Difference between revisions of "Gas constant" - New World Encyclopedia

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{|  class="wikitable" style="float: right;"
 
{|  class="wikitable" style="float: right;"
 
! Values of ''R''
 
! Values of ''R''
! Units
+
! Units <br /> [[Ideal gas law|(V·P·T<sup>-1</sup>·n<sup>-1</sup>)]]
 
|- [[International Organization for Standardization | ISO]]
 
|- [[International Organization for Standardization | ISO]]
 
| 8.314472
 
| 8.314472
J·K<sup>-1</sup>·mol<sup>-1</sup>
+
[[Joule|J]]·K<sup>-1</sup>·mol<sup>-1</sup>
 
|-  
 
|-  
| 0.08205784
+
| 0.0820574587
| L·atm·K<sup>-1</sup>·mol<sup>-1</sup>
+
| [[Liter|L]]·[[atmosphere (unit)|atm]]·[[Kelvin|K]]<sup>-1</sup>·[[Mole (unit)|mol]]<sup>-1</sup>
 
|-  
 
|-  
 
| 8.20574587 × 10<sup>-5</sup>
 
| 8.20574587 × 10<sup>-5</sup>
Line 17: Line 17:
 
|-  
 
|-  
 
| 8.314472  
 
| 8.314472  
| L·kPa·K<sup>-1</sup>·mol<sup>-1</sup>
+
| L·k[[Pascal (unit)|Pa]]·K<sup>-1</sup>·mol<sup>-1</sup>
 
|-  
 
|-  
 
| 8.314472  
 
| 8.314472  
| m<sup>3</sup>·Pa·K<sup>-1</sup>·mol<sup>-1</sup>
+
| m<sup>3</sup>·[[Pascal (unit)|Pa]]·K<sup>-1</sup>·mol<sup>-1</sup>
 
|-  
 
|-  
| 62.3637
+
| 62.36367
| L·mmHg·K<sup>-1</sup>·mol<sup>-1</sup>
+
| L·[[mmHg]]·K<sup>-1</sup>·mol<sup>-1</sup>
 
|-  
 
|-  
| 62.3637
+
| 62.36367
 
| L·Torr·K<sup>-1</sup>·mol<sup>-1</sup>
 
| L·Torr·K<sup>-1</sup>·mol<sup>-1</sup>
 
|-  
 
|-  
Line 32: Line 32:
 
|-  
 
|-  
 
| 1.987  
 
| 1.987  
| cal &middot; K<sup>-1</sup>·mol<sup>-1</sup>
+
| [[calorie|cal]]·K<sup>-1</sup>·mol<sup>-1</sup>
 
|-  
 
|-  
 
| 6.132440  
 
| 6.132440  
| lbf·ft·K<sup>-1</sup>·g·mol<sup>-1</sup>
+
| [[foot-pound|lbf]]·ft·K<sup>-1</sup>·g-mol<sup>-1</sup>
 
|-  
 
|-  
| 10.7316
+
| 10.73159
| ft<sup>3</sup>·psi&middot; °R<sup>-1</sup>·[[lb-mol]]<sup>-1</sup>
+
| ft<sup>3</sup>·psi· [[Rankine scale|°R]]<sup>-1</sup>·[[lb-mol]]<sup>-1</sup>
 
|-  
 
|-  
| 8.63 × 10<sup>-5</sup>
+
| 0.7302413
| eV·K<sup>-1</sup>·atom<sup>-1</sup>
+
| ft<sup>3</sup>·atm·°R<sup>-1</sup>·lb-mol<sup>-1</sup>
 
|-  
 
|-  
0.7302
+
998.9701
| ft<sup>3</sup>·atm·°R<sup>-1</sup>·lb-mol<sup>-1</sup>
+
| ft<sup>3</sup>·mmHg·K<sup>-1</sup>·lb-mol<sup>-1</sup>
 +
|-
 +
| 8.314472 × 10<sup>7</sup>
 +
|  erg·K<sup>-1</sup>·mol<sup>-1</sup>
 
|}
 
|}
The '''gas constant''' (also known as the '''universal''' or '''ideal gas constant''', usually denoted by symbol '''''R''''') is a [[physical constant]] used in [[equations of state]] to relate various groups of [[state function]]s to one another.  It is another name for the [[Boltzmann constant]], but when used in the [[ideal gas law]] it is usually expressed in the more convenient units of [[energy]] per [[kelvin]] per [[mole (unit)|mole]] rather than simply energy per kelvin per particle.
 
