2018
DOI: 10.1002/pamm.201800406
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Dynamical Modeling and LQR Control of a Gyroscopically Stabilized Bicycle

Abstract: This contribution focuses on the dynamical modeling and control of a self-balancing bicycle. The bicycle is equipped with two flywheels rotating at constant speed mounted via a hinge that is actuated by an additional motor and allows for rotation about the vertical axis. Due to the balance of angular momentum, a torque is generated around the axis perpendicular to the hinge and spinning axis, i.e. an axis along the forward motion direction. This gyroscopic effect is exploited for the stabilization of the bicyc… Show more

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Cited by 5 publications
(2 citation statements)
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“…Where 𝐷 represents the dimension problem and 𝑆 represents a random vector by size 1 × 𝐷 and 𝐿𝐹 is the levy fight function, and calculated as (8).…”
Section: Hard Besiegementioning
confidence: 99%
“…Where 𝐷 represents the dimension problem and 𝑆 represents a random vector by size 1 × 𝐷 and 𝐿𝐹 is the levy fight function, and calculated as (8).…”
Section: Hard Besiegementioning
confidence: 99%
“…CMG is only utilized for self-balancing while the two-wheeler is stationary or traveling at modest speeds (He and Zhao, 2015;Jin et al, 2015;Chi and Chou, 2016;Gattringer et al, 2018;Jain et al, 2020). This technique is inefficient at high speeds because it demands constant energy consumption from the CMG's continuously rotating flywheel.…”
mentioning
confidence: 99%