HYDRAULIC BEHAVIOUR OF HIGLEIG-PORTSUDAN PIPELINE AT OPERATION AND SHUTDOWN CONDITIONS
|
|
- Stephanie Todd
- 5 years ago
- Views:
Transcription
1 Journa of Engineering Science and echnoogy Vo. 9 No Schoo of Engineering ayor s Universiy HYRAULIC BEHAVIOUR OF HIGLEIG-PORSUAN PIPELINE A OPERAION AN SHUOWN CONIIONS MYSARA EISSA MOHYALINN Coege of Peroeum Engineering and echnoogy Sudan Universiy of Science and echnoogy Easern iem P. O. Box 73 Kharoum Sudan E-mai: mysara100@yahoo.com Absrac Experimena measuremens were carried ou o correae rheoogica properies of Nie bend wih emperaure wihin emperaure ranges a which Nie bend exhibis Newonian non-newonian and soidificaion behaviours. he deveoped correaions were used o describe he hydrauic condiions wihin each kiomere engh of he pipeine during operaion and he pressure difference required for resaring and fushing every kiomere engh of he pipeine afer specified shudown ime. Pressure osses wihin every kiomere engh of he pipeine a differen fow behaviours during he pipeine operaion have been sudied and anaysed. he required resaring pressure of every kiomere engh has aso been sudied aking ino consideraion he possibiiy of crude soidificaion. he pressure head ransverse beween every wo pump saions and he effec of fow rae on he pipeine overa pressure osses during operaing condiions were sudied. hese resus have been obained using numerica sofware deveoped by he auhor. Keywords: Nie bend Hydrauic Operaion Shudown. 1. Inroducion he hydrauic cacuaions of any pipeine ransporing crude oi highy depend on he rheoogica properies of he crude and he herma condiions of he pipeine. hese wo facors are ineraced as saed by Szias [1] any fuid fow hrough a pipeine creaes a paricuar amoun of hea which changes he origina hea condiion of he pipeine. he rae a which his hea is generaed depends on he rheoogica properies of he crude and i increases wih he viscosiy incremen. In fac his change in hea condiion wihin he pipeine resus in changing he viscosiy which in urns affecs he hydrauic condiions of he fuid. 463
2 464 Mysara E. Mohyadinn Nomencaures c Hea capaciy of he fuid J/kg. C Pipe diameer m f Fricion facor G Mass fow rae of he fuid kg/s hg Hydrauic gradien k Fuid consisency non-newonian behaviour K o Overa hea ransfer coefficien W/m. C L Pipeine engh m n Fow index non-newonian behaviour Re Reynods number Re M Reed and Merzner Reynods number for non-newonian fuids Re New Reynods number for Newonian fuids i Ine emperaure C o Surrounding emperaure C V Fuid veociy m/s Greek Symbos P f Pressure difference pressure oss due o fricion Pa P y Resaring pressure Pa µ Viscosiy Pa.s ρ f Fuid densiy kg/m 3 ρ 0 Fuid densiy a 0 C kg/m 3 τ y Yied sress Pa he Sudanese crude Nie bend which is produced from Higeig oi fied and ranspored hrough Higeig-PorSudan pipeine is a high wax conen crude oi wih high pour poin. I conains abou 5% w/w wax and is pour poins for differen heaing reamen emperaures wihou chemica addiives are in he range of 36 C~31.5 C. A a cerain emperaure above is pour poin Nie bend behaves as a high viscous pseudo pasic non-newonian fuid. Unike Newonian fuids whose rheoogica behavior is described by he inear Newon mode conaining a singe rheoogica parameer caed viscosiy and denoed µ pseudo pasic non-newonian fuids are described by he power aw mode which conains wo rheoogica parameers known as fuid consisency denoed as k and fow index denoed n []. ue o he non-ineariy of he reaionship beween he rheoogica properies of non-newonian fuids and emperaure hydrauic cacuaions of pipeines carrying non-newonian waxy crudes are very compex. As Nie bend exhibis non-newonian behavior wihin cerain emperaure range hydrauic cacuaions of Higeig-Porsudan pipeine shoud consider he emperaure dependency of a rheoogica properies wheher he crude exhibis Newonian or non-newonian behaviour. A very ow emperaures beow pour poin Nie bend may soidify and exhibi ge-ike behaviour a such condiions if he pipeine goes for panned or emergency shudown he resarabiiy coud no be achieved uness he avaiabe resaring pressure aows he rupure of he ge ike srucure. he force required o do so is known as yied sress and denoed as τ y. he yied sress is reaed o boh emperaure and shudown ime. Journa of Engineering Science and echnoogy Augus 014 Vo. 94
3 Hydrauic Behaviour of Higeig-Porsudan Pipeine a Operaion and Shudown 465 In his paper experimena measuremens have been carried ou o describe he rheoogica behavior of Nie bend. Rheoogica modes of Nie bend were deveoped a emperaure ranges wihin which Nie bend exhibis Newonian non-newonian and soidified behaviours. hese modes were hen used o simuae pressure ransverse beween pump saions during he pipeine operaion under specified condiions. he modes aso are used o predic resaring pressure afer various shudown imes.. Research Mehodoogy he sudy of hydrauic behavior of Higieg-Porsudan pipeine has been achieved in wo seps: he firs sep: experimena measuremens In his sep sampes of Nie bend were subjec o shear using he viscomeer HAAKE V 150. ifferen heaing reamen emperaures and measuremen emperaures have been conroed using a waer bah. he heaing reamen emperaure is a emperaure o which he crude is heaed before he measuremen in order o rever he sampe o is origina properies o