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Why are the transient temperature charts prepared using nondimensionalized quantities such as the Biot and Fourier numbers instead of the actual variables such as thermal conductivity and time?

Short Answer

Expert verified
Answer: Transient temperature charts are prepared using nondimensionalized quantities like Biot and Fourier numbers because they offer several advantages such as easier comparison across various conditions and systems, generalization, and easier interpretation. Nondimensionalization simplifies complex equations, reduces the number of variables involved, and allows for a more universally applicable chart. Using Biot and Fourier numbers enables us to create a single chart that can be easily referenced and scaled to actual variables as needed, making analysis and understanding of temperature-dependent processes more accessible.

Step by step solution

01

Define Biot and Fourier numbers

First, let's define the Biot number (Bi) and Fourier number (Fo). The Biot number is a dimensionless parameter that characterizes the ratio of internal thermal resistance to external (convective) thermal resistance, and mathematically it is defined as: \[Bi = \frac{hL}{k}\] where \(h\) is the heat transfer coefficient (W/m²K), \(L\) is the characteristic length (m), and \(k\) is the thermal conductivity (W/mK). The Fourier number, on the other hand, is a dimensionless parameter relating to the rate of heat conduction and the rate of heat storage, and is given by: \[Fo = \frac{\alpha t}{L^2}\] where \(\alpha\) is the thermal diffusivity (m²/s) and \(t\) is the time (s).
02

Explain the importance of nondimensionalization

Nondimensionalization is the process of scaling quantities to remove dimensions, and it's useful in several ways: 1. Simplifying complex equations: By using dimensionless quantities, we can simplify complex equations that involve multiple parameters and dimensions into simpler forms. 2. Easier comparison of different systems: With dimensionless quantities, it's easier to compare different systems that may have widely varying scales or units. This makes it easy to generalize the results for a wider range of applications. 3. Reduced number of variables in an equation: Using nondimensionalized quantities decreases the number of variables in an equation, making it easier to solve and analyze. 4. Universality: Nondimensionalization allows the equation to be valid across different systems, regardless of the initial units being used.
03

Advantages of using Biot and Fourier numbers in transient temperature charts

Using Biot and Fourier numbers in transient temperature charts offers several advantages: 1. Easier comparison: By using Biot and Fourier numbers, we eliminate units associated with thermal conductivity, heat transfer coefficient, characteristic length, and time, enabling easier comparison of transient temperature charts for various conditions and systems. 2. Generalization: Using nondimensionalized quantities like Biot and Fourier numbers allows us to develop a single chart for various conditions and systems that can be easily referenced and scaled to actual variables as needed. 3. Easier interpretation: Transient temperature charts with nondimensionalized quantities are often easier to interpret, as they provide a simple method to look at trends and patterns across various systems and conditions, without involving the complexities of actual variables. In conclusion, preparing transient temperature charts using Biot and Fourier numbers, instead of actual variables like thermal conductivity and time, provide us with a more generalized and easily interpreted chart. The nondimensionalized quantities make it possible to draw comparisons across various systems and conditions, simplifying the analysis and understanding of temperature-dependent processes.

