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ComputerAided_Design_Engineering_amp_Manufactur.pdf

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FIGURE 9.6<br />

FIGURE 9.7<br />

Geometric Interpretation of Spatial Relationships<br />

A spatial relationship can be interpreted as a constraint imposed on the degrees of freedom between mating<br />

or interacting features. In every mating feature (Nnaji, 1990-1; Nnaji, 1990-2), a mating-coordinate frame<br />

is attached. A mating-coordinate frame is derived to represent the coordinate frame needed for expressing<br />

degrees of freedom. The origin and axes of the mating coordinate frame are determined by mating<br />

condition or degrees of freedom of mating.<br />

In plane feature, a mating-coordinate frame is on the plane with Z-axis<br />

point out of the plane (Figure<br />

9.3(a)). In cylindrical feature, the X-axis<br />

of the mating-coordinate frame is coincident with the center line<br />

(Figure 9.3(b)) and, in spherical feature, the origin of the mating frame is coincident with the center of the<br />

sphere (Figure 9.3(c)). The degrees of freedom between mating components can be geometrically represented<br />

and interpreted in accordance with mating geometry. The element of degrees of freedom to describe spatial<br />

relationships can be described as follows:<br />

1. lin_n:<br />

linear translation along n-axis,<br />

where n contains a fixed point and a vector;<br />

2. rot_n:<br />

rotation about n-axis,<br />

where n contains a fixed point and a vector;<br />

3. plane_n,<br />

cyl_n,<br />

sph:<br />

translating along a planar, cylindrical, or spherical surface, etc.<br />

The degrees of freedom of a part can now be expressed as {degrees of freedom of moving along<br />

the feature of relative mating part :: degrees of freedom of moving the part with respect to itself} ,<br />

where the relative mating part is fixed. For ex<strong>amp</strong>le, in Figure 9.3(b), part p1 is against part p2 over<br />

a line. The degree of freedom for p1 with respect to p2 describes the relative motion that maintains<br />

a line contact. p1 may move along the mating planar face of p2 while maintaining fixed orientation.<br />

This can be described as the equation for an infinite plane, Ax+By+Cz�D.<br />

For p1 itself, p1 can rotate<br />

about the z-axis,<br />

which gives a new orientation about the contact line, and p1 can rotate about x-axis<br />

© 2001 by CRC Press LLC<br />

Incline-offset.<br />

Include-angle.

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