3.6: Capacidades térmicas de um gás ideal
- Page ID
- 184521
Ao final desta seção, você poderá:
- Defina a capacidade térmica de um gás ideal para um processo específico
- Calcule o calor específico de um gás ideal para um processo isobárico ou isocórico
- Explicar a diferença entre as capacidades térmicas de um gás ideal e de um gás real
- Estime a mudança no calor específico de um gás nas faixas de temperatura
Aprendemos sobre calor específico e capacidade térmica molar anteriormente; no entanto, não consideramos um processo no qual o calor é adicionado. Nós fazemos isso nesta seção. Primeiro, examinamos um processo em que o sistema tem um volume constante, depois o contrastamos com um sistema em pressão constante e mostramos como seus calores específicos estão relacionados.
Vamos começar examinando a Figura\(\PageIndex{1}\), que mostra dois vasos A e B, cada um contendo 1 mol do mesmo tipo de gás ideal a uma temperatura T e um volume V. A única diferença entre os dois vasos é que o pistão na parte superior de A é fixo, enquanto o que está no topo de B está livre para se mover contra uma pressão externa constante p. Agora, consideramos o que acontece quando a temperatura do gás em cada recipiente aumenta lentamente\(T + dT\) com a adição de calor.
Since the piston of vessel A is fixed, the volume of the enclosed gas does not change. Consequently, the gas does no work, and we have from the first law
\[dE_{int} = dQ - dW = dQ.\]
We represent the fact that the heat is exchanged at constant volume by writing
\[dQ = C_VndT,\] where \(C_V\) is the molar heat capacity at constant volume of the gas. In addition, since \(dE_{int} = dQ\) for this particular process,
\[dE_{int} = C_VndT. \label{3.9}\]
We obtained this equation assuming the volume of the gas was fixed. However, internal energy is a state function that depends on only the temperature of an ideal gas. Therefore, \(dE_{int} = C_VndT\) gives the change in internal energy of an ideal gas for any process involving a temperature change dT.
When the gas in vessel B is heated, it expands against the movable piston and does work \(dW = pdV\). In this case, the heat is added at constant pressure, and we write \[dQ = C_{p}ndT,\] where \(C_p\) is the molar heat capacity at constant pressure of the gas. Furthermore, since the ideal gas expands against a constant pressure,
\[d(pV) = d(RnT)\] becomes \[pdV = RndT.\]
Finally, inserting the expressions for dQ and pdV into the first law, we obtain
\[dE_{int} = dQ - pdV = (C_{p}n - Rn)dT.\]
We have found \(dE_{int}\) for both an isochoric and an isobaric process. Because the internal energy of an ideal gas depends only on the temperature, \(dE_{int}\) must be the same for both processes. Thus,
\[C_{V}ndT = (C_{p}n - Rn)dT,\]
and
\[C_p = C_V + R. \label{eq50}\]
The derivation of Equation \ref{eq50} was based only on the ideal gas law. Consequently, this relationship is approximately valid for all dilute gases, whether monatomic like He, diatomic like \(O_2\), or polyatomic like \(CO_2\) or \(NH_3\).
In the preceding chapter, we found the molar heat capacity of an ideal gas under constant volume to be
\[C_V = \dfrac{d}{2}R,\]
where d is the number of degrees of freedom of a molecule in the system. Table \(\PageIndex{1}\) shows the molar heat capacities of some dilute ideal gases at room temperature. The heat capacities of real gases are somewhat higher than those predicted by the expressions of \(C_V\) and \(C_p\) given in Equation \ref{eq50}. This indicates that vibrational motion in polyatomic molecules is significant, even at room temperature. Nevertheless, the difference in the molar heat capacities, \(C_p - C_V\), is very close to R, even for the polyatomic gases.
\(C_p\) | \(C_V\) | \(C_p - C_V\) | ||
---|---|---|---|---|
Type of Molecule | Gas | \(C_p\)" style="text-align:center;" class="lt-phys-4362">(J/mol K) | \(C_V\)" style="text-align:center;" class="lt-phys-4362">(J/mol K) | \(C_p - C_V\)" style="text-align:center;" class="lt-phys-4362">(J/mol K) |
Monatomic | Ideal | \(C_p\)" style="text-align:center;" class="lt-phys-4362">\(\frac{5}{2}R = 20.79\) | \(C_V\)" style="text-align:center;" class="lt-phys-4362">\(\frac{3}{2}R = 12.47\) | \(C_p - C_V\)" style="text-align:center;" class="lt-phys-4362">\(R = 8.31\) |
Diatomic | Ideal | \(C_p\)" style="text-align:center;" class="lt-phys-4362">\(\frac{7}{2}R = 29.10\) | \(C_V\)" style="text-align:center;" class="lt-phys-4362">\(\frac{5}{2}R = 20.79\) | \(C_p - C_V\)" style="text-align:center;" class="lt-phys-4362">\(R = 8.31\) |
Polyatomic | Ideal | \(C_p\)" style="text-align:center;" class="lt-phys-4362">\(4R = 33.26\) | \(C_V\)" style="text-align:center;" class="lt-phys-4362">\(3R = 24.04\) | \(C_p - C_V\)" style="text-align:center;" class="lt-phys-4362">\(R = 8.31\) |
Glossary
- molar heat capacity at constant pressure
- quantifies the ratio of the amount of heat added removed to the temperature while measuring at constant pressure
- molar heat capacity at constant volume
- quantifies the ratio of the amount of heat added removed to the temperature while measuring at constant volume