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")` Work done (in bar -L) on the gas in reversible isothermal compression is:
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 infinitiesimal amount, the work involved is given by dw= -P_("ext") dV, for irreversible process W= -P_("ext") Delta V (where DeltaV= V_(f)- V_(i) ). For reversible process P_("ext") = P_("int") +- dP ~~ P_("int") , so for reversible isothermal process W= -nRT ln (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)= 8 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 against a constant pressure of 20 bar until P_("gas") = P_("ext") . Total work done on the gas in two stage compression is
Derive the equation for 'W_("rev")' in isothermal reversible process.
During expansion of a gas into vaccum (P_("ext")=0) , Work done is zero if the process is (A) Reversible (B) Irreversible (C ) Isothermal
q=w=-p_(ext)(v_(f)-v_(i)) is for irreversible…. Change.
NARENDRA AWASTHI-THERMODYNAMICS-Level 3 - Match The Column