erase hisory effec whereas he measuremen emperaure is he emperaure a which a desired rheoogica propery is measured. In he pipeine arge scae he heaing emperaure simuaes he reamen emperaure of he ranspored crude whereas he measuremen emperaure simuaes he environmen surrounding emperaure he soi emperaure for buried pipeines. he second sep is numerica and compuaiona modeing his sep is achieved by empoying pubished mahemaica modes Appendix A o deveop a compuaiona oo. he modes used are discussed beow..1. Pressure difference Consider a horizona pipeine as iusraed in Fig. 1. he minimum pressure difference ha makes he fuid fow from he ine o he oue of he pipeine mus be greaer han he resisance force resuing from he fricion effec. So o evauae he fow efficiency of a pipeine ha equipped wih a specific energy generaion unis or o idenify he energy consumpion by fow he fricion pressure predicion is an essenia. Fig. 1. irecion of Fow and Fricion in a Pipe Segmen. he fricion pressure can be cacuaed using he foowing equaion [3]: ρlv P f = f 1 d Journa of Engineering Science and echnoogy Augus 014 Vo. 94
4 466 Mysara E. Mohyadinn In case of non-isoherma ransporaion boh ρ and f in Eq. 1 are emperaure-dependen. ifferen modes are used o describe he emperaure dependency of densiy. he mode used in his sudy considers he crude densiy a 0 o C as a reference densiy o obain he densiy a any emperaure [3]: ρ = ρ ρ he fricion facor f for differen fow regimes aminar or urbuen changes wih emperaure mainy due o emperaure effecs on rheoogica parameers wihin which crude behaves as Newonian or non-newonian fuid. A equaions ha used o cacuae he fricion facor f depend on he reaionship f = f Re where Re is he Newonian Reynods number or non-newonian Reed and Mezner Reynods number which can be obained from he foowing equaions: ρ v Re New = 3 µ Re M = 8 n 1 n n v ρ 3n + 1 k 4n ue o he variaion in rheoogica properies aong he pipeine differen poins aong he pipeine have differen Reynods numbers; accordingy assuming a consan fow rae fricion facor is obviousy varied wihin Newonian and non- Newonian ranges of emperaure. Laminar and urbuen regimes have aso been considered and Kemowski equaions were empoyed for fricion facor cacuaion when crude foow urbuen regime due o high fow veociy [4]. 4.. Hydrauic cacuaions of Higieg-Porsudan pipeine during operaion condiion he oa norma-force-curve sope of nose-cyinder-boaai body is deermined by he summaion of he norma-force-curve sopes of he nose wih he effec of cyindrica par and aferbody. Considering he pressure-emperaure dependency Eq. 1 has been appied o obain he pressure difference for each kiomeer engh variaion aong he pipeine. he hydrauic gradien beween wo poins can be cacuaed from he foowing equaion: hg P1 h1 + ρg L L = where P h and L are pressure eevaion and disance difference respecivey beween poin 1 and. abe 1 shows he eevaion of every pump saion aong Higeig-Porsudan pipeine and he disance beween he pipeine ine and every pump saion. 5 Journa of Engineering Science and echnoogy Augus 014 Vo. 94
5 Hydrauic Behaviour of Higeig-Porsudan Pipeine a Operaion and Shudown 467 abe 1. Sudan Pipeine Pumps Saions Locaions and Eevaions. Saion No. isance km Eevaion m PS# 1 in Higig PS# PS# PS# PS# PS# ermina in por Sudan Hydrauic cacuaions of Higieg-Porsudan pipeine during shudown condiion Resaring pressure is cacuaed considering a fow behaviours Newonian non-newonian and soidificaion of he crude. he resaring pressure for he soidificaion-absen condiion is simpy prediced using Eq. 1 considering he emperaure disribuion a any ime afer shudown and negecing he ransien pressure resuing from he acousic wave propagaion. If he pipeine is shudown for ong period of ime he emperaure of crude may drop o beow he crude soidificaion emperaure. In his case addiiona pressure is required o exceed he yied sress before crude fows smoohy. For soidified pipeines he resaring pressure which is equivaen o he yied pressure pus he fricion pressure srongy increases wih shudown ime due o he emperaure drop. he yied pressure is reaed o he yied sress by he foowing equaion: 4τ y Py = 6 3. Resus and iscussion 3.1. Experimena resus he soidificaion poin of he crude was found o be 9 C when he crude was preheaed o 60 C. he soidificaion emperaure is considered as an approximaed vaue used o disinguish beween he Newonian and non- Newonian ranges of emperaure. If he emperaure is 1 C above he soidificaion poin he crude is assumed o be Newonian. he heaing emperaure is a simuaed vaue of he pipeine ine emperaure. Using his vaue he experimens resu in he foowing rheoogica equaions µ = k = 6 10 e 8 n = Journa of Engineering Science and echnoogy Augus 014 Vo. 94
