Air: Its Composition and Properties
The Source of Industrial Gas Products
Nitrogen, Oxygen, Argon
Most of the time we take air for granted. We
breathe it with hardly any conscious thought. We use it to
burn fuels for heating, transportation, power generation and many
other purposes. Sometimes,
we do think about air. We recognize that it is essential for life as
we know it. We sometimes worry about what we and others
may be doing to local air quality and to the composition of our shared
global atmosphere. What is air? What is air made up of? What are some of its characteristics? What useful products are directly produced from air? This page provides answers to these and other questions. |
|
Table 1: Standard Composition of Dry Air (Detailed Analysis): |
Gas | % by Volume | % by Weight | Parts per Million (by Volume) | Chemical Symbol | Molecular Weight |
Nitrogen | 78.08 |
75.47
|
780790 | N2 | 28.01 |
Oxygen | 20.95 | 23.20 | 209445 | O2 | 32.00 |
Argon | 0.93 | 1.28 | 9339 | Ar | 39.95 |
Carbon Dioxide | 0.040 | 0.062 | 401 | CO2 | 44.01 |
Neon |
0.0018
|
0.0012
|
18.21 | Ne | 20.18 |
Helium |
0.0005
|
0.00007
|
5.24 | He | 4.00 |
Krypton |
0.0001
|
0.0003
|
1.14 | Kr | 83.80 |
Hydrogen |
0.00005
|
Negligible | 0.50 | H2 | 2.02 |
Xenon |
8.7 x 10-6
|
0.00004
|
0.087 | Xe | 131.30 |
Local additions to the composition of air
can be very site-specific. They depend on the immediate
surroundings, including wind direction, time of time of day and
season of the year. Non-standard components may be present due to natural processes (biological or
geological) or human activities (industrial, transportation,
agricultural).)
Some common but "non-standard"
components include methane and sulfur dioxide (which
can be present in the parts per million range) nitrous oxide,
nitrogen dioxide, ammonia and carbon monoxide. Carbon dioxide (CO2) is considered to be a "standard" component of air, although the average concentration of carbon dioxide in air has been increasing at the rate of about 2 ppmv per year, and the concentration varies somewhat by location and season of the year. Any "standard" value for the concentration of carbon dioxide in air is an approximation. It is more meaningful to assign a range to the concentration of atmospheric carbon dioxide than to use a single value. At this time, 401 ppmv +/- 3 ppmv is a reasonable value. View recent historical concentration data. Future CO2 ranges will presumably continue to rise at a rate of about 2 ppmv per year in the near term. Consequently, when designing systems which have long useful lifetimes, the ability to handle CO2 concentrations which may be present in a decade or two, as well as the current level, should be considered. (For more information on this and related topics, see the extended discussion of CO2 levels below) |
English Units |
Normal Boiling Point (1 atm) |
Gas Phase Properties @ 32°F & @1 atm |
Liquid Phase Properties
@ B P& @ 1 atm |
Triple Point | Critical Point | |||||||||
Temp. | Latent Heat of Vaporization | Specific Gravity | Specific Heat (Cp) | Density | Specific Gravity | Specific Heat (Cp) | Temp. | Pressure | Temp. | Pressure | Density | |||
Substance |
Chemical Symbol |
Mol. Weight |
° F | BTU/lb | Air = 1 | BTU/lb °F | lb/cu. ft | Water = 1 | BTU/lb °F | °F | psia | °F | psia | lb/cu ft |
Air | -- | 28.98 | -317.8 | 88.2 | 1 | 0.241 | 0.08018 | 0.873 | 0.4454 | -352.1 | -- | -221.1 | 547 | 21.9 |
Metric Units |
Boiling Point @ 101.325 kPa |
Gas Phase Properties @ 0° C & @ 101.325 kPa |
Liquid Phase Properties
@ B.P., & @ 101.325 kPa |
Triple Point | Critical Point | |||||||||
Temp. | Latent Heat of Vaporization | Specific Gravity | Specific Heat (Cp) | Density | Specific Gravity | Specific Heat (Cp) | Temp. | Pressure | Temp. | Pressure | Density | |||
Substance |
Chemical Symbol |
Mol. Weight |
°C | kJ/kg | Air = 1 | kJ/kg ° C | kg/m3 | Water = 1 | kJ/kg ° C | °C | kPa abs | ° C | kPa abs | kg/m3 |
Air | -- | 28.98 | -194.3 | 205.0 | 1 | 1.01 | 1.2929 | 0.873 | 1.865 | -213.4 | -- | -140.6 | 3771 | 351 |
Detailed data on the physical properties of the individual gases in air, including the air-derived industrial gas products (nitrogen, oxygen, argon, neon, krypton and xenon) and other commonly-encountered atmospheric components and contaminants can be found in tables on this website. The physical property data is presented in your choice of English or Metric units. |
As air temperature
increases,
so does its ability to hold water vapor.
