This invention relates to underwater adhesives.
Adhesives are ubiquitous in everyday life, including both pressure-sensitive adhesives (PSAs) that are activated by pressing the adhesive onto a substrate (e.g., scotch tape or sticky notes) and curable adhesives, which are applied in the liquid state and then cured by air, heat, or light into a solid (e.g., glue or epoxy). In either case, good adhesion strength is achieved by simultaneously maximizing the substrate-adhesive contact area and the cohesive strength of the bulk adhesive material. The former requires the adhesive to readily flow over a surface at accessible timescales while the latter requires sufficient physical or chemical crosslinking to dissipate energy. While conventional adhesives have been well-optimized for dry conditions, most lose adhesion in the presence of water, which is a critical concern for biomedical and structural applications. Underwater adhesives can be loosely classified as moisture-insensitive, water-resistant, or, in the most extreme case, underwater.
Understandably, the design of new synthetic adhesives for underwater use is challenging and has inspired many approaches. In many cases, researchers have adopted bio-inspired designs that use supramolecular or electrostatic interactions based on the underwater adhesion mechanisms of mussels, sand-castle worms, or remoras. An alternative approach is to design strongly hydrophobic self-adhesive materials that can remove interfacial water and maintain bulk cohesive strength by preventing water swelling.
However, these known approaches for underwater adhesives tend to suffer from significant disadvantages, such as requiring a curing step and/or not being pressure-sensitive, reusable and/or recyclable. Accordingly, it would be an advance in the art to provide improved underwater adhesives.
Here, we consider dynamic polymers with a hydrophobic backbone to minimize water uptake. The resulting pressure-sensitive adhesives have high adhesion strength and can be applied in fully underwater conditions to polyimide, glass, and steel substrates, without any solvent or covalent crosslinking, at room temperature, and without substrate modifications. Moreover, the polymer adhesive can be readily recycled and reused.
We hypothesized that the tunable structure of dynamic polymers could be used to design simple, solvent-free, hydrophobic PSAs with good underwater adhesion. We show that dynamic polymers which possess physical crosslinking from both supramolecular interactions and topological entanglements could exhibit high cohesive strength while also readily flowing over a surface, thus maximizing adhesive strength. In an example of this work, we embed periodically-placed urethane bonds into a PFPE backbone to create linear dynamic polymers with a nanophase-separated microstructure. We optimize the bonding interactions to tune the rheological properties of the polymers to obtain high strength adhesives and show that the hydrophobicity of PFPE enables underwater adhesion by removing interfacial water and preventing water diffusion into the bulk material. Importantly, these dynamic polymer PSAs can be applied in underwater conditions, at room temperature, without any solvent or curing steps, and can be reused and recycled due to the reversible dynamic crosslinks.
This can also include cases where there is covalent cross-linking of the dynamic polymer (before or after application) as well as the inclusion of other organic or inorganic fillers to modify material properties.
We have shown that combining a hydrophobic backbone with a reversible dynamic bond (e.g., hydrogen bonding, metal-ligand coordination, pi-pi stacking, dynamic covalent bond, etc.) can be used to create strong underwater adhesives. The use of a hydrophobic backbone creates a nanophase-separated morphology, with locally high concentrations of the dynamic bond phase surrounded by a hydrophobic matrix. This matrix prevents water from disrupting the dynamic bond formation, enabling strong underwater adhesion. In addition, the hydrophobic backbone helps remove water from the substrate-adhesive interface. The principles outlined here could be applied to or combined with other types of underwater adhesives such as those that have chemical crosslinking (i.e., curing steps), employ bio-inspired functional groups (e.g., catechols), or contain additives or particles (e.g., composites) to improve performance.
Applications include, but are not limited to biomarine or biomedical applications in which adhesion to wet surfaces is required, especially when this adhesion needs to be repeatedly adhered and de-adhered or the adhesion needs to be done quickly.
