ε (5) 4. Radiative Heat Transfer 4.1 Fundamentals of thermal radiation (1) W/m / K Stefan-Boltzmann-constant

Size: px
Start display at page:

Download "ε (5) 4. Radiative Heat Transfer 4.1 Fundamentals of thermal radiation (1) W/m / K Stefan-Boltzmann-constant"

Transcription

1 . Radatve Heat ranfer. Fundamental of thermal radaton 0 ( λ) q I dλ σ () max 8 σ 5,67 0 W/m / K Stefan-Boltzmann-contant λ ( λ) q I dλ () λ 0 emperature q λ / q Sun 6000 K 0, µm Hot materal 600 K 0 µm Envronment 300 K 5 50 µm q (3) σ emvty f( λ) aborptvty a Krchhoff la () λ λ mean emvty ( ) λ 0 ( λ) I( λ,) σ dλ emvty of gae exp( a p ) (5) λ λ Approxmaton A exp( B ) (6) Ga A B p n bar m n K 0,5 p 0. 0, 085 6,7 0 ( p ) 0,0,5 > ( p ) ,00 0,0 0,60 p 0, 0, 5,3 0 ( p ) 0, > p 0. 0,0 0, CO ( ) 6 H O ( ) 5 ( ) 7 ( a p a p ) exp λ CO λh O H O (7) CO (8) CO HO CO HO mean beam length

2 V 0,9 (9) A. Radaton beteen area (ve factor) Lambert la q q co ψ (0) ψ n q π / π q n ψ 0 ϕ 0 co ψ n ψ dψ dϕ π q n dq () σ da dq ϕ dq () coψ coψ ϕ A da da (3) π A A ϕ A ϕ A 0 ϕ for flat or convex urface (no element can ee an other) ϕ 0 for nfnte parallel plate or encloure (all radaton from element meet element k) ϕ k.3 Radaton exchange beteen urface ρ α q reflectvty aborptvty emvty heat flux (reflectance) (aborptance) (emttance) q h b h b radoty rradaton

3 h e e ρ b emon e q σ ρ [ e ( ρ ) h ] N b h k k ϕ k h ρ N k h k ϕ k e (ρ ϕ ) h ρ ϕ h K ρ ϕ h e ρ ϕ h ( ρ ϕ ) h L ρ ϕ h e N N N N N ρ ϕ h ρ ϕ h K ( ρ ϕ ) h N R h e N N N NN N e N R ρϕ ρϕ L ρϕn ρϕ ρϕ L ρϕn M M O M ρn ϕn ρn ϕn ρ L N ϕnn h M h N, h h, e e e. M e N e quaton for h h R e nvere matrx calculaton th commercal program q ρ [ e ( ρ ) h ] Example to parallel nfnte plate ϕ ϕ ϕ ϕ 0 no emon reache on urface h ρ h e

4 ρ h h e h e ρ e ρ ρ ρ q e e ( ) q σ ρ ρ q σ ( ) overall emvty Example for encloure ( ρ ϕ) h ρ ϕ h e ρ h ϕ ( ρ ϕ ) h h e [( ρ ϕ ) e ρ ϕ e ] j jj j j for, j or, j ( ρ ϕ ) ( ρ ϕ ) ρ ρ ϕ ϕ q ϕ ϕ ( ) σ A ϕ A ϕ A A Q σ A ( ) (8) urroundng area A < A

5 ( A A A Q σ ) (9). Radaton held ( 0 q σ ) (0) ( q σ ) () ( q σ ) () Replacng ( q σ ) (3), () ( ) q σ (5) q q 0 (6) : ( ) ( ) q q 0 (7) : q q 0 (8) : 0 q q (9)

6 .5 Heat tranfer by radaton and convecton.5. Radatve heat tranfer q α ( ) σ ( ) ( ) q ( α α ) α ( ) σ ( ) 3 3 α σ 3 3 << α σ 3 / α σ.5. hermocouple (tc) tc ( g tc Q α A ) ( 30) Q A σ tc tc ( ) tc (3) g tc tc tc σ α (3) Q α α A tc σ ( ) tc 3 tc tc (33) (3) tc α g α g α / α (35) α α α / α α / α 0 : tc g meaurng ga temperature accuratvly:. hgh convectve heat tranfer mall dameter of thermocouple Nu 0,66 Re 0,5 Pr 0,33 (36) α d tc d Nu, Re tc (37) λ ν

7 α ~ d... 0,5 tc d tc. lo radatv heat tranfer radaton held for thermocouple.5.3 Secondary radaton Q Q Q Q g Q g (38) adabatc all (39) Q Q Q g g α α g g A A σ A ( ) g ( ) g ( ) (0) () () from Eq. (39) th () and () Lnearzaton of radaton Q α A ( ) (3) α g g () α g α α Q α / αg α g A ( g ) (5) α / α g α α 0 e.g. 0 / g Q Q g α e.g. hgh /α g Q Q g

8 .6 Radatve heat tranfer beteen ga and old ( ) Q σ A g g g (6) g g (7) a g (8) a g a emvty of ga for g emvty of ga for emvty of all.7 Radatve heat tranfer beteen ga, old and all Q g g σ ( g ) A (9) g g ( g ) A Q σ (50) ( ) A Q σ (5) Q Q g Q (5) Q adabatc all (53) g Q g g g A A / A / A (5) Q g ( g ) A A σ (55) g A

9 Materal Metal th polhed and brght urface Ag, Al, Cr, Cu, Fe, Hg, Pb, Sn, Zn, bra Metal th reacted urface oxdzed, galvanzed, carburzed, ruty teel, cat ron Inorganc non-metallc materal concrete, gla, ceramc, porcellan, clay, brck, refractore, ce Organc materal Platc, pant, paper, rubber, ood Graphte ab. -: Approxmate value for emvte at ambent temperature Geometry of ga volumne nfnte lab, thckne t cube, length a retangular, man length a phere, dameter d long cylnder, dameter d long half cylnder, dameter d Mean beam length.8 t 0.6 a 0.9 a 0.6 d 0.9 d 0.6 d ab. -: Approxmate value for mean beam length

