4 research outputs found

    Bio-Inspired Water Strider Robots with Microfabricated Functional Surfaces

    Get PDF

    Experimental Studies and Dynamics Modeling Analysis of the Swimming and Diving of Whirligig Beetles (Coleoptera: Gyrinidae)

    Get PDF
    Whirligig beetles (Coleoptera, Gyrinidae) can fly through the air, swiftly swim on the surface of water, and quickly dive across the air-water interface. The propulsive efficiency of the species is believed to be one of the highest measured for a thrust generating apparatus within the animal kingdom. The goals of this research were to understand the distinctive biological mechanisms that allow the beetles to swim and dive, while searching for potential bio-inspired robotics applications. Through static and dynamic measurements obtained using a combination of microscopy and high-speed imaging, parameters associated with the morphology and beating kinematics of the whirligig beetle\u27s legs in swimming and diving were obtained. Using data obtained from these experiments, dynamics models of both swimming and diving were developed. Through analysis of simulations conducted using these models it was possible to determine several key principles associated with the swimming and diving processes. First, we determined that curved swimming trajectories were more energy efficient than linear trajectories, which explains why they are more often observed in nature. Second, we concluded that the hind legs were able to propel the beetle farther than the middle legs, and also that the hind legs were able to generate a larger angular velocity than the middle legs. However, analysis of circular swimming trajectories showed that the middle legs were important in maintaining stable trajectories, and thus were necessary for steering. Finally, we discovered that in order for the beetle to transition from swimming to diving, the legs must change the plane in which they beat, which provides the force required to alter the tilt angle of the body necessary to break the surface tension of water. We have further examined how the principles learned from this study may be applied to the design of bio-inspired swimming/diving robots. DOI: 10.1371/journal.pcbi.100279

    Mini-/Micro-Scale Free Surface Propulsion

    Get PDF
