Great information....and correlation with my theory about the mac and the
corresponding cg range.  My wings are going to be stretched so I have to be
very careful with the cg and that is causing me to relook at what was done
before.
On Aug 16, 2013 10:39 PM, "Mark Langford" <ml at n56ml.com> wrote:

> NetHeads,
>
> Here are two messages I fished out of the KRnet archive from 2001.  I just
> killed an hour sifting through that whole conversation.  Quite interesting.
> For those interested, this thread will take you off the streets for a few
> days.  I remember it well!
>
> Richard Mole is a good friend and very sharp English aero engineer, and
> Bill Marcy was the aerodynamics consultant for Jeanette Rand on occasion
> when she needed some aero work done on the KR.  Two different opinions, but
> definitely food for thought, either way.  Hopefully I'm not opening a huge
> can of worms here.
>
> For those who want to get lost in that discussion, rather than building
> their own personal KR time machine , a trip back in time to early March of
> 2001 can be had by visiting the KRnet archive at http://tugantek.com/**
> archmailv2-kr/search <http://tugantek.com/archmailv2-kr/search>.  This
> link is at the bottom of every email sent out from krnet at list.krnet.org .
>  Hopefull
> ------------------------------**-------------
>
> Date: Mar 8, 2001 3:28 PM
>
> Sender: Richard Mole
>
> Subject: Stability - ugh! - again - the last time - that's a promise!
>
> I felt that this post was required to try and clear the air. If you not a
> 'techie' its probably best to skip it completely.
>
> All the information in this posting is supplied without warranty of any
> sort
> implied or explicit. Aft cg limits shown here are calculated in good faith
> -
> but they have NOT been independently checked. They are not authoritative.
> They are one man's best shot.
>
> Results of own analysis; neutral points stick fixed and stick free.
> Datum: all aft of LE of stub wing kr2 Kr2S
> Stick fixed np 12.75" 13.5"
> Stick free np 11.8" 1.3 lbs/g at this limit 12.2" 1.3 lbs/g at this
> limit
>
> So there is very little difference, just 0.4", between the calculated aft
> cg for the kr2 and the kr2S.
> All numbers are power-off and the de-stabilising effects of power will
> bring
> them forward.
>
> Note that at least two Airworthiness authorities restrict the aft cg
> position:
> Australia aft cg limit is 12" aft of LE on stub wing (info posted by Malcom
> Bennet, krnet 23.12.98)
> South Africa aft cg limit is 13.44" aft of LE on stub wing (info posted by
> Kobus De Wet, 27.12.98)
>
> The stick fixed np is included in the table for interest only because the
> stick free case is always more stringent.
>
> It is possible to fly with the cg aft of the stick-free np but it is VERY
> dangerous and foolish to try this. The stick free manoeuvre margin is what
> makes it possible and this depends upon air density, so the margin reduces
> with density altitude.
>
> Bigger tails and moment arms both increase the tail volume and move the
> stick fixed np further aft. But this may be an illusory gain. What is
> really
> required is a rearward shift in the stick free n.p.
>
> The kr elevator floats with the relative wind because it has no aerodynamic
> balance. This floating tendency will always ensure that the stick free np
> is
> well forward of the stick fixed np whatever the tail volume may be.
>
> Aerodynamic balance is one (but only one) approach to improving the
> situation. Hence Dana's elevator horns.
>
> These horns add area and so they do improve the stick fixed np. More
> crucially, they reduce the tendency of the elevator to float with the
> relative wind. The stick free np is then much closer to the stick fixed np.
>
> It is hard to judge the correct horn geometry. Dana's horns are 'unshielded
> horns'. It is imperative to use the best data sheets available (ant to
> correct for the effects of the elevator cut-out). Do not try to eye-ball
> this for yourself as over-balancing is more dangerous than no balance.
>
> To do a longitudinal stability analysis requires a lot of work. These are
> some of the data that are required to be estimated to a high degree of
> accuracy. My full analysis covers 7 sides of single spaced paper.
>
> Estimates are required for:
>
> Wing lift slope a1 per rad (from Reynolds number, included angle at TE,
> transition point, Aspect ratio etc)
> Wing mean aerodynamic chord mac
> Tail lift slope a1t per rad (as for wing plus account of elevator cut out)
> Tail volume (from wing and tail areas, mac and tail arm)
> Rate of change of downwash with wing alpha
> Elevator lift slope a2 per rad
> Hinge moment rate due incidence b1
> Hinge moment rate due elevator deflection b2
> Stick free factor = 1- a2/a1t*b1/b2
> Elevator gearing
> Longitudinal a/c relative density
>
> So it's a long haul and fraught with opportunity for unintended error and
> plain mistakes. The table at the start of this post is my best shot. It is
> offered in good faith.
