Abstract
Inertial aquatic swimmers that use undulatory gaits range in length L from a few millimetres to 30 metres, across a wide array of biological taxa. Using elementary hydrodynamic arguments, we uncover a unifying mechanistic principle characterizing their locomotion by deriving a scaling relation that links swimming speed U to body kinematics (tail beat amplitude A and frequency ω) and fluid properties (kinematic viscosity ν). This principle can be simply couched as the power law Re ∼ Sw^{α}, where Re = UL/ν ≫ 1 and Sw = ωAL/ν, with α = 4/3 for laminar flows, and α = 1 for turbulent flows. Existing data from over 1,000 measurements on fish, amphibians, larvae, reptiles, mammals and birds, as well as direct numerical simulations are consistent with our scaling. We interpret our results as the consequence of the convergence of aquatic gaits to the performance limits imposed by hydrodynamics.
Main
Aquatic locomotion entails a complex interplay between the body of the swimmer and the induced flow in the environment^{1,2}. It is driven by motor activity and controlled by sensory feedback in organisms ranging from bacteria to blue whales^{3}. Locomotion at low Reynolds numbers (Re = UL/ν ≪ 1) is governed by linear hydrodynamics and is consequently analytically tractable, whereas locomotion at high Reynolds numbers (Re ≫ 1) involves nonlinear inertial flows and is less well understood^{4}. Although this is the regime that most macroscopic creatures larger than a few millimetres inhabit, as shown in Fig. 1a, the variety of sizes, morphologies and gaits makes it difficult to construct a unifying framework across taxa.
Thus, most studies have tried to take a more limited view by quantifying the problem of swimming in specific situations from experimental, theoretical and computational standpoints^{5,6,7}. Beginning more than fifty years ago, experimental studies^{8,9,10,11,12} started to quantify the basic kinematic properties associated with swimming in fish, while providing grist for later theoretical models. Perhaps the earliest and still most comprehensive of these studies was performed by Bainbridge^{8}, who correlated size and frequency f = ω/(2π) of several fish via the empirical linear relation U/L = (3/4)f − 1. However, he did not provide a mechanistic rationale based on fundamental physical principles.
The work of Bainbridge served as an impetus for a variety of theoretical models of swimming. The initial focus was on investigating thrust production associated with body motion at high Reynolds numbers, wherein inertial effects dominates viscous forces^{13,14}. Later models also accounted for the elastic properties of the body and muscle activity^{15,16,17,18}. The recent advent of numerical methods coupled with the availability of fast, cheap computational resources has triggered a new generation of direct numerical simulations to accurately resolve the full threedimensional problem^{19,20,21,22,23,24}. Although these provide detailed descriptions of the forces and flows during swimming, the large computational data sets associated with specific problems obscure the search for a broader perspective.
Inspired by the possibility of an evolutionary convergence of locomotory strategies ultimately limited by hydrodynamics, we bring together the specific and general perspectives associated with swimming using a combination of simple scaling arguments, detailed numerical simulations and a broad comparison with experiments. We start by recalling the basic physical mechanism underlying the inertial motion of a slender swimmer of length L, tail beat frequency ω and amplitude A, moving at speed U (Fig. 1b) in a fluid of viscosity μ and density ρ (kinematic viscosity ν = μ/ρ). At high Reynolds numbers Re = UL/ν ≫ 1, inertial thrust is generated by the bodyinduced fluid acceleration, and balanced by the hydrodynamic resistance. We assume that the oscillation amplitude of motion is relatively small compared to the length of the organism, and that its body is slender. This implies that fluid acceleration can be effectively channelled into longitudinal thrust^{14}. Furthermore, undulatory motions are considered to be in the plane, so that all quantities are characterized per unit depth.
