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First published online January 31, 2007
Journal of Experimental Biology 210, 553-560 (2007)
Published by The Company of Biologists 2007
doi: 10.1242/jeb.02682
Adhesive recruitment by the viscous capture threads of araneoid orb-weaving spiders
Department of Biological Sciences, Virginia Polytechnic Institute and State University, Blacksburg, VA 24061, USA
* Author for correspondence (e-mail: bopell{at}vt.edu)
Accepted 5 December 2006
| Summary |
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Key words: adhesive mechanism, capture thread, orb-web
| Introduction |
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The operation of cribellar and viscous capture threads differs in at least
four ways: (1) the adhesion achieved per volume of thread material; (2) the
scale at which a thread interacts with a surface; (3) the efficiency with
which adhesive forces are transferred to the thread's axial fibers; and (4)
the ability of a thread span to recruit adhesion from interior regions of
contact. Relative to the volume of material that they contain, viscous threads
achieves an average of 13 times more adhesion than cribellar threads
(Opell, 1998
). The surfaces of
cribellar threads are formed of thousands of fibrils, each with a diameter of
around 20 nm (Hawthorn and Opell,
2002
; Hawthorn and Opell,
2003
; Opell,
1994a
). These fibrils implement mechanical interlock to snag on
insect setae and irregular surfaces
(Opell, 1994b
) and additional
mechanisms to adhere to smooth surfaces. Fibrils of all but the most primitive
cribellar threads feature regularly spaced, 35 nm diameter nodes that
establish as many as 170 points of interaction with each µm2 of
surface they contact (Hawthorn and Opell,
2003
). At low relative humidity each of these nodes generates van
der Waals forces, but at a relative humidity of 45% or greater they generate
stronger capillary forces (Hawthorn and
Opell, 2003
). In contrast, viscous threads typically have 30 or
fewer droplets per mm and mean droplet dimensions of 10 µm or greater
(Craig, 1987a
;
Opell, 1998
). Thus, cribellar
thread generates adhesion at many small, diffuse points of contact, whereas
viscous thread generates adhesion at a few large points of contact.
As cribellar thread establishes a large number of very small points of
contact over a wide area, the force vectors of the fibrils are not aligned and
fibrils pull on one another as force is applied to axial fibers. Thus, the
adhesion generated at these points is probably not effectively summed and
transferred to the thread's axial fibers. In contrast, viscous thread
generates adhesion at a much smaller number of in-line droplets and appears
better equipped to effectively transfer this force to the axial fibers. A
striking feature of cribellar thread is its inability to generate increased
adhesion with increased length of contact. When cribellar threads were
anchored at their ends and pulled away from contacting surfaces of two or four
different widths, no significant increase in stickiness was observed as plate
width increased (Hawthorn and Opell,
2003
) (B.D.O., unpublished). Thus, it appears that useful adhesion
is generated only in narrow bands at the outer edges of a cribellar thread's
contact with a surface. When this adhesion is exceeded, the more central
regions of the thread peel free from the contacting surface without adding
substantially to the thread's adhesion.
The lower extensibility of cribellar thread when compared with viscous
thread (Opell and Bond, 2000
;
Opell and Bond, 2001
) may
contribute to the tendency of cribellar thread adhesion to fail in this way.
If a cribellar thread achieves only a small incident angle with a contacting
surface, then most of the force applied to the thread would be perpendicular
to the surface to which it is attached and little of the force would be
directed along the thread in a manner favoring the recruitment of adhesion
from more interior regions of thread contact
(Fig. 2). In contrast, the
greater extensibility of viscous threads should combine with the plasticity of
their regularly spaced, viscoelastic droplets to produce a highly extensible
system capable of generating a greater angle of incidence under a load
(Fig. 2). This configuration
would transfer more force along the thread's axial lines, thereby recruiting
adhesion generated by inner droplets.
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We test this hypothesis by measuring the stickiness of threads spun by six Araneoidea species, whose droplet profiles range from small, closely spaced droplets to large, widely spaced droplets. We measure the stickiness of each species' threads with contact plates of four widths to alter the number of droplets that contribute to the stickiness of a thread span. The SBM predicts that thread stickiness should increase as the length of thread contact increases. However, a thread's droplet profile may limit the effectiveness of the SBM, as internal droplets that are farthest removed from the edges of thread contact may contribute little to overall thread adhesion. To better understand this system, we use the 24 stickiness values generated in this study (mean values of four plate widths for each of six species' threads) to develop a model of thread performance that incorporates droplet spacing, contact plate width, and the adhesion of individual droplets.
| Materials and methods |
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Some of the species included in this study had smaller, secondary droplets
between the much larger primary droplets
(Fig. 1). When secondary
droplets were present, their size and distribution were variable.