>
> Richard
>
>
>
> ------------------------------**------------------------------**
> --------------------
>
> Then from Bill Marcy:
>
> Date: Mar 9, 2001 8:23 AM
>
> Sender: Bill Marcy
>
> Subject: tail stuff yet agan
>
>
>
> Tail Stuff again
>
> First things first: I have been challenged to knock off the discussion
> and publish the results of my calculations for the KR-2 and KR-2S. I did
> these calculations six years ago at the request of Jeannette Rand in
> response to concerns by the Australian CAA.
>
> The stick fixed, power off neutral point of the KR-2 is 7.24 inches aft
> of the wing 25 percent mean aerodynamic chord, or 31.06 inches aft of
> the aft face of the firewall. This is 3 inches further aft than the aft
> limit shown in the KR-2 manual I have had since about 1988.
>
> The stick fixed, power off neutral point of the KR-2S is 7.12 inches aft
> of the wing 25 percent mean aerodynamic chord, or 33.18 inches aft of
> the aft face of the firewall. This is a bit more than 5 inches behind
> the aft limit in the Rand manual (I assume the c.g. limits for the -2
> and -2S are the same).
>
> The difference between the two locations is almost entirely due to the
> 2.0 inch difference between the locations of the 25 percent mean
> aerodynamic chords of the two airplanes, and this difference is due to
> the increased wingspan and reduced tip chord of the KR-2S relative to
> the KR-2. Note that within the accuracy of calculation, the neutral
> points are exactly the same distance behind the 25 percent mean
> aerodynamic chords of the two airplanes.( Incidentally, don?t take the
> .01 inch accuracy of the numbers too seriously, they are probably no
> better than about .15 inches.)
>
> For those who want to check my neutral point calculations, here are the
> numbers.
> For the KR-2:
> wing area 74.22 square feet
> wing span 20.21 square feet
> mean aerodynamic chord 3.52 feet
> aspect ratio 5.50
> lift curve slope 4.401 per radian
> location of 25 percent mean aerodynamic chord 24.06 inches aft of the
> firewall aft face
> fuselage length 174 inches
> fuselage width 38.12 inches
> horizontal tail area 10.94 square feet
> horizontal tail span 20.21 feet
> mean aerodynamic chord 3.52 feet
> aspect ratio 3.20
> lift curve slope 3.482 per radian
> location of 25 percent mean aerodynamic chords 121.05 inches aft of the
> firewall aft face and 30 inches above the zero lift plane of the wing.
> downwash derivative at the horizontal tail 0.36 degrees per degree
> angle of attack
>
> For the KR-2S:
> wing area 81.15 square feet
> wing span 23.54 feet
> mean aerodynamic chord 3.28 feet
> aspect ratio 6.83
> lift curve slope 4.707 per radian
> location of 25 percent mean aerodynamic chord 26.06 inches aft of the
> firewall aft face
> fuselage length 190 inches
> fuselage width 38.12 inches
> horizontal tail dimensions are the same as KR-2 except the location of
> the 25 percent mean aerodynamic chord, which is 137.05 inches aft of
> the firewall and 34 inches above the wing zero lift line.
>
> In response to another question, I have not and am not building a KR,
> and I have never flown one of any kind. My personal airplane is a large,
> comfortable, very stable, ponderous, slow, and inefficient 1947 Navion;
> I have owned it since 1977. I have no axe to grind one way or another.
> However, I do lean toward improvements to the airplane that can be made
> by builders who are already flying. This is the reason I have stated
> that , as Dana Overall stated:
> stability is determined by the location of the center of gravity in
> relation to the center of pressure (lift).
> That is a qualitative, but nevertheless true, statement. More precisely,
> I will quote from NACA Technical Report No. 971, Appreciation and
> Prediction of Flying Qualities, by William H. Phillips, published in
> 1948:
> An airplane that is stable with stick fixed requires a forward movement
> of the stick to increase speed (same thing as decreasing angle of
> attack or lift coefficient) and a rearward movement of the stick to
> decrease speed (same thing as increasing angle of attack or lift
> coefficient).
> As the center of gravity moves aft toward the point of neutral
> stability, it takes less and less stick motion to pitch the airplane
> through its full range of lift, until at the neutral point, no motion at
> all is required, and aft of the neutral point the motion is reversed.
> This is a definition that anyone who flies can understand.
>
> Next, Phillips defines the stick-free stability:
> An airplane that is stable in pitch with its stick free requires not
> only forward motion to increase speed, but also requires that the stick
> must need a push force to move it forward and must need a pull force to
> move it aft.
> Because the elevator generally tends to float with the relative wind,
> the effective stabilizing area of a tail with the elevator free to move
> is less than with the stick fixed, and the aft limit of the center of
> gravity with stick free is more forward than the aft limit with stick
> fixed. This can result in a condition that appeals to the aerobatically
> inclined: there is a center of gravity that is slightly stable with
> stick held fixed, but that lets you move it back and forth with no
> resistance. This can be fun for awhile, but it gets tiresome if you are
> trying to fly straight and level on a cross country. Incidentally, stick
> free stability is what the FAA requires; in fact, it requires that the
> stability margin be high enough and control system slop and friction be
> low enough that with the airplane trimmed to zero stick force at any
> speed, it will return to within 10 percent of that speed if the stick is
> pushed or pulled for a moment and then released.
