Journal of Materials Science 【-逻*辑*与-】amp; Technology, 2020, 49(0): 106-116 doi: 10.1016/j.jmst.2020.02.022

Research Article

Superior anti-icing strategy by combined sustainable liquid repellence and electro/photo-responsive thermogenesis of oil/MWNT composite

Aeree Kim,a,*,1, Seonghyeon Kima,1, Myoung Huha, Hyungmo Kimb, Chan Leeb

a Department of Mechanical Engineering, Pohang University of Science and Technology (POSTECH), Pohang, 37673, Republic of Korea

b Korea Atomic Energy Research Institute (KAERI), Daejeon, 34057, Republic of Korea

Corresponding authors: * E-mail Kim).

First author contact:

1 These authors contributed equally as co-first authors to this work.

Received: 2019-10-21   Revised: 2020-01-30   Accepted: 2020-02-1   Online: 2020-07-15


This paper introduces an effective anti-icing strategy that uses passive anti-icing property and active de-icing functions concurrently. These dual capabilities can alleviate the icing problem more effectively than either a passive or active function alone. The developed material is a slippery liquid-repellent elastic conductor (SLEC); it is an organogel that is composed of multi-walled carbon nanotubes, oil, and polydimethylsiloxane. The SLEC maintains passive water-droplet sliding ability even on wet surfaces that frequently occur in cold conditions (e.g., during condensation and defrosting), suppresses ice nucleation, and shows ice adhesion strength as low as ~ 20 kPa. The SLEC releases heat when it is subject to electrical or photonic stimulation, and can therefore it can prevent ice formation and melt ice that has already formed on a surface. This material has sustainable liquid repellence by syneresis and replenishment; this ability ensures long-lasting anti-icing property, and results in exceptional durability. This durability is stable against mechanical damage. The superior dual anti-icing capabilities together with the sustainable and stable liquid repellence should generate synergistic effects, and yield a powerful anti-icing tool that can broaden the range of icing applications.

Keywords: Anti-icing ; De-icing ; Icephobic ; Soft conductor ; Self-healing ; Nanocomposite ; Liquid repellence

PDF (3532KB) Metadata Metrics Related articles Export EndNote| Ris| Bibtex  Favorite

Cite this article

Aeree Kim, Seonghyeon Kim, Myoung Huh, Hyungmo Kim, Chan Lee. Superior anti-icing strategy by combined sustainable liquid repellence and electro/photo-responsive thermogenesis of oil/MWNT composite. Journal of Materials Science & Technology[J], 2020, 49(0): 106-116 doi:10.1016/j.jmst.2020.02.022

1. Introduction

Ice formation and accretion on solid surfaces have caused tremendous economic losses and dangerous conditions [1,2]. Passive anti-icing materials to reduce these problems are effective and consume no energy [3,4]. Liquid-repellent surfaces, either generally superhydrophobic (SH) or slippery-liquid-infused porous surfaces (SLIPS), are generally considered to be ideal passive anti-icing surfaces due to one or more of the following capabilities [[5], [6], [7]]: (1) rejection of incoming liquids that can potentially become ice, before the liquids freeze (2) low ice adhesion strength (SIA) [8] (in general < 100 kPa [9]) so that natural forces (e.g., wind, vibration) can shed it, (3) delay of ice nucleation. [[10], [11], [12]]. Extremely low adhesion of water to the surface minimizes the contact time of the impinging drop (e.g., freezing rain) such that water can be shed before it freezes [7,13,14] or enables spontaneous jumping motion when condensate droplets merge. It decreases the speed of frost propagation and prevents the formation of a thick ice layer [4]. In addition, liquid-repellent surfaces generally delay ice nucleation time or lower the ice nucleation temperature by [5]: increasing the free energy barrier for ice nucleation [15], decreasing the water-solid contact area [16], and decreasing the viscosity of interfacial water [17]. However, icing is a complex process. The free-energy barrier can be reduced by many factors such as vibration or the presence of impurities, and variation in these factors can promote heterogeneous ice nucleation [18,19]. For these reasons, icing seems to be inevitable despite outstanding passive anti-icing by a liquid-repellent surface [1]. Therefore, passive anti-icing that exploits the properties of liquid-repellent surfaces has been unsatisfied, so elimination of ice accretion remains a challenge in the real world [20].

Liquid-repellent surfaces that also provide active heating could be more powerful to combat icing problems by combining passive and active anti-icing approaches synergistically [21]. With the liquid-repellence, the active heating ability of the surface can thaw the formed ice layer, and thereby recover the passive anti-icing property (i.e., liquid repellence) that was nullified by the formed ice covering the surface. Furthermore, during defrosting by heating, liquid-repellence allows melting water to form a slurry that easily slides off. Compared to non-liquid repellent surfaces, this process sheds water more quickly with less energy consumption, and leaves less melted water that can refreeze on the surface [22]. Recently, several hybrid passive-plus-active anti-icing surfaces that combine liquid repellence with active heating have been reported [20,23,24]. They usually involve electrically-conductive liquid-repellence, whereby the liquid repellent surface exploits an electrothermal or photothermal effect to generate heat that melts accreted ice [[23], [24], [25], [26]]. However, the reported surfaces have poor durability of liquid-repellence, and are fabricated by complex processes, which hinder their mass production and wide adoption in anti-icing applications [14,27].

Poor humidity tolerance of SH surfaces [28,29] or the drained lubricant in a SLIPS by icing/deicing cycles [30] or by volatilization [31,32,5] are the major impediments to their practical operation. These problems induce gradual loss of liquid-repellence locally or over the entire area. Several attempts to produce repairing/self-healing functionalities have made progress to extend the longevity of liquid repellence [31,[33], [34], [35], [36]]; examples from, Urata et al. [31], Zhu et al. [8], and Wang et al. [35] include organogels with regenerating liquid-repellent surfaces that can be replenished from inner matrices when damaged, and. Yan et al. [37] introduced a strategy for abrupt replenishment of lubricating layer onto locally depleted zone through well-designed internal pore structure in conjunction with surface structures. These strategies are desirable to extend the service lifetime. Other desirable attributes for practical anti-icing materials include multi-functionality, robustness against mechanical deformation, stability of liquid repellence against abrasion and scratching, and ease of fabrication with scaling availability [5,6].

In this paper, we report a highly durable liquid-repellent surface that has both passive anti-icing property and active de-icing capability. This surface is derived from a slippery liquid-repellent elastic conductor (SLEC) that has been previously pioneered by our group by mixing polydimethylsiloxane (PDMS) and oil with multi-walled carbon nanotubes (MWNTs) [38]. The developed SLEC is highly liquid-repellent (roll-off angle (ROA) < 5°) and can generate heat in response to electrical or photonic stimulation. These features of SLEC induce low SIA, retardation of ice nucleation, removal of contacting liquids, and de-icing, which are necessary in ideal anti-icing material [Fig. 1]. Above all, this surface has highly durable liquid repellence because the surface lubricant is self-healable and its lubricant supply can be easily replenished, so it has long service time. The SLEC has additional advantages such as simple fabrication process with easy scaling, low cost, high flexibility and stretchability, and stability of liquid-repellence against external stress. These hybrid anti-icing functions with practical advantages of the SLEC give it great application potential.

Fig. 1.   Comprehensive anti-icing strategy of SLEC. (a) Passive anti-icing property with (a-1) liquid repellence, and (b) active deicing function of the SLEC. FLIR and optical images when the SLEC is heated by (b-1) Joule heating, and by (b-2) laser illumination.

