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Kinematic and Dynamic Analysis of Spatial Six Degree of Freedom ...

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From equation (2.6) we have;<br />

or<br />

x<br />

z<br />

ρ<br />

o<br />

e<br />

Figure 2.2 – A unit screw with radius vector<br />

Pi + Qj<br />

+ Rk<br />

= ( Ny − Mz)<br />

i + ( Lz − Nx)<br />

j + ( Mx − Ly)<br />

k<br />

P = Ny − Mz Q = Lz − Nx R = Mx − Ly (2.7)<br />

Equations (2.7) are called as the equations <strong>of</strong> the screw axis, which are the equations<br />

<strong>of</strong> a line in space. The equations <strong>of</strong> the axis <strong>of</strong> a screw in Plücker coordinates are homogenous<br />

wrt. their coordinates. From (2.7) we can write:<br />

( λ N) y − ( λM<br />

) z − ( λP)<br />

= 0<br />

( λ L) z − ( λN)<br />

x − ( λQ)<br />

= 0<br />

( λ M ) x − ( λL)<br />

y − ( λr)<br />

= 0<br />

If (L,M,N,P,Q,R) satisfies the line equations then (λL, λM, λN, λP, λQ, λR) also<br />

satisfies the line equations. Since screw E is unit, E 2 = 1 + w·0, in coordinate form we have:<br />

e<br />

y<br />

E<br />

~ 2 ~ 2 ~ 2<br />

L + N + M = 1+<br />

w ⋅ 0<br />

(2.8)<br />

11

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