Mitigating memory effects during undulatory locomotion on hysteretic materials

  1. Perrin E Schiebel  Is a corresponding author
  2. Henry C Astley
  3. Jennifer M Rieser
  4. Shashank Agarwal
  5. Christian Hubicki
  6. Alex M Hubbard
  7. Kelimar Diaz
  8. Joseph R Mendelson III
  9. Ken Kamrin
  10. Daniel I Goldman  Is a corresponding author
  1. Department of Physics, Georgia Institute of Technology, United States
  2. Biology and the Department of Polymer Science, University of Akron, United States
  3. Department of Mechanical Engineering, Massachusetts Institute of Technology, United States
  4. Department of Mechanical Engineering, Florida A&M University-Florida State University, United States
  5. School of Biological Sciences, Georgia Institute of Technology, United States
  6. Zoo Atlanta, United States
14 figures, 4 tables and 1 additional file


Body shape, waveform, and ability to progress across GM varies among snake species.

(a–c) Snapshots of snakes moving on the surface of GM. Dashed lines roughly indicate the area of material disturbed by the motion of the animal. (a) The generalist pygmy rattlesnake Sistrurus miliarius attempting to move on natural sand collected from Yuma, Arizona, USA. The animal has completed several undulations, sweeping GM lateral to the midline of the body. This snake failed to progress further than pictured. (b) The generalist eastern indigo snake Drymarchon couperi. On the same GM as (a) (c) The sand-specialist shovel-nosed snake Chionactis occipitalis in the lab on 300 μm glass particles. (d–i) Digitized midlines of animals. Color indicates time from beginning to end of the trial. All scaled to the 10 cm scale bar shown. (d–g) are on Yuma sand and (h,i) are on glass particles. (d) Tiger rattlesnake Crotalus tigris, a rocky habitat specialist. The animal was unable to progress on the GM. Total length of the trial ttot= 25.7 s, time between plotted midlines δt=100 ms (e) Rock rattlesnake Crotalus lepidus, a rocky habitat specialist. ttot= 9.4 s, δt=33 ms (f) Egg-eating snake Dasypeltis scabra inhabits a wide range of habitats in Africa. ttot= 1.6 s, δt=33 ms (g) Nerodia sipedon, a water snake inhabiting most of the Eastern US extending into Canada. ttot= 6.0 s, δt=33 ms (h) C. occipitalis 130 and (i) 128. These trials represent the inter-individual variation in kinematics. Some of the animals moved approximately ‘in a tube’ where all segments of the body followed in the path of their rostral neighbors (e.g. (h), ttot= 1.25 s, δt=12 ms) while others used this strategy only on the anterior portion of the body, appearing to drag the posterior segments in a more or less straight line behind themselves (e.g. (i), ttot= 1.01 s, δt=12 ms).

Figure 2 with 2 supplements
Snake waveform parameters measured in experiment.

(a, left) θ=acos(x^t^) for local tangent angle, t^ and average direction of motion x^. Example body posture shown, colored by θ. (a, right) Example serpenoid curves (Equation 1) of different ξ on a body of fixed length and θm=48 deg. (b) C. occipitalis experimental measurements plotted in the (θm,ξ) parameter space. Color indicates animal number. Markers are the mean and range of each individual taken over all trials. N = 9 individuals, n = 30 trials. The gray region in the upper right corner are waves which are inaccessible given the flexibility of the snake (Sharpe et al., 2015). θm was comparable to values measured from images of tracks taken in the field (Figure 2—figure supplement 2). (inset) A close-up of the data with mean and range from each trial plotted individually. Color consistent with the main plot (Linear fit with 95% confidence interval to inset data: slope −0.016 (-0.020,–0.011) intercept 2.66 (2.42, 2.90), R-square = 0.6). (c) Axes as in (b), black cross is the combined C. occipitalis measurements. Colored crosses are the mean and range of values measured on a per-trial basis in the non-sand-specialists, different species indicated by color. N = 22 individuals, n = 38 trials.

Figure 2—figure supplement 1
Principal component analysis (PCA) of all sand snake shapes.

