Abstract
The traditional propeller-based propulsion of underwater robots is inefficient and poorly adapted to practice. By contrast, underwater biomimetic robots show better stability and maneuverability in harsh marine environments. This is particularly true of undulating propulsion biomimetic robots. This paper classifies the existing underwater biomimetic robots and outlines their main contributions to the field. The propulsion mechanisms of underwater biomimetic undulating robots are summarized based on theoretical, numerical and experimental studies. Future perspectives on underwater biomimetic undulating robots are also presented, filling the gaps in the existing literature.
Keywords: underwater biomimetic robots, undulating propulsion robots, undulating propulsion mechanism, experimental study
1. Introduction
Underwater robots have an important role to play in future marine development and underwater activities and have broad application prospects and great potential value [1,2,3,4,5]. Researchers have designed various underwater robots for underwater missions, such as remotely operated vehicles (ROVs) and autonomous underwater vehicles (AUVs) [6,7] (Figure 1). Traditional underwater robots are composed of rigid materials and most are propelled by propellers [8,9]. However, propeller propulsion is unsuitable for implementation in harsh marine environments as it can damage aquatic life or the seabed or even become trapped in weeds [10,11]. In addition, the low efficiency and stability of propeller-driven craft in low-speed attitude adjustment conditions greatly limit the applications of propeller propulsion. Therefore, novel underwater propulsion methods are desired and are currently being investigated [7].
Figure 1.
Overview of ROV and AUV application scenarios.
At present, increasing attention is being paid to bionics-based propulsion mechanisms. This propulsive method is validated in marine environments as its principle is inspired by various marine organisms. The soft bodies, good flexibility and strong environmental adaptability of marine organisms inspire new ideas for the development of underwater robots [12]. After a long period of evolution, fish have adapted to exploit the principle of hydrodynamics to move forward using tail fins or pectoral fins [13,14,15], which has become the best way to move in water [16,17]. The propulsion method employed by fish can maintain high maneuverability and change posture according to the changing environment. Inspired by the fish propulsion method, the first underwater bionic robot RoboTuna [18] was unveiled in 1994, and various types of underwater bionic robots continue to emerge. Equipped with various propulsion methods, underwater robots present positive development trends and broad application prospects [19,20,21,22,23] The term underwater biomimetic robot generally refers to robots that imitate the structure, function, or type of movement of fish species [24]. They have the basic movement characteristics of biomimetic fish and are continuously being optimized and improved on this basis. They have diverse functions, strong environmental adaptability and stability [25]. Undulating propulsion biomimetic robots are propelled by the undulating of pectoral fins, caudal fins and the body, an approach that has superior motion performance and can realize multiple motion modes [26]. In summary, undulating propulsion underwater biomimetic robots are increasingly favored by scholars due to their good maneuverability and stability. Distinct from previous reviews [7,27,28,29,30,31,32,33,34,35,36,37], this work provides a review of undulating propulsion biomimetic robots, especially the different types of propulsion mechanisms. The review is organized as follows: In Section 2, the swimming patterns of fish are described. In Section 3, an overview of existing underwater robots with undulating propulsion is presented. In Section 4, the propulsion mechanisms of undulating propulsion underwater robots are described. In Section 5, the limitations and perspectives of fluctuation-propelled underwater robots are outlined.
2. The Swimming Mode of Fish
Starting from the morphological function of fish, there are many swimming modes of fish in nature, the most authoritative classification of which, based on the organ of propulsion, was first proposed by Breder and Webb [38]. There are two main categories of propulsion methods, body caudal fin (BCF) propulsion and median paired fin (MPF) propulsion. In 1978, Lindsey [39] classified the different families of fish species according to their mode of propulsion, which provided the essential foundation for the improvement of the overall performance of undulating propulsion biomimetic robots.
