Molekularno – kinetički opis idealnog plina - 2.

${\bar{E}}_{\mathrm{k}\mathrm{i}\mathrm{n}}=\frac{2}{3}RT\backslash bar\{E\}\_\{\backslash mathrm\{kin\}\}=\backslash frac\{2\}\{3\}\; R\; T$

${\bar{E}}_{\mathrm{k}\mathrm{i}\mathrm{n}}=\frac{3}{2}RT\backslash bar\{E\}\_\{\backslash mathrm\{kin\}\}=\backslash frac\{3\}\{2\}\; R\; T$

${\bar{E}}_{\text{kin }}=\frac{2}{3}{k}_{\mathrm{B}}T\backslash bar\{E\}\_\{\backslash text\; \{kin\; \}\}=\backslash frac\{2\}\{3\}\; k\_\{\backslash mathrm\{B\}\}\; T$

${\bar{E}}_{\text{kin }}=\frac{3}{2}{k}_{\mathrm{B}}T\backslash bar\{E\}\_\{\backslash text\; \{kin\; \}\}=\backslash frac\{3\}\{2\}\; k\_\{\backslash mathrm\{B\}\}\; T$