1D STEADY STATE HEAT
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1 D SEADY SAE HEA CONDUCION () Pabal alukda Aociate Pofeo Depatment of Mecanical Engineeing II Deli Palukda/Mec-IID
2 emal Contact eitance empeatue ditibution and eat flow line along two olid plate peed againt eac ote fo te cae of pefect and impefect contact Palukda/Mec-IID
3 Conide eat tanfe toug two metal od of co-ectional aea A tat ae peed againt eac ote. Heat tanfe toug te inteface of tee two od i te um of te eat tanfe toug te olid contact pot and te gap in te noncontact aea and can be expeed a Q Q Q contact Q gap A Δ c int eface Mot expeimentally detemined value of te temal contact eitance fall between and m C/W (te coeponding ange of temal contact conductance i 000 to 00,000 W/m C). wee A i te appaent inteface aea (wic i te ame a te co- ectional aea of te od) and Δ inteface i te effective tempeatue diffeence at te inteface. e quantity c, wic coepond to te convection eat tanfe coefficient, i called te temal contact conductance and i expeed a eface It i elated to temal contact eitance by Palukda/Mec-IID c c Q Δ A int (W/m o C) Δ int eface (m o C/W) c Q A
4 Impotance of conideation e temal contact t eitance ange: between and m C/W Palukda/Mec-IID
5 wo paallel laye wo paallel laye ) ( Q Q Q total Q ' A k ' A k Palukda/Mec-IID total total wee
6 Combined eie-paallel Q total total 3 conv 3 conv ' ' k A k A 3 3 ' k A 3 3 conv A 3 Palukda/Mec-IID
7 Seie and paallel compoite wall and it temal cicuit D A C E B F C A B D E F 3 4 Q UA Δ (W) Palukda/Mec-IID wee U i te oveall eat tanfe coefficient UA total
8 Complex multi-dimenional poblem a -D poblem. Any plane wall nomal to te x-axi i iotemal. Any plane paallel to x-axi i adiabatic Palukda/Mec-IID
9 Heat conduction in cylinde Q cond, cyl ka d d A π Qcond,cyl d A kd Subtituting A π and pefoming te integation give Q cond,cyl πk ln( ) Q cond,cyl contant at teady tate Q cond,cyl cyl (W) Palukda/Mec-IID cyl ln( πk ) ln(oute adiu/inne adiu) π(lengt)(temal conductivity)
10 Heat conduction in pee Fo pee Q& cond,pee p p 4π k oute adiu - inne adiu 4π(oute adiu)(inne adiu)(temal conductivity) Palukda/Mec-IID
11 eitance Netwok cylindical total conv, cond conv, ln ( ) ( π ) π k ( π ) peical total conv, p conv, ( 4 π ) 4 π k ( 4 π ) e temal eitance netwok fo a cylindical (o peical) ell ubjected to convection fom bot te inne and te oute ide. Palukda/Mec-IID
12 Multilayeed cylinde total conv, cyl, cyl, cyl,3 conv, Palukda/Mec-IID ln ( ) ln ( ) ln ( ) A π k π k π k 3 A 4
13 adial eat conduction toug cylindical ytem k. φ k. φ k. z z g& ρc t d d d d 0 Integating te above equation twice, C ln C Subject to te bounday condition, at and at () ln ln ln ln ln Palukda/Mec-IID
14 C d C. k. d d ka Q π π ln )..( k. Q π ln ) k( Palukda/Mec-IID
15 Citical adiu of Inulation. Steady tate condition. One-dimenional eat flow only in te adial diection 3. Negligible temal eitance due to cylinde wall 4. Negligible adiation excange between oute uface of inulation and uounding Inulation, in wall Palukda/Mec-IID
16 Citical adiu of Inulation Pactically, it tun out tat adding inulation in cylindical and peical expoed wall can initially caue te temal eitance to deceae, teeby inceaing te eat tanfe ate becaue te outide aea fo convection eat tanfe i getting lage. At ome citical tickne, c, te temal eitance inceae again and conequently te eat tanfe i educed. o find an expeion fo c, conide te temal cicuit below fo an inulated cylindical wall wit temal conductivity k: Palukda/Mec-IID Inulation, in wall Q & ( ) ln πk t π
17 An inulated cylindical pipe expoed to convection fom te oute uface and te temal eitance netwok aociated wit it. Palukda/Mec-IID
18 o find c, et te oveall temal eitance d t /d 0 and olve fo : ln( ) i t πk π i inne adiu d d πk t c k π 0 Similaly fo a pee k c Fo inulation tickne le tat c te eat lo inceae wit inceaing and fo inulation tickne geate tat c te eat lo deceae wit inceaing If k 0.03 W/(m K) and 0 W/(m K): k 0.03W/(m K) cylinde c 0.003m 3mm 0W/(m K) pee Palukda/Mec-IID k c 6mm
19 Value of, and k ae contant o ee te condition maximize o minimize te total eitance d d total πk π 3 otal temal eitance pe unit lengt total Heat tanfe pe unit lengt At k/ d π( k ) ln πk π i total Q d total k k 3 πk Alway poitive, total eitance at k/ i minimum k c, cylinde (m) > 0 Optimum tickne i aociated wit, πk π 0 d total d k 0
20 o ( W m C) o ( W m C) k max, inulation 0.05 c,max 0.0m cm 5 min We can inulate ot wate pipe and team line witout woying te citical adiu of inulation Inulation of electic wie: -adiu of electic wie may be malle tan te citical adiu -Addition of inulation mateial inceae eat tanfe Citical adiu of inulation fo peical ell: c, pee k
21 Summay able Palukda/Mec-IID
22 D Conduction wit Heat Geneation Palukda/Mec-IID
