The Art of the Helicopter John Watkinson - Karatunov.net
The Art of the Helicopter John Watkinson - Karatunov.net
The Art of the Helicopter John Watkinson - Karatunov.net
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Technical background 57<br />
<strong>the</strong> inertia <strong>of</strong> <strong>the</strong> system that determine <strong>the</strong> maximum slew rate. Figure 2.23 showed<br />
<strong>the</strong> effect <strong>of</strong> different damping factors on system response. In <strong>the</strong> case <strong>of</strong> a servo <strong>the</strong><br />
amount <strong>of</strong> velocity feedback determines <strong>the</strong> damping factor. With little or no velocity<br />
feedback <strong>the</strong> slew rate will be high, but hunting will be excessive and <strong>the</strong> step response<br />
will be a decaying oscillation. With too much velocity feedback <strong>the</strong> response will have<br />
no overshoot, but will be very slow. In between <strong>the</strong>se is <strong>the</strong> condition known as critical<br />
damping. This is defined as <strong>the</strong> amount <strong>of</strong> damping which gives <strong>the</strong> fastest response<br />
without any overshoot. <strong>The</strong> critical damping condition is simply a definable condition,<br />
and it is not necessarily <strong>the</strong> optimum response. In most cases <strong>the</strong> response speed can<br />
be increased significantly with <strong>the</strong> penalty <strong>of</strong> a very small overshoot.<br />
In an unpowered system, if <strong>the</strong> pilot experiences resistance to a control input, he will<br />
automatically apply more force to obtain <strong>the</strong> desired control position. In a fully powered<br />
system, <strong>the</strong> pilot (or <strong>the</strong> autopilot) does not feel this resistance and cannot compensate.<br />
<strong>The</strong> feedback system must be designed to overcome resistance automatically. In a simple<br />
servo, <strong>the</strong> load will stop at a position where <strong>the</strong> force from <strong>the</strong> motor is balancing <strong>the</strong><br />
disturbing force. Clearly in a simple feedback system, <strong>the</strong> motor can only produce a<br />
force if <strong>the</strong>re is a position error. <strong>The</strong> result is that <strong>the</strong> external force pushes <strong>the</strong> load<br />
out <strong>of</strong> position until <strong>the</strong> position error is large enough to oppose fur<strong>the</strong>r motion. <strong>The</strong><br />
ability <strong>of</strong> a servo to oppose external force in this way is called stiffness.<br />
<strong>The</strong> stiffness <strong>of</strong> a servo can be improved by increasing <strong>the</strong> gain given to <strong>the</strong> position<br />
error. <strong>The</strong>n a given resistance to an external force will be obtained with a smaller position<br />
error. Increasing <strong>the</strong> gain may also speed up <strong>the</strong> step response, but not beyond <strong>the</strong><br />
slew rate limit. If a control input exceeds <strong>the</strong> slew rate limit, for a period <strong>of</strong> time <strong>the</strong><br />
position error will be large and <strong>the</strong> system is not feedback controlled. In this state<br />
<strong>the</strong> system is said to be in an open loop condition.<br />
Clearly high gain is desirable in a servo because it increases response speed and<br />
stiffness. However, high gain can also cause instability. During servo development, a<br />
control input is created which is sinusoidal and <strong>the</strong> frequency is swept upwards from a<br />
very low value. <strong>The</strong> amplitude and phase response are plotted against <strong>the</strong> frequency.<br />
As <strong>the</strong> frequency rises, <strong>the</strong> servo has to work harder to follow <strong>the</strong> rapid movement and<br />
so <strong>the</strong> position error may increase. This causes <strong>the</strong> load to lag <strong>the</strong> input. At some high<br />
frequency, <strong>the</strong> phase lag may reach 180 ◦ .<br />
With a 180 ◦ phase shift, a negative feedback system has turned into a positive feedback<br />
system. In o<strong>the</strong>r words <strong>the</strong> sense <strong>of</strong> <strong>the</strong> correcting action is wrong. If <strong>the</strong> loop<br />
gain is above unity at <strong>the</strong> frequency where <strong>the</strong> phase response has gone to 180 ◦ , <strong>the</strong><br />
system will oscillate at that frequency. This may be spontaneous upon applying power<br />
or result from a small control input. Clearly this would be catastrophic in any control<br />
system. In practice feedback systems must contain a filter to reduce <strong>the</strong> loop gain at<br />
high frequencies to prevent oscillation.<br />
Ano<strong>the</strong>r possibility that allows higher loop gain is to have a signal processor containing<br />
an inverse model <strong>of</strong> <strong>the</strong> phase characteristics <strong>of</strong> <strong>the</strong> servo loop. When <strong>the</strong> servo<br />
loop lags, <strong>the</strong> processor will introduce a phase lead to balance out <strong>the</strong> lag. <strong>The</strong> use <strong>of</strong><br />
<strong>the</strong>se filters and processors in a servo loop is called compensation.<br />
If high gain cannot be used for stability reasons, it is possible to improve <strong>the</strong> accuracy<br />
<strong>of</strong> a servo in <strong>the</strong> long term by integrating <strong>the</strong> error. Figure 2.36 shows a feedback system<br />
with integral control. A small error at <strong>the</strong> input to <strong>the</strong> integrator will become larger<br />
as <strong>the</strong> integrator operates until <strong>the</strong> loop acts to cancel it. Integral control is useful for<br />
overcoming friction in mechanisms.<br />
Feedback loops can be nested which means that one operates inside ano<strong>the</strong>r. For<br />
example, Figure 2.37 shows an automatic navigation system. <strong>The</strong> flight director error<br />
loop provides an error signal to <strong>the</strong> autopilot in order to keep <strong>the</strong> machine on track.