differenial Equaions and Boundary Value Problems, 9 h ediion, by William E. Boye and Rihard C. DiPrima, 2009 by John Wiley & Sons, In.

More information

Numerical Simulation of Thermal Stresses in Prismatic Concrete Beams Reinforced with FRP Bars under Low Temperatures

Numerical Simulation of Thermal Stresses in Prismatic Concrete Beams Reinforced with FRP Bars under Low Temperatures Cemisry and Maerials Resear, Vol.5 013 Speial Issue for Inernaional Congress on Maerials & Sruural Sabiliy, Raba, Moroo, 7-30 November 013 Numerial Simulaion of Termal Sresses in Prismai Conree Beams Reinfored

More information

I. OBJECTIVE OF THE EXPERIMENT.

I. OBJECTIVE OF THE EXPERIMENT. I. OBJECTIVE OF THE EXPERIMENT. Swissmero raels a high speeds hrough a unnel a low pressure. I will hereore undergo ricion ha can be due o: ) Viscosiy o gas (c. "Viscosiy o gas" eperimen) ) The air in

More information

This document is meant to encapsulate the discussion from Thursday July 9 th 2009 on the review of the paper:

This document is meant to encapsulate the discussion from Thursday July 9 th 2009 on the review of the paper: This doumen is mean o enapsulae he disussion from Thursday July 9 h 2009 on he review of he paper: No seady sae flows below he yield sress. A rue yield sress a las? -Møller, Fall, Bonn (ArXiv: 0904.1467v1

More information

SIMULATION STUDY OF STOCHASTIC CHANNEL REDISTRIBUTION

SIMULATION STUDY OF STOCHASTIC CHANNEL REDISTRIBUTION Developmens in Business Simulaion and Experienial Learning, Volume 3, 3 SIMULATIO STUDY OF STOCHASTIC CHAEL REDISTRIBUTIO Yao Dong-Qing Towson Universiy dyao@owson.edu ABSTRACT In his paper, we invesigae

More information

Correlating EUV TMOKE and ARPES measurements to understand the temporal

Correlating EUV TMOKE and ARPES measurements to understand the temporal Correlaing EUV TMOKE and ARPES measuremens o undersand he emporal and spaial lengh sales underlying ulrafas demagneizaion in ferromagnes Wenjing You 1, Phoebe Tengdin 1, Cong Chen 1, Xun Shi 1 *, Dmiriy

More information

Optimal Transform: The Karhunen-Loeve Transform (KLT)

Optimal Transform: The Karhunen-Loeve Transform (KLT) Opimal ransform: he Karhunen-Loeve ransform (KL) Reall: We are ineresed in uniary ransforms beause of heir nie properies: energy onservaion, energy ompaion, deorrelaion oivaion: τ (D ransform; assume separable)

More information

The Role of Money: Credible Asset or Numeraire? Masayuki Otaki (Institute of Social Science, University of Tokyo)

The Role of Money: Credible Asset or Numeraire? Masayuki Otaki (Institute of Social Science, University of Tokyo) DBJ Disussion Paper Series, No.04 The Role of Money: Credible Asse or Numeraire? Masayuki Oaki (Insiue of Soial Siene, Universiy of Tokyo) January 0 Disussion Papers are a series of preliminary maerials

More information

EE40 Summer 2005: Lecture 2 Instructor: Octavian Florescu 1. Measuring Voltages and Currents

EE40 Summer 2005: Lecture 2 Instructor: Octavian Florescu 1. Measuring Voltages and Currents Announemens HW # Due oday a 6pm. HW # posed online oday and due nex Tuesday a 6pm. Due o sheduling onflis wih some sudens, lasses will resume normally his week and nex. Miderm enaively 7/. EE4 Summer 5:

More information

PET467E-Analysis of Well Pressure Tests/2008 Spring Semester/İTÜ Midterm Examination (Duration 3:00 hours) Solutions