23 0 q d 0 k dx ( ) C x C x q x Bounday condition: ( ) C x C x k x y ( ), C,, ( ),,, k q C Palukda/Mec-IID ) (,,,, x x k q x
24 ,, q x ( x ) k q (0) o k dx Put x 0 If te uface tempeatue of te eat geneating body i unknown and te uounding fluid tempeatue i d Find tempeatue gadient Uing enegy balance k x ( ) fom te above Eq. at x We can obtain te uface tempeatue Palukda/Mec-IID q
25 d d d d q k 0 d q d kk C q ( ) C ln C 4kk Bounday condition: d d C Palukda/Mec-IID ( o ) C q o 4k q o ( ) 4k o ( Π o ) (Π o )( ) q q o
1D STEADY STATE HEAT
D SEADY SAE HEA CONDUCION () Prabal alukdar Aociate Profeor Department of Mechanical Engineering II Delhi E-mail: [email protected] Convection Boundary Condition Heat conduction at the urface in a
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The Eence of the Electomagnetic Wave i Not Enegy Zeng Qingping Ai Foce Rada Academy Pofeo cienceum@yahoocn Abtact The cutomay opinion i: electic ave o light ave i enegy, TYang expeiment i the intefeence
BUILT-IN DUAL FREQUENCY ANTENNA WITH AN EMBEDDED CAMERA AND A VERTICAL GROUND PLANE
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Gravitation and Kepler s Laws Newton s Law of Universal Gravitation in vectorial. Gm 1 m 2. r 2
F Gm Gavitation and Keple s Laws Newton s Law of Univesal Gavitation in vectoial fom: F 12 21 Gm 1 m 2 12 2 ˆ 12 whee the hat (ˆ) denotes a unit vecto as usual. Gavity obeys the supeposition pinciple,
Chapter 4. 4.3 Applications of Energy Balance
Capter 4 4. Appliation of Energy Balane We will diu exaple illutrating te analyi of erveral devie of interet in engineering, inluding nozzle and diffuer, turbine, opreor and pup, eat exanger, and trottling
Effects of a Price Decrease. Separating Income and Substitution Effects. Hicks and Slutsky Decompositions. Hicks Substitution and Income Effects
Effect of a Price Decreae Searating Incoe and Subtitution Effect ECON 37: Microeconoic Teor Suer 24 Rice Univerit Stanle Gilbert Can be broken down into two coonent Incoe effect Wen te rice of one good
Do Vibrations Make Sound?
Do Vibations Make Sound? Gade 1: Sound Pobe Aligned with National Standads oveview Students will lean about sound and vibations. This activity will allow students to see and hea how vibations do in fact
Chapter 3 Savings, Present Value and Ricardian Equivalence
Chapte 3 Savings, Pesent Value and Ricadian Equivalence Chapte Oveview In the pevious chapte we studied the decision of households to supply hous to the labo maket. This decision was a static decision,
Lesson 7 Gauss s Law and Electric Fields
Lesson 7 Gauss s Law and Electic Fields Lawence B. Rees 7. You may make a single copy of this document fo pesonal use without witten pemission. 7. Intoduction While it is impotant to gain a solid conceptual
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Viscosity. The popety of viscosity in gas is due to ) Cohesive foces between the moecues ) Coisions between the moecues ) Not having a definite voume ) Not having a definite size. When tempeatue is inceased
The EOQ Inventory Formula
Te EOQ Inventory Formula James M. Cargal Matematics Department Troy University Montgomery Campus A basic problem for businesses and manufacturers is, wen ordering supplies, to determine wat quantity of
Chapter 4: Fluid Kinematics
Oveview Fluid kinematics deals with the motion of fluids without consideing the foces and moments which ceate the motion. Items discussed in this Chapte. Mateial deivative and its elationship to Lagangian
Experiment 6: Centripetal Force
Name Section Date Intoduction Expeiment 6: Centipetal oce This expeiment is concened with the foce necessay to keep an object moving in a constant cicula path. Accoding to Newton s fist law of motion thee
Tangent Lines and Rates of Change
Tangent Lines and Rates of Cange 9-2-2005 Given a function y = f(x), ow do you find te slope of te tangent line to te grap at te point P(a, f(a))? (I m tinking of te tangent line as a line tat just skims
Warm medium, T H T T H T L. s Cold medium, T L
Refrigeration Cycle Heat flows in direction of decreasing temperature, i.e., from ig-temperature to low temperature regions. Te transfer of eat from a low-temperature to ig-temperature requires a refrigerator
STUDENT RESPONSE TO ANNUITY FORMULA DERIVATION
Page 1 STUDENT RESPONSE TO ANNUITY FORMULA DERIVATION C. Alan Blaylock, Hendeson State Univesity ABSTRACT This pape pesents an intuitive appoach to deiving annuity fomulas fo classoom use and attempts
F G r. Don't confuse G with g: "Big G" and "little g" are totally different things.
G-1 Gavity Newton's Univesal Law of Gavitation (fist stated by Newton): any two masses m 1 and m exet an attactive gavitational foce on each othe accoding to m m G 1 This applies to all masses, not just
