How oscillating aerodynamic forces explain the timbre of the hummingbird’s hum and other animals in flapping flight
Birds , bats , and insects flap their wings to generate unsteady aerodynamic forces that lift their body into the air , which enables them to fly . When their flapping wings move through air , they create unsteady pressure fluctuations that radiate outward at the speed of sound . In addition to furnishing flight , pressure waves serve various acoustic communication functions during behavioral displays . Male Drosophila use aerodynamically functional wings to create humming songs near their flapping frequency to increase female receptivity to mating ( von Schilcher , 1976 ) . In a more sophisticated form of courtship behavior , male and female mosquitoes duet at the third harmonic ( multiple ) of their wingbeat frequency ( Cator et al . , 2009 ) . In contrast , pigeons use modified primary feathers that sonate around 1 kHz when they start flapping their wings that incite flock members to fleeing and take-off behavior ( Davis , 1975; Hingee and Magrath , 2009; Niese and Tobalske , 2016; Murray et al . , 2017 ) . Feather sonation during flapping flight may also communicate information like flight speed , location in 3D space , and wingbeat frequency to conspecifics ( Larsson , 2012 ) . Hence , male broad-tailed hummingbirds generate a whistling sound with modified primary feathers in their flapping wings during displays to defend courting territories ( Miller and Inouye , 1983 ) . Silent fliers like owls , on the other hand , suppress the aerodynamic sound generated by their wings to mitigate interference with their hearing and escape prey detection ( Geyer et al . , 2013; Jaworski and Peake , 2020; Kroeger et al . , 1972; Sarradj et al . , 2011; Clark et al . , 2020 ) . Their flapping wings also generate less structural noise ( Clark et al . , 2020 ) because their feathers lack the noisy directional fastening mechanism that locks adjacent flight feathers during wing extension in other bird species ( Matloff et al . , 2020 ) . These diverse adaptations illustrate how a wide range of mechanisms can contribute to the sound that flapping wings generate . Consequently , it is not fully understood how flapping wings generate their characteristic sound—from the mosquito’s buzz , the hummingbird’s hum , to the larger bird’s whoosh . Our physical understanding of how wings generate sound is primarily based on aircraft wing and rotor aeroacoustics ( Brooks and Pope , 1989; Crighton , 1991 ) . In contrast to animals , however , engineered wings do not flap , do not change shape dynamically , are much larger , and operate at much higher speeds ( higher Reynolds numbers ) . They also operate at lower angles of attack to avoid stall , which results in more compact airflow patterns than animals generate in flapping flight ( Ellington et al . , 1996; Dickinson et al . , 1999; Mueller , 2001 ) . Despite these marked differences , rotors and flapping wings have one thing in common: they both revolve around a center pivot . Whereas flapping wings reciprocate along the joint , rotors revolve unidirectionally . The revolution of rotors generates loud tonal noise , because the pressure field they generate rotates in space at the same frequency ( Lighthill , 1954; Lowson , 1965 ) . Similarly , when animals flap their wing back and forth along the shoulder joint during each stroke , they create a high-pressure region below their wing and a low-pressure region above . The pressure differences are associated with the wing’s high lift and drag , respectively ( Sane and Dickinson , 2001; Wu and Sun , 2004 ) . Computational fluid dynamics ( CFD ) simulations of flapping insect wings suggest that the acoustic field can be characterized as a dipole at the wingbeat frequency ( Bae and Moon , 2008; Geng et al . , 2017; Seo et al . , 2019 ) . Further , flapping wing pitch reduction ( Nedunchezian et al . , 2018 ) and increased wing flexibility ( Nedunchezian et al . , 2019 ) reduces the simulated nearfield sound pressure level . All these findings point to the potential role of oscillating aerodynamic forces in generating wing hum . Indeed , numerical simulation of the Ffowcs Williams and Hawkings aeroacoustic equation ( Williams and Hawkings , 1969 ) showed that the farfield hum of flapping mosquito wings is primarily driven by aerodynamic force fluctuation ( Seo et al . , 2019 ) . Despite these important advances , in vivo acoustic near-field measurements are lacking . Finally , there is no simple model that can satisfactorily integrate flapping wing kinematics and aerodynamic forces to predict the acoustic near and far field generated by animals across taxa without using computationally expensive fluid dynamic simulations . Hummingbirds are an ideal subject for developing and testing a model of flapping wing hum: their wing kinematics and unsteady aerodynamic forces are very repeatable during hover ( Altshuler and Dudley , 2003; Tobalske et al . , 2007; Ingersoll and Lentink , 2018 ) . Further , hummingbird wing morphology and flight style share similarities with both birds and insects . In addition to high-frequency feather sonations , hummingbirds produce a prominent hum that is qualitatively similar to an insect’s buzz . Earlier aeroacoustics studies of hummingbirds have resolved the farfield acoustic pressure field at a distance greater than 10 or more body lengths away from the hummingbird ( Clark and Mistick , 2018a; Clark , 2008; Clark et al . , 2016; Clark and Mistick , 2018b ) . While this distance relates to how humans perceive and interact with these animals , hummingbirds frequently interact with conspecifics and other animals at more intimate distances—in the acoustic nearfield . Furthermore , wing hum can announce a hummingbird's presence , especially to the opposite sex ( Hunter , 2008 ) . Although their audiogram has yet to be established below 1 kHz ( Pytte et al . , 2004 ) , this and other behavioral evidence suggests hummingbirds may be able to perceive the wing hum from a conspecific . Finally , the hum may reveal the hummingbird’s presence to predators in plant clutter when vision is obstructed . To resolve how the oscillating aerodynamic force generated by flapping wings may contribute to wing hum , we developed a new aerodynamic force platform ( Ingersoll and Lentink , 2018; Lentink et al . , 2015; Hightower et al . , 2017 ) to directly measure the net 3D aerodynamic force generated by freely hovering hummingbirds . We integrated this data in a new aeroacoustics model to predict the sound radiated due to the oscillating forces from flapping wings . Our model is idealized in the sense that it assumes the wings are rigid airfoils , thereby neglecting auxiliary effects such as wingtip flutter , feather whistle and ( turbulent ) vortex dynamics . Next , we compared the predicted acoustic field with novel acoustic nearfield recordings for six freely hovering hummingbirds , which corroborates the predictive power of our minimal model . We then used our validated model to determine how flapping wing hum depends on the frequency content in the oscillating forces across mosquitos , flies , hawkmoths , hummingbirds , and parrotlets in slow hovering flight . Finally , we used these findings to determine how the hum scales with body mass and flapping frequency across 170 insect and bird species .