(a, top) Tangent angle, θ is the angle between t^ and the average direction of motion of the animal, x^. (bottom) Example space-time plot of θ, corresponding to the bottom trial in c. The diagonal bands indicate a head-to-tail traveling wave propagated at constant speed. (b) The two dominant PCs representing θ. The solid lines are the experimental results, the dashed lines are sine fits to Aisin(ξis+ϕi). Coefficients with 95% confidence bounds were A1=0.83(0.82,0.84), A2=0.92(0.90,0.94), ξ1=1.44(1.43,1.45), ξ2=1.40(1.39,1.41), ϕ1=0.05π(0.04π,0.06π), ϕ2=0.41π(0.42π,0.39π). Both vectors were divided by the same maximum value such that the maximum amplitude was one. These two PCs account for 91% of the variance. (c) The amplitudes α1 and α2 associated with the PCs in e. Color indicates the frame number for all trials (N = 9, n = 30) combined. The trajectories move counterclockwise around the circular structure, indicating a traveling wave. The radius of this circle is the amplitude of the wave of θ. See Stephens et al., 2008.

Figure 2—figure supplement 2
Kinematics of C. occipitalis compared to field measurements.

(Plot as in main text with field measurements added). The light gray rectangle illustrates the range of θm measured from photographs taken of C. occipitalis tracks found in the desert (17 measurements). Experimental measurements plotted in the {θm,ξ} parameter space. Color indicates animal number. Markers are the mean and range of each individual taken over all trials. N = 9 individuals, 30 trials. The gray cross is the waveform used by C. occipitalis when moving subsurface. The surface waveform was distinct from that used by this species when moving buried within the GM (Sharpe et al., 2015). While the angular amplitude was not significantly different (subsurface θm=54.7±11.9 deg compared to the surface value θm=48.3±7.0 deg for all snakes combined, 2-tailed t-test P=0.04 mean of all trials and std of mean of all trials), the value of ξ was less for surface swimming (ξ=3.53±0.85 subsurface versus ξ=1.90±0.14 at the surface, P < 0.001). The gray region in the upper right corner are waves which are inaccessible given the flexibility of the snake (Sharpe et al., 2015).

Figure 3 with 1 supplement
Characterizing granular forces experienced by snakes by empirically measuring stress on a partially buried plate.

(a) Side-view of C. occipitalis moving on the surface. Snake is moving from left to right. The surface was initially featureless, the piles of sand outlined by the black, dashed line were generated by the motion of the snake. Gray rectangle illustrates the flat plate snake body segment model, aligned with t^ of the midline moving in direction v^. (inset) Top view of a snake. βs is the angle between the local tangent and velocity unit vectors. (b) Aluminum plate, dimensions 3 × 1.5 × 0.3 cm3. The plate was kept at a constant depth, z, from the undisturbed free surface of the GM to the bottom of the intruder. (c) Top view of the plate moving in a direction vd^ at angle βd. Components σt and σn of the total stress, σ. (d) Raw drag data collected at βd=30 deg and vd=10 mm s-1 as a function of drag distance of the plate. The upper black curve is σn, the lower gray is σt. Force data collected at 1000 Hz, plotted here down-sampled by a factor of 10 to facilitate rendering.

Figure 3—video 1
Side view of C. occipitalis moving on GM.

Video is slowed ten times.

Figure 4 with 2 supplements
Granular drag stress as a function of speed and depth.

(a) Stress normal to the plate face as a function of vd at a constant depth z=8 mm (black points) and z=12 mm (blue points). As shown in the diagram at the upper left, βd=90 deg for all trials such that the total stress was equal to σn. Markers are mean and std. of three trials. Where error bar is not visible error is smaller than the marker. Gray curve is the model prediction for z=8 mm and light blue curve for z=12 mm. (inset) Normal force versus vd measured in experiment (circle markers) and as predicted by the model (solid curves). Color is consistent with the main plot. Each dot is the average force measured in one trial, all trials shown. (b) Stress normal to the plate face as a function of z at vd=10 mm s-1. All experimental data shown in this figure are averaged from 10 to 20 cm drag distance. Over this distance the force had reached steady state and the robot arm was moving at the commanded velocity.

