Since entropy is a state variable, then we can divide the pathway into 2 consercutive path.
The first path involves constant temperature, ie. 120K, 4atm to 120K, 1atm
The second path involves constant pressure, ie. 120K, 1atm to 90K, 1atm.
dSsys = nRln(P1/P2) + nCpln(T2/T1)
The expression in bold represents the first path.
The underlined expression represents the second path.
Hope this clears things up for you.