Calculation of enthalpy and entropy of fusion of an unknown solid?
Answer
551.4k+ views
Hint: Entropy is the amount of intrinsic disturbance within a compound, while enthalpy is the amount of internal energy present in the compound. For elemental compounds like hydrogen and oxygen, enthalpy is zero; however, enthalpy is nonzero for water (regardless of phase).
Complete answer:
$\Delta {S_{fus}} = 5.52J/mol\,K$
$\Delta {H_{fus}} = 2.36kJ/mol$
Explanation:
The Clapeyron equation in the form will be your tool of choice for this problem.
$\dfrac{{dP}}{{dT}} = \dfrac{{\Delta {S_{fus}}}}{{\Delta {T_{fus}}}}$ (i)
You now realise that the enthalpy change of fusion, $\Delta {H_f}$, and the entropy change of fusion, $\Delta {S_f}$have the following relationship.
$\Delta {S_{fus}} = \dfrac{{\Delta {H_{fus}}}}{T}$ (II)
The Gibb’s free energy transition at equilibrium is used to derive this.
$\Delta G = \Delta H - T\Delta S$
Since \[\Delta G = 0\] in equilibrium, it follows that you have
$
\Delta H = T \cdot \Delta S \\
\Rightarrow \Delta S = \dfrac{{\Delta H}}{T} \\
$
\[T\] will now reflect the melting temperature in your case. The average of the two melting temperatures is a reasonable rule of thumb to follow in this situation.
${T_{average}} = \dfrac{{427.15K + 429.26K}}{2} = 428.21K$
You should now rearrange equation (i) to solve for \[dT\] and then integrate, but if you assume that the temperature shift, \[dT\] , is small enough, you can skip this stage.
You can get away with such an estimate because you're working on the solid-liquid phase line, which means minor temperature shifts are inevitable. If you go this way, you'll be able to tell that
$\dfrac{{dP}}{{dT}} \approx \dfrac{{\Delta P}}{{\Delta T}} = \dfrac{{\Delta {S_{fus}}}}{{\Delta {V_{fus}}}}$
You have everything you need to solve $\Delta {S_{fus}}$ at this stage. You are aware, in particular, that
$\Delta T = {T_2} - {T_1} = 2.11K$
Here comes the tricky part - you need to convert \[\Delta {V_{fus}}\] and \[\Delta P\] to cubic meters per mole, \[{m^3}/mol,\]and \[pascals,{\text{ }}Pa\]
$
\Delta {V_{fus}} = {V_2} - {V_1} \\
\,\,\,\,\,\,\,\,\,\,\,\, = 156.6c{m^3} - 142.0c{m^3} \\
\,\,\,\,\,\,\,\,\,\,\,\, = 10.6c{m^3} \\
$
This implies that you've
\[10.6\dfrac{{c{m^3}}}{{mol}} \cdot \dfrac{{1{m^3}}}{{{{10}^6}c{m^3}}} = 10.6 \times {10^{ - 6}}{m^3}/mol\]
Finally, you have
$
\Delta P = 1.2 \times {10^6}Pa - 1.01325 \times {10^5}Pa \\
\,\,\,\,\,\,\,\, = 10.987 \times {10^5}Pa \\
$
As a result, plug in these numbers and solve for \[\Delta {S_{fus}}\]
$\Delta {S_{fus}} = \dfrac{{\Delta P}}{{\Delta T}} \cdot \Delta {V_{fus}}$
$\Delta {S_{fus}} = \dfrac{{10.987 \times {{10}^5}Pa}}{{2.11K}} \times 10.6 \times {10^{ - 6}}\dfrac{{{m^3}}}{{mol}}$
This will equal to
$\Delta {S_{fus}} = 55.195 \times {10^{ - 1}}{\dfrac{{Pam}}{{K\,mol}}^3}$
But, $Pa \times {m^3} = J$ , so the answer will be
$\Delta {S_{fus}} = 5.52\dfrac{J}{{mol\,K}}$
Now, use the equation (ii) to get
$
\Delta {H_{fus}} = \Delta {S_{fus}} \cdot {T_{average}} \\
\Delta {H_{fus}} = 5.52\dfrac{J}{{mol \cdot K}} \cdot 428.21K \\
\,\,\,\,\,\,\,\,\,\,\,\, = \,\,\,2363.72\dfrac{J}{{mol}} \\
$
This value will also be rounded to three sig figs, but expressed in kilojoules per mole.
