Chapter 4: Problem 37
A body of water at \(0^{\circ} \mathrm{C}\) is subjected to a constant surface temperature of \(-10^{\circ} \mathrm{C}\) for 10 days. How thick is the surface layer of ice? Use \(L=320 \mathrm{~kJ}\) \(\mathrm{kg}^{-1}, k=2 \mathrm{~J} \mathrm{~m}^{-1} \mathrm{~s}^{-1} \mathrm{~K}^{-1}, c=4 \mathrm{~kJ} \mathrm{~kg}^{-1} \mathrm{~K}^{-1}, \rho=\) \(1000 \mathrm{~kg} \mathrm{~m}^{-3}\).
Short Answer
Step by step solution
Understand the Problem
Establish Heat Transfer Equation
Relate Heat Lost to Ice Formation
Equate and Solve for Thickness
Calculate the Thickness
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Latent Heat of Fusion
This energy is absorbed during the phase change process, and in this exercise, it is crucial as it determines how much heat has to be removed to form a specific thickness of ice. The formula for latent heat of fusion is usually expressed as:
- \[ Q = mL \]
- \( Q \) is the heat absorbed or released,
- \( m \) is the mass,
- \( L \) is the latent heat of fusion.
In this exercise, we often express this concept in terms of "mass per unit area" as \( m = \rho \cdot A \cdot d \), where \( \rho \) is the density, \( A \) is the area, and \( d \) is the ice thickness. This helps relate heat loss to the formation of an ice layer.
Thermal Conductivity
In general terms, a material with high thermal conductivity conducts heat well, while a low value means the material is a good insulator. The equation used is:
- \[ Q = \frac{kA(T_s - T_i)t}{d} \]
- \( Q \) is the heat transferred,
- \( A \) is the cross-sectional area of heat flow,
- \( T_s \) and \( T_i \) are surface and initial temperatures respectively,
- \( t \) is time,
- \( d \) is the thickness of the material.
This means the rate at which ice forms depends on the thermal conductivity of the ice, which is part of why we use this property to calculate ice formation.
Ice Thickness Calculation
From the equation \( Q = \frac{kA(T_s - T_i)t}{d} = \rho A d L \), after canceling \( A \), the ice thickness formula is deduced:
- \[ d^2 = \frac{k(T_s - T_i)t}{\rho L} \]
- \( k \) is the thermal conductivity,
- \( T_s \) is the surface temperature,
- \( T_i \) is the initial temperature,
- \( t \) is the time,
- \( \rho \) is the density,
- \( L \) is the latent heat of fusion.
Once \( d^2 \) is found, taking the square root provides \( d \), the ice thickness.
Temperature Gradient in Solids
- \[ \text{temperature gradient} = \frac{\Delta T}{\Delta x} \]
- \( \Delta T \) is the temperature difference,
- \( \Delta x \) is the thickness or distance across the material.
In the context of ice formation, the temperature gradient drives the heat transfer through the ice. This is because heat naturally moves from a warmer area to a cooler one, which, in this case, is from the water at \(0^{\circ} \mathrm{C}\) to the surface at \(-10^{\circ} \mathrm{C}\).
Understanding the gradient helps in predicting how quickly energy is transferred, thus how rapidly ice forms. It links directly to the thermal conductivity and the calculated ice thickness, showing the interplay of these factors in a practical scenario.