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Design and Analysis of Kinematic Couplings for Modular Machine ...

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y Fball= ( b 3 – b 2 ) × z Fball. (3.7)Hence, the coordinates <strong>of</strong> ball 2 in F ball are (x, y, z) = (0,0,0) <strong>and</strong> <strong>of</strong> ball 3 are:b 3 = ( 0, b 1 – b 2 , 0). (3.8)To find the coordinates <strong>of</strong> ball 1 in F ball , use dot products:x 1 Fball, = ( b 2 – b 1 ) ⋅ ( b 3 – b 2 )<strong>and</strong> (3.9)y 1 Fball, = ( b 2 – b 1 ) ⋅ y Fball. (3.10)Next, the origin <strong>of</strong> F ball is shifted to the location <strong>of</strong> the coupling centroid. Specifically, the couplingcentroid is the point <strong>of</strong> intersection between two lines starting at the coupling locations <strong>and</strong> bisecting therespective angles <strong>of</strong> the coupling triangle. Hence, the coupling centroid is the solution <strong>of</strong> a system <strong>of</strong> twolinear equations in the x-y plane <strong>of</strong> F ball , each derived from applying the law <strong>of</strong> cosines to the trianglegeometry. The included angles <strong>of</strong> the coupling triangle are:⎛ ( b 2 – b 1 ) 2 + ( b 3 – b 2 ) 2 – ( b 3 – b 1 ) 2⎞θ 13 = acos⎜-------------------------------------------------------------------------------------------------⎟⎝ 2 ( b 3 – b 2 ) ( b 2 – b 1 ) ⎠<strong>and</strong> (3.11)⎛ ( b 3 – b 1 ) 2 + ( b 3 – b 2 ) 2 – ( b 2 – b 1 ) 2⎞θ 12 = acos⎜-------------------------------------------------------------------------------------------------⎟. (3.12)⎝ 2 ( b 3 – b 2 ) ( b 2 – b 1 ) ⎠And the pair <strong>of</strong> linear equations (suitably between any two balls), expressed relative to F ball , is:θy 13C–ball =tan⎛ ------⎞ xC . (3.13)⎝ 2 ⎠ – ballθy 12C–ball = tan ------⎛ ⎞( xC⎝ 2 ⎠ – ball – ( b 3 – b 2 ) ). (3.14)From this solution, the location <strong>of</strong> the coupling centroid in F ball as initially placed at b 2 is denoted as(x C-ball , y C-ball, 0). Note that even under perturbations in the vertex locations, which make the triangle nolonger equilateral or isosceles, the angle bisectors <strong>of</strong> a triangle always intersect at a point; hence the intersection<strong>of</strong> the bisectors originating at balls 2 <strong>and</strong> 3 defines the in-plane location <strong>of</strong> the coupling centroid.Now, sufficient in<strong>for</strong>mation has been derived to calculate the HTM between the measurement system<strong>and</strong> the coupling interface. When the axis vectors <strong>of</strong> F ball expressed in F MS are normalized to unit vectors,50

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