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Aircraft/Generic/wingflexer.nas
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Aircraft/Generic/wingflexer.nas
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# wingflexer.nas - A simple wing flex model.
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#
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# Copyright (C) 2014 Thomas Albrecht
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#
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# This program is free software; you can redistribute it and/or
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# modify it under the terms of the GNU General Public License as
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# published by the Free Software Foundation; either version 2 of the
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# License, or (at your option) any later version.
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#
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# This program is distributed in the hope that it will be useful, but
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# WITHOUT ANY WARRANTY; without even the implied warranty of
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# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU
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# General Public License for more details.
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#
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# You should have received a copy of the GNU General Public License
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# along with this program; if not, write to the Free Software
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# Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301, USA.
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#
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# -->
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# g
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# +-----+ +-----+
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# <--- | m_w |---/\/\/\---| |
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# +-----+ +-----+
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# Lift wing spring fuselage
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# force mass
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#
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# We integrate
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#
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# .. k d . 0.5*F_L ..
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# 0 = -z + --- z + ---- z - ------- - g - z_f
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# m_w m_w m_w
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#
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# where
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#
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# z : deflection
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# k : wing stiffness
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# d : damping
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# m_w = m_dw + fuel_frac * m_fuel
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# Total wing mass. Because the fuel is distributed over the wing, we use
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# a fraction of the fuel mass in the calculation.
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# 0.5*F_L : lift force/2 (we look at one wing only)
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# ..
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# z_f : acceleration of the frame of reference (fuselage)
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#
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# and write the deflection (z + z_ofs) in meters to /sim/model/wing-flex/z-m.
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# The offset z_ofs is calculated automatically and ensures that the dry wing
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# (which still has a non-zero mass) creates neutral deflection.
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#
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# Discretisation by first order finite differences:
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#
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# z_0 - 2 z_1 + z_2 k d (z_0 - z_1) 1/2 F_L ..
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# ----------------- + --- z_1 + --- ----------- - ------- - g - z_f = 0
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# dt^2 m_w m_w dt m_w
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#
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# It is convenient to divide k and d by a (constant) reference mass:
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#
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# K = k / m_dw
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# D = d / m_dw
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#
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# To adapt this to your aircraft, you need m_w, K, D.
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# How to estimate these?
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#
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# 1. Assume a dry wing mass m_dw. Research the wing fuel mass m_fuel.
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#
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# 2. Obtain estimates of
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# - the deflection z_flight in level flight, e.g by comparing photos
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# of the real aircraft on ground and in air,
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# - the wing's eigenfrequency, perhaps from videos of the wing's oscillation in
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# turbulence,
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# - the deflection with full and empty tanks while sitting on the ground.
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#
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# 3. Compute K to match in flight deflection with full tanks:
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# K = g * (m_ac / 2 - (fuel_frac * m_fuel)) / (z_in_flight / z_fac) / m_dw
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#
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# where
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# m_ac : aircraft mass
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# g : 9.81 m/s^2
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# z_fac: scaling factor for the deflection, start with 1.
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#
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# 4. Compute the eigenfrequency of this system for full and empty wing tanks:
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# f_full = sqrt(K * m_dw / (m_dw + fuel_frac * m_fuel)) / (2 pi)
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# f_empty = sqrt(K) / (2 pi)
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#
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# Ideally we want our model to match the eigenfrequency, the deflection
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# while sitting on the ground with full or empty tanks, and the deflection
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# during a hard landing. Getting real-world data for the latter is difficult.
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#
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# There's a python script wingflexer.py which assists you in tuning the parameters.
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#
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# Here are some relations:
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# - a lower wing mass increases the eigenfrequency, and weakens the touchdown bounce
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# - a higher stiffness K reduces the deflection and increases the eigenfrequency
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#
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# The 787 is known for its very flexible wings; the deflection in
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# unaccelerated flight is quoted as z = 3 m. One wing tank of FG's 787-8 holds
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# 23,000 kg of fuel. Because the fuel is distributed over the wing, we use a
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# fraction of the fuel mass in the calculation: fuel_frac = 0.75. For the same reason
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# we don't use the true wing mass, but rather something that makes our model look
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# plausible.
