1.0 kg of water at 35°C is mixed with 1.0 kg of water at 45°C in a well-insulated container. Estimate the net change in entropy of the system.

Short Answer

Expert verified

The net increase of entropy is \(1.1\;{\rm{J/K}}\).

Step by step solution

01

Concepts

The heat absorbed by the hot water equals the heat released by hot water.

The change in entropy is\(\Delta S = \frac{Q}{T}\)

02

Given data

The mass of both types of water is \(m = 1.0\;{\rm{kg}}\).

The initial temperature of the hot water is \({T_1} = {45 \circ }{\rm{C}}\).

The initial temperature of the cold water is \({T_2} = {35 \circ }{\rm{C}}\)

Let T be the final temperature of the water mixture.

03

Calculation

The amount of heat absorbed by the cold water equals the heat released by the hot water.

Now the amount of heat is \(Q = mc\left( {{T_1} - T} \right)\).

As both types of water have the same mass, then the final temperature is,

\(\begin{array}{c}T = \frac{{{T_1} + {T_2}}}{2}\\ = \frac{{{{45} \circ }{\rm{C}} + {{35} \circ }{\rm{C}}}}{2}\\ = {40 \circ }{\rm{C}}\end{array}\)

Now the average temperature of the hot water is,

\(\begin{array}{c}{{T'}_1} = \frac{{{T_1} + T}}{2}\\ = \frac{{{{45} \circ }{\rm{C}} + {{40} \circ }{\rm{C}}}}{2}\\ = {42.5 \circ }{\rm{C}}\\ = 315.5\;{\rm{K}}\end{array}\)

Now the average temperature of the cold water is,

\(\begin{array}{c}{{T'}_2} = \frac{{{T_2} + T}}{2}\\ = \frac{{{{35} \circ }{\rm{C}} + {{40} \circ }{\rm{C}}}}{2}\\ = {37.5 \circ }{\rm{C}}\\ = 310.5\;{\rm{K}}\end{array}\)

Now the rate of change in entropy for the hot water is \(\Delta {S_1} = - \frac{Q}{{{{T'}_1}}}\).

The rate of change in entropy for the cold water is \(\Delta {S_2} = \frac{Q}{{{{T'}_2}}}\).

Therefore the rate of change of net entropy is,

\(\begin{array}{c}\Delta S = \Delta {S_1} + \Delta {S_2}\\ = - \frac{Q}{{{{T'}_1}}} + \frac{Q}{{{T_2}}}\\ = mc\left( {{T_1} - T} \right)\left( {\frac{1}{{{{T'}_2}}} - \frac{1}{{{{T'}_1}}}} \right)\end{array}\)

Now substituting the values in the above equation, you get,

\(\begin{array}{c}\Delta S = mc\left( {{T_1} - T} \right)\left( {\frac{1}{{{{T'}_2}}} - \frac{1}{{{{T'}_1}}}} \right)\\ = \left( {1.0\;{\rm{kg}}} \right) \times \left( {4186\;{\rm{J/kg}}{ \cdot {\rm{o}}}{\rm{C}}} \right)\left( {{{45} \circ }{\rm{C}} - {{40} \circ }{\rm{C}}} \right) \times \left( {\frac{1}{{310.5\;{\rm{K}}}} - \frac{1}{{315.5\;{\rm{K}}}}} \right)\\ = 1.1\;{\rm{J/K}}\end{array}\)

Hence, the net increase of entropy is \(1.1\;{\rm{J/K}}\).

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Most popular questions from this chapter

Question: (II) How much less per year would it cost a family to operate a heat pump that has a coefficient of performance of 2.9 than an electric heater that costs \(2000 to heat their home for a year? If the conversion to the heat pump costs \)15,000, how long would it take the family to break even on heating costs? How much would the family save in 20 years?

Question: (II) In an engine, an almost ideal gas is compressed adiabatically to half its volume. In doing so, 2630 J of work is done on the gas. (a) How much heat flows into or out of the gas? (b) What is the change in internal energy of the gas? (c) Does its temperature rise or fall?

Question: (II) A 1.0-L volume of air initially at 3.5 atm of (gauge) pressure is allowed to expand isothermally until the pressure is 1.0 atm. It is then compressed at constant pressure to its initial volume, and lastly is brought back to its original pressure by heating at constant volume. Draw the process on a PV diagram, including numbers and labels for the axes.

An ideal monatomic gas expands slowly to twice its volume (1) isothermally; (2) adiabatically; (3) isobarically. Plot each on a PV diagram. In which process \(\Delta U\) is the greatest, and in which is \(\Delta U\) the least? In which is W the greatest and the least? In which is Q the greatest and the least?

Calculate the work done by an ideal gas while going from state A to state C in Fig. 15–28 for each of the following processes:

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FIGURE 15–28

Problem 68

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