314870
At \({\text{320 K,}}\) a gas \({{\text{A}}_{\text{2}}}\) is \({\rm{20}}\% \) dissociated to \({\rm{A(g)}}\). The standard free energy change at \(320 \mathrm{~K}\) and \(1 \mathrm{~atm}\) in \({\text{J}}\,{\text{mo}}{{\text{l}}^{{\text{ - 1}}}}\) is approximately:
\({\text{(R = 8}}{\text{.314J }}{{\text{K}}^{{\text{ - 1}}}}\;{\text{mo}}{{\text{l}}^{{\text{ - 1}}}}{\text{; ln2 = 0}}{\text{.693 ; ln3 = 1}}{\text{.098)}}\)
314870
At \({\text{320 K,}}\) a gas \({{\text{A}}_{\text{2}}}\) is \({\rm{20}}\% \) dissociated to \({\rm{A(g)}}\). The standard free energy change at \(320 \mathrm{~K}\) and \(1 \mathrm{~atm}\) in \({\text{J}}\,{\text{mo}}{{\text{l}}^{{\text{ - 1}}}}\) is approximately:
\({\text{(R = 8}}{\text{.314J }}{{\text{K}}^{{\text{ - 1}}}}\;{\text{mo}}{{\text{l}}^{{\text{ - 1}}}}{\text{; ln2 = 0}}{\text{.693 ; ln3 = 1}}{\text{.098)}}\)
314870
At \({\text{320 K,}}\) a gas \({{\text{A}}_{\text{2}}}\) is \({\rm{20}}\% \) dissociated to \({\rm{A(g)}}\). The standard free energy change at \(320 \mathrm{~K}\) and \(1 \mathrm{~atm}\) in \({\text{J}}\,{\text{mo}}{{\text{l}}^{{\text{ - 1}}}}\) is approximately:
\({\text{(R = 8}}{\text{.314J }}{{\text{K}}^{{\text{ - 1}}}}\;{\text{mo}}{{\text{l}}^{{\text{ - 1}}}}{\text{; ln2 = 0}}{\text{.693 ; ln3 = 1}}{\text{.098)}}\)
314870
At \({\text{320 K,}}\) a gas \({{\text{A}}_{\text{2}}}\) is \({\rm{20}}\% \) dissociated to \({\rm{A(g)}}\). The standard free energy change at \(320 \mathrm{~K}\) and \(1 \mathrm{~atm}\) in \({\text{J}}\,{\text{mo}}{{\text{l}}^{{\text{ - 1}}}}\) is approximately:
\({\text{(R = 8}}{\text{.314J }}{{\text{K}}^{{\text{ - 1}}}}\;{\text{mo}}{{\text{l}}^{{\text{ - 1}}}}{\text{; ln2 = 0}}{\text{.693 ; ln3 = 1}}{\text{.098)}}\)
314870
At \({\text{320 K,}}\) a gas \({{\text{A}}_{\text{2}}}\) is \({\rm{20}}\% \) dissociated to \({\rm{A(g)}}\). The standard free energy change at \(320 \mathrm{~K}\) and \(1 \mathrm{~atm}\) in \({\text{J}}\,{\text{mo}}{{\text{l}}^{{\text{ - 1}}}}\) is approximately:
\({\text{(R = 8}}{\text{.314J }}{{\text{K}}^{{\text{ - 1}}}}\;{\text{mo}}{{\text{l}}^{{\text{ - 1}}}}{\text{; ln2 = 0}}{\text{.693 ; ln3 = 1}}{\text{.098)}}\)