Figure 2 shows the fish species that employ BCF mode propulsion [32]. For this propulsion mode, the main body types are anguilliform, subcarangiform, carangiform, thunniform and ostraciiform, and the representative fish species for these body types are the eel, trout, herring, tuna and longhorn cowfish, respectively. Fish employing BCF mode propulsion gradually transition from undulating to oscillatory propulsion according to their different driving methods, as shown by the dashed line in Figure 2. In the figure, the first three propulsion modes are undulating and the last two are oscillatory. BCF propulsion modes are characterized by a high swimming speed—swordfish can reach a speed of 110 km/h—and good energy efficiency—tuna can maintain 90% energy efficiency while swimming for a long time [40]. Fish with the anguilliform body type employ fluctuations of the whole body and tail fin. This type of fish has a slender body and a faster swimming speed. Subcarangiform and carangiform fish species are relatively similar; the difference is that the former uses 1/2 of their body length for fluctuations, while the latter uses only about 1/3 of their body length for propulsion [41,42]. Compared with the anguilliform model, the fluctuation range is small, but the caudal fluctuation frequency is high. The propulsion of thunniform fish comes from the tail fin [43]. Based on hydrodynamic models, thunniform propulsion has been estimated to produce mechanical efficiencies in the range of 80–90% [18,44,45]. The fastest fish (tuna, dolphin) use this propulsion mode [46,47,48,49]. Fish species with the ostraciiform body type adopt an oscillatory propulsion mode. This type of fish simply oscillates the caudal fin, which induces only a small thrust; thus, the speed of travel is relatively slow [50].
Figure 2.
BCF propulsion mode [29].
Figure 3 shows the fish that employ MPF mode propulsion [32]. The main body types seen are rajiform, diofontiform, amiiform, gymnotiform, balistiform tetraodontidae and labriform, and the corresponding representative fish species are the stingray, puffer fish, bowfin fish triggerfish, yellowfin puffer and wrasse, respectively. The first five body types employ undulating propulsion, and the latter two employ oscillatory propulsion. As shown by the dotted line in Figure 3, most of the fish that employ MPF mode propulsion exhibit undulating propulsion. Rajiform fish species have soft and wide pectoral fins in a triangular shape and use the large fluctuations of the pectoral fins to generate driving power [51]. The most representative diodontiform fish species is the puffer fish. The puffer fish utilizes fluctuation of the pectoral fins on both sides of its body to propel [52]. Compared with rajiform fish species, the pectoral fins of diodontiform fish are smaller; thus, the traveling speed is slower. Amiiform fish generally have very long dorsal fins, which leads to larger amplitude waves during undulations, enabling larger movements [53]. Gymnotiform fish are similar to amiiform fish, except that their propelling fins are on the lower side of their bodies, and the power to move is generated through the oscillatory movement of the anal fin [54]. Balistiform fish generate the driving force using their dorsal and anal fins [55]. Balistiform-based locomotion has a very high propulsive efficiency compared to BCF propulsion modes. And compared to propulsion arising from the undulation of a slender fin, balistiform-based locomotion allows more maneuverability [56].
Figure 3.
MPF propulsion mode [29].
Overall, it appears that BCF-based propulsion permits a higher travel speed than MPF-based propulsion, and uses the rapid oscillation of wings to obtain efficient propulsion [56]. For example, in terms of BCF mode, the average swimming speed of Chinook salmon is 0.6 m/s, and their maximum swimming speed can exceed 6 m/s [57]. The swordfish, with its carangiform body type, has a swimming speed close to 2 m/s, and its maximum speed can even reach 27 m/s [58]. Conversely, with MPF mode, the average swimming speed of the fish is relatively slow. For example, the average swimming speed of the common stingray is 0.81 m/s, and its maximum speed is only 13 m/s [59]. It can be seen that most of the fish employing BCF-based propulsion swim faster than fish employing MPF-based propulsion. Different fish species have different morphological functions, which guarantee their survival. Researchers should study the morphological functions of fish species for use as the inspiration for bionics-based propulsion systems.
