| Literature DB >> 35424313 |
Guizhong Tian1, Dongliang Fan1, Xiaoming Feng1, Honggen Zhou1.
Abstract
In the past decades, drag-reduction surfaces have attracted more and more attention due to their potentiality and wide applications in various fields such as traffic, energy transportation, agriculture, textile industry, and military. However, there are still some drag-reduction materials that need to be deeply explored. Fortunately, natural creatures always have the best properties after long-term evolution; aquatic organisms have diversified surface microstructures and drag-reducing materials, which provide design templates for the development of thriving artificial underwater drag-reduction materials. Aquatic animals are tamed by the current while fighting against the water, and thus have excellent drag reduction that is unparalleled in water. Inspired by biological principles, using aquatic animals as a bionic object to develop and reduce frictional resistance in fluids has attracted more attention in the past few years. More and more aquatic animals bring new inspiration for drag-reduction surfaces and a tremendous amount of research effort has been put into the study of surface drag-reduction, with an aim to seek the surface structure with the best drag-reduction effect and explore the drag-reduction mechanism. This present paper reviews the research on drag-reduction surfaces inspired by aquatic animals, including sharks, dolphins, and other aquatic animals. Aquatic animals as bionic objects are described in detail, with a discussion on the drag-reduction mechanism and drag-reduction effect to understand the development of underwater drag-reduction fully. In bionic manufacturing, the effective combination of various preparation methods is summarized. Moreover, bionic surfaces are briefly explained in terms of traffic, energy sources, sports, and agriculture. In the end, both existing problems in bionic research and future research prospects are proposed. This paper may provide a better and more comprehensive understanding of the current research status of aquatic animals-inspired drag reduction. This journal is © The Royal Society of Chemistry.Entities:
Year: 2021 PMID: 35424313 PMCID: PMC8694127 DOI: 10.1039/d0ra08672j
Source DB: PubMed Journal: RSC Adv ISSN: 2046-2069 Impact factor: 3.361
Typical aquatic animal materials with drag-reduction properties
| Biological prototypes | Morphology | Research methods | Drag reduction mechanism | Drag reduction rate |
|---|---|---|---|---|
| Rainbow trout ( | Swimming fish surface | The particle image velocimetry (PIV) technique | Flow separation control[ | —[ |
| The sailfish ( | V-shaped protrusions pointing downstream | An open-circuit suction-type wind tunnel and floating element apparatus | Without obvious drag reduction effect | —[ |
| Boxfish | The shape of the carapace in boxfishes | Computational fluid dynamics simulations | Destabilizing flow over the boxfish's body promotes manoeuvrability | The drag coefficient of about 0.1531 |
| Fossil of sharks[ | Riblets | Examine the diverse adaptions and review the few attempts | Streamlined and separated control[ | —[ |
| Fossil of sharks | Shark scales | Analyzed the fossil record of shark scales | 62% as drag reduction scales | —[ |
| Hawaiian stream fish ( | Adsorption climbing | Climbing trials up artificial waterfalls | Low head height exposed to high fluidity | —[ |
| European sea bass ( | Fish scale pattern | A flow channel mimic and computational fluid dynamics simulations | Low-speed and high-speed streaks inside the boundary layer and delay transition[ | 9% (20 cm s−1)[ |
| The fish ( | Geometric structure of crescent-like ridge | Numerical simulations and theoretical calculations | The “water-trapping” effect[ | 3.014% (0.66 m s−1)[ |
| The bonnethead shark ( | The flexible 3D printed shark skin | 3D printed shark skin under dynamic conditions | A leading-edge vortex with greater vorticity than the smooth control | 6.6%[ |
| Shark | Simulated shark denticle | Numerical simulations and optimization | Wake vortex suppressed[ | —[ |
| The shortfin mako ( | Shark skin | Time-resolved digital particle image velocimetry (TR-DPIV) | Scale bristling controls flow separation[ | —[ |
| A male shortfin mako shark | Flexible shark skin foil | Digital particle image velocimetry (DPIV) and control shark skin movement | Denticles promote enhanced leading-edge suction | 12.3%[ |
| Swimming bottlenose dolphins ( | Dolphin skin | Digital particle image velocimetry (DPIV) | Anisotropic compliant wall and intermittent wave motion[ | —[ |
| Odontocetes | The ridged skin | Silicone moulding compound to make moulds | Smooth skin and flexibility[ | —[ |
Fig. 1(a) The Mako shark. (b) SEM of the non-bristled scales is replicated into riblets. Reproduced from ref. 5 with permission from IOP Publishing, copyright 2017. (c) Schematic picture of the riblets. Reproduced from ref. 50 with permission from the Royal Society, copyright 2018. (d) SEM of the bristled scales is replicated into denticles and attached to the bionic surface of the flexible substrate. Reproduced from ref. 5 with permission from IOP Publishing, copyright 2017. (e) Schematic picture of the denticles with 3D printing. Reproduced from ref. 43 with permission from the Company of Biologists Ltd, copyright 2014.