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#
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# So assuming a wing mass of 12000 kg, we get K=25.9 and f_empty = 0.5 Hz.
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# That frequency might be a bit low, videos of a 777 wing in turbulence show about
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# 2-3 Hz. (I didn't research 787 videos).
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#
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# To increase it, we could either reduce m_dw or increase K. A lower m_dw results
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# in a rather weak bounce on touchdown which might look odd. A higher K reduces
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# the deflection z_flight, but we can simply scale the animation to account for
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# that. We'll multiply the deflection z by a factor z_fac to get an angle for the
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# <rotate> animation later on anyway. So repeat 3. and 4. using e.g. z_fac = 10.
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# Now K = 259 and f_empty=2.6 Hz. While our model spring now only deflects
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# to 0.3 m instead of 3 m, the animation scale factor will make sure the wing
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# bends to 3 m. This way, we can match both eigenfrequency and observed deflection,
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# and still get a realistic bounce on touch down. Finally, adjust D such that an
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# impulse is damped out after about one or two oscillations; D = 12 seems to work
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# OK in our example.
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#
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# It's difficult to get real-world data on the deflection during touchdown.
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# Touchdown at more than 10 ft/s is considered a hard landing. There's a video of
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# a hard landing of an A346 (http://avherald.com/h?article=471e70e9), showing the
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# wings bend perhaps 1 m. But I couldn't find any data for the acceleration over
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# time during a hard landing.
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#
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# To assist you in tuning parameters for the touchdown bounce we can give our
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# wing mass the touchdown vertical speed via /sim/model/wing-flex/sink-rate_fps.
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#
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# Our model outputs the deflection in meters, but the <rotate> animation expects an
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# angle. It is up to you calculate an appropriate factor, depending on your wing
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# span and number of segments in the animation. Also don't forget to include z_fac.
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#
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# To use this with your JSBSim aircraft, use
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#
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# io.include("Aircraft/Generic/wingflexer.nas");
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# WingFlexer.new(1, K, D, mass_dry_wing_kg,
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# fuel_fraction, fuel_node_left, fuel_node_right);
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#
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# with apropriate parameters.
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#
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# Yasim does not write the lift to the property tree. But you can create a helper
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# function which computes the lift as
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# lift_force_lbs = aircraft_weight_lbs * load_factor - total_weight_on_wheels_lbs
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# and write lift_force_lbs to /fdm/jsbsim/forces/fbz-aero-lbs (or another location
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# passed to WingFlexer.new() as lift_node).
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#
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# TODO
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# - write Yasim helper
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# - perhaps use analytical solution of ODE
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# - input for fuselage acceleration should rather be acceleration at CG -- find property
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io.include("Aircraft/Generic/updateloop.nas");
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var WingFlexer = {
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parents: [Updatable],
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# FIXME: these defaults make the 787-8 wing flex look realistic, which is certainly not
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# the most generic airliner wing. Once someone obtains a set of parameters for e.g.
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# the 777, use them here.