PET467E-Analysis of Well Pressure Tests/2008 Spring Semester/İTÜ Midterm Examination (Duration 3:00 hours) Solutions M. Onur 03.04.008 PET467E-Analysis of Well Pressure Tess/008 Spring Semeser/İTÜ Miderm Examinaion (Duraion 3:00 hours) Soluions Name of he Suden: Insrucions: Before saring he exam, wrie your name clearly

More information

Generalized electromagnetic energy-momentum tensor and scalar curvature of space at the location of charged particle

Generalized electromagnetic energy-momentum tensor and scalar curvature of space at the location of charged particle Generalized eleromagnei energy-momenum ensor and salar urvaure of spae a he loaion of harged parile A.L. Kholmeskii 1, O.V. Missevih and T. Yarman 3 1 Belarus Sae Universiy, Nezavisimosi Avenue, 0030 Minsk,

More information

Number of modes per unit volume of the cavity per unit frequency interval is given by: Mode Density, N

Number of modes per unit volume of the cavity per unit frequency interval is given by: Mode Density, N SMES404 - LASER PHYSCS (LECTURE 5 on /07/07) Number of modes per uni volume of he aviy per uni frequeny inerval is given by: 8 Mode Densiy, N (.) Therefore, energy densiy (per uni freq. inerval); U 8h

More information

The Nottingham eprints service makes this work by researchers of the University of Nottingham available open access under the following conditions.

The Nottingham eprints service makes this work by researchers of the University of Nottingham available open access under the following conditions. Liu, Tao and Wadley, H.N.G. and Deshpande, V.S. (014) Dynami ompression o oam suppored plaes impaed by high veloiy soil. Inernaional Journal o Impa Engineering, 63. pp. 88-106. ISSN 0734-743X Aess rom

More information

Energy Momentum Tensor for Photonic System

Energy Momentum Tensor for Photonic System 018 IJSST Volume 4 Issue 10 Prin ISSN : 395-6011 Online ISSN : 395-60X Themed Seion: Siene and Tehnology Energy Momenum Tensor for Phooni Sysem ampada Misra Ex-Gues-Teaher, Deparmens of Eleronis, Vidyasagar

More information

CONSTRUCTION AND USE OF IMITATING MODEL IN THE PROCESS OF MULTI-CRITERIA OPTIMIZATION OF THE SEPARATE-FLOW NOZZLE

CONSTRUCTION AND USE OF IMITATING MODEL IN THE PROCESS OF MULTI-CRITERIA OPTIMIZATION OF THE SEPARATE-FLOW NOZZLE CONSTRUCTION AND USE OF IMITATING MODEL IN THE PROCESS OF MULTI-CRITERIA OPTIMIZATION OF THE SEPARATE-FLOW NOZZLE N.A.Zlenko*, S.V.Mikhaylov*, A.V.Shenkin* * TsAGI Keywords: nozzle, opimum aerodynami design

More information

v A Since the axial rigidity k ij is defined by P/v A, we obtain Pa 3

v A Since the axial rigidity k ij is defined by P/v A, we obtain Pa 3 The The rd rd Inernaional Conference on on Design Engineering and Science, ICDES 14 Pilsen, Czech Pilsen, Republic, Czech Augus Republic, 1 Sepember 1-, 14 In-plane and Ou-of-plane Deflecion of J-shaped

More information

A new flexible Weibull distribution

A new flexible Weibull distribution Communicaions for Saisical Applicaions and Mehods 2016, Vol. 23, No. 5, 399 409 hp://dx.doi.org/10.5351/csam.2016.23.5.399 Prin ISSN 2287-7843 / Online ISSN 2383-4757 A new flexible Weibull disribuion

More information

Fitting Parameters in a Differential Equation With a Non-Analytical Solution

Fitting Parameters in a Differential Equation With a Non-Analytical Solution NDSolve u.nb 1 Fiing Parameers in a Dierenial Equaion Wih a Non-Analyical Soluion Mahew Smih 9-Jan-005 In[]:= Remove "Global` " O General::"spell" O General::"spell1" Graphics` Oen dierenial equaions do