Additionally, secondary droplets comprised only a small percentage of the
total droplet volume per mm of capture thread
(Table 1). Therefore, we
included only primary droplets in this study. We compared the coordinates of
the profiles of each species' primary droplets with those generated by
equations for parabolas, half-circles, and half-ellipses. Regression analyses
showed that droplet coordinates most closely matched those of parabolas
(R2>0.97 for each species). Therefore, we computed
droplet volume as two times the integral of the equation of a parabola:
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We computed the spacing of each spider's droplets by multiplying the mean number of droplets per 1000 µm of thread length by mean droplet length in µm, subtracting this product from 1000 µm, and then dividing the remainder by the number of interdroplet regions in the 1000 µm span (= droplet number 1).
Stickiness measurements
We measured the stickiness of 12 thread strands per web, three sectors with
each of four contact plates having widths of 963, 1230, 1613, and 2133 µm.
Prior to beginning each measurement, temperature, barometric pressure and RH
were recorded. The mean value registered by each plate was recorded as an
individual's stickiness profile. We measured thread stickiness with a smooth
acetate plate (Scotch® MagicTM Tape 810 Product Information Sheet,
2002, St Paul, MN, USA) to maximize stickiness and to eliminate the
possibility that threads with different droplet profiles might respond
differently to a textured surface. We measured each thread with an unused
region of the surface and renewed the acetate frequently.
The instrument used to measure stickiness incorporated interchangeable contact plate units attached to the lever arm of a jeweled escapement that transferred force to a load cell machined to increase its sensitivity (Fig. 3). Each interchangeable plate unit consisted of a contact plate fastened to the tip of a small rod that could be threaded into the lever arm of the instrument and secured with a nut. On the back of each unit was a registration pin that extended perpendicular to the face of the contact plate. When a unit was being installed on the lever arm we aligned this pin with a reference jig that was mounted temporarily on the sample holder. This ensured that the face of the contact plate was parallel to the plane of the thread sampler and, therefore, to the threads whose stickiness would be measured. A thread sampler was then attached to the sample holder, which could be moved in three dimensions, permitting a thread strand to be centered on the width of a contact plate and orientated perpendicular to the plate's length before a stickiness measurement was made. After proper thread orientation was achieved, a linear actuator pressed the strand against a contact plate at a speed of 0.06 mm s1 until a force of 25 µN was generated, at which time the direction of travel was immediately reversed. As the thread strand was withdrawn, it exerted force on the plate and the maximum force achieved before the strand pulled free of the plate was recorded as the strand's stickiness.
Statistical and phylogenetic analyses
We used SAS (SAS Institute Inc., Cary, NC, USA) for statistical analyses.
To account for phylogenetic relationships among species, we used the PDAP
Module (Midford et al., 2005
)
run under Mesquite (Maddison and Maddison,
2005
) to perform independent contrast (IC) analyses
(Garland, Jr et al., 1999
;
Garland, Jr and Ives, 2000
;
Bloomberg and Garland, Jr,
2002
). Relationships among species
(Fig. 4) were based on Scharff
and Coddington (Scharff and Coddington,
1997
). We set all branch lengths to 1, as phylogeny was
drastically pruned.
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| Results |
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The inverse relationship between per-droplet stickiness and the number of droplets in a thread span documented the diminishing adhesive contribution of droplets that are more distant from the edges of thread contact. For each plate width an IC analysis of the stickiness per droplet (dependent variable) and the number of droplets contacting the plate (independent variable) had negative slopes: 963 µm: slope 7.77, two-tailed P=0.0255, R2=0.75; 1230 µm: slope 4.94, two-tailed P=0.0233, R2=0.76; 1613 µm: slope 3.77, two-tailed P=0.0237, R2=0.76; and 2133 µm: slope 2.47, two-tailed P=0.0254, R2=0.76). When all plate widths were included, a regression of percent change in stickiness per droplet (dependent variable) and percent inter-plate increase in the number of droplets contacting a plate (independent variable) was also negative (Fig. 6; y=0.556x1.864, P=0.0003, R2=0.57). This relationship and the model of thread performance described in the following paragraph explain the failure of plates of increasing widths to register increased stickiness for the threads of L. venusta and C. turbinata that have small, closely spaced droplets.
