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How to Calculate the
Weight of
Air and Model Hot Air Balloon Lift - overflite
Hot air balloons fly because balloon and heated air inside
weigh less than surrounding ambient air displaced by balloon.
Difference in air weights is gross lift. Difference minus weight
of balloon is net lift.
Absolute Fahrenheit is used to calculate air weights
at
different temperatures. It is the number of degrees above
Absolute Zero. Which is around minus 460 degrees
Fahrenheit.
As
prime example, 48 Fahrenheit is the same as 508 Absolute Fahrenheit,
and 175 degrees Fahrenheit is the same as 635 Absolute Fahrenheit.
The standard weight of normal average sea level air is .0765
pounds per cubic foot at 59 F (519 Absolute Fahrenheit). Or
1.224 ounces. When air temperature goes up, air weight goes
down. By inverse proportion. Do the math. Multiply
519 by 1.224 to
get 635. This means that the heated air will weigh exactly one
ounce per
cubic foot at 635 Absolute Fahrenheit. Or 175 F.
At 48 F (508 A) a cubic foot of normal pressure sea
level
air
weighs almost exactly 1 1/4 ounces. Heated by 127 degrees,
to 175 F (635 A), it weighs almost exactly an ounce, or 4/5 of its
original weight, for a gross lift of a 1/4 ounce per cubic foot.
When air temperature goes up, air weight goes down, by
an
inverse proportion. From the ambient of 48 F (508 A) to 175 F
(635 A), the increase is 635/508, or 5/4, since both numbers are
divisible by 127. So the heated air will weigh 4/5
of its original weight. Or a reduction of 1/5. From 1 1/4
ounces to an
ounce. For a lift of a 1/4 ounce per cubic foot.
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Calculating the Weight of
Air,
using the "635 Factor"
Mathematically, with two variables, if one goes down at the same
rate the other one goes up, the variables can be multiplied times each
other, and their product will be constant. So, at standard normal
pressure sea level, ie. 29.92 inches of mercury (1013.25 Millibars),
the following equations are true:
Absolute Air Temperature * Cubic Foot Air
Weight
= "635" (or other specific number, adjusted for air pressure)
Cubic Foot Air Weight = "635" /
Absolute Air
Temperature
Absolute Air Temperature = "635" / Cubic Foot
Air
Weight
Formulas for Model Hot
Air
Balloon Lift:
Gross lift is the weight of the ambient air minus the weight of the
heated air. On a per cubic foot basis, at standard normal sea level
pressure, this can be expressed as follows:
Gross Lift = ( "635" / Ambient Temperature )
- (
"635" / Heated Air Temperature )
Gross Lift = ( "635" / Ambient Temperature )
- (
"635" / (Ambient Temperature + Heat Rise ) )
Gross lift can also be expressed as
a
fraction, as follows:
Gross Lift = "635" * ( Heated Air Temp. -
Ambient
Temp. ) / ( Heated Air Temp. * Ambient Temp. )
Gross Lift = ( "635" * Heat Rise) / ( Ambient
Temperature
*
( Ambient Temperature + Heat Rise) )
Alternately, the heated air
temperature
and
the heat rise can be expressed in terms of gross lift, as follows:
Heated Air Temperature = ( "635" * Ambient )
/ (
"635" - ( Gross Lift * Ambient ) )
Heat Rise = ( Gross Lift * Ambient ^ 2) / (
"635" -
(
Gross Lift * Ambient ) )
Hot Air Balloon Gross
Lift --
