Yifan Si1,2, Zhichao Dong1, Lei Jiang1,2. 1. CAS Key Laboratory of Bio-inspired Materials and Interfacial Sciences, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China. 2. Key Laboratory of Bio-inspired Smart Interfacial Science and Technology of Ministry of Education, Beijing Advanced Innovation Center for Biomedical Engineering, School of Chemistry, Beihang University, Beijing 100191, China.
Abstract
Bioinspired designs of superhydrophobic and superhydrophilic materials have been an important and fascinating area of research in recent years for their extensive potential application prospects from industry to our daily life. Despite extensive progress, existing research achievements are far from real applications. From biomimetic performance to service life, the related research has faced serious problems at present. A timely outlook is therefore necessary to summarize the existing research, to discuss the challenges faced, and to propose constructive advice for the ongoing scientific trend. Here, we comb the process of development of bioinspired superhydrophobic and superhydrophilic materials at first. Then, we also describe how to design artificial superhydrophobic and superhydrophilic materials. Furthermore, current challenges faced by bioinspired designs of superhydrophobic and superhydrophilic materials are pointed out, separately, and the possible solutions are discussed. Emerging applications in this field are also briefly considered. Finally, the development trend within this field is highlighted to lead future research.
Bioinspired designs of superhydrophobic and superhydrophilic materials have been an important and fascinating area of research in recent years for their extensive potential application prospects from industry to our daily life. Despite extensive progress, existing research achievements are far from real applications. From biomimetic performance to service life, the related research has faced serious problems at present. A timely outlook is therefore necessary to summarize the existing research, to discuss the challenges faced, and to propose constructive advice for the ongoing scientific trend. Here, we comb the process of development of bioinspired superhydrophobic and superhydrophilic materials at first. Then, we also describe how to design artificial superhydrophobic and superhydrophilic materials. Furthermore, current challenges faced by bioinspired designs of superhydrophobic and superhydrophilic materials are pointed out, separately, and the possible solutions are discussed. Emerging applications in this field are also briefly considered. Finally, the development trend within this field is highlighted to lead future research.
Nature is always the wise
mentor of humans. Learning from nature
makes for rapid development of our science and technology. Bionics
is born out on the basis of this background, which is gradually becoming
an interdisciplinary central science research field. Superhydrophobic
and superhydrophilic materials[1−7] are the most representative biomimetic examples in surface and interfacial
research of physical chemistry. The discovery and development of superhydrophobic
and superhydrophilic materials led to a series of innovations and
opened the floodgates to new research.When a water drop is
placed on a solid surface, it tends to spread
toward a lower energy state. Then, there is a water contact angle
(WCA) measured at the edge (solid–liquid–air three-phase
contact line) of each droplet. Different WCAs can reflect the wettability
of the solid surface. In 1805, Thomas Young,[8] a pioneer scientist, proposed the concept of the contact angle of
a liquid and established Young’s equation to define the notion
of surface wettability. Some surfaces with extreme wettability have
attracted much of the attention of later scientists,[2,9−13] which are the above-mentioned superhydrophobic and superhydrophilic
surfaces, defined with a WCA larger than 150° or smaller than
10°, respectively.[14] The water drop
can stand on the superhydrophobic surface like a ball but spread completely
forming a water film on the superhydrophilic surface. A surface’s
morphology (surface roughness) and intrinsic material properties (surface
energy) cooperatively decide its wettability.[1,9,15]As shown in Figure a, how surface roughness and surface energy
affect surface wettability
is determined by the intrinsic wetting threshold (IWT) of the water,
which is the boundary of the wettability between hydrophilic and hydrophobic
when the liquid is deposited.[4,9] When the intrinsic WCA
(θ) on a flat solid surface is larger than θIWT, superhydrophobic surfaces can
be obtained by increasing the surface roughness. Conversely, when
the intrinsic WCA (θ) on a flat solid surface is smaller than θIWT, superhydrophilic
surfaces can be obtained. The relationship between surface roughness
and apparent contact angle (θa) can be described
by the Koch curve fractal formula:[15,16]. f2 is the
fraction of the air surface under the water droplet, and f1 + f2 = 1. L and l are the upper- and lower-limit scales of
the surface, respectively, and D is the fractal dimension.
Surface roughness and apparent contact angle have close ties to the
value of L/l. Thus, the existence
of a nanoscale structure promotes superwettability. It is worth mentioning
that 90° is considered as the intrinsic wetting threshold of
water according to Young’s equation. However, by considering
the interphase water molecular interactions and structures, a lower
intrinsic wetting threshold of 65° is proposed. The WCA of 65°
has also been proven to be the limit between hydrophilicity and hydrophobicity
when increasing surface roughness to construct superhydrophilic or
superhydrophobic surfaces.[9,17,18] It is the key criteria to construct artificial superhydrophilic
and superhydrophobic materials.
Figure 1
(a) Intrinsic wetting threshold (θIWT) of water, which
is regarded as the limit
between hydrophilicity and hydrophobicity. When the intrinsic WCA
(θ) on a flat solid surface is larger than θIWT, superhydrophobic surfaces can
be obtained by increasing the surface roughness. Conversely, when
the intrinsic WCA (θ) on a flat solid surface is smaller than θIWT, superhydrophilic
surfaces can be obtained. (b) Rapid increase of research interest
(number of papers) on the topic of “superhydrophobic”
and “superhydrophilic” materials.