    This work reports theoretical studies and experimental proofs of the propulsion of mini-/micro-scale floating objects that propel on air-liquid interface by using two different principles. The devices are extremely simple and do not include any moving parts. The first principle takes advantage of three-phase contact line oscillation that is activated by AC electrowetting on dielectric (EWOD) to propel the floating object. The capillary wave that is generated by the free surface oscillation is visualized by using the Free-Surface Synthetic Schlieren (FS-SS) method. A 3-D flow field sketch is constructed based on the flow visualizations and PIV measurements. The flow field and trajectories of seeded particles suggest that Stokes drift is the responsible mechanism for the propulsion. The propulsion speed of the floating object highly depends on the amplitude, frequency, and shape of the EWOD signal. These phenomena are also explained by the measured oscillation amplitudes and Stokes drift relations. Additionally, it is shown that a wider EWOD electrode generates a faster propelling speed. Finally, with stacked planar receiver coils and an amplitude modulated signal, a wirelessly powered AC EWOD propulsion is realized. The second principle of floating object propulsion is the Cheerios effect, which is also generally known as lateral capillary force. Four common physical configurations (interactions between two infinite vertical walls, two vertical circular cylinders, two spheres, and a sphere and a vertical wall) are reviewed. Through theoretical analysis, it has been revealed that not the wettability of the surface but the slope angle of the object is the most important parameter for the Cheerios effect. A general rule for this effect is that the lateral capillary force is attractive if the slope angles of the interacting objects have the same sign, otherwise the force is repulsive. In addition to the surface wettability, the size and the density of floating spheres are also important for the slope angle. Active control of the Cheerios effect is achieved by implementing EWOD and dielectrowetting methods to adjust the surface wettability. By sequentially activating micro-fabricated EWOD/dielectrowetting electrodes, linear translations of floating objects in the small scale channel are accomplished. A continuous rotational motion of the floating rod is achieved in a circular container by the EWOD method

    ์†Œ๊ธˆ์Ÿ์ด๊ณผ ๊ฑฐ๋Œ€ ์†Œ๊ธˆ์Ÿ์ด์˜ ์ˆ˜๋ฉด ์œ„ ๊ฑฐ๋™์— ๋Œ€ํ•œ ํ–‰๋™ ๋ฐ ํ˜•ํƒœํ•™์  ์ ์‘

    Get PDF
