📄 aerogrp.htm
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FDC help: Aerodynamics Group (Beaver)
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<h2>
Subsystem <i>Aerodynamics Group (Beaver)</i>
</h2>
<p>The subsystem <i>Aerodynamics Group (Beaver)</i> of the <i><a href="beaver.htm">Beaver</a></i> model contains blocks that determine the aerodynamic
forces and moments for the 'Beaver' aircraft. The block <i><a href=
"dimless.htm">Dimless</a></i> first computes the non-dimensional rotational
velocity components along the aircraft's body-axes. The dimensionless
force and moment coefficients are then calculated in the block <i><a href=
"aeromod.htm">Aeromod (Beaver)</a></i>, which contains the actual
(aircraft-dependent) aerodynamic model, and finally, the real values of
these forces and moments are determined by the block <i><a href=
"fmdims.htm">FMdims</a></i>.</p>
<p>As implied by its name, the subsystem <i>Aerodynamics Group (Beaver)</i>
is only valid for the De Havilland DHC-2 'Beaver', using the
aerodynamic model from <a href="#References">ref.[1]</a>. The internal
structure of similar models for other aircraft may look entirely different.
For instance, in this case the block <i>Dimless</i> is needed, because the
dimensionless rotational velocities are used as helpvariables for the
actual aerodynamic model in <i>Aeromod</i>, whereas aerodynamic models for
other aircraft may require entirely different helpvariables.</p>
<p>For this reason, the internal structure of the subsystem <i>Aerodynamics
Group</i> will <i>always</i> depend upon the aircraft model considered. </p>
<h3>
Inputs: <i>x</i>, <i>uaero</i>, <i>yad1</i>
</h3>
<pre>
x = [V alpha beta p q r psi theta phi xe ye H]' (states)
uaero= [deltae deltaa deltar deltaf]' (aerodyn. control-inputs)
yad1 = [a M qdyn]' (basic airdata variables,
coming from <a href=
"airdata1.htm">Airdata1</a>)
V : true airspeed [m/s]
alpha : angle of attack [rad]
beta : sideslip angle [rad]
p : roll-rate [rad/s]
q : pitch-rate [rad/s]
r : yaw-rate [rad/s]
{psi : yaw-angle [rad] }
{theta : pitch-angle [rad] }
{phi : roll-angle [rad] }
{xe : X-coordinate, relative to Earth-axes [m] }
{ye : Y-coordinate, relative to Earth-axes [m] }
{H : altitude above sea level [m] }
deltae: deflection of elevator [rad]
deltaa: deflection of ailerons [rad]
deltar: deflection of rudder [rad]
deltaf: deflection of flaps [rad]
{a : speed of sound [m/s] }
{M : Mach number [-] }
qdyn : dynamic pressure [N/m^2]
</pre>
<p>The variables which are not actually used by any of the masked subsystems
<i>Dimless</i>, <i>Aeromod (Beaver)</i>, and <i>FMdims</i> have been
displayed between curly braces. </p>
<h3>
Outputs: <i>ydl</i>, <i>Caero</i>, <i>FMaero</i>
</h3>
<pre>
ydl = [pb/2V qc/V rb/2V]' (outputs from <a href=
"dimless.htm">Dimless</a>)
Caero = [CXa CYa CZa Cla Cma Cna]' (outputs from <a href=
"aeromod.htm">Aeromod</a>)
FMaero= [Xa Ya Za La Ma Na]' (outputs from <a href=
"fmdims.htm">FMdims</a>)
CXa, CYa, CZa: dimensionless aerodynamic force coefficients
Cla, Cma, Cna: dimensionless aerodynamic moment coefficients
Xa, Ya, Za : aerodynamic forces [N]
La, Ma, Na : aerodynamic moments [Nm]
</pre>
<h3>
Parameters to be defined in the Matlab workspace
</h3>
<ul>
<li>
<i>GM1</i>: vector with some important geometrical properties of the
'Beaver' aircraft, and the mass of the aircraft (which is
assumed to be constant during the motions of interest). Here, it is
needed by <i>Dimless</i> in order to extract geometrical data.
</li>
<li>
<i>AM</i>: matrix with stability and control derivatives of the
'Beaver' (valid only for the nonlinear aerodynamic model of the
DHC-2 'Beaver', see <a href="#References">ref.[1]</a>). This
matrix is needed by <i>Aeromod (Beaver)</i>.
</li>
</ul>
<p><i>AM</i> and <i>GM1</i> can be loaded into the workspace from datafile by
running the utility <i><a href="datload.htm">DATLOAD</a></i>. Run <i><a
href="modbuild.htm">MODBUILD</a></i> first if the datafile does not yet
exist.</p>
<h3>
<a name="References">References</a>
</h3>
<ol>
<li>
R.T.H. Tjee and J.A. Mulder. <i>Stability and Control Derivatives of
the De Havilland DHC-2 "Beaver" aircraft</i>. Report LR-556,
Delft University of Technology, 1988.
</li>
</ol>
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