10 Formeln Kaptel E G AGe G. (.) H E ρ B W W W B H ϕ H ϕ τ H W G GW W WW GW G E G W. (.), (.3) (.) G q GW q WG GW e G e W (.5) α GW GW α W GW GW W GW σ G W (. (.6) Q A ) (.7) GW W G Q H B E H S. (.8) ( ) ( ) S S S S S ρs H E ρ B S S S S, W W W B H ϕ H ϕ τ H ϕ τ S G GS S SS GS W WS GW. (.9) H E ρ B (.0) W, (.a) B H ϕ H ϕ τ H ϕ τ W G GW S SW GS W WW GW. (.b) H S E SρS AS e G H SϕSSτ GS H WϕWSτGW, (.a) H W E W ρw AW e G H SϕSWτ GS H WϕWWτGW, (.b) S H W S, H W (.3) ϕ ρ τ ϕ ρ τ ϕ ϕ ρ ρ τ τ (.) ( ) ( ) SS S GS WW W GW WS SW S W GS GW ( ) ( S E S ϕww ρw τ GW E W ϕws ρs τ GW AS e G ρs ρw τgw ϕsw ϕ WW ), (.5a) ϕ ρ τ ( ϕ ρ τ ) ρ ρ τ ( ϕ ϕ ) W E S SW W GS E W SS S GS AW e G W S GS WS SS. (.5b) Q A ( K e K e K e ) S S S G G W W S S (.6) K G G [ ρwτgw( ϕsw ϕ WW)]

11 K W ϕswwτ GW, ( ) ( ) KS ϕssτgs ϕwwρwτgw ϕswϕwsρwτgsτ GW (.7a) (.7b) (.7c) τ GW τ GS : τ G G und ϕ SS 0 (.8) S Q S AS σ( KG G KWW KS S) (.0) ( ) ( ) KG G ϕwsρwτ G, K W Wτ G, K S ρ W τ G ϕ WS G, (.) [ ( ρ τ ϕ ρ τ )]. (.) W G WS S G Q H H. (.3) S W WS W S S W ρs ρw H E ϕ ρ τ (.) W S W WS S GW W S Q WS AW ϕws ( τgw e W τgs e S). (.5) Q Q Q. (.6) GW WS W W Q W AW { [( ϕss ρs τgs) ( ϕww τgw) ϕsw ϕws ρs τgs τgw ] e W ϕ τ e ϕ ϕ ρ τ e. [ ( ) ] WS S GS S WS SS S GS G G W Q GW AW {[ ( ϕws ϕss) ρ Sτ GS] G e G α ρ τ ϕ α ρ τ ϕ e [ ( ) ] GW S GS SS GS S GW WS W } }. (.7) (.8) S Q GS AS {[ ( ϕsw ϕww) ρw τgw ] G e G α ρ τ ϕ α ρ τ ϕ e [ ( ) ] GS W GW WW GW W GS SW S }. (.9) W S G Q τ WS AW WS σ( W S ) mt WS (.30) G W WS S G Q ( ϕ ρ τ ) GW AW GW σ( G W ) mt GW (.3)

12 G S WS W G Q ( ϕ ρ τ ) GS AS GS σ( G S ) mt GS, (.3) W ( ) WS S GS G G WS GS S S ϕ ρ τ ϕ τ ( ) τ ϕ ρ τ GW WS S GS. (.33) W GW G WS WS S ϕ ϕ GW WS WS. (.3) G GW W WS GS S ϕ ϕ GW WS GS. (.35) [ ] H E ρ A e H ϕ τ H ϕ τ S S S S G S SS GS W WS GW, (.36a) H A e H ϕ τ H ϕ τ W W G S SW GS W WW GW, (.36b) S Q GWS A S σ{ G [ ( ϕsw ϕww ) τgw] G SS GS WW GW SW WS GS GW S [( ϕ τ ) ( ϕ τ ) ϕ ϕ τ τ ] } (.37) ( ) ( ) ϕ ρ τ ϕ τ ϕ ϕ ρ τ τ. (.38) SS S GS WW GS SW WS S GS GW ( ) GWS S GWS σ G S. (.39) Q A ( ϕ τ) S G WS G GWS. (.0) G ϕ WS ( ρ S τ G) τg GWS GS ϕws WS GW. (.) Q W Q S. (.) Q E W ( ) W W W ρw H, Q S SH SE S ρs ( ). (.3) ρ H ρ H ρ E ρ E S W W W S S S W W S. (.) [ ( )] [ ( )] ϕ ρ ρ τ ϕ ϕ H ϕ ρ ρ τ ϕ ϕ H WS S W GW SW WW W SW W S GS WS SS S (.5) ϕ ρ E ϕ ρ E WS S W SW W S.

13 {[ ( ) ] [ ( ) } Q ϕ A SW S W WGS S σ ϕsw ϕww τgw W ϕws ϕss τgs] S, (.6) WS S [ ( SW WW) W GW] SW W [ ( WS SS) S GS (.7) ϕ ϕ ϕ ρ τ ϕ ϕ ϕ ρ τ ] Q A ) (.8) WGS S WGS σ W S ( WGS. (.9) ϕws ϕws ϕws τg S W Q ( E H ), Q S ( SH SE S ) (.50) ρ ρ ( ) WGS S WGS σ S (.5) Q A WGS ϕs τ ϕ τ S S G G S. (.5)

14 Fg..: Mono chromatc Intenty of black radaton Fg..: Spectral fracton of radaton Fg..3: Prncple profle of emvty

15 Fg..: Spectral emvty of alumnum and hte pant Fg..5: Spectral emvty of ome metal

16 Fg..6: Mean emvty of ome metal

17 Fg..7: Spectral emvty of ome refractore Fg..8: Mean emvty of ome refractore

18 Fg..9: Aborptvty of elected materal n dependence on temperature of emttent Fg..0: Spectral tranmon of gla

19 Fg..: Spectral emvty of CO and H O Fg..: Mean emvty of CO

20 Fg..3: Mean emvty of H O emvty 0,6 0,5 0, 0,3 0, , 0 0 0,5,5,5 3 (p CO p HO )* n bar*m Fg..: Emvty of combuton ga of natural ga

