Solid Freeform Fabrication from Gas Precursors Using Laser Processing
Final Report, 1996-2001
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Principal/co-Principal Investigator.
* PI/co-PI Name(s): Harris L. Marcus
* PI Institution: University of Connecticut, Storrs
* PI Phone Number: (860) 486-4623
* PI Fax Number: (860) 486-4745
* PI Street Address: 97 North Eagleville Road
* PI City,State,Zip: Storrs, CT 06269-3136
* PI E-mail Address: hmarcus@mail.ims.uconn.edu
* PI URL Home Page: http://www.ims.uconn.edu/metal/faculty/marcus.htm
* Grant/Contract Number: N00014-95-1-0978
* Period of Performance: 07/01/96 - 06/30/01
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Productivity Measures.
* Number of refereed papers submitted not yet published: 1
* Number of refereed papers published: 11
* Number of unrefereed reports and articles: 30
* Number of books or parts thereof submitted but not
published:
* Number of books or parts thereof published: 2
* Number of project presentations: 40
* Number of patents filed but not yet granted:
* Number of patents granted and software copyrights: 2
* Number of graduate students supported >= 25% of full
time: 6
* Number of post-docs supported >= 25% of full time: 1
* Number of minorities supported: 3
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Objective of Research
The objective of the research was to establish the
technical approaches required to use localized laser induced chemical vapor
deposition as an approach for solid freeform fabrication (SFF). The three processing approaches to be
developed are Selective Area Laser Deposition (SALD), Selective Area Laser
Deposition Vapor Infiltration (SALDVI), and Selective Area Laser Deposition
Joining (SALD-Joining) of ceramics.
Executive Summary
In this overall final report on the research into
the three processing approaches, Selective Area Laser Deposition (SALD),
Selective Area Laser Deposition Vapor Infiltration (SALDVI), and Selective Area
Laser Deposition Joining (SALD-Joining) of ceramics only limited details are
included. The reader can get greater
detail in the over forty publications listed below that resulted from this
research.
In terms of producing SFF shapes the SALDVI was the
most successful. It was used to produce
simple geometric parts of SiC or Si3N4 into SiC, Si3N4,
metal and other powders. One of the
more successful composites made was SiC deposited into Mo powder. The advantage of the layer by layer
infiltration technique was clearly shown.
The primary difficulties in the SALDVI processing were prevention of
SALD overlay onto each layer, some residual porosity, and the very slow
processing rate. The approach was
characterized for the different materials in terms of laser power, scanning
rate, preheat temperature, precursor gas pressure, precursor gases, raster
geometry, line overlap, and laser wavelength, primarily using Nd:YAG and CO2
lasers. As part of the effort finite
element calculations of the processing parameters were made to help define the
appropriate processing space.
To demonstrate the use of SALD and SALDVI together
devices buried in a bulk material were produced. The most successful were C/SiC embedded thermocouples. This used SALDVI to produce the bulk SiC,
SALD to coat the bulk SiC with Si3N4 as an insulator
followed by SALD deposition of the C and SiC legs of the thermocouple. The
thermocouple was then sealed with another SALD layer of Si3N4
and finally encapsulated in the multiple layers of SALDVI SiC. Samples with
multiple thermocouples were also produced and demonstrated. This showed the wide potential of the
combined SALD/SALDVI processing.
The third approach of SALD joining was fully
demonstrated. SALD deposition of SiC
deposited from the tetramethylsilane gas precursor joined two pieces of
SiC. Similar results were obtained for
Si3N4. This
ability to "weld" ceramics with the same material to be joined has
great promise. The primary difficulty
is associated with the limited throwing power of the approach due to the
surface being hotter than the inside of any joint geometry used.
A Solid Freeform Fabrication laboratory was designed and assembled, with a starting point of an empty room. Three unique and fully functional computer controlled gas phase laser-based SFF systems are presently in place. Overall the SALD, SALDVI and SALD Joining were all demonstrated and many of the processing parameters worked out. The potential availability of gas precursors for most materials makes them potentially a very strong possibility for SFF of many complex materials. Overall there will be a great deal of additional effort necessary to make the processes robust.
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Summary of Technical Progress.
