MULTISCALE SIMULATION OF FUNCTIONALIZATION OF SURFACES USING ATMOSPHERIC PRESSURE - PowerPoint PPT Presentation

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MULTISCALE SIMULATION OF FUNCTIONALIZATION OF SURFACES USING ATMOSPHERIC PRESSURE

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Title: MULTISCALE SIMULATION OF FUNCTIONALIZATION OF SURFACES USING ATMOSPHERIC PRESSURE


1
MULTISCALE SIMULATION OF FUNCTIONALIZATION OF
SURFACES USING ATMOSPHERIC PRESSURE
DISCHARGES Ananth N. Bhoja) and Mark J.
Kushnerb) a)Department of Chemical and
Biomolecular Engineering University of Illinois,
Urbana, IL 61801 bhoj_at_uiuc.edu b)Department of
Electrical and Computer Engineering Iowa State
University, Ames, IA 50011 mjk_at_iastate.edu http
//uigelz.ece.iastate.edu 32nd IEEE International
Conference on Plasma Science, 18th 23rd June
2005, Monterey, CA.
Work supported by the NSF.
2
OUTLINE
? Functionalization of Surfaces using Plasmas ?
Modeling Platform ? Pulsed Coronas in Humid Air,
He/O2/H2O mixtures ? Uniformity of surface
treatment ? O2 fraction ?
Discharge Polarity ? Surface
microstructure ? Concluding remarks
Iowa State University Optical and Discharge
Physics
ICOPS05_agenda
3
FUNCTIONALIZATION OF SURFACES USING PLASMAS
? Functionalization of surfaces occurs by their
interaction with plasma species - ions, radicals,
and photons. For hydrocarbon polymer
? Surface groups created in an O2 containing
plasma include ? Acids C(OH)O
? Carbonyl -CO ? Alkoxy C-O
? Peroxy C-O-O ? Alcohols
C-OH
Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_01
4
SURFACE MODIFICATION OF POLYMERS
? Pulsed atmospheric discharges (coronas) are
widely used in industry to treat commodity
polymers like polypropylene (PP).
? Tantec, Inc.
? Functionalization increases surface energy and
enhances wettability and adhesion.
? Akishev, et al, Plasmas Polym., 7, 261 (2002).
? PE Film
Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_02
5
TREATMENT OF NON-PLANAR SURFACES
  • M. Strobel, 3M

? Roughness of surface to be treated may range
from 100s nm to few µm.
  • SEM of polyester fabric (Borcia, et al, Plasma
    Sources Sci. Technol, 12, 235 (2003).

? Penetration of plasma species into surface
features determines the extent and uniformity of
functionalization.
Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_03
6
SCHEMATIC OF THE 2-D MODELING PLATFORM
  • Unstructured mesh
  • Plasma hydro-dynamics (multi-fluid, Poissons
    equation)
  • Radiation transport
  • Integrated plasma-surface kinetics model

Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_04
7
DBD TREATMENT OF PP SURFACE WITH MICROSTRUCTURE
  • Corona treating a polymer on the grounded
    electrode acts as a DBD.
  • Gas mixtures
  • ? He/O2/H2O
  • ? Humid air - N2/O2/H2O
  • How does uniformity of treatment vary over
    microscopic and macroscopic scales when
    repetitively pulsed?

? PRF 10 kHz
Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_05
8
PLASMA PROPERTIES IN He/O2/H2O MIXTURES
Potential (V)
Te (eV)
Positive Ions cm- 3
O cm- 3
- 5000 0 0 7.5
1011 1014 1011 1014
? - 5 kV, 760 Torr He/O2/H2O98/1/1, 0 2.5 ns
ANIMATION SLIDE
Iowa State University Optical and Discharge
Physics
MIN
MAX
ANANTH_ICOPS05_06
9
PLASMA PENETRATION INTO SURFACE FEATURES
e cm- 3
1010 1013
t 2.5 ns
t 5 ns
O cm- 3
1010 1013
t 2.5 ns
t 5 ns
Positive ions cm- 3

1011 1013
t 2.5 ns
t 5 ns
? - 5 kV, 760 Torr, He/O2/H2O98/1/1
Iowa State University Optical and Discharge
Physics
MIN
MAX
ANANTH_ICOPS05_07
10
EFFECT OF O2 FRACTION ON O DENSITY
He/O2/H2O 98 / 1 / 1
He/O2/H2O 89 / 10 / 1
t 5 ns
t 3 ns
? At higher O2 fraction, the density of reactive
O radicals at the surface increases during the
pulse.
He/O2/H2O 69 / 30 / 1

O cm- 3
2x1011
2x1014
t 3 ns
(log scale)
? - 5 kV, 760 Torr
Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_08
11
SURFACE REACTION MECHANISM FOR PP
? Gas phase radicals abstract H from the surface
and produce radical sites on the PP surface.
? Further reactions lead to formation of
functional groups like peroxy, alkoxy,
alcohols and other groups1.
1R. Dorai and M.J.Kushner, J. Phys. D 36, 666
(2003).
Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_09
12
DENSITY OF SURFACE RADICALS
  • ALKYL (PP? ) are formed by
  • O PP ? PP? OH
  • Nonuniformities result from both fluxes and
    shadowing.
  • ALKOXY (PP-O?)
  • O3 PP? ? PP-O?
  • O PP? ? PP-O?
  • take longer to form
  • but eventually
  • dominate.