The upper limit on water vapor content is
predictable for at a given temperature, but the actual amount of water
vapor which is present in air at a given time and place will be
determined by many factors.
In temperate areas, the water vapor content will typically be between 1 to 2% in spring and fall, less than one-half percent in winter, and as much as 5% on a hot, humid summer day. In humid tropical areas, the water vapor content can be even higher, while in deserts, the water vapor content of air with the same (dry bulb) temperature may be very low. In near-polar regions the water vapor content of air will be less than 0.1%. Water vapor is less dense than air. (The molecular weight of water is 18.02 vs.28.98 for dry air.) Consequently, when water vapor is mixed with air, the density of the mixture will be less than that of dry air. The difference in density between dry air and saturated air increases with temperature, because the percentage of water in saturated air increases. This difference in density leads to a long-recognized link between fluctuations in barometric pressure and weather conditions. "High" barometric pressure is associated with clear skies, while "low" barometric pressure is associated with cloudy skies and rain. This table illustrates the impact of temperature on maximum potential water vapor content and air density at a pressure of one atmosphere. |
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Air Density and Maximum Water Vapor Content at Various Temperatures | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
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Water vapor is the component of air which
can vary the most from place to place, from day to day,
even hour to hour. The amount of water vapor in air will literally
change with the
weather and other variables such as proximity
to large bodies of water, and the temperature of the water in those
nearby lakes, seas and oceans.
Both
"relative" and "absolute" humidity
measurements have been developed to quantify the amount of water vapor
present in atmospheric air.
The body
of knowledge and techniques which allow physical and thermodynamic
properties of air to be calculated for any set of temperature and
pressure conditions are known as
psychrometry.
Useful definitions and relationships
related to water content and other properties of air are summarized
below - and presented in more detail on the
psychrometry page.
|
Dry-Bulb Temperature: |
Dry bulb
temperature is what is usually meant by "air temperature". It
is
measured with a normal thermometer.
|
Dew Point: | Dew point is the temperature at which water vapor begins to condense out of the air. Dew points can be defined and specified for ambient air or for compressed air. |
Wet-Bulb Temperature: |
Wet bulb
temperature is never higher than dry bulb temperature. They are
equal when air is at its dew point or saturation temperature. The
difference between the dry bulb and wet bulb temperatures is an
indicator of the humidity level.
Wet-bulb
temperature is the lowest temperature that water will reach by
evaporative cooling, and that temperature is almost always lower than
dry bulb. Wet bulb temperature is a critical parameter for sizing,
and measuring the performance of evaporative-cooled cooling water
systems.
|
Relative Humidity: | Relative humidity at dew point conditions is 100%. Otherwise, relative humidity is the percentage of the amount of water vapor actually present in the air, to the maximum amount that the air could hold under those temperature and pressure conditions. This measurement is highly correlated with human comfort - with about 50% being most comfortable . |
Absolute Humidity: | With the aid of a psychrometric chart, or its computerized equivalent, absolute values for water content such as weight fraction of ambient air, or weight-per-unit-volume of ambient air can be determined for any combination of dry bulb and wet bulb temperatures, or combination of dry bulb temperature and relative humidity. This measurement is required to design various types of moisture removal or humidification systems. |
Psychrometric Charts and
Online Psychrometric Calculations:
Psychrometric charts graphically
represent the thermodynamic properties of air. They depict
inter-relationships between multiple properties, such as
temperature, moisture content, density and energy (enthalpy). Charts can
be drawn for various elevations. For each elevation two known
properties allow determination of all other properties
plotted on the chart.
|
|
Download psychrometric charts in pdf format, drawn for sea level (one atmosphere) conditions. Choose charts in: Or use an online psychrometric calculator to generate properties for air. Specify two properties (e.g. dry bulb temperature and % relative humidity) and calculate other thermodynamic and physical values. The calculator will correct for elevation (or ambient pressure).Inch-Pound (I-P) units or |
|
The I-P and SI psychrometric charts and the online psychrometric calculator are provided under license from the Linric Company. |
Elevation (Altitude) Affects Air Pressure and Temperature: |
For convenience, much information
about air is specified for "sea level" or "one atmosphere" conditions.