  
The ideal gas constant occurs in the simplest equation of state, the [[ideal gas law]], as follows:
+
The '''gas constant''' (also known as the '''molar''', '''universal''', or '''ideal gas constant''') is a [[physical constant]] that is featured in a number of fundamental equations in the physical sciences, such as the [[ideal gas law]] and the [[Nernst equation]]. It is expressed in units of [[energy]] (that is, the pressure-volume product) per [[kelvin]] per ''[[mole (unit)|mole]].'' It is equivalent to the [[Boltzmann constant]], except that the latter is expressed in units of energy per kelvin per ''particle.''
:<math>P = {RT\over{\tilde{V}}}</math>
+
 
where ''P'' is the [[pressure]] of an [[ideal gas]]<br/>
+
Denoted by the symbol '''''R''''', the value of the gas constant is:
''T'' is its [[temperature]]<br/>
+
:'''''R'' = 8.314472(15) J &middot; K<sup>-1</sup> &middot; mol<sup>-1</sup>'''
<math>\tilde{V}</math> is its [[molar volume]]<br/>  
+
The two digits in [[Bracket|parentheses]] indicate the uncertainty ([[standard deviation]]) in the last two digits of the value.
This can also be written as:<br/>
+
{{toc}}
:<math>\qquad PV=nRT</math>
+
[[Image:Gas-particles.jpg|200px|right|thumb|Movement of particles ([[atoms]], [[molecule]]s, or ions) in the [[gas]] phase. The gas constant is a factor in the [[ideal gas law]], which provides an approximation of some of the properties of gases.]]
where ''V'' is the volume the gas occupies<br/>
+
 
''n'' is the moles of gas
+
== Ideal gas law ==
 +
An '''ideal gas''' (or "perfect" gas) is a hypothetical [[gas]] consisting of a very large number of identical particles, each of zero volume, uniformly distributed in density, with no intermolecular forces. Additionally, the [[molecule]]s or [[atom]]s of the gas have complete randomness of direction and velocity, and they undergo perfectly elastic collisions with the walls of the container. The molecules of an ideal gas are often compared to rigid but elastic billiard balls.
 +
 
 +
The gas constant occurs in the [[ideal gas law]] (the simplest [[equation of state]]) as follows:
 +
:<math>P = \frac{nRT}{V} = \frac{RT}{V_{\rm m}}</math>
 +
where:
 +
: <math>P\,\!</math> is the absolute [[pressure]]
 +
: <math>T\,\!</math> is absolute [[thermodynamic temperature|temperature]]
 +
: <math>V\,\!</math> is the volume the gas occupies
 +
: <math>n\,\!</math> is the amount of gas (in terms of the number of [[mole (unit)|mole]]s of gas)
 +
: <math>V_{\rm m}\,\!</math> is the [[molar volume]]
  
''R'' appears in the [[Nernst equation]] as well as in the [[Lorentz-Lorenz]] formula.  
+
This equation does not exactly apply to real gases, because each molecule of a real gas does occupy a certain volume and the molecules are subject to intermolecular forces. Nonetheless, this equation is used as an approximation when describing the behavior of a real gas, except when the gas is at high pressures or low temperatures.
  
Its value is:
+
==Relationship with the Boltzmann constant==
:'''''R'' = 8.314472(15) J &middot; K<sup>-1</sup> &middot; mol<sup>-1</sup>'''
+
 
The two digits between the [[Bracket|parentheses]] denote the uncertainty ([[standard deviation]]) in the last two digits of the value.
+
The [[Boltzmann constant]] ''k<sub>B</sub>'' (often abbreviated ''k'') has the value 1.3807 x 10<sup>-23</sup> J.K<sup>-1</sup>. It may be used in place of the universal gas constant by working in pure particle count, ''N'', rather than number of moles, ''n'', since
 +
: <math>\qquad R=N_A k_B\,\!</math>,
 +
where <math>N_A</math> is [[Avogadro constant|Avogadro's number]] (= 6.022 x 10<sup>23</sup> particles per mole).
 +
 