Significant advantages are provided:
Section A describes general principles relating to embodiments of the invention. Section B is a detailed description of experimental examples of embodiments of the invention.
An embodiment of the invention is an underwater adhesive comprising: a hydrophobic polymer backbone having periodically embedded dynamic bonding units; where the underwater adhesive has nanophase separation between a first phase of the hydrophobic polymer backbone and a second phase of the dynamic bonding units (e.g., as shown on
The hydrophobic polymer backbone can be selected from the group consisting of: perfluoropolyether, polydimethylsiloxane, polybutadiene, and polyisoprene.
The dynamic bonding units can have a bonding mechanism selected from the group consisting of: hydrogen bonding, metal-ligand coordination, and pi-pi stacking. The dynamic bonding units can be selected from the group consisting of: urethanes, amides, urea, bipyridines, disulfide groups, and catechols.
In some embodiments, the underwater adhesive is pressure sensitive and curing-free. In some cases, the underwater adhesive can be applied when immersed in water. In some cases, the underwater adhesive is reusable.
Adhesives are ubiquitous in everyday life, including both pressure-sensitive adhesives (PSAs) that are activated by pressing the adhesive onto a substrate (e.g., scotch tape or sticky notes) and curable adhesives, which are applied in the liquid state and then cured by air, heat, or light into a solid (e.g., glue or epoxy). In either case, good adhesion strength is achieved by simultaneously maximizing the substrate-adhesive contact area and the cohesive strength of the bulk adhesive material. The former requires the adhesive to readily flow over a surface at accessible timescales while the latter requires sufficient physical or chemical crosslinking to dissipate energy.
While conventional adhesives have been well-optimized for dry conditions, most lose adhesion in the presence of water, which is a critical concern for biomedical and structural applications. Water interferes with adhesives via two key mechanisms. First, interfacial or boundary layer water can prevent good contact and reduce the available surface area between the substrate and adhesive. Second, water can diffuse into the bulk adhesive material and reduce the overall cohesive strength, either by interfering with physical crosslinks or as a chemically inert plasticizer. Adhesives developed to address these issues can be loosely classified as moisture-insensitive (i.e., adhered in conditions with interfacial water or high humidity), water-resistant (i.e., adhered in dry conditions and used in wet conditions), or, in the most extreme case, underwater (i.e., adhered and used while totally immersed in water). For example, there is a recent report of a moisture-insensitive adhesive for wound care that rapidly adheres to wet or bleeding tissues by removing boundary layer water. Importantly, however, the adhesive must remain totally dry before application, rendering the material unusable in underwater conditions.
Understandably, the design of new synthetic adhesives for underwater use is challenging and has inspired many approaches. In many cases, researchers have adopted bio-inspired designs that use supramolecular or electrostatic interactions based on the underwater adhesion mechanisms of mussels, sand-castle worms, or remoras. For example, many mussel-inspired designs incorporate catechol groups such as dihydroxyphenylalanine (DOPA) to mimic the functional groups present in mussels. Another promising alternative is the use of pre-crosslinked hydrogels, which have been show to reversibly adhere underwater to a variety of substrates through different combinations of supramolecular interactions. Critically, these mechanisms focus on achieving strong adhesion in a state where the adhesive is swollen with water.
An alternative approach is to design strongly hydrophobic self-adhesive materials that can remove interfacial water and maintain bulk cohesive strength by preventing water swelling. Previous work showed that combining hydrophobic poly(N-vinyl caprolactam) (PVCL) with short-molecular weight poly(ethylene glycol) (PEG) created a PSA with high adhesion strength for low water contents, but adhesion failed in conditions when water content exceeded 30 wt %. One report considers crosslinked ionogels with high reversible underwater adhesion strength that are filled with a fluorinated ionic liquid, to prevent water swelling for over 10 days. Another report demonstrated strong underwater adhesion of silicone surfaces using host-guest interactions, but this required pre-functionalization of the surfaces with cucurbituril host and aminomethylferrocene guest moieties. Alternatively, adding hydrophobic aliphatic side chains to polyesters with DOPA functional groups was shown to improve underwater adhesive performance, but required a UV-mediated, chemical crosslinking step. Finally, poly(catechol-styrene) polymers have shown exceptionally strong underwater adhesion but must be pre-dissolved in chloroform when applied to the substrate and cured for 24 hours before testing.