21 Fg..5: Emvty of oot Fg..6: Emvty of dut

22 Fg..7: Mean beam length Fg..8: Lambert la Fg..9: Hemphere radaton

23 Fg..0: Radaton beteen to fnte area Fg..: Fg..: Ve factor Fg..3: Radaton exchange beteen element

24 Fg..: Radaton held / h π π emperature n K Fg..5: Radatve heat tranfer coeffcent

25 Fg..6: Meaurng ga temperature nfluenced by encloure Fg..7: Secondary radaton Fg..8: Heat tranfer beteen ga and encloure

26 Fg. -3: emperature dependency of knematc vcoty for organc lqud

27 Fg. -3: hermal phycal properte for mneral ol

Problem #1. Known: All required parameters. Schematic: Find: Depth of freezing as function of time. Strategy:

Problem #1. Known: All required parameters. Schematic: Find: Depth of freezing as function of time. Strategy: BEE 3500 013 Prelm Soluton Problem #1 Known: All requred parameter. Schematc: Fnd: Depth of freezng a functon of tme. Strategy: In thee mplfed analy for freezng tme, a wa done n cla for a lab geometry,

More information

Radiation Chapter 12 L8 (MMV031) Martin Andersson

Radiation Chapter 12 L8 (MMV031) Martin Andersson Radaton Chapter 12 L8 (MMV031) Martn Andersson Contents Thermal Radaton Gas radaton Thermal radaton Thermal radaton s the electromagnetc radaton a body s emttng due to ts temperature electromagnetc radaton

More information

LECTURER: PM DR MAZLAN ABDUL WAHID PM Dr Mazlan Abdul Wahid

LECTURER: PM DR MAZLAN ABDUL WAHID  PM Dr Mazlan Abdul Wahid H E A R A N S F E R HEA RANSFER SME 4463 LECURER: PM DR MAZLAN ABDUL WAHID http://www.fkm.utm.my/~mazlan C H A P E R 3 Dr Mazlan - SME 4463 H E A R A N S F E R Chapter 5 ranent Conducton PM Dr Mazlan Abdul

More information

External Flow: Flow over Bluff Objects (Cylinders, Spheres, Packed Beds) and Impinging Jets

External 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 information

Reading Problems , 15-33, 15-49, 15-50, 15-77, 15-79, 15-86, ,

Reading Problems , 15-33, 15-49, 15-50, 15-77, 15-79, 15-86, , Radiation Heat Transfer Reading Problems 15-1 15-7 15-27, 15-33, 15-49, 15-50, 15-77, 15-79, 15-86, 15-106, 15-107 Introduction The following figure shows the relatively narrow band occupied by thermal

More information

Principles of Food and Bioprocess Engineering (FS 231) Solutions to Example Problems on Heat Transfer

Principles of Food and Bioprocess Engineering (FS 231) Solutions to Example Problems on Heat Transfer Prncples of Food and Boprocess Engneerng (FS 31) Solutons to Example Problems on Heat Transfer 1. We start wth Fourer s law of heat conducton: Q = k A ( T/ x) Rearrangng, we get: Q/A = k ( T/ x) Here,

More information

Radiation Heat Transfer. Introduction. Blackbody Radiation. Definitions ,

Radiation Heat Transfer. Introduction. Blackbody Radiation. Definitions , Radiation Heat Transfer Reading Problems 5-5-7 5-27, 5-33, 5-50, 5-57, 5-77, 5-79, 5-96, 5-07, 5-08 Introduction A narrower band inside the thermal radiation spectrum is denoted as the visible spectrum,

More information

Blackbody radiation. Main radiation laws. Sun as an energy source. Solar spectrum and solar constant.

Blackbody radiation. Main radiation laws. Sun as an energy source. Solar spectrum and solar constant. Lecture 3. lackbody radiation. Main radiation law. Sun a an energy ource. Solar pectrum and olar contant. Objective:. Concept of a blackbody, thermodynamical equilibrium, and local thermodynamical equilibrium..

More information

Thermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850)

Thermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850) hermal-fluds I Chapter 18 ransent heat conducton Dr. Prmal Fernando prmal@eng.fsu.edu Ph: (850) 410-6323 1 ransent heat conducton In general, he temperature of a body vares wth tme as well as poston. In

More information

Radiation Heat Transfer

Radiation Heat Transfer CM30 ranport I Part II: Heat ranfer Radiation Heat ranfer Profeor Faith Morrion Department of Chemical Engineering Michigan echnological Univerity CM30 ranport Procee and Unit Operation I Part : Heat ranfer

More information

Chapter 7: 17, 20, 24, 25, 32, 35, 37, 40, 47, 66 and 79.

Chapter 7: 17, 20, 24, 25, 32, 35, 37, 40, 47, 66 and 79. hapter 7: 17, 0,, 5,, 5, 7, 0, 7, 66 and 79. 77 A power tranitor mounted on the wall diipate 0.18 W. he urface temperature of the tranitor i to be determined. Aumption 1 Steady operating condition exit.

More information

Numerical Transient Heat Conduction Experiment

Numerical Transient Heat Conduction Experiment Numercal ransent Heat Conducton Experment OBJECIVE 1. o demonstrate the basc prncples of conducton heat transfer.. o show how the thermal conductvty of a sold can be measured. 3. o demonstrate the use

More information

Radiation Heat Transfer. Introduction. Blackbody Radiation

Radiation Heat Transfer. Introduction. Blackbody Radiation Radiation Heat Transfer Reading Problems 21-1 21-6 21-21, 21-24, 21-41, 21-61, 21-69 22-1 21-5 22-11, 22-17, 22-26, 22-36, 22-71, 22-72 Introduction It should be readily apparent that radiation heat transfer

More information

CHAPTER X PHASE-CHANGE PROBLEMS

CHAPTER X PHASE-CHANGE PROBLEMS Chapter X Phae-Change Problem December 3, 18 917 CHAPER X PHASE-CHANGE PROBLEMS X.1 Introducton Clacal Stefan Problem Geometry of Phae Change Problem Interface Condton X. Analytcal Soluton for Soldfcaton

More information

Physics 3 (PHYF144) Chap 2: Heat and the First Law of Thermodynamics System. Quantity Positive Negative

Physics 3 (PHYF144) Chap 2: Heat and the First Law of Thermodynamics System. Quantity Positive Negative Physcs (PHYF hap : Heat and the Frst aw of hermodynamcs -. Work and Heat n hermodynamc Processes A thermodynamc system s a system that may exchange energy wth ts surroundngs by means of heat and work.