3. Classification of Undulating Propulsion Underwater Robots
Inspired by various morphological functions of fish species, underwater biomimetic robots have been designed and developed. On the basis of inheriting the characteristics of biomimetic objects, different materials and structures have been applied to optimize biomimetic robots. In this section, according to the requirements of application scenarios, the motion performance and travel efficiency of underwater biomimetic robots are highlighted. The corresponding underwater biomimetic robots are classified according to the biometric fish model that serves as their inspiration, and recent developments are also briefly presented.
3.1. Anguilliform Biomimetic Robots
Anguilliform biomimetic robot fish, mainly inspired by the soft eel, have flexible joints and fluctuate their flexible bodies and tail fins to produce motion [60]. The AmphiBot II, which was designed by Alessandro Crespi, featured a maximum torque that was 3.5 times higher than that of the earlier AmphiBot I, which greatly enhanced its propulsion efficiency [61]. Salamandra Robotica II can crawl and swim both on land and in water. To further enhance the working capabilities of such robots, the Lampetra Project robot was proposed, which not only had muscle-like execution capabilities but also can work continuously for 5 h [62]. With the gradual maturation of the biomimetic robot design concept, the modular research method was applied in the Mamba Waterproof Snake Robot [63] and Multi-joint Underwater Robot [64], which not only facilitated the subsequent upgrading of the robots but also improved the propulsion efficiency. Details of the above-mentioned designs are presented in Table 1.
Table 1.
Anguilliform biomimetic robots.
Robot | Date | Description | Main Contributions | Picture |
---|---|---|---|---|
Multi-Joint Underwater Robot [64] | 2022 |
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Soft Eel Robot [65] | 2022 |
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Mamba Waterproof Snake Robot [63] | 2014 |
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Salamandra Robotica II [66] | 2013 |
|
|
N/A |
3.2. Subcarangiform and Carangiform Biomimetic Robots
Subcarangiform and carangiform fish have similar movement patterns. Robots with these forms have high undulating propulsion efficiency, fast swimming speed, and high application value, and hence, numerous studies have been conducted, as shown in Table 2. The G9fish was a relatively mature subcarangiform robotic fish [67]. Its design was derived from a set of mature underwater biomimetic robots motion modeling methods and it could realize two traveling modes, straight−line cruise and C−shaped sharp turn. Relying on mature motion modeling methods, the number of motion modes of biomimetic robots has constantly increased. Hydraulic Soft Robotic Fish could realize diving swimming and the Wire−Driven Robot Shark could realize ascending swimming and position−maintaining actions [68]. In addition, the Soft−Bodied Robotic Fish [69] could simulate escape response maneuvers and the Fabricated Bionic Robotic Fish [70] could actively avoid obstacles and quickly determine the shortest path to a target point. To further improve the kinematic performance of underwater robots, some scholars have focused their research on innovations in biomimetic materials. Compared with biomimetic robots with rigid structures such as ISplash−I [71], ISplash−II [72] and the Four−link Robotic Fish [73], the Biomimetic Fish Robot [74] used piezoelectric composites for the robot’s muscle structure. The Fabricated Bionic Robotic Fish utilized spring−based shape memory alloys as propulsion mechanisms, which not only improved its kinematic performance but also greatly enhanced its maneuverability [70].
Table 2.
Subcarangiform and carangiform biomimetic robots.
Robot | Date | Description | Main Contributions | Picture |
---|---|---|---|---|
Untethered High−Performance Robotic Tuna [75] | 2022 |
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Untethered Bioinspired Robotic fish [76] |
2022 |
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Bio−inspired AUV [77] | 2021 |
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Four−link Carangiform Fish Robot [78] | 2016 |
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Four−link Robotic Fish Large Pectoral Fin Control Surfaces [73] | 2014 |
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Soft−bodied Robotic Fish [69] | 2013 |
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Self−contained Hydraulic Fish [79] | 2013 |
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Improved ACP Robot Fish [80] | 2012 |
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G9fish [67] | 2010 |
|
|
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Fabricated Bionic Robotic Fish [70] | 2021 |
|
|
N/A |
ACP Robot Fish [81] | 2018 |
|
|
N/A |
3.3. Thunniform and Ostraciiform Biomimetic Robots
Thunniform and ostraciiform fish employ the oscillatory propulsion mode. Their traveling speed is fast; however, their mobility is inferior. There have been relatively few studies of this type of motion due to the limited number of application scenarios [82]. As shown in Table 3, the Miniature Robotic Fish took live fish as the biometric research object, studying the interaction between robotic fish and live fish to provide a basis for the study of fish habits [83]. The Gliding Robotic Dolphin combined the advantages of dolphins and underwater gliders, which not only increased the speed of the robots but also enabled the smooth gliding motion and attitude adjustment of the robot [84]. Although the Single−Motor−Actuated Robotic Fish [85] and Thunniform Robotic Fish [43] had a simple structure, they performed well in terms of motion and maneuverability.
