ISOBARIC PROCESS
 
 
AT CONSTANT PREESURE
 
   Heat supplied at constant pressure is also known as "ISOBARIC PROCESS". An isobaric process is one in    which no pressure change takes place during the supply of heat to system.
   In order to understand an isobaric process consider a cylinder fitted with a frictionless piston, the piston    is free to move. An ideal gas is enclosed in the cylinder.
   Let the internal energy of the system at initial state is E1, the temperature of system is T1, volume of    gas is V1 and pressure is P.
   If qp amount of heat is supplied to the system, its internal energy will increase from E1 to E2 and the    temperature of system also rises from T1 to T2,
   At the same time gas exerts some pressure on the piston, since the piston is free to move, it displaces    by "h" the volume of gas increases from V1 to V2 . Due to increase in volume, pressure again decreases    to its original value i.e. P1.
   ACCORDING TO THE FIRST LAWOFTHERMODYNAMICS
 Qp = DE + work    
Qp = DE + P DV   
                                                       Qp = DE + P DV         but (DE = E2- E1)                      
               Qp = E2-E1 + P (V2 – V1)
           Qp = E2-E1 + PV2- PV1
              Qp = E2+ PV2 – E1 – PV1

                       Qp = (E2+ PV2) – (E1+ PV1)
 
but
(E + PV =H)
(H= enthalpy)
therefore,
qP = D H
OR
q p = DE + P DV =D H
CONCLUSION
 
   This expression indicates that heat supplied at constant pressure is equal to increase in enthalpy of    system.
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