Kinematic and Dynamic Analysis of Spatial Six Degree of Freedom ...
Kinematic and Dynamic Analysis of Spatial Six Degree of Freedom ...
Kinematic and Dynamic Analysis of Spatial Six Degree of Freedom ...
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~ ~ ~ ~ ~ ~<br />
Let Ei ( Li<br />
, M i,<br />
Ni<br />
) <strong>and</strong> Ek ( Lk<br />
, M k , Nk<br />
) be two unit screws positioned arbitrarily in<br />
~ ~ ~<br />
space. A third unit screw E j ( L j , M j , N j ) , perpendicular to both E i <strong>and</strong> E k , thus E j lies on<br />
the line <strong>of</strong> shortest distance between E i <strong>and</strong> E k as shown in figure 2.5.<br />
Figure 2.5 – Three recursive screws in space<br />
In figure 2.5, the dual angles between E i , j E <strong>and</strong> Ek are given by 2 / π<br />
α = + = A ij ij waij<br />
( a = 0),<br />
A jk = α jk + wa jk = π / 2 ( a jk = 0),<br />
A ki = α ki + waki<br />
where αki is the twist angle <strong>and</strong><br />
ij<br />
e k<br />
// e i<br />
// n<br />
ei<br />
n<br />
αki<br />
αkn<br />
a ki is the shortest distance between screw axis E i <strong>and</strong> E k .<br />
~ ~ ~<br />
~ ~ ~<br />
Now, the recurrent screw equations to find E k ( Lk<br />
, M k , Nk<br />
) from E i ( Li<br />
, M i,<br />
Ni<br />
) <strong>and</strong><br />
~ ~ ~<br />
E j ( L j,<br />
M j , N j ) will be created. First <strong>of</strong> all we will describe the recurrent equations for unit<br />
vector ek ( Lk<br />
, M k , Nk<br />
) using known vectors ei ( Li<br />
, Mi<br />
, Ni<br />
) <strong>and</strong> e j ( L j,<br />
M j,<br />
N j ) . To have only<br />
e j<br />
aki<br />
21