More information

Combined Bending with Induced or Applied Torsion of FRP I-Section Beams

Combined Bending with Induced or Applied Torsion of FRP I-Section Beams Combined Bending wih Induced or Applied Torsion of FRP I-Secion Beams MOJTABA B. SIRJANI School of Science and Technology Norfolk Sae Universiy Norfolk, Virginia 34504 USA sirjani@nsu.edu STEA B. BONDI

More information

Summary of shear rate kinematics (part 1)

Summary of shear rate kinematics (part 1) InroToMaFuncions.pdf 4 CM465 To proceed o beer-designed consiuive equaions, we need o know more abou maerial behavior, i.e. we need more maerial funcions o predic, and we need measuremens of hese maerial

More information

ELASTO-PLASTIC FRACTURE MECHANICS FINITE ELEMENT ANALYSIS

ELASTO-PLASTIC FRACTURE MECHANICS FINITE ELEMENT ANALYSIS Third Serbian (8 h Yu) Congress on Theoreial and Applied Mehanis Vlasina lake, Serbia, 5-8 July C-3 ELASTO-PLASTIC FRACTURE MECHANICS FINITE ELEMENT ANALYSIS Emina S. Dzindo, A. Sedmak, B. Perovski Innovaion

More information

Mechanical Fatigue and Load-Induced Aging of Loudspeaker Suspension. Wolfgang Klippel,

Mechanical Fatigue and Load-Induced Aging of Loudspeaker Suspension. Wolfgang Klippel, Mechanical Faigue and Load-Induced Aging of Loudspeaker Suspension Wolfgang Klippel, Insiue of Acousics and Speech Communicaion Dresden Universiy of Technology presened a he ALMA Symposium 2012, Las Vegas

More information

The Asymptotical Behavior of Probability Measures for the Fluctuations of Stochastic Models

The Asymptotical Behavior of Probability Measures for the Fluctuations of Stochastic Models The Asympoial Behavior of Probabiliy Measures for he Fluuaions of Sohasi Models JUN WANG CUINING WEI Deparmen of Mahemais College of Siene Beijing Jiaoong Universiy Beijing Jiaoong Universiy Beijing 44

More information

Lorentz Transformation Properties of Currents for the Particle-Antiparticle Pair Wave Functions

Lorentz Transformation Properties of Currents for the Particle-Antiparticle Pair Wave Functions Open Aess Library Journal 17, Volume 4, e373 ISSN Online: 333-971 ISSN Prin: 333-975 Lorenz Transformaion Properies of Currens for he Parile-Aniparile Pair Wave Funions Raja Roy Deparmen of Eleronis and

More information

04. Kinetics of a second order reaction

04. Kinetics of a second order reaction 4. Kineics of a second order reacion Imporan conceps Reacion rae, reacion exen, reacion rae equaion, order of a reacion, firs-order reacions, second-order reacions, differenial and inegraed rae laws, Arrhenius

More information

BEng (Hons) Telecommunications. Examinations for / Semester 2

BEng (Hons) Telecommunications. Examinations for / Semester 2 BEng (Hons) Telecommunicaions Cohor: BTEL/14/FT Examinaions for 2015-2016 / Semeser 2 MODULE: ELECTROMAGNETIC THEORY MODULE CODE: ASE2103 Duraion: 2 ½ Hours Insrucions o Candidaes: 1. Answer ALL 4 (FOUR)

More information

Problem 1 / 25 Problem 2 / 10 Problem 3 / 15 Problem 4 / 30 Problem 5 / 20 TOTAL / 100

Problem 1 / 25 Problem 2 / 10 Problem 3 / 15 Problem 4 / 30 Problem 5 / 20 TOTAL / 100 Deparmen of Applied Eonomis Johns Hopkins Universiy Eonomis 60 Maroeonomi Theory and Poliy Miderm Exam Suggesed Soluions Professor Sanjay Chugh Summer 0 NAME: The Exam has a oal of five (5) problems and

More information

Effect of Aggregate Gradation on Compressive Strength and Elastic Modulus of Cement Treated Aggregate Base Material for Highway Pavement

