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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

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