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Jack Hill
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Geplaatst: 17-07-2020 03:37:06 Onderwerp: puma australia |
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ÿþ d i m 3 dZm3 2 d2d3m3 dgm2 J3yy J3== puma australia is the generalizedjoint force vector. r J2== Jzyv Jlzr Jizz; etc.The symbols [ q q ] and [q"] are notation for the n(-l)/Z-vector of C eating Z1 through 1 4 , which are constants of the mecha- nism, leads to a reduction from 35 to 3 multiplications and from[aq]velocity products and the n-vectorof squared velocities. and 18 to 3 additions. Computing the constant Z1 involves 18 calcu- lations. Since the simple parameters required for the calculation[ q 2 ] are given by: of 11 are the input to the RNE, theRNE will effectively carry out The procedure used to derive the dynamimc odel entails four the calculation of Z1 on every pass, producing considerable m-steps: necessary computation.
The first step was carried out with a LISP program, named by the PUMA model can be reduced from 126 to 39 with fourEMDEG, puma shoes which symbolically generates the dynamic model of an equations thathold on the derivatives of the kinetic energy matrixarticulatedmechanism.EMDEGemploys Kane's dynamic for- elements.The first two equationsaregeneral;the last two aremulation [Kane 19681, and produced a result comparable in form specific to the PUMA 560. The equations are:and size to that of ARM [Murry puma suede and Neuman 1984).
Equation ( obtains because the ki-multiply common variable expressions. This is the greatest source netic energy imparted by the velocity of a joint is independent ofof computational efficiency. Looking to the dynamic model of a 3 theconfiguration of thepriorjoints.Equation (9) resultsfromdof manipulator presented in [Murry and Neuman 19841,we see the symmetry of the sixth and terminal link of the PUMA arm.that the kinetic energy matrix element a11 is given by: Andequation (10) holdsbecausethesecond a d third axes of a11 = J322 c o s 2 ( & 83) J a Y y sin2(82 83) JzZr &m3 thePUMAarmareparallel.
puma womens shoes Themotors were mass of thearm. To makethismeasurementourcontrolsys-left installed in linkstwo and three when the inertia of these links tem was configured to command a motor torque proportional towere measured, so the effect of their mass as the supporting links displacement, effecting a torsional spring. By measuring the pe-move is correctly considered. The gyroscopic forces imparted by riod of oscillation of the resultant mass-spring system, the totalthe rotating motor armatures is neglected in the model, but the rotational inertia about each joint was determined. By subtract-data presented below include armature inertia andgear ratios, so ing the arm contributions, determinedfrom direct measurements,these forces can be determined.
ThetolerancevaluesarederivedMeasurement of Rotational Inertia from the precision or smallestgraduation of the measuring in- strument used, or from the repeatability of the measurement it- The two wire suspension shown in Figure1 was used to mea- self. Thetolerancesarereportedwhere the data are presented.surethe I,,, Iyyand I,, parameters of linkstwo and three *. The tolerance values assigned to calculated parameters were de-With this arrangement a rotational pendulum is created about termined by RMS combination of the tolerance assigned to eachanaxisparallel toand halfwaybetween the suspension wires.The link's center of gravity must lie on this axis.
If one is carefulwhenreleasing the link, it Link 2 17.40is possible puma mens shoes to start fundamentalmodeoscillationwithout visi- Link 3 4.80blyexcitingany of the other modes. The relationshipbetween Link 4* 0.82measured properties and rotational inertia is: Link 5* 0.34 Link 6* 0.09 * This method was suggested by Prof. David Powell. Link 3 wiCthomplete LVrist 6.04 Detached Wrist 2.24 * Values derived from external dimensions; f 2 5 % . The positions of the centers of gravity are reported in Table 5. The dimensions rz! ry and rz refer to the x, y and z coordinates 513of the center of gravity in the coordinate frame [img]http://www.simplypotterheads.com/images/lose/puma mens shoes-967raz.jpg[/img] attached t o the Table 5 . Centers of Gravity. |
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