Effect of Aggregate Gradation on Compressive Strength and Elastic Modulus of Cement Treated Aggregate Base Material for Highway Pavement IOSR Journal of Engineering (IOSRJEN) ISSN (e): 2250-3021, ISSN (p): 2278-8719 Vol. 07, Issue 10 (Oober. 2017), V2 PP 79-89 www.iosrjen.org Effe of Aggregae Gradaion on Compressive Srengh and Elasi Modulus

More information

Teacher Quality Policy When Supply Matters: Online Appendix

Teacher Quality Policy When Supply Matters: Online Appendix Teaher Qualiy Poliy When Supply Maers: Online Appendix Jesse Rohsein July 24, 24 A Searh model Eah eaher draws a single ouside job offer eah year. If she aeps he offer, she exis eahing forever. The ouside

More information

New Oscillation Criteria For Second Order Nonlinear Differential Equations

New Oscillation Criteria For Second Order Nonlinear Differential Equations Researh Inveny: Inernaional Journal Of Engineering And Siene Issn: 78-47, Vol, Issue 4 (Feruary 03), Pp 36-4 WwwResearhinvenyCom New Osillaion Crieria For Seond Order Nonlinear Differenial Equaions Xhevair

More information

Dual Phase Lag Model of Melting Process in Domain of Metal Film Subjected to an External Heat Flux

Dual Phase Lag Model of Melting Process in Domain of Metal Film Subjected to an External Heat Flux A C H I V E S o F O U N D Y E N G I N E E I N G Published uarerly as he organ o he Foundry Commission o he Polish Aademy o Sienes ISSN (1897-3310) Volume 16 Issue /016 85 90 16/ Dual Phase Lag Model o

More information

Molecular Motion in Isotropic Turbulence

Molecular Motion in Isotropic Turbulence Moleular Moion in Isoropi Turbulene Jing Fan, Jian-Zheng Jiang, and Fei Fei Laboraory of High Temperaure Gas Dynamis, Insiue of Mehanis Chinese Aademy of Sienes, Being 9, China Absra Moleular moion in

More information

κt π = (5) T surrface k BASELINE CASE

κt π = (5) T surrface k BASELINE CASE II. BASELINE CASE PRACICAL CONSIDERAIONS FOR HERMAL SRESSES INDUCED BY SURFACE HEAING James P. Blanhard Universi of Wisonsin Madison 15 Engineering Dr. Madison, WI 5376-169 68-63-391 blanhard@engr.is.edu

More information

From a detailed model of porous catalytic washcoat to the effective model of entire catalytic monolith

From a detailed model of porous catalytic washcoat to the effective model of entire catalytic monolith Insiue of Chemial ehnology Prague Ceh Republi From a deailed model of porous aalyi washoa o he effeive model of enire aalyi monolih Per Kočí Vladimír Nová Franiše Šěpáne Miloš Mare Milan Kubíče hp://www.vsh./monolih

More information

Mahgoub Transform Method for Solving Linear Fractional Differential Equations

Mahgoub Transform Method for Solving Linear Fractional Differential Equations Mahgoub Transform Mehod for Solving Linear Fraional Differenial Equaions A. Emimal Kanaga Puhpam 1,* and S. Karin Lydia 2 1* Assoiae Professor&Deparmen of Mahemais, Bishop Heber College Tiruhirappalli,

More information

A semi-analytical model for polymers subjected to high strain rates

A semi-analytical model for polymers subjected to high strain rates 5 h European LS-DYNA Users Conferene Maerial Tehnology A semi-analyial model for polymers subjeed o high srain raes Auhors: A. Haufe, DYNAmore GmbH P.A. Du Bois, Consuling Engineer S. Kolling & M. Feuh,

More information

A New Formulation of Electrodynamics

A New Formulation of Electrodynamics . Eleromagnei Analysis & Appliaions 1 457-461 doi:1.436/jemaa.1.86 Published Online Augus 1 hp://www.sirp.org/journal/jemaa A New Formulaion of Elerodynamis Arbab I. Arbab 1 Faisal A. Yassein 1 Deparmen

