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Project Gutenberg's Encyclopedia, vol. 1 ( A - Andropha

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speed, and then allowing for mechanical losses in the motor and 
propeller, which losses will generally be 50% of indicated 
h.p.  Close approximations are obtained by the above method 
when applied to full sized apparatus.  The following example 
will make the process clearer.  The weight to he carried 
by an apparatus was 189 lb. on concave wings of 143.5 sq. 
ft. area, set at a positive angle of 3 deg.  There were in 
addition rear wings of 29.5 sq. ft., set at a negative angle 
of 3 deg. ; hence, L= 189=.o.oo5XV2X143.5X0.545.  Whence 


$$V = \sqrt{189\over 0.005\times 143.5\times 0.545
= 22\hbox{ miles per hour},$$

at which the air pressure would be 2.42 lb. per sq. ft.  The area 
of spars and man was 17.86 sq. ft., reduced by various coefficients 
to an ``equivalent surface'' of 11.70 sq. ft., so that the 
resistances were:-- Drift front wings, 143.5X0.0285X2.42 . . . 
.= 9.90 lb.  Drift rear wings, 29.5X(o.o43-0.242X0.05235)X2.42 
= 2.17 lb.  Tangential force at 3 deg.  . . . . . . . . = 
0.00 lb.  Head resistance, 11.70X2.43 . . . . . = 28.31 

Total resistance . . . . . . . .= 40.38 

Speed 22 miles per hour.  Power = (40.38X22)/375 = 2.36 h.p. for 
the ``thrust'' or 4.72 h.p. for the motor.  The weight being 189 
lb., and the resistance 40.38 lb., the gliding angle of descent was 
40.38/189 = tangent of 12 deg. , which was verified by many experiments. 

The following expressions will be found useful in computing 
such projects, with the aid of the table above given: 


 
 1. Wind force, F = KV2.             8. Drift, D = KSV2esina
 2. Pressure, P = KV2S.              9. Head area E, get an equivalent 
 3. Velocity, V = sqrt. (W/(KSecosa))
                                    10. Head resistance, H = EF.
 4. Surface S varies as 1/V2.       11. Tangential force, T = Pa
 5. Normal, N = KSV2e.              12. Resistance, R = D + H (+ or -) T.
 6. Lift, L = KSV2ecsoa.            13. Ft. lb., M = RV.
 7. Weight, W = L = Ncosa.          14. Thrust, h.p., = RV/factor.
 

AEROSTATION.---Possibly the flying dove of Archytas of Tarentum 
is the earliest suggestion of true aerostation.  According to 
Aulus Genius (Noctes Atticae) it was a ``model of a dove or 
pigeon formed in wood and so contrived as by a certain mechanical 
art and power to fly: so nicely was it balanced by weights 
and put in motion by hidden and enclosed air.'' This ``hidden 
and enclosed air'' may conceivably represent an anticipation 
of the hot-air balloon, but it is at least as probable that 
the apparent flight of the dove was a mere mechanical trick 
depending on the use of fine wires or strings invisible to the 
spectators.  In the middle ages vague ideas appear of some 
ethereal substance so light that vessels containing it 
would remain suspended in the air.  Roger Bacon (1214-1294) 
conceived of a large hollow globe made of very thin metal and 
filled with ethereal air or liquid fire, which would float on 
the atmosphere like a ship on water.  Albert of Saxony, who 
was bishop of Halberstadt from 1366 to 1390, had a similar 
notion, and considered that a small portion of the principle 
of fire enclosed in a light sphere would raise it and keep it 
suspended.  The same speculation was advanced by Francis 
Mendoza, a Portuguese Jesuit, who died in 1626 at the age of 
forty-six, and by Gaspar Schott (1608-1666), also a Jesuit 
and professor of mathematics at Wurzburg, though for fire 
he substituted the thin ethereal fluid which he believed to 
float above the atmosphere.  So late as 1755 Joseph Galien 
(1699-1782), a Dominican friar and professor of philosophy 
and theology in the papal university of Avignon, proposed to 
collect the diffuse air of the upper regions and to enclose 
it in a huge vessel extending more than a mile every way, and 
intended to carry fifty-four times as much weight as did Noah's 
ark.  A somewhat different but equally fantastic method of 
making heavy bodies rise is quoted by Schott from Lauretus 
Laurus, according to whom swans' eggs or leather balls filled 
with nitre, sulphur or mercury ascend when exposed to the 
sun.  Laurus also stated that hens' eggs filled with dew will 
ascend in the same circumstances, because dew is shed by the 
stars and drawn up again to heaven by the sun's heat during the 
day.  The same notion is utilized by Cyrano de Bergerac 
(1619-1655) in his romances describing journeys to the moon 
and sun, for his French traveller fastens round his body a 
multitude of very thin flasks filled with the morning's dew, 
whereby through the attractive power of the sun's heat on the 
dew he is raised to the middle regions of the atmosphere, to 
sink again, however, on the breaking of some of the flasks. 

