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Gas constant
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== Dimensions == From the ideal gas law ''PV'' = ''nRT'' we get : <math>R = \frac{PV}{nT},</math> where ''P'' is pressure, ''V'' is volume, ''n'' is number of moles of a given substance, and ''T'' is [[temperature]]. As pressure is defined as force per area of measurement, the gas equation can also be written as : <math>R = \frac{ \dfrac{\text{force}}{\text{area}} \times \text{volume} } { \text{amount} \times \text{temperature} }. </math> Area and volume are (length)<sup>2</sup> and (length)<sup>3</sup> respectively. Therefore: : <math>R = \frac{ \dfrac{\text{force} }{ (\text{length})^2} \times (\text{length})^3 } { \text{amount} \times \text{temperature} } = \frac{ \text{force} \times \text{length} } { \text{amount} \times \text{temperature} }. </math> Since force Γ length = work, : <math>R = \frac{ \text{work} } { \text{amount} \times \text{temperature} }. </math> The physical significance of ''R'' is work per mole per kelvin. It may be expressed in any set of units representing work or energy (such as [[joule]]s), units representing temperature on an absolute scale (such as [[kelvin]] or [[Rankine scale|rankine]]), and any system of units designating a mole or a similar pure number that allows an equation of macroscopic mass and fundamental particle numbers in a system, such as an ideal gas (see [[Avogadro constant]]). Instead of a mole the constant can be expressed by considering the [[normal cubic metre]]. Otherwise, we can also say that : <math>\text{force} = \frac{ \text{mass} \times \text{length} } { (\text{time})^2 }. </math> Therefore, we can write ''R'' as : <math>R = \frac{ \text{mass} \times \text{length}^2 } { \text{amount} \times \text{temperature} \times (\text{time})^2 }. </math> And so, in terms of [[SI base units]], : ''R'' = {{physconst|R|unit=kgβ m<sup>2</sup>β s<sup>β2</sup>β K<sup>β1</sup>β mol<sup>β1</sup>|ref=no}}.
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