More information

Wrinkling Analysis of Rectangular Soft-Core Composite Sandwich Plates

Wrinkling Analysis of Rectangular Soft-Core Composite Sandwich Plates Wrinkling Analysis of Reangular Sof-Core Composie Sandwih Plaes Mohammad Mahdi Kheirikhah and Mohammad Reza Khalili Absra In he presen haper, a new improved higher-order heory is presened for wrinkling

More information

A Note on Fractional Electrodynamics. Abstract

A Note on Fractional Electrodynamics. Abstract Commun Nonlinear Sci Numer Simula 8 (3 589 593 A Noe on Fracional lecrodynamics Hosein Nasrolahpour Absrac We invesigae he ime evoluion o he racional elecromagneic waves by using he ime racional Maxwell's

More information

A comparative Study of Contact Problems Solution Based on the Penalty and Lagrange Multiplier Approaches

A comparative Study of Contact Problems Solution Based on the Penalty and Lagrange Multiplier Approaches Journal of he Serbian Soiey for ompuaional Mehanis / Vol. / o., 2007 / pp. 74-83 A omparaive Sudy of ona Problems Soluion Based on he Penaly and Lagrange Muliplier Approahes S. Vulovi, M. Zivovi,. Grujovi,

More information

MOMENTUM CONSERVATION LAW

MOMENTUM CONSERVATION LAW 1 AAST/AEDT AP PHYSICS B: Impulse and Momenum Le us run an experimen: The ball is moving wih a velociy of V o and a force of F is applied on i for he ime inerval of. As he resul he ball s velociy changes

More information

di Bernardo, M. (1995). A purely adaptive controller to synchronize and control chaotic systems.

di Bernardo, M. (1995). A purely adaptive controller to synchronize and control chaotic systems. di ernardo, M. (995). A purely adapive conroller o synchronize and conrol chaoic sysems. hps://doi.org/.6/375-96(96)8-x Early version, also known as pre-prin Link o published version (if available):.6/375-96(96)8-x

More information

Peakon, pseudo-peakon, and cuspon solutions for two generalized Camassa-Holm equations

Peakon, pseudo-peakon, and cuspon solutions for two generalized Camassa-Holm equations JOURNAL OF MATHEMATICAL PHYSICS 54 13501 (013) Peakon pseudo-peakon and uspon soluions for wo generalized Camassa-Holm equaions Jibin Li 1a) and Zhijun Qiao 3a) 1 Deparmen of Mahemais Zhejiang Normal Universiy

More information

Scientific Research of the Institute of Mathematics and Computer Science DIFFERENT VARIANTS OF THE BOUNDARY ELEMENT METHOD FOR PARABOLIC EQUATIONS

Scientific Research of the Institute of Mathematics and Computer Science DIFFERENT VARIANTS OF THE BOUNDARY ELEMENT METHOD FOR PARABOLIC EQUATIONS Scieniic Research o he Insiue o Mahemaics and Compuer Science DIERENT VARIANTS O THE BOUNDARY ELEMENT METHOD OR PARABOLIC EQUATIONS Ewa Majchrzak,, Ewa Ładyga Jerzy Mendakiewicz, Alicja Piasecka Belkhaya

More information

Modeling and Simulation of Viscoelastic Flows in Polymer Processing with Integral Constitutive Equations Evan Mitsoulis

Modeling and Simulation of Viscoelastic Flows in Polymer Processing with Integral Constitutive Equations Evan Mitsoulis Modeling and Simulaion of Viscoelasic Flows in Polymer Processing wih Inegral onsiuive Equaions Evan Misoulis AMP - R&D ompuer-aided Maerials Processing Rheology & Design School of Mining Engineering and

More information

Viscoelastic Catenary

Viscoelastic Catenary Viscoelasic Caenary Anshuman Roy 1 Inroducion This paper seeks o deermine he shape of a hin viscoelasic fluid filamen as i sags under is own weigh. The problem is an exension of he viscous caenary [1]

