one dimensional models for conduction heat transfer in manufacturing processes p m v subbarao...
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One Dimensional Models for Conduction Heat Transfer in Manufacturing Processes
P M V SubbaraoProfessor
Mechanical Engineering Department
I I T Delhi
Simplified Models for Complex Heat Transfer due to micro-molecular
Movements!!!
Steady-State One-Dimensional Conduction
• For conduction through a large wall the heat equation reduces to one dimensional Equation in Cartesian system .
• Assume a homogeneous medium with invariant thermal conductivity ( k = constant) :
),(2
2
txgx
Tk
t
TC p
One dimensional Transient conduction with heat generation.
21 CxCT
Heat Transfer in Metal Cutting
02
2
2
2
2
2
dz
Td
dy
Td
dx
Tdk
Axi-symmetric Conduction Models for Manufacturing Processes
),,,(1
2tzrg
z
Tk
z
Tk
rr
Tkr
rt
TC p
)(rgr
Tkr
rt
TC p
No changes in T along and z directions:
Steady state with no heat generation :
0
r
Tr
rk 0
r
TkA
rk
Axi-Symmetric Steady Conduction in Radial Systems
0
drdrdT
kAd
Homogeneous and constant property material
0
drdrdT
Ad
At any radial location the surface are for heat conduction in a solid cylinder is:
rlAcylinder 2
At any radial location the surface are for heat conduction in a solid sphere is:
24 rAsphere
The GDE for cylinder:0
drdrdT
rd
The GDE for sphere:0
2
drdrdT
rd
General Solution for Cylinder:
21 ln CrCrT
General Solution for Sphere:
r
CCrT 1
2
0dr
drdT
rd
Boundary Conditions
• No solution exists when r = 0. • Totally solid cylinder or Sphere have no physical
relevance!• Inner wall at finite radius is essential for steady state
conduction with no heat generation.
21 ln CrCrT r
CCrT 1
2
UNSTEADY-STATE HEAT CONDUCTION
Applications where rate/duration of heating/cooling is a Design Parameter……
Welding Process : How to decide the Rate of Welding?
Injection Molding Process
They need you to help them to the time required for a part in a mold to cool to an acceptable temperature for removal.
Resin Transfer Molding Process
(1) Insert fiber preform
(2) Close mold
(3) Inject mixed resin/catalyst
(4) Part solidifies via reaction
(5) Open mold
(6) Remove part
The cycle time for step (4) is approximately the same 25 minutes for parts of all sizes made by AeroForm.
All other molding operations (1), (2), (3), (5) and (6) take a total of 5 minutes.
Selective LASER Sintering
pC
txgT
t
T
),(2
General Conduction Equation
pC
tzyxg
z
T
y
T
x
T
t
T
):,,(
2
2
2
2
2
2
For Cartesian Geometry:
• The general form of these equations in multi-dimensions for homogeneous material is:
Cooling/Quenching of Hot Processed Products
Transient-conduction
• If we have a ball with initial temperature of T0 and it is left in fluid at Te.
• Heat is transferred by convection at the surface.
• As the surface temperature decreases, heat is transferred from the center of the ball to the surface, then to the fluid.
•Temperature will vary with location within a system and with time.•Temperature and rate heat transfer variation of a system are dependent on its internal resistance and surface resistance.
First Law Analysis of Cooling /Quenching of Hot Object s
Rate of Change in energy of hot object= Rate of Heat transfer
Rate of Heat Transfer = Rate of Convection by fluid =Rate of Conduction transfer in the metal ball
dt
dU :enegyin change of Rate
dt
cTdVd
dt
dU V
dt
drtrTrcd
dt
dU
R
0
2 ),(4For spherical objects
Total thermal resistance of the system: RtotT0
T
Rcond Rconv
TT0
At any instant:
econv
Rrcond
R
TtRThAdr
trdTkA
dt
drtrTrcd
),(
,),(4
0
2
•A Biot number is defined as:
Rrcond
conv
drtrdT
kA
TtRThABi
,),(
solid
sticcharacteri
sticcharacteri
cond
conv
cond
conv
k
hL
LkAhA
RTT
kA
TThABi
0
0
withinConductionby Object by Lost Heat
Object of Surface from removalheat Covection Bi
Relationship between the Biot number and the temperature profile.
System with negligible internal resistance
For this case Bi 1.0.and the temperature profile within the body is quite uniform.
The rate of change in internal energy of the body is equal to the rate of heat taken away from the surface by convection:
TtThAdt
dVtcTd
convV )(
)(
TtThAdt
cVTdconv )(
TtThAdt
dTcV conv )(
Rearranging:
dtcV
hA
TtT
dT conv
)(
Integrating to any time interval:
00)(
dtcV
hA
TtT
dT convT
T
cV
hA
TT
TT
0
ln
cV
hA
eTT
TT
0
Define, Thermal Time ConstanthA
cVc
ceTT
TT
0
TT
TTT
0
*
cV
thAtt
c *
Thermal Time Constant CVhAc
1
ththc CR
The total energy transferred during time t
t
convdtQQ0
t
dtTThAQ0
t t
dteTThAQ c
0
0
t t
dteTThAQ c
0
0
Hot Rolling of Steel Sheets
1solid
sticcharacteri
k
hLBi
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