$\Delta {H_{fus}} = 2.36kJ/mol$
Note:
Now, the question can arise: Does enthalpy increase as entropy increases? As a result, an enthalpy shift will affect entropy. The external entropy (entropy of the surroundings) increases in an exothermic reaction. The external entropy (entropy of the environment) decreases in an endothermic reaction.
Complete answer:
$\Delta {S_{fus}} = 5.52J/mol\,K$
$\Delta {H_{fus}} = 2.36kJ/mol$
Explanation:
The Clapeyron equation in the form will be your tool of choice for this problem.
$\dfrac{{dP}}{{dT}} = \dfrac{{\Delta {S_{fus}}}}{{\Delta {T_{fus}}}}$ (i)
You now realise that the enthalpy change of fusion, $\Delta {H_f}$, and the entropy change of fusion, $\Delta {S_f}$have the following relationship.
$\Delta {S_{fus}} = \dfrac{{\Delta {H_{fus}}}}{T}$ (II)
The Gibb’s free energy transition at equilibrium is used to derive this.
$\Delta G = \Delta H - T\Delta S$
Since \[\Delta G = 0\] in equilibrium, it follows that you have
$
\Delta H = T \cdot \Delta S \\
\Rightarrow \Delta S = \dfrac{{\Delta H}}{T} \\
$
\[T\] will now reflect the melting temperature in your case. The average of the two melting temperatures is a reasonable rule of thumb to follow in this situation.
${T_{average}} = \dfrac{{427.15K + 429.26K}}{2} = 428.21K$
You should now rearrange equation (i) to solve for \[dT\] and then integrate, but if you assume that the temperature shift, \[dT\] , is small enough, you can skip this stage.
You can get away with such an estimate because you're working on the solid-liquid phase line, which means minor temperature shifts are inevitable. If you go this way, you'll be able to tell that
$\dfrac{{dP}}{{dT}} \approx \dfrac{{\Delta P}}{{\Delta T}} = \dfrac{{\Delta {S_{fus}}}}{{\Delta {V_{fus}}}}$
You have everything you need to solve $\Delta {S_{fus}}$ at this stage. You are aware, in particular, that
$\Delta T = {T_2} - {T_1} = 2.11K$
Here comes the tricky part - you need to convert \[\Delta {V_{fus}}\] and \[\Delta P\] to cubic meters per mole, \[{m^3}/mol,\]and \[pascals,{\text{ }}Pa\]
$
\Delta {V_{fus}} = {V_2} - {V_1} \\
\,\,\,\,\,\,\,\,\,\,\,\, = 156.6c{m^3} - 142.0c{m^3} \\
\,\,\,\,\,\,\,\,\,\,\,\, = 10.6c{m^3} \\
$
This implies that you've
\[10.6\dfrac{{c{m^3}}}{{mol}} \cdot \dfrac{{1{m^3}}}{{{{10}^6}c{m^3}}} = 10.6 \times {10^{ - 6}}{m^3}/mol\]
Finally, you have
$
\Delta P = 1.2 \times {10^6}Pa - 1.01325 \times {10^5}Pa \\
\,\,\,\,\,\,\,\, = 10.987 \times {10^5}Pa \\
$
As a result, plug in these numbers and solve for \[\Delta {S_{fus}}\]
$\Delta {S_{fus}} = \dfrac{{\Delta P}}{{\Delta T}} \cdot \Delta {V_{fus}}$
$\Delta {S_{fus}} = \dfrac{{10.987 \times {{10}^5}Pa}}{{2.11K}} \times 10.6 \times {10^{ - 6}}\dfrac{{{m^3}}}{{mol}}$
This will equal to
$\Delta {S_{fus}} = 55.195 \times {10^{ - 1}}{\dfrac{{Pam}}{{K\,mol}}^3}$
But, $Pa \times {m^3} = J$ , so the answer will be
$\Delta {S_{fus}} = 5.52\dfrac{J}{{mol\,K}}$
Now, use the equation (ii) to get
$
\Delta {H_{fus}} = \Delta {S_{fus}} \cdot {T_{average}} \\
\Delta {H_{fus}} = 5.52\dfrac{J}{{mol \cdot K}} \cdot 428.21K \\
\,\,\,\,\,\,\,\,\,\,\,\, = \,\,\,2363.72\dfrac{J}{{mol}} \\
$
This value will also be rounded to three sig figs, but expressed in kilojoules per mole.
$\Delta {H_{fus}} = 2.36kJ/mol$
Note:
Now, the question can arise: Does enthalpy increase as entropy increases? As a result, an enthalpy shift will affect entropy. The external entropy (entropy of the surroundings) increases in an exothermic reaction. The external entropy (entropy of the environment) decreases in an endothermic reaction.
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