<table><tbody><tr><th>Quantity</th><th>Unit Price</th></tr><tr><td>1</td><td>$3411</td></tr><tr><td>2</td><td>$3240</td></tr><tr><td>5</td><td>$2899</td></tr><tr><td>10</td><td>$2728</td></tr><tr><td>25</td><td>$2387</td></tr><tr><td>50</td><td>$2217</td></tr><tr><td>100</td><td>$1876</td></tr></tbody></table>
<table><tbody><tr><th>Quantity</th><th>Unit Price</th></tr><tr><td>1</td><td>$3411</td></tr><tr><td>2</td><td>$3240</td></tr><tr><td>5</td><td>$2899</td></tr><tr><td>10</td><td>$2728</td></tr><tr><td>25</td><td>$2387</td></tr><tr><td>50</td><td>$2217</td></tr><tr><td>100</td><td>$1876</td></tr></tbody></table>
DSM's LFPA actuators are designed for applications that require a large travel range. The actuators were designed to oscillate specimens in a high magnetic field and are constructed of titanium and other non-ferromagnetic materials. The two-stage amplification enables the design to achieve a travel range of 6 mm at the mechanism's output.
<table ><tbody><tr><td></td><td></td><td>Units</td></tr><tr><td>Motion Direction</td><td>Contracting</td><td></td></tr><tr><td>Nominal Travel, 0V to 150V</td><td>4800</td><td>µm</td></tr><tr><td>Nominal Travel, -30V to 150V</td><td>6000</td><td>µm</td></tr><tr><td>Nominal Stiffness</td><td>0.006</td><td>N/µm</td></tr><tr><td>Unloaded Resonant Frequency</td><td>120</td><td>Hz</td></tr><tr><td>Blocked Force*</td><td>29</td><td>N</td></tr><tr><td>Capacitance</td><td>19.8</td><td>µF</td></tr><tr><td>Material</td><td>Titanium</td><td></td></tr><tr><td>Mass**</td><td>310</td><td>g</td></tr><tr><td>Electrical Interface</td><td>Flying leads</td><td></td></tr><tr><td>Mechanical Interface</td><td>Clearance Holes x4</td><td></td></tr><tr><td>Height</td><td>47</td><td>mm</td></tr><tr><td>Width</td><td>102</td><td>mm</td></tr><tr><td>Depth</td><td>19</td><td>mm</td></tr></tbody></table>
* Blocked force calculated as Stiffness x Travel Range at 0V to 150V
** Mass stated for reference