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Spatial mechanism
Name : Kaustubh S. Garud
Roll. No. 503006
Subject : ASOM
Guided by
Prof. S. T. Chavan
Introduction
• Mechanisms having three dimensional points
paths are called spatial mechanisms.
• If there is any relative motion that is not in the
same plane or in parallel planes, the
mechanism is called the spatial mechanism.
• Mobility of a kinematic chain can be obtained
from the Kutzbatch criterian which is
54321 2345)1(6 jjjjjnm 
• The coordinates of points G2 & G3 is written in
fixed coordinate system o1x1y1z1. The
coordinates of G2 are then
• The coordinates G3 will first be expressed with
respect to the system of axes , where
is parallel to x1 and axes is perpendicular to
both and z4 hence,
0
sin
cos
34
33
33



Gz
aG
aG


4R
4z
4R
44 zR 
• Using this now we can write coordinates of G3
with respect to o1x1y1z1 as
• The distance G2G3 which is equal to a2, so
writing in terms of the coordinates as
• By applications of trigonometric identities and
ordering terms this becomes
Symbolic Equations
• Symbolic notation allows the relative positions
of the axis of a mechanism to be completely
defined by specifying four parameters : a, α,θ
and s between each link and member
• Once the four parameters have been
established for each pair of linkage the
geometry of the linkage is completely
specified, and can be represented by a
symbolic equation of the form
Matrix method
• Once linkage has been described by means of
a symbolic equation, a rectangular coordinate
system is defined on each link.
• A change of coordinate or linear
transformation between adjacent system may
be represented by the 4 X 4 matrix ivolving
the parameters a, α,θ and s of the symbolic
equation.
References
• R. Hartenberg J. Denavit ‘Kinematic Synthesis
of mechanisms’
• Antonio Lopez-Gomez ‘Spatial Mechanisms:
Analysis and Systems’
• Shigley and Uicker ‘Theory of machines and
mechanism’
Thank you

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Spatial mechanism and DH parameters

  • 1. Spatial mechanism Name : Kaustubh S. Garud Roll. No. 503006 Subject : ASOM Guided by Prof. S. T. Chavan
  • 2. Introduction • Mechanisms having three dimensional points paths are called spatial mechanisms. • If there is any relative motion that is not in the same plane or in parallel planes, the mechanism is called the spatial mechanism. • Mobility of a kinematic chain can be obtained from the Kutzbatch criterian which is 54321 2345)1(6 jjjjjnm 
  • 3.
  • 4.
  • 5.
  • 6.
  • 7.
  • 8.
  • 9. • The coordinates of points G2 & G3 is written in fixed coordinate system o1x1y1z1. The coordinates of G2 are then
  • 10. • The coordinates G3 will first be expressed with respect to the system of axes , where is parallel to x1 and axes is perpendicular to both and z4 hence, 0 sin cos 34 33 33    Gz aG aG   4R 4z 4R 44 zR 
  • 11.
  • 12. • Using this now we can write coordinates of G3 with respect to o1x1y1z1 as • The distance G2G3 which is equal to a2, so writing in terms of the coordinates as
  • 13. • By applications of trigonometric identities and ordering terms this becomes
  • 14. Symbolic Equations • Symbolic notation allows the relative positions of the axis of a mechanism to be completely defined by specifying four parameters : a, α,θ and s between each link and member
  • 15.
  • 16. • Once the four parameters have been established for each pair of linkage the geometry of the linkage is completely specified, and can be represented by a symbolic equation of the form
  • 17.
  • 18.
  • 19.
  • 20.
  • 21. Matrix method • Once linkage has been described by means of a symbolic equation, a rectangular coordinate system is defined on each link. • A change of coordinate or linear transformation between adjacent system may be represented by the 4 X 4 matrix ivolving the parameters a, α,θ and s of the symbolic equation.
  • 22.
  • 23.
  • 24.
  • 25.
  • 26.
  • 27.
  • 28. References • R. Hartenberg J. Denavit ‘Kinematic Synthesis of mechanisms’ • Antonio Lopez-Gomez ‘Spatial Mechanisms: Analysis and Systems’ • Shigley and Uicker ‘Theory of machines and mechanism’