(a) Intrinsic wetting threshold (θIWT) of water, which
is regarded as the limit
between hydrophilicity and hydrophobicity. When the intrinsic WCA
(θ) on a flat solid surface is larger than θIWT, superhydrophobic surfaces can
be obtained by increasing the surface roughness. Conversely, when
the intrinsic WCA (θ) on a flat solid surface is smaller than θIWT, superhydrophilic
surfaces can be obtained. (b) Rapid increase of research interest
(number of papers) on the topic of “superhydrophobic”
and “superhydrophilic” materials.With the rapid development of nanotechnology at the beginning
of
the 21st century, basic scientific research started moving toward
practical applications. Therefore, the research of superhydrophobic
or superhydrophilic materials also enters a new period of rapid growth.
By searching in the ISI (Institute for Scientific Information) Web
of Science using the topic of “superhydrophobic” or
“superhydrophilic”, we can observe an accelerating increase
for the number of papers in 2004 (Figure b). Under amazing development momentum, some
fundamental problems still hide. As for superhydrophobic materials,
weak mechanical stability is the true crux of this topic.[14,19,20] Scientists have taken notes of
this point, and some research has also been carried out. So far, however,
no practical solutions have been proposed. More seriously, no authoritative,
standard, or effective evaluation system is established in this field.
The challenges in superhydrophilic materials are more obvious. The
ability of artificial superhydrophilic materials to imitate nature
is limited.[4,21] In addition, insufficient application
development of superhydrophilic materials is another bottleneck. How
to overcome these difficulties in the future is the main focus of
this Outlook.In this Outlook, we first briefly introduce the
processes of the
development of bioinspired superhydrophobic and superhydrophilic materials,
mainly focused on research during the past two decades. On the basis
of this understanding, in the following sections, the designs of bioinspired
superhydrophobic and superhydrophilic materials have been summarized.
Their respective challenges are pointed out, and the potential solutions
are also put forward. In Section , recently emerging applications of bioinspired superhydrophobic
and superhydrophilic materials are discussed as well. Finally, we
briefly present our personal view of the open questions, remaining
challenges, and development trend of this field.
Bioinspired
Superhydrophobic and Superhydrophilic
Processes of Development
Bioinspired Superhydrophobic
Processes
Researchers found that duck feathers cannot be
wetted by water a
long time ago (Figure a).[22] The modern study of superhydrophobic
surfaces has enjoyed a resurgence in the past two decades with the
rise of bionics. Scientists try to detect the mechanism behind the
lotus effect with the aid of scanning electron microscopy. In 1997,
the microscale papillae of lotus leaves were identified as the key
to its water-repellency (Figure b).[23] For further exploration,
dual-scale micro-/nanostructures of lotus leaves allowing the achievement
of both high apparent contact angles and low adhesion were demonstrated
by Jiang et al. in 2002 (Figure c).[15] This was the first
work to reveal that the multiscale structure is crucial to superhydrophobicity.
In the same year, Jiang et al. also discovered that the rice leaf
displayed anisotropic wettability (Figure d).[15] Rice leaf
papillae are parallel to the leaf edge and randomly in the other direction.
In 2004, Gao and Jiang[24] found that the
special hierarchical structure of superhydrophobic water strider legs
(Figure e) is the
main reason for water striders’ standing effortlessly and moving
quickly on water. Researchers reported the second anisotropic creature
surface in 2007, namely, butterfly wings (Figure f).[25] A water
droplet easily rolls off the wings along the outward direction of
the body but pinned in an inward direction, which resulted from the
direction-dependent arrangement of flexible nanotips on nanostripes
and microscales overlapped on the wings.
Figure 2
Time-line of bioinspired superhydrophobic and superhydrophilic
process of development. (a) Duck feather.[22] (b) Lotus effect.[23] (c) Micro–nano
cooperative lotus effect.[15] (d) Rice leaf.[15] (e) Legs of water striders.[24] (f) Butterfly wings.[25] (g) Rose
effect.[26] (h) Salvinia molesta.[27] (i) Bacterial biofilm.[28] (j) Collembola.[29] (k) Precorneal tear film. (l) Fish scale.[30] (m) Spider Silk.[31] (n) Shark skin.[32] (o) Cactus.[33] (p)
Tree frog.[34] (q) Lizard skin.[35] (r) Nepenthes alata.[36] Copyright 2002, 2009, 2010, 2013 Wiley; 2004,
2010, 2012, 2016 Nature publishing group; 2007, 2012 Royal Society
of Chemistry; 2008 American Chemical Society; 2015 Royal Society;
2011 PNAS; and 2012 Springer.
Time-line of bioinspired superhydrophobic and superhydrophilic
process of development. (a) Duck feather.[22] (b) Lotus effect.[23] (c) Micro–nano
cooperative lotus effect.[15] (d) Rice leaf.[15] (e) Legs of water striders.[24] (f) Butterfly wings.[25] (g) Rose
effect.[26] (h) Salvinia molesta.[27] (i) Bacterial biofilm.[28] (j) Collembola.[29] (k) Precorneal tear film. (l) Fish scale.[30] (m) Spider Silk.[31] (n) Shark skin.[32] (o) Cactus.[33] (p)
Tree frog.[34] (q) Lizard skin.[35] (r) Nepenthes alata.[36] Copyright 2002, 2009, 2010, 2013 Wiley; 2004,
2010, 2012, 2016 Nature publishing group; 2007, 2012 Royal Society
of Chemistry; 2008 American Chemical Society; 2015 Royal Society;
2011 PNAS; and 2012 Springer.The adhesion force of superhydrophobic surfaces is also of
great
interest to scientists. In the following year, a superhydrophobic
rose petal (Figure g) with high adhesion force[26] was reported.