Figure 4—figure supplement 1
C. occipitalis movement speed independent of waveform parameters.

(a) Center-of-mass velocity, vCoM, versus segment velocity (as if one were riding on the body), vseg. Lines are mean and std. of each measurement. Each data point is an individual trial, individual number as shown in colorbar to the far right. Colors are consistent with those in main text Figure 2. Gray line is the linear fit (mean and 95% confidence intervals of slope = 0.81 (0.74, 0.89), y-intercept = 0.67 (-4.63 5.94), R-squared = 0.94, RMSE = 2.88) N = 9 individuals, n = 30 trials. (b) Number of waves on the body, ξ, versus vCoM. Mean and std. for each trial, colored according to individual. (c) Attack angle, θm, versus vCoM. Mean and std. for each trial, colored according to individual.

Figure 4—figure supplement 2
C. occipitalis tracks.

(a) Diagram of the laser-line apparatus. A laser sheet spans the sand-fluidized bed. An off-axis camera (Logitech C920 HD Pro Webcam) captured images of the laser line. Both the laser and camera were affixed to a linear bearing and moved using a linear actuator (Firgelli). We used MATLAB to move the actuator and collect an image every 1 mm, verified using a ruler placed in view of the camera. The location of bright pixels in the images was used to estimate the height of the material at that x location as a function of y. (b) Track in the GM remaining after a trial. Warm colors indicate the piles formed rising above the free surface. The snake travelled in the direction indicated. The body intrudes beneath the free surface and yields the material, creating piles on the anterior edges of the path like those described by Mosauer, 1933 and seen in the tracks observed in the field. (c) Height of the material as a function of y at three x locations, i, ii, and iii as shown in (b). (d) Log of the probability density function of all z measurements shown in (b). The free surface is at zero.

Stress as a function of plate drag angle.

(a) Stress anisotropy versus drag distance. Since σt is small, values with noise included can approach zero. As we were interested in the force evolution over several cm (for the plotted drag speed this corresponds to signals <1 Hz), we removed fluctuations above 5 Hz using a low-pass butterworth filter. Curves from three trials are shown for each of four different, fixed βd=15 (darkest, bottom curve), 30, 45, and 60 deg (lightest, top curve) as labeled on the right of the plot. The slopes of a linear regression fit to the average of three trials as a function of drag distance were −1.8 × 10-5, −2.9 × 10-5, −5.0 × 10-5 and −6.4 × 10-5 cm-1 for βd= 15, 30, 45, and 60 deg, respectively (R-square = 0.6, 0.8, 0.8, and 0.7). (b) Average stress as a function of changing drag angle. Each measurement was calculated by averaging the raw stress data from 10 to 20 cm drag distance. Each data point is the mean and standard deviation of three trials; error bars are smaller than the markers. Solid lines are the fit functions used in the RFT calculations.

The ratio of granular normal to tangential stress, σn/σt, is not strongly dependent on speed or depth.

(a) σn/σt as a function of βd. Light gray horizontal line indicates σn/σt=1. All depths and speeds are plotted as indicated by color. Dashed curves are the anistropy for a low-Re swimmer in Newtonian fluid (green, Cn/Ct1.5 for a smooth, long, and slender swimmer Boyle, 2010) and subsurface in the same ≈ 300 µm GM used in this study (black). Labels are below the associated curves. The solid gray area is the probability density (pdf) of βs measured on the snake in experiment (N = 9 individuals, n = 30 trials). (b) σn/σttan(βd) versus βd for the surface granular drag at varying z and viscous fluid shown in (a). Line color and types consistent with (a). (c) σn/σt as a function of vd at the values of βs indicated. Colors correspond to the colored arrows on the horizontal axis in (a). Linear fits to the data (not shown) with slope, m, and 95% confidence bounds in parentheses for βd=60 deg m=-0.019 deg (−0.040,0.003) R-square = 0.88; βd=20 deg m=-0.003 deg (−0.007, 0.002) R-square = 0.75; βd=5 deg m=0.003 deg (−0.011, 0.016) R-square = 0.23, (d) σn/σt as a function of z. Colors and angles are the same as in (c).