Ostraciiform biomimetic robots have three propulsion modules, a tail fin and two pectoral fins. With the help of the CPG control network, the BoxyBot could swim in water and crawl on the ground [86]. The Boxfish−like Robot could swim in three dimensions and used a rolling motion for attitude control, which greatly enhanced its motion performance [87]. Details of the above−mentioned designs are provided in Table 4.
Table 3.
Thunniform biomimetic robots.
Robot | Date | Description | Main Contributions | Picture |
---|---|---|---|---|
Single−Motor−Actuated Robotic Fish [85] | 2016 |
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Gliding Robotic Dolphin [84] | 2015 |
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Thunniform Robotic Fish [43] | 2022 |
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N/A |
Mackerel Robot [88] | 2013 |
|
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N/A |
Table 4.
Ostraciiform biomimetic robots.
Robot | Date | Description | Main Contributions | Picture |
---|---|---|---|---|
Boxfish Robot [86] | 2017 |
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Boxfish−like Robot [87] | 2013 |
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BoxyBot [89] | 2007 |
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N/A |
3.4. Rajiform Biomimetic Robots
Inspired by rajiform fish, some biomimetic robot fish employing the MPF propulsion modes have been proposed, as listed in Table 5. The skate is a typical rajiform with a flat body, wide pectoral fins and large fluctuating motions. Inspired by the skate’s soft body skeleton, the Self−Powered Soft Robot developed by Zhejiang University had high application value and consisted of a full−body soft structure without any rigid structure [90]. In addition, it used a dielectric elastomer material for its flutter wings, with electronic components integrated into a silicone body, and was successfully launched in a field test in the Marianas Trench down to a depth of 10,900 m. Other rajiform underwater biomimetic robots also demonstrated good kinematic performance, such as the IPMC Manta Ray [91], the Manta Ray Robot [92] and the Bionic Fin Manta Ray [93]. The difference between these three robots is their material implementation, that is, IPMC Manta Ray was made of ionic polymer metal composite materials, the Manta Ray Robot was made of three flexible materials, and the Bionic Fin Manta Ray was made of flexible PVC material. Both the Soft Body Single−Dual Actuator Ray [94] and the Cartilage Structure Underwater Robot [95] were inspired by stingrays, with the former being made of silicon−based cartilage and the latter being made of steel.
Table 5.
Rajiform biomimetic robots.
Robot | Date | Description | Main Contributions | Picture |
---|---|---|---|---|
Cartilage Structure Underwater Robot [95] | 2021 |
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Manta Ray Robot [92] | 2021 |
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Hybrid Manta Ray Robot [96] | 2021 |
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RoMan−II [97] | 2012 |
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Self−powered Soft Robot [90] | 2021 |
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N/A |
Bionic Fin Manta Ray [93] | 2015 |
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N/A |
IPMC Manta Ray [91] | 2012 |
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|
N/A |
3.5. Amiiform Biomimetic Robots
The Amiiform differs from the gymnotiform in that its undulating propulsion mechanism is a dorsal fin. As shown in Table 6, RoboGnilos [98] and the Bio−inspired Amphibious Robot [99] were inspired by Gmnarchus Niloticus. The former had an undulating dorsal fin above the body and the latter had undulating fins symmetrically distributed on both sides of the body.
