Chapter 8 Sections 8.4 through 8.6 Internal Flow: Heat Transfer Correlations. In fully-developed region. Neglect axial conduction
|
|
- Alaina Carr
- 5 years ago
- Views:
Transcription
1 Chapter 8 Sectin 8.4 thrugh 8.6 Internal Flw: Heat Tranfer Crrelatin T v cu p cp ( rt) k r T T k x r r r r r x In fully-develped regin Neglect axial cnductin u ( rt) r x r r r r r x T v T T T T T u r x r r r x T T u r x r r r Unifr Surface Heat Flux Integrating twice 1 T u dt r r 1 r r r dx r u dt r r Trx (, ) Clnr C 4 dx 4 16r 1 The teperature reain finite at r 0 iplie C 1 0.
2 C u dt 3r T ( x) dx 16 Subtituting int T u r u r 4u T ( x) u r ur T ( x) T ( x) fr Eq. () 4 ur dt 3 1 r 1 r Trx (, ) T () x dx r0 4 r0 r u 1 r 8 ur T ( x) r 8 ur T ( x) r r 0 r u( x, r) T ( x, r) rdr dt dx T ( x, r) rdr ur dt dx dt dx ur dt dx dt dx dt dx 8 r r 3 1 r r r r r r r r 1 r 4 r 3 r 16 r 1 r 4 r r 16 r r dr 1 r 4 r q P c p q P u A c c p q u c 11 ur dt T( x) T( x) 48 dx p / u /4 4q 48 uc 11 q 48 c 11 q 48 k p p dr
3 11 ur dt T( x) T( x) 48 dx 11 q 48 k Since q h( T T ) r 48 k h 11 h 4.36 fr q cntant k independent f Re, Pr and axial lcatin.
4 1. Fully evelped Flw Lainar Flw in a Circular Tube: The lcal elt nuber i a cntant thrughut the fully develped regin, but it value depend n the urface theral cnditin. Unifr Surface Heat Flux ( q ): h k 4.36 Unifr Surface Teperature ( T ): h 3.66 k Turbulent Flw in a Circular Tube: Fr a th urface and fully turbulent cnditin ( Re 10, 000 ), the ittu Belter equatin ay be ued a a firt apprxiatin: n 0.03Re Pr 0.3 T n T n0.4 T T Pr 160 Re 10,000 L 10 The effect f wall rughne and tranitinal flw cnditin Re 3000 crrelatin: ay be cnidered by uing the Gnielinki Sth urface: f 8 Re 1000 Pr Pr f
5 6 f (0.790ln Re 1.64) 3000 Re 510 Surface f rughne >0 : f Figure8.3 Nncircular Tube: Ue f hydraulic diaeter a characteritic length: h 4A c P Since the lcal cnvectin cefficient varie arund the periphery f a tube, appraching zer at it crner, crrelatin fr the fully develped regin are aciated with cnvectin cefficient averaged ver the periphery f the tube. Lainar Flw: The lcal elt nuber i a cntant whe value (Table 8.1) depend n the urface theral cnditin ( T r q ) and the duct apect rati. Turbulent Flw: A a firt apprxiatin, the ittu-belter r Gnielinki crrelatin ay be ued with the hydraulic diaeter, irrepective f the urface theral cnditin.. Effect f the Entry Regin The anner in which the elt decay fr inlet t fully develped cnditin fr lainar flw depend n the nature f theral and velcity bundary layer develpent in the entry regin, a well a the urface theral cnditin. Lainar flw in a circular tube
6 Cbined Entry Length: Theral and velcity bundary layer develp cncurrently fr unifr prfile at the inlet. Theral Entry Length: Velcity prfile i fully develped at the inlet, and bundary layer develpent in the entry regin i retricted t theral effect. Such a cnditin ay al be aued t be a gd apprxiatin fr a unifr inlet velcity prfile if Pr 1.Why? Graetz Prble Average elt ber fr Lainar Flw in a Circular Tube with Unifr Surface Teperature: Cbined Entry Length: RePr L :
7 13 Re Pr 1.86 L RePr L : 3.66 Theral Entry Length: LRe Pr L Re Pr Average elt ber fr Turbulent Flw in a Circular Tube : Effect f entry and urface theral cnditin are le prnunced fr turbulent flw and can be neglected. Fr lng tube L 60 : 3, fd Fr hrt tubel 60 :, fd C C L Nncircular Tube: Lainar Flw: h depend trngly n apect rati, a well a entry regin and urface theral cnditin. See reference 11 and 1. Turbulent Flw: A a firt apprxiatin, crrelatin fr a circular tube ay be ued with replaced by h.
8 When deterining fr any tube geetry r flw cnditin, all prpertie are t be evaluated at T T T i,, Why d lutin t internal flw prble ften require iteratin? 3. The Cncentric Tube Annulu Fluid flw thrugh regin fred by cncentric tube. Cnvectin heat tranfer ay be fr r t inner urface f uter tube and uter urface f inner tube. Surface theral cnditin ay be characterized by unifr teperaturet, T r unifr heat flux q, q. i, i, Cnvectin cefficient are aciated with each urface, where q h T T i i, i q h T T, h h i k k i h h h i
9 Fully evelped Lainar Flw elt nuber depend n i / and urface theral cnditin (Table 8., 8.3) Fully evelped Turbulent Flw Crrelatin fr a circular tube ay be ued with replaced by h.