Figure 7 with 1 supplement
Comparison of RFT results with snake performance.

(a) vCoM as a function of the animal scale-grain friction. μ = 0.1 corresponding to C. occipitalis is indicated by the vertical dashed line. The light blue curve is RFT calculation for the snake parameters without any lifting and the dark blue curve was calculated for lifting of segments whose θ was in the lowest 41% (equivalent to the wave apexes Figure 7—figure supplement 1). The horizontal black line and gray bar are the average and range of vCoM calculated from experiment. (b) RFT calculation of vCoM as a function of θm using granular force relations measured at different depths, z, denoted by color. Three of the curves are dashed so that all six curves can be seen. The vertical line and blue bar denote the mean and range of θm measured in experiment. (c) Relationship between vCoM and vseg measured in C. occipitalis experiment (gray circles) and predicted by RFT using force relations measured at z=8 mm for constant vd=10 mm s-1 (light blue line) and vd=vseg (dark blue line and cross markers). Solid gray line is a linear fit to the animal data vCoM=0.82vseg+0.54 (R-square = 0.94).

Figure 7—figure supplement 1
Measurement of the vertical wave of lifting.

(a) An OptiTrack motion capture system (four Prime 17W cameras) captured 3D kinematics of C. occipitalis moving in the fluidized track way by tracking 3 mm diameter IR-reflective markers placed at 1.5 cm intervals along the mid-line. Space-time plot of θ is the fractional arclength from the neck at s=0 to the vent at s=1. (b) Space-time plot of the vertical position of the snake's midline measured relative to the free surface. Axes are as in (a). (c) Probability density of the wavenumber of the horizontal wave (gray) and vertical wave (red). The ratio of the median values of the two curves is 2.1, indicating that the spatial frequency of the wave of lifting is twice that of the wave in the horizontal plane. There were some outliers due to measurement error which were ξ>10 that have been excluded as unphysical. (d) The phase of the wave in z versus the wave in θ. The wave in z is traveling at twice the frequency of that in θ. The result is that the peaks of the wave in z align with the extrema in θ, that is, the apexes of the horizontal wave are lifted off of the substrate. N = 3 individuals (122–11 trials, 124–3 trials, 131–3 trials). Ratio of the median values of each curve is 2.1. (e) Diagram of the lifting used in RFT calculation. Shown is an example serpenoid curve of the average waveform measured in experiment. The CoM position of each of the 100 segments used in the calculation are displayed as circles, colored by whether they are in contact with the substrate (gray) or lifted (red, force set to zero).

Figure 8 with 1 supplement
Trade-off between external torque and internal actuation speed.

(a) RFT prediction of the peak joint level torque, τm,RFT, occurring during one undulation cycle as a function of θm and ξ. Color indicates the log of τm,RFT. White cross is the mean and range of animal θm and ξ. measured in experiment. (b) Heatmap of relative actuation speed, vrel=vshort,ovshort(θm,ξ,f)vshort.o at the nominal waveform of C. occipitalis (θm=48.4, ξ=1.9). Frequency, f, is calculated to yield the desired vCoM for a given waveform’s stride length (see Materials and methods for details). Diagram in upper left corner illustrates the bending beam. The nominal length of a segment at the midline is δs, blue dashed line. The length of the inside of a segment is δs, solid blue line. Relative actuation speed is the rate of change of δs at the nominal vCoM, assuming no-slip motion.

Figure 8—figure supplement 1
Surface RFT results for mCoT, BLC, and τm,RFT.

The horizontal axis of all plots is θm. Moving from left to right increases the amplitude of the body wave.Moving from left to right increases the amplitude of the body wave. The vertical axis is ξ, the number of waves on the body increases from bottom to top of each plot. White crosses are average ± range of mean values measured in 30 snake trials (N = 9 individuals). (a) Mechanical cost of transport, mCoT, calculated for each pair of θm and ξ. The color corresponds to log(mCoT). (b) Bodylengths traveled pedr cycle, BLC. Black cross is the waveform used by C. occipitalis when moving subsurface within the same ≈ 300 μm glass particles. Values from Sharpe et al., 2015.

