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Erschienen in: Meccanica 4/2016

04.08.2015 | Parallel Manipulators

Kinematics and dynamics of planar mechanisms reinterpreted in rigid-body’s configuration space

verfasst von: Raffaele Di Gregorio

Erschienen in: Meccanica | Ausgabe 4/2016

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Abstract

Mechanisms with lower mobility can be studied by using tools that are directly deduced from those of spatial kinematics as screw theory. Nevertheless, ad-hoc tools that fully exploit the peculiarities of the displacement subgroups these mechanisms move in are usually more efficient both in showing mechanisms’ features and when used to conceive numerical algorithms. Planar displacements constitute a three-dimensional subgroup with many peculiarities that allow the use of simplified tools (e.g., complex numbers) for studying planar mechanisms. Here, the systematic use of three-dimensional vector spaces to represent link poses and velocities in planar motion and planar system of forces is investigated. The result is a novel coherent set of tools that make it possible to geometrically describe kinematics and dynamics of planar mechanisms in the three-dimensional configuration space of links’ planar poses. The effectiveness of this novel approach is shown through a case study.

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Fußnoten
1
Here, the non-homogeneity is not a problem since these components will be always separately summed.
 
2
If σ A|1 = cos θ1 i + sin θ1 j + ζPA|1 k, σ A|2 = cos θ2 i + sin θ2 j + ζPA|2 k and σ A|3 = cos θ3 i + sin θ3 j + ζPA|3 k, then σ A|1 · σ A|2 × σ A|3 = ζPA|1sin(θ3 − θ2) + ζPA|2sin(θ1 − θ3) + ζPA|3sin(θ2 − θ1).
 
3
The addition and subtraction of slope angles, θrs, must be computed by choosing the values congruent modulo 2π that belong to the range ]−π, π] rad.
 
4
If σ A|1 = cos θ1 i + sin θ1 j + ζPA|1 k and σ A|2 = cos θ2 i + sin θ2 j + ζPA|2 k, then σ A|1 × σ A|2 = ζPA|1(cos θ2 j − sin θ2 i) − ζPA|2(cos θ1 j − sin θ1 i) + sin(θ2 − θ1)  k.
 
5
Here, “passive” means without actuators. Moreover, all the kinematic pairs are supposed “ideal constraints” (i.e., without friction).
 
6
R and P denote revolute and prismatic pair, respectively.
 
7
Hereafter, an underlined R denotes an actuated R pair.
 
8
A PPM with 2RRR-RR architecture has been proposed by Pennock and Israr [13] as an adjustable six-bar linkage.
 
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Metadaten
Titel
Kinematics and dynamics of planar mechanisms reinterpreted in rigid-body’s configuration space
verfasst von
Raffaele Di Gregorio
Publikationsdatum
04.08.2015
Verlag
Springer Netherlands
Erschienen in
Meccanica / Ausgabe 4/2016
Print ISSN: 0025-6455
Elektronische ISSN: 1572-9648
DOI
https://doi.org/10.1007/s11012-015-0251-8

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