10 Prble 8.43 Fr an air paage ued t cl a ga turbine vane, calculate the air utlet teperature and heat reved fr the vane. KNOWN: iaeter and length f cpper tubing. Teperature f cllectr plate t which tubing i ldered. Water inlet teperature and flw rate. FIN: (a) Outlet teperature f the air clant fr the precribed cnditin and (b) Cpute and plt the air utlet teperature T, a a functin f flw rate, kg/h. Cpare thi reult with the fr vane having paage diaeter f and 4. ASSUMPTIONS: (1) Steady-tate cnditin, () Ideal ga with negligible vicu diipatin and preure variatin. PROPERTIES: Table A.4, Air (aue T = 780 K, 1 at): c p = 1094 J/kgK, k = W/K, = N/, Pr = 0.706; (T = 650C = 93 K, 1 at): = N/. ANALYSIS: (a) Fr cntant wall teperature heating, fr Eq. 8.41b, T T, PLh exp T T,i cp where P =. Fr flw in a circular paage, (1)
11 kg h h Re N The flw i lainar, and ince L/ = 75 /3 = 5, the Sieder-Tate crrelatin including cbined entry length yield 1/ h Re Pr 1.86 k L 1/ W K h W K Hence, the air utlet teperature i 650 T, W K exp C kg 1094J kg K T, 578 C (b) Uing the IHT Crrelatin Tl, Internal Flw, fr Lainar Flw with cbined entry length, alng with the energy balance and rate equatin abve, the utlet teperature T, wa calculated a a functin f flw rate fr diaeter f =, 3 and 4. The plt belw hw that T, decreae nearly linearly with increaing flw rate, but i independent f paage diaeter. () (3) 650 Outlet teperature, T (C) Flw rate, dt (kg/h)
12 Baed upn the calculatin fr T, = 578 C, T = 775 K which i in gd agreeent with ur auptin t evaluate the therphyical prpertie. Why i T, independent f? Fr Eq. (3), nte that h i inverely prprtinal t, h ~ -1. Fr Eq. (1), nte that n the right-hand ide the prduct P h will be independent f. Hence, T, will depend nly n. Thi i, f cure, a cnequence f the lainar flw cnditin and will nt be the ae fr turbulent flw.
13 Prble 8.5 eterine effect f abient air teperature and wind velcity n teperature at which ven gae are dicharged fr a tack. KNOWN: Thin-walled, tall tack dicharging exhaut gae fr an ven int the envirnent. FIN: (a) Outlet ga and tack urface teperature, T, and T,, fr V=5 / and T 4 C; (b) Effect f wind teperature and velcity n T,. ASSUMPTIONS: (1) Steady-tate cnditin, () Negligible wall theral reitance, (3) Exhaut ga prpertie apprxiately the f atpheric air, (4) Negligible radiative exchange with urrunding, (5) Ideal ga with negligible vicu diipatin and preure variatin, (6) Fully develped
14 flw, (7) Cntant prpertie. PROPERTIES: Table A.4, air (aue T, = 773 K, T = 83 K, 1 at): c p = 1104 J/kgK, = N/, k = W/K, Pr = 0.71; Table A.4, air (aue T = 53 K, T = 4C = 77 K, T f = 400 K, 1 at): = /, k = W/ K, Pr = ANALYSIS: (a) Fr Eq. 8.45a, PL T, T T T,i exp U c p U1 1 1 hi h where h and h are average cefficient fr internal and external flw, repectively. i Internal flw: With a Reynld nuber f kg Re 33,87 i N The flw i turbulent, and auing fully develped cnditin thrughut the tack, the ittu-belter crrelatin ay be ued t deterine h i. h i 4/ Re Pr k i W K 4/5 0.3 h i , W K 0.5 External flw: Wrking with the Churchill/Berntein crrelatin and Hence, V Re 94, /5 0.6Re 1/ 1/3 5/8 Pr Re /3 1/4 8, Pr
15 h W K W K The utlet ga teperature i then T, 4 C C exp W K 543 C 0.5 kg 1104 J kg K The utlet tack urface teperature can be deterined fr a lcal urface energy balance f the fr, which yield, T, h T, T h T i ht i, ht W T, 3 C h i h W K b) The effect f the air teperature and velcity are a fllw 560 Ga utlet teperature, T(C) Freetrea velcity, V(/) Tinf = 35 C Tinf = 5 C Tinf = -5C ue t the elevated teperature f the ga, the variatin in abient teperature ha nly a all effect n the ga exit teperature. Hwever, the effect f the freetrea velcity i re prnunced. icharge teperature f apprxiately 530 and 560C wuld be repreentative f cld/windy and war/till atpheric cnditin, repectively.
16 COMMENTS: If there are cntituent in the ga dicharge that cndene r precipitate ut at teperature belw T,, related perating cnditin huld be avided.
7-84. Chapter 7 External Forced Convection
Chapter 7 External Frced Cnvectin 7-99 Wind i blwing ver the rf f a hue. The rate f heat tranfer thrugh the rf and the ct f thi heat l fr -h perid are t be deterined. Auptin Steady perating cnditin exit.