To determine how the flapping wings of hovering hummingbirds generate unsteady aerodynamic forces as well as their namesake acoustic humming signature , we combine aerodynamic force platform ( Figure 1A ) and microphone array recordings ( Figure 1D ) in vivo . The aerodynamic force platform integrates both the steady and unsteady components of the pressure field around the bird up to three times the wingbeat frequency , which are associated with its net 3D aerodynamic forces . In contrast , the microphone arrays measure the unsteady component of the pressure field around the bird up to ~1000 times the wingbeat frequency ( of which we studied the first ten harmonics ) : the acoustic field . Critically , these two representations of the pressure fluctuations generated by the bird should relate mechanistically if the acoustic field of the hummingbird’s hum originates primarily from the oscillating aerodynamic lift and drag forces generated by the flapping wings . The oscillating 3D aerodynamic forces were recorded simultaneously with the wingbeat kinematics using three calibrated stereo high-speed camera pairs ( Figure 1A; N = 6 birds , n = 2 flights per bird , n = 5 wingbeats per flight: 60 total wingbeats ) . We combined the 3D aerodynamic forces , 3D wing kinematics and wing morphology measurements to decompose the oscillating lift and drag forces that each wing generates throughout the wingbeat ( Figure 1B , C ) . The oscillating lift trace consists primarily of the peak force generated during downstroke , which corresponds to a peak in its spectrum at the first wingbeat harmonic ( 44 . 2 ± 1 . 8 Hz ) . The drag trace consists of two equivalent drag peaks during the upstroke and downstroke , which corresponds to a dominant peak in its spectrum at the second harmonic . We also measured the 3D beak contact force on the artificial flower from which the hummingbird was feeding , which is negligible ( 5 . 2 ± 2 . 3% bodyweight ) . The 3D acoustic field associated with the bird’s hum was quantitatively reconstructed from measurements recorded in a custom flight arena using four acoustic arrays ( Figure 1D; N = 6 birds , n = 18 flights total , see Supplementary file 1 for details ) . The recording by a single microphone centered above the bird shows a typical pressure trace throughout a single wingbeat ( Figure 1E ) . The many fluctuations explain the rich frequency content revealed in the acoustic spectrum averaged over all microphones ( Figure 1F ) . These include strong peaks at the fundamental frequencies of the wingbeat as well as its higher harmonics , which rise prominently above the background noise floor and characterize the hummingbird hum . To determine if the low frequency oscillating forces generated by the birds’ flapping wings drive the characteristic humming sound spectrum , we develop a simple aeroacoustics model based on the governing acoustics equations that predict the resulting acoustic field . Our minimal model of the acoustic pressure field radiated by the flapping wings ( Figure 1G ) depends only on the physical properties of air , the wing stroke kinematics ( Figure 1H ) , and the oscillating lift and drag forces that we measured in vivo ( Figure 1B ) . Aerodynamic analysis of propellers shows how a radial force distribution can be integrated and represented by the net force at the center of pressure , a characteristic radial location where the net force acts ( Weis-Fogh , 1973 ) . Analogously , we determine that the acoustic sound radiation of an unsteady aerodynamic force distribution over the wing can also be concentrated into an equivalent point force at the effective acoustic source location along the wing , similar to propeller noise theory ( Lowson , 1965 ) . The effective radius of this point , measured with respect to the shoulder joint , is equal to the point at which the net drag force results in the same net torque on the wing ( Lowson , 1965 ) . This radius lies at the wing-length-normalized third moment of area for flapping wings , R3/R ( Weis-Fogh , 1973 ) . For Anna’s hummingbirds R3/R is equal to 55% wing radius ( Kruyt et al . , 2014 ) . In practice , the effective radius for acoustic calculations can differ somewhat from the effective radius for a point force ( Lowson , 1965 ) . Therefore , we conduct a dimensional analysis to determine how acoustic pressure scales with radial position ( see Supplementary Information for details ) , which confirms R3 is the appropriate radius . This acoustic radius agrees with wind turbine acoustics measurements at lower harmonics of the blade passing frequency ( Oerlemans et al . , 2001 ) . Starting at the time and location where the acoustic wave was generated by the unsteady force on the left and right wing , we numerically solve how the acoustic wave propagates outward into space to the location where we observe it with a microphone . Mathematically , the acoustic equation describes how the unsteady aerodynamic point force , Fwing , generated by the flapping wing generates an air pressure fluctuation , p , in the stationary atmosphere at the so-called ‘retarded time’ , t , which radiates outward as a wave at the speed of sound , ao , as follows Lowson , 1965: ( 1 ) p=[14π|r|2 ( 1−Mr ) 2 ( 1|r| ( 1−M2 ) ( 1−Mr ) ( r⋅Fwing ) − ( Fwing⋅M ) ) ]⏟nearfield+[14πao|r|2 ( 1−Mr ) 2 ( ( r⋅∂Fwing∂t ) +11−Mr∂Mr∂t ( r⋅Fwing ) ) ]⏟farfield . The brackets indicate that the propagating pressure values , p , are evaluated at the retarded time , t . The vectorial distance from the moving point source on the flapping wing to the stationary microphone is measured by the vector , r , in a Cartesian reference frame fixed to earth . The wing’s velocity at the radial position where the point force acts , vR3 , is nondimensionalized with the acoustic wave velocity , ao , the speed of sound , which defines in the Mach vector M=defvR3/ao . The Mach number is simply the magnitude of the Mach vector M=def|M| . Similarly , the convective Mach number , Mr=defM⋅r/|r| , is simply the component of the Mach vector , M , along the vector , r , that runs from the wing source to the microphone . The acoustic pressure fluctuation , p , consists out of two components of which the respective strengths depend on how far the microphone is located away from the wing—measured in wavelengths of the acoustic frequency of interest ( Howe , 2014 ) . For a flapping hummingbird wing we choose the wingbeat frequency , because it is associated with the first harmonic we observe in the humming spectrum ( Figure 1F ) , λ1=a0/f1≈343/44 . 