More information

1. Basic introduction to electromagnetic field. wave properties and particulate properties.

1. Basic introduction to electromagnetic field. wave properties and particulate properties. Lecture Baic Radiometric Quantitie. The Beer-Bouguer-Lambert law. Concept of extinction cattering plu aborption and emiion. Schwarzchild equation. Objective:. Baic introduction to electromagnetic field:

More information

Types of Heat Transfer

Types of Heat Transfer ype of Heat ranfer * Dvz Dt x k d dx v S * * v Gr z HH vap lat uject in the coure conduction (Fourier Law) forced convection (due to flow) ource term free convection (fluid motion due to denity variation

More information

= (fundamental constants c 0, h, k ). (1) k

= (fundamental constants c 0, h, k ). (1) k Introductory Physics Laboratory, Faculty of Physics and Geosciences, University of Leipzig W 12e Radiation Thermometers Tasks 1 Measure the black temperature T s of a glowing resistance wire at eight different

More information

Lab 2e Thermal System Response and Effective Heat Transfer Coefficient

Lab 2e Thermal System Response and Effective Heat Transfer Coefficient 58:080 Expermental Engneerng 1 OBJECTIVE Lab 2e Thermal System Response and Effectve Heat Transfer Coeffcent Warnng: though the experment has educatonal objectves (to learn about bolng heat transfer, etc.),

More information

J.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.

J.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 information

B. X : in phase; Y: out of phase C. X : out of phase; Y: in phase D. X : out of phase; Y: out of phase

B. X : in phase; Y: out of phase C. X : out of phase; Y: in phase D. X : out of phase; Y: out of phase 2015 April 24 Exam 3 Physics 106 Circle the letter of the single best answer. Each question is worth 1 point Physical Constants: proton charge = e = 1.60 10 19 C proton mass = m p = 1.67 10 27 kg electron

More information

Types of Heat Transfer

Types of Heat Transfer Type of Heat Tranfer Dv Dt x = k dt dx v T S 2 * * ( v GrT * z = + z H vap lat uject in the coure conduction (Fourier Law forced convection (due to flow ource term free convection (fluid motion due to

More information

NEUTRON FLUX IN THE EXPOSURE ROOM OF THE TRIGA MARK II REACTOR IN LJUBLJANA

NEUTRON FLUX IN THE EXPOSURE ROOM OF THE TRIGA MARK II REACTOR IN LJUBLJANA Internatonal Conference Nuclear Energy n Central Europe 2000 Golf Hotel, Bled, Slovena, September 11-14, 2000 NEUTRON FLUX IN THE EXPOSURE ROOM OF THE TRIGA MARK II REACTOR IN LJUBLJANA Edvard S. Krštof

More information

High-resolution study of Gamow- Teller transitions in pf-shell nuclei. Tatsuya ADACHI

High-resolution study of Gamow- Teller transitions in pf-shell nuclei. Tatsuya ADACHI High-resolution study of Gamow- Teller transitions in pf-shell nuclei Tatsuya ADACHI Type II supernova Electron Capture (EC) & β decay Neutrino induced reaction A Z-1X N+1 daughter EC β A ZX N parent (A,Z)

More information

Heriot-Watt University

Heriot-Watt University Heriot-Watt University Distinctly Global www.hw.ac.uk Thermodynamics By Peter Cumber Prerequisites Interest in thermodynamics Some ability in calculus (multiple integrals) Good understanding of conduction

More information

INFRAMET. 2.1 Basic laws

INFRAMET. 2.1 Basic laws tel: 048 60844873, fax 48 6668780. Basic laws.. Planck law All objects above the temperature of absolute zero emit thermal radiation due to thermal motion of the atoms and the molecules. The hotter they

More information

3.185 Problem Set 6. Radiation, Intro to Fluid Flow. Solutions

3.185 Problem Set 6. Radiation, Intro to Fluid Flow. Solutions 3.85 Proble Set 6 Radiation, Intro to Fluid Flow Solution. Radiation in Zirconia Phyical Vapor Depoition (5 (a To calculate thi viewfactor, we ll let S be the liquid zicronia dic and S the inner urface

More information

Autumn 2005 THERMODYNAMICS. Time: 3 Hours

Autumn 2005 THERMODYNAMICS. Time: 3 Hours CORK INSTITUTE OF TECHNOOGY Bachelor of Engineering (Honours) in Mechanical Engineering Stage 3 (Bachelor of Engineering in Mechanical Engineering Stage 3) (NFQ evel 8) Autumn 2005 THERMODYNAMICS Time:

More information

Conduction Heat transfer: Unsteady state

Conduction Heat transfer: Unsteady state Conduction Heat tranfer: Unteady tate Chapter Objective For olving the ituation that Where temperature do not change with poition. In a imple lab geometry where temperature vary alo with poition. Near

More information

5 questions, 3 points each, 15 points total possible. 26 Fe Cu Ni Co Pd Ag Ru 101.

5 questions, 3 points each, 15 points total possible. 26 Fe Cu Ni Co Pd Ag Ru 101. Physical Chemistry II Lab CHEM 4644 spring 2017 final exam KEY 5 questions, 3 points each, 15 points total possible h = 6.626 10-34 J s c = 3.00 10 8 m/s 1 GHz = 10 9 s -1. B= h 8π 2 I ν= 1 2 π k μ 6 P

More information

ME 315 Exam 3 8:00-9:00 PM Thursday, April 16, 2009 CIRCLE YOUR DIVISION

ME 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 information

7.2 Sublimation. The following assumptions are made in order to solve the problem: Sublimation Over a Flat Plate in a Parallel Flow

7.2 Sublimation. The following assumptions are made in order to solve the problem: Sublimation Over a Flat Plate in a Parallel Flow 7..1 Sublimation Over a Flat Plate in a Parallel Flow The following assumptions are made in order to solve the problem: 1.. 3. The flat plate is very thin and so the thermal resistance along the flat plate

More information

Speed of light c = m/s. x n e a x d x = 1. 2 n+1 a n π a. He Li Ne Na Ar K Ni 58.