But much human activity takes place at higher elevations - in come
cases only a few feet or meters above sea level - in other cases
hundreds or thousands of feet or meters higher.
Almost all of our activities take place in the
lowest level of the Earth's atmosphere - the Troposphere. The
Troposphere extends to a height of about 6 kilometers (4 miles) at the
poles, and to 11 kilometers (36,000 feet or 7 miles) near the equator.
The Troposphere has similar composition
at all levels, but its average pressure, temperature and density
decrease with altitude. In the lowest levels of the atmosphere, air temperature decreases as elevation increases - on average, about 3.56˚F for every 1000 feet, or 6.5˚C for each 1000 meters of elevation. Atmospheric pressure drops as elevation increases - about 0.5 psia for each 1000 feet of elevation, or about 1.1 kPa for each 100 meters. Air density decreases rapidly with increasing altitude or elevation. |
Average Atmospheric Pressure at Typical City and Industrial Plant Elevations |
Feet
|
Meters
|
psia
|
Atm |
Bar (a)
|
kPa | kg/cm2 |
In Hg
|
Mm Hg
|
0
|
0
|
14.7
|
1.00 | 1.013 | 101 | 1.03 |
29.9
|
760
|
500
|
150
|
14.4
|
0.98 | 0.994 | 99.4 | 1.01 |
29.4
|
747
|
1000
|
300
|
14.2
|
0.96 | 0.976 | 97.6 | 1.00 |
28.9
|
734 |
1500
|
450
|
13.9
|
0.94 | 0.956 | 95.6 | 0.98 |
28.3
|
719
|
2000 | 600 | 13.7 | 0.93 | 0.939 | 93.9 | 0.96 | 27.8 | 706 |
2500
|
750
|
13.4
|
0.91 | 0.923 | 92.3 | 0.94 |
27.3
|
694
|
3000
|
900
|
13.2
|
0.89 | 0.906 | 90.6 | 0.92 |
26.8
|
681
|
3500
|
1070
|
12.9
|
0.88 | 0.888 | 88.8 | 0.91 |
26.3
|
668
|
4000
|
1220
|
12.7
|
0.86 | 0.871 | 87.1 | 0.89 |
25.8
|
655
|
4500
|
1370
|
12.4
|
0.85 | 0.858 | 85.8 | 0.87 |
25.4
|
645
|
5000
|
1520
|
12.2
|
0.83 | 0.842 | 84.2 | 0.86 |
24.9
|
633
|
5500
|
1680
|
12.0
|
0.81 | 0.825 | 82.5 | 0.84 |
24.4
|
620
|
NOTE: An expanded version of this table is available. Click here to view it. |
Just above the Troposphere is the Lower Stratosphere, which long-distance jet aircraft pass through. At the boundary between the Troposphere and Lower Stratosphere, atmospheric pressure is about 3.1 psia or 20.1 kPa and the temperature is about -69˚F or -56˚C. The Lower Stratosphere is an almost constant temperature region, to an altitude of about 25 Km (86,000 feet, or 15 miles). |
Oxygen, Nitrogen and Argon - Atmospheric Industrial Gas
Products Critical
to Modern Life:
|
Nitrogen, Oxygen and Argon, the three primary
constituents of air, can be recovered from air in air separation plants. Each of
these atmospheric industrial gases is valued for particular properties.
Each of these gases are used
extensively in industry, the medical field, and in some products
used in homes.
Oxygen is valued for
reactivity.
It supports biological processes and combustion in many industries. It
is used in steelmaking and other metals refining and fabrication processes,
as well as in chemicals, pharmaceuticals, petroleum processing, glass and ceramic
manufacture, pulp and paper manufacture, healthcare, environmental
protection (through treatment of municipal and industrial effluents) and
in other miscellaneous uses.
