To understand the classification of entropy, we first need to define what extensive and intensive properties are in thermodynamics.
Entropy is a fundamental thermodynamic property that measures the degree of randomness or disorder in a system. Let's look at the two forms mentioned: total entropy ($S$) and specific entropy ($s$).
Total entropy, denoted by $S$, represents the overall entropy of a system. Since entropy is related to the number of possible microscopic arrangements of the system's components, it naturally scales with the size of the system. For instance, a larger system (more mass or volume) generally has more possible arrangements and thus higher total entropy.
Therefore, Total Entropy ($S$) is an extensive property because its value depends directly on the amount of substance (mass) in the system. If you double the mass of the system, you double the total entropy.
Specific entropy, denoted by $s$, is defined as the total entropy ($S$) divided by the mass ($m$) of the system. The relationship is given by the formula:
$s = \frac{S}{m}$
When we calculate specific entropy, we are essentially normalizing the total entropy by the mass. If we increase the mass ($m$) of the system, the total entropy ($S$) also increases proportionally. However, their ratio ($s = S/m$) remains constant. For example, if we double the mass ($2m$), the total entropy also doubles ($2S$), but the specific entropy becomes $\frac{2S}{2m} = \frac{S}{m}$, which is the same value.
Because the value of specific entropy does not change with the size or mass of the system, Specific Entropy ($s$) is an intensive property.
Based on these definitions:
This matches the second option provided in the question.
Two blocks of ice when pressed together join to form one block because
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The total number of phonon modes in a solid of volume V is \(\int_{\rm{0}}^{{\rm{ω_ D}}} {{\rm{g}}\left( {\rm{ω }} \right)\,} {\rm{dω }}\) = 3N, where N is the number of primitive cells, ω Dis the Debye frequency and density of photon modes is g( ω ) = AV ω2 (with A > 0 a constant). If the density of the solid doubles in a phase transition, the Debye temperature θ D, will
The dispersion relation of a gas of non-interacting bosons in d dimensions is E(k) = ak s, where a and s are positive constants. Bose-Einstein condensation will occur for all values of
Example of thermoplastic among the following is