A water droplet can stand on the surface of the petal with spherical
shape, but it cannot roll off even when the petal is turned upside
down. This phenomenon is also called the “petal effect”.
Another unique superhydrophobic plant is discovered in 2010, called Salvinia. The Salvinia leaf (Figure h)[27] offers a novel mechanism for long-term air retention. Miraculously,
the terminal hair lacks the wax crystals and forms hydrophilic patches.
Authors demonstrate that these hydrophilic patches can stabilize the
air layer by pinning the air–water interface, which is also
called the “Salvinia effect”. The discovery
of these characteristic creature surfaces mentioned above has promoted
a deep understanding of superhydrophobicity. The revelation of an
intrinsic mechanism has also enriched the theory and guided the bioinspired
designs of artificial superhydrophobic materials.Aizenberg
et al.[28] reported a surprising
observation that Bacillus subtilis biofilm colonies
and pellicles (Figure i) were shown surpassing the repellency toward water and liquids
with lower surface tension. This nonwetting property benefits from
a synergistic effect of ECM (extracellular matrix, the slimelike “cement”
of biofilm) composition, multiscale roughness, reentrant topography,
and so on. Then, researchers (in 2012) found that springtails (Collembola)[29] (Figure j) can live in water and oil environments. It is because they
have robust surface plastrons consisting of hexagonal or rhombic comblike
patterns to capture an air cushion formed around them.
Bioinspired Superhydrophilic Processes
The bioinspired
superhydrophilic concept has not been popularized
for a long time. The essential reason is the lack of practical applications.
Long before, scientists found that tears can spread, forming a film
to protect human eyes (Figure k). By 2009, the discovery of superhydrophilic fish scales
(Figure l) opened
a new door for bioinspired superhydrophilic research.[30] Fish scales display good superoleophobicity under water,
which originates from the water-phase hierarchical micro-/nanostructures
structures. The oil drop shows low adhesion on the surface, so that
fish can keep clean under water. This work makes underwater self-cleaning
become one of the most important applications of superhydrophilicity.
In the past decade, intriguing wetting phenomena on the superhydrophilic
creature surfaces have been discovered continuously. Zheng and co-workers[31] have demonstrated that spider silk (Figure m) can collect water
efficiently from air in 2010. A unique silk structure with spindle-knots
results in a surface energy gradient and a difference in Laplace pressure
to achieve continuous directional water condensation around spindle-knots.Shark skin (Figure n) has been detected with an underwater drag reduction ability a
long time ago. In 2012, researchers also found its superhydrophilicity
similar to that of fish scales.[32] In the
same year, anther water-collection creature, the cactus, was in scientists’
spotlight (Figure o). Opuntia microdasys (cactus) have an efficient
fog collection system similar to spider silk.[33] Three main reasons, gradient of the Laplace pressure, surface-free
energy, and multifunction integration, endow the cactus with an efficient
fog collection ability. Tree-frog toe secretion (Figure p) can wet all kinds of surfaces,[34] and then adhere to the surfaces. The high-adhesion
wetting state of a tree-frog toe profits from its microstructure and
superhydrophilicity. In 2015, scientists found that special skin adaptations
enable the Texas horned lizard[35] (Figure q) to access water
sources such as moist sand and dew. Their skin is capable of directionally
transporting water without external energy input. Another classical
creature surface with a continuous directional water transport ability
found more recently is the peristome surface of Nepenthes
alata(36) (Figure r). The multiscale structure of the peristome
surface optimizes and enhances capillary rise in the transport direction,
and prevents water backflow in the reverse direction. This discovery
can be used to design bioinspired fluid-transport superhydrophilic
systems for practical applications. In general, according to all this
research, development of bioinspired superhydrophilic processes has
entered a new historical stage.
Current
Developments and Challenges of Designs
of Superhydrophobic and Superhydrophilic Materials
The most
critical part of bioinspired superwetting material design
is synergistic action between hierarchical dual-scale structures and
the intrinsic material properties.[1,9,14] Basically, two biomimetic principles can be summarized:
Hierarchical dual-scale structures have played a key role in determining
the wetting property. The arrangement, orientation, and curvature
of micro-/nanoscale structures can control the motion of the liquid.
Current Developments and Challenges of Designs
of Superhydrophobic Materials
Scientists have detected microscale
papillae (Figure a)
on the lotus leaf as early as 1997[23] and
deduced that this structure plays an important role in superhydrophobicity.