Oxygen is often used with, or instead of, air to maximize the amount of oxygen available for combustion or biological activity. It is used to assist breathing in hospitals and other places. In industry, oxygen is used to increase reaction rates in industrial equipment and processes, to allow greater throughput in existing equipment and smaller sizes for new equipment. In some cases, such as industrial and municipal effluent treatment, normal oxygen (O2) is first converted to ozone (O3), which is a more reactive form. Using ozone instead of normal oxygen enhances reaction rates and ensures complete elimination of undesired compounds. Gaseous nitrogen is valued for inertness. It is used to shield potentially reactive materials from contact with oxygen. It helps maintain quality, and ensure safety in numerous applications. Liquid nitrogen is valued for coldness plus inertness. Vaporizing liquid nitrogen and warming the gas to ambient temperature absorbs a large quantity of heat. Liquid nitrogen, combining inertness with intense cold, is an an ideal coolant for certain specialized applications. One of these is food freezing, where very rapid freezing results in minimal cell damage from ice crystals, leading to improved appearance, taste and texture. Liquid nitrogen is also used to facilitate machining or fracturing of soft or heat sensitive materials. These include plastics, certain metals, pharmaceuticals, and even sophisticated processes which shred used tires - turning a difficult to handle waste product into materials which can be recycled into other useful products. Argon is valued for its total inertness. It is used in critical industrial processes such as producing high quality stainless steels and growing impurity-free silicon crystals for semi-conductor manufacture. It is used as a shield gas in critical welding applications, as a filler gas for light bulbs and as a heavier-than-air filler gas for the space between glass panels in high-efficiency multi-pane windows. |
Neon, Krypton and Xenon - "Rare Gases" from the Atmosphere - Special Gases for Special Uses: |
The so-called
"rare" gases
Neon, Krypton and Xenon, are present in very low concentrations in
air, which makes them economically recoverable only in large air separation plants. All of
these gases
are monatomic. They are valued for chemical
inertness
and for their light
emitting properties when electrically charged.
The boiling point of Neon is significantly
lower than nitrogen (lower than all the gases except helium and hydrogen).
It can be used as a very low temperature working fluid in refrigeration
cycles. Krypton and Xenon have additional uses that take advantage of their inertness and high molecular weight (83.80 and 131.30, respectively). Krypton and Xenon are about two to three times as heavy as argon (molecular weight 39.95) and approximately three to four times as heavy as nitrogen (not a true inert gas) at 28.0. Krypton and Xenon are used in very high insulating value multi-pane windows as they minimize heat loss due to convection between the panes. These gases are also used in light bulbs, where these heavy filler gases slow evaporation of the hot tungsten filament, leading to longer useful operating life and/or the ability to use higher efficiency, thinner filaments while still retaining acceptable operating life. |
More Information on
Atmospheric Gas Properties, their Uses and Applications
|
General Information on
Industrial Gas Production, Delivery and Safety:
|
Seasonal Atmospheric Changes Affect Air Separation Plant Performance: |
Many aspects of air separation design and
operation are determined by the properties of air.
Air separation plants are designed to handle expected concentrations of non-standard air components safely, and in a manner which ensures the purity of protects. When the local atmosphere is known to contain (or potentially contain) unusually high concentrations of gases such as sulfur oxides, CO2, hydrogen, ammonia, methane or higher hydrocarbons, additional purification (impurity removal) processes are added to air compression and air separation systems. Average atmospheric pressure at a plant site (which is primarily a function of elevation) must be known to properly select air compression machinery. Air compressors are typically equipped with inlet guide vanes or other means of capacity control, but still have a limited range of operation. The maximum volume of inlet air that can be processed (as measured in actual cubic feet or cubic meters per minute) is similar at any inlet pressure. To deliver the same amount of air (measured in Pounds, Tons, Kilograms, Standard Cubic Feet, Normal Cubic Meters, etc.) when operating at high elevations, a compressor must process greater physical volumes of inlet air than would be required if the compressor were being operated near sea level (about 3.4% more for each 1000 feet or 1.1% more for each 100 meters). To achieve the same discharge pressure when the inlet pressure is lower than it would be at sea level, the pressure ratio across the compressor must be higher; which requires more power. Weather-related variations in atmospheric pressure have only minor impacts on the performance of installed air separation systems. However, seasonal and daily variations in air temperature and humidity can have significant impacts on plant operations: Temperature Impact on Compression Capacity: Cold, dry winter air can be 10% denser than dry summer air. Since air compression equipment has limited ability to adjust the volume of inlet air that will be compressed, lower density summer air decreases the air handling and production capacities of air separation systems while higher density, cooler winter air results in greater air compression capacity (as measured in standard cubic feet, standard cubic meters, or by weight).Because of these atmospheric effects, the effective production capacity of air separation equipment can be measurably reduced on hot, humid days compared to winter and yearly-average conditions. To assure satisfactory operation, the effects of ambient air temperature and moisture content must be taken into account when sizing new equipment, relocating used equipment, and comparing plant operating data taken at different times. |
*
* * Historical Background
* * *
Post-glacial warming was not a "straight line"
phenomenon. Temperatures rose to modern
levels about 9000 years ago; but then began to fluctuate.