    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ์ž์—ฐ๊ณผํ•™๋Œ€ํ•™ ์ƒ๋ช…๊ณผํ•™๋ถ€, 2023. 8. Piotr G. Jablonski.Allometry is a study of the relationships between body size and other morphological and behavioral characteristics of an organism that result from the physics of the habitat and the biology of the organism living in its typical habitat. Water striders, Gerridae, is a good model taxon to study the locomotion and morphological adaptations to the laws of physics of their semiaquatic habitat: the water surface. The hydrodynamics and biomechanics of jumping and striding by water striders are well-understood in certain genera such as Gerris and Aquarius. Also, the hydrodynamic functions of micro hair structures on insect bodies have been studied in a relatively narrow range of water strider species. I studied two large-sized subtropical SE Asian species: Gigantometra gigas and Ptilomera tigrina. The body sizes of these species are approximately 2-10 times heavier than those of the typically studied species. The existing theory of jump of water striders predicts water striders use surface tension-dominant jump without surface breaking, which improves take-off velocity and reduces take-off delay. However, I observed that two large-sized species jump with surface-breaking and do not follow the existing theory of jump. I corrected the previous model without concerning drag to a model that includes drag calculation. The model shows that heavy species should break the water surface and utilize drag for thrust to achieve enough jump performance to escape from underwater predators. I developed another model that simulates floating conditions and sliding resistance of striding water striders. The model reveals that in order to float on the water surface, heavy species should have developed long forelegs to support the anterior part of the body with symmetric striding (two forelegs support the anterior body and two midlegs thrust simultaneously), or use asymmetric striding (one stretched forward midleg support the anterior body and another midleg and a contralateral hindleg thrust). The data on behavior observations and morphological measurements were consistent with the results of the model simulations. I explored the detailed micro-morphology of hair structures of the two species and observed how these structures are used by insects, by using scanning electron microscopy, optical microscopy, x-ray microscopy, and high-speed videography. The feasible match between the locomotive behavior of using legs and morphological characteristics of hairs implied hypothetical adaptive functions of these distinct hair