In 2002, the micro-/nanostructure (Figure b) on lotus leaves was uncovered further.[15] The synergistic action of the micro-/nanostructure
makes the water droplet tend to stand on the surface in the Cassie–Baxter
state (Figure c).
The water drop cannot penetrate into small cavities between rough
dual-scale structures. The air is trapped in these cavities,[22] resulting in a solid–air–liquid
heterogeneous interface. Academics believe that the main contribution
of the microscale structure is to enhance the mechanical stability
of the superhydrophobic surface, and the aim of the nanoscale structure
is to retain the Cassie–Baxter state on the superhydrophobic
surface.
Figure 3
Models of the evolution from superhydrophobicity to superamphiphobicity.
(a) Microscale synapse model. (b) Micro-/nanoscale synapse model.
(c) Cassie–Baxter state model. (d) Various developed artificial
micro-/nanoscale models. (e) Pyramid micro-/nanoscale model shows
optimal comprehensive performance. (f) Classical superamphiphobic
models from T-shaped to mushroom-shaped to triply reentrant structure.
Models of the evolution from superhydrophobicity to superamphiphobicity.
(a) Microscale synapse model. (b) Micro-/nanoscale synapse model.
(c) Cassie–Baxter state model. (d) Various developed artificial
micro-/nanoscale models. (e) Pyramid micro-/nanoscale model shows
optimal comprehensive performance. (f) Classical superamphiphobic
models from T-shaped to mushroom-shaped to triply reentrant structure.On the basis of this understanding,
scientists have designed a
series of different micro–nano dual-scale superhydrophobic
materials (Figure d). Regular structures (cube, sphere, pyramid, and so on) can be
fabricated through physical methods, such as laser processing or lithography.[37,38] After chemical modification, various regular micro–nano dual-scale
superhydrophobic materials can be obtained. In addition, irregular
micro–nano dual-scale superhydrophobic materials can be prepared
by chemical methods including electrodeposition, sol–gel process,
hydrothermal method, and so on.[39,40] As to micro-/nanowires
or micro-/nanofibers, the electrospinning technique is one of the
best choices.[41] Dual-scale amorphous superhydrophobic
(carbon) materials can be achieved by incomplete combustion of long-chain
alkane.[42]We have summarized some
typical works around the development of
bioinspired superhydrophobic and superhydrophilic materials. In 2004,
Jiang et al.[43] reported one kind of lotus-leaf-like
superhydrophobic polystyrene film with a novel composite structure
consisting of porous microspheres and nanofibers by the versatile
electro-hydrodynamic method. Later scientists also tried to construct
a lotus-leaf-like artificial surface to obtain a similar superhydrophobicity.[44,45] One work made new progress recently by Lee et al.[46] They prepared artificial rice leaf surfaces in which nanoporous
multilayers were of a wavy microstructure. An increase in nanostructure
roughness led to a transition in the dynamic water droplet anisotropic
wetting states. Research about water strider legs is mostly about
the mechanism. Bioinspired designs of water striders can achieve microrobots
who can walk on the water surface.[47,48] Herein, Tan
and co-workers[49] presented a versatile
route via selective surface functionalization and subsequent electroless
deposition to duplicate the intact 3D organic butterfly wing scales
on metals such as cobalt, copper, nickel, and so on. Malvadkar et
al.[50] reported an array of poly(p-xylylene) nanorod film with anisotropic wetting behavior
by means of a pin-release droplet ratchet mechanism. The nanofilm
achieves directional transport of microliter droplets on a smooth
surface. In 2010, lotus/petal effect surfaces were successfully fabricated.
With the control of UV irradiation and heating profiles of the photochromic
compound, surface wettability can be controlled.[51] As for the Salvinia leaf with a fine eggbeater
shape, it is very difficult to construct this unique structure through
common physical or chemical methods. However, with the aid of advanced
3D printing technology, Yang et al.[52] have
reported a superhydrophobic eggbeater structure with controllable
surface morphology. Through the research on superoleophobicity creature
surfaces, scientists revealed that only one certain type of structure
with reentrant geometries is appropriate for constructing superoleophobic
surfaces (Figure f).
Tuteja et al.[53] first came up with the
T-shaped reentrant structure, which will not only strengthen the stability
of the superamphiphobic surface but also facilitate the choice of
corresponding oleophilic materials for preparing superamphiphobicity.