More informationME 315 Exam 2 Wednesday, November 11, 2015 CIRCLE YOUR DIVISION
ME 315 Exa edneday, Nveber 11, 015 Thi i a cled-bk, cled-nte exainatin. There i a frula heet rvided. Yu are al allwed t bring yur wn ne-age letter ize, dubleided crib heet. Yu ut turn ff all cunicatin
More informationCONVECTION IN MICROCHANNELS
CAPER. Intrductin CONVECION IN MICROCANNELS.. Cntinuu and hernaic ythei. Previu chater are baed n tw fundaental autin: () Cntinuu: Navier-Stke equatin, and the energy equatin are alicable () hernaic equilibriu:
More informationChapter 9 Compressible Flow 667
Chapter 9 Cmpreible Flw 667 9.57 Air flw frm a tank thrugh a nzzle int the tandard atmphere, a in Fig. P9.57. A nrmal hck tand in the exit f the nzzle, a hwn. Etimate (a) the tank preure; and (b) the ma
More informationrcrit (r C + t m ) 2 ] crit + t o crit The critical radius is evaluated at a given axial location z from the equation + (1 , and D = 4D = 555.
hapter 1 c) When the average bld velcity in the capillary is reduced by a factr f 10, the delivery f the slute t the capillary is liited s that the slute cncentratin after crit 0.018 c is equal t er at
More informationShort notes for Heat transfer
Furier s Law f Heat Cnductin Shrt ntes fr Heat transfer Q = Heat transfer in given directin. A = Crss-sectinal area perpendicular t heat flw directin. dt = Temperature difference between tw ends f a blck
More informationNONISOTHERMAL OPERATION OF IDEAL REACTORS Continuous Flow Stirred Tank Reactor (CSTR)
he 47 Fall 2005 LEURE 7 NONISOHERML OPERION OF IDEL REORS ntinuu Flw Stirred ank Reactr (SR) F, Q V F r F, Q V F Figure : Scheatic f SR with acket and cil uptin: Hgeneu yte a) Single Reactin υ 0 b) Steady
More informationChapter 4. Unsteady State Conduction
Chapter 4 Unsteady State Cnductin Chapter 5 Steady State Cnductin Chee 318 1 4-1 Intrductin ransient Cnductin Many heat transfer prblems are time dependent Changes in perating cnditins in a system cause
More informationChapter 8. Root Locus Techniques
Chapter 8 Rt Lcu Technique Intrductin Sytem perfrmance and tability dt determined dby cled-lp l ple Typical cled-lp feedback cntrl ytem G Open-lp TF KG H Zer -, - Ple 0, -, -4 K 4 Lcatin f ple eaily fund
More informationNONISOTHERMAL OPERATION OF IDEAL REACTORS Plug Flow Reactor. F j. T mo Assumptions:
NONISOTHERMAL OPERATION OF IDEAL REACTORS Plug Flw Reactr T T T T F j, Q F j T m,q m T m T m T m Aumptin: 1. Hmgeneu Sytem 2. Single Reactin 3. Steady State Tw type f prblem: 1. Given deired prductin rate,
More information3. Internal Flow General Concepts:
3. Internal Flow General Concet: ρ u u 4 & Re Re, cr 2300 μ ν π μ Re < 2300 lainar 2300 < Re < 4000 tranitional Flow Regie : Re > 4000 turbulent Re > 10,000 fully turbulent (d) 1 (e) Figure 1 Boundary
More informationCIRCLE YOUR DIVISION: Div. 1 (9:30 am) Div. 2 (11:30 am) Div. 3 (2:30 pm) Prof. Ruan Prof. Naik Mr. Singh
Nae: CIRCLE YOUR DIVISION: Div. 1 (9:30 a) Div. (11:30 a) Div. 3 (:30 p) Prof. Ruan Prof. Nai Mr. Singh School of Mechanical Engineering Purdue Univerity ME315 Heat and Ma Tranfer Exa # edneday, October
More informationNumerical Simulation of the Thermal Resposne Test Within the Comsol Multiphysics Environment
Presented at the COMSOL Cnference 2008 Hannver University f Parma Department f Industrial Engineering Numerical Simulatin f the Thermal Respsne Test Within the Cmsl Multiphysics Envirnment Authr : C. Crradi,
More informationExternal Flow: Flow over Bluff Objects (Cylinders, Spheres, Packed Beds) and Impinging Jets
External Flow: Flow over Bluff Object (Cylinder, Sphere, Packed Bed) and Impinging Jet he Cylinder in Cro Flow - Condition depend on pecial feature of boundary layer development, including onet at a tagnation
More informationBernoulli s equation may be developed as a special form of the momentum or energy equation.
BERNOULLI S EQUATION Bernoulli equation may be developed a a pecial form of the momentum or energy equation. Here, we will develop it a pecial cae of momentum equation. Conider a teady incompreible flow
More informationExaminer: Dr. Mohamed Elsharnoby Time: 180 min. Attempt all the following questions Solve the following five questions, and assume any missing data
Benha University Cllege f Engineering at Banha Department f Mechanical Eng. First Year Mechanical Subject : Fluid Mechanics M111 Date:4/5/016 Questins Fr Final Crrective Examinatin Examiner: Dr. Mhamed
More informationChapter 3. Electric Flux Density, Gauss s Law and Divergence
Chapter 3. Electric Flu Denity, Gau aw and Diergence Hayt; 9/7/009; 3-1 3.1 Electric Flu Denity Faraday Eperiment Cncentric phere filled with dielectric material. + i gien t the inner phere. - i induced
More informationTHE INFLUENCE OF SURFACE INCLINATION ON THE CALIBRATION OF SURFACE TEMPERATURE SENSORS
Prceeding, XVII IMEKO Wrld Cngre, June 22 27, 2003, Dubrvnik, Cratia Prceeding, XVII IMEKO Wrld Cngre, June 22 27, 2003, Dubrvnik, Cratia XVII IMEKO Wrld Cngre Metrlgy in the 3 rd Millennium June 22 27,
More informationY.J. Cho **, Hazim Awbi** & Taghi Karimipanah* *) Fresh AB, SWEDEN **) University of Reading, UK
The Characteristics f Wall Cnfluent Jets fr Ventilated Enclsures 9 th Internatinal Cnference n Air Distributin in Rs niversity f Cibra PORTGAL Y.J. Ch **, Hazi Awbi** & Taghi Kariipanah* *) Fresh AB, SWEDEN
More informationName Student ID. A student uses a voltmeter to measure the electric potential difference across the three boxes.
