Final Answer:
The entropy change (ΔS) when one mole of a perfect gas is expanded isothermally and reversibly from an initial pressure of 1.00 bar to a final pressure of 0.100 bar is -8.314 J/mol·K * ln(0.100/1.00) = -18.27 J/mol·K.
Step-by-step explanation:
In an isothermal and reversible expansion of a perfect gas, we use the equation for infinitesimal change in entropy dS = (dq_rev)/T. For an ideal gas undergoing isothermal expansion, dq_rev = pdV. Here, dV is an infinitesimal change in volume, and from the ideal gas law, we know that PV = nRT, so V = (nRT)/P. By differentiating this equation with respect to pressure (dV/dP) at constant temperature, we get dV = -(nRT)/(P^2) dP. Substituting this into the expression for dq_rev gives dq_rev = -nRT dP/P. Thus, dS = (-nRT/P) dP/T = -nR dP/P.
Integrating dS from the initial pressure (P_i = 1.00 bar) to the final pressure (P_f = 0.100 bar), we get ΔS = -nR * ln(P_f/P_i) = - (1 mol) * (8.314 J/mol·K) * ln(0.100/1.00) = -18.27 J/mol·K. This negative entropy change indicates the increase in disorder as the gas expands from higher pressure to lower pressure, aligning with the second law of thermodynamics.
The negative sign signifies that the system (the gas) is losing entropy to its surroundings during this process. The calculation involves utilizing the logarithmic relationship between initial and final pressures to determine the entropy change, emphasizing the directional change in entropy due to the expansion of the gas under isothermal conditions.