Furthermore, Kim et al.[54] designed one
kind of mushroom-shaped doubly reentrant structure. This surface with
doubly reentrant structure can repel completely wettable liquid, where
even perfluorohexane can bounce off this surface. Most recently, using
two-photon polymerization 3D printing technology, Gu et al.[55] fabricated triply reentrant arrays with super-repellence
from water to various organic liquids successfully. Even after treatment
by oxygen plasma, the superamphiphobicity of the triply reentrant
array surface can be kept well. This work proposed an advanced method
to construct a complex bioinspired reentrant structure. Further, except
for superhydrophobicity and superoleophobicity, in different media,
64 unique wetting states are achieved totally through different combinations
of water, oil, and air.[2,9]The tremendous application
potential of bioinspired superhydrophobic
materials in areas such as water repellence, self-cleaning, anti-icing,
drag reduction, and corrosion resistance[1,10,14,56] will make significant
changes in our daily life and industry. Despite significant progress,[57−60] bioinspired superhydrophobic materials were never as widespread
in fact as we expected. It is because two core issues have not been
addressed yet, which are chemical stability and, especially, mechanical
durability.[19] Micro-/nanostructures on
the superhydrophobic surface are highly susceptible to mechanical
wear, while surface compositions may also be altered by UV or acid–base
conditions.[20,61] Both processes can lead to the
loss of superhydrophobicity. Lots of scientists have committed to
resolve this problem. From the structural stability aspect, the micro–nano
dual-scale pyramid (Figure e) is considered the best choice.[62−64] The pyramid
structure has a large contact area with the substrate to resist a
greater degree of wear, while the acuminate top can reduce contact
area with liquid to increase the WCA. However, it is not realistic
to promote superhydrophobic materials with micro–nano dual-scale
pyramids in extensive areas because of the complex preparation and
high cost. Thus, the most mainstream approaches are a self-healing
superhydrophobic material[40,65−67] and a superhydrophobic surface with bonding layer.[60,61] These two approaches bring the research into a new stage but not
the end.Scientists who professionally
engaged in studying the durability
of superhydrophobic materials all face a common confusion, which is
the lack of a unified, authoritative, and comprehensive evaluation
system. At present, several strategies have been used to test the
durability of superhydrophobicity, such as the abrasion test, tape
peeling, blade scratching, sand abrasion, water jet tests, ultraviolet
radiation, high/low temperature, and acid–base marinating.[19,61,68] However, there is no consistency
about the test conditions such as types of abradant, applied pressure,
velocity, irradiation intensity, and so on. As a result, the lack
of standardization always makes comparison of different research results
impossible. In addition, how to evaluate the durability of superhydrophobic
materials is also an issue. By only using WCA, it is insufficient
and unconvincing. If these problems cannot be solved urgently, all
current research is blind and unavailing in this field. Therefore,
it is necessary and urgent to develop a unified, authoritative, and
comprehensive characterization and evaluation system. In addition
to developing new test methods, we need to introduce tribology knowledge
to analyze, solve and guide the design of bioinspired superhydrophobic
materials. The related research is still basically in the blank condition.
Then, WCA, SA, advancing/receding contact angle, adhesive force, and
integrity of microtopography should all be taken into evaluation systems.[69] The best solution is to develop a highly integrated
testing system which can test all-around surface wettability. With
the aid of an external humidity/temperature control system, gas circuit
system, and super-high-speed camera, liquid volatilization and icing
processes can be studied via this integrated system in different atmospheres
or in vacuum. Ultimately, professional evaluation institutions have
to be instituted.
Current Developments and
Challenges of Designs
of Superhydrophilic Materials
The research of bioinspired
superhydrophilic materials can be traced back to the research of the
cornea of the human eye. Water (tears) can spread completely forming
a water film to eliminate light scattering. Scientists have established
some relatively mature fabrication methods, which can be divided into
two categories: physical methods and chemical methods (Figure a).
Figure 4
(a) Common superhydrophilic
surface fabrication physical and chemical
methods. (b) Water spreading process on superhydrophilic interfaces
with the help of 2D capillary forces.[75] (c) Fish-scale-inspired artificial superhydrophilic/underwater superoleophobic
surfaces.[30] (d) Conical spine structure
of cactus spine,[33] spindle-knot fiber structure
of spider silk,[31] and in situ observation of water transport in carbon nanotubes.[80] (e) Through continual liquid deposition, dyed water could
unidirectionally spread in one single direction and pin in all the
others on superhydrophilic peristome-mimetic surfaces. Deposited liquid
also could flow downward along the spiral.[81] Copyright 2016, 2017 Wiley; 2010, 2012 Nature publishing group;
and 2004 American Chemical Society.
