What is the relation \((f / 2) \mathrm{Re}=\mathrm{Nu}=\mathrm{Sh}\) known as? Under what conditions is it valid? What is the practical importance of it? \(\mathrm{St}_{\text {mass }} \mathrm{Sc}^{2 / 3}\) and what are the names of the variables in it? Under what conditions is it valid? What is the importance of it in engineering?

Short Answer

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#tag_title# Short Answer The Chilton-Colburn analogy, expressed as \((f / 2) \mathrm{Re}=\mathrm{Nu}=\mathrm{Sh}\), is a useful relation for estimating heat, mass, and momentum transfer in fluid systems, provided that the flow is turbulent, steady-state, fully developed, and the fluid properties are constant. The term \(\mathrm{St}_{\text {mass }} \mathrm{Sc}^{2 / 3}\) is known as the Chilton-Colburn mass transfer Stanton number, and it provides an alternative method for estimating mass transfer coefficients under similar conditions. This analogy and the Stanton number are important in engineering for efficiently designing heat exchangers, cooling systems, mass transfer processes, and other equipment involved in heat and mass transfer.

Step by step solution

01

Relation \((f / 2) \mathrm{Re}=\mathrm{Nu}=\mathrm{Sh}\)

The relation \((f / 2) \mathrm{Re}=\mathrm{Nu}=\mathrm{Sh}\) is known as the Chilton-Colburn analogy or Chilton-Colburn j-factor analogy. This relation is useful in determining heat, mass, and momentum transfer in fluid systems.
02

Conditions for the Chilton-Colburn Analogy

The Chilton-Colburn analogy is valid under the following conditions: 1. The fluid flow is turbulent and steady-state. 2. The flow is fully developed in a pipe or over a flat plate. 3. The fluid properties, such as viscosity, density, thermal conductivity, and diffusivity, are constant.
03

Practical Importance of the Chilton-Colburn Analogy

The Chilton-Colburn analogy is important in engineering applications because it provides a useful tool for estimating heat and mass transfer coefficients in fluid systems. This helps engineers to efficiently design heat exchangers, cooling systems, and mass transfer processes.
04

Definition of \(\mathrm{St}_{\text {mass }} \mathrm{Sc}^{2 / 3}\)

The term \(\mathrm{St}_{\text {mass }} \mathrm{Sc}^{2 / 3}\) is known as the Chilton-Colburn mass transfer Stanton number (denoted as \(\mathrm{St}_{\text {mass }}\)). It includes the following variables: 1. \(\mathrm{Sc}\) : Schmidt number, the ratio of kinematic viscosity to mass diffusivity. 2. \(\mathrm{St}_{\text {mass }}\) : Mass transfer Stanton number, the ratio of mass transfer coefficient to average fluid velocity.
05

Conditions for the Validity of \(\mathrm{St}_{\text {mass }} \mathrm{Sc}^{2 / 3}\)

The term \(\mathrm{St}_{\text {mass }} \mathrm{Sc}^{2 / 3}\) is valid under certain conditions: 1. The fluid flow is turbulent. 2. The fluid properties, such as viscosity, density, thermal conductivity, and diffusivity, are constant. 3. The flow is fully developed in a pipe or over a flat plate.
06

Importance of \(\mathrm{St}_{\text {mass }} \mathrm{Sc}^{2 / 3}\) in Engineering

The Chilton-Colburn mass transfer Stanton number is important in engineering because it provides an alternative method for estimating mass transfer coefficients in fluid systems. It can be used to design mass transfer equipment, such as absorbers, evaporators, and distillation columns, by analyzing fluid flow and mass transfer behavior. This helps engineers optimize equipment efficiency and performance by accurately predicting mass transfer rates.

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Key Concepts

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

Heat Transfer
Understanding heat transfer is essential for a variety of engineering applications. Heat transfer is the movement of thermal energy from one object or medium to another. It occurs through three basic modes: conduction, convection, and radiation. In engineering, being able to predict and control heat transfer can be crucial for the design of systems such as heat exchangers, radiators, and HVAC systems.

When it comes to convection, which is the transfer of heat through fluid motion, the Chilton-Colburn analogy plays a key role. This analogy helps us estimate the convective heat transfer coefficient by relating it to the fluid’s momentum transfer. The convective heat transfer coefficient is necessary for calculating the rate of heat transfer in a system, which is vital for ensuring the appropriate functioning and safety of thermal devices.
Mass Transfer
Mass transfer involves the movement of particles from one location to another, often driven by a concentration gradient. This process is central to numerous engineering applications like separation processes, chemical reactors, and membrane technology. Analogous to how heat transfer is quantified, mass transfer also relies on coefficients that assess how effectively a species is transported in a fluid system.

