To solve this problem related to the thermodynamics of an ideal gas, let's consider the concepts involved:
Isothermal Process: An isothermal process is one in which the temperature \(T\) of the system remains constant. For an ideal gas undergoing an isothermal process, the internal energy change \(\Delta U\) is zero because internal energy of an ideal gas depends only on temperature, which is unchanged. Hence, \(\Delta U = 0\).
Entropy Change (\(\Delta S\)): The entropy change for an ideal gas undergoing an isothermal expansion from volume \(V_i\) to volume \(V_f = 2V_i\) is given by:
\(\Delta S = nR \ln \frac{V_f}{V_i}\)
Since \(V_f = 2V_i\), this becomes \(\Delta S = nR \ln 2\). Since \( \ln 2 > 0 \), it follows that \(\Delta S > 0\).
Helmholtz Free Energy Change (\(\Delta F\)): The Helmholtz free energy change is defined as:
\(\Delta F = \Delta U - T\Delta S\)
With \(\Delta U = 0\), the equation simplifies to \(\Delta F = -T\Delta S\). Since \(\Delta S > 0\), it follows that \(\Delta F < 0\).
Therefore, the correct statements are: \(\Delta S > 0\), \(\Delta U = 0\), and \(\Delta F < 0\).
Thus, the correct option is:
\(\Delta S > 0\), \(\Delta U = 0\), \(\Delta F < 0\)
One mole of an ideal gas expands isothermally and reversibly from $10 \mathrm{dm}^{3}$ to $20 \mathrm{dm}^{3}$ at $300 \mathrm{~K} . \Delta \mathrm{U}$, q and work done in the process respectively are : Given : $\mathrm{R}=8.3 \mathrm{JK}^{-1}$ and $\mathrm{mol}^{-1}$ In $10=2.3$ $\log 2=0.30$ $\log 3=0.48$