Equipment
A Solid Freeform Fabrication
laboratory was designed and assembled, with three SFF systems presently in
place. Two systems have Powder Delivery System (PDS) units for spreading out a
powder substrate, necessary for the SALDVI process. One system offers a four
inch by four and a half inch target area for large part production, while the
other system has a one inch diameter target area. The third system is used for
SALD/SALD joining and contains a SALD joining machine, incorporating a variable
speed rotational device designed to work with tube structures. The large PDS
sits in a 28 inch diameter, 15 inch tall vacuum system with a double-walled
cooling jacket. The two other systems are eight inch diameter, eight inch tall
vacuum chambers that have been nickel-plated to protect against the corrosive
environments of some precursors and reaction by-products. Two in-situ chemical
analysis tools have been implemented into the SALD/SALDVI systems. The first is
a residual gas analyzer, and the second is a four point sampling emission
spectrometer
Five lasers are operational,
25 and 50 watt continuous wave CO2 (10.6 micron wavelength), 50 and
150 watt Nd:YAG (1.064 micron wavelength), and a 6 watt harmonic generating
pulsed Nd:YAG (1.064, .532, .355, .266 micron wavelengths at the fundamental
and 2nd, 3rd, and 4th harmonic wavelengths, respectively). X-Y translational
equipment, optics, electronic components, three computers and associated
software are all utilized in laser scanning. Ancillary laboratory equipment
needed for proper laboratory procedures and safety has also been acquired and
put to use, including a glove box for liquid precursor handling, a micron
filter vacuum for powder cleanup, and compressed gas cylinder equipment.
An integrated temperature closed loop and scanning motion control computer program has been designed and refined in-house for the SFF systems. The program was written in Visual Basic. The closed loop uses the output from an emissivity-measuring infrared pyrometer to monitor temperature at the reaction zone of the laser beam. The program compares this readout to a user-defined temperature and makes adjustments in laser power by altering the input voltage to the laser controller with an analog voltage output card. Concurrent with this operation, the Visual Basic program directs the motion control hardware. Custom motion programs can be designed and inputted into the program. Data acquisition of the processing parameters such as laser power, pyrometer temperature and emissivity, and other signals is included. These processing control programs also have the capability to generate 2-D scan patterns automatically from 3-D computer geometrical models.
Technical Results
The
specific research programs at the UCONN SFF lab focus on ceramic fabrication
from the gas-phase reactions. Fundamental understanding of the SALD and SALDVI
processes are essential to applying the technology to real world
applications. The results below are
summaries of technical progress in the three SALD research areas. For greater details, the reader is referred
to the relevant publications.
SALDVI
The
SALDVI work is focused on fabricating SiC bulk shapes by infiltration of SiC
powder particles with vapor deposited SiC derived from tetramethylsilane (TMS)
gas, although other starting powders (carbides, nitrides, oxides, metals) were
also investigated. Powders of different
size were mixed to vary the packing fraction and surface area. Laser scanning was performed using a range
of gas precursor pressures using different temperature distributions and local
heating times. Quantitative
metallography was used to measure the variations in the amount of infiltration
with position in the samples for each powder and processing condition. A comparison of the measured infiltration
profiles shows that the properties of the starting powder influence the vapor
infiltration in the powder layer. The
variations in the measured infiltration profiles were analyzed and correlated
with the variations in the physical properties of the starting powders to
obtain a general predictive model of the process. The results show that solid density of more than 90 percent can
be obtained in a region within 250 microns of the free surface of the powder
layer under certain processing conditions. Process control was enhanced to
allow automatic control of the heating and cooling rate whenever the laser beam
is turned on or off. The capability to preheat the powder bed and SALDVI
workpiece was also added.
The feasibility of fabricating SiC cermets by SALDVI
was investigated, particularly by combining vapor deposited SiC with copper,
molybdenum, and nickel powder layers. The microstructures of the three SALDVI
cermets reveal varying degrees of reactions between the metal powders and the
vapor deposited SiC matrix. Both the Cu
and Ni powders react with vapor deposited SiC during the SALDVI process at all
of the processing temperatures (1000-1200 C) and heating times (200-800 s)
examined here. For the Cu powder,
particles at least 20 mm in diameter had reacted to form a Cu silicide phase even at the
shortest heating time of 200 s and lowest processing temperature of 1000
C. Further evidence of Cu silicide
formation was observed in x-ray diffraction measurements at 1000 and 1200 C
target temperatures. These results
indicate that Si is a fast diffuser in Cu.
