/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 17 Pressurized steam at \(450 \math... [FREE SOLUTION] | 91Ó°ÊÓ

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Pressurized steam at \(450 \mathrm{~K}\) flows through a long, thinwalled pipe of \(0.5-\mathrm{m}\) diameter. The pipe is enclosed in a concrete casing that is of square cross section and \(1.5 \mathrm{~m}\) on a side. The axis of the pipe is centered in the casing, and the outer surfaces of the casing are maintained at \(300 \mathrm{~K}\). What is the heat loss per unit length of pipe?

Short Answer

Expert verified
The heat loss per unit length of the pipe can be expressed as: \[Q_L = U \Delta T \times \frac{\pi}{2} \times L\] where \(U\) is the overall heat transfer coefficient, \(\Delta T\) is the temperature difference between the steam and the outer surfaces of the casing, and \(L\) is the length of the pipe. Without the exact values of the heat transfer coefficients and the thermal conductivity of the system, we cannot find an exact value for the heat loss. However, this expression allows us to determine the heat loss for any given overall heat transfer coefficient and temperature difference.

Step by step solution

01

Determine the effective thermal conductivity of the system

We have a long, thin-walled pipe enclosed in a square concrete casing. To analyze this problem, we will consider the system as two concentric cylinders. One represents the pipe (inner cylinder) and the other represents the concrete casing (outer cylinder). The effective thermal conductivity of the system can be found using the formula for the overall heat transfer coefficient: \[U = \frac{1}{\frac{1}{h_i} + \frac{\ln{(r_o / r_i)}}{2\pi k_c} + \frac{1}{h_o}}\] where: - \(U\) is the overall heat transfer coefficient - \(h_i\) is the convective heat transfer coefficient inside the pipe - \(h_o\) is the convective heat transfer coefficient outside the casing - \(r_i\) is the inner radius of the pipe - \(r_o\) is the outer radius of the concrete casing - \(k_c\) is the thermal conductivity of the concrete In this problem, we are not given the values for \(h_i\), \(h_o\), and \(k_c\). Therefore, we will be looking for the heat loss per unit length for any given heat transfer coefficients.
02

Calculate the heat transfer rate through the pipe and concrete

Given the temperature difference between the steam and the outer surfaces of the concrete casing, and the overall heat transfer coefficient, we can calculate the heat transfer rate per unit area of the pipe as: \[q = U \Delta T\] where: - \(q\) is the heat transfer rate per unit area - \(\Delta T = T_{steam} - T_{outer}\) is the temperature difference between the steam and the outer surfaces of the concrete casing
03

Find the heat loss per unit length of the pipe

Now that we have the heat transfer rate per unit area, we can calculate the heat loss per unit length of the pipe. To do this, we multiply the heat transfer rate per unit area by the surface area of the pipe over a given length. \[Q_L = q \times A_\text{pipe}\] where \(Q_L\) is the heat loss per unit length of the pipe, and \(A_\text{pipe}\) is the surface area per unit length. In this case, the pipe is cylindrical, so its surface area per unit length can be calculated as: \[A_\text{pipe} = 2\pi r_\text{pipe} \times L\] Substituting the values given in the problem statement, we have: \[Q_L = q \times 2\pi \frac{0.5}{2} \times L\] The heat loss per unit length of the pipe will be provided in terms of the overall heat transfer coefficient, so the final expression for the heat loss per unit length of the pipe can be written as: \[Q_L = U \Delta T \times \frac{\pi}{2} \times L\] Since we do not know the values of the heat transfer coefficients and the thermal conductivity of the system, we cannot find an exact value for the heat loss per unit length of the pipe. However, we have a general expression that we can use to determine the heat loss for any given overall heat transfer coefficient and temperature difference.

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Key Concepts

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

Convective Heat Transfer Coefficient
The convective heat transfer coefficient, often denoted as \(h\), is a crucial parameter in the analysis of heat transfer through fluids. It quantifies the heat transfer rate or efficiency between a solid surface and a fluid flowing over or adjacent to it. In our given problem, the convective heat transfer coefficients are \(h_i\) inside the pipe and \(h_o\) outside the casing.
These coefficients depend on several factors:
  • The nature of the fluid (such as air, steam, water)
  • Flow conditions (e.g., laminar or turbulent)
  • Surface characteristics of the solid
  • Temperature difference between the fluid and the surface
The coefficients are essential when linking the temperature gradient at the surface with the heat transfer occurring across the fluid boundary layer. To calculate \(U\), the overall heat transfer coefficient, in the original problem, knowing \(h_i\) and \(h_o\) would be necessary. When these are unknown, the formula allows estimation of potential heat loss under different hypothetical values for \(h_i\) and \(h_o\).
Thermal Conductivity
Thermal conductivity is a property that quantifies how well a material can conduct heat. Represented with \(k\), it reflects how easily heat can pass through a specific material. In the context of our exercise, it is denoted as \(k_c\), referring to the thermal conductivity of the concrete casing.
The value of thermal conductivity varies with
  • the type of material
  • temperature
  • the material's phase (solid, liquid, or gas)
In engineering applications, thermal conductivity is critical when designing systems that involve thermal insulation or heat dissipation. Within the original exercise, you'll see its influence play a vital role as a factor in calculating the overall heat transfer coefficient \(U\), especially for the casing that envelops the steam pipe.
Overall Heat Transfer Coefficient
The overall heat transfer coefficient, \(U\), serves as a comprehensive measure reflecting total resistance to heat transfer through a series of conductive and convective layers. Reflecting the entire heat exchange system, from the steam to the surrounding environment, \(U\) is crucial for assessing the system's thermal performance.
In the formula given:\[U = \frac{1}{\frac{1}{h_i} + \frac{\ln{(r_o / r_i)}}{2\pi k_c} + \frac{1}{h_o}}\]we account for both convective and conductive heat transfer processes:
  • \(\frac{1}{h_i}\): resistance due to the internal convective heat transfer within the pipe
  • \(\frac{\ln{(r_o / r_i)}}{2\pi k_c}\): conductive resistance offered by the concrete casing
  • \(\frac{1}{h_o}\): resistance from the external convection around the concrete casing
The calculation of \(U\) allows engineers to understand how alterations in materials, thickness, or fluid dynamics might influence heat loss. This parameter ultimately guides decision-making when it comes to improving heat transfer efficiency or reducing energy losses in thermal systems.