We hypothesized that the tunable structure of dynamic polymers could be used to design simple, solvent-free, hydrophobic PSAs with good underwater adhesion. Previous work has shown that long-chain, entangled polymers can dramatically improve adhesive strength of hydrogels by increasing bulk cohesive strength and preventing delamination or fracture at the interface. Similarly, we theorized that dynamic polymers which possess physical crosslinking from both supramolecular interactions and topological entanglements could exhibit high cohesive strength while also readily flowing over a surface. Moreover, our recent work has shown that dynamic polymers with evenly-spaced dynamic bonds along their backbone, termed periodic dynamic polymers, can exhibit well-defined supramolecular structures, which could improve nanophase separation between the backbones and the dynamic bonds and thus limit bulk water diffusion. For a hydrophobic backbone, we selected perfluoropolyether (PFPE) due to its high chain flexibility, low glass transition temperature, and excellent solvent resistance. PFPE-based dynamic polymers have been used for many applications including antifouling coatings or electrode coatings in batteries. Supramolecular telechelic PFPE polymers with 2-ureido-4[1H]-pyrimidone (Upy) end groups, PFPE-based vitrimers, and crosslinked PFPE polyurethanes have been previously reported but only exhibit terminal flow at or above 100° C., rendering them unsuitable for use as adhesives.
In this work, we embed periodically-placed urethane bonds into a PFPE backbone to create linear periodic dynamic polymers with a nanophase-separated microstructure. We optimize the bonding interactions to tune the rheological properties of the polymers to obtain high strength adhesives and show that the hydrophobicity of PFPE enables underwater adhesion by removing interfacial water and preventing water diffusion into the bulk material. Importantly, these dynamic polymer PSAs can be applied in underwater conditions to a variety of substrates, at room temperature, without any solvent or curing steps, and due to their reversible dynamic crosslinks they can be easily removed and reapplied without additional stimuli and readily recovered and recycled after use.
We synthesized the PFPE-based dynamic polymers using a solvent-free reaction between an initial PFPE-diol 1700 g/mol, FluorolinkE10-H) and various liquid diisocyanates (
We confirmed the successful polymerization by 1H-NMR and Fourier-transform infrared spectroscopy (FTIR) analysis (
We also characterized the microstructure of the polymers by small-angle x-ray scattering (SAXS). All polymers exhibited a single, characteristic peak corresponding to a domain size (d) between 4-5 nm (
We next characterized the rheological properties of the different PFPE polymers by performing frequency sweeps at various temperatures and performing time-temperature superposition (TTS). The resulting master curves at 55° C. for each polymer are plotted in
Plotting the shift factors for various temperatures shows a clear Arrhenius temperature dependence, which allows for the estimation of the flow activation energy (Ea,flow) for each polymer (
To characterize the adhesive properties of the various polymers, we performed 180° peel tests on pressed Kapton films prepared using a weighted hand roller. After each test, we inspected each sample to determine whether the failure mechanism was adhesive (i.e., polymer intact and separated from the substrate) or cohesive (i.e., polymer remains adhered to the substrate and breaks in the bulk). PFPE-MEBUr and PFPE-IUr exhibited the best dry adhesion strength of 11 and 9.5 N/cm, respectively (
