One way of measuring the thermal conductivity of a material is to sandwich an electric thermofoil heater between two identical rectangular samples of the material and to heavily insulate the four outer edges, as shown in the figure. Thermocouples attached to the inner and outer surfaces of the samples record the temperatures. During an experiment, two \(0.5-\mathrm{cm}\) thick samples \(10 \mathrm{~cm} \times\) \(10 \mathrm{~cm}\) in size are used. When steady operation is reached, the heater is observed to draw \(25 \mathrm{~W}\) of electric power, and the temperature of each sample is observed to drop from \(82^{\circ} \mathrm{C}\) at the inner surface to \(74^{\circ} \mathrm{C}\) at the outer surface. Determine the thermal conductivity of the material at the average temperature.

Short Answer

Expert verified
Answer: The thermal conductivity of the material at the average temperature is 1.5625 W/(m K).

Step by step solution

01

Determine the heat transfer rate

We know the electric power consumed by the heater is \(25\mathrm{~W}\). In steady-state conditions, the heat generated by the heater is transferred to the outer surface by conduction, thus the heat transfer rate \(q\) is equal to the electric power consumed: \(q=25\mathrm{~W}\).
02

Calculate the surface area of the material

The dimensions of each sample are given as \(10 \mathrm{~cm} \times 10 \mathrm{~cm}\). To calculate the surface area of the material, convert the dimensions to meters and multiply the length and width: $$A = (10\mathrm{~cm} \times 10\mathrm{~cm}) \times \left( \frac{1\mathrm{~m}}{100\mathrm{~cm}} \right)^2 = 0.01\mathrm{~m^2}$$
03

Calculate the temperature difference across the sample

The temperature of each sample drops from \(82^{\circ}\mathrm{C}\) at the inner surface to \(74^{\circ}\mathrm{C}\) at the outer surface, which gives a temperature difference of: $$\Delta T = 82^{\circ}\mathrm{C} - 74^{\circ}\mathrm{C} = 8^{\circ}\mathrm{C}$$
04

Calculate the thickness of the material

Given that each sample has a thickness of \(0.5\mathrm{-cm}\), we need to express the thickness in meters: $$\Delta x = 0.5\mathrm{~cm} \times \frac{1\mathrm{~m}}{100\mathrm{~cm}} = 0.005\mathrm{~m}$$
05

Determine the thermal conductivity

Now we can use the heat conduction formulation to calculate the thermal conductivity: $$q = kA \frac{\Delta T}{\Delta x} \Rightarrow k = \frac{q\Delta x}{A\Delta T}$$ $$k = \frac{25\mathrm{~W} \times 0.005\mathrm{~m}}{0.01\mathrm{~m^2} \times 8^{\circ}\mathrm{C}} = \frac{0.125\mathrm{~W}}{0.08\mathrm{~Km^2}} = 1.5625\mathrm{~W/(m~K)}$$ Therefore, the thermal conductivity of the material at the average temperature is \(1.5625\mathrm{~W/(m~K)}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Heat Transfer
Heat transfer is the physical act of thermal energy being exchanged between systems or bodies due to temperature differences. It's fundamental to the functioning of heaters, engines, and even our own bodies. There are three primary modes of heat transfer: conduction, convection, and radiation.

In the context of measuring thermal conductivity, we're interested in conduction, the process where heat is transferred through a solid material from the high temperature side to the lower temperature side. Imagine a metal rod with one end heated - the heat will travel down the rod to the cooler end because of conduction. The rate at which heat is transferred via conduction is influenced by the material's thermal conductivity, the temperature difference, the cross-sectional area through which heat is being transferred, and the distance the heat travels.
Steady-State Conduction
Steady-state conduction refers to the condition where the temperature distribution in the conducting medium does not change over time. In other words, despite continuous heat transfer, the temperatures at any given point in the material remain constant. This is a common assumption for many engineering problems because it greatly simplifies the analysis of thermal systems.

In steady-state conduction scenarios, such as the textbook exercise in question, the rate of heat input into the system equals the rate of heat output, leading to a balance that maintains constant temperatures throughout the material over time. The assumption of steady-state is crucial when applying thermal conductivity formulas since these are derived based on time-invariant conditions.
Thermal Conductivity Formula
The thermal conductivity formula embodies how materials conduct heat and is critical for solving heat transfer problems. The formula used to determine a material's thermal conductivity, often denoted as 'k', incorporates several factors: the rate of heat transfer 'q', the thickness of the material 'Δx', the surface area 'A' through which heat is transferred, and the temperature difference 'ΔT' across the material.

