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4 Questions around this concept.
At absolute zero temperature, the entropy of a pure crystal is:
The entropy change involved in the isothermal reversible expansion of 2 moles of an ideal gas from a volume of 10dm3 to a volume of 100dm3 at 27°C is:
The entropy of any pure crystalline substance approaches zero as the temperature approaches absolute zero. This is called the third law of thermodynamics.
At any pressure, the entropy of every crystalline solid in thermodynamic equilibrium at absolute zero is zero.
It is impossible to reduce the temperature of any system to absolute zero by any process.
As the absolute temperature approaches zero, increment in entropy for isothermal process in crystalline solids approaches zero,
i.e. S=0 at T=0
Or $\lim _{T \rightarrow 0}, S \rightarrow 0$
If molar heat capacities of a substance (Cp) are measured at different temperature and a graph between Cp/T vs T is drawn and it shows this type of behavior.
Now let $S_M^o$ be the entropy of the substance at zero Kelvin and SM is its molar entropy at Kelvin then
$\begin{aligned} & \Delta \mathrm{S}=\mathrm{S}_{\mathrm{M}}-\mathrm{S}_{\mathrm{M}}^{\mathrm{o}} \\ & \therefore \Delta \mathrm{S}=\mathrm{S}_{\mathrm{M}} \\ & (\because\left.\mathrm{S}_{\mathrm{M}}^{\mathrm{o}}=0, \text { according to 3rd Law of thermodynamics }\right) \\ & \Delta \mathrm{S}=\frac{\mathrm{q}}{\mathrm{T}} \\ & \Delta \mathrm{S}=\int_0^{\mathrm{T}} \frac{\mathrm{C}_{\mathrm{p}} \cdot \mathrm{dT}}{\mathrm{T}}, \quad \because \mathrm{q}=1 \times \mathrm{C}_{\mathrm{p}} \cdot \mathrm{dT} \\ & \therefore \Delta \mathrm{S}=\mathrm{S}_{\mathrm{M}}=\int_0^{\mathrm{T}} \frac{\mathrm{C}_{\mathrm{p}} \cdot \mathrm{dT}}{\mathrm{T}}\end{aligned}$
The area under the curve or graph of Cp/T vs T determined from zero Kelvin to any desired temperature would be molar entropy change going from zero to desired T.
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