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In Thermodynamics, What is Entropy? 📂Thermal Physics

In Thermodynamics, What is Entropy?

Definition

The quantity SS is defined as entropy if it satisfies the following equation.

dS=δQrevT dS = {{ \delta Q_{\text{rev} } } \over { T }}

Explanation

Entropy is a physical quantity representing ‘disorder,’ and it’s challenging to understand why it indicates disorder just by looking at its mathematical definition. Explanations for non-specialists like ‘messing up a room’ or ‘dropping ink into a glass of water’ can only explain ‘disorder,’ not dS=δQrevTdS = \dfrac{\delta Q_{\text{rev}} }{ T }.

To grasp the concept, it’s essential to think of entropy not as something derived but as a ‘definition.’ If you’ve ever wondered, ‘Why define it this way?’ a brief visual explanation might help. Consider the following two situations:

  • Case 1. When the system’s temperature is low

    20180809\_175434.png

    Imagine inputting thermal energy QQ into a cooled space. This is giving a change in thermal energy δQ\delta Q at a low temperature T1T_{1}. Let’s say the change in entropy is dS1d S_{1}.

  • Case 2. When the system’s temperature is high

    20180809\_175444.png

    Now, imagine adding the same thermal energy QQ to an already hot space as in Case 1. This is giving a change in thermal energy δQ\delta Q at a high temperature T2T_{2}. Let’s say the change in entropy is dS2d S_{2} in this case.

The inputted energy will diffuse to a colder area according to the Second Law of Thermodynamics. The space in Case 1. turns into a murky color that is hard to describe, compared to its original blue color, while the space in Case 2. barely becomes redder than before. This difference in color change signifies how much the space has changed due to the inputted energy, meaning dS1>dS2d S_{1} > d S_{2}. Mathematically, since T1<T2T_{1} < T_{2}, it follows that:

1T1>1T2 {{1} \over {T_{1} }} > {{1} \over {T_{2}}}

Thus, according to the definition of entropy, the following equation is a natural conclusion.

dS1=δQrevT1>δQrevT2=dS2 d S_{1} = {{\delta Q_{\text{rev} }} \over {T_{1} }} > {{\delta Q_{\text{rev} }} \over {T_{2}}} = d S_{2}

In thermodynamic terms, this means the increase in entropy in Case 1. is greater than in Case 2.. If explained by messing up a room, it means ’the same mischief causes a tidy room to become messier easier than a messy room.’ If explained by dropping ink, ’the same amount makes clear water dirtier easier than murky water.’