The Chilton-Colburn analogy is useful for estimating these mass transfer coefficients, especially when dealing with turbulent flow conditions. Understanding and using the mass transfer Stanton number, coupled with the Schmidt number, allows engineers to predict mass transfer rates accurately. Such predictions are essential for the design and optimization of equipment like distillation towers, scrubbers, and bioreactors, where precise control of mass transfer is critical.
Fluid Mechanics
Fluid mechanics is the study of fluids in motion and at rest. It is a cornerstone of many engineering fields, playing a crucial role in understanding the behavior of liquids and gases in various applications. Core concepts include flow dynamics, pressure, viscosity, and turbulence -- all crucial for describing how fluids interact with their environments.

The Chilton-Colburn analogy stems from this domain as it pertains to turbulent flow, a common occurrence in engineering systems. It draws parallels between fluid momentum and heat and mass transfer phenomena. Grasping these relationships is vital for engineers when designing and analyzing systems like pipelines, pumps, and turbines, where fluid behavior directly impacts performance and efficiency.
Engineering Applications
Engineering applications of the Chilton-Colburn analogy are far-reaching. This principle aids in the design and analysis of thermal and mass transfer equipment, offering a simplified approach to complex calculations. It streamlines processes in industries such as chemical manufacturing, environmental engineering, and energy systems.

For example, the analogy is particularly useful for heat exchanger design, allowing engineers to estimate transfer coefficients under turbulent flow conditions, which otherwise would require extensive experimentation or complex numerical methods. Additionally, it supports the design of mass transfer equipment by providing a way to correlate mass transfer rates to easily measurable fluid properties. This analogy is a powerful tool in the hands of engineers, enabling them to innovate and improve system designs across a multitude of platforms.

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Most popular questions from this chapter

A 2-mm-thick 5-L vessel made of nickel is used to store hydrogen gas at \(358 \mathrm{~K}\) and \(300 \mathrm{kPa}\). If the total inner surface area of the vessel is \(1600 \mathrm{~cm}^{2}\), determine the rate of gas loss from the nickel vessel via mass diffusion. Also, determine the fraction of the hydrogen lost by mass diffusion after one year of storage.

Using Henry's law, show that the dissolved gases in a liquid can be driven off by heating the liquid.

A sphere of ice, \(5 \mathrm{~cm}\) in diameter, is exposed to \(50 \mathrm{~km} / \mathrm{h}\) wind with 10 percent relative humidity. Both the ice sphere and air are at \(-1^{\circ} \mathrm{C}\) and \(90 \mathrm{kPa}\). Predict the rate of evaporation of the ice in \(\mathrm{g} / \mathrm{h}\) by use of the following correlation for single spheres: Sh \(=\left[4.0+1.21(\mathrm{ReSc})^{2 / 3}\right]^{0.5}\). Data at \(-1^{\circ} \mathrm{C}\) and \(90 \mathrm{kPa}: D_{\text {air- } \mathrm{H}, \mathrm{O}}=2.5 \times 10^{-5} \mathrm{~m}^{2} / \mathrm{s}^{3}\), kinematic viscosity (air) \(=1.32 \times 10^{-7} \mathrm{~m}^{2} / \mathrm{s}\), vapor pressure \(\left(\mathrm{H}_{2} \mathrm{O}\right)=\) \(0.56 \mathrm{kPa}\) and density (ice) \(=915 \mathrm{~kg} / \mathrm{m}^{3}\).

During cold weather periods, vapor in a room diffuses through the dry wall and condenses in the adjoining insulation. This process decreases the thermal resistance and degrades the insulation. Consider a condition at which the vapor pressure in the air at \(25^{\circ} \mathrm{C}\) inside a room is \(3 \mathrm{kPa}\), and the vapor pressure in the insulation is negligible. The 3 -m-high and 10 -m-wide dry wall is 12-mm thick with a solubility of water vapor in the wall material of approximately \(0.007 \mathrm{kmol} / \mathrm{m}^{3}\).bar, and diffusion coefficient of water vapor in the wall is \(0.2 \times 10^{-9} \mathrm{~m}^{2} / \mathrm{s}\). Determine the mass diffusion rate of water vapor through the wall.

A heated piece of steel, with a uniform initial carbon concentration of \(0.20 \%\) by mass, was exposed to a carburizing atmosphere for an hour. Throughout the entire process, the carbon concentration on the surface was \(0.70 \%\). If the mass diffusivity of carbon in steel in this process was uniform at \(1 \times\) \(10^{-11} \mathrm{~m}^{2} / \mathrm{s}\), determine the percentage of mass concentration of carbon at \(0.2 \mathrm{~mm}\) and \(0.4 \mathrm{~mm}\) below the surface after the process.

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