Between 8000 and 6000 years ago, and
several times since, the average temperature of the near-Earth atmosphere
has been the same or higher than its current value.
|
Some Very Long Term
Perspective - Evolution of the Earth's Atmosphere Over Geological Time:
|
The Earth's atmosphere has changed drastically over time.
The air that we are
accustomed to breathing is the product of billions of years of evolving
life forms interacting with the seas, the land, and the air.
The concentrations of both carbon
dioxide and oxygen in the air are the result of a dynamic balance between
mechanisms which remove these gases and others which replace them.
Oxygen is
reactive. Without replenishment by photosynthesis,
its concentration in air would decrease
as it combined with other elements to form various compounds.
Carbon dioxide is continually
produced and removed from the atmosphere by a multitude of natural
mechanisms. CO2 dissolves in water
(including rain) and carried into rivers, lakes and the oceans, and it
is removed by photosynthesis. It is replenished
by oxidation of dead organic matter and by animal respiration.
If the carbon dioxide content of air increases, it results in more vigorous plant growth, which
removes CO2 at a faster rate until a new equilibrium
between production and removal is established.
|
Correlation of Carbon Dioxide Levels in Air and Global Climate - 420,000 Years of Data: |
Changes in Atmospheric Carbon Dioxide Concentration - The Last Half-century: |
The charts below shows monthly data on
CO2 concentration in the atmosphere
between 2011 and mid-2015. Both monthly and annual average
atmospheric carbon dioxide concentrations are shown for data taken in the
mid-Pacific, at Mauna Loa, Hawaii. Data shows the dry air mole
fraction of air (after removing water vapor - with CO2 included in the
total). Monthly data is shown in red. Longer term moving averages are in
black. Mauna Loa Observatory is located at an elevation of 3397 m on the northern flank of Mauna Loa volcano at 200 north. Established in 1957, Mauna Lao Observatory has become the premier long-term atmospheric monitoring facility on earth. Source: NOAA http://www.cmdl.noaa.gov/ccgg/trends/ |
What do these historical records tell us about the current situation? |
Very simply, it says that
we
appear to be in uncharted waters.
Atmospheric carbon dioxide
concentrations measured over the past hundred years or so, have been
consistently higher than the approximately 300 ppmv level which appears to
have typically been reached
near the end of earlier interglacial periods; and they are rising at a
rapid rate.
There is disagreement
about many aspects of cause and potential effect; however, there is
general consensus that the rapid rise in carbon dioxide concentration is
cause for concern.
Many people are
concerned
that increasing levels of carbon dioxide in the atmosphere will
lead to increasingly hotter average worldwide temperatures,
with rising sea levels, changes in local climates, and inevitable
changes in local and global agriculture, water resource
availability, species
mix, etc.
Some people are concerned
that rapid heating may become so disruption to normal sea salinity levels
and heat transfer mechanisms in
the oceans, that a trend reversal may occur, triggering rapid cooling in near-polar areas and even faster
heating in equatorial regions.
These concerns have triggered
intense interest in increasing our collective understanding of what is
happening, why it is happening, how much of the relatively recent rise
in atmospheric carbon dioxide levels is due to human activity, and what
can and should be done to control emissions of carbon dioxide.
The rising atmospheric
CO2 level has become a political issue in addition to being a
scientific issue.
People throughout the world are debating the likely impacts of continuing
"business as usual" versus making conscious changes in the way we all
consume and discard carbon-containing materials.
We are seeing widespread efforts to better
understand the complex interactions between:
|
More Information on "Global Warming" Over the Past 11,000 years: |
"Global Warming"
is not a new phenomenon.