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Most popular questions from this chapter

Conduction within relatively complex geometries can sometimes be evaluated using the finite-difference methods of this text that are applied to subdomains and patched together. Consider the two-dimensional domain formed by rectangular and cylindrical subdomains patched at the common, dashed control surface. Note that, along the dashed control surface, temperatures in the two subdomains are identical and local conduction heat fluxes to the cylindrical subdomain are identical to local conduction heat fluxes from the rectangular subdomain. Calculate the heat transfer per unit depth into the page, \(q^{\prime}\), using \(\Delta x=\Delta y=\Delta r=10 \mathrm{~mm}\) and \(\Delta \phi=\pi / 8\). The base of the rectangular subdomain is held at \(T_{h}=20^{\circ} \mathrm{C}\), while the vertical surface of the cylindrical subdomain and the surface at outer radius \(r_{o}\) are at \(T_{c}=0^{\circ} \mathrm{C}\). The remaining surfaces are adiabatic, and the thermal conductivity is \(k=10 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\).

A rod of \(10-\mathrm{mm}\) diameter and \(250-\mathrm{mm}\) length has one end maintained at \(100^{\circ} \mathrm{C}\). The surface of the rod experiences free convection with the ambient air at \(25^{\circ} \mathrm{C}\) and a convection coefficient that depends on the difference between the temperature of the surface and the ambient air. Specifically, the coefficient is prescribed by a correlation of the form, \(h_{\mathrm{fc}}=2.89[0.6+0.624\) \(\left.\left(T-T_{\infty}\right)^{1 / 6}\right]^{2}\), where the units are \(h_{\mathrm{fc}}\left(\mathrm{W} / \mathrm{m}^{2} \cdot \mathrm{K}\right)\) and \(T(\mathrm{~K})\). The surface of the rod has an emissivity \(\varepsilon=0.2\) and experiences radiation exchange with the surroundings at \(T_{\text {sur }}=25^{\circ} \mathrm{C}\). The fi tip also experiences free convection and radiation exchange. Assuming one-dimensional conduction and using a finite-difference method representing the fin by five nodes, estimate the temperature distribution for the fin. Determine also the fin heat rate and the relative contributions of free convection and radiation exchange. Hint: For each node requiring an energy balance, use the linearized form of the radiation rate equation, Equation 1.8, with the radiation coefficient \(h_{r}\), Equation \(1.9\), evaluated for each node. Similarly, for the convection rate equation associated with each node, the free convection coefficient \(h_{\mathrm{fc}}\) must be evaluated for each node.

Consider nodal configuration 4 of Table \(4.2\). Derive the finite-difference equations under steady-state conditions for the following situations. (a) The upper boundary of the external corner is perfectly insulated and the side boundary is subjected to the convection process \(\left(T_{\infty}, h\right)\). (b) Both boundaries of the external corner are perfectly insulated. How does this result compare with Equation 4.43?

A common arrangement for heating a large surface area is to move warm air through rectangular ducts below the surface. The ducts are square and located midway between the top and bottom surfaces that are exposed to room air and insulated, respectively. For the condition when the floor and duct temperatures are 30 and \(80^{\circ} \mathrm{C}\), respectively, and the thermal conductivity of concrete is \(1.4 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\), calculate the heat rate from each duct, per unit length of duct. Use a grid spacing with \(\Delta x=2 \Delta y\), where \(\Delta y=0.125 L\) and \(L=150 \mathrm{~mm}\).

A long bar of rectangular cross section is \(60 \mathrm{~mm} \times\) \(90 \mathrm{~mm}\) on a side and has a thermal conductivity of \(1 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). One surface is exposed to a convection process with air at \(100^{\circ} \mathrm{C}\) and a convection coeffient of \(100 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), while the remaining surfaces are maintained at \(50^{\circ} \mathrm{C}\). (a) Using a grid spacing of \(30 \mathrm{~mm}\) and the Gauss-Seidel iteration method, determine the nodal temperatures and the heat rate per unit length normal to the page into the bar from the air. (b) Determine the effect of grid spacing on the temperature field and heat rate. Specifically, consider a grid spacing of \(15 \mathrm{~mm}\). For this grid, explore the effect of changes in \(h\) on the temperature field and the isotherms.

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