EAA Chapter 25

A Community of Aviation Enthusiasts in the Twin Cities

Cleared for Takeoff – February 2005

Filed under: Cleared for Takeoff — admin at 9:32 pm on Friday, February 11, 2005

by Pat Halligan, Chapter 25 President

from On Final February 2005

You’ve all heard of cabin fever; well I think I had hangar fever if there is such a thing. I hadn’t flown the Cessna since the first weekend in December when my black lab Molly and I flew to Faribault for the Tree of Hope gathering. Even though I’d only been to the hangar once to shovel snow, I found myself thinking about a peaceful ride above the white countryside on some smooth winter air. The problem was either the weather wasn’t cooperating or I was too busy. Last weekend we were in Grand Forks celebrating my daughter’s 21st birthday. If she is getting older, I must be getting older too. Before that I was in Colorado skiing with my family. Then there was Christmas and New Years. This weekend we were going to go snowmobiling, but surprise surprise the weather was too warm, so we stayed home and I got to go flying this morning.

My lab Molly was the only one home when I decided to go flying, so her and I headed to the hangar around 10am even though it was a little windy- south at 18G24. It was very bumpy during the climb, but not bad at 2500′. It was fun to be flying the Cessna again even if the ground isn’t white and the air wasn’t smooooth.

Some great news from the Lakeville airport. Matt Ketcham and Chris Damlo (two of our members) both got hired by Mesaba Airlines in the past month. These two fellows are the ones who own and operate the Airlake Flight School. Chris will be flying the Avro jet and Matt will be flying the manly Saab. And don’t worry, they are going to keep the flight school open.

I’m sure some of you have found a used book store or good website where you get a great deal on aviation books. I became one of those lucky people last week. I was on a layover in San Francisco wandering the streets after lunch when I went into a used book bookstore called Acorn. I found the aviation section and for the next hour or so I looked through a lot of old/used books and I ended up buying two. One was about the life of Charles Lindberg and it was a first print-first edition book in good shape. I paid $12 for a book that was $30 new. The second one is titled The Leading Edge by Walter Boyne and it has some absolutely beautiful aviation pictures in it and to top it off, it is signed by the author. That one was $7. If you know of any websites or stores in our area, just let me know and I’ll pass it on to the rest of the members.

Another way to spend an enjoyable hour is to take a morning out of your busy schedule and go to Washburn High School and visit with Peter, his kids and checkout the Sonex. If you wait until the airplane is flying all you’ll see is a finished airplane, but if you visit now you’ll see kids building it piece by piece and then when you see it fly you’ll remember the faces and work that went into the building process. This is not a Cessna coming off an assembly line; it is an expression of love being shaped by teenagers.

When the weather warms up a little more, we will have a work day at the hangar and clean it up and organize the books, magazines and videos. If you plan on donating something to the chapter let one of the officers know ahead of time, and don’t just drop things off as the hangar starts to look like a flea market. Or is that a fly market. Thanks for your consideration.

I’m already thinking about our banquet later this year and if you have something to donate that would make a great door prize or silent auction item, please let me know. I already have a new set of headphones, but we will need more items to make it as enjoyable as last year.

If you know of any company that would like to be a newsletter sponsor please drop me a line as we are always looking for ways to offset the cost of the newsletter. With our new website their ads will be seen by more people.

Pat and my backseat co-pilot Molly.

Centrifugal Force – The “Imaginary” Force (or, The Physics of Coordinated Turns)

Filed under: Technical Articles — admin at 3:49 am on Friday, February 11, 2005

by John Koser

from On Final February 2005

The diagram shown on page 45 of the August 1997 Issue of “Flight Training,” also in part of several other flight training aids (Jeppeson Pilot Manual, FAA Flight Training Handbook, & ASA Private Pilot Test Prep), is basically incorrect from the outside observer’s (as they illustrate it) point of view. Two features about the diagram need to be addressed. The diagram looks much like the one shown below, where the two horizontal vectors are the same length, and the upward pointing vertical vector is longer than the downward one.

A. The vectors shown all seem to be real from the point of view of the pilot aboard the aircraft (shown heading toward the reader), but from the point of view of an observer in the position of the reader, suspended in space, there is one vector shown that shouldn’t be there – the one labeled “Centrifugal Force.”

B. The relative lengths of the vectors shown also need to be addressed, as vector addition is a scale process, and the vectors shown aren’t drawn to correct scale.

