<table><tbody><tr><th>Quantity</th><th>Unit Price</th></tr><tr><td>1</td><td>$4001</td></tr><tr><td>2</td><td>$3801</td></tr><tr><td>5</td><td>$3401</td></tr><tr><td>10</td><td>$3201</td></tr><tr><td>25</td><td>$2801</td></tr><tr><td>50</td><td>$2601</td></tr><tr><td>100</td><td>$2200</td></tr></tbody></table>
<table><tbody><tr><th>Quantity</th><th>Unit Price</th></tr><tr><td>1</td><td>$4001</td></tr><tr><td>2</td><td>$3801</td></tr><tr><td>5</td><td>$3401</td></tr><tr><td>10</td><td>$3201</td></tr><tr><td>25</td><td>$2801</td></tr><tr><td>50</td><td>$2601</td></tr><tr><td>100</td><td>$2200</td></tr></tbody></table>
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 10 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>8000</td><td>µm</td></tr><tr><td>Nominal Travel, -30V to 150V</td><td>10000</td><td>µm</td></tr><tr><td>Nominal Stiffness</td><td>0.002</td><td>N/µm</td></tr><tr><td>Unloaded Resonant Frequency</td><td>70</td><td>Hz</td></tr><tr><td>Blocked Force*</td><td>16</td><td>N</td></tr><tr><td>Capacitance</td><td>26.4</td><td>µF</td></tr><tr><td>Material</td><td>Titanium</td><td></td></tr><tr><td>Mass**</td><td>320</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>106</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