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Key Concepts

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

Biot Number
The Biot Number, denoted as \(Bi\), is an essential concept in heat transfer. This dimensionless number helps determine the relationship between the internal resistance to heat conduction within a body and the external resistance to heat convection on its surface. The formula for the Biot number is given by:\[Bi = \frac{hL}{k}\]where:
  • \(h\) is the heat transfer coefficient (W/m²K)
  • \(L\) is the characteristic length (m)
  • \(k\) is the thermal conductivity of the material (W/mK)
The Biot number helps determine whether temperature gradients within a solid are significant compared to the temperature changes with its environment. A small Biot number (less than 0.1) means that the body can be considered as having uniform temperature (lumped system analysis). On the other hand, a large Biot number implies significant internal thermal resistance, necessitating a more detailed analysis of temperature variation within the object.
Fourier Number
In heat conduction analysis, the Fourier Number, denoted as \(Fo\), plays a crucial role. This dimensionless number indicates how heat diffuses through a material over time, balancing between heat conduction and heat storage. It is calculated using the formula:\[Fo = \frac{\alpha t}{L^2}\]where:
  • \(\alpha\) is the thermal diffusivity (m²/s)
  • \(t\) is the time (s)
  • \(L\) is the characteristic length (m)
A higher Fourier Number suggests that heat has had more time to spread through the material, meaning the object is approaching thermal equilibrium. Therefore, the Fourier Number is crucial for determining the transient heat conduction behavior of a system, including how quickly a material will respond to thermal changes.
Transient Temperature Charts
Transient temperature charts, or graphs, provide a visual representation of how temperature within a material changes over time under certain conditions. They are typically plotted using dimensionless numbers like the Biot and Fourier numbers. This practice is highly beneficial due to several aspects:
  • Simplification: Dimensionless numbers reduce the complexity of the problem, allowing users to focus on important trends and behaviors without getting bogged down in unit conversions or specific values.
  • Generalization: Using these charts, one can easily compare different materials and conditions, as the same chart applies to all systems with similar dimensionless parameters.
  • Visualization: The trends of temperature change over time become easy to visualize, helping to predict how a system reacts to thermal inputs.
Overall, these charts are often more intuitive and easier to interpret than raw data, offering insights across many scenarios.
Heat Conduction Analysis
Heat conduction analysis involves studying how heat flows through materials. This process is incredibly important in fields like engineering, where understanding material responses to heat inputs can be crucial. By employing nondimensional numbers such as the Biot and Fourier Numbers, heat conduction analysis becomes more manageable and unified:
  • Reduced Complexity: Using nondimensional forms simplifies equations, making it easier to spot patterns and predict behaviors.
  • Universal Application: With concepts like nondimensionalization, different systems can be compared and analyzed using the same principles, regardless of their initial conditions or material properties.
  • Enhanced Predictive Power: Engineers and scientists can effectively predict system responses, troubleshoot potential heat management issues, and improve thermal design and efficiency.
Employing these concepts ensures a comprehensive understanding of how various materials interact with heat, aiding in a wide array of practical applications.

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Most popular questions from this chapter

Consider a sphere and a cylinder of equal volume made of copper. Both the sphere and the cylinder are initially at the same temperature and are exposed to convection in the same environment. Which do you think will cool faster, the cylinder or the sphere? Why?

Thick slabs of stainless steel \((k=14.9 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) and \(\left.\alpha=3.95 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}\right)\) and copper \((k=401 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) and \(\left.\alpha=117 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}\right)\) are subjected to uniform heat flux of \(8 \mathrm{~kW} / \mathrm{m}^{2}\) at the surface. The two slabs have a uniform initial temperature of \(20^{\circ} \mathrm{C}\). Determine the temperatures of both slabs, at \(1 \mathrm{~cm}\) from the surface, after \(60 \mathrm{~s}\) of exposure to the heat flux.

How does \((a)\) the air motion and (b) the relative humidity of the environment affect the growth of microorganisms in foods?

A long roll of 2-m-wide and \(0.5\)-cm-thick 1-Mn manganese steel plate coming off a furnace at \(820^{\circ} \mathrm{C}\) is to be quenched in an oil bath \(\left(c_{p}=2.0 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K}\right)\) at \(45^{\circ} \mathrm{C}\). The metal sheet is moving at a steady velocity of \(15 \mathrm{~m} / \mathrm{min}\), and the oil bath is \(9 \mathrm{~m}\) long. Taking the convection heat transfer coefficient on both sides of the plate to be \(860 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), determine the temperature of the sheet metal when it leaves the oil bath. Also, determine the required rate of heat removal from the oil to keep its temperature constant at \(45^{\circ} \mathrm{C}\).

Oxy-fuel combustion power plants use pulverized coal particles as fuel to burn in a pure oxygen environment to generate electricity. Before entering the furnace, pulverized spherical coal particles with an average diameter of \(300 \mu \mathrm{m}\), are being transported at \(2 \mathrm{~m} / \mathrm{s}\) through a \(3-\mathrm{m}\) long heated tube while suspended in hot air. The air temperature in the tube is \(900^{\circ} \mathrm{C}\) and the average convection heat transfer coefficient is \(250 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Determine the temperature of the coal particles at the exit of the heated tube, if the initial temperature of the particles is \(20^{\circ} \mathrm{C}\).

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