Table 6.
Amiiform biomimetic robots.
Robot | Date | Description | Main Contributions | Picture |
---|---|---|---|---|
Bio−inspired Amphibious Robot [99] | 2021 |
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RoboGnilos [98] | 2009 |
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Dorsal Undulation Fin Robot [100] | 2016 |
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N/A |
3.6. Gymnotiform Biomimetic Robots
Gymnotiform and anguilliform fish are similar, but gymnotiform fish are propelled by undulating ventral and anal fins, while anguilliform fish are propelled by undulating body and caudal fins. As shown in Table 7, most of the gymnotiform biomimetic robots were inspired by the black ghost knife fish, such as the NKF−II [101], Gymnotiform Undulating Fin Robot [102] and Undulatory Fin Propulsion Bio−Inspired Robot [103]. The Robotic Knifefis was inspired by the South American electric knife fish, and its key drive parameters were investigated for the undulating propulsion of the ribbon fin [104].
Table 7.
Gymnotiform biomimetic robots.
Robot | Date | Description | Main Contributions | Picture |
---|---|---|---|---|
Undulatory Fin Propulsion Bio−Inspired Robot [103] | 2018 |
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Gymnotiform Undulating Fin Robot [102] | 2018 |
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Knifefish Robot [105] | 2011 |
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Robotic Knifefis [104] | 2011 |
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N/A |
3.7. Labriform Biomimetic Robots
Labriform biomimetic robotic fish employ the oscillatory propulsion mode, as shown in Table 8. Related underwater biomimetic robots use the oscillating travel of the pectoral and caudal fins, but to date, there have been few studies published. The Pectoral Fin and Dual Caudal Fin Robot used the tail fin as the main propeller and was capable of free swimming and active obstacle avoidance [106]. The Flexible Pectoral Fin Joint Labriform Robot used the rigid pectoral fin as the main propulsion structure, which was connected by flexible feather joints to enhance motion performance [107].
Table 8.
Labriform biomimetic robots.
Robot | Date | Description | Main Contributions | Picture |
---|---|---|---|---|
Wrasse Robot [108] | 2009 |
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Pectoral Fin and Dual Caudal Fin Robot [106] | 2016 |
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N/A |
4. Undulating Propulsion Underwater Robot Propulsion Mechanisms
Exploring the propulsion mechanisms of underwater biomimetic robots is essential for the development of new prototypes and the continuous refinement of existing types. Researchers have investigated propulsion mechanisms by three main methods: theoretical analysis, numerical simulation and experimental testing. The main findings are presented below.
4.1. Theoretical and Numerical Simulation Studies
British scholar James Gray observed the daily food intake and swimming distance of dolphins in 1936 and found that the work done by dolphins swimming was seven times the energy provided by the food they ate, which was called ‘Gray’s problem’ [109]. Gray pioneered the study of biomimetic fish. In 1952, the British physicist Geoffrey Taylor proposed an analytical model based on the resistance theory [110]. He used the ‘static fluid theory’ to solve the dynamics of fish movement. The theory considered the influence of viscous force but the effect of fluid inertial force was ignored, and hence, it was only suitable for small Reynolds number conditions. In 1955, Hancock [109] built on this achievement and put forward the ‘large−scale resistance theory’; however, the effect of fluid inertial force was still ignored. In 1960, Lighthill [111] derived an initial mathematical model of the propulsion mechanism of trevally fish; inspired by the ‘slender body theory’, he successfully applied the theory to the hydrodynamic analysis of fish swimming and then, in 1970, proposed the ‘large−oscillatory slender body theory’ according to the oscillatory amplitude of fish fins [112]. In 1960, Wu et al. [113,114,115] proposed the ‘two−dimensional undulating plate theory’, in which the research object was simplified into a flexible two−dimensional thin plate with zero thickness and simultaneously considered the inertia, leading−edge suction and wake spread. In 1971, based on the theory of two−dimensional plate fluctuations, the ‘unsteady two−dimensional undulating plate theory’ was proposed, and it was successfully used to analyze the motion performance of flat crescent−shaped fishes. In 1977, Chopra [116] studied the changes in shape of fish fins of different shapes when swimming and developed the ‘two−dimensional resistance theory’, which was considered to consist of the ‘large−oscillatory resistance theory’ and the ‘large−oscillatory slender body theory’. In 1991, Cheng et al. [117] simplified the fish model into a three−dimensional elastic plate and proposed the ‘three−dimensional undulating plate theory’.