2. Experimental

2.1. Materials

Silicone oil was purchased from Sigma Aldrich (viscosity μ =500 cSt) or SFX KOREA (μ =1000 cSt). MWNTs (outer diameter 10-30 nm, inner diameter 5-10 nm, length 10-30 μm) were purchased from Nanostructured and amorphous materials Inc. PDMS (prepolymer and curing agent) (Sylgard 184) was purchased from K1 solution. Calcium sulfate powder (Drierite) and stainless steel 304 were obtained from Han Lab. And, Plastikote spray was provided by Korea Atomic Energy Research Institute.

2.2. Fabrication

The SLECs are composites composed of PDMS, MWNT and silicone oil, and were obtained by mixing 1 g of PDMS prepolymer, 0.1 g of curing agent, silicone oil, and MWNTs in a planetary mixer (Thinky ARE-310) for 8 min at 2000 rpm. The resulting homogeneously-dispersed paste was placed onto glass and degassed in a desiccator for 20 min. The degassed paste was pressed manually between two glass sheets that were separated by 500 μm using a spacer to achieve SLEC layer that had that thickness. Then a pressure of ~20 N was applied using a calibration weight. The glass-paste-glass combination was cured at 90 ℃ on a hot plate for 3 h. Subsequently, the cured SLECs were baked in a convection oven at 70 ℃ to induce self-lubrication (syneresis).

Composites were fabricated with different mixing ratios; samples were named to express the weight percent of each component (e.g., M7L90 refers to composite prepared by mixing 7 wt% MWNTs (M) and 90 wt% lubricant (L) of PDMS weight. SLECs with names that start with M11,M14, and M0 were made with silicone oil that had μ =500 cSt, and SLECS with names that start with M12 and M15 were made silicone oil that had μ =1000 cSt. All anti-icing experiments used the M11 and M14 series. The self-lubricating organogels (SLUGs) (i.e., M0L90, M0L60) are composites of PDMS/silicone oil [31].

For the comparison to demonstrate the advantages of the SLEC, two SH surfaces were prepared. A black SH surface (SHPo) was achieved by spray-coating Plastikote onto a Si wafer, then drying in air for 60 min, then heating in an oven at 340 ℃. The resulting film was 12 μm thick. Another SH surface (named SS) was achieved on stainless steel by electrochemical etching [39]. Detailed wetting information (i.e., syneresis behavior, contact angle) for samples tested here are presented in Section 1 of the supplementary information (SI).

2.3. Characteristics of passive anti-icing properties

2.3.1. Experiment to confirm the retention of liquid repellence

SLUG, SLEC, and SHPo liquid-repellent surfaces were prepared for use in two tests to prove the retention of liquid repellence. To test under a condition in which condensation occurred, SLEC with M11L90, SLUG (M0L90), and SHPo were put on a Peltier plate for 10 min at temperature TP = 0 ℃ in ambient temperature TA = 23 ℃ and relative humidity (RH) ~ 40 %. After condensation for 10 min., 10- μL water droplets were deposited to check whether the surface had retained liquid repellence.

For another test after defrosting, SLEC with M14L90, and SHPo surfaces were used. They were frosted on the Peltier plate at TP = -11 ℃ for ~ 25 min, at TA = 23 ℃ and RH ~ 60 %. After a frost layer had covered the entire surface, the Peltier plate was turned off, so the frost layer melted. Then 10-μL water droplets were deposited to test the liquid repellence.

2.3.2. Experiments for delay of ice nucleation

Tests of ice-nucleation effect on onset of freezing and frost propagation were conducted on the SLECs with M11L90, M14L90 and SHPo. Samples with water droplet of 10 u L was placed on a Peltier plate with a setting temperature of -5 ℃. The entire process was video-recorded to allow observation of the onset of freezing, and the frost propagation process.

2.3.3. Experiment for ice adhesion strength

The test to measure SIA used a generally used method [11,26]. The experimental setup was composed of a lab-built cooling system equipped with a Peltier plate, a load cell (1 kg, Bongshinloadcell) clamped onto an XY motorized stage. The sample with a plastic cuvette (1 cm × 1 cm cross section) filled with water was put on the Peltier plate. A cuvette filled with deionized water (1 cm × 1 cm × 2 cm) was placed on the sample and cooled on the Peltier plate at TP = -15 °C for > 2 h, after which the water in the cuvette had fully frozen. After the water froze, probe connected to the motorized stage was moved toward the bottom of the cuvette column at ~83 μm/s; the speed was controlled by Labview software. When the probe contacted the cuvette, the force that the probe exerted increased until the interface between substrate and the ice fractured; at that point, the force suddenly dropped. SIA was obtained from the peak force. This test was repeated > 3 times. The measured values were normalized by the cross-sectional area of the cuvette to yield SIA.

2.4. Characteristics of active anti-icing properties

2.4.1. General heat generation capability

Temperature profiles during heat generation in response to electronic or photonic stimulation were obtained using a thermal (FLIR) camera (Sections 5 and 6 in SI).

2.4.2. Defrosting by electro-thermal effect

To demonstrate the effect of thermogenesis under electronic stimulation, two experiments were performed: (1) application of voltage before ice formation (2) application of voltage after ice formation. Both experiments used the M14L90 SLEC and the M0L90 SLUG. For experiment (1), the SLEC and SLUG were placed on a Peltier plate at TP = -7 ℃, TA = 23 ℃ and RH ~ 58 %. Voltage (25 V) was applied from the onset. The samples were monitored for 30 min, then 10-μL water droplets were dropped onto the SLEC to confirm its liquid repellence.

For experiment (2), the samples were frosted for ~ 20 min by being placed on a Peltier plate at TP = -11 ℃, TA ~23 ℃ and RH ~ 60 %. When the entire surfaces were covered by ice, voltage (25 V) was applied to test the de-icing function.

2.4.3. Defrosting by photo-thermal effect

To demonstrate the effect of thermogenesis under photonic stimulation, a laser (532 nm, 500 mW/cm2) was used to illuminate the ice layers. SLEC (M14L60) and SLUG (M0L60) were held on a Peltier plate at TP = -3 °C at TA =25 °C and RH ~ 64 %. After the ice layer had formed for > 40 min, they were irradiated at one spot for 30 s. Optical data were captured using an ordinary camera; temperature information was monitored using an IR camera.

2.5. Self-healable liquid repellence

2.5.1. General heat-generation capability

To quantify self-healable liquid repellence, syneresis behavior was induced by electric or photonic stimulation, and the efficacy of the replenishment process was demonstrated. These tests used the same electrical and photonic systems that had been used to quantify active deicing. The lubricant was removed from the surface, then electrical stimulation was given by applying voltages of 13 or 20 V 500 min, or photonic stimulation was applied using the laser (532 nm, 500 mW/cm2) for 1 h.

2.5.2. Replenishment

Replenishment was achieved simply by dropping lubricant (oil) onto the SLECs for 20 h. Then syneresis was induced at 70 °C for 24 h.

2.6. Practicality

To confirm the self-cleaning ability, calcium sulfate was spread on SLEC of M15L90 and cleaning by rolling water was observed. For the durability of liquid-repellence against abrasion, a 70-cm abrasion was applied to an M11L90 SLEC by dragging it on 2000-mesh sandpaper. ROA was measured every 10 cm along the abrasion (Smartdrop, Femtobiomed). After abrasion over 70 cm, it was stored in 70 °C for syneresis for > 24 h. Lastly, Durability confirmation of SLECs under cyclic loading of stretching (ε = 35 %) and bending (ε = 60 %) were conducted. The resistance change of M15L50 (1 cm x 1 cm x500 μm) during cycles was measured by a digital multimeter (34401A, Agilent technologies Inc.). Both ends of sample were clamped on a motorized XY stage with a gap of 2 cm where one end of sample was moved into the other end for bending, or was moved away from the other end for stretching up to given strain.

