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Heat flux meters use a very sensitive device known as a thermopile to measure the temperature difference across a thin, heat conducting film made of kapton \((k=0.345 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\). If the thermopile can detect temperature differences of \(0.1^{\circ} \mathrm{C}\) or more and the film thickness is \(2 \mathrm{~mm}\), what is the minimum heat flux this meter can detect?

Short Answer

Expert verified
Answer: The minimum detectable heat flux for this meter is 17.25 W/m².

Step by step solution

01

Formula for heat flux

The formula for heat flux (q) is given by Fourier's law: \(q = -k \cdot \frac{\Delta T}{d}\), where q is the heat flux, k is the thermal conductivity, \(\Delta T\) is the temperature difference, and d is the thickness of the film.
02

Plug in given values

We have the given values: \(k = 0.345\ \mathrm{W}/(\mathrm{m}\cdot\mathrm{K})\), \(\Delta T = 0.1^{\circ}\mathrm{C}\) (we can use Celsius as the temperature difference unit, because the conversion factor is a ratio, the offset of the Kelvin scale will cancel out), and \(d = 2\ \mathrm{mm} = 0.002\ \mathrm{m}\). We plug these values into the formula for heat flux: \(q = -0.345\frac{0.1}{0.002}\).
03

Calculate the minimum heat flux

Now, we can calculate the minimum heat flux this meter can detect: \(q = -0.345\frac{0.1}{0.002} = -17.25\ \mathrm{W}/\mathrm{m}^2\).
04

Interpret the result

The minimum detectable heat flux is \(-17.25\ \mathrm{W}/\mathrm{m}^2\). The negative sign indicates that the heat is detected to flow in the opposite direction, which is used mostly for convention. The absolute value of the heat flux, \(17.25\ \mathrm{W}/\mathrm{m}^2\), can be taken as the minimum detectable heat flux this meter can detect.

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Key Concepts

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

Thermopile
A thermopile is a sensitive instrument that consists of several thermocouples connected together. Thermocouples are devices that generate a voltage based on the temperature difference between two different conductors. By connecting multiple thermocouples in series or parallel, a thermopile can detect very small temperature differences, making it ideal for measuring heat flux.

The primary function of a thermopile in a heat flux meter is to accurately measure the temperature difference across a thin film. This capability is crucial because the temperature gradient is directly related to the heat flow, which the instrument aims to calculate. The higher the number of thermocouples in a thermopile, the greater its sensitivity to minute temperature changes.
  • Used for measuring small temperature differences.
  • Composed of multiple thermocouples.
  • Provides voltage output proportional to temperature difference.
Thermopiles are essential in applications requiring precision in thermal measurements, such as in building insulation assessments or during quality checks in manufacturing processes for heat-sensitive products.
Thermal Conductivity
Thermal conductivity is a measure of a material's capacity to conduct heat. It is an intrinsic property that indicates how well a substance can transfer thermal energy. For a given material, its thermal conductivity is usually denoted by the symbol \( k \) and is expressed in watts per meter-kelvin (\( ext{W/m} cdot ext{K} \)).

In the context of the original problem, kapton is used as the conducting film. Kapton's thermal conductivity is \( 0.345 ext{ W/m} cdot ext{K} \). This relatively low value suggests that kapton is not a particularly great conductor of heat, but rather an insulator. Here's why it matters:
  • The thermal conductivity of the material affects the rate of heat transfer.
  • A higher \( k \) value means better heat conduction.
  • Materials like metals have high thermal conductivity; insulators like kapton have low values.
Understanding thermal conductivity allows us to choose appropriate materials for specific thermal management applications, such as in electronics or in thermal insulation.
Fourier's Law
Fourier's Law is a fundamental principle in understanding heat transfer through materials. It states that the heat flux within a material is proportional to the negative gradient of temperature and to the material's thermal conductivity. The mathematical expression for Fourier's Law is \( q = -k \cdot \frac{\Delta T}{d} \), where \( q \) is the heat flux, \( k \) is the thermal conductivity, \( \Delta T \) is the temperature difference, and \( d \) is the distance (or thickness) over which the temperature change occurs.

