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Laser Beam Characterization with FEM Modeling in Laser Cladding

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Title: Laser Beam Characterization with FEM Modeling in Laser Cladding


1
Laser Beam Characterization with FEM Modeling in
Laser Cladding
Guofang Zhou zhou2001_at_iit.edu T. Calvin
Tszeng tszeng_at_iit.edu Philip Nash nash_at_iit.edu
Feb. 7th, 2003
2
Characteristics of High Power Diode Laser (HPDDL)
in the NUVONYX ISL-4000L
  • Wavelength 805 nm
  • Working Distance 82 mm
  • Beam Dimensions at the focal point 12.5 mm 1
    mm
  • Min Pulse Width 500 ?s
  • Maximum Output Power 4000 Watts
  • Heat Profile

Nearly tophat intensity profile along the long
axis Gaussian profile perpendicular to the line
along the short axis.
Reference http//www.nuvonyx.com, ISL-4000L
Operators Manual
3
Determination of Surface Heat Flux
Material 430 Melting Temperature 1510 C k
23.392 W/K/m rc 4.968 J/cm3/K
6000 kW/m2/s
4
FEM Solution
  • Newton's Law

Heat Transfer Rate Heat Transfer
Coefficient Instantaneous Temperature
Envoinment Temperature
Inverse calculation is performed with FEM
program HOTPOINT.
5
Analytical Solution
  • Conduction Heat Transfer by Vedat S. Arpaci

6
Temperature Distribution at 1 Second
TC
7
Comparison of FEM and ANA Results
  • The accuracy of both solutions are pretty good.
  • Analytical solution is more convenient and
    straightforward.

8
Determination the Distributed Heat Flux
Material 430 Melting Temperature 1510 C k
23.392 W/K/m rc 4.968 J/cm3/K
10000
5000
5000
Unit kW/m2/sec
9
Temperature Distribution at 0.5 Second
6
2
4
5
1
3
10
Comparison of FEM and ANA Results
  • Both results are sound.
  • FEM result is more accurate

FEM
Reasons The formula is based on one dimensional
heat flux but distributed heat flux has the heat
transfer at the normal direction.
ANA
11
Discussion
  • For one dimensional steady state heat flux,
    analytical solution is more desirable.
  • For two dimensional distributed heat transfer
    problem, inverse calculation with FEM can
    characterize the heat flux rate on the surface
    with temperature histories obtained from the back
    installed thermocouples.
  • One issue is the possible distortion may be
    induced in laser cladding.
  • Another issue is the number and locations of
    thermocouples.
  • Control of various parameters in inverse
    calculation.

12
Thermophysical Property Data
MPDB Program
13
Mechanical Properties
Allegheny Ludlum Company
14
FEM Modeling for Distortion Consideration
Material 430 Melting Temperature 1510 C
10000
5000
5000
y
y
x
Unit kW/m2/sec
15
Distortion Grid and Temperature Distribution at
0.5 Second
Strain Contour
Temperature Contour
16
Distortion Issue
  • The distortion may change the actual heat flux
    into the specimen slightly.
  • In the FEM calculation, the distortion can be
    ignored in the model.

17
FEM Model with Temperature Dependence Properties
Material 430 Melting Temperature 1510 C
6000
4500
3000
Unit kW/m2/sec
18
Temperature Distribution at 1 Second
2
3
1
19
Calculated Heat Flux
20
6 Unknown Thermal Boundary Conditions
5
3
4
6
2
1
21
Calculated Heat Flux
22
Conclusions
  • FEM inverse calculation with measured temperature
    from back installed thermocouple is reliable to
    characterize the heat flux in laser cladding.
  • Along the long axis, six thermocouples are
    reasonable and capable to trace the heat flux on
    the top surface.
  • The characterization of short axis is need to
    experimentally further investigated.
  • Mathematical model is needed to be developed to
    reconstruct the 3-dimensional profile.
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