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AT
CONSTANT PREESURE
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| 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. | ||||
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| 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 | ||||
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Qp
= DE + work
Qp = DE + P DV Qp = DE + P DV but (DE = E2- E1) |
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Qp
= E2-E1 + P (V2 – V1)
Qp = E2-E1 + PV2- PV1 Qp = E2+ PV2 – E1 – PV1 Qp = (E2+ PV2) – (E1+ PV1) |
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but
(E + PV =H) (H= enthalpy) therefore, qP = D H OR q p = DE + P DV =D H |
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CONCLUSION
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| This expression indicates that heat supplied at constant pressure is equal to increase in enthalpy of system. | ||||
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