Iowa State University Optical and Discharge
Physics
? - 5 kV, 760 Torr, 10 kHz, He/O2/H2O98/1/1
ANANTH_ICOPS05_10
13
DENSITY OF -OH FUNCTIONAL GROUPS
  • Non-uniformities occur on the macroscopic and
    microscopic (lt 1 µm) length scales and are site
    dependent

? - 5 kV, 760 Torr, He/O2/H2O98/1/1, 10 kHz
Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_11
14
TEMPORAL VARIATION OF FLUXES WITH O2 FRACTION
IP START
IP END
  • Larger fraction of reactive O is lost in the
    interpulse period at higher O2 fraction by
    three-body recombination and ozone formation.
  • Optimum composition is at O2 10 with
    significant O flux maintained through the long
    interpulse period.
  • At position along surface 0.05 cm,
    He/O2/H2O99-x/x/1
  • IP - interpulse period (duration 100 ms at 10
    kHz)

Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_13
15
SPATIAL VARIATION OF FLUXES WITH O2 FRACTION
O210
O275
  • As O2 fraction increases, there is greater
    non-uniformity in fluxes of O and O3 at the
    surface.
  • At end of IP, He/O2/H2O99-x/x/1
  • IP - interpulse period (duration 100 ms at 10
    kHz)

Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_13
16
EFFECT OF O2 FRACTION ON TREATMENT
  • Macroscopic non-uniformities in OH and OO
    ultimately arise from significant spatial
    variation of O, O3 and OH fluxes.
  • Microscopic scale non-uniformities arise due to
    transport limitations of reactive O at higher
    O2 fractions.

? - 5 kV, 760 Torr, He/O2/H2O99-x/x/1, 10 kHz,
1 s
Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_14
17
HUMID AIR - EFFECT OF VOLTAGE POLARITY
- 15 kV, 2.5 ns
15 kV, 10 ns
? O
? e
? e
- 15 kV, 2.5 ns
1011 - 1014
1010 - 1013
15 kV, 10 ns
  • Positive discharge spreads more uniformly on
    surface.
  • Surface recombination of O enhances O at
    surface.


1011 - 1014
5x1011 - 5x1014
? 760 Torr, N2/O2/H2O79/20/1
cm- 3
Iowa State University Optical and Discharge
Physics
MAX
MIN
log scale
ANANTH_ICOPS05_15
18
EFFECT OF POLARITY ON TREATMENT
  • Pulsed positive polarity operation gives higher
    uniformity of functionalization due to more
    uniform formation of O and O3 near the surface.

? 760 Torr, N2/O2/H2O79/20/1, 10 kHz, 0.15 s
Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_16
19
IONS AND PHOTONS IN SURFACE CHEMISTRY
  • UV photons from the plasma can cleave surface
    bonds.
  • Ions striking the surface transfer energy and can
    activate sites.
  • Postulate creation of intermediate active sites.
  • Active sites may crosslink in addition to
    standard reaction pathways.

Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_17
20
NON-UNIFORMITY DUE TO SHADOWING
CROSSLINKS
  • Line-of-sight photon transport fails to reach
    deep inside surface features.
  • Crosslinking is relatively higher on surface
    features exposed to the avalanche where ion and
    photon fluxes are higher.

? - 5 kV, 760 Torr, He/O2/H2O98/1/1, 10 kHz,
0.2 s
Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_18
21
CONCLUDING REMARKS
? Multiscale modeling using unstructured meshes
was applied to study DBD corona treatment of PP
surface with microstructure. ? Non-uniformity in
functionalization occurs on the macroscopic (few
mm) and microscopic ( lt 1 µm) scales. ? In
He/O2/H2O mixtures, the O2 fraction can be used
to optimize uniformity of treatment. ? In humid
air, pulsed positive polarity discharges produce
more uniform functionalization. ? Shadowing by
surface microstructure results in non-uniform
crosslinking with a mechanism using photon and
ion fluxes.
Iowa State University Optical and Discharge
Physics
ANANTH_ICOPS05_19
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