With the application of the digital particle imaging tester (DPIT) to the research of fish propulsion mechanisms, studies have become focused on the relationship between eddy currents and fish swimming [118]. In 1994, Stamhuis [119] first applied DPIT technology to study live fish and analyze the changes in the surrounding flow field when the fish swam. Triantfyllou [120] observed that jets appeared behind the body when fish swam, and put forward the ‘jet propulsion theory’. Recently, with the mature application of simulation software and fluid dynamics software, CFD is used increasingly for kinematics and dynamics analysis [121].
Wai Pik Lau [122] derived a propulsion model for underwater biomimetic robots based on elongated body theory and created a simulation model for kinematic analysis. The Mackerel Robot designed by Li Wen used this simulation model to analyze the relationship between amplitude, efficiency and propulsion speed [88]. As shown in Figure 4, a simulation of the kinematic body drag distribution of a robot fish was carried out by Iliya Mitin et al. [43]. Finite element analysis of the kinematics and hydrodynamics of a robot fish was carried out by Qimeng Liu et al. [92].
Figure 4.
Simulations of some biomimetic robotic fish. (a) Thunniform Robotic Fish [43] (b) Manta Ray Robot [92].
There is still a certain gap between theoretical derivation, numerical simulation results and actual testing of robot fish due to factors such as the material, structure, and operating environment of underwater biomimetic robots. Although simulation results can be utilized as a reference for mechanism exploration, it is still of critical importance to carry out an experimental study of the prototype.
4.2. Experimental Studies on the Propulsion Mechanism
4.2.1. Experimental Studies of Anguilliform Robots
As shown in Table 9, the Multi−joint Underwater Robot was tested in a river and the curves of lateral motion and longitudinal motion were obtained. The overall motion curve was smooth, which verified the good motion performance of the robot in the river [64]. The soft eel robot was tested in a water tank in the laboratory. With the help of high−speed cameras, it was found that swimming efficiency was dependent on both body fluctuations and body posture in situ [65]. The Lampetra Project has conducted experiments both in a laboratory tank and on land. They found that the robot was able to autonomously avoid different obstacles and swim continuously at the speed of a real creature for 5 h. The robot has a length of 0.99 m and a velocity of 0.3 m/s. For an anguilliform robot, this is a relatively high swimming speed [62]. Experiments on Salamandra Robotica II also showed that changing the curvature of the body can control the trajectory of the robot [66].
Table 9.
Anguilliform biomimetic robots: experimental research.
Robot | Test Objectives | Test Conclusions | Picture |
---|---|---|---|
Multi-Joint Underwater Robot [64] |
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Soft Eel Robot [65] |
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Salamandra Robotica II [66] |
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N/A |
4.2.2. Experimental Studies of Subcarangiform and Carangiform Robots
As shown in Table 10, G9fish demonstrated that biomimetic modeling with the approximation function was feasible. It has a length of 0.52 m and a speed of 0.2 m/s. [67]. Experiments with the Biomimetic Fish Robot showed that the shape and oscillating frequency of the tail fin directly affected the swimming speed, and the robot reached the highest swimming speed at the natural frequency of the driving tail system [74]. Experiments with the ACP Robot Fish proved that materials used in soft biomimetic robots needed to have different bending moments [81]. The Hydraulic Soft Robotic Fish was a flexible biomimetic robot that could achieve continuous body deformation in water, and it relied on the manufacture of soft drives, utilizing the creation of arbitrary fluid passages to achieve a wide range of continuous curved profiles [68]. The parameters of the Fabricated Bionic Robotic Fish [70], ISplash-I [71] and ISplash-II [72] were verified through experiments, and their speed in the tank was close to that of real fish, showing good motion performance. In particular, ISplash-I can reach 0.85 m/s, which is a relatively high speed [71]. According to experiments with the CPG-based Biomimetic Robotic Fish, the forward speed of the robot increased with the oscillating amplitude and frequency of the body [123].
