Standard

Motion of a solid driven by six rods of variable length. / Leonov, G. A.; Zegzhda, S. A.; Kuznetsov, N. V.; Tovstik, P. E.; Tovstik, T. P.; Yushkov, M. P.

In: Doklady Physics, Vol. 59, No. 3, 03.2014, p. 153-157.

Research output: Contribution to journal › Article › peer-review

Harvard

Leonov, GA, Zegzhda, SA, Kuznetsov, NV, Tovstik, PE, Tovstik, TP & Yushkov, MP 2014, 'Motion of a solid driven by six rods of variable length', Doklady Physics, vol. 59, no. 3, pp. 153-157. https://doi.org/10.1134/S1028335814030100, https://doi.org/10.1134/S1028335814030100

APA

Leonov, G. A., Zegzhda, S. A., Kuznetsov, N. V., Tovstik, P. E., Tovstik, T. P., & Yushkov, M. P. (2014). Motion of a solid driven by six rods of variable length. Doklady Physics, 59(3), 153-157. https://doi.org/10.1134/S1028335814030100, https://doi.org/10.1134/S1028335814030100

Vancouver

Leonov GA, Zegzhda SA, Kuznetsov NV, Tovstik PE, Tovstik TP, Yushkov MP. Motion of a solid driven by six rods of variable length. Doklady Physics. 2014 Mar;59(3):153-157. https://doi.org/10.1134/S1028335814030100, https://doi.org/10.1134/S1028335814030100

Author

Leonov, G. A. ; Zegzhda, S. A. ; Kuznetsov, N. V. ; Tovstik, P. E. ; Tovstik, T. P. ; Yushkov, M. P. / Motion of a solid driven by six rods of variable length. In: Doklady Physics. 2014 ; Vol. 59, No. 3. pp. 153-157.

BibTeX

@article{9658acd5e132443c83eff197f4d0a3ad,
title = "Motion of a solid driven by six rods of variable length",
abstract = "The driving of the Stewart platform motion is considered as a particular case of the motion of a solid fastened arbitrarily on six rods of variable length. The inertia and weight of the rods are taken into account. The purpose of driving is to obtain the set motion of the platform. Due to obvious instability of such motions, the full range operation of the stand can be provided only by introducing a feedback. It is possible to study the motions of the solid with the arrangement of the rods different from that for the Stewart platform. It is necessary to obtain the set motion of the solid under consideration due to a change in the lengths of the rods. The purpose of driving is to obtain the set motion of the platform. We assume for simplicity that the forces of inertia of the rods are negligible. However, such a method of control is impossible because the initial position of equilibrium is unstable.",
author = "Leonov, {G. A.} and Zegzhda, {S. A.} and Kuznetsov, {N. V.} and Tovstik, {P. E.} and Tovstik, {T. P.} and Yushkov, {M. P.}",
year = "2014",
month = mar,
doi = "10.1134/S1028335814030100",
language = "English",
volume = "59",
pages = "153--157",
journal = "Doklady Physics",
issn = "1028-3358",
publisher = "МАИК {"}Наука/Интерпериодика{"}",
number = "3",

}

RIS

TY - JOUR

T1 - Motion of a solid driven by six rods of variable length

AU - Leonov, G. A.

AU - Zegzhda, S. A.

AU - Kuznetsov, N. V.

AU - Tovstik, P. E.

AU - Tovstik, T. P.

AU - Yushkov, M. P.

PY - 2014/3

Y1 - 2014/3

N2 - The driving of the Stewart platform motion is considered as a particular case of the motion of a solid fastened arbitrarily on six rods of variable length. The inertia and weight of the rods are taken into account. The purpose of driving is to obtain the set motion of the platform. Due to obvious instability of such motions, the full range operation of the stand can be provided only by introducing a feedback. It is possible to study the motions of the solid with the arrangement of the rods different from that for the Stewart platform. It is necessary to obtain the set motion of the solid under consideration due to a change in the lengths of the rods. The purpose of driving is to obtain the set motion of the platform. We assume for simplicity that the forces of inertia of the rods are negligible. However, such a method of control is impossible because the initial position of equilibrium is unstable.

AB - The driving of the Stewart platform motion is considered as a particular case of the motion of a solid fastened arbitrarily on six rods of variable length. The inertia and weight of the rods are taken into account. The purpose of driving is to obtain the set motion of the platform. Due to obvious instability of such motions, the full range operation of the stand can be provided only by introducing a feedback. It is possible to study the motions of the solid with the arrangement of the rods different from that for the Stewart platform. It is necessary to obtain the set motion of the solid under consideration due to a change in the lengths of the rods. The purpose of driving is to obtain the set motion of the platform. We assume for simplicity that the forces of inertia of the rods are negligible. However, such a method of control is impossible because the initial position of equilibrium is unstable.

UR - http://www.scopus.com/inward/record.url?scp=84902333981&partnerID=8YFLogxK

U2 - 10.1134/S1028335814030100

DO - 10.1134/S1028335814030100

M3 - Article

VL - 59

SP - 153

EP - 157

JO - Doklady Physics

JF - Doklady Physics

SN - 1028-3358

IS - 3

ER -

ID: 5707420