6 468 Mysara E. Mohyadinn Equaions 7 8 and 9 describe he emperaure dependency of viscosiy for Newonian fow fuid consisency and fow index for non-newonian fuid. hese equaions are uiized o describe he hydrauic condiions aong he pipeine Beow he soidificaion emperaure he crude yied sress is found o be reaed o emperaure as foows: τ y = Equaion 10 is used o predic resaring pressure of he pipeine afer various shudown imes by inroducing he yied sress o Eq. 6. Wiiams [5] have obained a inear reaionship beween he waxy crude yied sress and he ime. heir reaionship was emphasized by Fig. which is obained from experimena measuremens carried ou by he auhor. he ony difference beween he wo resus is ha shorer sanding imes have been chosen in he presen measuremens. Fig.. he Reaionship beween Yied Srengh and Sanding ime. 3.. Numerica resus Operaion condiions Figures 3a and b show exampes of emperaure disribuion aong he pipeine. his disribuion is a fow rae of 0.33 m 3 /s equivaen o bb/day ine emperaure 60 C and soi emperaure 3 C and 43 C respecivey. Experimena resus indicae ha he abnorma emperaure he emperaure beow which he crude fow changes from Newonian fow o non-newonian fow of Nie bend is 40 C. Figure 3a shows ha he abnorma emperaure is reached a he disance 600 km whie Fig. 3b shows ha he emperaure is higher han he abnorma emperaure hroughou he pipeine engh because soi emperaure is higher he abnorma emperaure. Journa of Engineering Science and echnoogy Augus 014 Vo. 94
7 Hydrauic Behaviour of Higeig-Porsudan Pipeine a Operaion and Shudown 469 emperaure emperaure C isance km a Soi emperaure 3 C. b Soi emperaure 43 C. Fig. 3. emperaure isribuions aong Higeig-Porsudan Pipeine Ine emperaure 60 C and Fow Rae 0.33 m 3 /s. he pressure emperaure dependence is iusraed in Figs. 4a and b in which he disribuion of every kiomeer pressure difference pressure oss is obained. he boundary beween Newonian and non-newonian behavior is iusraed in Fig. 4a whie Fig. 4b indicaes ha he crude behaves as Newonian fuid hroughou he pipeine engh. Figure 4a shows a sudden increase of pressure oss afer more han 500 km. his sudden increase of pressure oss is due o emperaure decinaion a his poin o he abnorma emperaure as indicaed Fig. 3. In oher words from he pipeine ine o he sudden eevaion poin he crude behaves as Newonian whereas afer he sudden eevaion poin i behaves as non-newonian isance km Pressure oss kpa/km isance km a Soi emperaure 3 C. Pressure oss/km kpa/km isance km b Soi emperaure 43 C. Fig km Pressure Losses isribuion aong Higeig-Porsudan Pipeine Ine emperaure 60 C and Fow Rae 0.33 m 3 /s. Pressure ransverse beween every wo pump saions is normay iusraed by a sraigh ine wih sope equas o he hydrauic gradiens beween hese saions. he pressure difference is he fricion pressure of he pipeine segmen ha joins hese wo saions. Figures 5 and 6 iusrae he pressure head ransverse beween every wo pump saions using he same inpu daa ha resu in Figs. 3 and 4 respecivey. In Fig. 5 non-newonian fow appeared afer 350 km Newonian fow as iusraed in Fig. 3 whereas here is no non-newonian fow in Fig. 6. he Journa of Engineering Science and echnoogy Augus 014 Vo. 94
8 470 Mysara E. Mohyadinn eevaion of every pump saion has been indicaed by wriing he saion number a is specified ocaion on he pipeine profie. Fig. 5. Pressure ransverse beween Pump Saions of Higeig-Porsudan Pipeine Ine emperaure 60 C Soi emperaure 3 C Fow Rae 0.33 m 3 /s. Fig. 6. Pressure ransverse beween Pump Saions of Higeig-Porsudan Pipeine Ine emperaure 60 C Soi emperaure 4 C Fow Rae 0.33 m 3 /s. Effec of fow rae on overa pressure difference pressure oss he effecs of fow rae on he overa pressure difference for Nie bend fow were obained for differen soi emperaures as shown in abe. he abe shows ha for mass fow raes of more han 300 kg/s pressure osses highy increase so very high fow raes are no recommended. If increasing fow rae is a mus measures shoud be aken o decrease pressure osses. his can be achieved by heaing he crude or injecing fow modifiers o decrease viscosiy and hence decrease pressure osses. Journa of Engineering Science and echnoogy Augus 014 Vo. 94
9 Hydrauic Behaviour of Higeig-Porsudan Pipeine a Operaion and Shudown 471 abe. he Overa Pressure ifference Variaion wih Mass Fow Rae a ifferen Soi emperaures. Soi emperaure o C Mass Fow Rae kg/s he pipeine overa pressure drop kpa Shudown condiions Figures 7 o 1 show he emperaure and resaring pressure difference disribuion aong he pipeine every 1 hrs afer shudown. Newonian non- Newonian and soidified enghs of he pipeine have been indicaed by differen coored ines. A soi emperaure of 4 C which is greay higher he soidificaion poin he crude is exhibis Newonian fow no maer how ong he fow is sopped and hence i is easy o resar he pipeine. A soi emperaure 3 C he crude iniiay exhibis Newonian fow a earier shudown imes wihin near disances from he pipeine ine. For onger shudown imes he disance wihin which he crude exhibis Newonian fow becomes shorer uni reach he ime when he crude exhibis non-newonian for a he engh of he pipeine and hence resaring pressure increases. A soi emperaure 7 C which is ower han he soidificaion emperaure he crude wi exhibi non-newonian fow few hours afer he shudown and hen soidify. In his case very high resaring pressure is required which may exceed he pump saions capabiiy. Fig. 7. ransien emperaure isribuion aong he Pipeine every 1 Hours afer Shudown. Ine emperaure 60 C Soi emperaure 4 C Fow Rae 0.33 m 3 /s. Journa of Engineering Science and echnoogy Augus 014 Vo. 94
10 47 Mysara E. Mohyadinn Fig. 8. ransien emperaure isribuion aong he Pipeine every 1 Hours afer Shudown. Ine emperaure 60 C Soi emperaure 3 C Fow Rae 0.33 m 3 /s. Fig. 9. ransien emperaure isribuion aong he Pipeine every 1 Hours afer Shudown. Ine emperaure 60 C Soi emperaure 7 C Fow Rae 0.33 m 3 /s. Fig km ransien Resaring Pressure isribuion aong he Pipeine every 1 Hours afer Shudown. Ine emperaure 60 C Soi emperaure 4 C Fow Rae 0.33 m 3 /s. Journa of Engineering Science and echnoogy Augus 014 Vo. 94