2=7 . 8 m . The first term in Equation 1 dominates in the nearfield close to the wing up to a wavelength away from it . The associated pressure wave has a 3D dipole shape radiating in two opposing directions . Its strength is proportional to the force vector reorientation in space with respect to the radial vector , r , pointing from the source to the microphone . The second term dominates in the farfield starting at a wavelength away from the wing . The associated pressure wave has a 3D quadrupole shape along four primary directions . Its strength is proportional to the point force unsteadiness and the radial acceleration of its position in space . In the case of a hummingbird , the nearfield term decays exponentially with distance . This is because the hummingbird acts as a compact acoustic source ( Rienstra and Hirschberg , 2004 ) , since the wavelength at the wingbeat frequency ( first harmonic ) is much larger than the radius of the wing , R , the representative acoustic source length scale: R/λ1=0 . 007 for R=0 . 058±0 . 003 m . Consequently , a hummingbird wing acts as an approximate compact acoustic source up to its tenth wingbeat harmonic ( 10⋅f1 ) with wavelength λ10=a0/f10≈343/442=0 . 78 m . Because the hummingbird wing is acoustically compact across all the humming frequencies we study here , the wing is effectively acoustically transparent . The sound scattering over the wing is negligible and the time differences between local sound generating sources distributed over the wing can be ignored . Indeed , we observe a median difference of 0 . 1 dB between a single source model and a distributed model with 10 sources ( Figure 2—figure supplement 1A , Supplementary file 2 ) . The associated acoustic holograms of both models match spatially ( Figure 2—figure supplement 1B ) , confirming hummingbird wings are compact acoustic sources at humming frequencies . Using Equation 1 , we calculate the resulting pressure fluctuation at each of the 2176 microphones in our acoustic arena to directly compare the simulated and measured humming sound up to the tenth harmonic . Beyond the tenth harmonic the ambient noise floor of the experiment is approached ( Figures 1F and 2A ) . Since the in vivo flapping frequency is used as an input to our model , Equation 1 , there is exact frequency agreement between the modeled and in vivo spectra ( Figure 2A ) . Spatially , the model captures the wingstroke transitions in the top and front arrays in the holograms ( Figure 2B ) . The model and recordings are in good agreement , because the difference in the magnitude of the sound pressure is ~4 dB or less for the first four harmonics ( maximum difference between the model and the measurement ±1 SD; Figure 2A , Table 1 ) . The first four harmonics represent most of the radiated harmonic power: ~99% of the simulated power and ~67% of the measured power for ±2 . 5 Hz bands around each wingbeat harmonic up to 180 Hz . The percentage difference is due to at least three factors: ( i ) harmonics beyond the fourth contribute more power in the measured spectrum than in the simulated spectrum ( Table 2 ) , ( ii ) the experiment's ambient noise floor is substantially higher than the computational noise floor ( Figure 1F ) , and ( iii ) some low amplitude tonal noise sources observed between harmonics cannot be attributed to humming ( Figure 2A ) . The differences across all 10 harmonics may include some acoustic scattering by the wing and body , possible wingtip flutter ( Sane and Jacobson , 2006 ) and turbulent vortex dynamics contributions occurring multiple times during a wingbeat , so they overlap with the measured harmonics . The magnitude of these effects combined is bounded by the differences in the measured and simulated spectra ( Figure 2A ) , which ranges from ~0 . 5 to ~7 . 0 dB ( min . and max . difference ±1 SD; Table 1 ) . The directivity of the acoustic pressure field varies between harmonics . Odd harmonics are associated with a rotational pressure fluctuation mode while even harmonics are associated with a vertical pressure fluctuation mode . To assess the near and farfield directivity , we reconstruct 3D broadband pressure fields ( across 3–500 Hz ) over an entire wingbeat during stationary hovering flight . The reconstructed pressure fields start out at a radius of 8 cm centered on the body such that the inner spherical surface encloses the hummingbird ( the wing radius with respect to the body center is 5 . 8 ± 0 . 3 cm ) and the outer spherical surface ends at a radius of 10 m ( Figure 3A; animation in Video 1 ) . To evaluate acoustic pressure directivity in the nearfield ( 1 m distance , ~8 . 6 wingspans , Figure 3B ) and farfield ( 10 m distance , ~86 wingspans , Figure 3C ) , we calculate the cross-sections of the pressure field in the sagittal ( side ) and coronal ( frontal ) anatomical planes . Averaging directivity plots across all birds and flights , we find the 3D broadband pressure surface is roughly spherical in the nearfield and farfield ( plotted in the middle of Figure 3B , C in black ) . To observe the contribution from each harmonic , we decompose the broadband pressure with a bandwidth of ±2 . 