In the Ni case, the extent of the reactions progressed more notably with
increasing processing temperature and heating duration. X-ray diffraction (XRD) and energy
dispersive x-ray spectroscopy (EDS) measurements indicate the formation of the
Ni2Si phase, as well as additional phases not yet identified. For
the Mo/SiC cermet, no Mo-Si interdiffusion was detected by XRD or EDS for the
1000 C target temperature. This is not
surprising as the melting temperature of Mo is 2610 C, so diffusion would be
expected to occur slowly at 1000 C. The
Mo/SiC cermet shows the highest bending strength of 50 MPa of the three
cermets. This behavior is attributed to
the close thermal expansion match between the two materials resulting in few
particle debonds compared to the Cu and Ni cases. Figure 1 shows a typical as-fabricated single line, three layer,
20 mm long SALDVI Mo/SiC cermet (a) and a SEM image of a polished cross-section
through its centerline region (b). The
Mo particles appear well bonded to the SiC matrix and the solid density exceeds
95 % in this region, as measured by quantitative metallography.


Figure 1. As-fabricated three layer,
single line macrostructure (a) and SEM image of the microstructure of Mo/SiC
SALDVI cermet.
The role of the starting powder on the development
of the final SALDVI structure was also investigated. Silicon carbide was deposited by SALDVI from the gas precursor
tetramethylsilane, Si(CH3)4, into loosely packed powder
layers of SiC, ZrO2, WC or Mo.
Layered samples were fabricated for each powder material using both
single line (bar) and multiple line (rectangle) laser scan patterns and 10 Torr
Si(CH3)4, 2.5 mm/s scan speed, 1000°C target temperature, and 120 mm layer thickness. Samples of SiC and ZrO2 are prone
to surface cracking in the bar geometry, and cracking and delamination of
layers in the rectangle geometry.
Samples fabricated with Mo powder have no cracks or delamination defects
in either bar or rectangle geometry as well as a better surface appearance.
Figure 2 shows a Mo powder/SiC matrix rectangle with 6 layers (a) as-fabricated
and (b) cross-section across layers. Thermal stress plays a major role in
cracking in bar and rectangle samples of SiC matrix/SiC powder and SiC matrix/
ZrO2 powder made by SALDVI.
The effective thermal conductivity (keff )of the SALDVI
workpiece correlates well with the severity of thermal cracking. The lower keff the more severe
the cracking. SiC matrix/Mo powder samples
have the highest keff, and show no cracking. The irregular shape of the SiC and ZrO2
powders, as well as a higher surface roughness, could provide stress risers in
the matrix during processing, increasing their susceptibility to thermal
cracking compared to the spherical Mo powder. The type of powder was found to
affect the surface appearance and internal structure of SiC matrix multiple
layer SALDVI rectangles. Samples with
SiC and ZrO2 powder show a porous surface appearance due to
displacement of the powder during processing.
Mo and WC powder samples have a dense surface and continuous solid
material across adjacent layers. The
lower density of the SiC and ZrO2 powders and convective effects in
the gas are the likely cause of their poor structure and rough surface
appearance.
Figure 2. Mo powder/SiC
matrix rectangle with 6 layers (a) as-fabricated and (b) cross-section across
layers.
A 3D finite element model
was also developed to simulate the SALDVI of silicon carbide. The model
predicts the laser input power and the distribution of vapor deposited SiC
within the powder bed as well as on the surface of the powder bed (SALD). The
model includes closed-loop control of the laser power to achieve a desired
target processing temperature on the top surface of the power bed. This model
considers a moving Gaussian distribution laser beam, temperature- and
porous-dependent thermal conductivity, specific heat and temperature-dependent
deposition rate. A schematic of the model is shown in Figure 3. The simulation results compare well with
experimental data as shown in Figure 4.

Figure 3. Finite
element model of the SALDVI process.

Figure 4. Comparison between the experimental and
simulated solid fraction distribution in depth direction under the center of
the laser beam after the scanning process at x=7 mm.
The simulation results of the incident
laser power history and the distribution of vapor infiltrated SiC in the powder
bed agree fairly well with the experiments. As the laser scanning rate decreases,
the incident laser power increases. As the laser scanning rate decreases, the
deposition of SiC both within the powder bed as well as on the surface of the
powder bed (SALD) increases (Figure 4).
Uniform temperature on the top surface of powder bed during laser
scanning process needs non-uniform laser power at the initial scanning period
and nearly uniform laser power elsewhere. These simulation results offer
guidelines for further experimental studies of the SALDVI process.