Speed of light c = m/s. x n e a x d x = 1. 2 n+1 a n π a. He Li Ne Na Ar K Ni 58. Physical Chemistry II Test Name: KEY CHEM 464 Spring 18 Chapters 7-11 Average = 1. / 16 6 questions worth a total of 16 points Planck's constant h = 6.63 1-34 J s Speed of light c = 3. 1 8 m/s ħ = h π

More information

2010 Black Engineering Building, Department of Mechanical Engineering. Iowa State University, Ames, IA, 50011

2010 Black Engineering Building, Department of Mechanical Engineering. Iowa State University, Ames, IA, 50011 Interface Energy Couplng between -tungsten Nanoflm and Few-layered Graphene Meng Han a, Pengyu Yuan a, Jng Lu a, Shuyao S b, Xaolong Zhao b, Yanan Yue c, Xnwe Wang a,*, Xangheng Xao b,* a 2010 Black Engneerng

More information

Lecture 3 Basic radiometric quantities.

Lecture 3 Basic radiometric quantities. Lecture 3 Baic radiometric quantitie. The Beer-Bouguer-Lambert law. Concept of extinction cattering plu aborption and emiion. Schwarzchild equation.. Baic introduction to electromagnetic field: Definition,

More information

Half Cell / redox potentials. Context. Task. Evaluation

Half Cell / redox potentials. Context. Task. Evaluation Half Cell / redox potentials Context Students often struggle when asked to apply redox potentials and to combine reduction half equations correctly. This activity aims to involve all the individuals in

More information

11. Advanced Radiation

11. Advanced Radiation . Advanced adiation. Gray Surfaces The gray surface is a medium whose monochromatic emissivity ( λ does not vary with wavelength. The monochromatic emissivity is defined as the ratio of the monochromatic

More information

ECE 6340 Intermediate EM Waves. Fall Prof. David R. Jackson Dept. of ECE. Notes 1

ECE 6340 Intermediate EM Waves. Fall Prof. David R. Jackson Dept. of ECE. Notes 1 EE 6340 Intermediate EM Waves Fall 2016 Prof. David R. Jackson Dept. of EE Notes 1 1 Maxwell s Equations E D rt 2, V/m, rt, Wb/m T ( ) [ ] ( ) ( ) 2 rt, /m, H ( rt, ) [ A/m] B E = t (Faraday's Law) D H

More information

(C) Pavel Sedach and Prep101 1

(C) Pavel Sedach and Prep101 1 (C) Pavel Sedach and Prep101 1 (C) Pavel Sedach and Prep101 1 (C) Pavel Sedach and Prep101 2 (C) Pavel Sedach and Prep101 2 (C) Pavel Sedach and Prep101 3 (C) Pavel Sedach and Prep101 3 (C) Pavel Sedach

More information

2.7 Aerosols and coagulation

2.7 Aerosols and coagulation 1 Note on 1.63 Advanced Environmental Fluid Mechanic Intructor: C. C. Mei, 1 ccmei@mit.edu, 1 617 53 994 December 1,.7 Aerool and coagulation [Ref]: Preent, Kinetic Theory of Gae Fuch, Mechanic of Aerool

More information

02/05/09 Last 4 Digits of USC ID: Dr. Jessica Parr

02/05/09 Last 4 Digits of USC ID: Dr. Jessica Parr Chemistry 05 B First Letter of PLEASE PRINT YOUR NAME IN BLOCK LETTERS Exam last Name Name: 02/05/09 Last 4 Digits of USC ID: Dr. Jessica Parr Lab TA s Name: Question Points Score Grader 2 2 9 3 9 4 2

More information

Termisk Strålning; Thermal radiation

Termisk Strålning; Thermal radiation Termsk Strålnng; Thermal radaton Termsk strålnng är den elektromagnetska strålnng som en kropp emtterar p.g.a. sn temperatur. Thermal radaton s the electromagnetc radaton a body s emttng due to ts temperature

More information

CHEM 4641 Fall questions worth a total of 32 points. Show your work, except on multiple-choice questions. 1 V α=

CHEM 4641 Fall questions worth a total of 32 points. Show your work, except on multiple-choice questions. 1 V α= Physical Chemistry I Final Exam Name: KEY CHEM 4641 Fall 017 15 questions worth a total of 3 points. Show your work, except on multiple-choice questions. 1 V 1 V α= κt = V T P V P T Gas constant R = 8.314

More information

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 10 August 2005

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 10 August 2005 ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER 0 August 2005 Final Examination R. Culham & M. Bahrami This is a 2 - /2 hour, closed-book examination. You are permitted to use one 8.5 in. in. crib

More information

V. Electrostatics. Lecture 25: Diffuse double layer structure

V. Electrostatics. Lecture 25: Diffuse double layer structure V. Electrostatcs Lecture 5: Dffuse double layer structure MIT Student Last tme we showed that whenever λ D L the electrolyte has a quas-neutral bulk (or outer ) regon at the geometrcal scale L, where there

More information

Geometrical Optics Mirrors and Prisms

Geometrical Optics Mirrors and Prisms Phy 322 Lecture 4 Chapter 5 Geometrcal Optc Mrror and Prm Optcal bench http://webphyc.davdon.edu/applet/optc4/default.html Mrror Ancent bronze mrror Hubble telecope mrror Lqud mercury mrror Planar mrror

More information

PORE STRUCTURE AND THERMAL CONDUCTIVITY OF BURNT CLAY BRICKS INTRODUCTION

PORE STRUCTURE AND THERMAL CONDUCTIVITY OF BURNT CLAY BRICKS INTRODUCTION PORE STRUCTURE AND THERMAL CONDUCTIVITY OF BURNT CLAY BRICKS Olga Koronthalyova, Peter Matasovsky Insttute of Constructon and Archtecture, Slovak Academy of Scences, Dubravska 9, 845 43 Bratslava, Slovaka.