 +
In terms of Boltzmann's constant, the ideal gas law may be written as:
 +
: <math>PV=Nk_BT\,\!</math>
 +
where ''N'' is the number of particles (atoms or molecules) of the ideal gas.
 +
 
 +
Given its relationship with the Boltzmann constant, the ideal gas constant also appears in equations unrelated to gases.
 +
 
 +
==Specific (or individual) gas constant==
  
===Boltzmann constant===
+
The '''specific gas constant''' or '''individual gas constant''' of a gas or mixture of gases (''R<sub>gas</sub>'' or just ''R'') is given by the universal gas constant, divided by the [[molar mass]] (<math>M</math>) of the gas or mixture. Whereas the universal gas constant is the same for all ideal gases, the specific (or individual) gas constant is applicable to a particular gas (or mixture of gases such as air).<ref name = "toolbox">[http://www.engineeringtoolbox.com/individual-universal-gas-constant-d_588.html The Individual and Universal Gas Constant.] ''The Engineering ToolBox''. Retrieved July 15, 2008.</ref>
The [[Boltzmann constant]] ''k<sub>B</sub>'' (often abbreviated ''k'') may be used in place of the other forms of the ideal gas constant by working in pure particle count rather than number of moles of gas; this simply requires carrying a factor of [[Avogadro constant|Avogadro's number]]. Writing:
 
:<math>k_B = \frac{R}{N_A}</math>
 
  
One can then express the ideal gas law in direct terms of Boltzmann's constant:
+
The equation to calculate the specific gas constant for a particular gas is as follows:
:<math>\qquad PV=Nk_BT</math>
+
:<math> R_{\rm gas} = \frac{\bar{R}}{M} </math>
 +
where:
 +
:<math>R_{\rm gas}\,\!</math> is the specific gas constant
 +
:<math>\bar{R}</math> is the universal gas constant
 +
:<math>M\,\!</math> is the molar mass (or molecular weight) of the gas
  
===Specific gas constant===
+
In the SI system, the units for the specific gas constant are J·kg<sup>-1</sup>·K<sup>-1</sup>; and in the imperial system, the units are ft·lb·°R<sup>-1</sup>·[[slug (unit)|slug]]<sup>-1</sup>.<ref>To calculate the value of the specific gas constant of a gas in SI units, one should divide the value of the universal gas constant (in SI units) by the molar mass (or molecular weight) of the gas in kilograms per mole.</ref>
  
The '''specific gas constant''' of a gas or a mixture of gases ( <math>\bar{R} </math> ) is given by the universal gas constant, divided by the [[molar mass]] ( <math>M</math> ) of the gas/mixture.
+
The specific gas constant is often represented by the symbol ''R'', and it could then be confused with the universal gas constant. In such cases, the context and/or units of ''R'' should make it clear as to which gas constant is being referred to. For example, the equation for the [[speed of sound#speed in ideal gases and in air|speed of sound]] is usually written in terms of the specific gas constant.
:<math> \bar{R} = \frac{R}{M} </math>
 
  
It is common to represent the specific gas constant by the symbol <math>R</math>. In such cases the context and/or units of <math>R</math> should make it clear as to which gas constant is being referred to. For example, the equation for the [[speed of sound#speed in ideal gases and in air|speed of sound]], is usually written in terms of the specific gas constant.
+
The values of the individual gas constant for air and some other common gases are given in the table below.<ref name = "toolbox"/>
  
The specific gas constant of dry [[air]] is
+
{|  class="wikitable" style="left;"
:<math>R_\mathrm{dry\,air} = 287.05 \frac{\mbox{J}}{\mbox{kg} \cdot \mbox{K}}</math>
+
! Gas
 +
! Individual Gas Constant <br /> SI Units <br /> (J·kg<sup>-1</sup>·K<sup>-1</sup>)
 +
! Individual Gas Constant <br /> Imperial Units <br /> (ft·lb·°R<sup>-1</sup>·slug<sup>-1</sup>)
 +
|-
 +
| Air
 +
| 286.9
 +
| 1,716
 +
|-
 +
| Carbon dioxide (CO<sub>2</sub>)
 +
| 188.9
 +
| 1,130
 +
|-
 +
| Helium (He)
 +
| 2,077
 +
| 12,420
 +
|-
 +
| Hydrogen (H<sub>2</sub>)
 +
| 4,124
 +
| 24,660
 +
|-
 +
| Methane (CH<sub>4</sub>)
 +
| 518.3
 +
| 3,099
 +
|-
 +
| Nitrogen (N<sub>2</sub>)
 +
| 296.8
 +
| 1,775
 +
|-
 +
| Oxygen (O<sub>2</sub>)
 +
| 259.8
 +
| 1,554
 +
|-
 +
| Water vapor (H<sub>2</sub>O)
 +
| 461.5
 +
| 2,760
 +
|}
  