Fig. 2(a) The typical cross-sectional geometries of riblets with‘ blade’,‘ sawtooth’, and ‘scalloped’ geometries. (b) Drag change rate as a function of the dimensionless parameters of riblets spacing (s), height (h), and thickness (t). The spacing and height of the riblets are the keys to the drag reduction rate, while the thickness does not seem to have any effect. The optimal spacing s+ = 15–20, height h+ ≈ 8–10, and thickness t+ = small. Compared with the oil fluid medium, the height and spacing have a strong correlation with the drag reduction rate. The optimal ratio of spacing and height gives a ratio of h/s ≈ 0.5. Reproduced from ref. 74 with permission from Cambridge University Press, copyright 2014. (c) Blade geometry shows the greatest drag reduction (11.6%). The optimization of riblet spacing (s+ = 25.3) makes the large-scale vortex lift from the wall and the small-scale vortex acts on the groove to reduce the resistance. The increase in the spacing (s+ = 41.2) makes the large vortex ‘slide down’ into the inner wall. Reproduced from ref. 69 with permission from Academic Press Inc., copyright 2016.
Fig. 3(a) Flat boundary layer structure. x = 0 as the starting point for the development of the boundary layer. Reproduced from ref. 17 with permission from American Society of Mechanical Engineers (ASME), copyright 2016. (b) Regional division and functional representation of the mean velocity profile of a smooth-flat-plate boundary layer. Reproduced from ref. 17 with permission from American Society of Mechanical Engineers (ASME), copyright 2016. (c) The schematic diagram of the velocity profile along the flow direction (left) and the span direction (right) at the crest and trough of the riblet wall. A hollow circle represents the virtual origin. Reproduced from ref. 78 with permission from Cambridge University Press, copyright 2019. (d) The evolution from large-scale vortex to a small-scale vortex. Reproduced from ref. 79 with permission from Elsevier BV, copyright 2016. (e) Comparison of average velocity profile in the boundary layer between the smooth plate and riblet. Reproduced from ref. 73 with permission from Chinese Journal of Aeronautics, copyright 2019.
Fig. 4(a) Three-dimensional reconstructed micro-CT denticle model of a mako shark (Isurus oxyrinchus). Reproduced from ref. 43 with permission from Company of Biologists Ltd, copyright 2014. (b) Scanning electron microscopy (SEM) image of dermal dentin with drag reduction. Reproduced from ref. 33 with permission from Inter-Research, copyright 2017. (c) Parameters of denticles arranged linearly on the membrane substrate. The depth of the anchor (AD), the spacing between two adjacent denticles along the stream-wise direction (SS), and the spacing between two adjacent denticles along the lateral direction (SL). Reproduced from ref. 43 with permission from Inter-Research, copyright 2014. (d) Surface profilometry images from shark skin in different parts. Reproduced from ref. 65 with permission from John Wiley and Sons Inc., copyright 2018.
Fig. 5(a) Optimization of shark single denticle. The flow velocity of the optimized denticle in the wake area is more uniform. Also, the denticles act as vortex generators to energize the boundary layer to reduce the drag. Reproduced from ref. 89 with permission from IOP Publishing Ltd, copyright 2019. (b) Flexible shark skin and bristled shark denticles (magnified 40 times). Reproduced from ref. 36 with permission from Marine Technology Society Inc., copyright 2008. (c) The evolution of fluid in the fish-spindle form. Laminar flow to turbulent flow and then to boundary layer separation to form a wake area. Comparing the non-smooth surface on the axis with the smooth surface under the axis, it has been found that the denticles control the separation of the boundary layer to decrease the wake area, thereby reducing the pressure drag. Reproduced from ref. 11 with permission from the Royal Society, copyright 2014.
Fig. 6(a) Bottlenose dolphin (Tursiops truncatus) swimming on the water. (b) Flipper, dorsal fin, and flukes of dolphin streamlined design. Reproduced from ref. 99 with permission from Elsevier, copyright 2019. (c) Distribution of pressure coefficient (flow velocities Ue = 10 m s−1 and the turbulence intensity is 1%). Reproduced from ref. 100 with permission from Springer, copyright 2013. (d) Visualization of vortices created by swimming dolphins. Reproduced from ref. 54 with permission from Elsevier, copyright 2014.
