Fg. Barth et al., DYNAMICS OF ARTHROPOD FILIFORM HAIRS .2. MECHANICAL-PROPERTIES OF SPIDER TRICHOBOTHRIA (CUPIENNIUS-SALEI KEYS), Philosophical transactions-Royal Society of London. Biological sciences, 340(1294), 1993, pp. 445-461
Adults of the wandering spider Cupiennius salei (Ctenidae) have 936 (/- 31 s.d.) trichobothria or filiform hairs on their legs and pedipalp
s. This is the largest number of these air movement detectors recorded
for a spider. The trichobothria are 100-1400 mum long and 5-15 mum wi
de (diameter at base). Many of them are bent distally pointing towards
the spider body. Their feathery surface increases drag forces and thu
s mechanical sensitivity by enlarging the effective hair diameter. Typ
ically, trichobothria are arranged in clusters of 2-30 hairs which inc
rease in length towards the leg tip. The trichobothria's mechanical di
rectionality is either isotropic or it exhibits a preference for air f
low parallel or perpendicular (from lateral) to the long leg axis. The
se differences are neither due to the distal bend of the hair nor to t
he bilateral symmetry of the cuticular cup at the hair base but to the
spring supporting the hair. Different directional properties may be c
ombined in the same cluster of hairs. Trichobothria are tuned to best
frequency ranges between 40 and 600 Hz depending on hair length. Becau
se, with increasing hair length, absolute mechanical sensitivity chang
es as well, the arrangement of hairs in a cluster provides for a fract
ionation of both the intensity and frequency range of a stimulus, in a
ddition, in some cases, to that of stimulus direction. Boundary layer
thickness above the spider leg in oscillating airflow varies between a
bout 2600 mum at 10 Hz and 600 mum at 950 Hz. It is well within the ra
nge of hair lengths. In airflow perpendicular to the long leg axis par
ticle velocity above the leg increases considerably as compared to the
free field. The curved surface of the cuticular substrate has therefo
re to be taken into account when calculating hair motion. The experime
ntally measured properties of hair and air motion were also determined
numerically using the theory developed in the companion paper (Humphr
ey et al. Phil. Trans. R. Soc. Lond. B 340, 423-444 (1993)). There is
good agreement between the two. Short hairs are as good or better velo
city sensors as long hairs but more sensitive acceleration sensors. In
agreement with most of our measurements optimal hair length is not la
rger than boundary layer thickness at a hair's best frequency. Best fr
equencies of hair deflection and of ratio a (maximum hair tip displace
ment:air particle displacement) differ from each other. The highest me
asured value for ratio a was 1.6. In only 22% of the cases hair tip di
splacement exceeded air particle displacement. Hair motion is insensit
ive to changes in hair mass as shown by the numerical comparison of a
solid and a hollow hair.