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		In
        Their Own Words
         
		 ilbur 
		and Orville left Kitty Hawk, North Carolina on October 23, 1900 and 
		arrived at Dayton, Ohio a few days later. After 
		settling back into his routine and thinking about his experience in the 
		Outerbanks for a few weeks, Wilbur sat down and described his 
		experiences to Octave Chanute: 
		Octave Chanute 
		Chicago, Illinois 
		November 16, 1900 
		In October my brother and myself spent a vacation 
		of several weeks at Kitty Hawk, North Carolina, experimenting with a 
		soaring machine. We located on the bar which separates Albemarle Sound 
		from the ocean. South of Kitty Hawk the bar is absolutely bare of 
		vegetation and flat as a floor, from sound to ocean, for a distance of 
		nearly five miles, except a sand hill one hundred and five ft. high 
		which rises almost in its center. The main slope of the hill is to the 
		northeast, which is facing the prevailing winds. The slope is one in six 
		(9° 28'). To the north, northeast, east, and southeast there is nothing 
		but flat plain and ocean for a thousand miles nearly. It is an ideal 
		place for gliding experiments except for its inaccessibility. The person 
		who goes there must take everything he will possibly need, for he cannot 
		depend on getting any needed article from the outside world in less than 
		three weeks. 
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		The machine we used was a double-decker with surfaces 17 ft. by 5 ft. A 
		space eighteen inches wide was cut out of the lower surface, so the net 
		surface was about one hundred and sixty-five feet, and the weight with 
		operator was 190 lbs. The ribs were of ash bent to this shape. (See 
		Figure 1.) The depth of curve was two and one half inches, or about 
		one in twenty-three. The main cross-pieces were of white pine. The 
		forward pieces were triangular in cross section and located at the 
		extreme front. The rear pieces were square and located about a foot from 
		the rear edge. (See Figure 2.) An extra piece of cloth ran up 
		over it to lessen resistance. The covering of the machine was French 
		sateen, and it was put on bias so that no wire stays were needed to 
		brace the surfaces diagonally. All the ribs were enclosed thus. (See 
		Figure 3.) The uprights were jointed to the surfaces with flexible 
		hinges and the whole machine trussed the long way, that is laterally, 
		but not in the fore-and-aft direction. We used 
		fifteen-gauge spring steel wire. By tightening the wire "a" every other 
		wire was tightened. (See Figure 4.) The surfaces were thus left 
		capable of torsion, and this was the method we used to maintain lateral 
		equilibrium. We laid down flat on the lower surface and maintained 
		fore-and-aft balance by means of a forward rudder. We used no rear 
		rudder; and neither horizontal nor vertical tails. At first the machine 
		was curved laterally to obtain the effect of dihedral angles, but we 
		found the effect very unsatisfactory in gusty winds. Control was much 
		easier after we made it straight. We began experiments by testing the 
		machine as a kite, and found that a wind of twenty-five miles would more 
		than support it with operator on it. Our final estimate of its soaring 
		speed was twenty-two miles. We soon found that our arrangements for 
		working the front rudder and twisting the planes were such that it was 
		very difficult to operate them simultaneously. As we had neither the 
		material nor the tools to change these so as to correct the trouble we 
		were compelled to test them separately. Two minutes' trial was 
		sufficient to prove the efficiency of twisting the planes to obtain 
		lateral balance. We also found our system of fore-and-aft balancing 
		quite effective but it was only when we came to gliding that we became 
		positive of this. 
		We spent quite a large portion of our time in 
		testing the lift and drift of the machine in winds of different 
		velocities, and with various loads. I will not go into this matter 
		deeply just now but will say that in a wind blowing twenty miles per 
		hour the drift of the machine when loaded to bring its weight up to 
		fifty pounds was eight pounds. With the same wind blowing up a hill 
		having a rise of one in twelve the drift was only three or four pounds 
		and on a still steeper hill but with a lighter wind the drift became a 
		negative quantity and the machine both rose and made its way against the 
		wind till it lost its balance. The resistance of the framing is 
		certainly much less than Mr. Herring estimates in his article in the '97 
		Annual, for our machine is 25% larger than his, yet the drift due to a 
		lift of fifty lbs. added to the drift of the framing is less than his 
		estimate of framing drift alone. Our experiments also indicate that with 
		the operator lying down, the resistance is less than one tenth of the 
		estimate of Mr. Herring for the upright position. On the other hand we 
		found the drift of the surfaces under full load was greater than the 
		Lilienthal tables would indicate, but it may be that this is due to the 
		fact that our curve was only one in twenty-three instead of one in 
		twelve. The fact that our cloth was not varnished may also partly 
		account for it. 
		After we found the difficulty of simultaneously 
		maintaining both fore-and-aft and lateral balance we almost gave up the 
		idea of attempting to glide, but just before returning we went down to 
		the big hill which was about three miles from our camp and spent a day 
		in gliding. Our plan of operation was for the aeronaut to lie down on 
		the lower plane while two assistants grasped the ends of the machine and 
		ran forward till the machine was supported on the air. The fore-and-aft 
		equilibrium was in entire control of the rider, but the assistants ran 
		beside the machine and pressed down the end which attempted to rise. We 
		soon found that the machine could soar on a less angle than one in six 
		and that if the machine was kept close to the slope (which was one in 
		six by measurement) the speed rapidly increased till the runners could 
		no longer keep up. The man on the machine then brought the machine 
		slowly to the ground, so slowly in fact that the marks of the machine 
		could be seen for twenty or thirty feet back from the point where it 
		finally stopped. We had intended to have the operator turn his body to 
		an upright position before landing but a few preliminary tests having 
		shown that it was feasible to let the machine settle down upon its lower 
		surface with the operator maintaining his recumbent position, we used 
		this method of landing entirely. And although in appearance it was a 
		dangerous practice we found it perfectly safe and comfortable except for 
		the flying sand, and the machine was not once injured although we 
		sometimes landed at a rate of very nearly thirty miles per hour. The 
		operators did not receive a single bruise. With the conditions which 
		obtain at Kitty Hawk there is no need at all of using the upright 
		position. The distance glided was between three and four hundred feet at 
		an angle of one in six and the speed at landing was more than double 
		that of starting. 
		The wind was blowing about twelve miles. We found 
		no difficulty in maintaining fore-and-aft balance. The ease with which 
		it was accomplished was a matter of great astonishment to us. It was so 
		different from what the writings of other experimenters led us to 
		expect. This may have been partly due to the steadiness of the wind, 
		partly to the fixed position of the operator, and partly to a fortunate 
		combination of circumstances of which we were not aware, but it is our 
		hope that it was due to a new method of grouping our surfaces and to 
		the particularly efficient rudder which we used.1 I will write to you 
		later in regard to these. Our rudder had an area of twelve square feet, 
		and it was our sole means of guiding and balancing longitudinally. We 
		never found it necessary to shift the body. 
		Kitty Hawk is a splendid place to observe soaring 
		flight. I think at least a hundred buzzards, eagles, ospreys, and hawks 
		made their home within a half mile of our camp. We were enabled to make 
		a number of observations and settle conclusively to our minds some 
		points which have been much disputed among writers on the soaring 
		problem. 
		Wilbur Wright 
		Dayton, Ohio 
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		Figure 1. The shape of the ribs of the 1900 Wright Glider.
		
		  
		Figure 2. The shapes and locations of the spars in the 1900 Wright 
		Glider.
		
		  
		Figure 3. How the cloth wing covering encases the ribs of the 1900 
		Wright Glider.
		
		  
		Figure 4. How the 1900 Wright Glider is rigged.
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