In an incompressible, irrotational and inviscid flow the mass of fluid set into motion by the deforming body scales as ρL^{2} per unit depth^{25}, assuming that the wavelength associated with the undulatory motions scales with the body length L, consistent with experimental and empirical observations. The acceleration of the surrounding fluid scales as Aω^{2} (Fig. 1c) and therefore the reaction force exerted by the fluid on the swimmer scales as ρL^{2}Aω^{2}. As the body makes a local angle with the direction of motion that scales as A/L, this leads to the effective thrust ρω^{2}A^{2}L, as shown in Fig. 1c.
The viscous resistance to motion (skin drag) per unit depth scales as μUL/δ, where δ is the thickness of the boundary layer^{26}. For fast laminar flows the classical Blasius theory shows δ ∼ LRe^{−1/2}, so that the skin drag force due to viscous shear scales as ρ(νL)^{1/2}U^{3/2}, as shown in Fig. 1c. Balancing thrust and skin drag yields the relation U ∼ A^{4/3}ω^{4/3}L^{1/3}ν^{−1/3} which we may rewrite as where Sw = ωAL/ν is the dimensionless swimming number, which can be understood as a transverse Reynolds number characterizing the undulatory motions that drive swimming. This simple scaling relationship links the locomotory input variables that describe the gait of the swimmer A, ω via the swimming number Sw to the locomotory output velocity U via the longitudinal Reynolds number Re.
At very high Reynolds numbers (Re > 10^{3}–10^{4}), the boundary layer around the body becomes turbulent and the pressure drag dominates the skin drag^{26}. The corresponding force scales as ρU^{2}L per unit depth, which when balanced by the thrust yields As most species when swimming at high speeds maintain an approximately constant value of the specific tail beat amplitude A/L (refs 8, 11), relation (2) reduces to U/L ∼ f, providing a mechanistic basis for Bainbridge’s empirical relation.
In Fig. 2a, we plot all data from over 1,000 different measurements compiled from a variety of sources (Supplementary Information) in terms of Re and Sw, for fish (from zebrafish larvae to stingrays and sharks), amphibians (tadpoles), reptiles (alligators), marine birds (penguins) and large mammals (from manatees and dolphins to belugas and blue whales). The organisms varied in size from 0.001 to 30 m, while their propulsion frequency varied from 0.25 to 100 Hz. The dimensionless numbers we use to scale the data provides a natural division of aquatic organisms by size, with fish larvae at the bottom left, followed by small amphibians, fish, birds, reptiles, and large marine mammals at the top right. We see that the data, which span nearly eight orders of magnitude in the Reynolds number, are in agreement with our predictions, and show a natural crossover from the laminar power law (1) to the turbulent power law (2) at a Reynolds number of approximately Re ≃ 3,000. To understand this, we note that the skin friction starts to be dominated by the pressure drag when the thickness of the laminar boundary layer is comparable to half the oscillation amplitude. Therefore, a minimal estimate for the critical Reynolds number Re_{critical} associated with the laminar–turbulent transition is given by the relation δ ≃ A/2. For a flat plate^{26} and given a typical value of A/L = 0.2, we obtain Re_{critical} ≃ (10L/A)^{2} = 2,500, which is in agreement with experimental data.
Naturally, some organisms do not hew exactly to our scaling relationships. Indeed, sirenians (manatees) slightly fall below the line, whereas anuran tadpoles lie slightly above it (Supplementary Information). We ascribe these differences to intermittent modes of locomotion involving a combination of acceleration, steady swimming and coasting that these species often use. Other reasons for the deviations could be related to different gaits in which part or the entire body is used, as in carangiform or anguilliform motion. Moreover, morphological variations associated with the body, tail and fins may play a role by directly affecting the hydrodynamic profile, or indirectly by modifying the gaits. However, the agreement with our minimal scaling arguments suggests that the role of these specifics is secondary, given the variety of shapes and gaits encompassed in our experimental data set.