3. Results and discussion

3.1. Passive anti-icing property of the SLEC: capability to maintain liquid repellence in harsh condition

The SLEC must retain their liquid repellence in harsh conditions. This ability is important because after anti-icing surfaces lose their liquid repellence, water that is deposited on them by condensation or rain can freeze, and the resulting ice can be difficult to remove. These changes nullify all of the advantages of the icephobic properties of liquid-repellent surfaces. Liquid-repellent surfaces must overcome these complications to increase anti-icing activity.

We performed tests under condensation conditions and de-icing conditions, which are plausible situations that cause ice accretion that has caused trouble for many liquid-repellent surfaces. To quantify the retention of liquid repellence under condensation, SLUG, SLEC, and SHPo liquid-repellent surfaces were held below the dew point (Wetting information at room temperature is in SI). While the surfaces went through a temperature drop to 0 ℃ for 10 min, condensed liquids covered them entirely (Supplementary video S1). Impacting droplets slid off the SLUG and SLEC, but stuck to SHPo (Fig. 2a, and Supplementary video S1). This result for SHPo occurs because it loses its liquid repellence when condensed liquids form within its surface structures [4,40].

Fig. 2.

Fig. 2.   Results for sustainable liquid repellence. (a) Test to show maintenance of liquid-repellence after condensation with SLEC (M11L90), SHPo, and SLUG (M0L90). (b) Melting frost slides down M14L90, and (c) subsequent impinging droplets slide off of it. (d) Melting frost remained on SHPo, and (e) subsequent droplets stuck to it. (f) Time lapse images for icing delay time and (g) frost coverage ratio over time on SHPo, M14L90, and M11L90. (h) Frost propagation on M11L90.

A similar tendency was observed in another de-icing test (Fig. 2b-e). After the ice layer was melted by a de-icing process, the resulting water droplets rolled of the SLEC, but remained on the SHPo. Subsequently, water droplets that struck the surfaces could only slide off the SLEC. They did not slide off the SHPo, because water that permeates its structures can pin them.

These results demonstrate that SLEC surfaces have better anti-icing property than SH surfaces. We believe that use of SLIPS series (including SLECs), which are relatively insensitive to condensed water, can be an effective passive anti-icing strategy. These experiments also demonstrated that the SLEC can retain its liquid repellence.

3.2. Passive anti-icing property of the SLEC: delay of ice nucleation

To further explore the passive anti-icing property of SLEC, the ice nucleation effectiveness was characterized (Fig. 2f-h). For the test, time of onset of freezing and frost coverage were measured. Water droplets of 10 μL on M11L90, M14L90 and SHPo were cooled down to -5 °C. Droplets froze at 115 s on the SHPo first, at 318 s on M14L90, and at 413 s on M11L90. From the perspective of icephobicity, SLIPS benefits from a reduction in the potential nucleation sites because it provides chemically homogeneous interface and can presumably get rid of potential nucleation sites [1,41,42]. Apart from this, SLIPS is less vulnerable to the humidity. In contrast, SHP surfaces are generally prone to localized coating peeling, cracks, scratches by external stress according to the fabrication process or materials [30]. Such defects provide initiation sites for ice nucleation. We believe these characteristics explain the longer icing delay time on SLECs than on SHPo. The prepared SHPo was made on the silicon wafer by spray silicone based material coating which can induce the delamination at interface due to modulus mismatch by external stress [43] or low robustness such as low hardness. These might play the role of initiation sites. Apart from the comparison between SHPo and SLEC, M11L90 shows longer onset of freezing time than M14L90. It might take advantage of the thicker lubricant film and lower thermal conductivity of M11L90 than M14L90. Note that water droplet floats on the lubricant (Section 3 in SI).

Similarly, a test for frost propagation shows benefits of lubricant film on anti-icing. After onset of frost, the coverage percentage in frost area was measured over time. Frost covered the surface of M5.8L0 for 61 s, of M14L90 for 460 min, and of M11L90 for 774 min. Frost nucleates at defects or edges, and proceeds to propagate by forming an inter-bridge (e.g., ice dendrites) among peripheral condensates [4]. The frost is restrained to grow when condensate droplets are cloaked in lubricant [30] so, we presume that condensate droplets cloaked in thin lubricant film suppress the growth of ice dendrite that was caused by vapor of neighboring condensate droplets. Also, lubricants provide low thermal conductivity and suppress the nucleation chances by removing possible nucleation sites. The SLEC forms cloaking droplets (Section 3 in SI). The effect of lubricant is also observed in the comparison between SLECs. On the oil film, frost propagates along the thin oil layer first, then the thick oil. So, frost spreads more slowly on M11L90 than M14L90. Lower speed of frost propagation on M11L90 also might be attributed to lower thermal conductivity, suppression of the nucleation sites, and thickness of the oil.

Additionally, ease of tuning in SLEC’s property offers a way to increase icing delay time and reduce frost propagation speed. The surface structuring, lower ratio of MWNTs and higher ratio of oil could be the examples. However, despite the better ice nucleation, these efforts could adversely affect the active anti-icing functions (e.g., Joule heating for defrosting). Therefore, materials should be selected to match applications.

3.3. Passive anti-icing abilities of the SLEC: ice adhesion strength

SIA is another important measure of passive anti-icing ability. SIA as low as ~20 kPa can allow removal of ice by natural forces like wind and vibration [1,32]. Low SIA can be achieved by non-interlocking of ice with a surface structure, low shear modulus, and low chemical or physical interaction between ice and substrate [[44], [45], [46]]. SIA (Fig. 3a) were obtained for as-prepared SLECs with different MWNTs and oil contents. As-prepared SLECs had SIA ~ 20 kPa, which is similar to a value reported for other SLIPS [33]. Compared to SHPo and SS SH surfaces (Fig. S3 in SI) and M09L0 that have high SIA > 50 kPa, we confirm that highly-mobile lubricant guarantees weakening of the interaction between ice and the substrates, and yields promising anti-icing materials. Reported SIA of SH surfaces are typically 50-100 kPa [1,47]; i.e., SLIPS achieve superior reduction in ice adhesion.

Fig. 3.

Fig. 3.   Ice adhesion strength (a) of SLECs with different oil and MWNTs contents, (b) in cycling ice adhesion tests of M14L60.

Among SLECs with different content of components, M11L90 had the lowest SIA ~14 kPa, and M14L60 had the highest SIA ~25 kPa. These results are easily predictable, because an excess of oil films greatly reduces ice adhesion (i.e., cohesive failure) [46,48]. Under the same MWNTs amounts, the higher content of oil leads to lower SIA as a result of the lower shear modulus. Incorporation of oil reduced SIA by ~2/3 compared to M09L0. Nevertheless, SIA of M09L0 is still quite small, possibly as a result of the large difference in elastic modulus EY between ice and SLEC [49].

The result of the ice adhesion cycle did not show significant increase in SIA even though no oil layer could be seen (Fig. 3b). This stable SIA may be a result of weak interaction and the viscoelastic property of the SLEC. SLEC consists of PDMS and oil, which infiltrates the crosslinked network of the PDMS. At the outermost surface of the SLEC, oil is exposed to the environment although oil is not visible. When water freezes on the SLEC, the resulting ice contacts the oil beneath it. The low EY of the SLEC may also explain the consistently low SIA. SLEC has a lower EY (i.e., is softer) than unadulterated PDMS. The large difference in EY induces mismatch in strain when force is applied to remove the ice. The stress induced by applied force to remove the ice is not evenly distributed in the SLEC, but builds up at the interface which fractures [49]. As a result, the low interaction between two results in low SIA. This viscoelastic property and the oil components of the SLEC are also beneficial in outdoor applications even when oil films are lost. These results demonstrate that the SLEC has desirably low SIA.

