Solved Problem on Heat
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In a container thermally insulated from the environment a mixture of ice and water is placed at 0 °C at atmospheric pressure. By supplying a certain amount of energy by heat to the mixture, we verify that the temperature of the mixture does not change and the volume of the system decreases by 0.5 cm3.
a) Calculate the mass of ice that turns into liquid water;
b) Determine the amount of energy by heat received in the mixture.
Data: density of ice 0.92 g/cm3, the density of water 1 g/cm3, and latent heat of fusion of ice 80 cal/g.


Problem data:
  • Temperature of the water and ice mixture:    t = 0 °C;
  • Mixture volume variation:    ΔV = −0.5 cm3;
  • Water density:    dw = 1 g/cm3;
  • Ice density:    di = 0.92 g/cm3;
  • Latent heat of fusion of ice:    LF = 80 cal/g.
Problem diagram:

Initially, the system is at a temperature of 0 °C, after receiving energy by heat the temperature remains the same, but the volume decreases, this indicates that there has been a phase transition (Figure 1). As the density of ice is less than the density of water (di < dw) the volume occupied by the system initially is greater than the volume of the system after a mass m of ice has melted, the negative sign in the volume change indicates this situation.
Figure 1

Solution

a) The change in volume is given by the difference between the final volume of water, Vw, that formed and the initial volume of ice, Vi, that melted
\[ \begin{gather} \Delta V=V_{w}-V_{i} \tag{I} \end{gather} \]
The density of a substance is given by
\[ \bbox[#99CCFF,10px] {d=\frac{m}{V}} \]
writing this expression for ice and water
\[ \begin{gather} d_{i}=\frac{m}{V_{i}}\\ V_{i}=\frac{m}{d_{i}} \tag{II-a} \end{gather} \]
\[ \begin{gather} d_{w}=\frac{m}{V_{w}}\\ V_{w}=\frac{m}{d_{w}} \tag{II-b} \end{gather} \]
substituting expressions (II-a) and (II-b) into expression (I)
\[ \Delta V=\frac{m}{d_{w}}-\frac{m}{d_{i}} \]
factoring the mass m on the right-hand side of the equation and substituting the data of the problem
\[ \begin{gather} \Delta V=m\left(\frac{1}{d_{w}}-\frac{1}{d_{i}}\right)\\ -0.5=m\left(\frac{1}{1}-\frac{1}{0.92}\right) \end{gather} \]
multiplying the numerator and denominator of the first term in parentheses by 0.92
\[ \begin{gather} -0.5=m\left(\frac{1}{1}\times \frac{0.92}{0.92}-\frac{1}{0.92}\right)\\[5pt] -0.5=m\left(\frac{0.92}{0.92}-\frac{1}{0.92}\right)\\[5pt] -0.5=m\left(\frac{0.92-1}{0.92}\right)\\[5pt] -0.5=m\left(\frac{-{0.08}}{0.92}\right)\\[5pt] 0.5=\frac{0.08}{0.92}m\\m=\frac{0.5\times 0.92}{0.08}\\[5pt] m=\frac{0,46}{0.08} \end{gather} \]
\[ \bbox[#FFCCCC,10px] {m=5.75\;\text{g}} \]

b) The amount of energy supplied by heat to melt the ice is calculated by the expression of the latent heat
\[ \bbox[#99CCFF,10px] {Q=mL} \]
\[ \begin{gather} Q=mL_{F}\\ Q=5.75\times 80 \end{gather} \]
\[ \bbox[#FFCCCC,10px] {Q=460\;\text{cal}} \]
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