 
==US Standard Atmosphere==
 
==US Standard Atmosphere==
The [[US Standard Atmosphere]], 1976 (USSA1976) defines the Universal Gas Constant (R) as:<ref>[http://www.sworld.com.au/steven/space/atmosphere/ "Standard Atmospheres". ''Sworld.com.au''. Retrieved December 2, 2007</ref><ref name="USSA1976">[http://ntrs.nasa.gov/archive/nasa/casi.ntrs.nasa.gov/19770009539_1977009539.pdf "U.S. Standard Atmosphere"], 1976, U.S. Government Printing Office, Washington, D.C. Retrieved December 2, 2007.</ref>
+
The [[US Standard Atmosphere]], 1976 (USSA1976) defines the Universal Gas Constant as:<ref>[http://www.sworld.com.au/steven/space/atmosphere/ Standard Atmospheres.] Retrieved July 15, 2008.</ref><ref name="USSA1976">[http://ntrs.nasa.gov/archive/nasa/casi.ntrs.nasa.gov/19770009539_1977009539.pdf U.S. Standard Atmosphere, 1976.] National Oceanic and Atmospheric Administration; National Aeronautics and Space Administration; United States Air Force. Retrieved July 15, 2008.</ref>
  
:<math>R = 8.31432\mbox{ x }10^3 \frac{\mathrm{N \cdot m}}{\mathrm{kmol \cdot K}} </math>
+
:<math>\bar{R} = 8.31432\times 10^3 \frac{\mathrm{N \cdot m}}{\mathrm{kmol \cdot K}} </math>
  
The USSA1976 does recognize, however, that this value is not consistent with the cited values for the Avogadro constant and the Boltzmann constant.<ref name="USSA1976"/> Still, the USSA1976 uses this value of R for all the calculations of the standard atmosphere. This disparity is not a significant departure from accuracy.  When using the [[International Organization for Standardization | ISO]] value of R, the calculated pressure increases by only 0.62 pascals at 11,000 meters (the equivalent of a difference of only 0.174 meters or 6.8 inches) and an increase of 0.292 pascals at 20,000 meters (the equivalent of a difference of only 0.338 meters or 13.2 inches).
+
The USSA1976 does recognize, however, that this value is not consistent with the cited values for the [[Avogadro constant]] and the Boltzmann constant.<ref name="USSA1976"/> This disparity is not a significant departure from accuracy, and USSA1976 uses this value of ''R'' for all the calculations of the standard atmosphere. When using the [[International Organization for Standardization|ISO]] value of ''R'', the calculated pressure increases by only 0.62 pascals at 11,000 meters (the equivalent of a difference of only 0.174 meters, or 6.8 inches) and an increase of 0.292 pascals at 20,000 meters (the equivalent of a difference of only 0.338 meters, or 13.2 inches).
  
 
== See also ==
 
== See also ==
* [[Boltzmann constant]]
 
  
==Notes==
+
* [[Earth's atmosphere]]
 +
* [[Gas]]
 +
* [[Mole (unit)]]
 +
* [[Pressure]]
 +
* [[Temperature]]
 +
* [[Volume]]
  
<!--See [[Wikipedia:Footnotes]] for an explanation of how to generate footnotes using the <ref(erences/)> tags—>
+
== Notes ==
 