RFT reveals waveform balances internal and external concerns in C. occipitalis.

(a) Segment-power-limited velocity, vpl, divided by vmax, the largest value of vpl, in the θm, ξ space. Black cross is the snake waveform as in (Figure 2(c)). (b) vpl/vmax versus ξ for θm=48.4 deg, the average experimental value. This is a vertical slice of (a). The vertical dashed line and gray shaded area are the mean and range of snake ξ values. (c) Solid black curve vpl/vmax (left vertical axis) and gray dashed curve τm,RFT (right vertical axis) versus θm for ξ=1.90 (the average snake value) are horizontal slices of (a) and Figure 8(a), respectively. The vertical dashed line and light gray shaded area are the mean and range of snake θm. Horizontal gray bars are the estimated muscle torque capabilities of the snakes (see Materials and methods for details). The upper bar, τm,snake is the estimated maximum muscle torque and the bottom bar, speed adjusted τm,snake, is the maximum torque reduced to reflect the average muscle shortening speed of the snakes at the average experimentally measured velocity.

Figure 10 with 2 supplements
Performance depends on aspect ratio and waveform.

(a) Slip as a function of aspect ratio, L/w as illustrated on the snapshot of a snake (Acrantophis dumerili, L/w=23.2) where L is the total length of the snake (blue curve) and w is the width at the widest point (yellow line). Circle markers and vertical lines indicate the mean and std. of each trial. Horizontal bars are the range of aspect ratios measured from video stills by two different researchers. Black are successful trials, red are failures, green is C. occipitalis. Each animal tested had a unique aspect ratio; for the non-sand-specialists, multiple data points at the same L/w indicate multiple trials for the same animal. N = 22 animals, n = 38 trials. Only mean shown for C. occipitalis (N = 9, n = 30). Black curve is the RFT estimation of slip using a scale friction of μ = 0.15. Gray area indicates predictions for μ = 0.1 (lower slip) and 0.2 (higher slip). Square markers indicate RFT prediction of slip for that animal using a scale friction of μ = 0.15 with vertical lines showing range from μ = 0.1 to 0.2. For C. occipitalis μ = 0.1 (Sharpe et al., 2015) and min/max = 0.05/0.15. All RFT predictions used force relations for 300 µm glass beads assuming intrusion depth of 8 mm. (b) Slip versus θm for animals with L/w<26. Mean and standard deviation of all measurements in a trial. Square marker is the snake L/w>26 which failed. If an animal performed more than one trial we combined the measurements of all trials before taking the mean and std. dev. Successful trials in black, failures in red. Black curve is the RFT prediction using the average waveform and anatomy values calculated using all species studied, ξ=2.5, mass = 0.63 kg, L = 89 cm, and an estimated scale friction of μ = 0.15. Gray band indicates predictions for friction μ = 0.1 and 0.2. (inset) Black and red circles are the averages from the main plot. Blue markers are successful trials L/w>26.

Figure 10—figure supplement 1
Wave efficiency versus slip.

(a) Wave efficiency, average distance traveled in one undulation cycle divided by the average wavelength, as a function of slip. Black markers are from each experimental trial taken using the various snake species on natural sand. Vertical gray line is at βs=30 deg and horizontal line is at wave efficiency of 0.35. (b) Wave efficiency of the robot, distance traveled in one undulation cycle (calculated as the total distance traveled divided by three) divided by the wavelength, as a function of slip. Black markers are from each experimental trial taken using the robot for all trials wavenumber 1, 1.2, and 1.4. Vertical gray line is at βs=30 deg and horizontal line is at wave efficiency of 0.35.

Figure 10—figure supplement 2
Slip measured in experiment versus RFT prediction.

Horizontal axis is the average slip measured in experiment. For animals with more than one trial the mean of the averages is plotted. Vertical axis is the difference between slip measured in experiment and that estimated using RFT and that individual’s parameters (mass, length, average wavenumber, and average attack angle). Points colored by aspect ratio. Black line is a linear fit, R2=0.75.