5 Hz around each of the first four harmonics ( Figure 3D–K ) . Each individual directivity plots’ principal axis is oriented perpendicular to the waistline of the dipole lobes we measured ( average , gray line; ±1 standard deviation , light gray arc ) and simulated ( comparison in Table 2 ) . The principal axis is mostly vertical because the net aerodynamic force generated during hover opposes gravity . The dipole shape also manifests in the ovoid 3D pressure surface at these harmonics ( Figure 3D–K ) . The orientation of the measured and predicted broadband holograms in the sagittal and coronal plane agrees within one standard deviation or less ( Figure 3B , C; Table 2 ) . This is explained by the reasonable correspondence between the measured and predicted directivity ( Figure 3D–G ) and amplitude ( Figure 2A ) of the first and second harmonic , which have the largest amplitudes across all harmonics . Both the near and farfield broadband directivity plots are pointed aft in the sagittal plane because the dominant first harmonic is oriented aft . The correspondence between the predicted and measured amplitude ( Table 1 ) and directivity in the sagittal ( but not coronal ) plane ( Table 2 ) weakens starting at the fourth and third harmonic respectively . Higher harmonics contribute less to the broadband directivity , because their amplitude is much lower ( <48 dB beyond the third harmonic , Table 1 ) . Due to the symmetry between the left and right wing , the coronal directivity points upwards at 90° across all measured and simulated harmonics ( Figure 3 , Table 2 ) , showing the hummingbirds performed symmetric hovering flight . In summary , the first harmonic of the hummingbird hum is formed by an acoustic dipole , tilted aft in the coronal plane , which corresponds to the fluctuation of the net vertical and asymmetric horizontal force over a wingbeat . The associated rotational mode can be observed in the time-dependent 3D hologram ( Video 2 ) . The second harmonic is formed by an upward pointing dipole , corresponding to the vertical force generation that occurs twice per wingbeat ( Figure 3F , G ) . This is visible as a vertically oriented mode in the time-dependent 3D hologram ( Video 3 ) . The third harmonic consists also of a rotational mode like the first harmonic ( Figure 3H , I ) , as seen in the time-dependent 3D hologram ( Video 4 ) . Likewise , the fourth harmonic consists of a vertical mode like the second harmonic ( Figure 3J , K; Video 5 ) . Using our model , we predict the acoustic sound generated by flapping wings for a wide range of insects and birds that hover or perform slow flapping flight during takeoff and landing across seven orders of magnitude in body mass , m , and three orders of magnitude in wing flapping frequency , fw . We generalize the flapping animals we consider here into five distinct groups for which we found data: generalist birds ( Aves except Trochilidae ) , hummingbirds ( Trochilidae ) , moths and butterflies ( Lepidoptera ) , compact flies ( Cyclorrhapha ) , and elongated flies ( Nematocera ) , which fly with marked shallower stroke amplitudes than compact flies . Since 3D aerodynamic force and wing kinematics data are not available for all these species , and most of the radiated acoustic sound is directed vertically ( Figure 3B–K ) , we simplified the model . We chose a well-studied animal for which a wingbeat-resolved vertically-oriented force component has been reported previously to act as a paradigm for each group . Respectively , the vertical force of pacific parrotlets ( Forpus coelestis Chin and Lentink , 2017 ) for generalist birds , the vertical force of Anna’s hummingbird ( Calypte anna; Ingersoll and Lentink , 2018 ) for hummingbirds , the lift force of hawkmoths ( Manduca sexta Zheng et al . , 2013 ) for moths and butterflies , the lift force of mosquitos ( Culex quinquefasciatus; Bomphrey et al . , 2017 ) for elongated flies and the net force of Drosophilid flies ( Drosophila hydei; Muijres et al . , 2014 ) for compact flies ( Supplementary file 5 ) . To simplify the comparison further , we approximate the stroke plane as horizontal and the normalized lift profile to have the same shape as the reported vertically oriented force profile , so that the lift generated during a wingbeat sums up to body weight for all associated species in the same way . To calculate the associated drag profile , we used previously reported quasi-steady lift/drag ratio data for Anna’s hummingbirds ( Ingersoll and Lentink , 2018; Kruyt et al . , 2014 ) and assume it is representative for all animals . Finally , to compute the acoustic field for each animal’s wing , we locate the lift and drag force at the third moment of area of a hummingbird wing , 55% of the wing radius ( which compares to 58% for parrotlets Chin and Lentink , 2017 ) . In our comparison , we make the exact same approximations for hummingbirds as we do for the other animals . Despite these assumptions , the simplified model matches the original model for a hummingbird well ( Figure 2—figure supplement 2 , Supplementary file 3 ) . Between each of the four groups , the instantaneous weight support , stroke amplitude , and frequency content throughout the wingbeat change based on the associated paradigm animal ( Figure 4A , B ) . In contrast , the mass , wingspan , and flapping frequency change across all individual animals in each group . Calculating the ratio of the wing length versus acoustic wavelength at the wingbeat frequency across all species , we find Rfw/ao=R/λ1≲0 . 01 ( Figure 4—figure supplement 1 ) . Indeed , synchronized acoustic and video recordings show that the measured first acoustic harmonic overlaps with the wingbeat frequency across insects ( Cator et al . , 2009; Aldersley and Cator , 2019 ) and hummingbirds ( Figure 1 ) as well as other birds and bats ( Boonman et al . , 2020 ) . Thus , similar to the hummingbird , the flapping wings of all these animals act as compact acoustic sources from the first to tenth harmonic . Furthermore , because wing length is inversely proportional to flapping frequency ( Greenewalt , 1962 ) , the assumption of acoustic compactness holds across species . Consequently , the humming sound generated across flapping animal wings can be modeled accurately with a single point force source per wing half , similar to what we found for hummingbirds ( Figure 2—figure supplement 1 ) . This even holds for mosquito buzz , the most extreme case among our five paradigm animals , because the mosquito wing’s compactness , R/λ1=0 . 006 , is equivalent to that of a hummingbird’s 0 . 