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Table 1 Static water and CH2I2 contact angles on the substrates and the
surface free energies of the substratesa
Water contact CH2I2 contact Surface free energy
Substrate angle (1)
angle (1)
(gS) (mJ mꢀ2
)
Gold
Glass
PDMS
154.5
156.8
155.6
154.5
154.7
156.3
153.6
148.6
149.1
148.6
137.9
142.1
144.4
140.2
0.279 (gDS : 0.251, gPS: 0.028)
0.256 (gDS : 0.249, gPS: 0.007)
0.274 (gDS : 0.258, gPS: 0.015)
0.929 (gDS : 0.910, gPS: 0.019)
0.581 (gDS : 0.581, gPS: 0.000)
0.458 (gDS : 0.458, gPS: 0.000)
0.706 (gDS : 0.706, gPS: 0.000)
Fig. 3 Static water contact angles of the bare and f-DOPA-coated substrates. PET
V foil
Zn foil
TiO2
coating of the polymerized f-DOPA involved the same processes
as the polydopamine coating, which was thought to result from
the presence of the catechol and amine groups,6,16 although the
adhesion strength would be lower than that of polydopamine
due to the perfluorinated group in f-DOPA.
a
Contact angles are the averaged values from three different samples.
The surface free energies, and their dispersive and polar components
are calculated with the averaged contact angles based on the Owens–
Wendt geometric mean equation.
Fig. 3 shows the static water contact angles before and after
coating, confirming that all the f-DOPA-coated substrates were
superhydrophobic. Regardless of different contact angles
before coating, the coating made the contact angle of all the
substrates to be about 1551 (Fig. 3). Interestingly, PTFE, which
exhibits the low surface energy (19.1 mJ mꢀ2) and is non-sticky,17
also became a self-cleaning, superhydrophobic surface with a static
water contact angle of 1491 after f-DOPA coating (data not shown).
The wetting properties were further investigated by the tilting-plate
method that measured the dynamic contact angles, because it was
essential in the confirmation of self-cleaning properties to investi-
gate the dynamic water contact angles and surface free energies.
The advancing (yadv) and receding (yrec) water contact angles of
f-DOPA-coated substrates were measured, and the contact angle
hysteresis (i.e., (yadv ꢀ yrec)) of each substrate was calculated
(Table S1, ESI†). For example, the gold substrate, after coating,
showed a low contact angle hysteresis of 9.91. A water droplet on
the substrate easily rolled off at a tilt angle of 5.31, which is clear
evidence of self-cleaning properties. All other f-DOPA-coated sub-
strates also showed the low contact angle hysteresis and self-
cleaning properties with low sliding angles of 2.51 to 6.71. In
addition, the surface free energy (gS) was calculated based on the
Owens–Wendt geometric mean equation that divides the surface
free energy into the dispersive (gDS ) and polar (gSP) ones.17
surface free energy and realization of superhydrophobic, self-
cleaning properties.
Interestingly, the wetting characteristic of the f-DOPA films
was changed to non-superhydrophobic by simple O2-plasma
treatment: after 1 min of treatment, the static water contact angle of
the f-DOPA-coated gold substrate was changed from 154.451 to
124.181. The spatio-selective oxidation of the film could be utilized
for manipulation of water droplets and flow. For example, when a
small square area of the film was made relatively hydrophilic by
plasma treatment, a water droplet was captured at that hydrophilic
area after fast rolling on superhydrophobic area with slight tilting.
Droplet-based microfluidic channels could be fabricated with ease,
demonstrated by a hydrophilic line on the superhydrophobic
surface (Fig. S3, ESI†).
In summary, we demonstrated a simple coating method for
generating superhydrophobic, self-cleaning surfaces by using a
perfluorinated dopamine derivative (f-DOPA) as a polymerization
precursor. f-DOPA was coated on various substrates via oxidative
polymerization, forming a rough structure of low surface free
energy (0.2–0.9 mJ mꢀ2) without any additional fabrication.
Although the f-DOPA coating was not transparent intrinsically
because of the chemical nature of the polydopamine moiety,
we believe that the universality of the coating method would
widen the substrate scope for certain applications of self-
cleaning, superhydrophobic surfaces.
qffiffiffiffiffiffiffiffiffiffi
qffiffiffiffiffiffiffiffiffi
ð1 þ cos yÞgL ¼ 2 gDS gLD þ 2 gSPgLP
This work was supported by the Basic Science Research
Program through the National Research Foundation of Korea
(NRF) funded by the Ministry of Science, ICT & Future Planning
(MSIP) (NRF-2012R1A3A2026403 and NRF-2013R1A1A1059642).
where y is the measured contact angle of a liquid on the surface,
and gL is the surface tension of the liquid.
The surface free energy (gS; gS = gDS + gSP) of each surface was
determined by measuring the contact angles with water and
diiodomethane (CH2I2) (Table 1). The surface free energy of the
f-DOPA-coated gold surface was calculated to be 0.279 mJ mꢀ2
,
Notes and references
1 W. Barthlott and C. Neinhuis, Planta, 1997, 202, 1.
2 X.-M. Li, D. Reinhoudt and M. Crego-Calama, Chem. Soc. Rev., 2007,
36, 1350.
3 X. J. Feng and L. Jiang, Adv. Mater., 2006, 18, 3063.
4 K. Teshima, H. Sugimura, Y. Inoue, O. Takai and A. Takano, Appl.
Surf. Sci., 2005, 244, 619; S. Minko, M. Muller, M. Motornov,
M. Nitschke, K. Grundke and M. Stamm, J. Am. Chem. Soc., 2003,
125, 3896.
5 J. H. Waite and M. L. Tanzer, Science, 1981, 212, 1038.
6 H. Lee, S. M. Dellatore, W. M. Miller and P. B. Messersmith, Science,
2007, 318, 426.
and the other substrates have the surface free energies between
0.2 and 0.9 mJ mꢀ2. These values are extremely low, probably
because of both the structural roughness and the incorporated
perfluoro groups. For comparison, the surface free energy of a
smooth surface modified with CF3 groups in hexagonal close-
packing was reported to be 6.7 mJ mꢀ2 18
In our system, the
.
simple f-DOPA coating, therefore, led to structurally hetero-
geneous rough films of perfluorinated materials without any
further treatments, which definitely contributed to reduction of
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Chem. Commun., 2014, 50, 11649--11652 | 11651