When comparing these adhesion results to the structural and rheological characterization of the polymers presented above, we show that the dominant molecular design principle related to the adhesive strength of the polymer is tuning the G′, G″ crossover frequency (ωxc). This is consistent with the goal of balancing the cohesive strength or bulk energy dissipation of the adhesive with the ability for the adhesive to spread over the substrate, which increases surface area. The same mechanism is seen in how spiders tune glue viscosity to maximize adhesion strength. In our case, PFPE-MCUr, which exhibits the strongest hydrogen bonding and has the largest cohesive strength but its low ωxc means that it is unable to sufficiently spread over the surface for good adhesion. Alternatively, PFPE-CHUr and PFPE-HUr have high ωxc and can easily flow over the surface and maximize surface area, but this reduces their cohesive strength. Thus, PFPE-MEBUr and PFPE-IUr have a ωxc which enables them to efficiently maximize surface contact while maintaining high cohesion strength. This relationship can be seen by plotting adhesion strength versus ωxc for all of the polymers (
To study the underwater adhesion of the polymers, we conducted 180° peel tests of the polymers when fully immersed in water before and after contact with the substrate. Due to the hydrophobic nature of the PFPE backbone combined with the nanophase-separated morphology, we hypothesized that the PFPE would shield the hydrogen bonds from water and enable underwater substrate adhesion. Indeed, all the polymers maintained ˜90% of their dry adhesion strength under wet conditions (100% when considering measurement error), with PFPE-MEBUr and PFPE-IUr exhibiting the highest underwater adhesion strengths of and 8 N/cm, respectively (
We also tested the adhesion strength of PFPE-MEBUr and PFPE-IUr on different substrates. We saw similarly strong adhesion strength on steel for both polymers under dry conditions (˜11 N/cm). When tested underwater, PFPE-MEBUr and PFPE-IUr retained 70% and 50% of their dry adhesion strength, respectively, which was slightly lower than observed when adhering to Kapton film. Both PFPE-MEBUr and PFPE-IUr exhibited reduced dry and wet adhesion to high-density polyethylene, which has a much lower surface energy (˜34 mJ/m2) compared to Kapton (˜57 mJ/m2) or steel (˜50 mJ/m2). Further optimization to improve substrate-specific adhesion is an area for future study.
To make a comparison to a broader range of developed underwater adhesives, we next performed dry and underwater lap shear tests for both PFPE-MEBUr and PFPE-IUr. These results are presented in
We summarized this comparison in
Lastly, we demonstrated the underwater adhesive properties of PFPE-MEBUr by lifting fishing weights of different sizes using a small amount of adhesive placed on the fingertip. A single adhesive application of a gloved fingertip (˜1 cm2, 50 mg) was able to repeatedly lift a 10 g, and 60 g weight all while continuously adhering and de-adhering underwater. Importantly, since the material is a PSA, no curing step was needed and re-adhesion could be easily achieved in a few seconds by re-applying pressure between the glove and the weight. We also show that the weights can be lifted out of the water and remain adhered to the finger. Finally, we compared the underwater adhesion performance of PFPE-MEBUr to commercial double-sided tape, which fails to adhere to either the fishing weight or Kapton film.
In this work, we report the successful synthesis of a series of PFPE-based dynamic polymers with periodically-placed hydrogen bonding units. The synthesis is simple, scalable, and solvent-free. We show that changes in the dynamic bond can tune the rheological behavior of the samples by changing the bond strength, while periodic placement of these bonds along the PFPE backbone ensures the formation of a nanophase-separated morphology for all bond types as shown by SAXS. We evaluate the adhesion capability of all synthesized PFPE dynamic polymers and find that PFPE-MEBUr and PFPE-IUr show the best adhesive performance up to 11 N/cm under dry conditions. We show that this strong performance arises from optimizing the rheological crossover point (ωxc) and note that this point varies across the polymers due to changes in the molecular level bonding geometry of the selected dynamic bonds. Due to the hydrophobic nature of the PFPE backbone, all the polymers retain more than 90% of their dry adhesion strength in underwater conditions, leading to an achieved underwater adhesive peel strength of 10 N/cm and underwater lap shear strength of 0.26 MPa for the best performing polymer, PFPE-MEBUr.
