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Experiments with Supersonic Beams as a Source of Cold Atoms

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Figure 3.7: A CAD image <strong>of</strong> the rotor. The rotor h<strong>as</strong> 50.4 cm radius at the center <strong>of</strong><br />

the crystal holder, and a maximum thickness <strong>of</strong> 2.54 cm in the center. The diameter<br />

<strong>of</strong> the rotor itself is linearly tapered from 0.3175 cm where the rotor joins the crystal<br />

holder, to the maximal thickness 2.54 cm from the middle <strong>of</strong> the rotor. The small<br />

hole seen in the middle <strong>of</strong> the rotor allows precise centering <strong>of</strong> the rotor via a pin in<br />

the spindle. A 5 mm diameter crystal (4 mm exposed) is held in place by a set screw.<br />

Figure Courtesy Max Riedel.<br />

Figure 3.8: A finite element calculation <strong>of</strong> the stress exerted on the rotor by rotation<br />

at 140 Hz. This is expressed in MPa, since it is the force per unit area <strong>of</strong> material,<br />

rather than the absolute force, which is relevant. For reference, the peak stress place<br />

on the rotor is only a factor <strong>of</strong> 5 smaller than the yield tensile strength <strong>of</strong> the titanium<br />

alloy used.<br />

36

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