Fig. 7(a) Schematic description of the swimming process of dolphins. Leap, burst, and coast as a fast dolphin sailing a loop. Reproduced from ref. 101 with permission from Oxford University Press, copyright 2002. (b) The speed diagram corresponding to the above picture. The dolphin leaps out of the water at a speed of Uf. When hopping into the water, the speed maintained is also Uf, to a shallow depth, and it begins to coast horizontally and gradually slows down until it reaches Ui, and then rapidly bursts to Uf to start the next round of leaping. Reproduced from ref. 101 with permission from Oxford University Press, copyright 2002.
Fig. 8(a) Dermal ridges and skin folds of a dolphin. Reproduced from ref. 3 with permission from IOP Publishing, copyright 2017. (b) Three-dimensional skin structure of a bottlenose dolphin. The surface of the skin is smooth and has no obvious bulges, and the traces of skin furrows and folds can be seen. Reproduced from ref. 62 with permission from the Royal Society, copyright 2019. (c) The distribution of dolphin fold skin throughout the body. Reproduced from ref. 3 with permission from IOP Publishing, copyright 2017. (d) Schematic picture of the internal imitation of a dolphin. Reproduced from ref. 56 with permission from IOP Publishing Ltd, copyright 2006.
Fig. 9(a) Compliant wall models. Reproduced from ref. 103 with permission from Cambridge University Press, copyright 2019. (b) Compliant wall structure and the simulation for the deformation of dolphin skin along with shear stress. Reproduced from ref. 56 with permission from IOP Publishing Ltd, copyright 2006.
Fig. 10(a) Schematic diagram of the thermal boundary layer over the wing. Reproduced from ref. 107 with permission from Elsevier Ltd, copyright 2017. (b) Schematic diagram of energy conservation in the heated boundary layer. Reproduced from ref. 108 with permission from Elsevier Ltd, copyright 2019.
Fig. 11(a) The effect of the change in the pregnant fish body shape on the surrounding flow field. Reproduced from ref. 114 with permission from the Royal Society, copyright 2019. The morphological changes in the fish bottom cause the boundary layer to separate earlier due to pregnancy, thereby increasing the drag. (b) Cycloid scales and lateral line of fish (Rutilus rutilus). Reproduced from ref. 78 with permission from Cambridge University Press, copyright 2019. (c) Water-trapping effect of fish scales (Ctenopharyngodon idellus). Reproduced from ref. 41 with permission from Springer Verlag, copyright 2017. (d) The skin of sailfish. Reproduced from ref. 30 with permission from AIP Publishing, copyright 2008. (e) Scales of a paradise fish (Macropodus opercularis). Many bulges at the end of the scales. Reproduced from ref. 78 with permission from Cambridge University Press, copyright 2019. (f) The skin of filefish (N. septentrionalis). Reproduced from ref. 24 with permission from Wiley-VCH Verlag, copyright 2014. (g) The skin of fish (Carassius auratus). Reproduced from ref. 115 with permission from Science Press, copyright 2012. (h) Spines of the adult puffer. Reproduced from ref. 116 with permission from Wiley-Liss Inc., copyright 2020.
Fig. 12(a) SEM and X-ray images of the morphological structure of mucus storage. Two pictures of loach on the left, two pictures of hagfish on the right. Reproduced from ref. 120 with permission from Royal Society of Chemistry, copyright 2019. (b) Schematic diagram of bionic surface slippage injected with mucus. (c) Scales from the central region of fish (Lepomis macrochirus). Reproduced from ref. 121 with permission from Elsevier GmbH, copyright 2016. (d) Fish scales and mucus work together to form streaks. Reproduced from ref. 39 with permission from Company of Biologists Ltd, copyright 2019.
