We have the state relation -
"TdS=dU+PdV"
R=8.314Jmol−1
"\u200b\\frac{V2}{V1}" =10
Since expansion is isothermal, there will be no change in temperature and consequently no change in internal energy ("dU = 0" ).
It reduces to -
"ds=\\frac{PdV}{T}"
From ideal gas relation, "Pv= nRT"
"dS=\\frac{nRdV}{V}\n\u200b"
"S 2\u2212S1 =nRln( \\frac{V1}{V2}\n\u200b\n\u200b\t\n \n\u200b\t\n )"
n = 1 (1 mole of gas), R=8.314Jmol-1K,
S2−S1=8.314×ln(10)
⟹S2−S1=19.15K-1mole-1
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