<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AJOR</journal-id><journal-title-group><journal-title>American Journal of Operations Research</journal-title></journal-title-group><issn pub-type="epub">2160-8830</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ajor.2014.44019</article-id><article-id pub-id-type="publisher-id">AJOR-47677</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>PHYSICS &amp; MATHEMATICS</subject></subj-group></article-categories><title-group><article-title>Dynamic Model of Flying Machines with the Autopilot</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Toghrul</surname><given-names>Karimli</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Azerbaijan National Academy of Aviation, Baku, Azerbaijan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>tkarimli@mail.ru</email></corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>07</month><year>2014</year></pub-date><volume>04</volume><issue>04</issue><fpage>197</fpage><lpage>201</lpage><history><date date-type="received"><day>25</day>	<month>May</month>	<year>2014</year></date><date date-type="rev-recd"><day>27</day>	<month>June</month>	<year>2014</year>	</date><date date-type="accepted"><day>4</day>	<month>July</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>The article considers negative effects of mechanical oscillations of a
fuselage on the flying machine autopilot. The dynamic model of control system
of flight is made which provides stability and compensates the mechanical
oscillations arising in flight of flying machine with the autopilot.</p></abstract><kwd-group><kwd>Flying Machine</kwd><kwd> Autopilot</kwd><kwd> Dynamic Model</kwd><kwd> Transfer Functions</kwd><kwd> Deviation</kwd><kwd> Control</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Autopilot comprises closed loop systems providing control about one or more of the flying machine’s (FM) primary axes (roll, pitch and yaw). The function of an autopilot is to provide a means of automatically control- ling an FM thus relieving the pilot from the manual tasks of flying the FM for long periods. With the autopilot engaged, the pilot selects the required flight conditions and monitors the functioning of the autopilot in achiev- ing the tasks. Autopilots employ closed loop control systems which sense deviations from steady flight and ap- ply corrections via the flying controls to the rate of deviation [<xref ref-type="bibr" rid="scirp.47677-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.47677-ref2">2</xref>] .</p><p>Carried out researches when air speed of flying machine (FM) changes the occurrence of mechanical oscilla- tions on fuselage is considered to be one of the disadvantages while solving operational tasks in flight performed on autopilot [<xref ref-type="bibr" rid="scirp.47677-ref3">3</xref>] .</p></sec><sec id="s2"><title>2. Proposed Approach</title><p>Among these mechanical oscillations the first harmonic is the most effective. Recurrence of this harmonic is ra- ther small, but its amplitude is quite big. To eliminate this problem stabilizing gyrocompass was used on FM with autopilot, and the system of automated control of FM stabilized by gyrocompass was developed [<xref ref-type="bibr" rid="scirp.47677-ref4">4</xref>] . The block diagramme of such control system is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><fig id="fig1"><label>Figure 1</label><caption><p> The general block-diagramme of simplified dynamic model of aircraft with the autopilot</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\6437dbc2-fdc6-4bbc-8480-1cc5a69dbf45.png"/></fig><p>Transfer functions of links of the block diagramme [<xref ref-type="bibr" rid="scirp.47677-ref5">5</xref>] are resulted as following.</p><p>Taking into consideration the first harmonic of mechanical oscillations arising during flight transfer function of the FM can be written down in the following form:</p><disp-formula id="scirp.47677-formula153"><label>(1)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\be59bbf7-4a93-44dd-be1f-dabb2665ab2f.png"/></disp-formula><p>Part of the block diagramme in <xref ref-type="fig" rid="fig1">Figure 1</xref>, concerning to this transfer function is shaded. The transfer function of the rudder is:</p><disp-formula id="scirp.47677-formula154"><label>(2)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\fcf5099d-e731-46aa-8302-b668038bfb7e.png"/></disp-formula><p>The transfer function of stabilizing gyroscope which is dampering mechanical oscillations arising in a fuse- lage is:</p><disp-formula id="scirp.47677-formula155"><label>(3)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\034f9629-7566-49d4-9889-7c2a22ea8adc.png"/></disp-formula><p>Transfer function of a gyroscope defining a course is:</p><disp-formula id="scirp.47677-formula156"><label>(4)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\04daa0b3-742b-4818-bb6b-f67309027587.png"/></disp-formula><p>Transfer functions of the correcting devices are:</p><disp-formula id="scirp.47677-formula157"><label>(5)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\b38d0bd3-d2e4-4d5f-b5f8-9a91ebef18f9.png"/></disp-formula><p>Transfer functions of the amplifier is:</p><disp-formula id="scirp.47677-formula158"><label>(6)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\a97566df-4b82-4aa1-93db-63f950aa6801.png"/></disp-formula><p>For formation of the closed-loop system the following equation is used:</p><disp-formula id="scirp.47677-formula159"><label>(7)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\29e92a3f-c33e-444b-96d4-bfcd12771448.png"/></disp-formula><p>Transfer function of the converter is:</p><disp-formula id="scirp.47677-formula160"><label>(8)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\11ba6686-b5b4-4b5e-aabe-f77cedb09b8d.png"/></disp-formula><p>In <xref ref-type="fig" rid="fig1">Figure 1</xref> is shown the scheme of automatic control of the FM with the autopilot. Using transfer functions of elements it is possible to write down the general transfer function concerning the simplified block dia- gramme.