11 Hydrauic Behaviour of Higeig-Porsudan Pipeine a Operaion and Shudown 473 Fig km ransien Resaring Pressure isribuion aong he Pipeine every 1 Hours afer Shudown. Ine emperaure 60 C Soi emperaure 3 C Fow Rae 0.33 m 3 /s. Fig km ransien Resaring Pressure isribuion aong he Pipeine every 1 Hours afer Shudown. Ine emperaure 60 C Soi emperaure 7 C Fow Rae 0.33 m 3 /s. 4. Concusions Combining he experimena work wih he deveoped compuaiona oo he foowing remarks can be concuded: Nie bend exhibis differen rheoogica behaviours a differen ranges of emperaure. I is recommended o operae he pipeine a high emperaures a which crude is expeced o exhibi Newonian fow o reduce fricion osses and hence save pumping energy. Journa of Engineering Science and echnoogy Augus 014 Vo. 94
12 474 Mysara E. Mohyadinn he rheoogica properies of Nie bend are markedy emperaure-dependan. his fac shoud be considered for predicion of hydrauic behavior of Higeig- Porsudan pipeine during operaion and shudown condiions. he soidificaion emperaure of Nie bend was found o be 9 C. A emperaures beow his vaue he crude is expeced o form a ge-ike srucure ha hinders resaring of he pipeine. epending on fow and herma characerisics Nie bend may exhibis differen behaviours wihin differen segmens. he far disance from he ine he more possibiiy o exhibi non-newonian fow and hence he more pumping pressure is required o fush a uni engh. A he wors condiion he crude may be geed a emperaures ower han is soidified poin. I is imporan o resar he pipeine as quicky as possibe when i goes for panned or emergency shudown o avoid pressure decrease beow he soidified poin. References 1. Szias A.P Producion and ranspor of oi and gas. nd Ed. Par B. Esevier Science Pubisher.. Wasp E.J.; Kenny J.P.; and Ghandi R.L Soid-iquid fow surry pipeine ransporaion. rans ech Pubn. 3. Xiaoheng Y.; and Gouzhong Z Oi pipeine design and conro. universiy of peroeum China press Bansa R.K A exbook of fuid mechanics and hydrauic machines. Laxmi Pubicaions P Ld New ehi. 5. Wiiams.M.; Hsu J.J.C.; and Paerson H.L Sysem deveoped o predic waxy crude s breakaway yied sress. Oi and Gas Journa 94 51; Appendix A Mahemaica modes in operaion condiion emperaure a engh L from he ine can be obained from Eq. A-1 k + π i 0exp A Gc = o he cacuaed emperaure is hen used o cacuae he densiy and viscosiy a he engh. he densiy is cacuaed from Eq. A- beow whereas he viscosiy is cacuaed from he formuaed viscosiy-emperaure equaion. ρ = ρ ρ 0 A- 0 0 he fow behavior is idenified wheher i is Newonian or non-newonian by comparing he emperaure wih he pour poin. Consequeny he fricion facor is cacuaed from he foowing equaions for aminar or urbuence regimes. Journa of Engineering Science and echnoogy Augus 014 Vo. 94
13 Hydrauic Behaviour of Higeig-Porsudan Pipeine a Operaion and Shudown 475 Newonian fow fricion facor cacuaion ρ 1v Re New = A-3 µ - Laminar regime 64 f = A-4 Re New - urbuen regime < Re New Re New f = A Re New Re New Non-Newonian fow fricion facor cacuaion Re M = 8 n n n 1 - Laminar regime v ρ A-6 3n + 1 k 4n f 16 = Re A-7 MR Criica Reed and Mezner Reynods number: 6464n Re = A-8 MRC n + n - urbuen regime + n 1+ n m = 0.314n n φ = exp n E = exp3.57n φ f = E Re.3 m MR / ReMR 4. A-9 Fricion facor is reaed o he coefficien facor of fow by his equaion: f i = 4 f A-10 Journa of Engineering Science and echnoogy Augus 014 Vo. 94
14 476 Mysara E. Mohyadinn Journa of Engineering Science and echnoogy Augus 014 Vo. 94 Fricion pressure 1 LV f P i f = ρ A-11 Mahemaica modes in shudown condiions he foowing equaions are used for shudown cacuaions. In addiion o he disance a parameers are funcions in ime. emperaure disribuion + = b Gc k o ine π exp A-1 where s s o o c c k b ρ ρ = Resaring Pressure: - Newonian crude Resaring Re v New µ ρ = A-13 Re 64 f i = A-14 - Non-Newonian crude resaring Re 1 k n n v n n n MR + = ρ A-15 Re 64 f i = A-16 - Geed crude Resaring p y y 4000 τ = A-17
Sub Module 2.6. Measurement of transient temperature
Mechanical Measuremens Prof. S.P.Venkaeshan Sub Module 2.6 Measuremen of ransien emperaure Many processes of engineering relevance involve variaions wih respec o ime. The sysem properies like emperaure,
More informationResearch Article Developing a Series Solution Method of q-difference Equations
Appied Mahemaics Voume 2013, Arice ID 743973, 4 pages hp://dx.doi.org/10.1155/2013/743973 Research Arice Deveoping a Series Souion Mehod of q-difference Equaions Hsuan-Ku Liu Deparmen of Mahemaics and
More informationNavneet 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 informationTHE EFFECT OF SUCTION AND INJECTION ON UNSTEADY COUETTE FLOW WITH VARIABLE PROPERTIES
Kragujevac J. Sci. 3 () 7-4. UDC 53.5:536. 4 THE EFFECT OF SUCTION AND INJECTION ON UNSTEADY COUETTE FLOW WITH VARIABLE PROPERTIES Hazem A. Aia Dep. of Mahemaics, College of Science,King Saud Universiy
More informationRC, RL and RLC circuits
Name Dae Time o Complee h m Parner Course/ Secion / Grade RC, RL and RLC circuis Inroducion In his experimen we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors.
