Ideal gas: Heat capacity: Difference between revisions
Jump to navigation
Jump to search
Carl McBride (talk | contribs) No edit summary |
Carl McBride (talk | contribs) m (Removed resultbox as it seems to break the MathJax) |
||
| (7 intermediate revisions by the same user not shown) | |||
| Line 1: | Line 1: | ||
:<math> | The [[heat capacity]] at constant volume is given by | ||
:<math>\left. | |||
:<math>C_V = \left. \frac{\partial U}{\partial T} \right\vert_V </math> | |||
where <math>U</math> is the [[internal energy]]. Given that an [[ideal gas]] has no interatomic potential energy, the only term that is important is the [[Ideal gas: Energy | kinetic energy of an ideal gas]], which is equal to <math>(3/2)RT</math>. Thus | |||
:<math>C_V = \frac{\partial ~ }{\partial T} \left( \frac{3}{2}RT \right) = \frac{3}{2} R </math> | |||
At constant [[pressure]] one has | |||
:<math>C_p = \left. \frac{\partial U}{\partial T} \right\vert_p + p \left.\frac{\partial V}{\partial T} \right\vert_p</math> | |||
we can see that, just as before, one has | |||
:<math>\left. \frac{\partial U}{\partial T} \right\vert_p = \frac{3}{2} R </math> | |||
and from the [[Equation of State: Ideal Gas | equation of state of an ideal gas]] | |||
:<math>p \left.\frac{\partial V}{\partial T} \right\vert_p = \frac{\partial }{\partial T} (RT) = R</math> | |||
thus | |||
:<math>C_p = C_v + R = \frac{5}{2} R</math> | |||
where <math>R</math> is the [[molar gas constant]]. | |||
==References== | ==References== | ||
#Donald A. McQuarrie "Statistical Mechanics" (1976) Eq. 1-1 | #Donald A. McQuarrie "Statistical Mechanics" (1976) Eq. 1-1 | ||
#Landau and Lifshitz Course of Theoretical Physics Volume 5 Statistical Physics 3rd Edition Part 1 Equation 42.11 | #Landau and Lifshitz Course of Theoretical Physics Volume 5 Statistical Physics 3rd Edition Part 1 Equation 42.11 | ||
[[Category: Ideal gas]] | [[Category: Ideal gas]] | ||
Latest revision as of 15:34, 11 May 2012
The heat capacity at constant volume is given by
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle C_{V}=\left.{\frac {\partial U}{\partial T}}\right\vert _{V}}
where is the internal energy. Given that an ideal gas has no interatomic potential energy, the only term that is important is the kinetic energy of an ideal gas, which is equal to Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle (3/2)RT} . Thus
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle C_V = \frac{\partial ~ }{\partial T} \left( \frac{3}{2}RT \right) = \frac{3}{2} R }
At constant pressure one has
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle C_p = \left. \frac{\partial U}{\partial T} \right\vert_p + p \left.\frac{\partial V}{\partial T} \right\vert_p}
we can see that, just as before, one has
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left. \frac{\partial U}{\partial T} \right\vert_p = \frac{3}{2} R }
and from the equation of state of an ideal gas
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle p \left.\frac{\partial V}{\partial T} \right\vert_p = \frac{\partial }{\partial T} (RT) = R}
thus
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle C_p = C_v + R = \frac{5}{2} R}
where is the molar gas constant.
References[edit]
- Donald A. McQuarrie "Statistical Mechanics" (1976) Eq. 1-1
- Landau and Lifshitz Course of Theoretical Physics Volume 5 Statistical Physics 3rd Edition Part 1 Equation 42.11