Surface force spectroscopic point load measurements and viscoelastic modelling of the micromechanical properties of air flow sensitive hairs of a spider (Cupiennius salei)

被引:38
作者
McConney, Michael E. [2 ,3 ]
Schaber, Clemens F. [1 ]
Julian, Michael D. [4 ]
Eberhardt, William C. [5 ,6 ]
Humphrey, Joseph A. C. [5 ,6 ]
Barth, Friedrich G. [1 ]
Tsukruk, Vladimir V. [2 ,3 ]
机构
[1] Univ Vienna, Fac Life Sci, Dept Neurobiol & Cognit Res, A-1090 Vienna, Austria
[2] Georgia Inst Technol, Sch Mat Sci & Engn, Atlanta, GA 30332 USA
[3] Georgia Inst Technol, Sch Polymer Fiber & Text Engn, Atlanta, GA 30332 USA
[4] Calif State Univ Stanislaus, Dept Chem, Turlock, CA 95382 USA
[5] Univ Virginia, Dept Mech & Aerosp Engn, Charlottesville, VA 22904 USA
[6] Univ Virginia, Dept Biol, Charlottesville, VA 22904 USA
关键词
trichobothria; spider; arthropod medium flow sensilla; atomic force microscope; force spectroscopy; ARTHROPOD FILIFORM HAIRS; BIOLOGICAL THERMAL DETECTION; SPRING CONSTANTS; RANGE FRACTIONATION; DYNAMICS; TRICHOBOTHRIA; MOVEMENT; CUTICLE; WIND; LEG;
D O I
10.1098/rsif.2008.0463
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
The micromechanical properties of spider air flow hair sensilla (trichobothria) were characterized with nanometre resolution using surface force spectroscopy (SFS) under conditions of different constant deflection angular velocities (theta)over dot (rad s(-1)) for hairs 900-950 mu m long prior to shortening for measurement purposes. In the range of angular velocities examined (4 x 10(-4)-2.6 x 10(-1) rad s(-1)), the torque T (Nm) resisting hair motion and its time rate of change (T)over dot (Nm s(-1)) were found to vary with deflection velocity according to power functions. In this range of angular velocities, the motion of the hair is most accurately captured by a three-parameter solid model, which numerically describes the properties of the hair suspension. A fit of the three-parameter model (3p) to the experimental data yielded the two torsional restoring parameters, S-3p = 2.91 x 10(-11) Nm rad(-1) and S'(3p) = 2.77 x 10(-11) Nm rad(-1) and the damping parameter R-3p = 1.46 x 10(-12) Nm s rad(-1). For angular velocities larger than 0.05 rad s(-1), which are common under natural conditions, a more accurate angular momentum equation was found to be given by a two-parameter Kelvin solid model. For this case, the multiple regression fit yielded S-2p = 4.89 x 10(-11) Nm rad(-1) and R-2p = 2.83 x 10(-14) Nm s rad(-1) for the model parameters. While the two-parameter model has been used extensively in earlier work primarily at high hair angular velocities, to correctly capture the motion of the hair at both low and high angular velocities it is necessary to employ the three-parameter model. It is suggested that the viscoelastic mechanical properties of the hair suspension work to promote the phasic response behaviour of the sensilla.
引用
收藏
页码:681 / 694
页数:14
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