3.4. Active anti-icing abilities of the SLEC: electro-thermogenesis

At temperature < 0 °C, water could eventually freeze on a surface, even if it has outstanding passive anti-icing properties. Once ice has accreted on a surface, the phase change of subsequent water to ice accelerates as a result of heterogeneous nucleation, and this acceleration aggravates the icing problem. Therefore, a promising anti-icing surfaces must remove the accreted ice on the surface as well recover passive anti-icing capability quickly and reliably.

The SLEC generates heat by electro-thermogenesis when it is stimulated electrically. The MWNTs in the SLEC form conductive pathways that undergo Joule heating when an electrical current passes through them. The maximum temperature that can be reached can be tuned by adjusting the amount of each component in the SLEC, and by adjusting the applied voltage (ref [38]; sections 5 and 6 in SI). To combat icing, electro-thermogenesis could be exploited to prevent ice formation, and to remove an ice layer after it has formed.

To quantify the ability of electro-thermogenesis to prevent water from freezing, SLUG and SLEC were placed on a Peltier plate at -7 ℃, then voltage of 25 V applied to them until their temperature reached 17 ℃. The SLUG does not contain MWNTs, so it did not generate heat; as a result, ice accreted in 20 min (Fig. 4a and b, and Supplementary video 2). The SLEC was warmed by Joule heating so ice did not form; only condensate droplets formed (Fig. 4a and b, and Supplementary video S2). Moreover, droplets could still slide when they fell onto a surface that was covered by condensate droplets (Fig. 4c). This sustainable liquid-repellence of SLEC with icing/deicing cycle and condensation is an advantageous anti-icing property for outdoor applications. Many SH surfaces lose liquid repellence when liquids condense on them (Fig. 2). These results demonstrate that the electro-thermogenesis capability of the SLEC in response to voltage effectively prevents ice formation while maintaining liquid repellence.

Fig. 4.

Fig. 4.   Active anti-icing using electro-thermogenesis. Capability of (a,b) SLUG (M0L90) and SLEC (M14L90) on ice prevention by application of voltage (25 V) on low-temperature Peltier plate (-7 ℃). (c) Water-droplet dripping after test of (a, b). Sample is still on the low-temperature plate. Defrosting capability of (d) SLUG (M0L90) and SLEC (M14L90) on a Peltier plate at 11 ℃, by application of voltage (25 V).

After ice has accreted, it should be removed to avoid exacerbation of the icing problem. In this situation, electro-thermogenesis can stop worsening of the problem. After voltage was applied, ice remained on the SLUG surface (Fig. 4d), but the entire ice surface melted from the SLEC as a result of Joule heating (Fig. 4d). The melting ice can slide off the surface. This electro-themogenesis can act synergistically with the liquid-repellent property, because without complete melting, the ice-slurry can easily slide off the surface due to its low adhesion to water [22]. These results demonstrate that electro-thermogenesis boosted by liquid repellence can amplify the anti-icing effect in real environments.

3.5. Active anti-icing abilities of the SLEC: photo-thermogenesis

The SLEC can also undergo photo-thermogenesis, which is heat generation in response to photonic stimulation. This heat generation is also induced by the MWNTs, so the power of the heat-generation can be tuned by the adjusting the content of MWNTs in the material, and by selecting an appropriate laser wavelength.

Photo-thermogenesis of the SLEC offers a remarkable alternative when electro-thermogenesis is not available to melt the ice. This substitutional choice provides flexibility for application. To confirm the capability of defrosting by the photo-thermal effect, a laser with wavelength of 532 nm was beamed at ice layer on the SLEC surface. The characteristics of thermogenesis in response to photonic energy in this system were investigated (Fig. S5 in SI). Beams with power density of 500 mW/cm2 irradiated the ice-layered samples. The SLUG does not have a photo-thermogenesis effect, so the ice was not affected. In contrast, on the SLEC the ice melted in the spots that were irradiated by the laser (Fig. 5, and Supplementary video S3), because the light is absorbed by MWNTs and increases their temperature. The temperature of the SLEC increased from -3 °C to 25 °C after irradiation for 30 s (Fig. 5). Photo-thermogenesis by the SLEC can offer the significant benefit of eliminating ice buildup.

Fig. 5.

Fig. 5.   Active anti-icing function using photo-thermogenesis. (a) Capability of ice prevention of SLUG (M0L60) and SLEC (M14L60) by laser illumination (532 nm, 500 mW/cm2). (b) FLIR images that correspond to (a).

3.6. Self-healable liquid repellence

The self-healing property of SLIPS ensures more stable liquid repellence than SH surfaces can achieve [50], but SLIPS still lack durability for outdoor applications [32]. The poor durability is mainly a result of depletion of the lubricant by processes such as volatilization, leakage, and migration. Especially, cloaking of the droplet in oil accelerates the depletion of lubricant (Section 3, 4 in SI). Water is cloaked on the SLEC. For these reasons, to attain long-lasting liquid repellence, the SLEC should have self-sustainable liquid repellence with minimized dependence on the environmental conditions. Self-lubricating organogels can show a special thermo-responsive syneresis behavior that can recover their liquid repellence [31,38]. Nevertheless, in reality, an environment that can allow the system to control the surrounding temperature is rare. In addition, although liquid-repellence can be recovered by syneresis, the amount of oil entrapped in the crosslinked PDMS network is finite, so the syneresis rate gradually decreases, and eventually fails to maintain sufficient liquid repellence. Therefore, an ice-repellent surface must have sustainable syneresis ability.

From these perspectives, our SLEC has superior advantages for better durability than SLIPS without self-lubrication or refill function. The thermogenesis in the SLEC in response to stimulation by electricity or light allows for syneresis because of temperature dependence of the SLEC’s syneresis. Additionally, by a replenishment process, the amount of oil entrapped in the crosslinked PDMS network can be maintained above a level that ensures sustainable syneresis.

On the SLEC, syneresis occurred under electrical and photonic stimulation (Fig. 6). Syneresis by external stimulation has rarely been observed in other materials. Thermogenesis in the SLEC in response to electrical or photonic energy can make syneresis available as syneresis of the SLEC is presumably driven by the diffusion. Electronic energy with voltage applications of 13 or 20 V for 500 min imparted lubrication (Fig. 6a). The syneresis rate increased as the temperature of the SLEC increased (Fig. 6a). Syneresis reduced the ROA from ~20° to < 5° after electrical stimulation for 4 h, so liquid easily rolled off the surfaces (Fig. S6b).

Fig. 6.

Fig. 6.   (a) Syneresis behavior induced by Joule heating for 500 min (b) Temperature increase induced by laser irradiation (532 nm, 500 mW/cm2) for 1 h, and syneresis behavior induced by photothermogenesis. (c) Demonstration of lubricant replenishment. Optical images of SLECs: (left) SLEC in its initial condition after complete removal of remained oil. SLECs after syneresis for 24 h at 70 °C: (middle) sample without replenishment and (right) sample with replenishment. (d) Comparison of weight loss of the two samples.

The SLEC also shows photo-responsive syneresis behavior (Fig. 6b). The photonic system is useful as an alternative way to induce self-lubrication in environments where Joule heating is not feasible. This photo-responsive thermogenesis induces syneresis (Fig. 6b). M12L90 that was lubricant-wiped was irradiated for 1 h; the irradiated spot released lubricant. This combination of slipperiness and heat-generating ability under voltage or laser illumination may have practical advantages in outdoor applications.