More information

Chapter 11 FUNDAMENTALS OF THERMAL RADIATION

Chapter 11 FUNDAMENTALS OF THERMAL RADIATION Chapter Chapter Fundamentals of Thermal Radiation FUNDAMENTALS OF THERMAL RADIATION Electromagnetic and Thermal Radiation -C Electromagnetic waves are caused by accelerated charges or changing electric

More information

Formal solvers of the RT equation

Formal solvers of the RT equation Formal solvers of the RT equaton Formal RT solvers Runge- Kutta (reference solver) Pskunov N.: 979, Master Thess Long characterstcs (Feautrer scheme) Cannon C.J.: 970, ApJ 6, 55 Short characterstcs (Hermtan

More information

8. Relax and do well.

8. Relax and do well. CHEM 34.02 and 34.03 Name Exam III John III. Gelder TA's Name November 5, 2000 Lab Section INSTRUCTIONS:. This examination consists of a total of 9 different pages. The last three pages include a periodic

More information

Numerical Heat and Mass Transfer

Numerical Heat and Mass Transfer Master Degree in Mechanical Engineering Numerical Heat and Mass Transfer 11-Radiative Heat Transfer Fausto Arpino f.arpino@unicas.it Nature of Thermal Radiation ü Thermal radiation refers to radiation

More information

REVIEW QUESTIONS Chapter 19

REVIEW QUESTIONS Chapter 19 Chemistry 10 ANSWER KEY REVIEW QUESTIONS Chapter 19 1. For each of the following unbalanced equations, (i) write the half-reactions for oxidation and reduction, and (ii) balance the overall equation in

More information

T h e C S E T I P r o j e c t

T h e C S E T I P r o j e c t T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T

More information

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng

More information

HEAT TRANSFER THROUGH ANNULAR COMPOSITE FINS

HEAT TRANSFER THROUGH ANNULAR COMPOSITE FINS Journal of Mechancal Engneerng and Technology (JMET) Volume 4, Issue 1, Jan-June 2016, pp. 01-10, Artcle ID: JMET_04_01_001 Avalable onlne at http://www.aeme.com/jmet/ssues.asp?jtype=jmet&vtype=4&itype=1

More information

Level 7 Post Graduate Diploma in Engineering Heat and mass transfer

Level 7 Post Graduate Diploma in Engineering Heat and mass transfer 9210-221 Level 7 Post Graduate Diploma in Engineering Heat and mass transfer 0 You should have the following for this examination one answer book non programmable calculator pen, pencil, drawing instruments

More information

Chemistry 431 Practice Final Exam Fall Hours

Chemistry 431 Practice Final Exam Fall Hours Chemistry 431 Practice Final Exam Fall 2018 3 Hours R =8.3144 J mol 1 K 1 R=.0821 L atm mol 1 K 1 R=.08314 L bar mol 1 K 1 k=1.381 10 23 J molecule 1 K 1 h=6.626 10 34 Js N A = 6.022 10 23 molecules mol

More information

Element Cube Project (x2)

Element Cube Project (x2) Element Cube Project (x2) Background: As a class, we will construct a three dimensional periodic table by each student selecting two elements in which you will need to create an element cube. Helpful Links

More information

Goal: The theory behind the electromagnetic radiation in remote sensing. 2.1 Maxwell Equations and Electromagnetic Waves

Goal: The theory behind the electromagnetic radiation in remote sensing. 2.1 Maxwell Equations and Electromagnetic Waves Chapter 2 Electromagnetic Radiation Goal: The theory behind the electromagnetic radiation in remote sensing. 2.1 Maxwell Equations and Electromagnetic Waves Electromagnetic waves do not need a medium to

More information

If anything confuses you or is not clear, raise your hand and ask!

If anything confuses you or is not clear, raise your hand and ask! CHM 1045 Dr. Light s Section December 10, 2002 FINAL EXAM Name (please print) Recitation Section Meeting Time This exam consists of six pages. Make sure you have one of each. Print your name at the top

More information

Numerical Heat and Mass Transfer

Numerical Heat and Mass Transfer Master Degree in Mechanical Engineering Numerical Heat and Mass Transfer 15-Convective Heat Transfer Fausto Arpino f.arpino@unicas.it Introduction In conduction problems the convection entered the analysis

More information

True/False. Circle the correct answer. (1pt each, 7pts total) 3. Radiation doesn t occur in materials that are transparent such as gases.

True/False. Circle the correct answer. (1pt each, 7pts total) 3. Radiation doesn t occur in materials that are transparent such as gases. ME 323 Sample Final Exam. 120pts total True/False. Circle the correct answer. (1pt each, 7pts total) 1. A solid angle of 2π steradians defines a hemispherical shell. T F 2. The Earth irradiates the Sun.

More information

If there is convective heat transfer from outer surface to fluid maintained at T W.

If there is convective heat transfer from outer surface to fluid maintained at T W. Heat Transfer 1. What are the different modes of heat transfer? Explain with examples. 2. State Fourier s Law of heat conduction? Write some of their applications. 3. State the effect of variation of temperature

More information

Lab Day and Time: Instructions. 1. Do not open the exam until you are told to start.

Lab Day and Time: Instructions. 1. Do not open the exam until you are told to start. Name: Lab Day and Time: Instructions 1. Do not open the exam until you are told to start. 2. This exam is closed note and closed book. You are not allowed to use any outside material while taking this

More information

Lecture 3. Interaction of radiation with surfaces. Upcoming classes

Lecture 3. Interaction of radiation with surfaces. Upcoming classes Radaton transfer n envronmental scences Lecture 3. Interacton of radaton wth surfaces Upcomng classes When a ray of lght nteracts wth a surface several nteractons are possble: 1. It s absorbed. 2. It s

More information

ME 315 Final Examination Solution 8:00-10:00 AM Friday, May 8, 2009 CIRCLE YOUR DIVISION

ME 315 Final Examination Solution 8:00-10:00 AM Friday, May 8, 2009 CIRCLE YOUR DIVISION ME 315 Final Examination Solution 8:00-10:00 AM Friday, May 8, 009 This is a closed-book, closed-notes examination. There is a formula sheet at the back. You must turn off all communications devices before

More information

Statistical and Thermal Physics. Problem Set 5

Statistical and Thermal Physics. Problem Set 5 Statistical and Thermal Physics xford hysics Second year physics course Dr A. A. Schekochihin and Prof. A. T. Boothroyd (with thanks to Prof. S. J. Blundell Problem Set 5 Some useful constants Boltzmann

