Page 224 - Robotics Designing the Mechanisms for Automated Machinery
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212                           Transporting Devices

        In Table 6.1 we see the ratios for several numbers of slots in the driven links.
           Any other mechanism that provides interrupted rotation can obviously also be used
        for driving the drum. We will consider some possibilities in the next section of this
        chapter while discussing the drives of circular transporting devices.
           Attention must be paid to the fact that conveyor-type transporting devices consume
        a great deal of power just to move the mass of the chain or belt, etc. Obviously, this
        power is in essence useless, and one must reduce such power losses. One way would
        be to find a chainless solution, where the additional masses moving together with the
        part or body being treated are minimal. Figure 6.9 represents one such solution. This
        device consists of two systems of mechanical pushers, one immovable 1 and the second
        2 moving. The pushers are provided with a set of pawls 3 actuated by springs 4. The
        moving pusher slides in guides 5 and is driven by, say, a pneumocylinder 6. Blanks 7
        are located on the machine table 8. The mechanism operates as follows. Cylinders 6
        (or any other drive—electromagnetic, mechanical, etc.) pull pusher 2 rightward to the
        position shown in the figure. Then pawls 3 of this pusher are retracted into the body
        of the pusher due to their inclined back face (the blanks press against the pawls and
        overcome the force of spring 4). At the same time pawls 3 of immovable pushers 1 stay
        extended and keep the blanks in their places (the straight front faces of the pawls
        prevent "retreat" of the blanks). The second stage of operation begins with the reverse
        movement of cylinder 6. Then, pawls 3 of pusher 2 push the blanks leftward, while
        pawls 3 of immovable pushers 1 now (because of the inclined faces of the pawls) do
        not prevent displacement of the blanks. Obviously, as a result of this reciprocating
        movement of element 2, all blanks on table 8 are moved by one pitch of the system.
        The resting time of the blanks is not restricted, and the control mechanism can be
        tuned as necessary. The time in motion depends on the dynamic parameters of the
        system and can be estimated during design.
           Another approach for an analogous task is presented in Figure 6.10. This mecha-
        nism also consists of two systems. One keeps blanks 1 in their positions during pro-
        cessing. This system consists of shaft 2 rotating in bearings 3 provided with clamps 4
        and lever 5 driven by pneumocylinder 6 (or some other drive). Thus, shaft 2 is only
        able to rotate in its bearings. The other system must move the blanks and consists of
        shaft 7 that can both rotate and slide in guides 8, and which has pawls 9. Shaft 7 is
        rotated by cylinder 10 through lever 11 and key 12. The reciprocating motion of this
        shaft is provided by cylinder 13 through cross-piece 14. The connection between the



        TABLE 6.1 Time components ratios on the output of the Geneva
        mechanism for different numbers of slots on driven link.

         Z     T 2/T     TZ/TT.
        3      0.167    0.200
        4      0.250    0.333
         5     0.300    0.429
        6      0.333    0.500
        7      0.357    0.555
        8      0.375    0.600
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