The self-healing capability of the SLEC induced by syneresis is necessary for lifetime-long liquid repellence. The reduction of syneresis rate may accelerate when an SLEC is used outdoors, and this loss of lubrication can be fatal to anti-icing applications. However, the SLECs can be replenished by bringing them into contact with the silicone oil that is used as the lubricant (Fig. 6c). The silicone oil wicks into the crosslinked PDMS network, so the PDMS swells; the silicone oil may dissolve into the network [51]. We prepared an SLEC from which most of the oil had been consumed, and that did not release sufficient oil. Then we compared this sample to one in which the oil had been replenished by contact with a reservoir of the lubricant. The quantity of released oil differed greatly between the two samples (Fig. 6d). The sample that had been replenished released as much oil as the as-prepared sample; this result confirms that contact with the lubricant can restore the liquid repellence. The durability of liquid repellence is the most important requirement for practical anti-icing applications, so this replenishment approach is useful.

3.7. Practicality

SHPo and SLIPS have been proven to be effective anti-icing surfaces, so their practicality such as ease of fabrication or durability has been considered important [5,52]. To meet these requirements, the SLEC was developed with the intention of achieving a strong practical coating strategy. First, SLEC is a PDMS-based material made by standard physical mixing process, thus the process is scalable, inexpensive, and applicable to diverse shapes (Fig. 7). Furthermore, this method also allows the material’s properties to be easily tuned simply by changing the components’ ratio, which offers versatility for a wide range of applications. We strongly believe that such simplicity and effectiveness of fabrication process for such multi-functionality has value in fields of engineering and surface modification, to name a few. Secondly, SLEC possesses promising stability against external stress such as mechanical and environmental damages. In practical applications, this stability is another important consideration to maintain the surface’s original property against external stress and to achieve longevity.

Fig. 7.

Fig. 7.   (a) Scalable SLEC fabrication (b) self-cleaning property of SLEC. The dirt is removed by the rolling droplet. Stability of liquid repellence after (c) abrasion test, and (d) blade-cutting test. (e) mechanical stability of SLEC under multi-cycles of stretching and bending loading. Here, resistance change ΔR (i.e. the difference resistance after strain to initial resistance R0) was normalized to R0: ΔR⁄R0. (left. ΔR/R0 of M15L90 as a function of multiple (> 100 times) bending cycles with displacement of 1.2 cm. (right) ΔR/R0 of M15L90 with different off-times TOFF as a function of multiple (> 100 times) stretching and releasing cycles with 35 % strain.

Many factors can impede the maintenance of functionality in real circumstances. Accordingly, we tested the stability of SLEC under four conditions: impurity, mechanical stress (i.e., abrasion, scratch, stretching and bending). These stresses are commonly encountered in many applications. Impurities such as dirt can contaminate the surface and reduce its functionality. Although SHP surfaces or SLIPS have self-cleaning function, it does not always remove the dirt [53]. Furthermore, self-cleaning by a rolling motion is more efficient than by a sliding motion [54,55]. An SLEC that is composed of an appropriate material can remove powdered calcium sulfate dirt by a rolling motion (Fig. 7b, Supplementary video). This result demonstrates a reliable self-cleaning ability.

Next, we confirmed stability against abrasion and scratching. Although the depletion of the lubricant due to abrasion with sandpaper increased the wettability (i.e., increased ROA), it remains low (ROA < 15°). More importantly, after self-lubrication, the surface recovered its repellence (ROA ~2°) (Fig. 7c). Similarly, a water droplet smoothly passed a line of damage that was imposed by cutting using a blade (Fig. 7d). All results demonstrate that the outer liquid layer yields high liquid repellence that is resilient to physical damage.

Further tests of stability against mechanical stress were performed under cyclic stretching and bending deformation (Fig. 7e). The SLEC composed of M15L50 shows good mechanical compliance under repetitive stretching (35 % strain) and bending deformation (60 % strain with displacement of 1.2 cm from an initial gap of 2 cm). This elastomer/nanofiller composite provides a method to fabricate materials with superior mechanical compliance comparing to the material with low strain to break ratio [56]. We believe that the simple fabrication process, durability of liquid repellence and mechanical compliance increase the practicality and reliability of the material in a wide range of real applications.

4. Conclusion

We have shown a superior anti-icing strategy (SLEC) that is capable of both passive anti-icing and active de-icing. The SLEC has a slippery surface that imparts liquid repellence, and undergoes thermogenesis in response to electric or photonic stimulation. The liquid repellence of the SLEC enables water droplets to slide off a wet surface that frequently encounters conditions that cause condensation and defrosting. The lubricant can retard ice nucleation. The slippery oil of the material and undermatching in modulus between SLEC and PDMS induce low ice adhesion. The electrical or photonic stimulation cause the SLEC to heat up, and this process can help prevent ice accretion or melt an accreted ice layer on the SLEC. The liquid repellence of the SLEC is sustainable by self-lubrication behaviour, which is boosted by thermogenesis with the help of an electronic/photonic system. Oil that is lost during service can be replenished by simple immersion. As a result, SLEC shows exceptional durability of the anti-icing property and extended service time. SLEC has many practical advantages such as stability against mechanical stress, and a simple and scalable fabrication process. These passive and active anti-icing functionalities in conjunction with practical advantages such as durable liquid repellence offer strong potential as an anti-icing tool in a general icing environment.

Declaration of Competing Interest

The authors declare no competing financial interests.


We thank Dr. Junghwan Byun, Dr. Hyejeong Kim, Dr. Joonphil Choi, Dr. Changyong Yim and MNT for valuable comments, supports, and discussion.

Appendix A. Supplementary data

Supplementary material related to this article can be found, inthe online version, at doi:


M.J. Kreder, J. Alvarenga, P. Kim, J. Aizenberg, Nat. Rev. Mater. 1 (2016) 1-15.

[Cited within: 5]

K. Golovin S.P.R. Kobaku, D.H. Lee, E.T. DiLoreto, J.M. Mabry, A. Tuteja, Sci. Adv. 2 (2016), e1501496.

DOI:10.1126/sciadv.1501496      URL     PMID:26998520      [Cited within: 1]

L. Wang, Q. Gong, S. Zhan, L. Jiang, Y. Zheng, Adv. Mater. 28 (2016) 7729-7735.

DOI:10.1002/adma.201602480      URL     PMID:27375270      [Cited within: 1]

A material with superhydrophobic and anti-ice/de-icing properties, which has a micro-/nanostructured surface, is produced by a straightforward method. This material comprises a poly(dimethylsiloxane) (PDMS) microstructure with ZnO nanohairs and shows excellent water and ice repellency even at low temperatures (-20 degrees C) and relatively high humidity (90%) for over three months. These results are expected to be helpful for designing smart, non-wetting materials that can be adapted to low-temperature environments for the development of anti-icing systems.

A. Kim, C. Lee, H. Kim, J. Kim, ACS Appl. Mater. Interfaces 7 (2015) 7206-7213.

DOI:10.1021/acsami.5b00292      URL     PMID:25782028      [Cited within: 4]

Frost formation can cause operational difficulty and efficiency loss for many facilities such as aircraft, wind turbines, and outdoor heat exchangers. Self-propelled jumping by condensate droplets on superhydrophobic surfaces delays frost formation, so many attempts have been made to exploit this phenomenon. However, practical application of this phenomenon is currently unfeasible because many processes to fabricate the superhydrophobic surfaces are inefficient and because self-propelled jumping is difficult to be achieved in a humid and low-temperature environment because superhydrophobicity is degraded in these conditions. Here, we achieved significantly effective anti-icing superhydrophobic aluminum. Its extremely low adhesive properties allow self-propelled jumping under highly supersaturated conditions of high humidity or low surface temperature. As a result, this surface helps retard frost formation at that condition. The aluminum was made superhydrophobic by a simple and cost-effective process that is adaptable to any shape. Therefore, it has promise for use in practical and industrial applications.

