The pressure-volume of various thermodynamic process is shown in graphs: Work is the mole of transference of energy. It has been observed that reversible work done by the system is the maximum obtainable work. `w_(rev) gt w_(irr)` The works of isothermal and adiabatic processes are different from each other. `w_("isothermal reversible") = 2.303 nRT log_(10) ((V_(2))/(V_(1)))` `= 2.303 nRT log_(10)((P_(2))/(P_(1)))` `w_("adiabatic reversible") = C_(V) (T_(1)-T_(2))` A thermodynamic system goes in a cyclic process as represented in the following `P -V` diagram: The net work done during the complete cycle is given by the areaA. cycle ACBDAB. `A A_(1),B_(1)BDA`C.D. `A A_(2)B_(2)B`

The pressure-volume of various thermodynamic process is shown in graph

1.	The pressure-volume of various thermodynamic process is shown in graphs: Work is the mole of transference of energy. It has been observed that reversible work done by the system is the maximum obtainable work. `w_(rev) gt w_(irr)` The works of isothermal and adiabatic processes are different from each other. `w_("isothermal reversible") = 2.303 nRT log_(10) ((V_(2))/(V_(1)))` `= 2.303 nRT log_(10)((P_(2))/(P_(1)))` `w_("adiabatic reversible") = C_(V) (T_(1)-T_(2))` A thermodynamic system goes in a cyclic process as represented in the following `P -V` diagram: The net work done during the complete cycle is given by the areaA. cycle ACBDAB. `A A_(1),B_(1)BDA`C.D. `A A_(2)B_(2)B`
Answer» Correct Answer - A w=work done=Area under curve.

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