SALD and integrated SALD/SALDVI
SALD
research looked at multiple material deposition. Specifically, silicon nitride,
from TMS and ammonia, and silicon carbide and carbon, from TMS and acetylene
respectively, were examined. The silicon nitride was deposited as a thin film,
and analyzed with respect to its insulative quality. The deposition was
performed at low ammonia pressures, approximately 10 to 20 torr, using a carbon
dioxide laser. The successful formation of the nitride layer countered previous
notions of not being able to use ammonia gas precursors with a CO2
laser. Silicon carbide and carbon were deposited in line formations, with the
resulting electrical properties coming under scrutiny. The line resistances and
emf response to temperature changes were tested with respect to varied line
widths (a function of scan speed and laser beam size) and deposition
temperature field. These SALD/SALDVI investigations were applied to an embedded
sensor project sponsored by DARPA. The DARPA program studied the feasibility to
fabricate a ceramic matrix with an operational, in-situ thermocouple formed
inside the matrix structure in one continuous process. An example of a
SALD/SALDVI silicon carbide/carbon thermocouple in a silicon carbide matrix,
along with its temperature and emf response, can be found at
the UCONN website.
It
was found that the experimental results are in excellent agreement with the
theoretical thermodynamic predictions.
With the use of acetylene (C2H2),
tetramethylsilane (TMS), and a mixture of TMS and ammonia, graphite, SiC, and
Si3N4 were successfully deposited, respectively. Strong temperature dependency of the SALD
products in morphology, composition, crystal structure and size, growth
kinetics and relevant properties were revealed. The predicted carbon co-deposition and the role of hydrogen gas
in eliminating this co-deposition in SiC or Si3N4 were
experimentally confirmed by a Raman scattering study. The functional test on the fabricated device showed that the
embedded SiC/C thermocouples exhibited stable and repeatable response to
temperature variations. Thus, the
overall results indicated that it is feasible to embed the in-situ sensors
within a ceramic matrix using the combined SALD/SALDVI techniques.
SALD-Joining
Another
area of investigation in the SFF laboratory is ceramic joining by SALD, a
patented process for substrate-involved SALD deposition. The joining of ceramic
parts is accomplished by using a filler material deposited from the gas-phase
reaction in SALD. In this manner, the ceramic joint can be tailored to match
the material composition of the constituent ceramic part to be joined. The
initial efforts focused on joining clay-bonded silicon carbide (approximate 75
to 80% density) tubes with silicon carbide deposited from TMS precursor. The adhesion
of the SALD material to the tube is excellent. In fact, the interface between
the SALD material and the tube is inconspicuous. The success of joints in this
initial phase has been inconsistent. While the adhesion is outstanding,
successful connective bonding of the SALD material across the joint has been
challenging. An example of two clay-bonded silicon carbide tubes connected by
the SALD joining method can be found at the UCONN website.
Investigation
on this project has yielded several successfully joined silicon carbide tube
structures using silicon carbide deposited filler from the gas-phase pyrolosis
of tetramethylsilane. Adhesion of the deposit to the tube surface remains
excellent. Bend testing of joined samples produced poor strength values, likely
due to the butt-end nature of the joint geometry. This leaves an existing
'crack' at the joint seam the length of the tube wall. Beveling of the tube
ends has become a central focus to achieve stronger joints, not only to reduce
the initial crack length but to also increase the surface area of tube/deposit
adhesion interface. The hermetic quality of the several joints was examined,
compared to a monolithic standard of the base tube used. The SALD joints held a
steady-state vacuum (in Torr) within a factor of 10 of the vacuum held by the
standard. Improvements in the deposit morphology, from a billowy, porous nature
to a more laminar deposition, are expected to improve these hermeticity values.
Preheating
the silicon carbide substrate during the SALD deposition process is a
controlling parameter for producing high density, high purity, defect-reduced
silicon carbide filler. The preheating
reduces the thermal gradient occurring during the joining process. SALD tube joint structures show greatly
reduced mechanical bend strengths compared to monolithic tube standards. The origins for the lower strength are the
initial crack found at the joint seam of the butt-end tube configuration and
the reduction in the cross-sectional area of the SALD filler deposit compared
to the full tube cross-sectional area due to the poor ‘throwing power’ of the
laser associated with localized CVD.
The SALD gas-phase decomposition of tetramethylsilane, with and without
hydrogen, deposits nano-crystalline silicon carbide. Characterization of the SALD silicon carbide filler material
shows deviations from the expected beta-polytype in the XRD, NMR and TEM
patterns that are attributed to twinning faults. This is the first evidence of twins in SALD silicon carbide but
is consistent with the very low stacking fault energy for silicon carbide.
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Transitions and DOD Interactions.