Y. Shen, X. Wu, J. Tao, C. Zhu, Y. Lai, Z. Chen, Prog. Mater. Sci. 103 (2019) 509-557.

[Cited within: 5]

S. Zhang, J. Huang, Y. Cheng, H. Yang, Z. Chen, Y. Lai, Small 1 (2017), 1701867.

[Cited within: 2]

M.I. Jamil, A. Ali, F. Haq, Q. Zhang, X. Zhan, F. Chen, Langmuir 34 (2018) 15425-15444.

URL     PMID:30445813      [Cited within: 2]

L. Zhu, J. Xue, Y. Wang, Q. Chen, J. Ding, Q. Wang, ACS Appl. Mater. Interfaces 5 (2013) 4053-4062.

URL     PMID:23642087      [Cited within: 2]

X. Wu, Z. Chen, J. Mater. Chem. A 6 (2018) 16043-16052.

[Cited within: 1]

B. Liu, K. Zhang, C. Tao, Y. Zhao, X. Li, K. Zhu, X. Yuan, RSC Adv. 6 (2016) 70251-70260.

[Cited within: 1]

S. Bengaluru Subramanyam, V. Kondrashov, J. Ruhe, K.K. Varanasi, ACS Appl. Mater. Interfaces 8 (2016) 12583-12587.

DOI:10.1021/acsami.6b01133      URL     PMID:27150450      [Cited within: 2]

Ice adhesion on superhydrophobic surfaces can significantly increase in humid environments because of frost nucleation within the textures. Here, we studied frost formation and ice adhesion on superhydrophobic surfaces with various surface morphologies using direct microscale imaging combined with macroscale adhesion tests. Whereas ice adhesion increases on microtextured surfaces, a 15-fold decrease is observed on nanotextured surfaces. This reduction is because of the inhibition of frost formation within the nanofeatures and the stabilization of vapor pockets. Such

T.-B. Nguyen, S. Park, H. Lim, Appl. Surf. Sci. 435 (2018) 585-591.

DOI:10.1016/j.apsusc.2017.11.137      URL     [Cited within: 1]

L. Mishchenko, B. Hatton, V. Bahadur, J.A. Taylor, T. Krupenkin, J. Aizenberg, ACS Nano 4 (2010) 7699-7707.

DOI:10.1021/nn102557p      URL     PMID:21062048      [Cited within: 1]

Materials that control ice accumulation are important to aircraft efficiency, highway and powerline maintenance, and building construction. Most current deicing systems include either physical or chemical removal of ice, both energy and resource-intensive. A more desirable approach would be to prevent ice formation rather than to fight its build-up. Much attention has been given recently to freezing of static water droplets resting on supercooled surfaces. Ice accretion, however, begins with the droplet/substrate collision followed by freezing. Here we focus on the behavior of dynamic droplets impacting supercooled nano- and microstructured surfaces. Detailed experimental analysis of the temperature-dependent droplet/surface interaction shows that highly ordered superhydrophobic materials can be designed to remain entirely ice-free down to ca. -25 to -30 degrees C, due to their ability to repel impacting water before ice nucleation occurs. Ice accumulated below these temperatures can be easily removed. Factors contributing to droplet retraction, pinning and freezing are addressed by combining classical nucleation theory with heat transfer and wetting dynamics, forming the foundation for the development of rationally designed ice-preventive materials. In particular, we emphasize the potential of hydrophobic polymeric coatings bearing closed-cell surface microstructures for their improved mechanical and pressure stability, amenability to facile replication and large-scale fabrication, and opportunities for greater tuning of their material and chemical properties.

H.Y. Erbil, Surf. Innov. 4 (2016) 214-217.

DOI:10.1680/jsuin.16.00026      URL     [Cited within: 2]

P. Irajizad, M. Hasnain, N. Farokhnia, S.M. Sajadi, H. Ghasemi, Nat. Commun. 7 (2016) 13395.

URL     PMID:27824053      [Cited within: 1]

A. Alizadeh, M. Yamada, R. Li, W. Shang, S. Otta, S. Zhong, L. Ge, A. Dhinojwala, K.R. Conway, V. Bahadur, A.J. Vinciquerra, B. Stephens, M.L. Blohm, Langmuir 28 (2012) 3180-3186.

DOI:10.1021/la2045256      URL     PMID:22235939      [Cited within: 1]

Prevention of ice accretion and adhesion on surfaces is relevant to many applications, leading to improved operation safety, increased energy efficiency, and cost reduction. Development of passive nonicing coatings is highly desirable, since current antiicing strategies are energy and cost intensive. Superhydrophobicity has been proposed as a lead passive nonicing strategy, yet the exact mechanism of delayed icing on these surfaces is not clearly understood. In this work, we present an in-depth analysis of ice formation dynamics upon water droplet impact on surfaces with different wettabilities. We experimentally demonstrate that ice nucleation under low-humidity conditions can be delayed through control of surface chemistry and texture. Combining infrared (IR) thermometry and high-speed photography, we observe that the reduction of water-surface contact area on superhydrophobic surfaces plays a dual role in delaying nucleation: first by reducing heat transfer and second by reducing the probability of heterogeneous nucleation at the water-substrate interface. This work also includes an analysis (based on classical nucleation theory) to estimate various homogeneous and heterogeneous nucleation rates in icing situations. The key finding is that ice nucleation delay on superhydrophobic surfaces is more prominent at moderate degrees of supercooling, while closer to the homogeneous nucleation temperature, bulk and air-water interface nucleation effects become equally important. The study presented here offers a comprehensive perspective on the efficacy of textured surfaces for nonicing applications.

K. Li, S. Xu, W. Shi, M. He, H. Li, S. Li, X. Zhou, J. Wang, Y. Song, Langmuir 28 (2012) 10749-10754.

URL     PMID:22741592      [Cited within: 1]

C. Marcolli, Sci. Rep. 7 (2017) 16634.

DOI:10.1038/s41598-017-16787-3      URL     PMID:29192142      [Cited within: 1]

Homogeneous ice nucleation needs supercooling of more than 35 K to become effective. When pressure is applied to water, the melting and the freezing points both decrease. Conversely, melting and freezing temperatures increase under negative pressure, i.e. when water is stretched. This study presents an extrapolation of homogeneous ice nucleation temperatures from positive to negative pressures as a basis for further exploration of ice nucleation under negative pressure. It predicts that increasing negative pressure at temperatures below about 262 K eventually results in homogeneous ice nucleation while at warmer temperature homogeneous cavitation, i. e. bubble nucleation, dominates. Negative pressure occurs locally and briefly when water is stretched due to mechanical shock, sonic waves, or fragmentation. The occurrence of such transient negative pressure should suffice to trigger homogeneous ice nucleation at large supercooling in the absence of ice-nucleating surfaces. In addition, negative pressure can act together with ice-inducing surfaces to enhance their intrinsic ice nucleation efficiency. Dynamic ice nucleation can be used to improve properties and uniformity of frozen products by applying ultrasonic fields and might also be relevant for the freezing of large drops in rainclouds.

S.J. Cox, S.M. Kathmann, B. Slater, A. Michaelides, J. Chem. Phys. 142 (2015), 184704.

DOI:10.1063/1.4919714      URL     [Cited within: 1]

T. Matsubayashi, M. Tenjimbayashi, K. Manabe, M. Komine, W. Navarrini, S. Shiratori, ACS Appl. Mater. Interfaces 8 (2016) 24212-24220.