(a) Common superhydrophilic
surface fabrication physical and chemical
methods. (b) Water spreading process on superhydrophilic interfaces
with the help of 2D capillary forces.[75] (c) Fish-scale-inspired artificial superhydrophilic/underwater superoleophobic
surfaces.[30] (d) Conical spine structure
of cactus spine,[33] spindle-knot fiber structure
of spider silk,[31] and in situ observation of water transport in carbon nanotubes.[80] (e) Through continual liquid deposition, dyed water could
unidirectionally spread in one single direction and pin in all the
others on superhydrophilic peristome-mimetic surfaces. Deposited liquid
also could flow downward along the spiral.[81] Copyright 2016, 2017 Wiley; 2010, 2012 Nature publishing group;
and 2004 American Chemical Society.Physical methods can be applied to create regular patterned
microstructures,
such as laser treatment,[70] and to obtain
a new relatively homogeneous layer by physical vapor deposition or
spray coating.[71] For instance, Vorobyev
and Guo[70] created a novel surface pattern
that transformed regular silicon to being superhydrophilic using high-intensity
femtosecond laser pulses. Because of the superhydrophilicity, water
can spread vertically uphill against gravity. The driving force of
water motion is the supercapillary effect benefited from the surface
structures. Zheng and co-workers[72] have
reported superhydrophilic colloidal TiO2/SiO2 nanoparticle coatings in a spray-and-dry way. Li et al.[71] fabricated one kind of long-time stable superhydrophilic
hierarchical TiO2 ordered by pulsed laser deposition and
subsequent annealing. This TiO2 hierarchical particle array
exhibited superhydrophilicity with a water contact angle of nearly
0° without further UV irradiation.As for chemical methods,
it is more beneficial to obtain complex
precise structures in micro-/nanoscale. The chemical method can also
create hydrophobic functional groups on the surface through external
field stimulation, such as UV illumination. TiO2 has become
one of the most famous “photoresponsive” wetting materials
since the discovery of its photoinduced superhydrophilic property
was reported in Nature.[73] Recently, superhydrophilic/-hydrophobic
fabric with self-propelled directional wetting patterns controlled
by UV illumination and temperature has been successfully created by
a one-step coating process involving nano-TiO2.[74] Random frameworks can also be generated by chemical
methods such as etching/oxidation, layer-by-layer, sol–gel
methods, and so on. Zhu et al.[75] reported
a simple three-step treatment method to generate superamphiphilic
silicon wafer surfaces with contact angles near 0° for both water
and typical organic liquids. Taking advantage of lateral force mode
(LFM) atomic force microscopy images, the alternating hydrophilic
and hydrophobic nanodomains can be detected. The mechanism has also
been revealed to explain its superamphilicity. Liquids infiltrate
the hydrophilic (or hydrophobic) nanodomains giving rise to a 2D capillary
effect (Figure b),
which pulls liquids across the nanodomains continuously. By making
use of these superamphiphilic silicon wafer surfaces, uniform organic
thin films were generated in both water and organic solvent. Most
recently, Zheng and co-workers[76] have reported
a superhydrophilic cellulose membrane through an electrospinning cellulose
acetate method followed by a process of hydrolysis inspired from Chinese
Xuan papers. Water can spread out rapidly along the X–Y 2D plane but seldom permeates through
the Xuan papers. This is because of the multilayered spreading mechanism
resulting from the layered anisotropic micro-/nanofibrous structures.After being proposed, the concept of superhydrophilicity has not
been widely dispersed and studied. This is because the potential applications
have not been discovered for a long time. The mystical nature gives
us answers again, which brings a new revolution for bioinspired superhydrophilic
materials research. In 2009, Liu et al. found that fish scales showed
natural superhydrophilicity.[30] Superhydrophilic
fish scales displayed a unique underwater superoleophobicity. The
reason is that the water layer can be trapped within the micro-/nanostructures
of fish scale surfaces. By virtue of this property, fish can keep
clean under water showing a great antifouling property. Bioinspired
superhydrophilic/underwater superoleophobic materials are also achieved
in this work. Superhydrophilic/underwater superoleophobic artificial
polyacrylamide film with fish-scale structures and silicon surface
with microstructure or micro-/nanostructure (Figure c) has been fabricated successfully. These
studies extended superwettability research to oil/water/solid triphasic
systems. Thus, the underwater antifouling property of the superhydrophilic
surface has drawn increasing attention. On the basis of this understanding,
researchers further explore the oil/water separation property of superhydrophilic/underwater
superoleophobic materials. Xue et al.[77] prepared a novel superhydrophilic and underwater superoleophobic
polyacrylamide hydrogel-coated mesh which can achieve selective separation
of water from oil/water mixtures with high separation efficiency.From the perspective of bioinspired designs, the relevant superhydrophilic
materials for antifouling and oil/water separation are concentrated
in 2D films or membranes. One-dimensional superhydrophilic materials
seem to have not much room for development. A turning point came in
2010 and 2012; the discovery of the unique liquid transport ability
of spider silk[31] and cactus[33] opens the new door for the research of 1D superhydrophilic
fibers and channels (Figure d). The combination of Laplace pressure and surface energy
resulted in controllable transport of liquid by designing 1D superhydrophilic
interfaces. It is also the core guiding ideology of bioinspired designs
of 1D superhydrophilic materials. Bai et al.[78] designed a series of artificial spider silks with spindle-knots
to drive tiny water drops (tens of picoliters) with controllable transport
by optimizing the cooperation of curvature, chemical composition,
and roughness gradients on fiber surfaces. The key for artificial
spider silk bioinspired designs for fog or water collection is to
construct a spindle-knot structure, while the main aim of artificial
cactus bioinspired designs is to obtain microscale cone structures.
Ju and co-workers[79] bioinspired designed
a dual-gradient one-dimensional fog collector, namely, conical copper
wire with gradient wettability. With the help of field-emission scanning
electron microscopy, scientists detected that water can transport
in carbon nanotubes.[80] The WCAs in carbon
nanotubes range from 5° to 15°. On the basis of this pioneering
research, superhydrophilic nanochannel materials have attracted more
and more attention in recent years. These great works have opened
up a favorable new situation of bioinspired designs of superhydrophilic
materials.Now, the main cutting-edge focus for bioinspired
designs of superhydrophilic
materials has become liquid’s continuously unidirectional transport
inspired by lizard skin[35] and Nepenthes
alata.[36] Most recently, Li et
al.[81] fabricated mimicking biological surfaces
with sophisticated structures through the stereolithography fabrication
method (Figure e).
