Robert Deters wrote:
> Andy Ross wrote:
> > Robert Deters wrote:
> > > Actually the F-4 is unstable, but only marginally.
>
> > Not in pitch, certainly?
>
> Yes in pitch.  Besides, I think you are confusing static stability
> and dynamic stability.

Er, normally one interprets an unqualified use of "stable" as
referring to static stability.  The rest of the conversation has been
about stability augmentation systems (which have to do only with
static stability -- phugoid damping can be done with an autopilot).  I
even went out of my way (two paragraphs worth!)  to point out that I
wasn't talking about the phugoid when we got into this.  Apologies if
I didn't get that across; and apologies for trying to explain to you
stuff that you already knew. :)

For those who are wondering what the difference is: static stability
refers to weathervane behavior.  If you point the aircraft "forward"
(for whatever definition of forward you are using) in an airstream and
then perturb it a little bit, does the aircraft feel a torque that
tries to return it to the forward direction?

Dynamic stability is a different beast.  I described the phugoid
earlier --- this is the "pitch up, slow down, pitch down, speed up,
rinse, repeat" process.  It turns out that, because of an interaction
(a "coupling" in the strict sense) between the period of this
oscillation and the regular "weathervane" static oscillation, some
aircraft are unstable in the phugoid.  Each time they pitch up, the
pitch up a bit farther, and then lose more energy and pitch down
farther, and the process diverges over a period of minutes.

One way to imagine it is that the aircraft always "lags" the gravity
effect.  It has to wait a bit at the top of the curve to "point"
downward again, so it loses a bit more energy than it should and
slows down farther than it "should".  When it gets back to the bottom
of the curve, it's going faster, *and* it takes a bit longer to pitch
back up to the right value.  As you decrease the rate at which it
changes its pitch to match its velocity (i.e. as you decrease the
static stability) you eventually reach a point where the phugoid
oscillation is no longer damped, or is actually augmented.

So, the aircraft always tries to point toward its velocity vector, so
it meets the criteria for being statically stable.  But if you leave
it alone, it's velocity doesn't approach any single asymptotic value.
So it's not stable, either.  This kind of effect is called "dynamic"
instability.  In principle, there are other kinds of dynamic
instabilities.  In practice, this is the only one people mean when
they say an aircraft is dynamically unstable.

As Rob points out, it's usually treated in textbooks as a set of
differential equations in variables like: height, Vx, Vy and pitch
angle.  That is: "the time derivative of Vy is gravity plus thrust
times the sin of pitch angle", etc...  It turns out that after a
series of variable substitutions that make my eyes cross*, you can
characterize the solution as a polynomial.  The difference between a
convergent and divergent solution turns out to be equivalent to the
existence of real or complex roots to the polynomial.  But the effect
is qualitatively understandable without the math.

Andy

-- 
Andrew J. Ross                NextBus Information Systems
Senior Software Engineer      Emeryville, CA
[EMAIL PROTECTED]              http://www.nextbus.com
"Men go crazy in conflagrations.  They only get better one by one."
 - Sting (misquoted)


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