structures of the two large species in comparison to the typical medium-sized water strider, A. paludum, that lives on stagnant water. Special hair brushes on the thrusting legs of P. tigrina were linked with their extremely fast striding behavior and fast-flowing habitat preference proven in this thesis. The theoretical modeling, observations, and experiments show how Gerridae illustrate adaptative links between the behavior, morphology, and habitat characteristics of organisms.Allometry๋Š” ์„œ์‹์ง€์˜ ๋ฌผ๋ฆฌ๋ฒ•์น™๊ณผ ์œ ๊ธฐ์ฒด์˜ ์ƒ๋ฌผํ•™์  ํŠน์„ฑ์œผ๋กœ ๊ฒฐ์ •๋œ ํ˜•ํƒœํ•™ ๋ฐ ํ–‰๋™ํ•™์  ํŠน์„ฑ์ด ๋ชธ ํฌ๊ธฐ์™€ ์ฃผ๊ณ  ๋ฐ›๋Š” ์ƒํ˜ธ๊ด€๊ณ„์— ๋Œ€ํ•œ ์—ฐ๊ตฌ์ด๋‹ค. ์†Œ๊ธˆ์Ÿ์ด๊ณผ์— ์†ํ•˜๋Š” ๋ฐ˜์ˆ˜์ƒ ๊ณค์ถฉ๋“ค์€ ์ˆ˜ํ‘œ๋ฉด์ด๋ผ๋Š” ํŠน์ •ํ•œ ํ™˜๊ฒฝ์— ์‚ด๊ธฐ ๋•Œ๋ฌธ์— ์ˆ˜๋ฉด์—์„œ ํ™œ๋™ํ•˜๋Š” ์ƒ๋ช…์ฒด์˜ ์šด๋™์„ ๊ด€์ฐฐํ•˜๊ณ  ์ˆ˜๋ฉด์˜ ๋ฌผ๋ฆฌ๋ฒ•์น™์— ์ ์‘ํ•˜์—ฌ ์Šต๋“ํ•œ ํ˜•ํƒœํ•™์  ํŠน์ง•์„ ์—ฐ๊ตฌํ•˜๊ธฐ ์œ„ํ•œ ์ ํ•ฉํ•œ ๋ถ„๋ฅ˜๊ตฐ์ด๋‹ค. ์†Œ๊ธˆ์Ÿ์ด์˜ ์ˆ˜์ง๋„์•ฝ๊ณผ ์ˆ˜ํ‰์ด๋™์— ๋Œ€ํ•œ ๊ธฐ์กด ์—ฐ๊ตฌ๋“ค์€ Gerris ๋ฐ Aquarius ์™€ ๊ฐ™์€ ํŠน์ • ๋ถ„๋ฅ˜๊ตฐ์— ์†ํ•˜๋Š” ์ข…์„ ๋Œ€์ƒ์œผ๋กœ ์œ ์ฒด ์—ญํ•™ ๋ฐ ์ƒ์ฒด ์—ญํ•™์  ์›๋ฆฌ์— ์ดˆ์ ์„ ๋งž์ถฐ์™”๋‹ค. ๋˜ํ•œ ๋ชธ์ฒด์— ์žˆ๋Š” ๋ฏธ์„ธ๋ชจ ๊ตฌ์กฐ์˜ ์œ ์ฒด ์—ญํ•™์  ๊ธฐ๋Šฅ๋„ ๋น„๊ต์  ์ข์€ ๋ฒ”์œ„์˜ ์†Œ๊ธˆ์Ÿ์ด ์ข…์—์„œ ์—ฐ๊ตฌ๋˜์—ˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ๋Š” ๋™๋‚จ์•„์—์„œ ์„œ์‹ํ•˜๋Š” Gigantometra gigas์™€ Ptilomera tigrina๋ฅผ ๊ด€์ฐฐ, ์‹คํ—˜ ๋ฐ ์ด๋ก ์  ๋ชจ๋ธ๋ง์„ ์ง„ํ–‰ํ•จ์œผ๋กœ์„œ ์†Œ๊ธˆ์Ÿ์ด๊ณผ(Gerridae)์˜ ์ ์‘์„ ํ–‰๋™, ํ˜•ํƒœ ๋ฐ ์„œ์‹์ง€ ํŠน์„ฑ์œผ๋กœ ์„ค๋ช…ํ•˜๊ณ ์ž ํ•˜์˜€๋‹ค. ์ด ์ข…๋“ค์˜ ๋ชธ๋ฌด๊ฒŒ๋Š” ๊ธฐ์กด ์—ฐ๊ตฌ์—์„œ ๋„๋ฆฌ ๋‹ค๋ค˜๋˜ ์ข…๋“ค๋ณด๋‹ค 2๋ฐฐ์—์„œ 10๋ฐฐ ๊ฐ€๋Ÿ‰ ๋ฌด๊ฒ๊ธฐ ๋•Œ๋ฌธ์— ์ง€๊ธˆ๊ป ๋ณด๊ณ ๋˜์—ˆ๋˜ ์—ฐ๊ตฌ ๋ชจ๋ธ์˜ ๊ฐ€์šฉ์„ฑ์€ ๋ฒ ์ผ์— ์Œ“์—ฌ ์žˆ์—ˆ๋‹ค. ์†Œ๊ธˆ์Ÿ์ด์˜ ์ˆ˜์ง๋„์•ฝ์„ ์˜ˆ์ธกํ•˜๋Š” ๊ธฐ์กด ์—ฐ๊ตฌ ๋ชจ๋ธ์€ ์ˆ˜๋ฉด์˜ ํ‘œ๋ฉด ์žฅ๋ ฅ์ด ๋„์•ฝ์˜ ์ฃผ์š” ์ถ”์ง„๋ ฅ์„ ์ œ๊ณตํ•˜๊ธฐ ๋•Œ๋ฌธ์— ์†Œ๊ธˆ์Ÿ์ด๊ฐ€ ์ˆ˜๋ฉด์„ ๊นจ์ง€ ์•Š๊ณ  ๋„์•ฝํ•˜์—ฌ ๋„์•ฝ ์†๋„๋ฅผ ํ–ฅ์ƒ์‹œํ‚ค๊ณ  ์ˆ˜ํ‘œ๋ฉด ํƒˆ์ถœ ์ง€์—ฐ์‹œ๊ฐ„์„ ์ค„์ด๋Š” ๊ฒƒ์œผ๋กœ ์˜ˆ์ธกํ–ˆ๋‹ค. ํ•˜์ง€๋งŒ ๋ณธ ์—ฐ๊ตฌ์—์„œ ๋‹ค๋ฃจ๋Š” ๋‘ ๋Œ€ํ˜• ์ข…์€ ๊ธฐ์กด์˜ ์˜ˆ์ธก๊ณผ ๋‹ฌ๋ฆฌ ์ˆ˜๋ฉด์„ ๊นจ๋œจ๋ฆฌ๋ฉด์„œ ๋„์•ฝํ•˜๊ธฐ ๋•Œ๋ฌธ์— ๊ธฐ์กด ๋ชจ๋ธ์— ํ•ญ๋ ฅ๊ณผ ํ‘œ๋ฉด์žฅ๋ ฅ์„ ๋ชจ๋‘ ํฌํ•จํ•˜๋„๋ก ์ˆ˜์ •ํ•˜์˜€๋‹ค. ์ด๋ฅผ ํ† ๋Œ€๋กœ ๋‘ ์ข…์˜ ์ˆ˜์ง๋„์•ฝ์„ ์˜ˆ์ธกํ•ด๋ณธ ๊ฒฐ๊ณผ, ํ‘œ๋ฉด์žฅ๋ ฅ ์™ธ์—๋„ ํ•ญ๋ ฅ์„ ์ถ”์ง„๋ ฅ์œผ๋กœ ํ™œ์šฉํ•ด์•ผ๋งŒ ์ˆ˜์ค‘ ํฌ์‹์ž๋กœ๋ถ€ํ„ฐ ํƒˆ์ถœํ•˜๊ธฐ์— ์ถฉ๋ถ„ํ•œ ๋„์•ฝ ์„ฑ๋Šฅ์„ ๋‚ผ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์ด๋ฐ–์—๋„ ์†Œ๊ธˆ์Ÿ์ด๊ฐ€ ์ˆ˜๋ฉด ์œ„์— ๋– ์žˆ๊ธฐ ์œ„ํ•œ ์กฐ๊ฑด๊ณผ ์ˆ˜๋ฉด ์œ„์—์„œ ๋ฏธ๋„๋Ÿฌ์งˆ ๋•Œ์˜ ์ €ํ•ญ์„ ์˜ˆ์ธกํ•˜๋Š” ๋ชจ๋ธ๋„ ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. ๊ทธ ๊ฒฐ๊ณผ๋กœ ๋ฌด๊ฑฐ์šด ์†Œ๊ธˆ์Ÿ์ด ์ข…์€ ์ขŒ์šฐ ๋น„๋Œ€์นญ ์ถ”์ง„(์•ž์œผ๋กœ ๋ป—์€ ํ•˜๋‚˜์˜ ์ค‘๊ฐ„ ๋‹ค๋ฆฌ๊ฐ€ ์•ž์ชฝ ๋ชธ์ฒด๋ฅผ ๋– ๋ฐ›์น˜๊ณ  ๋ฐ˜๋Œ€ํŽธ ์ค‘๊ฐ„๋‹ค๋ฆฌ์™€ ๋’ค์ชฝ์˜ ๋’ท๋‹ค๋ฆฌ๋กœ ์ถ”์ง„ํ•˜๋Š” ๋ฐฉ์‹)์„ ํ•˜๊ฑฐ๋‚˜ ์ขŒ์šฐ ๋Œ€์นญ ์ถ”์ง„(์–‘์ชฝ ์•ž๋‹ค๋ฆฌ๊ฐ€ ์•ž์ชฝ ๋ชธ์ฒด๋ฅผ ๋– ๋ฐ›์น˜๊ณ  ์–‘์ชฝ ์ค‘๊ฐ„๋‹ค๋ฆฌ๋กœ ๋™์‹œ์— ์ถ”์ง„ํ•˜๋Š” ๋ฐฉ์‹)์„ ํ•˜๋˜ ๋‹ค๋ฅธ ์ข…๋“ค๋ณด๋‹ค ๊ธด ์•ž๋‹ค๋ฆฌ๋กœ ์•ž์ชฝ ๋ชธ์ฒด๋ฅผ ์ง€์ง€ํ•ด์•ผ๋งŒ ์ˆ˜๋ฉด์— ๋– ์žˆ์„ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ ์‹œํ–‰๋œ ํ–‰๋™ ๊ด€์ฐฐ๊ณผ ํ˜•ํƒœํ•™์  ์ธก์ • ๋ฐ์ดํ„ฐ ๋˜ํ•œ ๋ชจ๋ธ ์˜ˆ์ธก ๊ฒฐ๊ณผ์™€ ์ผ์น˜ํ–ˆ๋‹ค. ๋‘ ์ข…์˜ ์ž์„ธํ•œ ๋งˆ์ดํฌ๋กœ ํ„ธ ๊ตฌ์กฐ์ฒด์™€ ๊ทธ ์‚ฌ์šฉ๋ฐฉ์‹์€ ์ฃผ์‚ฌ์ „์žํ˜„๋ฏธ๊ฒฝ, ๊ด‘ํ•™ํ˜„๋ฏธ๊ฒฝ, X์„ ํ˜„๋ฏธ๊ฒฝ, ๊ณ ์†์˜์ƒ์ดฌ์˜์„ ์ด์šฉํ•˜์—ฌ ๊ด€์ฐฐ๋˜์—ˆ๋‹ค. ํ๋ฅด์ง€ ์•Š๋Š” ๋ฌผ ์œ„์— ์‚ฌ๋Š” ์ผ๋ฐ˜์  ํฌ๊ธฐ์˜ ์†Œ๊ธˆ์Ÿ์ด ์ข…์ธ A. paludum๊ณผ ๋น„๊ตํ–ˆ์„ ๋•Œ, ๋‘ ๊ฑฐ๋Œ€ํ•œ ์†Œ๊ธˆ์Ÿ์ด ์ข…์˜ ๋‹ค๋ฆฌ ์‚ฌ์šฉ ๋ฐฉ์‹๊ณผ ํ„ธ์˜ ํ˜•ํƒœํ•™์  ํŠน์„ฑ์˜ ์ผ์น˜๋Š” ๋‘ ์ข…์˜ ๋…ํŠนํ•œ ํ„ธ ๊ตฌ์กฐ์ฒด์˜ ์ ์‘์— ๋Œ€ํ•œ ๊ฐ€์„ค์„ ์‹œ์‚ฌํ•œ๋‹ค. P. tigrina์˜ ์ถ”์ง„์šฉ ์ค‘๊ฐ„๋‹ค๋ฆฌ์— ์ž๋ผ ์žˆ๋Š” ํŠน์ˆ˜ํ•œ ๋น—ํ˜• ํ„ธ ๊ตฌ์กฐ์ฒด๋Š” ์ด ์—ฐ๊ตฌ์—์„œ ๋ณด์—ฌ์ค€ ๋น ๋ฅธ ์œ ์† ์„œ์‹์ง€ ์„ ํ˜ธ๋„ ๋ฐ ๊ณ ์† ์ˆ˜ํ‰ ์ด๋™๊ณผ ๊ด€๋ จ์ด ์žˆ์—ˆ์œผ๋ฉฐ G. gigas์˜ ์ค‘๊ฐ„๋‹ค๋ฆฌ์˜ ๊ธด ๋ฏธ์„ธ๋ชจ์™€ ๋’ท๋‹ค๋ฆฌ์˜ ํŠน์ˆ˜ํ•œ ๋ฏธ์„ธ๋ชจ๋กœ ์ด๋ฃจ์–ด์ง„ ๋น”ํ˜•ํƒœ์˜ ๊ตฌ์กฐ์ฒด ๋˜ํ•œ ์ขŒ์šฐ ๋น„๋Œ€์นญ ์ถ”์ง„๊ณผ ๊ด€๋ จ์ด ์žˆ๋Š” ๊ฒƒ์œผ๋กœ ๋ณด์ธ๋‹ค. ๋ณธ ์—ฐ๊ตฌ๋Š” ์ด๋ก ์  ๋ชจ๋ธ๋ง๊ณผ ๊ด€์ฐฐ ๋ฐ ์‹คํ—˜์„ ์‚ฌ์šฉํ•ด ์†Œ๊ธˆ์Ÿ์ด๊ณผ(Gerridae)์˜ ํ–‰๋™ ๋ฐ ํ˜•ํƒœํ•™์  ์ ์‘์„ ์„œ์‹์ง€ ํŠน์„ฑ์— ์—ฐ๊ฒฐํ•˜์—ฌ ์„ค๋ช…ํ•œ๋‹ค.Chapter 1. General Introduction 5 Chapter 2. Two different jumping mechanisms of water striders are determined by body size 12 Chapter 3. Physics of sliding on water predicts morphological and behavioral allometry across a wide range of body sizes in water striders (Gerridae) 72 Chapter 4. Functional micro-morphology of setae on legs of the heaviest semi-aquatic insect, the giant water strider (Gigantometra gigas) 119 Chapter 5. The micro-morphology of ribbon-like setae on midlegs of a large water strider from lotic habitats, Ptilomera tigrina, and their role in locomotion on the water surface 164 Chapter 6. Locomotion and flow speed preferences in natural habitats by large water striders, Ptilomera tigrina, with micro-morphological adaptations for rowing 187 Chapter 7. General discussion 210 References 221 Abstract in Korean 236๋ฐ•
    corecore