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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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