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Work is the mose of transfrence of energ...

Work is the mose of transfrence of energy. If the system involves gaseous substance and there is difference of pressure between system and surroundings, such a work is referred to as pressure - volume work `(W_(PV)= -P_(ext)DeltaV)`. It has been observed that reversible work done by the system is the maximum obtainable work. `w_(rev) gt w_(ir r)`
The works of isothermal and adiabatic processes are different from each other. for isothermal reversible proces,
`W_("isothermal reversible")=2.303 nRT log_(10) (V_(2)/V_(1))`
`W_("adiabatic reversible")=C_(V) (T_(1)-T_(2))`
A thermodynamic system goes in acyclic process as represented in the following `P-V` diagram:
1. For an ideal gas, consider only `P-V` work in going from an initial state

The net work done during the complete cycle is given by the area:

A

Cycle ACBDA

B

`A A_(1)B_(1)BDA`

C

`A A_(2)B_(2)B`

D

Half of area bonded by curve.

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The correct Answer is:
A
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Work is the mose of transfrence of energy. If the system involves gaseous substance and there is difference of pressure between system and surroundings, such a work is referred to as pressure - volume work (W_(PV)= -P_(ext)DeltaV) . It has been observed that reversible work done by the system is the maximum obtainable work. w_(rev) gt w_(ir r) The works of isothermal and adiabatic processes are different from each other. for isothermal reversible proces, W_("isothermal reversible")=2.303 nRT log_(10) (V_(2)/V_(1)) W_("adiabatic reversible")=C_(V) (T_(1)-T_(2)) Calculate work done when 1 mole of an ideal gas is expended reversibly from 20 L to 40 L at a constant temperature of 300 K.

if work is done by the system then W is

The pressure-volume of varies 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 network done during the complete cycle is given by the area

The pressure-volume of varies 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)) P-V plots for two gases during adiabatic processes are given in the given figure: Plot D and Plot C should correspond to

The pressure-volume of varies 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)) Calculate work done when 1 mole of an ideal gas is expanded reversibly form 30L to 60L at a constant temperature of 300k

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The pressure-volume of varies 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)) The q value and work done in isothermal reversible expansion of one mole of an ideal gas from initial pressure of 1 bar to final pressure of 0.1 bar at constant temperature 273K are:

The pressure-volume of varies 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)) If w_(1),w_(2),w_(3) and w_(4) are work done in isothermal, adiabatic, isobaric, and isochoric reversible processes, respectively then the correct sequence (for expansion) would be