Our results show that careful control of the G′ and G″ crossover frequency (ωxc) is preferred to optimize the adhesive strength of the polymers. We achieve this control by controlling the molecular geometry of the dynamic bonding unit along the PFPE backbone without changing the chain architecture (e.g., bond concentration, bond spacing, or chain length), which is responsible for maintaining the nanophase-separated morphology. More broadly, this work shows how dynamic polymers with tunable structures and properties are a promising platform to design materials for specific functional applications such as high strength, recyclable underwater adhesives. These adhesives could be used to enable readily attachable and detachable waterproof wearable devices that are also fully recyclable.
Diol-terminated perfluoropolyether (PFPE) oligomers (Fluorolink® E10-H, Mn=1.7 kDa) were purchased from Solvay (Belgium). Various diisocyanates, including 4,4′-methylenebis(cyclohexyl isocyanate) (MCUr), 1,3-bis(1-isocyanato-1-methylethyl)benzene (MEBUr), isophorone diisocyanate (IUr), hexamethylene diisocyanate (HUr) and 1,3-bis(isocyanatomethyl)cyclohexane (CHUr) were purchased from Sigma-Aldrich (USA). All reagents and solvents were commercially available and used without further purification.
This procedure was adapted from a previous report. PFPE-diol (Mn≈1700 g/mol, FluorolinkE10-H, 2 g.) was placed at 90° C. under vacuum for 2 hours to remove trace water. The selected diisocyanate was added in a 1:1.05 molar ratio of alcohol/isocyanate functional groups and stirred vigorously. The flask was placed under vacuum for 5 min, then flushed with N2. This process was repeated 3 times. Dibutyltin dilaurate (DBDTL, 1-2 drops) was added as a catalyst then the mixture was heated to 70° C. for 48 hours. Compared to the previous report at 125° C., we found that a lower reaction temperature of 70° C. reduced sample discoloration and prevented crosslinking of the isocyanate into a trimer, while still fully reacting all isocyanate groups (as seen by FTIR). The mixture was solidified after 48 hours. The reacted mixture was cooled to room temperature, dissolved in 8 mL of 2,2,2-trifluoroethanol (TFE), precipitated from dichloromethane (DCM), and dried. The final product was a clear, highly transparent, sticky polymer.
1H NMR data were obtained on a Varian 400 MHz spectrometer with trifluoroacetic acid-d as the solvent at room temperature. Tetramethylsilane (TMS) was used as the standard, with chemical shifts reported in 5 (ppm downfield from TMS).
ATR-FTIR (attenuated total reflection-Fourier Transform InfraRed) spectra were recorded using a Nicolet iS50 with a diamond attenuated total reflectance attachment. The polymer samples were placed directly on the sample stage and measured in air.
Dynamic mechanical analyses were conducted using an Ares G2 Rheometer with an 8 mm parallel plate set-up in a temperature-controlled convection oven. Samples were placed on 8 mm diameter discs. Frequency sweep tests were collected from 100 rad/s to 0.1 rad/s at designated temperatures with an applied strain of 1% under an axial force of 0.02N. Temperature sweeps were performed in 10° C. steps with a wait time of 180 s between steps to allow the sample temperature to equilibrate. Time-temperature superposition (TTS) was executed in Trios software when appropriate (as deemed by successful overlap in G′, G″, and tan(5) for all shifted samples). To ensure full contact between the sample and the plates, a pre-conditioning step was used, in which the sample was heated above 100° C. and a frequency sweep was performed from 100 rad/s to 0.1 rad/s under a compressive force between 0.05-2N.
Differential scanning calorimetry (DSC) was conducted using a TA instruments Q2000 DSC. Approximately 10 mg of polymer were placed in sealed aluminum pans. Samples were ramped from −50° C. to 150° C. at a rate of 10° C./min. Glass transition and melting temperatures were extracted using TA Universal Analysis software.
