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If \({\bf{1}}{\bf{.00}}\;{{\bf{m}}{\bf{3}}}\) of water at 0°C is frozen and cooled to \( - {\bf{8}}{\bf{.}}{{\bf{0}}{\bf{o}}}{\bf{C}}\) by being in contact with a great deal of ice at \( - {\bf{8}}{\bf{.}}{{\bf{0}}{\bf{o}}}{\bf{C}}\) estimate the total change in entropy of the process.

Short Answer

Expert verified

The change in entropy is \(1.28 \times {106}\;{\rm{J/K}}\).

Step by step solution

01

Concepts

The extracted heat from the water is \(Q = mL\) during the freezing.

The change in entropy is\(\Delta S = \frac{Q}{T}\)during the freezing, and the change in entropy is\(\Delta S = mc\ln \frac{{{T_{\rm{f}}}}}{{{T_{\rm{i}}}}}\)while lowering the temperature of ice.

02

Given data

The volume of the water is \(V = 1.00\;{{\rm{m}}{\rm{3}}}\).

The initial temperature of the water is \({T_1} = {0 \circ }{\rm{C}} = 273\;{\rm{K}}\).

The final temperature is \({T_2} = - {8.0 \circ }{\rm{C}} = 265\;{\rm{K}}\).

03

Calculation

You know the latent heat for freezing is \(L = 3.33 \times {105}\;{\rm{J/kg}}\) , the density of the water is \(\rho = 1000\;{\rm{kg/}}{{\rm{m}}{\rm{3}}}\), and the specific heat of ice is \({c_{\rm{i}}} = 2100\;{\rm{J/kg}} \cdot {\rm{K}}\)

Now the mass of the water is \(m = \rho V\).

Then, the heat energy is taken away from the water to become the ice \({0 \circ }{\rm{C}}\),

\(\begin{array}{c}Q = mL\\ = \rho VL\end{array}\)

Therefore the change in entropy during freezing,

\(\begin{array}{c}\Delta {S_1} = - \frac{Q}{{{T_1}}}\\ = - \frac{{\rho VL}}{{{T_1}}}\\ = - \frac{{\left( {1000\;{\rm{kg/}}{{\rm{m}}{\rm{3}}}} \right) \times \left( {1.00\;{{\rm{m}}{\rm{3}}}} \right) \times \left( {3.33 \times {{10}5}\;{\rm{J/kg}}} \right)}}{{273\;{\rm{K}}}}\\ = - 1.22 \times {106}\;{\rm{J/K}}\end{array}\)

Now the change in entropy due to lowering the temperature of the ice is,

\(\begin{array}{c}\Delta {S_1} = m{c_{\rm{i}}}\ln \frac{{{T_2}}}{{{T_1}}}\\ = \rho V{c_{\rm{i}}}\ln \frac{{{T_2}}}{{{T_1}}}\\ = \left[ {\left( {1000\;{\rm{kg/}}{{\rm{m}}{\rm{3}}}} \right) \times \left( {1.00\;{{\rm{m}}{\rm{3}}}} \right) \times \left( {2100\;{\rm{J/kg}} \cdot {\rm{K}}} \right)} \right]\ln \frac{{265\;{\rm{K}}}}{{273\;{\rm{K}}}}\\ = - 6.25 \times {104}\;{\rm{J/K}}\end{array}\)

Therefore the total change in entropy is,

\(\begin{array}{c}\Delta S = \Delta {S_1} + \Delta {S_2}\\ = \left( { - 1.22 \times {{10}6}\;{\rm{J/K}}} \right) + \left( { - 6.25 \times {{10}4}\;{\rm{J/K}}} \right)\\ = - 1.28 \times {106}\;{\rm{J/K}}\end{array}\)

Hence, the change in entropy is \(1.28 \times {106}\;{\rm{J/K}}\).

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Most popular questions from this chapter

(II) A gas is enclosed in a cylinder fitted with a light frictionless piston and maintained at atmospheric pressure. When 254 kcal of heat is added to the gas, the volume is observed to increase slowly from to \({\bf{16}}{\bf{.2}}\;{{\bf{m}}^{\bf{3}}}\).Calculate (a) the work done by the gas and (b) the change in internal energy of the gas.

On a very hot day, could you cool your kitchen by leaving the refrigerator door open?

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(d) No, the heat exhausted by the refrigerator into the room is more than the heat the refrigerator takes out of the room.

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(e) both the temperature and pressure of the gas increase

Can mechanical energy ever be transformed completely into heat or internal energy? Can the reverse happen? In each case, if your answer is no, explain why not, if yes, give one or two examples.

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