<references/>
 
<references/>
 +
 +
==References==
 +
* American Institute of Chemical Engineers. ''Ideal Gas Law, Enthalpy, Heat Capacity, Heats of Solution and Mixing.'' New York: American Institute of Chemical Engineers, 1984. ISBN 0816902607.
 +
* Atkins, Peter, and Loretta Jones. ''Chemical Principles: The Quest for Insight,'' 4th ed. New York: W.H. Freeman, 2008. ISBN 0716799030.
 +
* Chang, Raymond. ''Chemistry,'' 9th ed. New York: McGraw-Hill Science/Engineering/Math, 2006. ISBN 0073221031.
 +
* Cotton, F. Albert, and Geoffrey Wilkinson. ''Advanced Inorganic Chemistry,'' 4th ed. New York: Wiley, 1980. ISBN 0471027758.
 +
* McMurry, J., and R.C. Fay. ''Chemistry,'' 4th ed. Upper Saddle River, NJ: Prentice Hall, 2004. ISBN 0131402080.
  
 
== External links ==
 
== External links ==
 +
All links retrieved April 17, 2024.
  
All links retrieved December 2, 2007
+
* [http://www.engineeringtoolbox.com/individual-universal-gas-constant-d_588.html The Individual and Universal Gas Constant.] The Engineering ToolBox.
  
* [http://physics.nist.gov/cgi-bin/cuu/Value?r|search_for=gas+constant Gas Constant CODATA Value] at [[NIST]]
 
* [http://physics.nist.gov/cgi-bin/cuu/Value?k|search_for=boltzmann Boltzmann Constant CODATA Value] at [[NIST]]
 
  
 
[[Category:Physical sciences]]
 
[[Category:Physical sciences]]
 
[[Category:Physics]]
 
[[Category:Physics]]
 +
[[Category:Chemistry]]
  
{{credit|172490929}}
+
{{credits|225748431}}

Latest revision as of 04:37, 18 April 2024

Values of R Units
(V·P·T-1·n-1)
8.314472 J·K-1·mol-1
0.0820574587 L·atm·K-1·mol-1
8.20574587 × 10-5 m3·atm·K-1·mol-1
8.314472 cm3·MPa·K-1·mol-1
8.314472 L·kPa·K-1·mol-1
8.314472 m3·Pa·K-1·mol-1
62.36367 L·mmHg·K-1·mol-1
62.36367 L·Torr·K-1·mol-1
83.14472 L·mbar·K-1·mol-1
1.987 cal·K-1·mol-1
6.132440 lbf·ft·K-1·g-mol-1
10.73159 ft3·psi· °R-1·lb-mol-1
0.7302413 ft3·atm·°R-1·lb-mol-1
998.9701 ft3·mmHg·K-1·lb-mol-1
8.314472 × 107 erg·K-1·mol-1

The gas constant (also known as the molar, universal, or ideal gas constant) is a physical constant that is featured in a number of fundamental equations in the physical sciences, such as the ideal gas law and the Nernst equation. It is expressed in units of energy (that is, the pressure-volume product) per kelvin per mole. It is equivalent to the Boltzmann constant, except that the latter is expressed in units of energy per kelvin per particle.

Denoted by the symbol R, the value of the gas constant is:

R = 8.314472(15) J · K-1 · mol-1

The two digits in parentheses indicate the uncertainty (standard deviation) in the last two digits of the value.

Movement of particles (atoms, molecules, or ions) in the gas phase. The gas constant is a factor in the ideal gas law, which provides an approximation of some of the properties of gases.

Ideal gas law

An ideal gas (or "perfect" gas) is a hypothetical gas consisting of a very large number of identical particles, each of zero volume, uniformly distributed in density, with no intermolecular forces. Additionally, the molecules or atoms of the gas have complete randomness of direction and velocity, and they undergo perfectly elastic collisions with the walls of the container. The molecules of an ideal gas are often compared to rigid but elastic billiard balls.

The gas constant occurs in the ideal gas law (the simplest equation of state) as follows:

where:

is the absolute pressure
is absolute temperature
is the volume the gas occupies
is the amount of gas (in terms of the number of moles of gas)
is the molar volume

This equation does not exactly apply to real gases, because each molecule of a real gas does occupy a certain volume and the molecules are subject to intermolecular forces. Nonetheless, this equation is used as an approximation when describing the behavior of a real gas, except when the gas is at high pressures or low temperatures.