Briefing on SFF applications to future naval
operations to Fellows of the Chief of Naval Operations' Strategic Studies
Group, Capt. T.D. Glass USN, Capt. D.R. Ellison USN, and LCDR S.L. Kruppa USN,
at Newport, RI April, 1996
Presentation on "Laser Solid Freeform
Fabrication: SLS, SALD, SALDVI" at the ONR review meeting in Woods Hole,
MA, May 29th-30th, 1996
Presentation on "Solid Freeform Fabrication at
the University of Connecticut" at the ONR annual review meeting in Woods
Hole, MA, June 16th , 1997
Presentation of research programs and tour of the
SFF laboratory for Dr. William Coblenz of DARPA, August 8th, 1997
Dr. Marcus took a 4 day trip on the USS Tunney
submarine from San Diego, CA to Seattle, WA, September, 1997
Breifing on SFF at Navy War College, Newport, RI,
1998.
Sustained contacts and interactions with Bettis and
Knowles Atomic Power Laboratory on SALD, SALDVI, and SALD joining of ceramics.
Presentations on SALD SFF techniques to Carderock
Division of NSWC, 2000.
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Software and Hardware Prototypes.
1. Prototype Name:
SALD and SALDVI System Prototypes
+
URL:
+
Availability: Available in SFF
laboratory, Institute of Materials Science, UCONN
+
Description: Hardware and software of
performing gas phase SFF of structures and infiltration of powder layers.
Invited Presentations
Presentations on "Selective Area Laser
Deposition: A Gas Phase Solid Freeform Fabrication Approach" and
"Solid Freeform Fabrication Processing Using Gas Phase Approaches" at
the ASM/TMS Materials Week conference, Cleveland, OH, October 30th-November
2nd, 1995
Presentation on "Solid Freeform Fabrication
Using Powder and Gas Precursors" at the Dept. of Mechanical Engineering,
Aeronautical Engineering and Mechanics Colloquium series, Renssalaer Polytechnic
Institute, November 17th, 1995
Presentation on "Solid Freeform
Fabrication" at the Institute of Materials Science Associate Program
Annual Meeting, University of Connecticut, May 23rd, 1996
Presentation on "Solid Freeform Fabrication at
The University of Connecticut" at the Solid Freeform Fabrication Symposium
at The University of Texas at Austin, August 12th-14th, 1996
Presentation on "Solid Freeform Fabrication of
Powders Using Laser Processing" at the PM2TEC conference, Washington,
D.C., June 19th, 1996
Presentation on "Solid Freeform Fabrication of
Ceramics" at the Society of Manufacturing Engineers conference, Newton,
MA, October 23rd, 1996
Presentation on "Solid Freeform Fabrication: An
Overview" at the ASME/MED Symposium on Rapid Response Manufacturing,
Atlanta, GA, November, 1996
"Recent Advances in SALD and SALDVI,"
Seventh International Conference on Rapid Prototyping 1997, San Francisco,
March 31-April 3, 1997
"Gas Phase Solid Freeform Fabrication at the
University of Connecticut," MRS Annual Meeting, Solid Freeform Fabrication
Session, San Francisco, March 31 - April 4, 1997
"Selective Area Laser Deposition (SALD) of
Titanium Oxide," 6th European Conference on Rapid Prototyping and
Manufacturing 1997, Nottingham, UK, July 1-3, 1997
Solid Freeform Fabrication Symposium 1997, Austin,
TX , August 11-13, 1997, 4 presentations on the following topics: a) The Use of
VRML to Integrate Design and Solid Freeform Fabrication, b) Gas Phase SFF
Control System for Silicon Nitride Deposition by SALD/SALDVI, c) Fabrication of
In-Situ SiC/C Thermocouples by Selective Area Laser Deposition, d) Net Shape
Functional Parts Using Diode Laser
"Selective Area Laser Deposition Joining of
Silicon Carbide," American Ceramic Society 1997 Fall Meeting, San Francisco,
October 12-15, 1997
Workshop on Layered Manufacturing, Oxford, England,
June, 1998, Invited Speaker
"Gas-Phase Selective Area Laser Deposition
(SALD) Joining of SiC Tubes with SiC Filler Material", 1998 Solid Freeform
Fabrication Symposium, August 10th 12th, 1998, Austin, TX
"Preparation and Properites of In-Situ Devices
Using the SALD and SALDVI Techniques", 1998 Solid Freeform Fabrication
Symposium, August 10th-12th, 1998, Austin, TX
"Properties of SiC/C Thermocouple Device Made
with SALD and SALDVI Techniques", 1998 American Ceramic Society Meeting,
May 3rd -May 6th, 1998, Cincinnati, OH
"Selective Area Laser Deposition of Silicon
Nitride", 1998 American Ceramic Society Meeting, May 3rd -May 6th, 1998,
Cincinnati, OH
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