Title: LASER CLADDING OF SHIP COMPONENTS MICROSTRUCTURAL EVALUATION
1LASER CLADDING OF SHIP COMPONENTS
MICROSTRUCTURAL EVALUATION
- 18 OCTOBER 2002
- BIJAYA ADAK
- DR. PHILIP NASH
2Overview
- Basic Concepts of Microstructure in Clad Region
- Discussion on Clad Zone Microstructure and
Solidification - Discussion on Laser Cladding with / on Stainless
Steel - Discussion on Dependence of Melt Height of
Substrate on Laser parameters.
3Basic concepts The Clad Region can be divided
into three parts
- Clad material
- Interface
- Heat Affected Zone
4Basic concepts The Overall Composition and
Microstructure of the Clad Material depends On
- Power density ( the laser beam power absorbed per
unit area of the material surface). - Interaction time.
- Cooling rate.
- Thermal Property of the Material.
- Degree of mixing due to conduction and convection.
5Basic concepts Microstructure f (Rate of
Solidification)
- Once Laser Irradiation stops
- Rapid cooling occurs due to heat transfer to the
bulk. - Due to high solidification, resulting
microstructure is fine and frequently contain
non-equilibrium phases. - Increased solid solubility occurs.
- As a result of the above microstructure, a
variety of improved surface conditions with
desired properties can be achieved. Foe example
- High Wear resistance
- High temperature oxidation resistance
- High Surface Hardness
- High Corrosion Resistance.
6Basic concepts SOLIDIFICATION
- The Cooling Rate in Laser Cladding is very high
(5 x 103 5 x 105 K/s). - Hence, Solidification in the clad zone can be
predicted by Rapid Solidification Theory. - The Thermal Gradient is highest at the bottom of
the melt pool and decreases quickly to a constant
value. - Local Solidification Rate increases as the
surface is approached from the bottom of the melt
pool. During most of the solidification it
remains constant. - The melt zone can be divided into three sub zones
from solidification point of view - Plane Front solidification
- Does not need nucleation.
- Proceeds unidirectionally from bottom to the
top. - Cellular Zone A very narrow Zone
- Dendritic Zone Most of the melt zone consists
of dendritic Structure.
7Laser Cladding with Stainless Steel
- Cladding carbon steel or low alloy steel by
various grades of stainless steel is a method of
producing materials with good corrosion
resistance and mechanical strength at a
relatively low cost. -
8Laser Cladding with Stainless Steel A coating
of AISI 316L S.S on a plate of 0.2 Carbon Steel
using powder injection technique.
- Microstructure consists of Austenitic dendritic
structure with small volume fraction of
interdendritic delta ferrite formed due to the
segregation of Cr and Mo. - Results
- Better Stress and Pitting Corrosion Cracking
Resistance than bulk material - In the overlapping area corrosion rate is high
due to the presence of delta ferrite.
9Laser Cladding with Stainless Steel UNS S44700
(Fe-30,Cr-4.4,Mo) used as clad material on
Carbon Steel
- Conventional Stainless steel (SS) has low
resistance to Pitting and Crevice corrosion in
Sea Water. - Several Stainless steel have been developed by
simultaneous addition of Molybdenum and Nitrogen
to achieve higher resistance to above type of
corrosion. - Overcome by cladding UNS S44700 on Carbon Steel
- Result
- Homogeneous Clad Layer
- Dilution was negligible
- Highly Dendritic Structure
- Microstructure Consists Mainly Ferrite. Cr Mo
segregate to the inter-denritic spaces.
10Laser Cladding on Steel Cr, Mn and Carbon
powder used as clad material on AISI 1016 as
substrate.
- Exhibits better wear properties than Stellite.
- The microstructure was divided into two parts.
- A blocked shaped region- A very closely spaced
carbide in ferrite matrix.carbides had hexagonal
structure which was M7C3 type. - A different type of carbide (M6C) was dispersed
on the ferrite matrix with a very uniform and
fine distribution.
11Dependence of Melt Height on Laser parameter
Laser Cladding and alloying of a Ni-base
super-alloy on plain carbon steel
- One of the objectives in a laser cladding process
is to decrease the melt height of the substrate
as much as possible. - Dependence of melt height on Laser parameters has
been demostrated in this paper. - Dilution factor Cact/Csup R/(DR)
- 1/(l 1)
- Where
- Cact Actual Concentration in alloyed / cladded
layer - Csup Concentration in untreated super alloy
- D Thickness of the substrate melted together
with the super-alloy. - l D / R
- R Initial thickness of the super-alloy sheet
12Dependence of Melt Height on Laser parameter
. Contd.
When l ltlt 1 Composition of the molten pool
is same with untreated super alloyResults
Cladding l gtgt 1 Results Alloying
- Conclusion
- The impact of the Interaction time on the
interface position is more than the impact of
beam power.