Report of the Second Piloted Aircraft Flight Control System - Acgsc.org
Report of the Second Piloted Aircraft Flight Control System - Acgsc.org
Report of the Second Piloted Aircraft Flight Control System - Acgsc.org
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The solution to equation (11) , is<br />
iB<br />
The term Ae is a vector quantity having an' amplitude A and<br />
a phase angle fd. From equation (12)<br />
High frequency amgUtude attenuation. - At no-load <strong>the</strong> piston velocity<br />
is at all times proportional to <strong>the</strong> valve opening; <strong>the</strong>refore in <strong>the</strong><br />
response to a sinusoidal input at no-load <strong>the</strong> pilot valve area is zero<br />
at <strong>the</strong> ends <strong>of</strong> <strong>the</strong> output travel (<strong>the</strong> velocity 'being zero). Under an<br />
inertia load <strong>the</strong> piston velocity is not linearly proportional to <strong>the</strong><br />
pilot valve opening and hence in <strong>the</strong> response to a sinusoidal input <strong>the</strong><br />
valve area is not necessarily zero at <strong>the</strong> ends <strong>of</strong> <strong>the</strong> output travel. If<br />
at high frequencies, <strong>the</strong> response <strong>of</strong> <strong>the</strong> servomotor is assumed to be<br />
essentially sinuaoidal, <strong>the</strong> maximum acceleration can be considered to<br />
occur at <strong>the</strong> Limits <strong>of</strong> <strong>the</strong> output travel and hence when <strong>the</strong> piston veloc-<br />
ity ie zero. Under <strong>the</strong> condition <strong>of</strong> negligible mass <strong>of</strong> <strong>the</strong> hydraulic<br />
fluid, <strong>the</strong> pressure difference across <strong>the</strong> piston at any instant when <strong>the</strong><br />
piston velocity is zero and <strong>the</strong> pilot valve area is greater than zero,<br />
is <strong>the</strong> pressure difference acrose <strong>the</strong> servomotor. Above some frequency<br />
<strong>the</strong> system may <strong>the</strong>n be approximated by a Unear system wherein <strong>the</strong> preseure<br />
difference across <strong>the</strong> piston varies sinurroidally with an amplitude<br />
<strong>of</strong> (P,-P~) and with <strong>the</strong> frequency <strong>of</strong> <strong>the</strong> input. On <strong>the</strong> baeie <strong>of</strong> this<br />
app~oximetion <strong>the</strong> acceleration <strong>of</strong> <strong>the</strong> piston is<br />
Integrating equation (15) and introducing <strong>the</strong> condition that x<br />
varies about zero and neglecting changes in sign