007 . The weight support profiles of each of the five paradigm animals has distinct harmonic content ( Figure 4B ) . To understand how this drives acoustic power and timbre , we use our acoustic model to assign each of the five paradigm animals all five weight support profiles . For example , we variously assign the weight support profile of a mosquito , fly , hawkmoth , hummingbird , and parrotlet to our hummingbird model . This allows us to investigate the weight support profile’s effects on differences in radiated acoustic power ( Figure 4C ) and the acoustic spectrum ( Figure 4D ) . The weight support profiles of the mosquito and fly consistently generate more acoustic power and sound pressure than the other weight support profiles . Lastly , we extend the acoustic model from the five paradigm animals to 170 animals across the five groups . Body mass and flapping frequency for hummingbirds , compact flies , elongated flies , and moths and butterflies were obtained from Greenewalt , 1962 , while the values for larger birds were obtained from Pennycuick , 1990; Figure 4E , F . Comparing the model simulation results with the isometric scaling relation we derived based on the model ( Equations A25–50 ) shows that radiated acoustic power scales allometrically with body mass ( Figure 4E ) except for compact flies and moths and butterflies , which scale isometrically . Considering flapping wing parameters are known to scale allometrically with body mass , we test the scaling law itself ( Figure 4F ) , which collapses the data well on average across species ( average slope = 0 . 9; ideal slope = 1 ) , confirming the scaling law represents our model .
Our idealized aeroacoustic model shows the hummingbird’s hum originates from the oscillating lift and drag forces generated by their flapping wings . Remarkably , the low frequency content in the aerodynamic forces also drives higher frequency harmonics in the acoustic spectrum of the wing hum . The higher harmonics originate from nonlinear frequency mixing in the aeroacoustic pressure equation between the frequency content in the wing’s aerodynamic forces and kinematics . The predicted humming harmonics of the wingbeat frequency overlap with the measured acoustic spectrum ( averaged over all microphones ) . In addition to the good frequency match , the sound pressure level magnitudes of the first four harmonics match with a difference of 0 . 5–6 . 0 dB ( Table 1 ) . This agreement is similar or better compared to more detailed aeroacoustic models of drone and wind turbine rotors , that predict noise due to blade-wake interactions and boundary layer turbulence ( Oerlemans and Schepers , 2009; Zhang et al . , 2018; Wang et al . , 2019 ) . Further , comparing the measured and predicted spatial acoustic-pressure holograms for the top and front arrays ( reconstructed holograms at a plane 8 cm from the bird; Figure 2B ) , we find that the hologram phase , shape , and magnitude correspond throughout the stroke . The regions of high and low pressure in the hologram are associated with wing stroke reversals , similar to the pressure extrema observed at stroke reversal in computational fluid dynamics simulations of flapping insect wings ( Geng et al . , 2017; Seo et al . , 2019; Nedunchezian et al . , 2018 ) . Even though the input forces were lowpass filtered beyond the fourth harmonic , the amplitudes of higher harmonics are predicted . This is due to two distinct stages of nonlinear frequency mixing in our wing hum model: ( i ) the calculation of the resulting aerodynamic force vector generated by each flapping wing and its oscillatory trajectory in space , and ( ii ) the calculation of the resulting acoustic pressure waves ( see Supplementary Information for details ) . Our acoustic model predicts hum harmonics that lie in an intermediate frequency range between the wingbeat frequency ( ~40 Hz ) and the lower bound of feather sonations ( typically >300 Hz; Clark et al . , 2013a; Clark et al . , 2013b ) . Hence our model allows for an objective contrast between wing hum sound and other possible aerodynamic noise generation mechanisms . Indeed , we observe small tonal peaks between the prominent harmonics in Figure 2A that are not radiated by the oscillating aerodynamic forces generated by the flapping wing , according to our hum model . Consequently , these low amplitude peaks must radiate from another acoustic source such as aeroelastic feather flutter ( Clark et al . , 2011 ) or vortex dynamics ( Ellington et al . , 1996 ) . In the under-studied frequency regime of the hum , the first two harmonics are paired as they have similar sound pressure levels ( Figure 2A ) . For the hummingbird , the pairing of the first and second harmonics is due to the dominance of the pressure differential generated twice per wingbeat during the downstroke and upstroke . The associated substantial weight support during the upstroke ( Figure 1B; Ingersoll and Lentink , 2018 ) has been found across hummingbird species ( Ingersoll et al . , 2018 ) , which generalizes our findings . The sound pressure level pairing also mirrors the harmonic content in the lift and drag forces ( Figure 1C ) as well as the stroke and deviation kinematics ( Figure 1I ) . Given that the first and second harmonics dominate both the forces and kinematics spectra , the harmonic content of the resulting acoustics is a mixture of these two . The third harmonic and beyond resemble the first paired harmonic because they are associated with the noise generation mechanisms of the first two harmonics ( Rienstra and Hirschberg , 2004 ) . In concert , the first four harmonics constitute most of the acoustic radiated power of the hum timbre—the distinct sound quality that differentiates sounds from distinct types of sources even at the same pitch and volume—which is determined by the number and relative prominence of the higher harmonics present in a continuous acoustic wave ( Sethares , 2005 ) . Acoustic directivity is consistent from near to farfield , but changes based on the harmonic . In the 3D holograms , the dipole structures are associated with the high vertical forces to offset weight ( Ingersoll and Lentink , 2018 ) . These dipole orientations are not evident in the broadband holograms ( Figure 3B , C ) because slight variations between the flights are averaged and smear out the dominant dipole lobes ( individual flights for each directivity plot shown in Figure 3—figure supplement 1 ) . The first and third harmonics resemble dipoles that are tilted aft . For example , for the first harmonic in the sagittal plane in both the nearfield and farfield , the dipole is tilted aft ( Figure 3D , E; Table 2 ) , which is associated with the pressure generated during the downstroke once per wingbeat . In contrast , second and fourth harmonics are more vertically oriented . The second harmonic is directed upwards in the nearfield and farfield ( Figure 3F , G; Table 2 ) and is associated with the pressure generation for the vertical weight support that occurs twice per wingbeat . The third and fourth harmonics have more