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| Discussion |
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The SBM explains how droplet profile affects a thread's ability to generate increased stickiness and why threads of L. venusta and C. turbinata with small, closely spaced droplets failed to register increased stickiness when measured with contact plates of increasing widths. For threads of L. venusta with 31.4 droplets mm1, a maximum efficiency span comprising 12 droplets is approximately 382 µm, only 40% of the narrowest contact plate that we used. Consequently, it is not surprising that these threads failed to register increased stickiness when measured with plates wider than 1000 µm. In contrast, the maximum efficiency span for threads of A. marmoreus with 4.3 droplets mm1, is approximately 2790 µm, indicating that these threads can achieve greater stickiness than we measured.
By attracting atmospheric moisture, the hydrophilic compounds in a viscous
thread cause droplet volume to fluctuate with changes in RH
(Vollrath et al., 1990
;
Townley et al., 1991
). By
photographing and measuring each spider's thread under the same RH we closely
linked the physical and performance characteristics of threads. Daily and, in
most instances, weekly changes in laboratory RH were small, as indicated by
the small standard errors of the mean RH under which each species' threads
were measured (Table 1).
However, laboratory RH did change seasonally, resulting in threads of A.
marmoreus, A. pegnia, and M. labyrinthea being measured around
53% RH, those of A. trifasciata and L. venusta
being measured around 41% RH, and C. turbinata being measured at 32%
RH. Reduced droplet volume resulting from lower RH may decrease droplet
plasticity and reduce the effectiveness of the SBM. However, even at 38% RH
A. trifasciata threads still exhibited the greatest inter-plate
differences in thread stickiness of the six species. Therefore, the failure of
L. venusta and C. turbinata threads to exhibit inter-plate
differences in stickiness cannot be explained entirely by the low RH under
which they were measured and must be influenced substantially by their small,
closely spaced droplets.
The SBM documented by this study adds a new dimension to the complex issues
of orb web architecture, prey interception and profitability
(Eberhard, 1986
;
Eberhard, 1990
;
Craig, 1987a
;
Craig, 2003
;
Wise, 1993
), and underscores
the important role that spider size plays
(Craig, 1987b
). Both the volume
and spacing of a spider's viscous droplets tend to be directly related to
spider size (Opell, 1998
;
Opell, 2002
). Prior our study,
it appeared that the close spacing of droplets produced by small spiders
compensated for smaller per droplet adhesion. However, the SBM appears to
severely limit the amount of adhesive summation that is possible. This raises
the question of why there has apparently been no selection for small spiders
to produce larger, more widely spaced droplets, features that would improve
the economy of thread adhesion by taking fuller advantage of the SBM. The rate
at which a spider's aggregate glands produce or release viscous material
probably limits droplet size by determing how much material is available to
coalesce into droplets. Thus, selection could more easily favor the production
of small, closely spaced droplets by larger spiders, such as Micrathena
gracilis (Opell, 2002
),
than of large, more widely spaced droplets by smaller spiders. Evidence for
the resource limitation of droplet size comes from the observation that, when
starved, C. turbinata produce threads with even smaller, more closely
spaced droplets (Crews and Opell,
2006
).
Small spiders like C. turbinata and L. venusta, as well
as larger spiders like Micrathena gracilis
(Opell, 2002
) that produce
threads with small, closely spaced droplets, have closely spaced spirals. This
arrangement may partially compensate for the low stickiness of their threads
by summing the adhesion of adjacent capture strands that contact an insect.
Capture threads with small, closely spaced droplets may be more effective at
holding certain surfaces, such as the legs of small insects, or at resisting a
force pulling asymmetrically on a thread or pulling parallel to the surface
that the thread has contacted. As we measured the adhesion generated by
threads that were pulled symmetrically from smooth, flat surfaces, our results
do not encompass the range of demands placed on capture threads.
In this study we used a single, smooth surface to measure thread stickiness to facilitate comparisons and modeling. However, the stickiness of viscous threads differs when measured with insect surfaces that have setae of different sizes and densities (B.D.O. and H. S. Schwend, manuscript in preparation). Threads with larger, more widely spaced droplets, like those of A. trifasciata and A. marmoreus, held insect surfaces more securely than threads with small, closely spaced viscous droplets like C. turbinata. However, compared to A. trifasciata and A. marmoreus, threads of C. turbinata registered greater relative stickiness values on fly wings, which are covered by larger setae, and lower relative stickiness on the smooth surfaces of beetle elytra. Thus, an assessment of the prey retention capabilities of an orb web must account for many factors, including capture thread spacing and the insect-surface-specific performance of capture threads.
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