Name Student ID II. [25 pt] Thi quetin cnit f tw unrelated part. Part 1. In the circuit belw, bulb 1-5 are identical, and the batterie are identical and ideal. Bxe,, and cntain unknwn arrangement f linear
More informationCANKAYA UNIVERSITY FACULTY OF ENGINEERING MECHANICAL ENGINEERING DEPARTMENT ME 313 HEAT TRANSFER
CANKAYA UNIVERSITY FACUTY OF ENGINEERING MECHANICA ENGINEERING DEPARTMENT ME 313 HEAT TRANSFER CHAPTER-3 EXAMPES 1) Cnsider a slab f thicness as illustrated in figure belw. A fluid at temperature T 1 with
More information7.0 Heat Transfer in an External Laminar Boundary Layer
7.0 Heat ransfer in an Eternal Laminar Bundary Layer 7. Intrductin In this chapter, we will assume: ) hat the fluid prperties are cnstant and unaffected by temperature variatins. ) he thermal & mmentum
More information(b) Using the ideal gas equation of state, and noting that the total mass of gas occupies the same total volume at the final state as initially: where
6.55 Given: An inulated cylinder i initially divided int halve y a itn. On either ide the itn i a ga at a knwn tate. The itn i releaed and equiliriu i attained. Find: Deterine the inal reure, inal teerature,
More informationStudy Group Report: Plate-fin Heat Exchangers: AEA Technology
Study Grup Reprt: Plate-fin Heat Exchangers: AEA Technlgy The prblem under study cncerned the apparent discrepancy between a series f experiments using a plate fin heat exchanger and the classical thery
More informationLecture 2: Single-particle Motion
Lecture : Single-particle Mtin Befre we start, let s l at Newtn s 3 rd Law Iagine a situatin where frces are nt transitted instantly between tw bdies, but rather prpagate at se velcity c This is true fr
More informationth th th The air-fuel ratio is determined by taking the ratio of the mass of the air to the mass of the fuel,
Cheical Reactins 14-14 rpane is burned wi 75 percent excess during a cbustin prcess. The AF rati is t be deterined. Assuptins 1 Cbustin is cplete. The cbustin prducts cntain CO, H O, O, and N nly. rperties
More informationDisclaimer: This lab write-up is not
Diclaier: Thi lab write-up i nt t be cpied, in whle r in part, unle a prper reference i ade a t the urce. (It i trngly recended that yu ue thi dcuent nly t generate idea, r a a reference t explain cplex
More informationInternal Forced Convection. Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Internal Forced Convection Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Introduction Pipe circular cross section. Duct noncircular cross section. Tubes small-diameter
More informationSediment transport mechanisms 1. Bed-load transport
10 Sediment tranprt mechanim 1. Bed-lad tranprt 10.1 Intrductin When the bed hear tre exceed a critical value, ediment are tranprted in the frm f bed-lad and upended lad. Fr bed-lad tranprt, the baic mde
More informationIntroduction to Heat and Mass Transfer. Week 14
Introduction to Heat and Mass Transfer Week 14 Next Topic Internal Flow» Velocity Boundary Layer Development» Thermal Boundary Layer Development» Energy Balance Velocity Boundary Layer Development Velocity
More informationNonisothermal Chemical Reactors
he 471 Fall 2014 LEUE 7a Nnithermal hemical eactr S far we have dealt with ithermal chemical reactr and were able, by ug nly a many pecie ma balance a there are dependent react t relate reactr ize, let
More informationconvection coefficient. The different property values of water at 20 C are given by: u W/m K, h=8062 W/m K
Practice rblems fr Cnvective Heat Transfer 1. Water at 0 C flws ver a flat late 1m 1m at 10 C with a free stream velcity f 4 m/s. Determine the thickness f bndary layers, lcal and average vale f drag cefficient
More informationTime varying fields and Maxwell's equations Chapter 9
Tie varying fields and Maxwell's equatins hapter 9 Dr. Naser Abu-Zaid Page 9/7/202 FARADAY LAW OF ELETROMAGNETI INDUTION A tie varying agnetic field prduces (induces) a current in a clsed lp f wire. The
More informationChapter 5: Diffusion (2)
Chapter 5: Diffusin () ISSUES TO ADDRESS... Nn-steady state diffusin and Fick s nd Law Hw des diffusin depend n structure? Chapter 5-1 Class Eercise (1) Put a sugar cube inside a cup f pure water, rughly
More informationHEAT CONDUCTION IN CONVECTIVELY COOLED ECCENTRIC SPHERICAL ANNULI A Boundary Integral Moment Method
Yilazer, A., et al.: Heat Cnductin in Cnvectively Cled Eccentric... THERMAL SCIENCE, Year 017, Vl. 1, N. 5, pp. 55-66 55 Intrductin HEAT CONDUCTION IN CONVECTIVELY COOLED ECCENTRIC SPHERICAL ANNULI A Bundary
More informationProblem 1 Known: Dimensions and materials of the composition wall, 10 studs each with 2.5m high
Prblem Knwn: Dimensins and materials f the cmpsitin wall, 0 studs each with.5m high Unknwn:. Thermal resistance assciate with wall when surfaces nrmal t the directin f heat flw are isthermal. Thermal resistance
More informationPHY 140Y FOUNDATIONS OF PHYSICS Problem Set #2
PHY 140Y FOUNDATIONS OF PHYSICS 2001-2002 Prble Set #2 HANDED OUT: DUE: Friday, Octber 5, 2001 (in cla) 5:00 PM, Thurday, Octber 18, 2001 in the apprpriate bx, labeled by tutrial grup, in the baeent at
More informationModeling Crystallization in CMSMPR: Results of Validation Study on Population Balance Modeling in FLUENT
Mdeling Crystallizatin in CMSMPR: Results f Validatin Study n Ppulatin Balance Mdeling in FLUENT Bin Wan and Terry A. Ring Dept. Cheical Engineering Uniersity f Utah Salt Lake City, UT 84 and Kuar M. Dhanasekharan
More informationElectric Current and Resistance
Electric Current and Resistance Electric Current Electric current is the rate f flw f charge thrugh sme regin f space The SI unit f current is the ampere (A) 1 A = 1 C / s The symbl fr electric current
More informationwhich represents a straight line whose slope is C 1.