Because aquatic organisms live in water, testing the dependence of our scaling relationships on viscosity requires manipulating the environment. Although this has been done on occasion^{27} and is consistent with our scaling relations (Supplementary Information), numerical simulations of the Navier–Stokes equations coupled to the motion of a swimming body allow us to test our power laws directly by varying Sw via the viscosity ν only (Supplementary Information). In Fig. 3, we show the results for twodimensional anguilliform swimmers^{28,29}. The data from our numerical experiments straddle both sides of the crossover from the laminar to the turbulent regime and are in quantitative agreement with our minimal scaling theory, and our simple estimate for Re_{critical}. To further challenge our theoretical scaling relationships, in Fig. 3, we plot the results of threedimensional simulations performed by various groups using different numerical techniques^{19,22,24,28}; they also collapse onto the same power laws (details in Supplementary Information). The agreement with both two and threedimensional numerical simulations, which are not affected by environmental and behavioural vagaries, gives us further confidence in our theory.
Traditionally, most studies of locomotion use the Strouhal number St = ωA/U, a variable borrowed from engineering, to characterize the underlying dynamics. Although this is reasonable for many engineering applications such as vortex shedding, vibration and so on, in a biological context it is worth emphasizing that St confounds input A–ω and output U variables, captures only one length scale by assuming A ∼ L, and does not account for varying fluid environments characterized by ν. For biological locomotion, Sw is a more natural variable as it captures the two length scales associated with the tail amplitude and the body size, accounts for the fluid environment, and allows us to seamlessly relate the input kinematics A–ω to the output velocity U. Nevertheless, writing equations (1) and (2) in terms of St yields Sw = Re ⋅ St; therefore St ∼ Re^{−1/4}, for laminar flows, and St = const, for turbulent flows, showing little or no influence of the Reynolds number on the Strouhal number. This direct consequence of our theory is consistent with experimental observations (Fig. 2b) and provides a physical basis for the findings^{30} that most swimming and flying animals operate in a relatively narrow range of St.
Despite the vast phylogenetic spread of inertial swimmers (Supplementary Information), we find that their locomotory dynamics is governed by the elementary hydrodynamical principles embodied in the power law Re ∼ Sw^{α}, with α = 4/3 for laminar regimes and α = 1 for turbulent boundary layers. This scaling relation follows by characterizing the biological diversity of aquatic locomotion in terms of the physical constraints of inertial swimming, a convergent evolutionary strategy for moving through water in macroscopic creatures. Recalling that the phase space Sw–Re relates the input transverse Reynolds number Sw to the output longitudinal Reynolds number Re, our scaling relations might also be interpreted as the edge of optimal steady locomotor performance in this space, separating the inefficient (below) from the unattainable (above) steady regimes in oscillatory aquatic propulsive systems. We anticipate that if general principles for aerial or terrestrial locomotion exist, they may well be found by considering the physical limits dictated by their respective environments.
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Acknowledgements
We thank the Swiss National Science Foundation, and the MacArthur Foundation for partial financial support. We also thank W. van Rees, B. Hejazialhosseini and P. Koumoutsakos of the CSElab at ETH Zurich for their help with the computational aspects of the study, and Margherita Gazzola for her sketches.
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Affiliations
School of Engineering and Applied Sciences, Harvard University, Cambridge, Massachusetts 02138, USA
 Mattia Gazzola
 & L. Mahadevan
Université Nice SophiaAntipolis, Institut non linéaire de Nice, CNRS UMR 7335, 1361 route des lucioles, 06560 Valbonne, France
 Médéric Argentina
Institut Universitaire de France, 103, boulevard SaintMichel, 75005 Paris, France
 Médéric Argentina
Department of Organismic and Evolutionary Biology, Department of Physics, Wyss Institute for Biologically Inspired Engineering, Kavli Institute for Nanobio Science and Technology, Harvard University, Cambridge, Massachusetts 02138, USA
 L. Mahadevan
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Contributions
M.G., M.A. and L.M. conceived the study, developed the theory, collected and analysed the experimental data and wrote the paper. M.G. performed the 2D numerical simulations.
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The authors declare no competing financial interests.
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Correspondence to Mattia Gazzola or L. Mahadevan.
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