complex shapes ( Figure 3H–K ) that bear resemblances to the first two because they are associated with the first two harmonics ( Rienstra and Hirschberg , 2004 ) . The acoustic model also shows these directionality effects over the first two harmonics in the sagittal and coronal near and farfield . In contrast , the simulation has more symmetry between the upstroke and downstroke , resulting in a symmetric and better-defined dipole structure . The dipoles that we measured for the first four hummingbird harmonics ( Figure 3D–K ) are strikingly similar to the ones found for hovering insects in computational fluid dynamics simulations ( Geng et al . , 2017; Seo et al . , 2019 ) . Although the mosquito dipoles are oriented more horizontally , because their wings generate unusually high drag at these harmonics ( Seo et al . , 2019 ) , due to their particularly shallow wingstroke ( Bomphrey et al . , 2017 ) . The sound magnitude that flapping wings produce depends heavily on the weight the flapping wings must support , and the timbre depends on the unique frequency content of each weight support profile ( Figure 4B ) . Flies and mosquitos are orders of magnitude lighter than our three other paradigm animals and produce less acoustic power accordingly ( Figure 4C ) . Yet the fly and mosquito weight support profiles have the highest harmonic content ( Figure 4B ) and therefore , when all else is equal , consistently radiate the most power ( Figure 4C ) . In contrast , the parrotlet weight support profile has the lowest harmonic content ( Figure 4B ) ; with most of the force being generated once per wingbeat during the downstroke , hence it radiates the least power when all else is equal ( Figure 4C ) . For hummingbirds and hawkmoths , the proportion of weight support in upstroke versus downstroke is similar ( Geng et al . , 2017; Ingersoll and Lentink , 2018 ) ; this gives them roughly similar vertical force profiles and leads to similar acoustic power ( Figure 4C ) . The effect of altering the weight support profile is also visible in the acoustic spectrum . At the scale of a hummingbird ( Figure 4C , inset ) , the prescribed weight support profiles distinguish the distribution of the overall decibel level for the first four harmonics ( Figure 4D ) . This explains why flies and mosquitos may seem loud relative to their small size: while they have little mass , it is partially offset by the high harmonics in their weight support profiles . Furthermore , it is the higher harmonics present in the weight support profile that directly affect the perceived quality of the sound—the timbre . Body mass is a strong predictor of radiated acoustic power because the aerodynamic forces needed to sustain slow hovering flight must be proportionally larger for heavier animals ( Weis-Fogh , 1973; Altshuler et al . , 2010; Skandalis et al . , 2017 ) . The associated increase in aerodynamic force amplitude drives acoustic pressure ( Equation 1 ) . The resulting radiated acoustic power , P , scales with the square of the acoustic pressure , p ( Equation A25 ) . Increasing flapping frequency also increases the radiated acoustic power; flapping faster requires more power from the animal and injects more acoustic energy into the air . Applying scaling analysis to Equation 1 ( derived in Supplementary Information; Equations A25–50 ) , we can predict the order of magnitude of the radiated acoustic power in the farfield ( Howe , 2014 ) : ( 2 ) Po=4Fo2Φo2fw2πρoao3≈2 . 5⋅10−6Φo2m2fw2 , where the subscript 'o' corresponds to the reference value and F0=mg is the aerodynamic force magnitude required to maintain hover . The resulting acoustic power law scales with the product of wing stroke amplitude , Φo , body mass , m , and wingbeat frequency , fw , squared . Further , since Φo is dimensionless , it has order of magnitude one , measured in radians , across flapping birds ( Nudds et al . , 2004 ) and insects ( Azuma , 2006 ) . The remaining terms , 4/π , the gravitational constant g=9 . 81ms−2 , the air density ρo≈1 . 23kgm−3 , and speed of sound in air , ao≈343ms−1 are constants that determine the factor 2 . 5×10−6 kg−1s−1 between the radiated acoustic power and its scaling variables . When acoustic power is plotted as a function of mass ( Figure 4E ) , the predicted exponent of 2 . 0 is higher than the observed average exponent of 1 . 3 . Among the five groups , compact flies and moths and butterflies do match the scaling law prediction , showing their acoustic power scales isometrically with body mass . The other groups scale allometrically with either higher , elongated flies , or lower , hummingbirds and other birds , exponents of body mass . Allometric divergence can more readily explain why larger hummingbirds are quieter , because they have disproportionally larger wings combined with an approximately constant wing velocity across an order of magnitude variation in body mass , which is thought to maintain constant burst flight capacity ( Skandalis et al . , 2017 ) . Conversely , for insects , the gracile bodies and larger wings of moths and butterflies are offset by the higher flapping frequency of compact flies . Therefore , flies use asynchronous flight muscles to achieve these high flapping frequencies ( Deakin , 1970 ) . Large , elongated flies are unusually noisy for their body mass , with radiated acoustic power values well above the average scaling law ( Figure 4E ) . The disproportional noise generated by elongated flies is due to two combined effects: the higher harmonic content of their weight support profile ( Figure 4A , B ) and their consistent allometric acoustic power scaling ( Figure 4E ) . The difference between the scaling exponents for mass is primarily due to allometric scaling of wingbeat frequency with body mass because the simulated acoustic power scales with the right-hand side of scaling Equation 2 with an exponent of 0 . 9 ( on average ) , close to 1 ( Figure 4F ) . Scaling Equation 2 is precise for birds , compact flies , and moths and butterflies , but the two other groups scale allometrically: larger birds get more silent ( slope = 0 . 9 ) while elongated flies ( 1 . 