Average temperatures did
not rise slowly and smoothly to present levels following the last glacial period.
Instead,
average temperatures increased fairly rapidly until about 8,000 years
ago, at which time they were close to current levels. But then, warming continued for almost two thousand years,
rising to higher levels than we have seen recently.
Around six thousand years
ago, average
temperatures dropped rapidly; reaching levels lower than today,
and stayed lower for a thousand years.
In fact, over the past seven thousand
years, there appear to have been six significant cycles of interglacial cooling and warming.
Warm periods have coincided with significant
periods of societal change and architectural accomplishment in many
parts of the world. The Medieval Warm Period, from about 850
until 1250 AD, was a time of
unusually warm climate in Europe. Other warm periods spanned the peak
of Egyptian civilization (2600 to 2200 BC), the late Roman
Republic and peak of the Roman empire (roughly 100 BC through 200 AD) ,
and the Twentieth Century,
The Medieval Warm Period was followed by a cooler period
which is often referred to as the Little Ice Age. It lasted from about the mid to late
1300s into the late 1800s, almost 500 years. The the bitter cold winters
depicted in scenes of the American
Revolution, in the 1770s, occurred during this period.
A hundred years ago, following
the end of the last prolonged cool period, the
Titanic hit an iceberg that was one of many which were released as a
then-welcome spell of global warming
began to be felt.
The end of the "Little Ice
Age" period, in the mid to late 1800s, roughly coincided with the
start of a significant rise in
industrial activities. Some people claim that industrialization is
the cause of the warming trend since then. It may be equally true
that the warming trend spawned the vibrant growth of society and industry
that began as temperatures began to rise.
It is currently popular to point
to the increasing industrialization of the world,
coupled with significant human population growth, as primary
factors contributing to increases in the concentration of carbon dioxide
in the atmosphere. However, it is very likely that there are
multiple interrelated links between the rise in average global temperatures and
the rising carbon dioxide
content of air over the past hundred years.
|
Linkages Between Global Air Temperature, Average Ocean Temperature, and CO2 in Air: |
The Pre-Industrial Rise of Atmospheric
Carbon Dioxide:
At the
end of the last glacial period,
when air and sea water temperatures were well below current levels, the
concentration of carbon dioxide in the air was approximately 180 to 200
ppmv.
As the world warmed, the concentration of CO2 in the atmosphere rose. In the early to mid-1800s, prior to the end of the "Little Ice Age", the concentration of CO2 in the air was about 280 ppmv. This value has been referred to by many analysts as the "pre-industrial" CO2 level in the atmosphere.
Much of the rise from the post-glacial level of CO2 in the atmosphere, to the mid-1800s level, has been linked to warming of the oceans.
Carbon Dioxide in the Oceans:
The
US National Oceanic and Atmospheric Administration estimates the oceans
contain about 50 times more CO2 than the atmosphere and 10
times more than plant and soil carbon stores.
The amount of CO2 that the oceans can hold is temperature dependent, with much of it held in deep cold waters. Circulation patterns transport CO2 up and down in the ocean, and there is constant interchange of carbon dioxide between the oceans and the atmosphere.
Average temperatures in the ocean change much more slowly than average air temperatures. As the average and surface temperatures of the world's oceans have increased, a portion of the stored CO2 has been released to the atmosphere.
The Situation Today:
The rise in atmospheric CO2
concentration
which occurred between the early-1800s to the mid-1900s was gradual. In
1960, the average concentration of CO2 in the atmosphere was
about 315 ppmv. Since the mid-1900s, the concentration of CO2 in the atmosphere has increased significantly, and the rate of rise has been accelerating. Currently, the average measurement is about 390 ppmv, and the annual average value is rising at about 2.1 ppmv / year.
Since the acceleration of population growth and industrialization throughout the world in the past 60 years or so coincides with an increase of more than 25% in the concentration of carbon dioxide in the atmosphere during that same period, it is reasonable to assume that many human activities, including the use of carbon-containing fuels for heating, industry and transportation, and wide-spread de-forestation, have been and are contributing to the rapid rise in atmospheric carbon dioxide concentration.
What can be done, what should be done, and the best way to do what seems prudent to do about the rising level of carbon dioxide in the atmosphere, are the subjects of intense global research and debate.
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