More information

Advanced Heat and Mass Transfer by Amir Faghri, Yuwen Zhang, and John R. Howell

Advanced Heat and Mass Transfer by Amir Faghri, Yuwen Zhang, and John R. Howell Advanced Heat and Mass Transfer by Amir Faghri, Yuwen Zhang, and John R. Howell 9.2 The Blackbody as the Ideal Radiator A material that absorbs 100 percent of the energy incident on it from all directions

More information

Spin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia

Spin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia Commun. Theor. Phys. (Beijing, China) 43 (005) pp. 709 718 c International Academic Publishers Vol. 43, No. 4, April 15, 005 Spin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia

More information

Hierarchical Modeling for Univariate Spatial Data

Hierarchical Modeling for Univariate Spatial Data Hierarchical Modeling for Univariate Spatial Data Geography 890, Hierarchical Bayesian Models for Environmental Spatial Data Analysis February 15, 2011 1 Spatial Domain 2 Geography 890 Spatial Domain This

More information

CHE 226 ANALYTICAL CHEMISTRY Spring 2005

CHE 226 ANALYTICAL CHEMISTRY Spring 2005 CHE 226 ANALYTICAL CHEMISTRY EXAM II March 10, 2005 Name WRITE YOUR NAME ON EACH EXAM PAGE NOW. THERE ARE 10 QUESTIONS AND 109 POINTS TOTAL IN THIS EXAM. Show clearly all work on these pages. Use the proper

More information

Last 4 Digits of USC ID:

Last 4 Digits of USC ID: Chemistry 05 B Practice Exam Dr. Jessica Parr First Letter of last Name PLEASE PRINT YOUR NAME IN BLOCK LETTERS Name: Last 4 Digits of USC ID: Lab TA s Name: Question Points Score Grader 8 2 4 3 9 4 0

More information

Greenhouse Steady State Energy Balance Model

Greenhouse Steady State Energy Balance Model Greenhouse Steady State Energy Balance Model The energy balance for the greenhouse was obtained by applying energy conservation to the greenhouse system as a control volume and identifying the energy terms.

More information

Investigations of hot water temperature changes at the pipe outflow

Investigations of hot water temperature changes at the pipe outflow Investigations of hot water temperature changes at the pipe outflow Janusz Wojtkowiak 1,*, and Czesław Oleśkowicz-Popiel 1 1 Poznan University of Technology, Faculty of Civil and Environmental Engineering,

More information

Radiometric Dating (tap anywhere)

Radiometric Dating (tap anywhere) Radiometric Dating (tap anywhere) Protons Neutrons Electrons Elements on the periodic table are STABLE Elements can have radioactive versions of itself called ISOTOPES!! Page 1 in your ESRT has your list!

More information

TFAWS 2005 Short Course

TFAWS 2005 Short Course C&R ECHNOLOGIES FAWS 005 Short Course Non-Grey and emperature Dependent Radiation Analysis Methods im Panczak Additional Charts & Data Provided by Dan Green Ball Aerospace Corporation djgreen@ball.com

More information

s f o r s o l v i n g t h e n o n l i n

s f o r s o l v i n g t h e n o n l i n M M R M q q D O : q 7 8 q q q M q x- q M M M 9 R R D O : 78 / x q D MO : M 7 9 8 / D q P F x z M q M q D T P - z P G S F q q q q q q q D q q PZ w - z q - P q q q w q q q w q q w z q - w P w q w w - w w

More information

University of Rome Tor Vergata

University of Rome Tor Vergata University of Rome Tor Vergata Faculty of Engineering Department of Industrial Engineering THERMODYNAMIC AND HEAT TRANSFER HEAT TRANSFER dr. G. Bovesecchi gianluigi.bovesecchi@gmail.com 06-7259-727 (7249)

More information

Very Large Hadron Collider - phase 2 Optimization of the beam screen cooling & Impact of the photon stop on the cryogenic system

Very Large Hadron Collider - phase 2 Optimization of the beam screen cooling & Impact of the photon stop on the cryogenic system Very Large Hadron Collider - phase 2 Optimization of the beam screen cooling & Impact of the photon stop on the cryogenic system VLHC workshop on the beam tube vacuum Saturday June 23, 21 - Christine Darve

More information

Solutions and Ions. Pure Substances

Solutions and Ions. Pure Substances Class #4 Solutions and Ions CHEM 107 L.S. Brown Texas A&M University Pure Substances Pure substance: described completely by a single chemical formula Fixed composition 1 Mixtures Combination of 2 or more

More information

FI 3221 ELECTROMAGNETIC INTERACTIONS IN MATTER

FI 3221 ELECTROMAGNETIC INTERACTIONS IN MATTER 6/0/06 FI 3 ELECTROMAGNETIC INTERACTION IN MATTER Alexander A. Ikandar Phyic of Magnetim and Photonic CATTERING OF LIGHT Rayleigh cattering cattering quantitie Mie cattering Alexander A. Ikandar Electromagnetic

More information

Atoms and the Periodic Table

Atoms and the Periodic Table Atoms and the Periodic Table Parts of the Atom Proton Found in the nucleus Number of protons defines the element Charge +1, mass 1 Parts of the Atom Neutron Found in the nucleus Stabilizes the nucleus

More information

Convection and conduction and lumped models

Convection and conduction and lumped models MIT Hea ranfer Dynamc mdel 4.3./SG nvecn and cndcn and lmped mdel. Hea cnvecn If we have a rface wh he emperare and a rrndng fld wh he emperare a where a hgher han we have a hea flw a Φ h [W] () where

More information

CHEM 107 (Spring-2005) Exam 3 (100 pts)

CHEM 107 (Spring-2005) Exam 3 (100 pts) CHEM 107 (Spring-2005) Exam 3 (100 pts) Name: ------------------------------------------------------------------------, Clid # ------------------------------ LAST NAME, First (Circle the alphabet segment

More information

Chem Exam 1. September 26, Dr. Susan E. Bates. Name 9:00 OR 10:00

Chem Exam 1. September 26, Dr. Susan E. Bates. Name 9:00 OR 10:00 Chem 1711 Exam 1 September 26, 2013 Dr. Susan E. Bates Name 9:00 OR 10:00 N A = 6.022 x 10 23 mol 1 I A II A III B IV B V B VI B VII B VIII I B II B III A IV A V A VI A VII A inert gases 1 H 1.008 3 Li

