2002
DOI: 10.1109/37.980248
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Serpentine locomotion with robotic snakes

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Cited by 344 publications
(31 citation statements)
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“…This model has been widely used to study and model the terrestrial motion of snakes (e.g. Hirose and Morishima (1990), Dowling (1999), Prautsch and Mita (1999), Saito et al (2002), Mori and Hirose (2002), Chernousko (2005), Maladen et al (2011) and Enner et al (2012)). Here, we modify this model to consider the 3D motion of snakes through air.…”
Section: Methodsmentioning
confidence: 99%
“…This model has been widely used to study and model the terrestrial motion of snakes (e.g. Hirose and Morishima (1990), Dowling (1999), Prautsch and Mita (1999), Saito et al (2002), Mori and Hirose (2002), Chernousko (2005), Maladen et al (2011) and Enner et al (2012)). Here, we modify this model to consider the 3D motion of snakes through air.…”
Section: Methodsmentioning
confidence: 99%
“…Let us assume viscous friction between robot and pipe as in Saito et al (2002), Liljebäck et al (2010), Ariizumi and Matsuno (2017), and Ariizumi et al (2018). The friction is assumed to be proportional to the normal force from the pipe as in Hicks and Ito (2005) and Ariizumi and Matsuno (2017).…”
Section: Model Including Slip Between Robot and Pipementioning
confidence: 99%
“…These methods can be separated into two approaches. One considers the sideslip of the robot body (Saito et al, 2002;Mohammadi et al, 2015;Ariizumi et al, 2018), and the other considers non-holonomic constraints without sideslip (Matsuno and Sato, 2005;Tanaka et al, 2015;Nakajima et al, 2019). These methods have the advantages of simple environments and essentially planar surfaces but are unsuitable for complex or unknown environments because it is difficult to construct the dynamic model including the interaction with such environments.…”
Section: Introductionmentioning
confidence: 99%
“…It also pushed against and propelled its wheels up the vertical surface, which reduced the load of pitching segments and increased the Royal Society Open Science (2020), 7: 191192; https://li.me.jhu.edu 19 maximal cantilevering length. We note that our robot still has the potential to achieve even higher speeds with high traversal probability, because in our experiments the motors were actuated at only 50% full speed to protect the robot from breaking after drastically flipping over as well as motor overload due to inertial forces and we have yet to systematically test and identify optimal serpenoid wave parameters [62]. [28,31,[35][36][37][38]40]…”
Section: Contribution To Roboticsmentioning
confidence: 99%