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new: func(enable = 1, K=259., D=12., mass_dry_wing_kg = 12000., fuel_fraction = 0.75,
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fuel_node_left = "consumables/fuel/tank/level-kg",
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fuel_node_right = "consumables/fuel/tank[1]/level-kg",
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node = "sim/model/wing-flex/", lift_node = "fdm/jsbsim/forces/fbz-aero-lbs") {
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var m = { parents: [WingFlexer] };
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m.node = node;
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m.m_dw = mass_dry_wing_kg;
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m.k = K * m.m_dw;
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m.d = D * m.m_dw;
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m.fuel_frac_on_2 = fuel_fraction / 2.; # so we don't have to divide each frame
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m.fuel_node_left = fuel_node_left;
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m.fuel_node_right = fuel_node_right;
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m.lift_node = lift_node;
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m.loop = UpdateLoop.new(components: [m], enable: enable);
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return m;
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},
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reset: func {
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me.z = 0.;
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me.z1 = 0.;
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me.z2 = 0.;
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setprop(me.node ~ "z-m", 0.);
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setprop(me.node ~ "mass-wing-kg", me.m_dw);
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setprop(me.node ~ "K", me.k/me.m_dw);
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setprop(me.node ~ "D", me.d/me.m_dw);
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setprop(me.node ~ "fuel-fac", me.fuel_frac_on_2 * 2);
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setprop(me.node ~ "sink-rate_fps", 0.);
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me.g_on_2_times_LB2KG = getprop("/environment/gravitational-acceleration-mps2") / 2. * globals.LB2KG;
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me.calc_z_ofs();
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setlistener(me.node ~ "mass-wing-kg", func(the_node) {
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me.m_dw = the_node.getValue();
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me.calc_z_ofs();
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}, 0, 0);
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setlistener(me.node ~ "K", func(the_node) {
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me.k = the_node.getValue() * me.m_dw;
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me.calc_z_ofs();
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}, 0, 0);
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setlistener(me.node ~ "D", func(the_node) { me.d = the_node.getValue() * me.m_dw; }, 0, 0);
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setlistener(me.node ~ "fuel-fac", func(the_node) { me.fuel_frac_on_2 = the_node.getValue() / 2.; }, 0, 0);
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# The following helped me getting wing flex look OK. It's no longer
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# needed once you get the parameters right, so it's disabled by default.
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# Look for DEV to re-enable.
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# Include z-fac here, so you don't have to adjust the animation .xml
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# setprop(me.node ~ "z-fac", 3.);
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# me.last_dt = 1/30.;
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# me.max_z = 0.;
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# setlistener(me.node ~ "sink-rate_fps", func(the_node) {
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# var dz = me.last_dt * the_node.getValue() * globals.FT2M;
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# me.z0 = me.z1 - dz;
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# me.z2 = me.z1 + dz;
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# me.max_z = 0.;
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# }, 1, 0);
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},
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calc_z_ofs: func() {
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print ("wingflex: calc z_ofs");
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me.z_ofs = getprop("/environment/gravitational-acceleration-mps2") * me.m_dw / me.k;
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},
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update: func(dt) {
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# limit time step to avoid numerical instability
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if (dt > 0.2) dt = 0.2;
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# DEV:
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# me.last_dt = dt;
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# fuselage z (up) acceleration in m/s^2
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# we get -g in unaccelerated flight, and large negative numbers on touchdown
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var a_f = getprop("accelerations/pilot/z-accel-fps_sec") * globals.FT2M;
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# lift force. Convert to N and use 1/2 (one wing only)
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var F_l = getprop(me.lift_node) * me.g_on_2_times_LB2KG;
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# compute total mass of one wing, using the average fuel mass in both wing tanks.
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# The averaging factor 0.5 is lumped into fuel_frac_on_2
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me.m = me.m_dw + me.fuel_frac_on_2 * (getprop(me.fuel_node_left) + getprop(me.fuel_node_right));
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# integrate discretised equation of motion
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# reverse sign of F_l because z in JSBsim body coordinate system points down
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me.z = (2.*me.z1 - me.z2 + dt * ((me.d * me.z1 + dt * (-F_l - me.k * me.z1))/me.m + dt *
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a_f)) / (1. + me.d * dt / me.m);
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me.z2 = me.z1;
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me.z1 = me.z;
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me.z += me.z_ofs;
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# output to property
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setprop(me.node ~ "z-m", me.z);
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# DEV: scale output and log max deflection
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# var z_fac = getprop(me.node ~ "z-fac");
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# if (me.z * z_fac < me.max_z) me.max_z = me.z * z_fac;
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# print (sprintf(" z %4.2f max %4.2f m %7.1f", me.z * z_fac, me.max_z, me.m));
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# setprop(me.node ~ "z-m", me.z * z_fac);
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},
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enable: func { me.loop.enable() },
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disable: func { me.loop.disable() },
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};
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