Table 10.
Anguilliform biomimetic robots: experimental research.
Robot | Test Objectives | Test Conclusions | Picture |
---|---|---|---|
Untethered High-Performance Robotic Tuna [75] |
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Untethered Bioinspired Robotic Fish [76] |
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G9fish [67] |
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Bio-inspired AUV [77] |
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Soft-bodied Robotic Fish [69] |
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Improved ACP Robot Fish [80] |
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Four-link Carangiform Fish Robot [78] |
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Four-link Robotic Fish Large Pectoral Fin Control Surfaces [73] |
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Fabricated Bionic Robotic Fish [70] |
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N/A |
ACP Robot Fish [81] |
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N/A |
4.2.3. Experimental Studies of Thunniform Robots
As shown in Table 11, researchers analyzed the motion speed of Thunniform Robotic Fish and the mechanical characteristics of the tail fin and it was found that speed increases with increasing vibration frequency of the tail fin [43]. The vortex field behind the Miniature Robotic Fish’s movement and on both sides of its body was analyzed and it was found that non-static water flow would attract live fish [83]. The relationship between the amplitude, efficiency and travel speed of the Mackerel Robot was studied to determine the optimal propulsion efficiency of the robot. It has a length of 0.588 m and a speed of 0.3 m/s [88]. The Single-Motor-Actuated Robotic Fish has a length of 0.37 m and a speed of 1.14 m/s, and, thus, it travels relatively fast [85].
Table 11.
Thunniform biomimetic robots: experimental research.
Robot | Test Objectives | Test Conclusions | Picture |
---|---|---|---|
Gliding Robotic Dolphin [84] |
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Single-Motor-Actuated Robotic Fish [85] |
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Thunniform Robotic Fish [43] |
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N/A |
Mackerel Robot [88] |
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N/A |
4.2.4. Experimental Studies of Rajiform Robots
As shown in Table 12, Self-Powered Soft Robots achieved good results in physical tests. Relevant experimental researches were not only completed in lakes but also at a depth of 10,900 m in the Mariana Trench, and the robot swam autonomously in the deep sea at 3224 m in the South China Sea. Thus, experiments proved that underwater biomimetic robots can work in the deep sea, a result that has high application value [90]. Experimental tests of the Cartilage Structure Underwater Robot were similarly successful, although only in laboratory tanks, and the cartilage structure showed extremely high undulating propulsion efficiency [95]. The Manta Ray Robot achieved simple pitch and roll motion patterns in the tank, very close to the motion performance of live fish [92]. The swimming speed of IPMC Manta Ray is 0.067 BL/s, and the mobile power consumption is below 2.5 W [91].
Table 12.
Rajiform biomimetic robots: experimental research.
Robot | Test Objectives | Test Conclusions | Picture |
---|---|---|---|
Cartilage Structure Underwater Robot [95] |
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Manta Ray Robot [92] |
|
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Self-Powered Soft Robot [90] |
|
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N/A |
IPMC Manta Ray [91] |
|
|
N/A |
Bionic Fin Manta Ray [93] |
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N/A |
4.2.5. Experimental Studies of Amiiform and Gymnotiform Robots
In the RoboGnilos undulating propulsion experiment, inclined fin rays produced higher speed and efficiency than vertical fin rays. The Bio-inspired Amphibious Robot could realize three-dimensional swimming in the water and could crawl on the ground [99]. Its motion frequency was 0.5 Hz to 2.5 Hz, and the speed and thrust increased with frequency both underwater and on the ground. The Undulatory Fin Propulsion Bio-Inspired Robot was able to perform various swimming movements like a live fish, and the swimming efficiency was studied [103]. Details of experimental studies of amiiform and gymnotiform robots are presented in Table 13 and Table 14.