More informationBasic Circuit Elements Professor J R Lucas November 2001
Basic Circui Elemens - J ucas An elecrical circui is an inerconnecion of circui elemens. These circui elemens can be caegorised ino wo ypes, namely acive and passive elemens. Some Definiions/explanaions
More information( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is
UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires
More information04. 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 informationUnsteady flow in a porous medium between parallel plates in the presence of uniform suction and injection with heat transfer
Waer- Hydroogy Unseady fow in a porous medium beween parae paes in he presence of uniform sucion and injecion wih hea ransfer Absrac H. A. Aia, W. A. E-Meged, W. Abbas, M. A. M. Abdeen 3, * Received: January,
More informationChapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws
Chaper 5: Phenomena Phenomena: The reacion (aq) + B(aq) C(aq) was sudied a wo differen emperaures (98 K and 35 K). For each emperaure he reacion was sared by puing differen concenraions of he 3 species
More informationLab 10: RC, RL, and RLC Circuits
Lab 10: RC, RL, and RLC Circuis In his experimen, we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors. We will sudy he way volages and currens change in
More informationRandom Walk with Anti-Correlated Steps
Random Walk wih Ani-Correlaed Seps John Noga Dirk Wagner 2 Absrac We conjecure he expeced value of random walks wih ani-correlaed seps o be exacly. We suppor his conjecure wih 2 plausibiliy argumens and
More informationVehicle Arrival Models : Headway
Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where
More informationPhysics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle
Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,
More informationABOUT THE DESIGN OF PRESTRESSED FRAMES WITH THE INFINITELY RIGID BEAM, SUBJECTED TO HORIZONTAL FORCES
NTERNTONL SCENTFC CONFERENCE CBv 00 November 00, Braşov BOUT THE DESGN OF PRESTRESSED FRES WTH THE NFNTELY RGD BE, SUBJECTED TO HORZONTL FORCES Dan PRECUPNU*, Codrin PRECUPNU** *Prof., Universiy G. saci
More informationStochastic 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 informationA First Course on Kinetics and Reaction Engineering. Class 19 on Unit 18
A Firs ourse on Kineics and Reacion Engineering lass 19 on Uni 18 Par I - hemical Reacions Par II - hemical Reacion Kineics Where We re Going Par III - hemical Reacion Engineering A. Ideal Reacors B. Perfecly
More informationCombined 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 informationLesson 03 Transient Response of Transmission Lines
Eecromagneics P- esson Transien esponse of Transmission ines Inroucion Paria refecion an ransmission occur wheneer a wae mees wih a isconinuiy ie an inerface beween feren maerias Muipe isconinuiies cause
More informationQ.1 Define work and its unit?
CHP # 6 ORK AND ENERGY Q.1 Define work and is uni? A. ORK I can be define as when we applied a force on a body and he body covers a disance in he direcion of force, hen we say ha work is done. I is a scalar
More informationA Two Stage Mixture Model for Predicting EAD
A wo Sage Mixure Mode for Predicing EAD Credi Scoring & Credi Conro, Edinburgh 2013 Mindy Leow & Jonahan Crook Credi Research Cenre, Universiy of Edinburgh, UK 1 Moivaion Reguaory Capia ase II requires
More informationSome Basic Information about M-S-D Systems
Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,
More informationMIT Amorphous Materials
MIT 3.071 Amorphous Maerials 7: Viscoelasiciy and Relaxaion Juejun (JJ) Hu 1 Afer-class reading lis Fundamenals of Inorganic Glasses Ch. 8, Ch. 13, Appendix A Inroducion o Glass Science and Technology
More information2 Weighted Residual Methods
2 Weighed Residua Mehods Fundamena equaions Consider he probem governed by he differenia equaion: Γu = f in. (83) The above differenia equaion is soved by using he boundary condiions given as foows: u
More informationMathcad Lecture #8 In-class Worksheet Curve Fitting and Interpolation
Mahcad Lecure #8 In-class Workshee Curve Fiing and Inerpolaion A he end of his lecure, you will be able o: explain he difference beween curve fiing and inerpolaion decide wheher curve fiing or inerpolaion
More informationArea A 0 level is h 0, assuming the pipe flow to be laminar. D, L and assuming the pipe flow to be highly turbulent.
Pipe Flows (ecures 5 o 7). Choose he crec answer (i) While deriving an expression f loss of head due o a sudden expansion in a pipe, in addiion o he coninuiy and impulse-momenum equaions, one of he following
More informationLecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.
Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in
More informationPHYS 1401 General Physics I Test 3 Review Questions
PHYS 1401 General Physics I Tes 3 Review Quesions Ch. 7 1. A 6500 kg railroad car moving a 4.0 m/s couples wih a second 7500 kg car iniially a res. a) Skech before and afer picures of he siuaion. b) Wha
More informationResearch Article Asymptotic Method of Solution for a Problem of Construction of Optimal Gas-Lift Process Modes
Hindawi Pubishing Corporaion Mahemaica Probems in Engineering Voume 21, Arice ID 19153, 1 pages doi:1.1155/21/19153 Research Arice Asympoic Mehod of Souion for a Probem of Consrucion of Opima Gas-Lif Process
More informationNumerical Simulation of the Overall Flow Field for Underwater Vehicle with Pump Jet Thruster
Available online a www.sciencedirec.com Procedia Engineering 31 (2012) 769 774 Inernaional Conference on Advances in Compuaional Modeling and Simulaion Numerical Simulaion of he Overall Flow Field for
More informationInventory Control of Perishable Items in a Two-Echelon Supply Chain
Journal of Indusrial Engineering, Universiy of ehran, Special Issue,, PP. 69-77 69 Invenory Conrol of Perishable Iems in a wo-echelon Supply Chain Fariborz Jolai *, Elmira Gheisariha and Farnaz Nojavan
More informationFlow-Induced Vibration Analysis of Supported Pipes with a Crack
Flow-Induced Vibraion Analsis of Suppored Pipes wih a Crack Jin-Huk Lee, Samer Masoud Al-Said Deparmen of Mechanical Engineering American Universi of Sharjah, UAE Ouline Inroducion and Moivaion Aeroacousicall
More informationDevelopment of a new metrological model for measuring of the water surface evaporation Tovmach L. Tovmach Yr. Abstract Introduction
Developmen of a new merological model for measuring of he waer surface evaporaion Tovmach L. Tovmach Yr. Sae Hydrological Insiue 23 Second Line, 199053 S. Peersburg, Russian Federaion Telephone (812) 323
More informationElectrical 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 informationCHAPTER 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 informationExponential Weighted Moving Average (EWMA) Chart Under The Assumption of Moderateness And Its 3 Control Limits
DOI: 0.545/mjis.07.5009 Exponenial Weighed Moving Average (EWMA) Char Under The Assumpion of Moderaeness And Is 3 Conrol Limis KALPESH S TAILOR Assisan Professor, Deparmen of Saisics, M. K. Bhavnagar Universiy,
More informationSolutions to Assignment 1
MA 2326 Differenial Equaions Insrucor: Peronela Radu Friday, February 8, 203 Soluions o Assignmen. Find he general soluions of he following ODEs: (a) 2 x = an x Soluion: I is a separable equaion as we
More informationSecond Law. first draft 9/23/04, second Sept Oct 2005 minor changes 2006, used spell check, expanded example
Second Law firs draf 9/3/4, second Sep Oc 5 minor changes 6, used spell check, expanded example Kelvin-Planck: I is impossible o consruc a device ha will operae in a cycle and produce no effec oher han
More informationModule 2 F c i k c s la l w a s o s f dif di fusi s o i n
Module Fick s laws of diffusion Fick s laws of diffusion and hin film soluion Adolf Fick (1855) proposed: d J α d d d J (mole/m s) flu (m /s) diffusion coefficien and (mole/m 3 ) concenraion of ions, aoms
More informationLinear Response Theory: The connection between QFT and experiments
Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and
More informationNature Neuroscience: doi: /nn Supplementary Figure 1. Spike-count autocorrelations in time.
Supplemenary Figure 1 Spike-coun auocorrelaions in ime. Normalized auocorrelaion marices are shown for each area in a daase. The marix shows he mean correlaion of he spike coun in each ime bin wih he spike
More information1. VELOCITY AND ACCELERATION
1. VELOCITY AND ACCELERATION 1.1 Kinemaics Equaions s = u + 1 a and s = v 1 a s = 1 (u + v) v = u + as 1. Displacemen-Time Graph Gradien = speed 1.3 Velociy-Time Graph Gradien = acceleraion Area under
More informationMath 333 Problem Set #2 Solution 14 February 2003
Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial
More informationScientific Herald of the Voronezh State University of Architecture and Civil Engineering. Construction and Architecture
Scienific Herald of he Voronezh Sae Universiy of Archiecure and Civil Engineering. Consrucion and Archiecure UDC 625.863.6:551.328 Voronezh Sae Universiy of Archiecure and Civil Engineering Ph. D. applican
More informationEvaluation of Mean Time to System Failure of a Repairable 3-out-of-4 System with Online Preventive Maintenance
American Journal of Applied Mahemaics and Saisics, 0, Vol., No., 9- Available online a hp://pubs.sciepub.com/ajams/// Science and Educaion Publishing DOI:0.69/ajams--- Evaluaion of Mean Time o Sysem Failure
More informationPET467E-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 informationAt the end of this lesson, the students should be able to understand
Insrucional Objecives A he end of his lesson, he sudens should be able o undersand Sress concenraion and he facors responsible. Deerminaion of sress concenraion facor; experimenal and heoreical mehods.
More informationThe Contradiction within Equations of Motion with Constant Acceleration
The Conradicion wihin Equaions of Moion wih Consan Acceleraion Louai Hassan Elzein Basheir (Daed: July 7, 0 This paper is prepared o demonsrae he violaion of rules of mahemaics in he algebraic derivaion
More informationSTATISTICAL MODELLING PRACTICAL VI SOLUTIONS
VI-1. TATITICAL MODELLING PRACTICAL VI OLUTION VI.1 The following daa are from a Lain square experimen designed o invesigae he moisure conen of urnip greens. The experimen involved he measuremen of he
More informationInventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions
Muli-Period Sochasic Models: Opimali of (s, S) Polic for -Convex Objecive Funcions Consider a seing similar o he N-sage newsvendor problem excep ha now here is a fixed re-ordering cos (> 0) for each (re-)order.
More information3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon
3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of
More informationChapter 13 Homework Answers
Chaper 3 Homework Answers 3.. The answer is c, doubling he [C] o while keeping he [A] o and [B] o consan. 3.2. a. Since he graph is no linear, here is no way o deermine he reacion order by inspecion. A
More informationnot to be republished NCERT MATHEMATICAL MODELLING Appendix 2 A.2.1 Introduction A.2.2 Why Mathematical Modelling?
256 MATHEMATICS A.2.1 Inroducion In class XI, we have learn abou mahemaical modelling as an aemp o sudy some par (or form) of some real-life problems in mahemaical erms, i.e., he conversion of a physical
More informationAPPM 2360 Homework Solutions, Due June 10
2.2.2: Find general soluions for he equaion APPM 2360 Homework Soluions, Due June 10 Soluion: Finding he inegraing facor, dy + 2y = 3e µ) = e 2) = e 2 Muliplying he differenial equaion by he inegraing
More informationLecture 24. Calderon-Zygmund Decomposition Technique: Cube decomposition
Lecure 24 May 3 h, 2004 Our moivaion for his as ecure in he course is o show a resu using our reguariy heory which is oherwise unprovabe using cassica echniques. This is he previous Theorem, and in paricuar
More informationErrata (1 st Edition)
P Sandborn, os Analysis of Elecronic Sysems, s Ediion, orld Scienific, Singapore, 03 Erraa ( s Ediion) S K 05D Page 8 Equaion (7) should be, E 05D E Nu e S K he L appearing in he equaion in he book does
More informationIB Physics Kinematics Worksheet
IB Physics Kinemaics Workshee Wrie full soluions and noes for muliple choice answers. Do no use a calculaor for muliple choice answers. 1. Which of he following is a correc definiion of average acceleraion?
