Question #79364

Two litres of hydrogen at a pressure of 10^5 Pa expands adiabatically to 1.5 times the initial volume. Find the work done?

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Answer on Question #79364 - Physics - Molecular Physics / Thermodynamics

Question: Two litres of hydrogen at a pressure of 10510^{\wedge}5 Pa expands adiabatically to 1.5 times the initial volume. Find the work done?

Answer:

The first law of thermodynamics [1] can be formulated in the following way:


Q=ΔU+A,Q = \Delta U + A,


where QQ is the amount of heat supplied to the system, ΔU\Delta U is the change in the internal energy of the system, AA is the work done by the system. For adiabatic process Q=0Q = 0, so that the work can be done due to the loss of the internal energy only:


A=ΔU.A = - \Delta U.


Hydrogen is a diatomic (ideal) gas, and each of its molecules possesses i=5i = 5 degrees of freedom. Hence, the change in its internal energy should be written as:


ΔU=52νR(T2T1).\Delta U = \frac {5}{2} \nu R \left(T _ {2} - T _ {1}\right).


According to Mendeleev-Clapeyron equation


p1V1=νRT1,p _ {1} V _ {1} = \nu R T _ {1},p2V2=νRT2,p _ {2} V _ {2} = \nu R T _ {2},


Hence,


νR(T2T1)=p2V2p1V1.\nu R \left(T _ {2} - T _ {1}\right) = p _ {2} V _ {2} - p _ {1} V _ {1}.


There is also one more useful relation for the adiabatic processes:


pVγ=Const,p V ^ {\gamma} = \text{Const},


where γ\gamma is the adiabatic index (= heat capacity ratio). For diatomic ideal gases γ=75\gamma = \frac{7}{5} (see [2] for details).

As a result, one can show that:


p2=p1(V1V2)γ.p _ {2} = p _ {1} \left(\frac {V _ {1}}{V _ {2}}\right) ^ {\gamma}.


Combining (2)-(3), (5), (7) together and taking into account the relation V2=1.5V1=32V1V_{2} = 1.5V_{1} = \frac{3}{2} V_{1}, we deduce


A=52(p2V2p1V1)=52p1V1[1(V1V2)y1]=52p1V1[1(23)2/5].A = - \frac {5}{2} \left(p _ {2} V _ {2} - p _ {1} V _ {1}\right) = \frac {5}{2} p _ {1} V _ {1} \left[ 1 - \left(\frac {V _ {1}}{V _ {2}}\right) ^ {y - 1} \right] = \frac {5}{2} p _ {1} V _ {1} \left[ 1 - \left(\frac {2}{3}\right) ^ {2 / 5} \right].


Substituting the numerical values, we obtain:


A521052103(10.85)=425J.A \approx \frac {5}{2} \cdot 1 0 ^ {5} \cdot 2 \cdot 1 0 ^ {- 3} (1 - 0. 8 5) = 4 2 5 J.


[1] (Electronic resource) https://en.wikipedia.org/wiki/First_law_of_thermodynamics

[2] (Electronic resource) https://en.wikipedia.org/wiki/Heat_capacity_ratio

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