Various fabrication methods used in drag reduction
| Manufacture methods | Morphology | Material | Reason for drag reduction | Drag reduction rate |
|---|---|---|---|---|
| Composite micro-imprinting method with subsequent electrodeposition | A durable, metallic surface with highly-ordered hierarchical structures | Polydimethylsiloxane (PDMS) nanomold, polymerization of a UV method | Air-layer effect/secondary vortex generation | 36%[ |
| 3D printed[ | The sinusoidal shape of the dermal ridges of the dolphin | 3D printing materials | Separation control to delay flow separation in turbulent boundary layers | —[ |
| Direct micro-imprinting method | Hook-like scales | Toluene-diluted PDMS | Anisotropic oil repellence | —[ |
| Laser engraving method[ | Shark inspired low-drag microstructured surface | Cast acrylic | Lifting and pinning vortices | 26%[ |
| Lathe machining[ | Bionic pipelines with transverse microgrooves | Aluminum[ | Vortex ‘cushioning’ and ‘driving’ effects | 3.21%[ |
| Spray-painting | The fish scales ( | The substrate with the paint mixture | Slip and gas–solid contact instead of liquid–solid contact | 10%[ |
| Coating[ | Self-texturing compliant bionic materials | ZnO and PDMS mesh modified with | Rolling friction instead of sliding friction | 49% (0.6 m s−1)[ |
| 3D printed | The fish ( | 3D printing materials | Microstructure produces a fluid-lubrication layer | 2.805% (0.66 m s−1)[ |
| Magnetron sputtering | Riblets structured coatings | Nickel base alloy | The reduction of the wall shear stress | 4.9%[ |
| Bio-replicated rolling method | Shark-fin-like superhydrophobic surface | Poly(dimethylsiloxane) (PDMS) and zinc oxide (ZnO) | The “air layer” formed[ | —[ |
| Bio-replicated rolling method | Hark-skin-inspired micro-riblets | Polyvinyl chloride (PVC) and polyethene terephthalate (PET) films | — | —[ |
| Micro-electrical discharge machining (micro-EDM) | Microgrooves | Soft gelatin gel | — | —[ |
| Bio-replicated rolling method | Continuous shark-skin manufactured surface | A semi-cured coating | The ‘backflowing’ and vortex phenomenon is weakened[ | 11%[ |
| High-speed wire electric discharge machining | Microgrooves | Metal plates | — | —[ |
| Casting and spraying | Dual-function surface | Liquid polyurethane and 3-(aminopropyl)triethoxysilane (APTES) | Slip and gas–solid contact instead of liquid–solid contact | 36.7%[ |
| The cold rolling process | The micro-dimples | Metal (Al/Cu) | Increase in water contact angles[ | 12%[ |
| 3D printing with anodic oxidation | Transverse microstructures | Nanoporous TiO2 films on Ti foils | Sliding friction changes to rolling friction | 40% (1.5 m s−1)[ |
| Etching and coating | Microchannel with superhydrophobic | Zinc substrate | Slip and gas–solid contact instead of liquid–solid contact | 4%[ |
| Micro-moulding technique | A nylon honeycomb microstructure coated with parylene C | Nylon and parylene C | Slip and gas–solid contact instead of liquid–solid contact[ | 36 ± 0.6%[ |
| Photolithography, micro-moulding, and dip-transfer printing | Bio-inspired surface micropillar coating | Photoresist, silicone rubber, liquid polyurethane, and rigid polyurethane | Reduces flow separation but does not rely on hydrophobicity[ | Lift coefficient increase 25%–40%[ |
| Gas-blowing process | Micro through-hole array by a flexible skin-like device | PDMS-treated polyamide screen | Gas–solid contact instead of liquid–solid contact, reduce vortex formation and flexibility[ | 34%[ |
| Bio-replication rolling and coating technology | Bio-replication shark-skin by large-area fabrication | Rapid UV curable paint | Hydrophobicity and slip[ | 12%[ |
| Direct micro-imprinting method | Bio-replicated shark skin with polymer additive | Polyacrylamide (PAM) and silicone rubber | Combined drag-reduction effect | 24.6% (8 m s−1) & 80% (polymer)[ |
| Direct micro-imprinting method | Large-scale equal-proportional amplification bio-replication sharkskin | Solvent-swelling PDMS | — | 11%[ |
| UV grafting process[ | Biomimetic riblet surfaces | The grafted PAM and PDMS | — | 14%[ |
| Direct micro-imprinting method | Biomimetic shark surfaces | Epoxy resin and silicon rubber | Riblets and slip[ | 12.5%[ |
| Direct micro-imprinting method[ | Large-proportional shrunken bio-replication of shark skin | The shrinkage of UV-cured material | — | 11%[ |
| Bio-replicated rolling method[ | Continuous vivid shark-skin surface | Silicon rubber and original shark skin | — | —[ |
| Direct micro-imprinting method | Transverse or longitudinal stretched shark-skin | Resin polymer and silicon rubber | The second vortexes are generated, gas–solid contact instead of liquid–solid contact and slip[ | 14%[ |
| 3D printed[ | A textured surface with different shark-skin scale orientation | Acrylonitrile butadiene styrene (ABS) | Less energy exchange between the fluid layers[ | 9%[ |
| High precision milling[ | Micro/nano-texture with biocompatibility | Ti-6Al-4V | — | —[ |