More informationPhys1112: DC and RC circuits
Name: Group Members: Dae: TA s Name: Phys1112: DC and RC circuis Objecives: 1. To undersand curren and volage characerisics of a DC RC discharging circui. 2. To undersand he effec of he RC ime consan.
More informationwritten by Soma Vesztergom
8 h Block Invesigaions Concerning he Viscosiy of Gases and he Mean Free Pah of he Molecules English-speaking physical chemisry laboraory classes Auumn 009/010 wrien by Soma Veszergom 1.) Inroducion The
More informationThermal Modeling of a Honeycomb Reformer including Radiative Heat Transfer
Thermal Modeling of a Honeycomb Reformer including Radiaive Hea Transfer J Schöne *1, A Körnig 1, W Becer 1 and A Michaelis 1 1 Fraunhofer IKTS, Winerbergsraße 8, 0177 Dresden *Corresponding auhor: jaobschoene@isfraunhoferde
More informationDiebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles
Diebold, Chaper 7 Francis X. Diebold, Elemens of Forecasing, 4h Ediion (Mason, Ohio: Cengage Learning, 006). Chaper 7. Characerizing Cycles Afer compleing his reading you should be able o: Define covariance
More informationThe electromagnetic interference in case of onboard navy ships computers - a new approach
The elecromagneic inerference in case of onboard navy ships compuers - a new approach Prof. dr. ing. Alexandru SOTIR Naval Academy Mircea cel Bărân, Fulgerului Sree, Consanţa, soiralexandru@yahoo.com Absrac.
More informationAP Chemistry--Chapter 12: Chemical Kinetics
AP Chemisry--Chaper 12: Chemical Kineics I. Reacion Raes A. The area of chemisry ha deals wih reacion raes, or how fas a reacion occurs, is called chemical kineics. B. The rae of reacion depends on he
More informationWEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x
WEEK-3 Reciaion PHYS 131 Ch. 3: FOC 1, 3, 4, 6, 14. Problems 9, 37, 41 & 71 and Ch. 4: FOC 1, 3, 5, 8. Problems 3, 5 & 16. Feb 8, 018 Ch. 3: FOC 1, 3, 4, 6, 14. 1. (a) The horizonal componen of he projecile
More informationTraveling Waves. Chapter Introduction
Chaper 4 Traveling Waves 4.1 Inroducion To dae, we have considered oscillaions, i.e., periodic, ofen harmonic, variaions of a physical characerisic of a sysem. The sysem a one ime is indisinguishable from
More informationSymmetry and Numerical Solutions for Systems of Non-linear Reaction Diffusion Equations
Symmery and Numerical Soluions for Sysems of Non-linear Reacion Diffusion Equaions Sanjeev Kumar* and Ravendra Singh Deparmen of Mahemaics, (Dr. B. R. Ambedkar niversiy, Agra), I. B. S. Khandari, Agra-8
More information20. Applications of the Genetic-Drift Model
0. Applicaions of he Geneic-Drif Model 1) Deermining he probabiliy of forming any paricular combinaion of genoypes in he nex generaion: Example: If he parenal allele frequencies are p 0 = 0.35 and q 0
More informationChapter 7 Response of First-order RL and RC Circuits
Chaper 7 Response of Firs-order RL and RC Circuis 7.- The Naural Response of RL and RC Circuis 7.3 The Sep Response of RL and RC Circuis 7.4 A General Soluion for Sep and Naural Responses 7.5 Sequenial
More informationCHAPTER 2 Signals And Spectra
CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par
More information1 Differential Equation Investigations using Customizable
Differenial Equaion Invesigaions using Cusomizable Mahles Rober Decker The Universiy of Harford Absrac. The auhor has developed some plaform independen, freely available, ineracive programs (mahles) for
More informationSolving the Inverse Problems of Wave Equation by a Boundary Functional Method
Journa of Shipping and Ocean Engineering 6 (7) 33-49 doi.765/59-5879/7.6. D DAVID PUBLISHING Soving he Inverse Probems of Wave Equaion by a Boundary Funciona Mehod Chein-Shan Liu and Yung-Wei Chen 3. Cener
More informationMatlab 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 informationLecture 4: Exponential Smoothing for Trended and Seasonal Time Series
NATCOR: Forecasing & Predicive Anayics Lecure 4: Exponenia Smoohing for Trended and Seasona Time Series John Boyan Lancaser Cenre for Forecasing Deparmen of Managemen Science Srucure of his Lecure Par
More informationClass Meeting # 10: Introduction to the Wave Equation
MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion
More informationChapter 12: Velocity, acceleration, and forces
To Feel a Force Chaper Spring, Chaper : A. Saes of moion For moion on or near he surface of he earh, i is naural o measure moion wih respec o objecs fixed o he earh. The 4 hr. roaion of he earh has a measurable
More informationMaintenance Models. Prof. Robert C. Leachman IEOR 130, Methods of Manufacturing Improvement Spring, 2011
Mainenance Models Prof Rober C Leachman IEOR 3, Mehods of Manufacuring Improvemen Spring, Inroducion The mainenance of complex equipmen ofen accouns for a large porion of he coss associaed wih ha equipmen
More informationHeat Transfer. Revision Examples
Hea Transfer Revision Examples Hea ransfer: energy ranspor because of a emperaure difference. Thermal energy is ransferred from one region o anoher. Hea ranspor is he same phenomena lie mass ransfer, momenum
More informationThe Simple Linear Regression Model: Reporting the Results and Choosing the Functional Form
Chaper 6 The Simple Linear Regression Model: Reporing he Resuls and Choosing he Funcional Form To complee he analysis of he simple linear regression model, in his chaper we will consider how o measure