DOI:10.1021/acsami.6b07844      URL     PMID:27540638      [Cited within: 2]

Ice formation causes numerous problems in many industrial fields as well as in our daily life. Various functional anti-ice coatings have been extensively studied during the past several decades; however, the development of feasible ice-repellent surfaces with long-term stability has been found to be extremely difficult. Here, we report the conductive superhydrophobic coatings with freezing rain repellency that simultaneously possess electrothermogenic ability to rapidly melt newly formed frosts due to the Joule heat. The obtained films have high mechanical flexibility and abrasion resistance produced by composite nanoparticles of poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate) embedded in ethyl cyanoacrylate. In addition, excellent water repellency (corresponding contact angle >160 degrees ) and efficient heating ability (with an estimated energy consumption as low as 260.8 degrees C cm(2)/W) generated by applying voltage through the conductive film surface have been demonstrated. The proposed concept of combining super-repellency with electrothermal heating may provide a new strategy of addressing problems related to ice formation.

M. Elsharkawy, D. Tortorella, S. Kapatral, C.M. Megaridis, Langmuir 32 (2016) 4278-4288.

DOI:10.1021/acs.langmuir.6b00064      URL     PMID:27021948      [Cited within: 1]

Frost formation is omnipresent when suitable environmental conditions are met. A good portion of research on combating frost formation has revolved around the passive properties of superhydrophobic (SHPO) and slippery lubricant-impregnated porous (SLIP) surfaces. Despite much progress, the need for surfaces that can effectively combat frost formation over prolonged periods still remains. In this work, we report, for the first time, the use of electrically conductive SHPO/SLIP surfaces for active mitigation of frost formation. First, we demonstrate the failure of these surfaces to passively avert prolonged (several hours) frosting. Next, we make use of their electroconductive property for active Joule heating, which results in the removal of any formed frost. We study the role of the impregnating lubricant in the heat transfer across the interface, the surface, and the ambient. We show that, even though the thermal properties of the impregnating lubricant may vary drastically, the lubricant type does not noticeably affect the defrosting behavior of the surface. We attribute this outcome to the dominant thermal resistance of the thick frost layer formed on the cooled surface. We support this claim by drawing parallels between the present system and heat transfer through a one-dimensional (1D) composite medium, and solving the appropriate transient transport equations. Lastly, we propose periodic thermal defrosting for averting frost formation altogether. This methodology utilizes the coating's passive repellent capabilities, while eliminating the dominant effect of thick deposited frost layers. The periodic heating approach takes advantage of lubricants with higher thermal conductivities, which effectively enhance heat transfer through the porous multiphase surface that forms the first line of defense against frosting.

J.B. Boreyko, B.R. Srijanto, T.D. Nguyen, C. Vega, M. Fuentes-Cabrera, C.P. Collier, Langmuir 29 (2013) 9516-9524.

URL     PMID:23822157      [Cited within: 2]

B. Park, W. Hwang, Scr. Mater. 113 (2016) 118-121.

DOI:10.1016/j.scriptamat.2015.10.018      URL     [Cited within: 2]

M. Wu, Y. Li, N. An, J. Sun, Adv. Funct. Mater. 26 (2016) 6777-6784.

[Cited within: 2]

G. Jiang, L. Chen, S. Zhang, H. Huang, ACS Appl. Mater. Interfaces 10 (2018) 36505-36511.

DOI:10.1021/acsami.8b11201      URL     PMID:30273481      [Cited within: 1]

For faster and greener anti-icing/deicing, a new generation of anti-icing materials are expected to possess both passive anti-icing properties and active deicing properties. The photothermal effect of carbon nanotubes (CNTs) is used in the field of photothermal cancer therapy, while the application in anti-icing/deicing is seldom investigated. Superhydrophobic SiC/CNTs coatings with photothermal deicing and passive anti-icing properties were first prepared by a simple spray-coating method. The results of 3D profile and microstructure observed via scanning electron microscopy demonstrate that the micronanostructure combined with peaklike SiC microstructure and villiform CNTs nanostructure makes the coatings surface superhydrophobic, exhibiting a water contact angle of up to 161 degrees and a roll angle as low as 2 degrees . This micronanostructure can also reduce ice anchoring and ice adhesion strength. Utilizing the photothermal effect of CNTs, the surface temperature of the coatings is rapidly increased upon near-infrared light (808 nm) irradiation. The heat is transferred rapidly to the surroundings by highly thermal conductive CNTs. The light-to-heat conversion efficiency in deicing tests is approximately 50.94%, achieving a highly efficient remote deicing effect. This superhydrophobic coating combining photothermal deicing and passive anti-icing properties is expected to be further used in various practical applications and in development of a new generation of anti-icing/deicing coatings.

X. Yin, Y. Zhang, D. Wang, Z. Liu, Y. Liu, X. Pei, B. Yu, F. Zhou, Adv. Funct. Mater. 25 (2015) 4237-4245.

[Cited within: 2]

N. Wang, D. Xiong, S. Pan, K. Wang, Y. Shi, Y. Deng, New J. Chem. 41 (2017) 1846-1853.

[Cited within: 1]

S. Ozbay, C. Yuceel, H.Y. Erbil, ACS Appl. Mater. Interfaces 7 (2015) 22067-22077.

URL     PMID:26375386      [Cited within: 1]

S.B. Subramanyam, K. Rykaczewski, K.K. Varanasi, Langmuir 29 (2013) 13414-13418.

DOI:10.1021/la402456c      URL     PMID:24070257      [Cited within: 1]

Ice accretion is an important problem and passive approaches for reducing ice-adhesion are of great interest in various systems such as aircrafts, power lines, wind turbines, and oil platforms. Here, we study the ice-adhesion properties of lubricant-impregnated textured surfaces. Force measurements show ice adhesion strength on textured surfaces impregnated with thermodynamically stable lubricant films to be higher than that on surfaces with excess lubricant. Systematic ice-adhesion measurements indicate that the ice-adhesion strength is dependent on texture and decreases with increasing texture density. Direct cryogenic SEM imaging of the fractured ice surface and the interface between ice and lubricant-impregnated textured surface reveal stress concentrators and crack initiation sites that can increase with texture density and result in lowering adhesion strength. Thus, lubricant-impregnated surfaces have to be optimized to outperform state-of-the-art icephobic treatments.

K. Rykaczewski, S. Anand, S.B. Subramanyam, K.K. Varanasi, Langmuir 29 (2013) 5230-5238.

URL     PMID:23565857      [Cited within: 3]

C. Urata, G.J. Dunderdale, M.W. England, A. Hozumi, J. Mater. Chem. A 3 (2015) 12626-12630.

[Cited within: 4]

A. Sandhu, O.J. Walker, A. Nistal, K.L. Choy, A.J. Clancy, Chem. Commun. 55 (2019) 3215-3218.

[Cited within: 3]

Y. Wang, X. Yao, J. Chen, Z. He, J. Liu, Q. Li, J. Wang, L. Jiang, Sci. China Mater. 58 (2015) 559-565.

DOI:10.1007/s40843-015-0069-7      URL     [Cited within: 2]

Y.H. Yeong, C. Wang, K.J. Wynne, M.C. Gupta, ACS Appl. Mater. Interfaces 8 (2016) 32050-32059.

URL     PMID:27797475      [Cited within: 1]

Y. Wang, X. Yao, S. Wu, Q. Li, J. Lv, J. Wang, L. Jiang, Adv. Mater. 29 (2017), 1700865.

DOI:10.1002/adma.v29.26      URL     [Cited within: 2]

Q. Li, Z. Guo, J. Mater. Chem. A 6 (2018) 13549-13581.

[Cited within: 1]

M. Yan, C. Zhang, R. Chen, Q. Liu, J. Liu, J. Yu, L. Gao, G. Sun, J. Wang, J. Mater. Chem. A 7 (2019) 24900-24907.

[Cited within: 1]

A. Kim, S. Kim, M. Huh, J. Kim, in: Proceeding to the 2018 IEEE Micro Electro Mechanical Systems (MEMS), Belfast Waterfront, Belfast, Northern Ireland, 2018, January, 21-25. 21-25.

