If the boundary of system moves by an infinitesimal amount, the work involved is given by dw= -P_("ext") dV, for irreversible process W= -P_("ext") Delta V (where Delta V= V_(f) - V_(i)). For reversible process. P_("ext") = P_("int") +- dP ~= P_("int"), so for reversible isothermal process W = -nRT "In" (V_(f))/(V_(i)) 2 mole of an ideal gas undergoes isothermal compression along three different paths: (i) reversible compression from P_(i) = 2 bar and V_(i) = 8L " to" P_(f) = 20 bar (ii) a single stage compression against a constant external pressure of 20 bar (iii) a two stage compression consisting initially of compression against a constant external pressure of 10 bar until P_("gas") = P_("ext"), followed by compression aganist a constant pressure of 20 bar until P_("gas") = P_("ext") Order of magnitude work is

If the boundary of system moves by an infinitesimal amount, the work i

1.	If the boundary of system moves by an infinitesimal amount, the work involved is given by dw= -P_("ext") dV, for irreversible process W= -P_("ext") Delta V (where Delta V= V_(f) - V_(i)). For reversible process. P_("ext") = P_("int") +- dP ~= P_("int"), so for reversible isothermal process W = -nRT "In" (V_(f))/(V_(i)) 2 mole of an ideal gas undergoes isothermal compression along three different paths: (i) reversible compression from P_(i) = 2 bar and V_(i) = 8L " to" P_(f) = 20 bar (ii) a single stage compression against a constant external pressure of 20 bar (iii) a two stage compression consisting initially of compression against a constant external pressure of 10 bar until P_("gas") = P_("ext"), followed by compression aganist a constant pressure of 20 bar until P_("gas") = P_("ext") Order of magnitude work is
Answer» `w_(1) gt w_(2) gt w_(3)` `w_(3) gt w_(2) gt w_(1)` `w_(2) gt w_(3) gt w_(1)` `w_(1) = w_(2) = w_(3)` SOLUTION :`W_("REV")` compression `lt W_("irr")` Less the STEPS, HIGHER the W