A gas is enclosed in a cylinder with a movable frictionless piston. Its initial thermodynamic state at
pressure P
i
= 10
5
Pa and volume V
i
= 10
-3
m
3
changes to a final state at P
f
= \left( {{1 \over {32}}} \right) \times {10^5}\,Pa and
V
f
= 8 \times 10
-3
m
3
in an adiabatic quasi-static process, such that P
3
V
5
= constant. Consider another
thermodynamic process that brings the system from the same initial state to the same final state in two
steps: an isobaric expansion at P
i
followed by an isochoric (isovolumetric) process at volume V
f
. The amount of heat supplied to the system in the two-step process is approximately