Per Cubic Foot -- Sea Level -- At Different Ambients and Heat Rises
Ambient /
Heat Rise |
30 F (490 A)
1.296 oz |
40 F (500 A)
1.270 oz |
50 F (510 A)
1.245 oz |
60 F (520 A)
1.221 oz |
70 F (530 A)
1.198 oz |
80 F (540 A)
1.176 oz |
90 F (550 A)
1.155 oz |
| + 10 F |
- 1.270 = .026 |
- 1.245 = .025 |
- 1.221 = .024 |
- 1.198 = .023 |
- 1.176 = .022 |
- 1.155 = .021 |
- 1.134 = .021 |
| + 20 F |
- 1.245 = .051 |
- 1.221 = .049 |
- 1.198 = .047 |
- 1.176 = .045 |
- 1.155 = .043 |
- 1.134 = .042 |
- 1.114 = .041 |
| + 30 F |
- 1.221 = .075 |
- 1.198 = .072 |
- 1.176 = .069 |
-1.155 = .066 |
- 1.134 = .064 |
- 1.114 = .062 |
- 1.095 = .060 |
| + 40 F |
- 1.198 = .098 |
- 1.176 = .094 |
- 1.155 = .090 |
- 1.134 = .087 |
- 1.114 = .084 |
- 1.095 = .081 |
- 1.076 = .079 |
| + 50 F |
- 1.176 = .120 |
- 1.155 = .115 |
- 1.134 = .111 |
- 1.114 = .107 |
- 1.095 = .103 |
- 1.076 = .100 |
- 1.058 = .097 |
| + 60 F |
- 1.155 = .141 |
- 1.134 = .136 |
- 1.114 = .131 |
- 1.095 = .126 |
- 1.076 = .122 |
- 1.058 = .118 |
- 1.041 = .114 |
| + 70 F |
- 1.134 = .162 |
- 1.114 = .156 |
- 1.095 = .150 |
- 1.076 = .145 |
- 1.058 = .140 |
- 1.041 = .135 |
- 1.024 = .131 |
| + 80 F |
- 1.114 = .182 |
- 1.095 = .175 |
- 1.076 = .169 |
- 1.058 = .163 |
- 1.041 = .157 |
- 1.024 = .152 |
- 1.008 = .147 |
| + 90 F |
- 1.095 = .201 |
- 1.076 = .194 |
- 1.058 = .187 |
- 1.041 = .180 |
- 1.024 = .174 |
- 1.008 = .168 |
- .992 = .163 |
| + 100 F |
- 1.076 = .220 |
- 1.058 = .212 |
- 1.041 = .204 |
- 1.024 = .197 |
- 1.008 = .190 |
- .992 = .184 |
- .977 = .178 |
| + 110 F |
- 1.058 = .238 |
- 1.041 = .229 |
- 1.024 = .221 |
- 1.008 = .213 |
- .992 = .207 |
- .977 = .199 |
- .962 = .193 |
| + 120 F |
- 1.041 = .255 |
- 1.024 = .246 |
- 1.008 = .237 |
- .992 = .229 |
- .977 = .221 |
- .962 = .214 |
- .948 = .207 |
| + 130 F |
- 1.024 = .272 |
- 1.008 = .262 |
- .992 = .253 |
- .977 = .244 |
- .962 = .236 |
- .948 = .228 |
- .934 = .221 |
| + 140 F |
- 1.008 = .288 |
- .992 = .278 |
- .977 = .268 |
- .962 = .259 |
- .948 = .250 |
- .934 = .242 |
- .920 = .235 |
| + 150 F |
- .992 = .304 |
- .977 = .293 |
- .962 = .283 |
- .948 = .273 |
- .934 = .264 |
- .920 = .256 |
- .907 = .248 |
| + 160 F |
- .977 = .319 |
- .962 = .308 |
- .948 = .297 |
- .934 = .287 |
- .920 = .278 |
- .907 = .269 |
- .894 = .261 |
Effects of Different
Ambient
Temperatures on Gross Lift
Cold weather increases lift. Hot weather reduces lift. This
happens in two ways. First is by the change in the weight of the
displaced ambient air. Second is by the change in the ratio of
the temperatures of the heated air and the ambient air, for a given
heat rise. As the formulas make clear, ambient temperature
changes affect lift by a modified squared function of the change.
As example, if the ambient temperature goes up 20
degrees,
from 48 F (508 A) to 68 F (528 A), the increase in temperature and the
decrease in air weight is about 4%, and sea level air weighs around
1.20 ounces per cubic foot. Heated by 127 degrees, to 207 F (655
A), the temperature increases by 655/528, or about 24%, and the air
weight decreases proportionately to about .97 ounces per cubic
foot. So, the gross lift is about .23 ounces per cubic foot, or
about 8% less than at an ambient of 48 F.