More informationAnalyze patterns and relationships. 3. Generate two numerical patterns using AC
envision ah 2.0 5h Grade ah Curriculum Quarer 1 Quarer 2 Quarer 3 Quarer 4 andards: =ajor =upporing =Addiional Firs 30 Day 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 andards: Operaions and Algebraic Thinking
More informationSummary 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 informationCOS 2AB Physics Year 11 Programme 2012
COS AB Physics Year 11 Programme 01 Semeser Week 1 & 30 Jan 6 Feb Monday is School Dev Day Week 3 13 Feb Week 4 0 Feb a & b Disribue Programme, Assessmen srucure, Syllabus, Course ouline Heaing and cooling
More informationθ with respect to time is
From MEC '05 Inergraing Prosheics and Medicine, Proceedings of he 005 MyoElecric Conrols/Powered Prosheics Symposium, held in Fredericon, New Brunswick, Canada, Augus 17-19, 005. A MINIMAL JERK PROSTHESIS
More informationExcel-Based Solution Method For The Optimal Policy Of The Hadley And Whittin s Exact Model With Arma Demand
Excel-Based Soluion Mehod For The Opimal Policy Of The Hadley And Whiin s Exac Model Wih Arma Demand Kal Nami School of Business and Economics Winson Salem Sae Universiy Winson Salem, NC 27110 Phone: (336)750-2338
More informationV AK (t) I T (t) I TRM. V AK( full area) (t) t t 1 Axial turn-on. Switching losses for Phase Control and Bi- Directionally Controlled Thyristors
Applicaion Noe Swiching losses for Phase Conrol and Bi- Direcionally Conrolled Thyrisors V AK () I T () Causing W on I TRM V AK( full area) () 1 Axial urn-on Plasma spread 2 Swiching losses for Phase Conrol
More informationAdvanced Organic Chemistry
Lalic, G. Chem 53A Chemisry 53A Advanced Organic Chemisry Lecure noes 1 Kineics: A racical Approach Simple Kineics Scenarios Fiing Experimenal Daa Using Kineics o Deermine he Mechanism Doughery, D. A.,
More informationMathcad Lecture #7 In-class Worksheet "Smart" Solve Block Techniques Handout
Mahcad Lecure #7 In-class Workshee "Smar" Solve Block echniques Handou A he end of his lecure, you will be able o: use funcions in solve block equaions o improve convergence consruc solve blocks wih minimal
More informationPolymer 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 informationIntroduction to Probability and Statistics Slides 4 Chapter 4
Inroducion o Probabiliy and Saisics Slides 4 Chaper 4 Ammar M. Sarhan, asarhan@mahsa.dal.ca Deparmen of Mahemaics and Saisics, Dalhousie Universiy Fall Semeser 8 Dr. Ammar Sarhan Chaper 4 Coninuous Random
More informationFinal Exam Advanced Macroeconomics I
Advanced Macroeconomics I WS 00/ Final Exam Advanced Macroeconomics I February 8, 0 Quesion (5%) An economy produces oupu according o α α Y = K (AL) of which a fracion s is invesed. echnology A is exogenous
More informationSTATE-SPACE MODELLING. A mass balance across the tank gives:
B. Lennox and N.F. Thornhill, 9, Sae Space Modelling, IChemE Process Managemen and Conrol Subjec Group Newsleer STE-SPACE MODELLING Inroducion: Over he pas decade or so here has been an ever increasing
More informationSOLUTIONS TO ECE 3084
SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no
More information2) Of the following questions, which ones are thermodynamic, rather than kinetic concepts?
AP Chemisry Tes (Chaper 12) Muliple Choice (40%) 1) Which of he following is a kineic quaniy? A) Enhalpy B) Inernal Energy C) Gibb s free energy D) Enropy E) Rae of reacion 2) Of he following quesions,
More informationMechanical 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 informationLAPLACE TRANSFORM AND TRANSFER FUNCTION
CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions
More information2017 3rd International Conference on E-commerce and Contemporary Economic Development (ECED 2017) ISBN:
7 3rd Inernaional Conference on E-commerce and Conemporary Economic Developmen (ECED 7) ISBN: 978--6595-446- Fuures Arbirage of Differen Varieies and based on he Coinegraion Which is under he Framework
More informationChapter 5: Control Volume Approach and Continuity Principle Dr Ali Jawarneh
Chaper 5: Conrol Volume Approach and Coninuiy Principle By Dr Ali Jawarneh Deparmen of Mechanical Engineering Hashemie Universiy 1 Ouline Rae of Flow Conrol volume approach. Conservaion of mass he coninuiy
More informationActivity 4 Solutions: Transfer of Thermal Energy
Aciviy 4 Soluions: Transfer of Thermal nergy 4.1 How Does Temperaure Differ from Thermal nergy? a) Temperaure Your insrucor will demonsrae molecular moion a differen emperaures. 1) Wha happens o molecular
More informationApproach to Ergodicity in Monte Carlo Simulations
Universiy of Rhode Isand DigiaCommons@URI Chemisry Facuy Pubicaions Chemisry 2 Approach o Ergodiciy in Mone Caro Simuaions J. P. Neiroi Universiy of Rhode Isand David L. Freeman Universiy of Rhode Isand,
More informationChapter 14 Homework Answers
4. Suden responses will vary. (a) combusion of gasoline (b) cooking an egg in boiling waer (c) curing of cemen Chaper 4 Homework Answers 4. A collision beween only wo molecules is much more probable han
More informationSPH3U: Projectiles. Recorder: Manager: Speaker:
SPH3U: Projeciles Now i s ime o use our new skills o analyze he moion of a golf ball ha was ossed hrough he air. Le s find ou wha is special abou he moion of a projecile. Recorder: Manager: Speaker: 0
More information