A distinct advance on Schott is marked by the scheme for aerial 
navigation proposed by the Jesuit, Francis Lana (1631-1687), 
in his book, published at Brescia in 1670, Prodromo ovvero 
Saggio di alcune invenzioni nuove promesso all' Arte Maestra. 
His idea, though useless and unpractical in so far that it 
could never be carried out, is yet deserving of notice, as 
the principles involved are sound; and this can be said of 
no earlier attempt.  His project was to procure four copper 
balls of very large dimensions (fig. 1), yet so extremely 
thin that after the air was exhausted from them they would 
be lighter than the air they displaced and so would rise; 
and to those four balls he proposed to attach a boat, with 
sails, &c., which would carry up a man.  He submitted the 
whole matter to calculation, and proposed that the globes 
should be about 25 ft. in diameter and 1/225th of an inch 
in thickness; this would give from all four balls a total 
ascensional force of about 1200 lb., which would be quite enough 
to raise the boat, sails, passengers, &c. But the obvious 
objection to the whole scheme is, that it would be quite 
impossible to construct a globe of so large a size and of 
such small thickness which would even support its own weight 
without collapsing if placed on the ground, much less bear 
the external atmospheric pressure when the internal air was 
removed.  Lana himself noticed this objection, but he 
thought that the spherical form of the copper shell would, 
notwithstanding its extreme thinness, enable it, after the 
exhaustion was effected, to sustain the enormous pressure, 
which, acting equally on every point of the surface, would tend 
to consolidate rather than to break the metal.  His proposal 
to exhaust the air from the globes by attaching to each a 
tube 36 ft. long, fitted with a stopcock, and so producing 
a Torricellian vacuum, suggests that he was ignorant of the 
invention of the air-pump by Otto von Guericke about 1650. 

We now come to the invention of the balloon, which was 
due to Joseph Michel Montgolfier (1740-1810) and Jacques 
Etienne Montgolfier (1745-1799), sons of Pierre Montgolfier, 
a large and celebrated papermaker at Annonay, a town about 
40 m. from Lyons.  The brothers had observed the suspension 
of clouds in the atmosphere, and it occurred to them that 
if they could enclose any vapour of the nature of a cloud in 
a large and very light bag, it might rise and carry the bag 
with it into the air.  Towards the end of 1782 they inflated 
bags with smoke from a fire placed underneath, and found 
that either the smoke or some vapour emitted from the fire 
did ascend and carry the bag with it.  Being thus assured 
of the correctness of their views, they determined to have a 
public ascent of a balloon on a large scale.  They accordingly 
invited the States of Vivarais, then assembled at Annonay, 
to witness their aerostatic experiment; and on the 5th of 
June 1783, in the presence of a considerable concourse of 
spectators, a linen globe of 105 ft. in circumference was 
inflated over a fire fed with small bundles of chopped straw.  
When released it rapidly rose to a great height, and descended, 
at the expiration of ten minutes, at the distance of about 
1 1/2m.  This was the discovery of the balloon.  The brothers 
Montgolfier imagined that the bag rose because of the levity 
of the smoke or other vapour given forth by the burning straw; 
and it was not till some time later that it was recognized that 
the ascending power was due merely to the lightness of heated 
air compared to an equal volume of air at a lower temperature.  
In this balloon, no source of heat was taken up, so that the 
air inside rapidly Cooled, and the balloon soon descended. 

The news of the experiment at Annonay attracted so much 
attention at Paris that Barthelemi Faujas de Saint-Fond 
(1741-1819), afterwards professor of geology at the Musee 
d'Histoire Naturelle, set on foot a subscription for paying 
the expense of repeating the experiment.  The balloon was 
constructed by two brothers of the name of Robert, under 
the superintendence of the physicist, J. A. C. Charles.  The 
first suggestion was to copy the process of Montgolfier, but 
Charles proposed the application of hydrogen gas, which was 
adopted.  The filling of the balloon, which was made of 
thin silk varnished with a solution of elastic gum, and was 
about 13 ft. in diameter, was begun on the 23rd of August 
1783, in the Place des Victoires.  The hydrogen gas was 
obtained by the action of dilute sulphuric acid upon iron 
filings, and was introduced through leaden pipes; but as the 
gas was not passed through cold water, great difficulty. was 
experienced in filling the balloon completely; and altogether 
about 300 lb. of sulphuric acid and twice that amount of iron 
filings were used (fig. 2). Bulletins were issued daily of 
the progress of the inflation; and the crowd was so great 
that on the 26th the balloon was moved secretly by night 
to the Champ de Mars, a distance of 2 m.  On the next day 
an immense concourse of people covered the Champ de Mars, 
and every spot from which a view could be ob obtained was 
crowded.  About five o'clock a cannon was discharged as the 
signal for the ascent, and the balloon when liberated rose to 
the height of about 3000 ft. with great rapidity.  A shower 
of rain which began to fall directly after it had left the 
earth in no way checked its progress; and the excitement was so 
great, that thousands of well-dressed spectators, many of them 
ladies, stood exposed, watching it intently the whole time 
it was in sight and were drenched to the skin, The balloon, 
after remaining in the air for about three-quarters of an 
hour, fell in a field near Gonesse, about 15 m. off, and 
terrified the peasantry so much that it was torn into shreds by 
them.  Hydrogen gas was at this time known by the name of 
inflammable air; and balloons inflated with gas have ever 
since been called by the people air-balloons, the kind invented 
by the Montgolfiers being designated fire-balloons.  French 
Writers have also very frequently styled them after their 
inventors, Charlieres and Montgolfieres. On the 19th 
of September 1783 Joseph Montgolfier repeated the Annonay 
experiment at Versailles, in the presence of the king, the 
queen, the court and an immense number of spectators.  The 
inflation was begun at one o'clock, and completed in eleven 
minutes, when the balloon rose to the height of about 1500 
ft., and descended after eight minutes, at a distance of 
about 2 m., in the wood of Vaucresson.  Suspended below the 
balloon: in a cage, had been placed a sheep, a cock and a duck, 
which were thus the first aerial travellers.  They were quite 
uninjured, except the cock, which had its right wing hurt in 
consequence of a kick it had received from the sheep; but this 
took place before the ascent.  The balloon, which was painted 
with ornaments in oil colours, had a very showy appearance 
(fig. 3). Francois Pilatre de Rozier (1756-1785), a native 
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