>
> Nothing here says that the only way to get more distance between the
> center of gravity and the stick-fixed or stick-free neutral points is by
> moving the neutral points to the rear. The same effect can be gotten by
> balancing the airplane so its center of gravity is more forward. Now,
> just how far forward can the center of gravity be? First, for a
> taildragger especially, it can?t be so nose heavy that it falls over
> when brakes are applied. Second, it can?t be so nose heavy that the tail
> can?t balance it throughout its speed range. The landing gear problem
> can be solved by tilting the gear legs forward, so let?s look at the
> tail effectiveness, starting with the condition for maximum lift.
>
> S.F. Hoerner in his book, Fluid Dynamic Lift, lists the max lift
> coefficient of the RAF 48 as 1.45. For the KR-2S wing, the angle of
> attack for this coefficient is 1.45/4.71 = .308 radians or 17.6 degrees.
> Including 3.5 degrees incidence, the zero lift line of the wing is
> approximately 3 degrees nose down, so the airplane angle of attack at
> maximum lift is 14.6 degrees. This should be the angle of attack of the
> horizontal tail, but that neglects the downwash behind the wing. The
> stability calculations gave the downwash as 36 percent, so the true
> angle of attack of the tail is 14.6 degrees minus 0.36 times 17.6
> degrees, which equals 8.3 degrees. The max elevator deflection is 30
> degrees up, and the elevator effectiveness, assuming 50 percent chord
> ratio, is about 65 percent. This means that 30 degrees elevator
> deflection is equivalent to 20 degrees angle of attack. Subtract 8.3
> degrees from that, and the down tail load is what can be produced by
> 11.7 degrees angle of attack. The tail lift curve slope is 3.482, so the
> tail lift coefficient is -0.711. The area of the KR-2S tail is 10.94
> square feet, and the dynamic pressure at max lift (1050 lb weight) is
> 8.94 pounds per square foot. Then the maximum tail down load with 30
> degrees up elevator at maximum lift is 69.5 pounds. The 25 percent mean
> aerodynamic chord of the tail is 8.08 feet aft of the wing 25 percent
> mean aerodynamic chord, so the nose up moment at the 25 percent wing
> chord is 562 foot pounds. The airplane weighs 1050 pounds (in this
> example), but you can?t get a full forward center of gravity with two
> persons, so we should subtract 170 pounds. This reduces the dynamic
> pressure at stall to 7.49 pounds per square foot, so the maximum down
> load at the tail can only be 58.2 pounds and the nose up moment can only
> be 471 pounds. Then the furthest forward the center of gravity can be is
> 562/1050 = 0.535 feet, or 6.42 inches forward of the 25 percent wing
> mean aerodynamic chord. This is 17.6 inches aft of the aft face of the
> firewall. My KR-2 construction manual (NOTE: KR-2, not KR-2S) gives the
> forward limit as 8 inches aft of the wing leading edge, or only 4.0
> inches forward of the 25 percent mean aerodynamic chord. So these
> calculations let you have 2.4 inches more forward center of gravity than
> specified in the plans. However, be aware that I have neglected the tail
> down load required to counter the nose-down moment of the wing-fuselage
> combination that is due to camber; I have neglected any power effects,
> and I have used an elevator effectiveness curve that ignores the gap
> between the elevator and the stabilizer.
>
> I have included all the details of this calculation to give you all an
> idea of what is involved in analyzing an airplane design. Note that I
> have not done the calculation of the tail angle of attack, elevator
> deflection, and down load required for the high speed dive condition,
> because I don?t have the zero lift pitching moment coefficient for the
> RAF 48.
>
> However, all this is mere discussion. The proof of the pudding is that
> dozens of KR-1?s and KR-2?s, and not a few KR-2S?s, have been built and
> flown for hundreds of hours. This does not mean it can?t be improved.
> The early Bonanza revolutionized the post WWII aviation market, but
> compared to the Bonanza that has evolved since 1946 it is completely
> outclassed. Let?s do the same for the KR.
>
> Well, I?ve gotten carried away by enthusiasm again. I had some other
> stuff but I will put it off until I get some feedback on what I?ve given
> you here.
> Now I?ve got to get cracking on static test loads for Chris Kogelmann.
> Keep the airspeed up and the dirty side down, guys!
>
> Bill Marcy
> old paper and pencil engineer
>
>
>
> ------------------------------**------------------------------**
> --------------------
>
> Mark Langford
> ML at N56ML.com
> website at http://www.N56ML.com
> ------------------------------**--------------------------
>
>
> ______________________________**_________________
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