hmt 6

2
CONDUCTION THROUGH A CYLINDRICAL WALL Terms Inside radius=r1, outside radius = r2 T inside = Ts1, T outside = Ts2 Length L Assumptions one dimension / without generation / steady state General Heat Equation Cylindrical Coordinates : One Dimension / Without Generation / Steady State d 2 T dr 2 + 1 r dT dr =0 1 r d dr ( r dT dr ) =0 d dr ( r dT dr ) =0 if 1 r 0 Integrating r dT dr = C1 …………….... (i) T=C1 log r + C2………… (ii) Boundary conditions T= Ts1 at r=r1 AND T=Ts2 at r=r2 TEMPERATURE DISTRIBUTION Applying boundary conditions and solving ** Temperature distribution is logarithmic not linear as in plane walls: but almost linear if r 2 / r 11

Upload: manu-gupta

Post on 06-Sep-2015

216 views

Category:

Documents


2 download

DESCRIPTION

HMT 6

TRANSCRIPT

CONDUCTION THROUGH A CYLINDRICAL WALL

TermsInside radius=r1, outside radius = r2T inside = Ts1, T outside = Ts2Length L

Assumptionsone dimension / without generation / steady stateGeneral Heat Equation Cylindrical Coordinates: One Dimension / Without Generation / Steady State

if Integrating

= C1 .... (i)T=C1 log r + C2 (ii)Boundary conditionsT= Ts1 at r=r1 AND T=Ts2 at r=r2

TEMPERATURE DISTRIBUTIONApplying boundary conditions and solving

HEAT FLOW

qr= - kA = -k (2rL)

=

loge = Ts2 - Ts1

Or q = (2kL) =

Where Rt =

** Temperature distribution is logarithmic not linear as in plane walls: but almost linear if

qr= - kAmean = q = (2kL)

Amean =

rmean =