Specific heat: Difference between revisions

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Created page with "Category:Compressible flow Category:Thermodynamics __TOC__ For thermally perfect and calorically perfect gases <math display="block"> \begin{aligned} &C_p=\frac{dh}{dT}\\ &C_v=\frac{de}{dT} \end{aligned} </math> From the definition of enthalpy and the equation of state <math>p=\rho RT</math> <math display="block"> h=e+\frac{p}{\rho}=e+RT </math> Differentiate Eqn. \ref{eq:enthalpy} with respect to temperature gives <math display="block"> \frac{dh}{dT}=\fra..."
 
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[[Category:Thermodynamics]]
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For thermally perfect and calorically perfect gases
For thermally perfect and calorically perfect gases


<math display="block">
{{NumEqn|<math>
\begin{aligned}
\begin{aligned}
&C_p=\frac{dh}{dT}\\
&C_p=\frac{dh}{dT}\\
&C_v=\frac{de}{dT}
&C_v=\frac{de}{dT}
\end{aligned}
\end{aligned}
</math>
</math>|label=eq-specific-heat}}


From the definition of enthalpy and the equation of state <math>p=\rho RT</math>
From the definition of enthalpy and the equation of state <math>p=\rho RT</math>


<math display="block">
{{NumEqn|<math>
h=e+\frac{p}{\rho}=e+RT
h=e+\frac{p}{\rho}=e+RT
</math>
</math>|label=eq-enthalpy}}


Differentiate Eqn. \ref{eq:enthalpy} with respect to temperature gives
Differentiate {{EquationNote|label=eq-enthalpy}} with respect to temperature gives


<math display="block">
{{NumEqn|<math>
\frac{dh}{dT}=\frac{de}{dT}+\frac{d(RT)}{dT}
\frac{dh}{dT}=\frac{de}{dT}+\frac{d(RT)}{dT}
</math>
</math>}}


Inserting the specific heats gives
Inserting the specific heats gives


<math display="block">
{{NumEqn|<math>
C_p=C_v+R
C_p=C_v+R
</math>
</math>|label=eq-specific-heat-b}}


Dividing Eqn. \ref{eq:specificheat:b} by <math>C_v</math> gives
Dividing {{EquationNote|label=eq-specific-heat-b}} by <math>C_v</math> gives


<math display="block">
{{NumEqn|<math>
\frac{C_p}{C_v}=1+\frac{R}{C_v}
\frac{C_p}{C_v}=1+\frac{R}{C_v}
</math>
</math>|label=eq-specific-heat-c}}


Introducing the ratio of specific heats defined as
Introducing the ratio of specific heats defined as


<math display="block">
{{NumEqn|<math>
\gamma=\frac{C_p}{C_v}
\gamma=\frac{C_p}{C_v}
</math>
</math>|label=eq-gamma}}


Now, inserting Eqn. \ref{eq:gamma} in Eqn. \ref{eq:specificheat:c} gives
Now, inserting {{EquationNote|label=eq-gamma}} in Eqn. \ref{eq:specificheat:c} gives


<math display="block">
{{NumEqn|<math>
C_v=\frac{R}{\gamma-1}
C_v=\frac{R}{\gamma-1}
</math>
</math>}}


In the same way, dividing Eqn. \ref{eq:specificheat:b} with <math>C_p</math> gives
In the same way, dividing {{EquationNote|label=eq-specific-heat-b}} with <math>C_p</math> gives


<math display="block">
{{NumEqn|<math>
1=\frac{C_v}{C_p}+\frac{R}{C_p}=\frac{1}{\gamma}+\frac{R}{C_p}
1=\frac{C_v}{C_p}+\frac{R}{C_p}=\frac{1}{\gamma}+\frac{R}{C_p}
</math>
</math>}}


and thus
and thus


<math display="block">
{{NumEqn|<math>
C_p=\frac{\gamma R}{\gamma-1}
C_p=\frac{\gamma R}{\gamma-1}
</math>
</math>}}