More information

Band-bending. EE 436 band-bending 1

Band-bending. EE 436 band-bending 1 Band-bending In the p-n junction and BJT, we saw that the semiconductor band edges were bent in the depletion layers. We used the depletion approximation and Poisson s equation to relate the band-bending

More information

INSTRUCTIONS: Exam III. November 10, 1999 Lab Section

INSTRUCTIONS: Exam III. November 10, 1999 Lab Section CHEM 1215 Exam III John III. Gelder November 10, 1999 Name TA's Name Lab Section INSTRUCTIONS: 1. This examination consists of a total of 7 different pages. The last page includes a periodic table and

More information

Chem GENERAL CHEMISTRY I MIDTERM EXAMINATION

Chem GENERAL CHEMISTRY I MIDTERM EXAMINATION Concordia University CHEM 205 Fall 2009, B LAST NAME: FIRST NAME: STUDENT ID: Chem 205 - GENERAL CHEMISTRY I MIDTERM EXAMINATION PLEASE READ THIS BOX WHILE WAITING TO START INSTRUCTIONS: Calculators are

More information

INFLUENCE OF SURFACE EMISSIVITY AND OF LOW EMISSIVITY SHIELDS ON THE THERMAL PROPERTIES OF LOW DENSITY INSULATING MATERIALS

INFLUENCE OF SURFACE EMISSIVITY AND OF LOW EMISSIVITY SHIELDS ON THE THERMAL PROPERTIES OF LOW DENSITY INSULATING MATERIALS 8th International Conference on Heat Transfer, Fluid Mechanics and Thermodynamics HEFAT2011 8 th International Conference on Heat Transfer, Fluid Mechanics and Thermodynamics 11 13 July 2011 Pointe Aux

More information

123MEAN thermal properties KATEDRA MATERIÁLOVÉHO INŽENÝRSTVÍ A CHEMIE

123MEAN thermal properties KATEDRA MATERIÁLOVÉHO INŽENÝRSTVÍ A CHEMIE 123MEAN thermal properties KATEDRA MATERIÁLOVÉHO INŽENÝRSTVÍ A CHEMIE Heat transport in substances: conduction transfer of kinetic energy on the bases of disorded movement of molecules. Own heat transfer

More information

Oxidation Numbers, ox #

Oxidation Numbers, ox # Oxidation Numbers, ox # are or numbers assigned to each or assuming that the are transferred from the electronegative element to the electronegative element. now mimic systems. ox # are written followed

More information

Advanced Heat and Mass Transfer by Amir Faghri, Yuwen Zhang, and John R. Howell

Advanced Heat and Mass Transfer by Amir Faghri, Yuwen Zhang, and John R. Howell Heat Transfer Heat transfer rate by conduction is related to the temperature gradient by Fourier s law. For the one-dimensional heat transfer problem in Fig. 1.8, in which temperature varies in the y-

More information

8. Relax and do well.

8. Relax and do well. CHEM 1215 Exam III John III. Gelder November 11, 1998 Name TA's Name Lab Section INSTRUCTIONS: 1. This examination consists of a total of 7 different pages. The last page includes a periodic table and

More information

Fundamental Concepts of Radiation -Basic Principles and Definitions- Chapter 12 Sections 12.1 through 12.3

Fundamental Concepts of Radiation -Basic Principles and Definitions- Chapter 12 Sections 12.1 through 12.3 Fundamental Concepts of Radiation -Basic Principles and Definitions- Chapter 1 Sections 1.1 through 1.3 1.1 Fundamental Concepts Attention is focused on thermal radiation, whose origins are associated

More information

ELECTROCHEMISTRY. these are systems involving oxidation or reduction there are several types METALS IN CONTACT WITH SOLUTIONS OF THEIR IONS

ELECTROCHEMISTRY. these are systems involving oxidation or reduction there are several types METALS IN CONTACT WITH SOLUTIONS OF THEIR IONS Electrochemistry 1 ELECTROCHEMISTRY REDOX Reduction gain of electrons Cu 2+ (aq) + 2e > Cu(s) Oxidation removal of electrons Zn(s) > Zn 2+ (aq) + 2e HALF CELLS these are systems involving oxidation or

More information

Radiative heat transfer

Radiative heat transfer Radiative heat transfer 22 mars 2017 Energy can be transported by the electromagnetic field radiated by an object at finite temperature. A very important example is the infrared radiation emitted towards

More information

Transient Heat Transfer Experiment. ME 331 Introduction to Heat Transfer. June 1 st, 2017

Transient Heat Transfer Experiment. ME 331 Introduction to Heat Transfer. June 1 st, 2017 Transient Heat Transfer Experiment ME 331 Introduction to Heat Transfer June 1 st, 2017 Abstract The lumped capacitance assumption for transient conduction was tested for three heated spheres; a gold plated

More information

MODULE 2: Worked-out Problems

MODULE 2: Worked-out Problems MODUE : Worked-out Problems Problem : he steady-state temperature dstrbuton n a one dmensonal wall of thermal conductvty 5W/m and thckness 5 mm s observed to be ( C) abx, where a C, B- c/ m, and x n meters

More information

"INDEPENDENT IN AI.L THINOS. NEUTRAI. IN NOTHINO' LOWELL, MICHIGAN, JAM AHV, 19, WHOLE NO. 290.

INDEPENDENT IN AI.L THINOS. NEUTRAI. IN NOTHINO' LOWELL, MICHIGAN, JAM AHV, 19, WHOLE NO. 290. > HS U H V V 8 W HG J HV 9 899 WH 29 H G S J G W W W WS 4 5 6 898 K H q $ U S S U G 8 G H - J W U S G Y K - «H - W S HW W»U W 8 W H WS H G U Y Y J H q x U 2 VV GV W H W H G 8 H S G K W W W H J? 5? G S-

More information

PROBLEM Node 5: ( ) ( ) ( ) ( )

PROBLEM Node 5: ( ) ( ) ( ) ( ) PROBLEM 4.78 KNOWN: Nodal network and boundary conditions for a water-cooled cold plate. FIND: (a) Steady-state temperature distribution for prescribed conditions, (b) Means by which operation may be extended

More information