Relationship with the Boltzmann constant

The Boltzmann constant kB (often abbreviated k) has the value 1.3807 x 10-23 J.K-1. It may be used in place of the universal gas constant by working in pure particle count, N, rather than number of moles, n, since

,

where is Avogadro's number (= 6.022 x 1023 particles per mole).

In terms of Boltzmann's constant, the ideal gas law may be written as:

where N is the number of particles (atoms or molecules) of the ideal gas.

Given its relationship with the Boltzmann constant, the ideal gas constant also appears in equations unrelated to gases.

Specific (or individual) gas constant

The specific gas constant or individual gas constant of a gas or mixture of gases (Rgas or just R) is given by the universal gas constant, divided by the molar mass () of the gas or mixture. Whereas the universal gas constant is the same for all ideal gases, the specific (or individual) gas constant is applicable to a particular gas (or mixture of gases such as air).[1]

The equation to calculate the specific gas constant for a particular gas is as follows:

where:

is the specific gas constant
is the universal gas constant
is the molar mass (or molecular weight) of the gas

In the SI system, the units for the specific gas constant are J·kg-1·K-1; and in the imperial system, the units are ft·lb·°R-1·slug-1.[2]

The specific gas constant is often represented by the symbol R, and it could then be confused with the universal gas constant. In such cases, the context and/or units of R should make it clear as to which gas constant is being referred to. For example, the equation for the speed of sound is usually written in terms of the specific gas constant.

The values of the individual gas constant for air and some other common gases are given in the table below.[1]

Gas Individual Gas Constant
SI Units
(J·kg-1·K-1)
Individual Gas Constant
Imperial Units
(ft·lb·°R-1·slug-1)
Air 286.9 1,716
Carbon dioxide (CO2) 188.9 1,130
Helium (He) 2,077 12,420
Hydrogen (H2) 4,124 24,660
Methane (CH4) 518.3 3,099
Nitrogen (N2) 296.8 1,775
Oxygen (O2) 259.8 1,554
Water vapor (H2O) 461.5 2,760

US Standard Atmosphere

The US Standard Atmosphere, 1976 (USSA1976) defines the Universal Gas Constant as:[3][4]

The USSA1976 does recognize, however, that this value is not consistent with the cited values for the Avogadro constant and the Boltzmann constant.[4] This disparity is not a significant departure from accuracy, and USSA1976 uses this value of R for all the calculations of the standard atmosphere. When using the ISO value of R, the calculated pressure increases by only 0.62 pascals at 11,000 meters (the equivalent of a difference of only 0.174 meters, or 6.8 inches) and an increase of 0.292 pascals at 20,000 meters (the equivalent of a difference of only 0.338 meters, or 13.2 inches).

See also

Notes

  1. 1.0 1.1 The Individual and Universal Gas Constant. The Engineering ToolBox. Retrieved July 15, 2008.
  2. To calculate the value of the specific gas constant of a gas in SI units, one should divide the value of the universal gas constant (in SI units) by the molar mass (or molecular weight) of the gas in kilograms per mole.
  3. Standard Atmospheres. Retrieved July 15, 2008.
  4. 4.0 4.1 U.S. Standard Atmosphere, 1976. National Oceanic and Atmospheric Administration; National Aeronautics and Space Administration; United States Air Force. Retrieved July 15, 2008.

References
ISBN links support NWE through referral fees

  • American Institute of Chemical Engineers. Ideal Gas Law, Enthalpy, Heat Capacity, Heats of Solution and Mixing. New York: American Institute of Chemical Engineers, 1984. ISBN 0816902607.
  • Atkins, Peter, and Loretta Jones. Chemical Principles: The Quest for Insight, 4th ed. New York: W.H. Freeman, 2008. ISBN 0716799030.
  • Chang, Raymond. Chemistry, 9th ed. New York: McGraw-Hill Science/Engineering/Math, 2006. ISBN 0073221031.
  • Cotton, F. Albert, and Geoffrey Wilkinson. Advanced Inorganic Chemistry, 4th ed. New York: Wiley, 1980. ISBN 0471027758.
  • McMurry, J., and R.C. Fay. Chemistry, 4th ed. Upper Saddle River, NJ: Prentice Hall, 2004. ISBN 0131402080.

External links

All links retrieved April 17, 2024.

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