All boomerangs are either right or left-handed - one is an exact mirror image
of the other. This is to allow right and left-handed throwers to launch their
boomerangs with relative ease because it's far more comfortable to throw
away from, rather than across, the body. Having said this, it is possible
to throw an opposite handed boomerang, with a few adjustments to your throwing
action.
During the flight of the boomerang, the effect of many different aerodynamic
principles can be seen. Bernoulli's theorem, Newton's laws of motion, gyroscopic
stability, gyroscopic precession and many others all have a bearing on the
action of the boomerang.
When the boomerang leaves the thrower's hand, it will be spinning very fast.
As each arm of the boomerang has an aerofoil shape, similar in cross-section to
that of an aircraft wing, air moving over the top of each wing has to travel
further, and therefore faster, than air passing beneath the wings. Bernoulli's
theorem states that 'air travelling at a higher speed creates less pressure than
slower moving air'. As a result, the boomerang experiences a 'lift'1 force.
Newton's second law of motion states that 'the rate of change of momentum of
an object is equal to the force applied to that object'. For an object with
constant mass, this reduces to the well-known formula Force applied = Mass x
Acceleration. The force here is a combination of friction and other
resistive forces. To reduce the acceleration (or deceleration, since the force
is negative), the mass needs to be large, but not so large that the boomerang
falls quickly to the ground.
The length of the boomerang's arms, and the angle at which they are joined,
allow the boomerang to spin in a stable plane as a result of the spin imparted
on launching. This is known as gyroscopic stability. If this were not the case,
the motion of the boomerang would at best be unpredictable. At worst, the
boomerang would lose its spin rapidly, and be unable to sustain flight.
We now have a stable, rapidly spinning boomerang, moving forward from the
force of the throw. We now need to take a slightly closer look at the effect of
Bernoulli's theorem. As each wing rotates forward, into the direction of travel,
it creates more lift than the other wing because the relative air speed is
higher. If you imagine the spinning boomerang as a clock face, sideways on, this
leads to the maximum force being created near the 12 o'clock position.
Due to the gyroscopic stability of the spinning boomerang, the effect of this
force manifests itself at 90° further round the cycle of spin - at the 9 o'clock
position of our clock face. The action of this force is to change the direction
of flight - to the left for a right-handed boomerang and vice versa. Compare
this with a 'no hands' bicycle turn - the only difference being the magnitude of
the force. A small force over most of the duration of the flight produces a
large, smooth turn for the boomerang, while a sudden strong force produces an
abrupt bicycle turn.
As the boomerang travels, it loses velocity2. Eventually, gyroscopic precession becomes the
dominant force. Coupled with the initial 'off-vertical' tilt, the effect is to
push the boomerang over on its side, so that it spins in a horizontal plane.
The effect of each of these principles varies with the way in which the
boomerang is thrown. The basic flight path of a boomerang is circular, although
advanced throwers can produce a virtually triangular flight path.