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LLNL-PRES-725737
This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under contract DE-AC52-07NA27344. Lawrence Livermore National Security, LLC
Coating hollow 3D objects with uniform low-
density films by combining EPD and ALD
D. Malone, M. Worsley, M. Wang, M. Biener
March 13, 2017
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2
Fabrication of a foam liner on the inside of a hollow cylinder (=hohlraum)• sub 50 mg/cm3
• ~200 micron thick
Goal
Peak power
Au material contour
Peak power
20 mg/cm3 Ta2O5, 300 umhohlraum liner
low fill hohlraum(0.03 – 0.6 mg/cm3 Helium)
Why do we need this?
Foam liner reduces wall motion and increases shape control
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electrophoresis
+ -
ElectrophoreticDeposition (EPD)
Coattemplate
removetemplate
Atomic LayerDeposition (ALD)
Burn/wash
electrode PS bead layer
Low density foam with controlled density/pore size
Approach: EPD + ALD
2) Transfer process to cylindrical geometry
Counter Electrode
Deposition ElectrodePolystyrene Suspension
1) Deposit thin layers of foams on flat geometry
0 1 2 3 4 5 6 7 8 9 10
0
20
40
60 2 nm Al2O3
5 nm Al2O3
10 nm Al2O3
de
nsity
of te
mp
late
d m
ate
rial m
g/c
c
diameter of sphere in micron
Projected density:
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Tasks and Challenges
Deposit PS beads on Au flat by EPD • Finding the right beads and EPD conditions• Surface smoothness• Drying/cracking• Thickness (200 micron)
Homogeneously coat PS deposit with ALD• Diffusion of ALD precursor into polymer• ALD temperature (deformation, crack formation)
Remove PS template• Complete removal of PS• Crack formation
Transfer to cylindrical geometry
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vendor X linked carboxylated bead size
ST X 1 um
ST X 1 um
ST 710 nm
PS X X 1 um
PS 1 um
Proper bead selection is critical for coating uniformity
EPD wellST: Spherotech, PS: Polyscience
Parameters explored:• Bead concentration• Flow rate• pH• Electrode pretreatment• Voltage
PS beads result in unconformal coating under various conditions:
Identifying the right beads for EPD requires testing
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Control of EPD layer thickness
0
100
200
300
400
500
600
700
800
0 5 10 15 20 25 30 35 40
Esti
mate
d D
ep
osit
Th
ickn
ess (
um
)
Time (min)
1mAmpthickness
2mAmpthickness
1 mA
2 mA
Spherotech beads (710 nm) deposit: thickness over deposition time
Induction period
Good control of EPD layer thickness by linear growth rate
desired thickness
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Prevention of crack formation during drying
7
Slow drying/freeze drying:
ST/Bang beads after EPD (no ALD coating)Dried in air (3 hours)
Ambient drying:
ST beads after EPD (no ALD coating)Dried in ethanol vapor (1 week)
Cracks can be avoided by carefully controlling the drying conditions (slow drying or freeze drying)
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Surface roughness
Ra of ~1.8 um over mm2 has been achieved for a 140 micron thick EPD film
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PS beads: carboxylated15c Al2O3 after burnout
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PS beads: not functionalized15c Al2O3 after burnout
10 micron
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ALD coating on different bead typesMass gain analysis on bulk pieces after 15 c Al2O3 @ 90C (expected ~3 nm)
X-
linked
carbox
ylated
Bead
size
Mass
gain %
Equivalent
ALD
coating
thickness
Density of
material
(mg/cm3)
Expected
density of
material
(mg/cm3)
ST X 1 um 25 10.5 nm 174 50
ST X 1 um 25 10.6 nm 177 50
ST 710 nm 30 9.1 nm 212 70
PS X X 1 um 10 4.4 nm 73 50
PS 1 um 22 9.5 nm 157 50
ST: Spherotech, PS: Polyscience
ALD growth rate depends on the type of beads (resulting foam density varies by a factor of 1.5 to 3.5 for same ALD conditions)
x 3.5
x 3.5
x 3.0
x 1.5
x 3.1
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Polyscience beads, non functionalized
Density: 157 mg/cm3
(~3x higher than expected)caused by subsurface deposition
“on surface”
“sub surface”
Parsons, ALD on Soft Materials, Wiley-VCH Verlag GmbH 2011, pp. 271.
ALD on
surface
functional
polymer
ALD on
surface-inert
polymer
ALD on polymers: diffuse or abrupt interface?
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ST 6.8 um 4.2 12 nm 29 10
ST 5.3 um 8.3 18 nm 58 13
Reduce density by using larger beads 20c Al2O3 @ 90C (expected: ~4 nm)
Mass gain analysis15c Al2O3 @ 90C (expected: ~3nm)
ST: Spherotech, PS: Polyscience
For 15c Al2O3 on 6.8 um beads: 22 mg/cm3
X-
linked
carbox
ylated
Bead
size
Mass
gain %
Equivalent
ALD
coating
thickness
Density of
material
(mg/cm3)
Expected
density of
material
(mg/cm3)
ST X 1 um 25 10.5 nm 174 50
ST X 1 um 25 10.6 nm 177 50
ST 710 nm 30 9.1 nm 212 70
PS X X 1 um 10 4.4 nm 73 50
PS 1 um 22 9.5 nm 157 50
reduce
x 3.5
x 3.5
x 3.0
x 1.5
x 3.1
x 2.9
x 4.5
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ST beads 6.8 um, 20c Al2O3, 450C/air/2h, residual PS mass 1.6%
large cracks
Some beads pop
open,
Some have “vent
holes”
Some beads
“shrivel”
Burning leads to PS removal but also large crack formation
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0
20
40
60
80
100
0 20 40 60 80
PS
Perc
ent
(%)
Time (hr)
Percent of PS Plasma Etched over Time (20c ALD)
Only minor cracks
Some beads are not etched
or only partially etched
Beads at cracks are
completely etched
ST beads 6.8 um, 20c Al2O3, residual PS mass 16%
Air plasma drastically reduces cracks, but no complete PS removal (even after 72 h)
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ST beads 6.8 u, 15c Al2O3, air plasma for 48 hours, 1.3 % of PS mass left
no visible PS
cores left
Minor cracks
(< 10 micron)
Complete PS removal for thinner ALD coatings
Plasma etching efficiently removes PS without major crack formation
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Cylindrical geometryEPD successfully transferred to cylindrical geometry
7 mm
3D printed sample holder
Polystyrene
Suspension
Stainless steel tube
with counter electrode
5.75 mm
Current Challenges:
• Inhomogeneous coating
• Side effects from
inhomogeneous field
• delamination of PS
coating~50 micron thick PS
bead deposit on
inside of SS cylinder
Work in progress:
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Demonstrated flat PS bead deposits by EPD on Au electrodes, 200 microns thick, without cracks
Templated PS films with ALD
Successfully removed the PS core with only minor crack formation
Achieved a Al2O3 foam density of ~20 mg/cm3
Working on optimization of 3D setup
Need: PS bead synthesis capability in-house
Summary
0 1 2 3 4 5 6 7 8 9 10
0
20
40
60 2 nm Al2O3
5 nm Al2O3
10 nm Al2O3
den
sity
of
tem
pla
ted
ma
teria
l mg
/cc
diameter of sphere in micron