Liquids with varied surface tensions and viscosities can spontaneously
propagate in a preferred single direction. The overflow-controlled[64,82] unidirectional transport mechanism has been revealed by microcomputerized
tomography scanning observations. Furthermore, this group found that
the impact of a water drop can achieve unidirectional transport on
the Nepenthes alata inspired superhydrophilic surface.[83]The research of bioinspired designs of
superhydrophilic materials
has good momentum of development. However, the problems beneath the
prosperous surface are pretty obvious. The performance of artificial
superhydrophilic materials cannot reach natural superhydrophilic materials.
For example, the water collection test of artificial 1D superhydrophilic
materials is under high-humidity atmosphere. This condition can hardly
exist in nature. Moreover, it is hard to simulate the fine structure
on the creature surface of artificial superhydrophilic materials.
Advanced 3D printing technology could resolve, to a certain extent,
this challenge.[84] However, the scale of
printed structures is always much larger than the scale of the creature
surface structure. Therefore, where is the future of bioinspired superhydrophilic
materials? At first, scientists should make an earnest effort to find
out new materials or methods to reach the properties of natural creatures.
Developing high-precision 3D printer and laser writing technology
is another good solution. Second, we must never cease to work for
new applications of superhydrophilic materials from a static to dynamic
fluid and from 1D to 3D. Combining superhydrophilicity and other material
properties, such as humidity-response, is a good approach.[85] Finally, the reversible rapid wettability transition
between superhydrophobicity and superhydrophilicity is a promising
research field.
Emerging Applications of
Bioinspired Superhydrophobic
and Superhydrophilic Materials
Scientists and engineers have
investigated the utility of superhydrophobic
and superhydrophilic materials in different fields. Nowadays, a great
number of applications have been commercialized. Here, a systematic
summary has been concluded in this section. We try to focus on both
applications that take advantage of a single wetting state or two
extreme wetting states.Oil–water separation is of great
importance for industrial
water purification and oil spill collection. Both superhydrophobic
and superhydrophilic materials have proven to be highly efficient
for this purpose.[86−88] After the development of recent years, the research
of oil–water separation has entered the liquid–liquid
separation stage.[89,90] On the basis of the θIWT for different liquids, the membranes
with different wettabilities can be further applied to separate two
different organic liquids. Furthermore, Li and co-workers[91] achieved tiny water-in-oil droplet separation
into pure water and oil droplets via a “go-in-opposite-ways”
mechanism on curved bioinspired peristome-mimetic surfaces without
energy input (Figure a). The separations of tiny water-in-oil droplets, emulsions, and
liquid/air will continue to be the focus of the future research.[89,92−95] Superhydrophilic materials show dramatic antifogging behavior, where
the water droplets will instantaneously spread to form a thin liquid
film. It is interesting that, inspired by mosquito compound eyes (Figure b), superhydrophobic
materials also display great antifogging behaviors, which can rapidly
expel condensed droplets from their surfaces.[96] Densely packed micro-ommatidia structures covered by hexagonal nanonipples
resulted in this ability of mosquito eyes.[97] The synergistic effect of wettability and surface topography can
regulate the surface bioadhesion ability by cytophilic interactions
and a size-matching mechanism (Figure c).[98] The surfaces with
great bioadhesion ability are applicable for cancer detection. Superhydrophilic
nanowire arrays can selectively capture circulating tumor cells while
inhibiting the adhesion of normal blood cells.[98] Bioinspired superhydrophobic surfaces can be used to deliver
analytes to Raman-sensitive sites in highly diluted fluids (Figure d). The essential
reason is that the solution becomes increasingly concentrated during
the no-pinning evaporation process.[9,99] Improving
biocompatibility of superwetting sensors and extending the range of
usable fluids will be the major concerns. Another well-known commercial
application of bioinspired superhydrophobic and superhydrophilic materials
is self-cleaning (Figure e). Superhydrophobic materials are mainly aimed at solid pollutants.[23] However, superhydrophilic materials are mainly
aimed at liquid pollutants.[100] Combining
advantages of the two together to make omnipotent self-cleaning superwetting
materials is significant. As mentioned in earlier sections, bioinspired
superhydrophobic and superhydrophilic materials display a unique water
collection property (Figure f). How to improve water collection efficiency under a low-humidity
environment and how to prevent water evaporation are open questions.
The novel green printing based on superoleophilic nanomaterials on
superhydrophilic plate substrates has solved high-cost and environmental
pollution problems (Figure g). Regulating the morphology and wettability of printed materials
can achieve the contact line of the aqueous protecting liquid. Then,
the printed ink microdroplet pinned on the nonprinted and printed
regions results in high-quality images with fine resolution.[101] Liquid unidirectional transport on a solid
surface with special wettability is a very unique and intriguing phenomenon
(Figure h). The driving
mechanism of liquid unidirectional transport can be divided into four
parts: Laplace pressure, gradient wettability, ratchet mechanism,
and capillary rise.[18,33,36,50,81,83,102,103] In general, asymmetric surface morphology and/or surface energy
make the force or resistance at the three-phase contact line of a
liquid uneven in different directions, thus driving the liquid in
a particular direction. However, a further application based on the
liquid unidirectional transport is insufficient. How to develop its
value behind the phenomenon in a smart microfluidic system, laboratory-on-a-chip
devices, and advanced biochemistry microreactor is the prime concern
of many scientists.[18,81,83,104,105]
Figure 5
Emerging applications
of superhydrophobic and superhydrophilic
surfaces in various fields. (a) Liquid–liquid separation.[91] (b) Antifogging.[97] (c) Bioadhesion.[98] (d) Sensors.[99] (e) Self-cleaning.[23] (f) Water collection.[79] (g) Printing.[101] (h) Liquid transport.[36] Copyright 2007, 2011, 2013, 2015, 2017 Wiley; 2016 Nature publishing
group; 1997 Springer; and 2013 Royal Society of Chemistry.
