In both planes and birds, different wing shapes yield
different types of flight. The Global Hawk surveillance
drone, like the albatross, has wings that are long,
thin, and narrow, ideal for long-distance, low-speed
flight. Planes that need to maneuver at high speeds,
like the F-16 Fighting Falcon, have stubbier, swept-back
wings, which produce enough lift but with less drag.
Eagles and hawks, likewise, have shorter wings for
greater agility.
But birds and planes control their flight very
differently. Conventional airplanes maneuver by means of
moving surfaces: flaps and ailerons on the wings,
horizontal sections called elevators on the tail, and
also the rudder. Birds, on the other hand, can bend,
twist, and deform their wings and bodies to turn, change
their speed, and adapt to unforeseen conditions such as
wind gusts. If planes could do the same, they would have
more lift and less drag, gaining agility and consuming
less fuel.
We studied the wings of various birds in search of an
appropriate model for our aircraft. Hawks and eagles
looked promising, but what really grabbed our attention
was the pteranodon, a carnivorous pterosaur that soared
through the skies more than 75 million years ago. With
membranous wings each nearly 5 meters long, this animal
was a formidable glider.
But was that the ideal wing shape for us? To find out,
we turned to a computer program called Wind. Created by
researchers at the Air Force's Arnold Engineering
Development Center, NASA's Glenn Research Center, and
Boeing, Wind is a computational fluid dynamics program
that lets you simulate an airplane's wing—or, more
accurately, its airfoil, the shape characterized by its
teardrop cross section—under varying conditions.
From our studies, we needed a thin and slightly curved
airfoil that would approximate that of a pteranodon
wing. Consulting databases that catalog thousands of
existing airfoils, we found a few with the right
profile, bearing the code names Selig 1091, Selig 1223,
and Eppler 378. Using Wind, we simulated each airfoil
for high-altitude flight at relatively low velocities of
up to 64.6 meters per second, or Mach 0.19. The analysis
produced two parameters that are essential in any
aircraft design: the lift coefficient (which, as the
name implies, is a measure of the wing's ability to push
the aircraft upward) and the drag coefficient (a measure
of unwanted resistance to motion). These two parameters
vary according to the wing's angle of attack, its
front-to-back inclination relative to airflow. It's kind
of like flying a kite: to get it up in the air, you pull
it at an angle to the ground, so as to maximize lift.
When designing an aircraft, then, you study how lift
and drag vary as you angle the airfoil. Our initial
tests showed that for an angle of attack of 10 degrees,
the Selig 1091 has a maximum lift coefficient of 1.5 and
a drag coefficient of 0.05—good enough, aerodynamically
speaking, for our type of aircraft. But our plane, like
a bird, will constantly change how it angles its wings
forward, so we had to study our wing's aerodynamics over
a wide range of angles.
Before we settle on a final airfoil, we'll also test
two- and three-dimensional computer models, as well as
actual scale models in a wind tunnel, simulating myriad
steady-state and turbulent conditions as the plane
flaps, glides, and soars.
Flapping-wing
airplanes, sometimes called ornithopters,
have fascinated humanity for centuries. Leonardo da
Vinci proposed a few such designs, to be powered by a
human, but whether they were built remains unknown. More
recently, inventors have successfully demonstrated both
small and large ornithopters. A team at the University
of Toronto, for example, developed an ingenious flapping
plane, powered by an internal-combustion engine, that
even carries a pilot on board.
Despite such successes, we decided to depart
altogether from traditional aircraft design paradigms.
In most planes, the wing is a cantilevered framework
covered by metal plates that give the wing its
aerodynamic shape. We rejected the framework structure
in favor of layering together different materials to
form a compact, nonhollow body.
Enter the aforementioned ionic polymer-metal
composite, or IPMC. Outwardly, it looks like ordinary
plastic, but its core is made of perfluorinated sulfonic
acid, a compound that works as an ion-exchange membrane:
when exposed to an electric field of a few tens of volts
per millimeter, it allows water molecules and hydrated
ions to migrate across it. This flow of water and ions
creates internal forces that make one side of the sheet
expand and the other contract, resulting in a bending
motion. The deformation is proportional to the electric
field's strength, and once the field is removed, the
sheet returns to its original shape.
The solid-state aircraft will have wing-shaped sheets
of the material sandwiched between two metal grids: an
anode grid on the bottom and a cathode grid on top, each
containing thousands or even tens of thousands of
electrodes. A computer control system will supply
voltage to the electrodes. By applying different voltage
levels to different portions of the sheet, we can make
it change its shape to flap. Our hope is that with a
very fine grid we'll be able to emulate the wings of
flying vertebrates.
We're far from that level of control. In our first
test, we started small, with two 5-centimeter-long IPMC
strips. We then attached control electrodes to each
little wing and applied a variable voltage. It was
fascinating to see this primitive contraption beating
its wings fairly well, even at high flapping rates.