In an adiabatic process, heat exchange is absent, and work performed is contingent upon the volume alteration. This is quantified by the equation:\[W = \int_{V_i}^{V_f} P \, dV\]where \( P \) signifies pressure, and \( V_i \) and \( V_f \) represent the initial and final volumes, respectively.Consequently, the work performed is dictated by the volume change.