The mathematical expression is given by Fourier’s law of conduction: \[ k = \frac{q\Delta x}{A\Delta T} \]

In essence, a material with high thermal conductivity will transfer heat quickly (think metals like copper), while materials with low thermal conductivity do so much more slowly (such as wood or foam). The unit of thermal conductivity is Watts per meter-Kelvin (\(\frac{W}{mK}\)), signifying the amount of heat that passes through a unit area of a material with a unit temperature gradient per unit distance.
Thermocouples
Thermocouples are devices composed of two different types of metal wires joined at one end, used to measure temperature. When the join point, or 'junction', is exposed to a certain temperature, a voltage is created that can be measured and translated into a temperature reading. This phenomenon is known as the Seebeck effect.

They are important in experiments that measure thermal conductivity because they can provide accurate and continuous temperature readings at various points in the material. By attaching thermocouples to different surfaces of the samples in the textbook exercise, one can track the temperature gradient needed to determine thermal conductivity. Due to their reliability and simplicity, thermocouples are an essential tool in many industrial and scientific applications where temperature monitoring is critical.

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Most popular questions from this chapter

Hot air at \(80^{\circ} \mathrm{C}\) is blown over a 2-m \(\times 4\) - \(\mathrm{m}\) flat surface at \(30^{\circ} \mathrm{C}\). If the average convection heat transfer coefficient is \(55 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), determine the rate of heat transfer from the air to the plate, in \(\mathrm{kW}\).

An AISI 316 stainless steel spherical container is used for storing chemicals undergoing exothermic reaction that provides a uniform heat flux of \(60 \mathrm{~kW} / \mathrm{m}^{2}\) to the container's inner surface. The container has an inner diameter of \(1 \mathrm{~m}\) and a wall thickness of \(5 \mathrm{~cm}\). For safety reason to prevent thermal burn on individuals working around the container, it is necessary to keep the container's outer surface temperature below \(50^{\circ} \mathrm{C}\). If the ambient temperature is \(23^{\circ} \mathrm{C}\), determine the necessary convection heat transfer coefficient to keep the container's outer surface temperature below \(50^{\circ} \mathrm{C}\). Is the necessary convection heat transfer coefficient feasible with free convection of air? If not, discuss other option to prevent the container's outer surface temperature from causing thermal burn.

Consider steady heat transfer between two large parallel plates at constant temperatures of \(T_{1}=290 \mathrm{~K}\) and \(T_{2}=150 \mathrm{~K}\) that are \(L=2 \mathrm{~cm}\) apart. Assuming the surfaces to be black (emissivity \(\varepsilon=1\) ), determine the rate of heat transfer between the plates per unit surface area assuming the gap between the plates is (a) filled with atmospheric air, \((b)\) evacuated, \((c)\) filled with fiberglass insulation, and \((d)\) filled with superinsulation having an apparent thermal conductivity of \(0.00015 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\).

An engineer who is working on the heat transfer analysis of a house in English units needs the convection heat transfer coefficient on the outer surface of the house. But the only value he can find from his handbooks is \(22 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), which is in SI units. The engineer does not have a direct conversion factor between the two unit systems for the convection heat transfer coefficient. Using the conversion factors between \(\mathrm{W}\) and \(\mathrm{Btu} / \mathrm{h}, \mathrm{m}\) and \(\mathrm{ft}\), and \({ }^{\circ} \mathrm{C}\) and \({ }^{\circ} \mathrm{F}\), express the given convection heat transfer coefficient in Btu/ \(\mathrm{h} \cdot \mathrm{ft}^{2}{ }^{\circ} \mathrm{F}\). Answer: \(3.87 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft}^{2}{ }^{\circ} \mathrm{F}\)

A 3-m-internal-diameter spherical tank made of 1 -cm-thick stainless steel is used to store iced water at \(0^{\circ} \mathrm{C}\). The tank is located outdoors at \(25^{\circ} \mathrm{C}\). Assuming the entire steel tank to be at \(0^{\circ} \mathrm{C}\) and thus the thermal resistance of the tank to be negligible, determine \((a)\) the rate of heat transfer to the iced water in the tank and \((b)\) the amount of ice at \(0^{\circ} \mathrm{C}\) that melts during a 24 -hour period. The heat of fusion of water at atmospheric pressure is \(h_{i f}=333.7 \mathrm{~kJ} / \mathrm{kg}\). The emissivity of the outer surface of the tank is \(0.75\), and the convection heat transfer coefficient on the outer surface can be taken to be \(30 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Assume the average surrounding surface temperature for radiation exchange to be \(15^{\circ} \mathrm{C}\).

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