Emerging applications
of superhydrophobic and superhydrophilic
surfaces in various fields. (a) Liquid–liquid separation.[91] (b) Antifogging.[97] (c) Bioadhesion.[98] (d) Sensors.[99] (e) Self-cleaning.[23] (f) Water collection.[79] (g) Printing.[101] (h) Liquid transport.[36] Copyright 2007, 2011, 2013, 2015, 2017 Wiley; 2016 Nature publishing
group; 1997 Springer; and 2013 Royal Society of Chemistry.
Outlook
In this
Outlook, we have concluded the development of bioinspired
superhydrophobic and superhydrophilic progress. The renaissance in
this field, to a large extent, has been brought about by recent advances
in nanotechnology. The designs of bioinspired superhydrophobic and
superhydrophilic materials have also been summarized. The challenges,
opportunities, and solutions are mentioned in this section. It is
also worth it for us to pay attention to emerging applications of
superhydrophobic and superhydrophilic materials. As we have highlighted
in this outlook, superwetting materials with unprecedented properties
and functionalities can be generated and integrated into devices for
emerging applications.Although great progress has been made,
there are still some difficult
challenges to overcome. How can further impulses in the development
in this field be created? It is a tough question. Advanced 3D printing
technology could be a good solution. Three-dimensional printing technology
can rapidly, precisely prepare a bioinspired surface structure and
morphology similar to that of creature surfaces.[18,55,81,84] Compared with
traditional chemical or physical methods, 3D printing technology displays
great controllability, integration, and repeatability with low cost.
More importantly, 3D printing technology brings light to efficiently
construct superamphiphobic surfaces/substrates with specific delicate
structures with reentrant geometries, which display high theoretical
research and practical application values.[42,55,105−107] Although it is still
in its infancy, there are still some limitations, such as the size
of products or the choice of raw materials, but predictably it will
give play to enormous value in this field in the future.Throughout
the development of the superwetting field, we find that
the current research focus is moving from static droplets to dynamic
liquid flow.[11,18,64,108−112] Because liquids in nature tend to have a
certain velocity, the hydrodynamic properties or behavior of liquid
have gradually become a major concern in the design of superhydrophilic
and superhydrophobic materials, for example, the rapid, continuous,
spontaneous flow or transport of a large amount of liquid on the surface
or bulk phase of bioinspired superhydrophilic materials. The wetting/dewetting/impact
process of fluids on the edge of the superhydrophobic surface is another
hydrodynamic research topic in the future. The rapid transition between
superhydrophilic and superhydrophobic by regulating liquid is also
a new research hot-spot. Research on these problems is at an early
stage, and it is possible to greatly expand the application of bioinspired
superhydrophobic and superhydrophilic materials.In terms of fundamental
research, scientists should try to reveal
the deeper essence of nature. Direct imaging and recording have attracted
broad scientific attention for both theoretical research and practical
applications. Nano-X-ray CT, confocal laser scanning microscopy (CLSM),
environmental scanning electron microscopy (ESEM), and the ultra-high-speed
camera are pretty useful for the future research. Moreover, tremendous
effort should be concentrated on developing the highly integrated
3D imaging approaches with high resolution.[113] New theories and concepts should be explored from microscale to
nanoscale or molecular scale to understand delicate wetting phenomena.
Setting up a perfect theoretical system can provide guidance for us
to design required bioinspired superhydrophobic and superhydrophilic
materials. Finally, there are still a great deal of secrets to find
out from nature. With the joint efforts of researchers, the research
of bioinspired designs of superhydrophobic and superhydrophilic materials
will open a new page tomorrow.
Authors: Philipp Comanns; Gerda Buchberger; Andreas Buchsbaum; Richard Baumgartner; Alexander Kogler; Siegfried Bauer; Werner Baumgartner Journal: J R Soc Interface Date: 2015-08-06 Impact factor: 4.118
Authors: Yilun Li; Duy Xuan Luong; Jibo Zhang; Yash R Tarkunde; Carter Kittrell; Franklin Sargunaraj; Yongsung Ji; Christopher J Arnusch; James M Tour Journal: Adv Mater Date: 2017-05-12 Impact factor: 30.849
Authors: Emilia Irzmańska; Mariusz Siciński; Aleksandra Smejda-Krzewicka; Agnieszka Adamus-Włodarczyk; Magdalena Makowicz; Tomasz Gozdek Journal: Int J Environ Res Public Health Date: 2022-04-26 Impact factor: 3.390