12.07.2015 Views

Design of a Hybrid Positioner-Fixture for Six-axis Nanopositioning ...

Design of a Hybrid Positioner-Fixture for Six-axis Nanopositioning ...

Design of a Hybrid Positioner-Fixture for Six-axis Nanopositioning ...

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

<strong>Design</strong> <strong>of</strong> a <strong>Hybrid</strong> <strong>Positioner</strong>-<strong>Fixture</strong> <strong>for</strong> <strong>Six</strong>-<strong>axis</strong> <strong>Nanopositioning</strong> and Precision FixturingSubmitted to Precision EngineeringStaticCS GrooveDisplacedCSC r 1br 1b||Dyr x zBr 1ar 1cEr A zFigure 5: Detailed view <strong>of</strong> in-plane kinematic model in relationship to kinematic coupling geometry(top component removed <strong>for</strong> clarity). Note the static coordinate system (CS) and displaced CS. Thecoordinate systems lie at the coupling centroid as calculated from the layout <strong>of</strong> the ball positions whenall r ib = 0.For each loop i, Eqxn. 3 represents the two relationships shown in Eqxns. 4 and 5.LLiaiaiaLibcosiaLibsiniaLiccos icXccos || (4)iaLibsiniaLibcosiaLicsin icYcsin || (5)The variables L ij represent the length <strong>of</strong> vector r ij . In this model ic and z are linked by Eqxn. 6, and L iais equal to L ic .ic ia z(6)When Eqxn. 6 is substituted into Eqxns. 4 and 5, L ic is substituted <strong>for</strong> L ia , and we assume small angleapproximations (sin(z c )~ (z c ) and cos(z c )~1), we obtain the matrix equation provided in Eqxn. 7.101010010101 L L L L L L1c1c2c2c3c3c sin cos sin cos sin cos cos1a sin1a 0 cos2a 0 sin2a 00 cos3a 00 sin3a1a1a002a2a00003a3a Xc L1b sin 1a Yc L1b cos1a z c L2b sin2a L1b|| L2b cos2a L 2b||L3b sin3a L3b|| L3b cos 3aSmall angle approximations are appropriate as the second order effects on position due to angle couplingresult in errors on the order <strong>of</strong> 10 -3 – 10 -6 smaller than the displacements <strong>of</strong> interest. The right side <strong>of</strong>Eqxn. 7 consists <strong>of</strong> the actuation inputs, L ib , and geometry variables. This kinematic relationship isdifferent from previous approaches in that it enables the immediate calculation <strong>of</strong> <strong>for</strong>ward and reversekinematic solutions without iteration.(7)6

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!