1 ) get louder than predicted by isometric scaling incorporating the allometric body mass and wing frequency relationship . The deviation may be partially explained by variation in wing stroke amplitude ( Bomphrey et al . , 2017; Nudds et al . , 2004; Azuma , 2006 ) . Further , body size and wingspan in insects are highly variable amongst individuals of even the same species ( Debat et al . , 2003 ) , which may explain the larger variation . Finally , the assumptions underpinning our scaling analysis may explain some deviation . The extension of our simple model to predict flapping wing hum across a wide range of species ( Figure 4 ) makes it a useful tool to study insects , birds , and bats performing a variety of complex behaviors . Like the acoustic power scaling law ( Equation 2 ) , Equation 1 can be simplified further ( Figure 4—figure supplements 1 , 2 ) for comparative biomechanical and neuroethological studies: ( 3 ) p=14π|r|3 ( r⋅Fwing ) ⏟nearfield+14πao|r|2 ( r⋅∂Fwing∂t+4ΦoRfw2ao ( r⋅Fwing ) ) ⏟farfield . Our study shows how this model can elucidate the mechanistic origin of wing hum timbre ( and modulation ) in vivo by integrating acoustic recordings with high-speed videography and aerodynamic force recordings . Likewise , we showed it can be used to make predictions or interpret acoustic measurements by integrating a simplified wing kinematics and aerodynamic force model . It can also be used to estimate the auditory detection distance of wing hum by combining it with an audiogram . Finally , the ability to distinguish between the nearfield versus farfield provides an additional lens for behavioral inquiry . The predicted range over which wing hum can be perceived is even larger in rock pigeons; approximately four meters or ~12 wing radii ( Columba livia: flapping frequency 7 Hz , mass 400 g , wing length 32 cm; Pennycuick , 1968 ) . The perception distance scales up with body mass ( Figure 4E ) and the auditory threshold of pigeons is exquisitely sensitive to the wingbeat frequency ( Kreithen and Quine , 1979 ) , which can thus potentially inform flocking behavior ( Larsson , 2012 ) . Conversely , while the low-frequency oscillating aerodynamic forces also radiate high-frequency humming harmonics up to the tenth wingbeat harmonic ( Figure 2A , Table 1 ) and beyond , the corresponding decibel amplitudes are insignificant compared to harmonics close to the wingbeat frequency ( Figure 1F ) . This helps explain why some birds rely on specialized flight feathers that sonate loudly at high frequency to signal over longer distances how they are flapping their wings during flock takeoff ( Hingee and Magrath , 2009; Niese and Tobalske , 2016; Murray et al . , 2017 ) , mating displays ( Clark et al . , 2016 ) and displays to defend courting territories ( Miller and Inouye , 1983 ) . Perception of wing whoosh also has implications for bird-insect predation , because moths have been shown to respond to the wingbeat hum of birds in playback experiments ( Fournier et al . , 2013 ) . Finally , an acoustic model analogous to the one we present here has recently been used to simulate mosquito buzz ( Seo et al . , 2019 ) in conjunction with computational fluid dynamics to predict how aerodynamic forces ( Bomphrey et al . , 2017 ) color the mosquito’s aerial courtship song ( Cator et al . , 2009 ) . Intriguingly , whereas mosquitos fly with a shallow wing stroke to generate high harmonic content , fruit flies do not ( Bomphrey et al . , 2017 ) . When fruit flies use their wing as an aeroacoustic instrument during terrestrial courtship serenades; however , they reduce their stroke amplitude to a similar degree ( von Schilcher , 1976; Bennet-Clark and Ewing , 1968 ) , which likely colors their timbre as in mosquitos ( Figure 4A–D ) . Our acoustic model explains how the oscillating lift and drag forces generated by each wing of a hovering hummingbird radiate the distinctive humming timbre . It integrates in vivo 3D aerodynamic force and wing kinematics measurements and is corroborated spatially and temporally through in vivo nearfield acoustic holography . The measurements and model show that hovering hummingbirds generate a highly directional hum . The broadband acoustic pressure is primarily oriented downward opposing gravity , while the acoustic directivity and orientation of the harmonic components depend on harmonic parity . The model explains how perceived differences in hum loudness and timbre across birds and insects stem primarily from the harmonic content in the aerodynamic weight support profile . Higher harmonic content throughout the wing stroke makes flies and mosquitos buzz , equivalent first and second harmonic content makes hummingbirds hum , while dominant first harmonic content gives birds their softer whoosh . The associated scaling relation for radiated acoustic power shows how it is proportional to the product of stroke amplitude , body mass and wingbeat frequency squared . Our scaling analysis across 170 different animals in slow hovering flight reveals how the radiated acoustic power scaled with mass . Allometric deviation explains why larger birds radiate less acoustic power than expected and why elongated flies have a remarkably loud buzz as perceived by a casual observer . Finally , our acoustic model and scaling equation can help neuroethologists and bioacousticians interpret the loudness and timbre of the hum generated by flapping winged animals performing complex behaviors as well as guide bioinspired engineers how to design more silent flapping robots ( Wood , 2008; Keennon et al . , 2012 ) .
The 3D aerodynamic force platform flight arena consisted of a 0 . 5 × 0 . 5 × 0 . 5 m ( height , width , depth ) chamber , where each of the six sides is an instrumented carbon fiber force plate that mechanically integrates pressure and shear forces generated by the freely flying hummingbird ( Ingersoll and Lentink , 2018; Lentink et al . , 2015; Hightower et al . , 2017 ) . Three high-speed stereo cameras captured the wingbeat kinematics through three orthogonal imaging windows in the plates . Each plate is statically determined and attached to three vee blocks ( VB-375-SM , Bal-tec ) , each instrumented by a Nano 43 6-axis force/torque sensor ( 4000 Hz sampling rate , lowpass filtered with an eighth order digital lowpass Butterworth filter at 180 Hz , silicon strain gage based , with SI-9–0 . 125 calibration , 2 mN resolution , ATI Industrial Automation ) . There are also two force sensors instrumenting a beam attached to the artificial flower to measure hummingbird contact forces and body weight . For detailed analysis , we selected 3D force traces over five consecutive wingbeats per flight ( N = 6 birds , each bird did two flights , n = 5 wingbeats per flight for 60 wingbeats total ) for which we manually tracked the 3D wing kinematics of four points on the bird ( right shoulder , distal end of the leading-edge covert , wingtip , and tip of the fifth primary feather ) . We recorded wingbeat kinematics through three orthogonal acrylic access ports using stereo high-speed videography at 2000 Hz using three pairs of DLT calibrated ( Hedrick , 2008 ) cameras ( four Phantom Micro M310s , one R-311 , and one LC310; Vision Research ) . We filtered the kinematics with a fourth order digital lowpass Butterworth filter with a cutoff frequency of 400 Hz ( ~10 times the wingbeat frequency ) . The acoustic setup consisted of a chamber that is 0 . 