B4 g) Small-Angle x-Ray Scattering Methods
Small-angle x-ray scattering (SAXS) was conducted in transmission mode on bulk polymer films at beamline 4-2 at Stanford Synchrotron Radiation Light source (SSRL) of SLAC National Accelerator Laboratory (SLAC, Menlo Park, CA). Bulk polymer films were tested as free-standing films with a thickness of ˜0.1 mm. The x-ray wavelength was 0.827 Å (beam energy 15 keV) with a sample-to-detector distance of 3.512 m. The Pilatus 1M fast detector was used for 2D scattering data acquisition and reduction into scattering intensity profiles as a function of the scattering vector q was done using customized code at the beamline. For each sample, 10 frames of 1 second exposure were averaged to improve the signal-to-noise ratio. Measurements were performed in ambient air.
Contact angle measurements with water were performed on a custom set-up in ambient conditions at room temperature. Fresh films of each polymer were prepared by dropcasting from 2,2,2-trifluroroethanol (100 mg/mL), evaporating under a covered petri dish overnight, and heating at 70° C. for 24 hours. Contact angle images were analyzed with First Ten Angstroms (FTA) software.
The adhesive properties of the PFPE polymers were measured by a 180° peel test at room temperature at a peel rate of 300 ram/min. The polymers were placed on 10 mm stripe of Kapton sheet and heated on 70° C. for 24 hours to anneal a square film with a thickness of ˜0.1 mm. Kapton, steel and high-density polyethylene (HDPE) was used as a test substrate. The polymer was adhered onto the test substrates using a 2 kg hand roller rolled twice in each direction at approximately 10 mm/s. The test samples were stored in ambient conditions for 1 hour before testing. The end of the tape was pulled back at 180°, mounted in an Instron 5565 extensometer, and pulled at 300 ram/min. Peel tests were repeated three times, and the results were averaged.
The polymers were placed on 10 mm stripe of Kapton sheet and heated on 70° C. for 24 hours to anneal a square film with a thickness of ˜0.1 mm. The underwater adhesive properties of the PFPE polymers were measured by first immersing the polymers and substrates in deionized water for 1 hour. Contact between the adhesive and the substrate was made underwater by light pressing. A 2 kg hand roller was then rolled over the sample twice in each direction at approximately 10 mm/s. The adhered sample was then continually immersed in water for another hour. Finally, the sample was then immediately mounted onto the Instron 5565 extensometer for the peel adhesion test, conducted at room temperature at a peel rate of 300 ram/min. Peel tests were repeated three times, and the results were averaged.
The polymers were placed on 10 mm stripe of Kapton-covered glass slide and heated on 70° C. for 24 hours. Another Kapton slide was placed on top of the first and lightly pressed to form a lap shear joint. Samples were measured on an Instron 5565 extensometer and pulled apart at a measurements speed of 600 ram/min. The maximum force at joint failure divided by the overlap area provided the adhesion strength. Each sample was tested a minimum of three times and averaged. Double-sided scotch tape was tested in the same manner, by adhering between two Kapton-covered glass slides.
For underwater lap shear adhesion tests, the polymer-coated Kapton slide and the fresh Kapton slide were placed underwater for 1 hour. The samples were joined underwater by lightly pressing them together and then remained submerged underwater for another hour. Samples were then tested on an Instron 5565 extensometer. Each sample was tested a minimum of three times and averaged. Double-sided scotch tape was tested in the same manner, by adhering between two Kapton-covered glass slides.
Each adhesion test (peel or lap shear) was measured three times for each sample (n=3) and the error was determined by the sample standard deviation between the measurements. No pre-processing of the data or advanced statistical methods were used.
This application claims priority from US Provisional Patent Application 63/393,700 filed Jul. 29, 2022, which is incorporated herein by reference.
This invention was made with Government support under contract W911NF-21-1-0092 awarded by the Department of Defense. The Government has certain rights in the invention.
Number | Date | Country | |
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63393700 | Jul 2022 | US |