Alternately, if the ambient goes down 20 degrees to 28
F
(488
A), the air weighs around 4% more, or about 1.30 ounces per cubic
foot. Heated 127 degrees to 155 F (615 A) the temperature
increases by 615/488, or about 26% and the air weight decreases
proportionately to about 1.03 ounces per cubic foot. The result
is a gross lift of about .27 ounces per cubic foot, or about 8% more
than at an ambient of 48 F, and about 16% more than at an ambient
of 68 F ambient.
In reality though, the changes in lift are believed to
be
slightly less than predicted. In cold ambients there is "more air
to heat," and at higher ambients there is "less air to heat."
This causes slightly lower heat rises in cold weather, and slightly
higher heat rises in warm weather, of up to several degrees, for a
given amount of engine power.
Adjusting the "635
Factor" to
Account for Weather and Elevation
Humid air weighs slightly less than dry air, by a fraction of a
percent. Depending on weather, air pressure will normally vary by
around 1 1/2% up, and by around 2% down. So, covering most
conditions, the temperature where sea level air weighs exactly an ounce
per cubic foot will vary from around 160 F (620 A) to around 185 F (645
A). This means that the sea level "635 factor" will vary
from around 620 to around 645. For lift calculations though,
these changes are not very significant.
Elevation reduces air pressure, air weight, and the
temperature where air weighs exactly an ounce per cubic foot by around
3% per thousand feet, slightly more for lower elevations, and slightly
less for higher elevations. This reduces the "635 factor" by
around 20 degrees per thousand feet. Adjustments for altitudes of
up to 25,000 feet, that are over 99% accurate, can be calculated using
the following formula:
Air Pressure Adjustment = 1 - ( (
Elevation
--
in thousands ) / ( 27 + ( Elevation -- in thousands / 2 ) ) )
Note: For altitudes of up to
35,000
feet, adjustments that are close to 99% accurate can be calculated by
increasing the addition factor to 28; for up to 40,000 feet by
increasing the factor to 29, and for up to 45,000 feet by increasing
the factor to 30, etc. See Standard
Atmospheric Pressure Tables - (2).
| Elevation |
1,000 feet |
2,000 feet |
3,000 feet |
4,000 feet |
5,000 feet |
6,000 feet |
8,000 feet |
10,000 feet |
| % of Sea Level Air |
96.4% |
92.9% |
89.4% |
86.2% |
83% |
80% |
74.2% |
68.7% |
| "635 Factor" |
612 |
590 |
568 |
547 |
527 |
508 |
471 |
436 |
Accordingly, for a given heat rise, the
resulting
lift will be approximately the same as the percentage of sea level
air. In reality though, higher elevation air is believed to get
somewhat more lift than predicted, since higher elevation air has "less
air to heat," resulting in a greater heat rise from a given amount of
engine power than at sea level.
Guidelines for Balloon
Weights
at Sea Level:
For powered model hot air balloons, a gross weight 1/5 ounces per cubic
foot or less should provide reasonable net lift, assuming adequate
heating, and cool weather. To learn how birthday candle power
translates into model hot air balloon heating see Mathematical
Model for Heating Birthday Candle
Powered Balloons.
For unpowered paper balloons the maximum weight
shouldn't be
much more than around 1/8th ounces per cubic foot, since they will tend
to cool down fairly quickly, and you want to have reasonable flight
time.
For manned hot air balloons, you can
figure
that
the gross lift is probably around 1/5th of an ounce per cubic foot,
assuming the air is heated by around 100 degrees in mild weather, and
slightly more in warm weather. In this example, 80 cubic feet of
volume is required for each pound of gross lift. So, to lift a
thousand pounds, 80,000 cubic feet of volume would be required.
By Thomas
Taylor
-- balloons@overflite.com
www.overflite.com
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