More information

ERRATA. Figure GL. 2 TRANSVERSE CROSS SECTION OF A SCREW SLOT

ERRATA. Figure GL. 2 TRANSVERSE CROSS SECTION OF A SCREW SLOT srew slo: a semi-hollow in an exrusion inended o reain a srew arallel o he axis of he exrusion. (See Figure GL.). Figure GL. TRANSVERSE CROSS SECTION OF A SCREW SLOT self-drilling srew: a srew ha drills

More information

Amit Mehra. Indian School of Business, Hyderabad, INDIA Vijay Mookerjee

Amit Mehra. Indian School of Business, Hyderabad, INDIA Vijay Mookerjee RESEARCH ARTICLE HUMAN CAPITAL DEVELOPMENT FOR PROGRAMMERS USING OPEN SOURCE SOFTWARE Ami Mehra Indian Shool of Business, Hyderabad, INDIA {Ami_Mehra@isb.edu} Vijay Mookerjee Shool of Managemen, Uniersiy

More information

Lecture 4 Kinetics of a particle Part 3: Impulse and Momentum

Lecture 4 Kinetics of a particle Part 3: Impulse and Momentum MEE Engineering Mechanics II Lecure 4 Lecure 4 Kineics of a paricle Par 3: Impulse and Momenum Linear impulse and momenum Saring from he equaion of moion for a paricle of mass m which is subjeced o an

More information

A. V. SVISHCHUK AND A. V. KALEMANOVA

A. V. SVISHCHUK AND A. V. KALEMANOVA Teoriχ $imovir. a maem. sais. Vip. 61, 1999 Theor. Probabiliy and Mah. Sais. No. 61, UDC 519.1 THE STOCHASTIC STABILITY OF INTEREST RATES WITH JUMP CHANGES A. V. SVISHCHUK AND A. V. KALEMANOVA Absra. The

More information

Problem Set 9 Due December, 7

Problem Set 9 Due December, 7 EE226: Random Proesses in Sysems Leurer: Jean C. Walrand Problem Se 9 Due Deember, 7 Fall 6 GSI: Assane Gueye his problem se essenially reviews Convergene and Renewal proesses. No all exerises are o be

More information

SUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL

SUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL HE PUBLISHING HOUSE PROCEEDINGS OF HE ROMANIAN ACADEMY, Series A, OF HE ROMANIAN ACADEMY Volume, Number 4/200, pp 287 293 SUFFICIEN CONDIIONS FOR EXISENCE SOLUION OF LINEAR WO-POIN BOUNDARY PROBLEM IN

More information

Analysis of composite T beam composed of timber, concrete and carbon strip

Analysis of composite T beam composed of timber, concrete and carbon strip WSEAS TRANSACTONS on APPLED and THEORETCAL ECHANCS Analysis o omposie T beam omposed o imber onree and arbon srip ATJAŽ TAJNK PETER DOBRLA ROSLAV PREROV Fauly o ivil engineering Universiy o aribor Smeanova

More information

Electrical and current self-induction

Electrical and current self-induction Elecrical and curren self-inducion F. F. Mende hp://fmnauka.narod.ru/works.hml mende_fedor@mail.ru Absrac The aricle considers he self-inducance of reacive elemens. Elecrical self-inducion To he laws of

More information

Biol. 356 Lab 8. Mortality, Recruitment, and Migration Rates

Biol. 356 Lab 8. Mortality, Recruitment, and Migration Rates Biol. 356 Lab 8. Moraliy, Recruimen, and Migraion Raes (modified from Cox, 00, General Ecology Lab Manual, McGraw Hill) Las week we esimaed populaion size hrough several mehods. One assumpion of all hese

More information

arxiv: v1 [physics.data-an] 14 Dec 2015

arxiv: v1 [physics.data-an] 14 Dec 2015 1/ noise rom he nonlinear ransormaions o he variables Bronislovas Kaulakys, Miglius Alaburda, and Julius Ruseckas Insiue o Theoreical Physics and Asronomy, Vilnius Universiy, A. Gošauo 1, 118 Vilnius,