</p><p>To receive the general transfer function we must accept some simplifications [<xref ref-type="bibr" rid="scirp.47677-ref3">3</xref>] :</p><disp-formula id="scirp.47677-formula161"><label>(9)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\d586192c-7728-48fa-97b9-ddc809787623.png"/></disp-formula><disp-formula id="scirp.47677-formula162"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\ef29ecc9-3e8a-4950-98d4-2febb43eaef6.png"/></disp-formula><disp-formula id="scirp.47677-formula163"><label>(10)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\2a3850c8-263b-415b-9ac5-3f446c65ebc8.png"/></disp-formula><disp-formula id="scirp.47677-formula164"><label>(11)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\260336b8-96c7-4ead-bbe3-f5df74e2b845.png"/></disp-formula><disp-formula id="scirp.47677-formula165"><label>(12)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\718bcd53-617f-47f1-a6e3-1914ea13a53e.png"/></disp-formula><disp-formula id="scirp.47677-formula166"><label>(13)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\1ad618ea-188c-4a04-9bb5-f4828941f349.png"/></disp-formula><disp-formula id="scirp.47677-formula167"><label>(14)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\5c64a4df-37fd-4164-bf32-8a8f5000c439.png"/></disp-formula><disp-formula id="scirp.47677-formula168"><label>(15)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\6300690f-9960-472e-a075-55da4b262da7.png"/></disp-formula><disp-formula id="scirp.47677-formula169"><label>(16)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\6f26035c-34d1-4354-a70c-0d5a548fe532.png"/></disp-formula><p>Equation (16) expresses dynamic model of a flight control which provides stability and compensates mechani- cal oscillations arising during flight of the FM with the autopilot.</p><p>The compensating system works as in parallel connected proof-reader to a fuselage. After synthesis of a reg- ulator of the most compensating system it turns to an inertial element of the first order:</p><disp-formula id="scirp.47677-formula170"><label>(17)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\19b2e85e-ef8c-4097-9e12-7234744e55be.png"/></disp-formula></sec><sec id="s3"><title>3. Numerical Results</title><p>On the basis of approximate data and calculations the structural model of the FM with compensating system in MATLAB program environment is made [<xref ref-type="bibr" rid="scirp.47677-ref4">4</xref>] :</p><disp-formula id="scirp.47677-formula171"><label>(18)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\d3ac8d33-94c2-4f2a-a42f-573bc345810e.png"/></disp-formula><disp-formula id="scirp.47677-formula172"><label>(19)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\6ea57885-191e-459c-8495-6ac7354053e3.png"/></disp-formula><p>After simulation of structural model following features are revealed. At oscillations with harmonics:</p><disp-formula id="scirp.47677-formula173"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\ee537746-8fea-4fe6-91d7-d4fab91ad655.png"/></disp-formula><disp-formula id="scirp.47677-formula174"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\ee537746-8fea-4fe6-91d7-d4fab91ad655.png"/></disp-formula><p>the steady condition of the FM can be kept with amplifier<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\83d4255c-2d91-4fc7-a9f2-8b8886fec152.png" xlink:type="simple"/></inline-formula>, reducing its factor from 1.2 to 0.8.</p><p>Simulations at oscillations above<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\caba96b0-1d39-491c-a59e-92e04c88a206.png" xlink:type="simple"/></inline-formula>:</p><p>All told are visually given on <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>should join automatically compensating system and the action counteracts increase in oscillations to destructive value.</p><p>All told are visually given on <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p></sec><sec id="s4"><title>4. Conclusion</title><p>A control strategy has been proposed to stabilize the FM at autonomous hovering. Some values of amplitude arising oscillations can be kept without connection of compensating system. It is necessary to reduce a target</p><fig-group id="fig2"><caption><title>Figure 2</title><p> Curves received from simulation of flying object with compensating system. (a) Regulation without com- pensating system; (b) Inclusion of compensating system</p></caption><fig id ="fig2_1"><label>(a) (b)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\9fad33f4-15d0-4334-9b53-6672f4f7df48.png"/></fig></fig-group><p>signal of the amplifier of the rudder. At oscillations with harmonics<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\10c6e6ee-36bd-4ab4-a6fa-db6735d94c2e.png" xlink:type="simple"/></inline-formula>, the steady condition of the FM can be kept with amplifier<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\2700c6fb-1424-4b19-bc8e-ce16263f915f.png" xlink:type="simple"/></inline-formula>, reducing its factor from 1.2 to 0.8. At oscillations above <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1040320x\24aba8d6-ff21-4567-942f-e1b4c2128673.png" xlink:type="simple"/></inline-formula> should join automatically compensating system and the action counteracts increase in oscillations to destructive value.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.47677-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">JOINT AVIATION AUTHORITIES, AIRLINE TRANSPORT PILOT LICENCE (2001) THEORETICAL KNOWLEDGE MANUAL, INSTRUMENTATION: OXFORD AVIATION. FRANKFURT, 662 P.</mixed-citation></ref><ref id="scirp.47677-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">EMPRESA BRASILEIRA DE AERONÁUTICA (EMBRAER) (2011) AIR TRANSPORT ASSOCIATION 22—AUTO FLIGHT: MAINTENANCE TRAINING MANUAL, REV. 2. EMBRAER S.A. 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