Adiabatic process is a process in which a thermodynamic system does not exchange heat or substance with its surroundings. Hence, in the given adiabatic compression, the heat transfer Q is equal to zero.
The first quantity we can determine is the work done by the system on its surroundings. It is calculated by taking the following integral:
W=∫V1V2pdV, where p is pressure, and V1=0.2m3 and V2=0.05m3 is the initial and final volume, respectively. The pressure as a function of volume is provided by the conditions of the problem: pV1.3=const=p1V11.3, where p1=0.5MPa=0.5×106N/m2 is the initial pressure. Hence,
p=p1(VV1)1.3.Substituting this into the above integral and performing the elementary integration, we obtain
W=0.3p1V1[1−(V2V1)0.3]≈−1.72×105J,where we have taken into account that N⋅m=J. Thus, the positive work is actually done by the surroundings on the system.
The change ΔU in the internal energy of the system is determined from the first law of thermodynamics:
ΔU=Q−W=−W=1.72×105J, since Q=0.
The enthalpy of a system is defined as H=U+pV. The change in enthalpy in the given process is, therefore,
ΔH=ΔU+p2V2−p1V1.
To find the product p2V2, we use the equation p2V21.3=p1V11.3, whence p2V2=p1V1(V1/V2)0.3. Eventually,
ΔH=ΔU+p1V1[(V2V1)0.3−1]=−W−0.3W=−1.3W≈2.24×105J.
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