More information

New effective moduli of isotropic viscoelastic composites. Part I. Theoretical justification

New effective moduli of isotropic viscoelastic composites. Part I. Theoretical justification IOP Conference Series: Maerials Science and Engineering PAPE OPEN ACCESS New effecive moduli of isoropic viscoelasic composies. Par I. Theoreical jusificaion To cie his aricle: A A Sveashkov and A A akurov

More information

Matlab and Python programming: how to get started

Matlab and Python programming: how to get started Malab and Pyhon programming: how o ge sared Equipping readers he skills o wrie programs o explore complex sysems and discover ineresing paerns from big daa is one of he main goals of his book. In his chaper,

More information

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits EEE25 ircui Analysis I Se 4: apaciors, Inducors, and Firs-Order inear ircuis Shahriar Mirabbasi Deparmen of Elecrical and ompuer Engineering Universiy of Briish olumbia shahriar@ece.ubc.ca Overview Passive

More information

A Numerical Hydraulic Fracture Model Using the Extended Finite Element Method

A Numerical Hydraulic Fracture Model Using the Extended Finite Element Method nernaional Conferene on Mehanial and ndusrial Engineering (CME'2013) Augus 28-29, 2013 Penang (Malaysia) A Numerial Hydrauli Fraure Model Using he Exended Finie Elemen Mehod Ashkan. Mahdavi, and Soheil.

More information

Types of Exponential Smoothing Methods. Simple Exponential Smoothing. Simple Exponential Smoothing

Types of Exponential Smoothing Methods. Simple Exponential Smoothing. Simple Exponential Smoothing M Business Forecasing Mehods Exponenial moohing Mehods ecurer : Dr Iris Yeung Room No : P79 Tel No : 788 8 Types of Exponenial moohing Mehods imple Exponenial moohing Double Exponenial moohing Brown s

More information

CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK

CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK 175 CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK 10.1 INTRODUCTION Amongs he research work performed, he bes resuls of experimenal work are validaed wih Arificial Neural Nework. From he

More information

Vectorautoregressive Model and Cointegration Analysis. Time Series Analysis Dr. Sevtap Kestel 1

Vectorautoregressive Model and Cointegration Analysis. Time Series Analysis Dr. Sevtap Kestel 1 Vecorauoregressive Model and Coinegraion Analysis Par V Time Series Analysis Dr. Sevap Kesel 1 Vecorauoregression Vecor auoregression (VAR) is an economeric model used o capure he evoluion and he inerdependencies

More information

A state space approach to calculating the Beveridge Nelson decomposition

A state space approach to calculating the Beveridge Nelson decomposition Eonomis Leers 75 (00) 3 7 www.elsevier.om/ loae/ eonbase A sae spae approah o alulaing he Beveridge Nelson deomposiion James C. Morley* Deparmen of Eonomis, Washingon Universiy, Campus Box 08, Brookings

More information

Stochastic Model for Cancer Cell Growth through Single Forward Mutation

Stochastic Model for Cancer Cell Growth through Single Forward Mutation Journal of Modern Applied Saisical Mehods Volume 16 Issue 1 Aricle 31 5-1-2017 Sochasic Model for Cancer Cell Growh hrough Single Forward Muaion Jayabharahiraj Jayabalan Pondicherry Universiy, jayabharahi8@gmail.com

More information

SOLVING AN OPTIMAL CONTROL PROBLEM WITH MATLAB

SOLVING AN OPTIMAL CONTROL PROBLEM WITH MATLAB SOLVING AN OPIMAL CONROL PROBLEM WIH MALAB RGeeharamani, SSviha Assisan Proessor, Researh Sholar KG College O Ars and Siene Absra: In his paper, we presens a Ponryagin Priniple or Bolza problem he proedre

More information

BUCKLING AND REDUCED STIFFNESS CRITERIA FOR FRP CYLINDRICAL SHELLS UNDER COMPRESSION

BUCKLING AND REDUCED STIFFNESS CRITERIA FOR FRP CYLINDRICAL SHELLS UNDER COMPRESSION Asia-Paifi Conferene on FRP in Sruures (APFIS 7) S.T. Smih (ed) 7 Inernaional Insiue for FRP in Consruion BUCKLIG AD REDUCED STIFFESS CRITERIA FOR FRP CYLIDRICAL SHELLS UDER COMPRESSIO K. Masumoo 1, S.