hapte, Slutin 5. Ye, thi claim i eanable ince in the abence any heat eatin the ate heat tane thugh a plain wall in teady peatin mut be cntant. But the value thi cntant mut be ze ince ne ide the wall i
More informationAdvanced Heat and Mass Transfer by Amir Faghri, Yuwen Zhang, and John R. Howell
6.5 Natural Cnvectin in Enclsures Enclsures are finite spaces bunded by walls and filled with fluid. Natural cnvectin in enclsures, als knwn as internal cnvectin, takes place in rms and buildings, furnaces,
More informationGEOTHERMAL DEICING IN A MINE TUNNEL
POCEEDINGS, Thirty-Sith rkhp n Getheral eervir Engineering Stanfrd Univerity, Stanfrd, Califrnia, January - February, 0 SGP-T-9 GEOTHEMAL DEICING IN A MINE TUNNEL Anik Tth Univerity f Miklc Miklc-Egyetevar,
More informationGAUSS' LAW E. A. surface
Prf. Dr. I. M. A. Nasser GAUSS' LAW 08.11.017 GAUSS' LAW Intrductin: The electric field f a given charge distributin can in principle be calculated using Culmb's law. The examples discussed in electric
More informationLecture 13 - Boost DC-DC Converters. Step-Up or Boost converters deliver DC power from a lower voltage DC level (V d ) to a higher load voltage V o.
ecture 13 - Bt C-C Cnverter Pwer Electrnic Step-Up r Bt cnverter eliver C pwer frm a lwer vltage C level ( ) t a higher la vltage. i i i + v i c T C (a) + R (a) v 0 0 i 0 R1 t n t ff + t T i n T t ff =
More informationThe Journal of Supercritical Fluids
J. f Supercritical Fluids 7 (212) 75 89 ntents lists available at SciVerse ScienceDirect The Jurnal f Supercritical Fluids ju rn al h m epage: www.elsevier.cm/lcate/supflu Flw and heat transfer characteristics
More informationHEAT TRANSFER AND PRESSURE DROP CHARACTERISTICS OF A HORIZONTAL ANNULAR PASSAGE IN THE TRANSITIONAL FLOW REGIME
HEAT TRANSFER AND PRESSURE DROP CHARACTERISTICS OF A HORIZONTAL ANNULAR PASSAGE IN THE TRANSITIONAL FLOW REGIME Ndenguma D.D., Dirker J.* and Meyer J.P. *Authr fr crrespndence Department f Mechanical and
More informationChE 471: LECTURE 4 Fall 2003
ChE 47: LECTURE 4 Fall 003 IDEL RECTORS One f the key gals f chemical reactin engineering is t quantify the relatinship between prductin rate, reactr size, reactin kinetics and selected perating cnditins.
More informationConvection Workshop. Academic Resource Center
Convection Workshop Academic Resource Center Presentation Outline Understanding the concepts Correlations External Convection (Chapter 7) Internal Convection (Chapter 8) Free Convection (Chapter 9) Solving
More informationA Kinetic Model Framework for Combined Diffusion and Adsorption Processes
BRINKMANN, E.A. and KING, R.P. A kinetic del fraewrk fr cbined diffuin and adrptin prcee. APCOM 87. Prceeding f the Twentieth Internatinal Sypiu n the Applicatin f Cputer and Matheatic in the Mineral Indutrie.