Systematic exploration of substrate memory effects using a robophysical model.

(a) The 10 joint, 11 segment robot constructed using ten Dynamixel AX-12A servo actuators (Robotis) with a stall torque of 15.3 kg·cm. Yellow and white segments are 3D printed cylindrical casings, each housing one motor. Length = 72 cm and L/w=11.3. (b,c) Stills of the robot taken after it has completed 2.75 undulation cycles. θm=52 deg in (b), θm=105 deg in (c), and ξ=1 in both cases. Robot is artificially colored yellow to distinguish the body from the tail cord in white. Note the large appearance of the tail cord in c is due to perspective as the researcher was standing and loosely holding the cord above the substrate.

Robot performance is sensitive to the waveform and poorly predicted by RFT.

(a) Slip versus θm. Robot measurements are circles connected by solid lines. ξ is indicated by color, yellow is 1.4, teal is 1.2, and blue is 1. Mean and std. of three trials. Where error bars are not visible they are smaller than the marker. RFT prediction is the solid black curve. The gray shaded region indicates uncertainty in our knowledge of the robot’s mass (because of the weight of the tail cord which is held above the substrate) and friction coefficient. (b) Body lengths traveled in a single undulation cycle (BLC) as a function of attack angle. Colors and lines are consistent with (a). (c,d) Robot and (e,f) RFT predicted kinematics for ξ=1. Color indicates time from the beginning to the end (darker to lighter gray). Both robot and RFT trajectories include three complete undulations. (c,e) θm=52 deg. (d,f) θm=105 deg.

Figure 13 with 3 supplements
Material remodeling determines kinematics of the robot.

(a) Snapshot of the robot moving on poppy seeds with grain velocity vectors estimated using PIV shown in yellow. We measured the grain velocity vector angle, ψv as shown. A mask of the body (yellow) and tail (red) was used in all PIV calculations and vectors both too close and too far from the body were not included in calculating ψv. Vectors shown are representative of those included. We collected three trials per condition and three complete undulation cycles per trial. (inset) Diagram of ψv for an example estimated grain velocity vector in red. vCoM is pointing in the average direction of motion of the robot. (b) Probability density of ψv for each of the three θm tested, θm=105 (yellow), 79 (green), and 52 (blue) as labelled on the plot. Curves were calculated using all ψv measured in space and time in a single trial. Solid lines are the average curve and the shaded area indicates the standard deviation across the three trials. (c) Distance traveled by the robot in a single step, normalized by body length, measured at the end of each of three consecutive undulation cycles. ξ=1 for all trials shown. From darkest to lightest gray color: circles are θm=30 deg, square are 70 deg, and stars are 105 deg. Three trials are plotted separately for each step. RFT prediction shown as a horizontal lines with color corresponding to experiment.

Figure 13—video 1
Snake robot moving on poppy seeds.

Three undulations Top row is overhead video, bottom row is an oblique view from behind the robot (tail is at bottom of video). Left column is an intermediate waveform (θm=79 deg, ξ=1). Right column is high attack angle (θm=105 deg, ξ=1). Waveform parameters are also displayed in the top left corner of each overhead video.

Figure 13—video 2
Robot and snake failure comparison.

To the left is the robot moving on poppy seeds using an intermediate (79 deg) attack angle with one wave on the body, to the right is the pygmy rattlesnake, Sistrurus miliarus on natural sand collected near Yuma, Arizona, USA. The robot video begins after the robot has completed two full undulation cycles.

Figure 13—video 3
Snake robot replaced in old tracks.

Movie of the snake robot moving across the surface of poppy seeds using one wave on the body and a high (107 deg) attack angle. Left video shows three undulations on undisturbed poppy seeds, right is three undulations where the robot has been placed back in the track made during the trial to the left.

RFT prediction of slip gives a heuristic for performance.