Table 13.
Amiiform biomimetic robots: experimental research.
Robot | Test Objectives | Test Conclusions | Picture |
---|---|---|---|
RoboGnilos [98] |
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Bio-inspired Amphibious Robot [99] |
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Dorsal Undulation Fin Robot [100] |
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N/A |
Table 14.
Gymnotiform biomimetic robots: experimental research.
Robot | Test Objectives | Test Conclusions | Picture |
---|---|---|---|
Undulatory Fin Propulsion Bio-Inspired Robot [103] |
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Robotic Knifefis [104] |
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N/A |
5. Limitations and Future Perspectives
The use of undulating propulsion for underwater robots plays a significant role in harsh marine environments. Although there have been many achievements, there are still some limitations in terms of motion performance, energy utilization and environmental perception. Firstly, the motion performance and maneuverability of undulating propulsion underwater biomimetic robots still need to be enhanced. Recent studies have mainly been conducted in stable fluid environments and how to deal with the impact of harsh water environments still needs to be supplemented and improved. Secondly, improving the energy utilization of underwater biomimetic robots is required for engineering applications, especially solving the energy consumption problem of long-term motion. Thirdly, how to improve robotic perception is the key to expanding the application of robots. Biomimetic robots usually rely on a few simple sensors to perceive the surrounding environment, but they cannot perceive the surrounding environment in harsh conditions as real fish can. Research on undulating propulsion underwater biomimetic robots is still in its infancy and needs continuous optimization in many aspects.
With the further development of biomimetics and material science, underwater biomimetic robots will achieve breakthroughs. Undulating propulsion underwater biomimetic robots will also have new prospects. These prospects include: (1) Given the complexity of the operating environment and tasks, future underwater biomimetic robots will need to not only possess the ability to swim but also possess other abilities, such as underwater grasping, sampling, transport, etc. (2) Increased biological similarity: underwater biomimetic robots will be closer in shape and movement to biological fish, and the degree of simulation and biological similarity will be continuously improved. (3) Improvement of movement efficiency and operation efficiency: with the improvement in control methods and battery technology, it is believed that future underwater biomimetic robots will have higher movement efficiency and operation efficiency. To sum up, future undulating propulsion underwater biomimetic robots will get closer to the form and function of natural organisms, and their motion performance and operating ability will also be continuously enhanced. At the same time, they will have a wider range of applications, including underwater exploration, underwater rescue, submarine engineering, underwater archaeology and aquarium-based entertainment.
6. Conclusions
Underwater biomimetic robots have strong operability, stability and mobility in the complex marine environment, all of which play a significant role in underwater exploration, rescue, mining, maintenance and scientific research. This paper provides a brief introduction to fish-based biometric propulsion. Existing underwater biomimetic robots are classified and the main achievements in this field are outlined, as well as the characteristics and advantages of each type. The main propulsion mechanisms of current underwater biomimetic robots are presented mainly through the content of experimental studies, emphasizing the importance of experimental studies to the discipline. The limitations and prospects of underwater biomimetic robots are also outlined, demonstrating that, in the future, underwater biomimetic robots will be developed with multiple functionalities and high bio-similarity and operational efficiency.
Author Contributions
Conceptualization, Methodology, Software, Validation, Investigation, Resources, Writing-original draft, G.L. (Gongbo Li); Supervision, Project administration, Funding acquisition, G.L. (Guijie Liu); Writing—review & editing, Supervision, D.L.; Visualization, X.F., G.L. (Guanghao Li) and W.W. All authors have read and agreed to the published version of the manuscript.
Institutional Review Board Statement
Not applicable.
Data Availability Statement
Data available within the article.
Conflicts of Interest
The authors declare no conflict of interest.
Funding Statement
This article was funded by the National Science Foundation of China (No. 61540010).
Footnotes
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