More informationAircraft Performance - Drag
Aircraft Perfrmance - Drag Classificatin f Drag Ntes: Drag Frce and Drag Cefficient Drag is the enemy f flight and its cst. One f the primary functins f aerdynamicists and aircraft designers is t reduce
More informationbulk velocity through orifice,
150A Review Sessin Other Frictin Lsses Bernulli hf accunts fr all types f drag: is drag due t skin frictin is drag due t fittings (tabulated fractin f the velcity head) is drag due t units (a given r calculated
More informationStudy on the Heat Transfer Performance of the Annular Fin under Condensing Conditions Abdenour Bourabaa, Malika Fekih, Mohamed Saighi
Study n the Heat Tranfer Perfrmance f the Annular Fin under Cndening Cnditin Adenur Buraaa, Malika Fekih, Mhamed Saighi Atract A numerical invetigatin f the fin efficiency and temperature ditriutin f an
More informationMAE 101A. Homework 3 Solutions 2/5/2018
MAE 101A Homework 3 Solution /5/018 Munon 3.6: What preure gradient along the treamline, /d, i required to accelerate water upward in a vertical pipe at a rate of 30 ft/? What i the anwer if the flow i
More informationCompressibility Effects
Definitin f Cmpressibility All real substances are cmpressible t sme greater r lesser extent; that is, when yu squeeze r press n them, their density will change The amunt by which a substance can be cmpressed
More informationQ1. In figure 1, Q = 60 µc, q = 20 µc, a = 3.0 m, and b = 4.0 m. Calculate the total electric force on q due to the other 2 charges.
Phys10 Secnd Majr-08 Zer Versin Crdinatr: Dr. I. M. Nasser Saturday, May 3, 009 Page: 1 Q1. In figure 1, Q = 60 µc, q = 0 µc, a = 3.0 m, and b = 4.0 m. Calculate the ttal electric frce n q due t the ther
More informationC. Kranenburg \ VERVALL~\J \ Internal Report No Laboratory of Fluid Mechanics. Department of Civil Engineering. Delft University of Technology
A I {ple diffuin-cntrled del f ixing acr a tabie denity interface C. Kranenburg \ VERVALL~\J \ Internal Reprt N. 2-79 Labratry f Fluid Mechanic Departent f Civil Engineering Delft Univerity f Technlgy
More information, which yields. where z1. and z2
The Gaussian r Nrmal PDF, Page 1 The Gaussian r Nrmal Prbability Density Functin Authr: Jhn M Cimbala, Penn State University Latest revisin: 11 September 13 The Gaussian r Nrmal Prbability Density Functin
More informationNONISOTHERMAL OPERATION OF IDEAL REACTORS Plug Flow Reactor
NONISOTHERMAL OPERATION OF IDEAL REACTORS Plug Flow Reactor T o T T o T F o, Q o F T m,q m T m T m T mo Aumption: 1. Homogeneou Sytem 2. Single Reaction 3. Steady State Two type of problem: 1. Given deired
More informationENGI 4430 Parametric Vector Functions Page 2-01
ENGI 4430 Parametric Vectr Functins Page -01. Parametric Vectr Functins (cntinued) Any nn-zer vectr r can be decmpsed int its magnitude r and its directin: r rrˆ, where r r 0 Tangent Vectr: dx dy dz dr
More informationConcept of Reynolds Number, Re
Concept of Reynold Nuber, Re Ignore Corioli and Buoyancy and forcing Acceleration Advection Preure Gradient Friction I II III IV u u 1 p i i u ( f u ) b + u t x x x j i i i i i i U U U? U L L If IV <
More informationMaterials Engineering 272-C Fall 2001, Lecture 7 & 8 Fundamentals of Diffusion
Materials Engineering 272-C Fall 2001, Lecture 7 & 8 Fundamentals f Diffusin Diffusin: Transprt in a slid, liquid, r gas driven by a cncentratin gradient (r, in the case f mass transprt, a chemical ptential
More informationFrequency Response of Amplifiers
類比電路設計 (3349-004 Frequency epne f Aplifier h-uan an Natinal hun-h Univerity epartent f Electrical Eneer Overview ead B azavi hapter 6 ntrductin n thi lecture, we tudy the repne f le-tae and differential
More information1 The limitations of Hartree Fock approximation
Chapter: Pst-Hartree Fck Methds - I The limitatins f Hartree Fck apprximatin The n electrn single determinant Hartree Fck wave functin is the variatinal best amng all pssible n electrn single determinants
More informationCHAPTER 8b Static Equilibrium Units
CHAPTER 8b Static Equilibrium Units The Cnditins fr Equilibrium Slving Statics Prblems Stability and Balance Elasticity; Stress and Strain The Cnditins fr Equilibrium An bject with frces acting n it, but
More informationJ.P. Holman: 3.09) T sur := Use table 3-1 to determine the shape factor for this problem. 4π r S := T sphere := 30K r 1. S = m k := 1.
.P. Holman:.09) T ur : 0 Ue table - to determine the hape factor for thi problem. D :.m r : 0.5m π r S : T phere : 0 r D S 7.0 m :.7 m Ue eq. - to calculate the heat lo. q : S T phere T ur q 57.70 .P.
More informationPhysics 212. Lecture 12. Today's Concept: Magnetic Force on moving charges. Physics 212 Lecture 12, Slide 1
Physics 1 Lecture 1 Tday's Cncept: Magnetic Frce n mving charges F qv Physics 1 Lecture 1, Slide 1 Music Wh is the Artist? A) The Meters ) The Neville rthers C) Trmbne Shrty D) Michael Franti E) Radiatrs
More informationConservation of Momentum
Cnervatin f Mmentum PES 1150 Prelab Quetin Name: Lab Statin: 003 ** Diclaimer: Thi re-lab i nt t be cied, in whle r in art, unle a rer reference i made a t the urce. (It i trngly recmmended that yu ue
More informationCONVECTIVE HEAT TRANSFER
CONVECTIVE HEAT TRANSFER Mohammad Goharkhah Department of Mechanical Engineering, Sahand Unversity of Technology, Tabriz, Iran CHAPTER 4 HEAT TRANSFER IN CHANNEL FLOW BASIC CONCEPTS BASIC CONCEPTS Laminar
More informationFlipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System
Flipping Physics Lecture Ntes: Simple Harmnic Mtin Intrductin via a Hrizntal Mass-Spring System A Hrizntal Mass-Spring System is where a mass is attached t a spring, riented hrizntally, and then placed
More informationQ1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string?