(a) Color denotes slip as θm and ξ vary, calculated using RFT for robot dimensions and poppy seed force relations. Circles indicate the parameter combinations tested on the robot. Waveforms which were successful over three undulations are black, red markers denote unsuccessful parameters (distance per undulation over wavelength <0.35, Figure 10—figure supplement 1). Purple line indicates where RFT predicts βs30 deg. The lightly shaded region denotes waveforms which the robot cannot perform. White areas indicate where the RFT calculation did not converge on a solution for at least half of the time steps. (b) Slip calculated for C. occipitalis morphology moving on 300 µm glass particles. Color is the same as in (a). White cross denotes mean and range of trial averages from sand-specialist experiments.


Table 1
List of frequently-used symbols and abbreviations
GMGranular Material
RFTResistive Force Theory
ReReynolds number. Ratio of inertial to viscous forces in a system.
θangle between body segment tangent and average direction of motion
θmaverage maximum θ, attack angle
ξspatial frequency, number of waves on the body
vCoMcenter-of-mass velocity
vsegsegment velocity (as if riding on the trunk)
ωCoMangular velocity about the center-of-mass
βdgranular drag angle
vdplate drag velocity
zdepth intrusion into GM, measured from the free surface
ρdensity of granular material
βssnake body slip angle
σncomponent of granular stress normal to area element
σtcomponent of granular stress tangential to area element
σn/σtanisotropy factor. Ratio of normal to tangential stress
μscale-GM friction coefficient
Ltotal body length
L/wAspect Ratio, snake body length divided by width at the widest point
ggravitational constant = 9.81 ms-2
sarclength along snake body midline measured from the head
Table 2
Anatomical information for the non-sand-specialist species.
SpeciesSubfamilyFamilyLength (cm)Max width (cm)Mass (g)
Acranthophis dumeriliBoidae1837.95620
Agkistrodon bilineatusCrotalinaeViperidae75.43.3306.7
Agkistrodon contortrixCrotalinaeViperidae803.1359.5
Agkistrodon piscivorusCrotalinaeViperidae924.5569.5
Agkistrodon piscivorusCrotalinaeViperidae874.5
Agkistrodon piscivorusCrotalinaeViperidae572.7161
Aspidites ramsayiPythonidae1.33.4749
Bothriechis schlegeliiCrotalinaeViperidae66.71.7104
Crotalus lepidusCrotalinaeViperidae432.244
Crotalus molossusCrotalinaeViperidae82.14370.7
Crotalus tigrisCrotalinaeViperidae71.13.1331.6
Crotalus willardiCrotalinaeViperidae473134.5
Dasypeltis scabraColubridae711.151
Drymarchon couperiColubridae1624.21018
Epicrates subflavusBoidae1533738
Lampropeltis getulaColubrinaeColubridae1213680
Lichanura trivirgataBoidae712.6243.5
Loxocemus bicolorLocoxemidae1113.3607.5
Nerodia sipedonNatricinaeColubridae793.5453.5
Senticolus triaspisColubrinaeColubridae1011.8198
Sistrurus catenatusCrotalinaeViperidae522.8174.5
Sistrurus miliariusCrotalinaeViperidae472.8146
Table 3
Anatomical information for the individual sand-specialist snakes.

The species Chionactis occipitalis is in the family Colubridae. Average and standard dev. of lengths 38.0±1.3 cm.

IndividualLength (cm)Max width (cm)Mass (g)
Table 4
Coefficients for fourier fits used for Ft in RFT calculations.

Fit function is Ft(βd)=a0+a1cos(wβd)+b2sin(wβd)+a2cos(wβd)+b2sin(wβd). a0, a1, b1, a2, and b2 have units of Newtons. w is dimensionless.

Z (mm)a0a1b1a2b2W

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  1. Perrin E Schiebel
  2. Henry C Astley
  3. Jennifer M Rieser
  4. Shashank Agarwal
  5. Christian Hubicki
  6. Alex M Hubbard
  7. Kelimar Diaz
  8. Joseph R Mendelson III
  9. Ken Kamrin
  10. Daniel I Goldman
Mitigating memory effects during undulatory locomotion on hysteretic materials
eLife 9:e51412.