Why can we differentiate this entropy total derivative with repect to Temperature?

In summary, the ability to differentiate the entropy total derivative with respect to temperature arises from the relationship between entropy, heat, and temperature in thermodynamic systems. The total derivative of entropy accounts for changes in both internal energy and volume, which are functions of temperature. This differentiation is valid because temperature serves as a variable that influences the state of the system, allowing us to analyze how entropy changes with respect to temperature while considering other thermodynamic variables.
  • #1
zenterix
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Homework Statement
I am going through a thermodynamics course and there is a section about natural variables.
Relevant Equations
In that section, there is the following derivation
Ignoring chemical potential for now, the natural variables of ##U## are ##S## and ##V##. Thus

$$dU=\left (\frac{\partial U}{\partial S}\right )_VdS+\left (\frac{\partial U}{\partial V}\right )_SdV=TdS-pdV\tag{1}$$

which we can rewrite for ##dS## as

$$dS=\frac{dU}{dT}+\frac{pdV}{T}\tag{2}$$

We wish to determine how the entropy depends on temperature.

We can differentiate the expression for ##dS## with respect to temperature at constant volume to obtain ##\left (\frac{\partial S}{\partial T}\right )_V##.

Apply the derivative to obtain

$$\left (\frac{\partial S}{\partial T}\right )_V=\frac{1}{T}\left (\frac{\partial U}{\partial T}\right )_V+\frac{p}{T}\left (\frac{\partial V}{\partial T}\right )_V$$

$$=\frac{1}{T}\left (\frac{\partial U}{\partial T}\right )_V=\frac{C_V}{T}$$

Mathematically, what is happening exactly?

In other words, why/how does ##dS## become ##\left (\frac{\partial S}{\partial T}\right )_V##?

Here is my current understanding.

##dS## is the total derivative function for ##S(T,V)##.

##dS## is a linear function of ##dT## and ##dV## and this linear function is a function of ##T## and ##V##.

That is, at each ##T## and ##V## we have a different function ##dS##.

If we differentiate ##dS## relative to ##T## we are determining the rate of change of ##dS## relative to ##T## at fixed ##V##.

Notation-wise, it seems we would have ##\frac{\partial (dS)}{\partial T}##, which is a notation I have never seen before.

If this is correct so far, then it seems that ##\frac{\partial (dS)}{\partial T}## is written as just ##\left (\frac{\partial S}{\partial T}\right )_V##.

But this latter step isn't very clear to me.

So my question is essentially how to understand what is going on from a mathematical perspective in this derivation.
 
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  • #2
No, don't differentiate dS, rather use the differential of S with variables T and V, ## dS(T,V)=\left(\partial S/\partial T\right)_V dT + \left (\partial S /\partial V\right)_T dV## and a similar expression for dU(T,V).
 

FAQ: Why can we differentiate this entropy total derivative with repect to Temperature?

What is the significance of differentiating the entropy total derivative with respect to temperature?

Differentiating the entropy total derivative with respect to temperature allows us to understand how the entropy of a system changes as the temperature varies. This is crucial for analyzing thermodynamic processes and helps in deriving fundamental relationships in thermodynamics, such as the heat capacity and the relationship between entropy and other state functions.

What does the total derivative of entropy represent in thermodynamics?

The total derivative of entropy represents the change in entropy of a system due to changes in its state variables, such as temperature, volume, and number of particles. It captures how entropy responds to infinitesimal changes in these variables, providing insights into the system's thermodynamic behavior.

Why is temperature considered an independent variable when differentiating entropy?

Temperature is considered an independent variable because it is one of the primary state variables that can be controlled in a thermodynamic system. By treating temperature as an independent variable, we can examine how entropy changes in response to variations in temperature, which is essential for understanding thermal equilibrium and energy transfer processes.

How does the differentiation of entropy relate to the second law of thermodynamics?

The differentiation of entropy is closely related to the second law of thermodynamics, which states that the total entropy of an isolated system can never decrease over time. By differentiating entropy with respect to temperature, we can derive expressions that illustrate how energy disperses in a system, reinforcing the concept of irreversibility and the direction of spontaneous processes.

What are the practical applications of differentiating the entropy total derivative with respect to temperature?

Practical applications include calculating heat capacities, understanding phase transitions, and analyzing thermodynamic cycles in engines and refrigerators. This differentiation is vital for engineers and scientists working in fields such as chemical engineering, materials science, and environmental science, where thermodynamic principles are applied to real-world problems.

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