Term: 111 Thursday, January 05, 2012 Page: 1 Q1. A string f length L is fixed at bth ends. Which ne f the fllwing is NOT a pssible wavelength fr standing waves n this string? Q2. λ n = 2L n = A) 4L B)
More informationAssume that the water in the nozzle is accelerated at a rate such that the frictional effect can be neglected.
1 HW #3: Cnservatin f Linear Mmentum, Cnservatin f Energy, Cnservatin f Angular Mmentum and Turbmachines, Bernulli s Equatin, Dimensinal Analysis, and Pipe Flws Prblem 1. Cnservatins f Mass and Linear
More information( ) kt. Solution. From kinetic theory (visualized in Figure 1Q9-1), 1 2 rms = 2. = 1368 m/s
.9 Kinetic Mlecular Thery Calculate the effective (rms) speeds f the He and Ne atms in the He-Ne gas laser tube at rm temperature (300 K). Slutin T find the rt mean square velcity (v rms ) f He atms at
More informationFundamental Concepts in Structural Plasticity
Lecture Fundamental Cncepts in Structural Plasticit Prblem -: Stress ield cnditin Cnsider the plane stress ield cnditin in the principal crdinate sstem, a) Calculate the maximum difference between the
More informationME 315 Exam 3 8:00-9:00 PM Thursday, April 16, 2009 CIRCLE YOUR DIVISION
ME 315 Exam 3 8:00-9:00 PM Thurday, Aril 16, 009 Thi i a cloed-book, cloed-note examination. There i a formula heet at the back. You mut turn off all communication device before tarting thi exam, and leave
More informationAn Experimental Study for Mixed Convection through a Circular Tube Filled with Porous Media and Fixed Horizontally and Inclined
www.ccenet.rg/ma Mdern Applied Science Vl., N. ; April 0 An Experimental Study fr Mixed Cnvectin thrugh a Circular Tube Filled with Pru Media and Fixed Hrizntally and Inclined Taheen Ahmad Taheen Mechanical
More informationh = 0 km for your table in (a)], and for T0 = 316 K. Then obtain a Homework 1 AERE355 Fall 2017 Due 9/1(F)
1 Herk 1 AERE355 Fall 17 Due 9/1(F) SOLUION NOE: If yur slutin des nt adhere t the frat described in the syllabus, it ill be grade as zer Prble 1(5pts) In the altitude regin < h < 1k, e have the flling
More informationME 331 Homework Assignment #6
ME 33 Homework Assignment #6 Problem Statement: ater at 30 o C flows through a long.85 cm diameter tube at a mass flow rate of 0.020 kg/s. Find: The mean velocity (u m ), maximum velocity (u MAX ), and
More informationCHEM Thermodynamics. Change in Gibbs Free Energy, G. Review. Gibbs Free Energy, G. Review
Review Accrding t the nd law f Thermdynamics, a prcess is spntaneus if S universe = S system + S surrundings > 0 Even thugh S system
More informationL a) Calculate the maximum allowable midspan deflection (w o ) critical under which the beam will slide off its support.
ecture 6 Mderately arge Deflectin Thery f Beams Prblem 6-1: Part A: The department f Highways and Public Wrks f the state f Califrnia is in the prcess f imprving the design f bridge verpasses t meet earthquake
More informationAerodynamic Separability in Tip Speed Ratio and Separability in Wind Speed- a Comparison
Jurnal f Physics: Cnference Series OPEN ACCESS Aerdynamic Separability in Tip Speed Rati and Separability in Wind Speed- a Cmparisn T cite this article: M L Gala Sants et al 14 J. Phys.: Cnf. Ser. 555
More information4.5 Evaporation and Diffusion Evaporation and Diffusion through Quiescent Air (page 286) bulk motion of air and j. y a,2, y j,2 or P a,2, P j,2
4.5 Evaporation and Diffuion 4.5.4 Evaporation and Diffuion through Quiecent Air (page 86) z bul otion of air and j z diffuion of air (a) diffuion of containant (j) y a,, y j, or P a,, P j, z 1 volatile
More informationMECHANICS OF SOLIDS TORSION TUTORIAL 2 TORSION OF THIN WALLED SECTIONS AND THIN STRIPS
MECHANICS OF SOLIDS ORSION UORIAL ORSION OF HIN WALLED SECIONS AND HIN SRIPS Yu shuld judge yur prgress by cmpleting the self assessment exercises. On cmpletin f this tutrial yu shuld be able t d the fllwing.