More information

DEPARTMENT OF STATISTICS

DEPARTMENT OF STATISTICS A Tes for Mulivariae ARCH Effecs R. Sco Hacker and Abdulnasser Haemi-J 004: DEPARTMENT OF STATISTICS S-0 07 LUND SWEDEN A Tes for Mulivariae ARCH Effecs R. Sco Hacker Jönköping Inernaional Business School

More information

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid

More information

3. Differential Equations

3. Differential Equations 3. Differenial Equaions 3.. inear Differenial Equaions of Firs rder A firs order differenial equaion is an equaion of he form d() d ( ) = F ( (),) (3.) As noed above, here will in general be a whole la

More information

STUDY ON A METHOD TO IDENTIFY EXTERNAL FORCES AND DAMPING PARAMETERS OF STRUCTURE FROM RANDOM RESPONSE VALUES

STUDY ON A METHOD TO IDENTIFY EXTERNAL FORCES AND DAMPING PARAMETERS OF STRUCTURE FROM RANDOM RESPONSE VALUES STUDY ON A METHOD TO IDENTIFY ETERNAL FORCES AND DAMPING PARAMETERS OF STRUCTURE FROM RANDOM RESPONSE VALUES 114 M KANDA 1, E MARUTA, D INABA 3 And T MATSUYAMA 4 SUMMARY Proposed in his paper is a mehod

More information

Appendix to Creating Work Breaks From Available Idleness

Appendix to Creating Work Breaks From Available Idleness Appendix o Creaing Work Breaks From Available Idleness Xu Sun and Ward Whi Deparmen of Indusrial Engineering and Operaions Research, Columbia Universiy, New York, NY, 127; {xs2235,ww24}@columbia.edu Sepember

More information

Solutions to Odd Number Exercises in Chapter 6

Solutions to Odd Number Exercises in Chapter 6 1 Soluions o Odd Number Exercises in 6.1 R y eˆ 1.7151 y 6.3 From eˆ ( T K) ˆ R 1 1 SST SST SST (1 R ) 55.36(1.7911) we have, ˆ 6.414 T K ( ) 6.5 y ye ye y e 1 1 Consider he erms e and xe b b x e y e b

More information

Optimal Dynamic Pricing Strategies for High Occupancy/Toll (HOT) Lanes

Optimal Dynamic Pricing Strategies for High Occupancy/Toll (HOT) Lanes Opimal Dynami Priing Sraegies for High Oupany/oll HO Lanes Yingyan Lou, Yafeng Yin and Jorge A. Laval Deparmen of Civil and Coasal Engineering, Universiy of Florida Shool of Civil and Environmenal Engineering,

More information

STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN

STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN Inernaional Journal of Applied Economerics and Quaniaive Sudies. Vol.1-3(004) STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN 001-004 OBARA, Takashi * Absrac The

More information

Topic Astable Circuits. Recall that an astable circuit has two unstable states;

Topic Astable Circuits. Recall that an astable circuit has two unstable states; Topic 2.2. Asable Circuis. Learning Objecives: A he end o his opic you will be able o; Recall ha an asable circui has wo unsable saes; Explain he operaion o a circui based on a Schmi inverer, and esimae

More information

Position, Velocity, and Acceleration

Position, Velocity, and Acceleration rev 06/2017 Posiion, Velociy, and Acceleraion Equipmen Qy Equipmen Par Number 1 Dynamic Track ME-9493 1 Car ME-9454 1 Fan Accessory ME-9491 1 Moion Sensor II CI-6742A 1 Track Barrier Purpose The purpose

More information