[Cited within: 3]

A. Kim, C. Lee, J. Kim, Surf. Coat. Technol. 344 (2018) 394-401.

[Cited within: 1]

K.K. Varanasi, M. Hsu, N. Bhate, W. Yang, T. Deng, Appl. Phys. Lett. 95 (2009), 094101.

[Cited within: 1]

P.W. Wilson, W. Lu, H. Xu, P. Kim, M.J. Kreder, J. Alvarenga, J. Aizenberg, Phys. Chem. Chem. Phys. 15 (2013) 581-585.

URL     PMID:23183624      [Cited within: 1]

M. Zhang, J. Yu, R. Chen, Q. Liu, J. Liu, D. Song, P. Liu, L. Gao, J. Wang, J. Alloy, Compd. 803 (2019) 51-60.

[Cited within: 1]

C. Bocking, A. Reynolds, T.I. Met, Finish 89 (2013) 298-302.

[Cited within: 1]

Z. He, E.T. Vagenes, C. Delabahan, J. He, Z. Zhang, Sci. Rep. 7 (2017) 42181.

URL     PMID:28169370      [Cited within: 1]

Z. He, Y. Zhuo, J. He, Z. Zhang, Soft Matter 14 (2018) 4846-4851.

DOI:10.1039/c8sm00820e      URL     PMID:29845173      [Cited within: 1]

The mitigation of ice on exposed surfaces is of great importance to many aspects of life. Ice accretion, however, is unavoidable as time elapses and temperature lowers sufficiently. One practical solution is to reduce the ice adhesion strength on a surface to as low as possible, by either decreasing the substrate elastic modulus, lowering surface energy or increasing the length of cracks at the ice-solid interface. Herein, we present a facile preparation of polydimethylsiloxane (PDMS) based sandwich-like sponges with super-low ice adhesion. The weight ratio of the PDMS prepolymer to the curing agent is tuned to a lower surface energy and elastic modulus. The introduction of PDMS sponge structures combined the advantages of both a reduced apparent elastic modulus and most importantly, the macroscopic crack initiators at the ice-solid interface, resulting in dramatic reduction of the ice adhesion strength. Our design of sandwich-like sponges achieved a low ice adhesion strength as low as 0.9 kPa for pure PDMS materials without any additives. The super-low ice adhesion strength remains constant after 25 icing and deicing cycles. We thus provide a new and low-cost approach to realize durable super-low ice adhesion surfaces.

D.L. Beemer, W. Wang, A.K. Kota, J. Mater, Chem. A 4 (2016) 18253-18258.

[Cited within: 2]

S.A. Kulinich, M. Farzaneh, Langmuir 25 (2009) 8854-8856.

DOI:10.1021/la901439c      URL     PMID:19719211      [Cited within: 1]

In this work, we measured the adhesion strength of artificially created glaze ice (similar to accreted in nature) on rough fluoropolymer-based hydrophobic surfaces with different contact angle (CA) and wetting hysteresis. The previously reported direct correlation between ice repellency and CA on superhydrophobic surfaces is shown to be only valid for surfaces with low wetting hysteresis. Another correlation was found between wetting hysteresis and ice adhesion strength on rough surfaces with similar chemistry.

S.B. Subramanyam, K. Rykaczewski, K.K. Varanasi, Langmuir 29 (2013) 13414.

DOI:10.1021/la402456c      URL     PMID:24070257      [Cited within: 1]

Ice accretion is an important problem and passive approaches for reducing ice-adhesion are of great interest in various systems such as aircrafts, power lines, wind turbines, and oil platforms. Here, we study the ice-adhesion properties of lubricant-impregnated textured surfaces. Force measurements show ice adhesion strength on textured surfaces impregnated with thermodynamically stable lubricant films to be higher than that on surfaces with excess lubricant. Systematic ice-adhesion measurements indicate that the ice-adhesion strength is dependent on texture and decreases with increasing texture density. Direct cryogenic SEM imaging of the fractured ice surface and the interface between ice and lubricant-impregnated textured surface reveal stress concentrators and crack initiation sites that can increase with texture density and result in lowering adhesion strength. Thus, lubricant-impregnated surfaces have to be optimized to outperform state-of-the-art icephobic treatments.

C. Wang, T. Fuller, W. Zhang, K.J. Wynne, Langmuir 30 (2014) 12819-12826.

DOI:10.1021/la5030444      URL     PMID:25299447      [Cited within: 2]

Minimizing adhesion of ice has been the subject of extensive studies because of importance to applications such aircraft wings, spacecraft, and power transmission wires. A growing interest concerns coatings for wind turbine blades and refrigeration. Herein, a new laboratory test was employed to obtain the thickness dependence of ice adhesion for Sylgard 184-a filled polydimethylsiloxane elastomer. A correlation between ice adhesion and coating thickness (t) was found that follows a relationship developed by Kendall over 40 years ago for removal of a rigid object from an elastomer. With a 0.05 mm/s probe speed a nearly linear relationship between peak removal stress (Ps) and 1/t(1/2) was obtained with Ps approximately 460 kPa for an 18 mum coating, decreasing to approximately 120 kPa for 533 mum. Preliminary results suggest that below approximately 10 mum Ps departs from the 1/t(1/2) correlation while above approximately 500 mum a limiting value for Ps may be reached. We previously reported that probe speed has negligible effect on the glassy polymer PMMA. In contrast, probe speed is identified as an important variable for testing ice release on elastomeric Sylgard 184 coatings. While work of adhesion, which is related to surface free energy, is recognized as an important factor that can affect ice release, the results reported herein show that coating thickness can override this single parameter for elastomeric substrates.

T.S. Wong, S.H. Kang, S.K. Tang, E.J. Smythe, B.D. Hatton, A. Grinthal, J. Aizenberg, Nature 477 (2011) 443-447.

DOI:10.1038/nature10447      URL     PMID:21938066      [Cited within: 1]

J. Lv, X. Yao, Y. Zheng, J. Wang, L. Jiang, Adv. Mater. 29 (2017), 1703032.

[Cited within: 1]

X. Wu, Y. Tang, V.V. Silberschmidt, P. Wilson, Z. Chen, Adv. Mater. Interfaces 5(2018).

[Cited within: 1]

M. Cao, D. Guo, C. Yu, K. Li, M. Liu, L. Jiang, ACS Appl. Mater. Interfaces 8 (2016) 3615-3623.

DOI:10.1021/acsami.5b07881      URL     PMID:26447551      [Cited within: 1]

Bioinspired water-repellent materials offer a wealth of opportunities to solve scientific and technological issues. Lotus-leaf and pitcher plants represent two types of antiwetting surfaces, i.e., superhydrophobic and lubricant-infused

J.D. Smith, R. Dhiman, S. Anand, E. Reza-Garduno, R.E. Cohen, G.H. McKinley, K.K. Varanasi, Soft Matter 9 (2013) 1772-1780.

DOI:10.1039/C2SM27032C      URL     [Cited within: 1]

Y. Wang, H. Zhang, X. Liu, Z. Zhou, J. Mater, Chem. A 4 (2016) 2524-2529.

[Cited within: 1]

M. Amjadi K.-U. Kyung, I. Park, M. Sitti, Adv. Funct. Mater. 26 (2016) 1678-1698.

DOI:10.1002/adfm.v26.11      URL     [Cited within: 1]

ISSN: 1005-0302
CN: 21-1315/TG
Editorial Office: Journal of Materials Science & Technology , 72 Wenhua Rd.,
Shenyang 110016, China
Tel: +86-24-83978208

Copyright © 2016 JMST, All Rights Reserved.