Analogy – Ball on a String With Vectors

To examine the two ideas, look at a simple analogy – a ball suspended on a string, which is whirled around in a horizontal circle. The airplane shown in the diagram is supposedly flying in a horizontal circle, so from our position in front of it as readers, we would be in relatively the same position with respect to the ball, and in the same horizontal plane.

If one considers a ball being swung on a string so its path is a horizontal circle, and asks, “What forces act on the ball?” one could see that the two forces (ignoring air friction) acting in the plane of the paper are: weight W, and string tension T. See Figure 2, noticing that no other forces act on the ball.



Since the ball is not accelerating in the vertical direction (no unbalanced forces, therefore no acceleration – Newton’s Second Law), the vertical component of the vector T must just be balanced by the downward pointing vector W. See Figure 3.
Notice that the vector T has no component pointing to the right. Its only components in the x and y directions (horizontal & vertical) point up and to the left (toward the center of the horizontal circle in which it is moving). The component of T which points to the left Tx, which is also toward the center of the horizontal circle of the ball’s movement is a center-pointing force, or centripetal force. It is an unbalanced force, therefore it produces acceleration (Newton’s Second Law again). The direction of this resulting acceleration must be in the same direction as the unbalanced force, which is to the left in the diagram, and this direction is along a radius, which points toward the center of the circle. In effect, the ball, going in a horizontal circle is always being accelerated toward the center of the horizontal circle.

Is there an Outward (Centrifugal) Force?

Where does the idea of a centrifugal (outward-pointing) force come from? If you are the pilot of the aircraft coming toward the reader (Figure 1), you feel an outward pointing force, just as does the driver of a car going around a horizontal curve. If you were riding on the ball in Figure 2, you would perceive that same outward pointing force. You think you feel this force, because the car, or the ball, or the airplane, to which you are secured by the seat/shoulder belt system, is pushing you inward. It does this because it’s an accelerated system, not an inertial system. In our everyday experience, we tend to think of all forces as balanced by equal and opposite forces (Newton’s Third Law). We tend to think there must be a force opposing this inward – pointing force, but that’s not true. It is this inward pointing force that makes you go in a circle. If you suddenly could remove it, you would continue in a straight line tangent to the curve at that point, except that gravity would make you begin to accelerate downward (an unbalanced force).

Comparison of Ball on String with the Airplane
The tension vector T on the ball is analogous to the lift vector provided by the airplane’s wings. The lift is produced because the wings are moving toward us through the air, whether the wings are oriented horizontally or at some angle (angle of bank). This lift vector describes a cone as the airplane banks at a constant angle about a vertical axis, just as does the string suspending the ball. The airplane then, generates lift perpendicular to its path, and that lift vector has two components, vertical and horizontal. The vertical component must be equal and opposite to the airplane’s weight and the horizontal component is completely unbalanced, therefore generating acceleration in the direction it points – toward the center of the horizontal circle.

Vector Addition and Vector LengthsNotice in Figure 3, the vertical component of lift and the weight vector are the same length. That must be true since there is no vertical acceleration. When a vector is resolved into its components along coordinate axes, the components are defined to the same scale. If the angle of bank to the horizontal is Ø, and if we define the Lift Vector as L, we use trigonometry to define the components as:

(Vertical Component) Ly = L(sin Ø), and

(Horizontal Component) Lx = L(cos Ø).

That’s why the “Resultant Lift” vector shown in Figure 1 is too long for the vector diagram’s scale.

Conclusion
There is no centrifugal force – only a perceived such sensation as felt by the pilot because the pilot is accelerating toward the axis of the horizontal circle, but it’s really the airplane exerting an inward force (which he/she perceives as an outward force) on the pilot.

The only force that’s unbalanced is the center-pointing force, which causes the acceleration toward the center of the circular path.

Anything going in a horizontal circular path is constantly being accelerated toward its center by an unbalanced force, the centripetal force.

Corrected Diagram
The diagram in Figure 1 can easily be corrected by making the vectors of correct length to represent components of lift L and by removing the fictitious centrifugal force vector. See Figure 4 below.

In this diagram, L has been divided into its components, Ly and Lx. These two components replace L. Since Ly is countered by the airplane’s weight W as it moves in a horizontal circle (not accelerating up or down), Ly & W disappear, and the only remaining force is Lx, the net force, which is a centripetal force.