| Nanosecond pulse laser process[ | Riblets on a wind turbine airfoil | — | Separation control and boundary layer theory[ | 6%[ |
| Electrochemical micromachining[ | Micromilling of microgrooves | Titanium | — | —[ |
| Laser shock imprinting | Surface morphology of the micro-pattern | Aluminium foil | — | —[ |
| Abrasive machining | The converging riblets surface | — | Riblets, protruding height theory and hence secondary flow[ | —[ |
Fig. 13(a) Brief process of shark's two types of direct bio-replicated micro-imprinting method. Method I: PDMS mixed with the curing agent is utilized in the positive template and then epoxy resin is added as a copy surface material to be used in the positive template. Method II: the hot embossing method for the positive template (the flat polymethyl methacrylate (PMMA) and epoxy resin are the same as method one as the surface material to be utilized in the positive template). The final replicated surface has a high degree of similarity with real skin in performance. Reproduced from ref. 133 with permission from American Scientific Publishers, copyright 2014. (b) Schematic of the improved direct bio-replicated micro-imprinting method. The replicated shark surface is stretched horizontally or vertically to achieve higher drag reduction. Reproduced from ref. 136 with permission from Springer Berlin Heidelberg, copyright 2015. (c) Illustrations of the reproduction of the prototype with a biological skin-like hair. On the far right is the SEM image of the skin replica. The replicated skin maintains a high degree of similarity with the original skin and the oleophobic properties are not lost. Reproduced from ref. 24 with permission from Elsevier GmbH, copyright 2014.
Fig. 14(a) Image of the bio-replicated rolling method. Compared with the direct bio-replicated micro-imprinting method, large-area manufacturing is its main feature. The real shark skin is processed by pre-treatment and fixation, sputtering, and lithography, which eliminate the disadvantages of the wedge angle and make the shark-skin softer to make it into a roller. Finally, a bionic surface is prepared through the rolling and turnover steps. Reproduced from ref. 172 with permission from Company of Elsevier B.V, copyright 2013. (b) Image of the replication of shark skin-inspired micro-riblets by the rolling method. Imitation of the shark micro-rib structure as the surface of the roller. Reproduced from ref. 158 with permission from Institution of Engineering and Technology, copyright 2017. (c) Bio-replicated rolling method to manufacture a shark-fin-like surface. Reproduced from ref. 157 with permission from Elsevier B.V, copyright 2019.
Fig. 15(a) Images of the 3D print of a mako shark (Isurus oxyrinchus) skin denticle. Reproduced from ref. 2 with permission from Company of American Physical Society, copyright 2016. (b) 3D-printed shark denticles are combined with a flexible substrate to prepare a bionic shark skin (each denticle is about 1.5 mm length). Reproduced from ref. 43 with permission from Company of Biologists Ltd, copyright 2014. (c) Three-dimensional modelling of the shark skin surface and 3D printing formed by arranging the scales in different directions. Reproduced from ref. 174 with permission from Company of Springer Nature, copyright 2018.
Fig. 16(a) Precision grinding of the microstructures. Reproduced from ref. 185 with permission from MDPI (Basel, Switzerland), copyright 2020. (b) Schematic diagram of the cutting steps of the micro-textured surface. Reproduced from ref. 145 with permission from SAGE Publications Ltd, copyright 2016. (c) Image of the electrochemical machining method (ECM) to process the sub-millimetre microstructures. Reproduced from ref. 186 with permission from Springer Nature, copyright 2019. (d) Schematic illustration of a laser interference lithography processing method to process the microstructures on the metal surface. Reproduced from ref. 176 with permission from Royal Society of Chemistry, copyright 2019.
Fig. 17(a) Image of riblet surfaces with the superhydrophobic coating. Reproduced from ref. 189 with permission from Elsevier, copyright 2018. (b) Schematic diagram of the compliant surface of the bottom of the ship. Reproduced from ref. 37 with permission from Society of Naval Architects and Marine Engineers, copyright 2019. (c) Schematic diagram of smooth and riblet surfaces with UV grafting polymerization. Reproduced from ref. 170 with permission from John Wiley and Sons Inc., copyright 2015.
Fig. 18(a) Image of manufacturing a micro through-hole layer by gas-blowing and the SEM image of a flexible substrate. Reproduced from ref. 190 with permission from IOP Publishing, copyright 2017. (b) Schematic diagram of laser shock micro-pattern imprinting. Reproduced from ref. 181 with permission from Elsevier Ltd, copyright 2019.
Fig. 19Application of bionic drag-reduction surfaces (traffic, energy resources, sports, agriculture, and other applications).