3 × 0 . 9 ×0 . 9 m ( height , width , depth ) . The sides of the chamber were made of IR transparent acrylic ( Plexiglass 3143 ) to allow visual access into the chamber while controlling what the hummingbird views from inside the chamber . Two battery-powered LED lights ( Neewer CN126 ) sustained a constant light level of 3000 lux at the flower . Combined , the arrays surrounded the hummingbird with 2176 microphones ( of which 25 ± 7 were disabled during each measurement; see Supplementary Information for details ) while it freely hovered in front of a flower to feed . The top and bottom arrays ( Sorama CAM1Ks ) each consist of 1024 microelectromechanical ( MEMS ) microphones , while the two frontal arrays ( Sorama CAM64s ) feature 64 microphones each with a sampling frequency of 46 , 875 Hz . During the actual flight , these arrays were covered by an acoustically transparent cloth ( Acoustone speaker grille cloth ) to protect both the bird and the microphones . To limit wall effects encountered in flight arenas ( Hightower et al . , 2017 ) , the feeder was centered 15 cm horizontally from the edge and 15 cm above the bottom array . The sides of the acoustic arena featured optically accessible panels in the infrared range , which were used to film the hummingbirds with four direct linear transformation calibrated high-speed infrared cameras at 500 fps . The 3D pressure field was reconstructed from the planar array measurements using broadband nearfield acoustic holography ( NAH ) . Each frequency component of the holograms was regularized independently using a Bayesian evidence method ( Wijnings , 2015 ) before adding them all together to create the broadband NAH results . To reduce distortions due to frequency leakage , linear predictive border padding ( Scholte , 2008; van Dalen et al . , 2012 ) was applied to the time signals . The radial directivity was computed using spherical NAH ( Williams , 1999 ) .
How hummingbirds hum is not fully understood , but its biophysical origin is encoded in the acoustic nearfield . Hence , we studied six freely hovering Anna’s hummingbirds , performing acoustic nearfield holography using a 2176 microphone array in vivo , while also directly measuring the 3D aerodynamic forces using a new aerodynamic force platform . We corroborate the acoustic measurements by developing an idealized acoustic model that integrates the aerodynamic forces with wing kinematics , which shows how the timbre of the hummingbird’s hum arises from the oscillating lift and drag forces on each wing . Comparing birds and insects , we find that the characteristic humming timbre and radiated power of their flapping wings originates from the higher harmonics in the aerodynamic forces that support their bodyweight . Our model analysis across insects and birds shows that allometric deviation makes larger birds quieter and elongated flies louder , while also clarifying complex bioacoustic behavior .
Anyone walking outdoors has heard the whooshing sound of birdwings flapping overhead , the buzzing sound of bees flying by , or the whining of mosquitos seeking blood . All animals with flapping wings make these sounds , but the hummingbird makes perhaps the most delightful sound of all: their namesake hum . Yet , how hummingbirds hum is poorly understood . Bird wings generate large vortices of air to boost their lift and hover in the air that can generate tones . Further , the airflow over bird wings can be highly turbulent , meaning it can generate loud sounds , like the jets of air coming out of the engines of aircraft . Given all the sound-generating mechanisms at hand , it is difficult to determine why some wings buzz whereas others whoosh or hum . Hightower , Wijnings et al . wanted to understand the physical mechanism that causes animal wings to whine , buzz , hum or whoosh in flight . They hypothesized that the aerodynamic forces generated by animal wings are the main source of their characteristic wing sounds . Hummingbird wings have the most features in common with different animals’ wings , while also featuring acoustically complex feathers . This makes them ideal models for deciphering how birds , bats and even insects make wing sounds . To learn more about wing sounds , Hightower , Wijnings et al . studied how a species of hummingbird called Anna’s hummingbird hums while drinking nectar from a flower . A three-dimensional ‘acoustic hologram’ was generated using 2 , 176 microphones to measure the humming sound from all directions . In a follow-up experiment , the aerodynamic forces the hummingbird wings generate to hover were also measured . Their wingbeat was filmed simultaneously in slow-motion in both experiments . Hightower , Wijnings et al . then used a mathematical model that governs the wing’s aeroacoustics to confirm that the aerodynamic forces generated by the hummingbirds’ wings cause the humming sound heard when they hover in front of a flower . The model shows that the oscillating aerodynamic forces generate harmonics , which give the wings’ hum the acoustic quality of a musical instrument . Using this model Hightower , Wijnings et al . found that the differences in the aerodynamic forces generated by bird and insect wings cause the characteristic timbres of their whines , buzzes , hums , or whooshes . They also determined how these sounds scale with body mass and flapping frequency across 170 insect species and 80 bird species . This showed that mosquitos are unusually loud for their body size due to the unusual unsteadiness of the aerodynamic forces they generate in flight . These results explain why flying animals’ wings sound the way they do – for example , why larger birds are quieter and mosquitos louder . Better understanding of how the complex forces generated by animal wings create sound can advance the study of how animals change their wingbeat to communicate . Further , the model that explains how complex aerodynamic forces cause sound can help make the sounds of aerial robots , drones , and fans not only more silent , but perhaps more pleasing , like the hum of a hummingbird .