More informationLiquid or gas flow through pipes or ducts is commonly used in heating and
cen58933_ch08.qxd 9/4/2002 11:29 AM Page 419 INTERNAL FORCED CONVECTION CHAPTER 8 Liquid or gas flow through pipes or ducts is commonly used in heating and cooling applications. The fluid in such applications
More informationEE247B/ME218: Introduction to MEMS Design Lecture 7m1: Lithography, Etching, & Doping CTN 2/6/18
EE247B/ME218 Intrductin t MEMS Design Lecture 7m1 Lithgraphy, Etching, & Dping Dping f Semicnductrs Semicnductr Dping Semicnductrs are nt intrinsically cnductive T make them cnductive, replace silicn atms
More informationI. Analytical Potential and Field of a Uniform Rod. V E d. The definition of electric potential difference is
Length L>>a,b,c Phys 232 Lab 4 Ch 17 Electric Ptential Difference Materials: whitebards & pens, cmputers with VPythn, pwer supply & cables, multimeter, crkbard, thumbtacks, individual prbes and jined prbes,
More informationModelling of NOLM Demultiplexers Employing Optical Soliton Control Pulse
Micwave and Optical Technlgy Letters, Vl. 1, N. 3, 1999. pp. 05-08 Mdelling f NOLM Demultiplexers Emplying Optical Slitn Cntrl Pulse Z. Ghassemly, C. Y. Cheung & A. K. Ray Electrnics Research Grup, Schl
More informationInertial Mass of Charged Elementary Particles
David L. Bergan 1 Inertial Mass Inertial Mass f Charged Eleentary Particles David L. Bergan Cn Sense Science P.O. Bx 1013 Kennesaw, GA 30144-8013 Inertial ass and its prperty f entu are derived fr electrdynaic
More informationPhy 212: General Physics II 1 Chapter 18 Worksheet 3/20/2008
Phy 1: General Physics II 1 hapter 18 rksheet 3/0/008 Thermal Expansin: 1. A wedding ring cmpsed f pure gld (inner diameter = 1.5 x 10 - m) is placed n a persn s finger (diameter = 1.5 x 10 - m). Bth the
More informationModule 4: General Formulation of Electric Circuit Theory
Mdule 4: General Frmulatin f Electric Circuit Thery 4. General Frmulatin f Electric Circuit Thery All electrmagnetic phenmena are described at a fundamental level by Maxwell's equatins and the assciated
More informationECEN 4872/5827 Lecture Notes
ECEN 4872/5827 Lecture Ntes Lecture #5 Objectives fr lecture #5: 1. Analysis f precisin current reference 2. Appraches fr evaluating tlerances 3. Temperature Cefficients evaluatin technique 4. Fundamentals
More informationMODULE 5 Lecture No: 5 Extraterrestrial Radiation
1 P age Principle and Perfrmance f Slar Energy Thermal Sytem: A Web Cure by V.V.Satyamurty MODULE 5 Lecture N: 5 Extraterretrial Radiatin In Mdule 5, Lecture N. 5 deal with 5.1 INTRODUCTION 5. EXTRA TERRESTRIAL
More informationPhysics 102. Second Midterm Examination. Summer Term ( ) (Fundamental constants) (Coulomb constant)
ε µ0 N mp T kg Kuwait University hysics Department hysics 0 Secnd Midterm Examinatin Summer Term (00-0) July 7, 0 Time: 6:00 7:0 M Name Student N Instructrs: Drs. bdel-karim, frusheh, Farhan, Kkaj, a,
More informationChapter 2 Analysis of Power System Stability by Classical Methods
Chapter Analyi f wer Syte Stability by Claical Methd.1 Claical Mdel A dicued in the previu Chapter, the firt tep in analyzing pwer tability i t repreent the pwer yte cpnent atheatically. The iplet yet
More informationEntropy Generation Analysis for Various Cross-sectional Ducts in Fully Developed Laminar Convection with Constant Wall Heat Flux
Korean Chem. Eng. Res., 52(3), 294-301 (2014) http://dx.doi.org/10.9713/kcer.2014.52.3.294 PISSN 0304-128X, EISSN 2233-9558 Entropy Generation Analysis for Various Cross-sectional Ducts in Fully Developed
More informationPhys101 Final Code: 1 Term: 132 Wednesday, May 21, 2014 Page: 1
Phys101 Final Cde: 1 Term: 1 Wednesday, May 1, 014 Page: 1 Q1. A car accelerates at.0 m/s alng a straight rad. It passes tw marks that are 0 m apart at times t = 4.0 s and t = 5.0 s. Find the car s velcity
More informationDesign and Analysis of Gas Turbine Blade by Potential Flow Approach
V. Vijaya kumar et al Int. Jurnal f Engineering Research and Applicatins RESEARCH ARTICLE OPEN ACCESS Design and Analysis f Gas Turbine Blade by Ptential Flw Apprach V. Vijaya Kumar 1, R. Lalitha Narayana
More informationAn Empirical Study of Frost Accumulation Effects on Louvered-Fin, Microchannel Heat Exchangers
Purdue Univerity Purdue e-pub Internatinal Refrigeratin and Air Cnditining Cnference Schl f Mechanical Engineering 4 An Empirical Study f Frt Accumulatin Effect n Luvered-Fin, Micrchannel Heat Exchanger
More information1) p represents the number of holes present. We know that,
ECE650R : Reliability Physics f Nanelectrnic Devices Lecture 13 : Features f FieldDependent NBTI Degradatin Date : Oct. 11, 2006 Classnte : Saakshi Gangwal Review : Pradeep R. Nair 13.0 Review In the last
More informationBuoyancy Effect on the Fully Developed Air Flow in Concentric Inclined Annulus
Internatinal Jurnal f Mechanical & Mechatrnics Engineering IJMME-IJENS Vl:3 N:0 46 Buyancy Effect n the Fully Develped Air Flw in Cncentric Inclined Annulus Asmaa Ali Hussein Lecturer Fundatin Of Technical
More informationChapter 30. Inductance
Chapter 30 nductance 30. Self-nductance Cnsider a lp f wire at rest. f we establish a current arund the lp, it will prduce a magnetic field. Sme f the magnetic field lines pass thrugh the lp. et! be the
More information