This equation allows us to calculate how much heat is being transferred through a material based on these factors. In practical terms, Fourier's Law is crucial for designing systems that efficiently manage heat dissipation, like in HVAC systems or heat sinks in electronic devices.
  • Describes heat flow through materials.
  • Heat flow is proportional to temperature gradient and thermal conductivity.
  • Used to calculate heat transfer across different media.
Knowing how to apply Fourier's Law helps engineers and scientists determine energy efficiency and develop technologies to manage heat effectively, ensuring systems function safely and optimally.

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Most popular questions from this chapter

When a long section of a compressed air line passes through the outdoors, it is observed that the moisture in the compressed air freezes in cold weather, disrupting and even completely blocking the air flow in the pipe. To avoid this problem, the outer surface of the pipe is wrapped with electric strip heaters and then insulated. Consider a compressed air pipe of length \(L=6 \mathrm{~m}\), inner radius \(r_{1}=3.7 \mathrm{~cm}\), outer radius \(r_{2}=4.0 \mathrm{~cm}\), and thermal conductivity \(k=14 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) equipped with a 300 -W strip heater. Air is flowing through the pipe at an average temperature of \(-10^{\circ} \mathrm{C}\), and the average convection heat transfer coefficient on the inner surface is \(h=30 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Assuming 15 percent of the heat generated in the strip heater is lost through the insulation, \((a)\) express the differential equation and the boundary conditions for steady one-dimensional heat conduction through the pipe, \((b)\) obtain a relation for the variation of temperature in the pipe material by solving the differential equation, and \((c)\) evaluate the inner and outer surface temperatures of the pipe.

Consider a homogeneous spherical piece of radioactive material of radius \(r_{o}=0.04 \mathrm{~m}\) that is generating heat at a constant rate of \(\dot{e}_{\text {gen }}=5 \times 10^{7} \mathrm{~W} / \mathrm{m}^{3}\). The heat generated is dissipated to the environment steadily. The outer surface of the sphere is maintained at a uniform temperature of \(110^{\circ} \mathrm{C}\) and the thermal conductivity of the sphere is \(k=15 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). Assuming steady one-dimensional heat transfer, \((a)\) express the differential equation and the boundary conditions for heat conduction through the sphere, \((b)\) obtain a relation for the variation of temperature in the sphere by solving the differential equation, and \((c)\) determine the temperature at the center of the sphere.

A spherical shell, with thermal conductivity \(k\), has inner and outer radii of \(r_{1}\) and \(r_{2}\), respectively. The inner surface of the shell is subjected to a uniform heat flux of \(\dot{q}_{1}\), while the outer surface of the shell is exposed to convection heat transfer with a coefficient \(h\) and an ambient temperature \(T_{c \infty}\). Determine the variation of temperature in the shell wall and show that the outer surface temperature of the shell can be expressed as \(T\left(r_{2}\right)=\left(\dot{q}_{1} / h\right)\left(r_{1} / r_{2}\right)^{2}+T_{\infty \text { co }}\).

Heat is generated in a 10 -cm-diameter spherical radioactive material whose thermal conductivity is \(25 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) uniformly at a rate of \(15 \mathrm{~W} / \mathrm{cm}^{3}\). If the surface temperature of the material is measured to be \(120^{\circ} \mathrm{C}\), the center temperature of the material during steady operation is (a) \(160^{\circ} \mathrm{C}\) (b) \(205^{\circ} \mathrm{C}\) (c) \(280^{\circ} \mathrm{C}\) (d) \(370^{\circ} \mathrm{C}\) (e) \(495^{\circ} \mathrm{C}\)

The temperature of a plane wall during steady onedimensional heat conduction varies linearly when the thermal conductivity is constant. Is this still the case when the thermal conductivity varies linearly with temperature?

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