When plotting the thermal resistance network associated with a heat transfer problem, explain when two resistances are in series and when they are in parallel.

Short Answer

Expert verified
Two thermal resistances are in series when there is no branching in the heat flow path, and the same heat transfer rate flows through both resistances. They are in parallel when they share the same initial and final temperatures, with the heat transfer rate splitting between the resistances. In a thermal resistance network, series connections can be observed in a composite wall with layers of different thermal conductivities, while parallel connections can be found in situations where there are multiple heat flow paths, such as parallel layers of insulation in a roof.

Step by step solution

01

Introduction to Thermal Resistance Networks

Thermal resistance networks help in simplifying and analyzing heat transfer problems. They are analogous to electrical resistance networks, where instead of electrical resistance and electric current, we have thermal resistance and heat transfer rate.
02

Definition of Series and Parallel Connections

In general, two components are said to be in series if they share a common node and the same current (or heat transfer rate) flows through both. Components are said to be in parallel if they are connected across the same pair of nodes and are subjected to the same voltage (or temperature) difference.
03

Thermal Resistances in Series

Two thermal resistances are in series when there is no branching in the heat flow path, and the same heat transfer rate flows through both resistances. In this case, the total thermal resistance is the sum of the individual resistances. For example, if we consider heat flow through a composite wall composed of layers with different thermal conductivities, we can represent the thermal resistance of each layer in series, as the heat transfer rate is the same through each layer.
04

Mathematical Representation of Series Connection

Let \(R_{1}\) and \(R_{2}\) be two thermal resistances in series. The total thermal resistance, \(R_{total}\), can be calculated as: \[R_{total} = R_{1} + R_{2}\]
05

Thermal Resistances in Parallel

Two thermal resistances are in parallel when they share the same initial and final temperatures, with heat transfer rate splitting between the resistances. In this case, the total thermal resistance is determined by the reciprocal of the sum of the reciprocals of the individual resistances. For example, when there are two possible heat flow paths (e.g., heat flow through the parallel layers of insulation in a roof), the thermal resistances can be represented in parallel.
06

Mathematical Representation of Parallel Connection

Let \(R_{1}\) and \(R_{2}\) be two thermal resistances in parallel. The total thermal resistance, \(R_{total}\), can be calculated as: \[\frac{1}{R_{total}} = \frac{1}{R_{1}} + \frac{1}{R_{2}} \] Or alternatively, \[R_{total} = \frac{R_{1} \cdot R_{2}}{R_{1} + R_{2}}\]

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Key Concepts

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

Understanding Heat Transfer Analysis
Heat transfer analysis is a fundamental concept that relates to the movement of thermal energy from one point to another due to temperature difference. This movement can occur through various mechanisms: conduction, which occurs in solids; convection, which involves liquids or gases; and radiation, which does not require a medium and can happen through a vacuum.

To analyze heat transfer effectively, engineers often use an approach that models the transfer of heat as an equivalent electrical circuit, known as a thermal resistance network. This model allows us to simplify complex systems into a series of thermal resistances that can predict the heat transfer rate through different materials or across boundaries. Understanding this analysis is crucial to designing and optimizing thermal systems, like insulation in buildings, cooling systems in electronics, or heat exchangers in industrial processes.

Applying Thermal Resistance Networks

By creating a diagram representing the network of thermal resistances, which are an analogy to electrical resistors, we can effectively plot the pathways of heat transfer. These pathways must obey the laws of thermodynamics and physics, with the direction of heat flow always moving from hot to cold regions. Each component in the network adds to the overall resistance to heat flow, and can be calculated in a manner similar to electrical circuits, with series and parallel arrangements.
Series and Parallel Resistances in Thermal Systems
The arrangement of thermal resistances in a system, whether in series or parallel, greatly affects the overall heat transfer rate. Just like in electrical circuits, these configurations change how thermal energy flows through the system and thus how the total resistance to heat flow is calculated.

Series Thermal Resistances

When two thermal resistances are in series, they share a common heat flow path, and thus the same amount of heat must pass sequentially through both resistances. This is typically seen in layered structures, like walls with multiple material layers. The total resistance is just the sum of individual resistances since they act as barriers one after another, making heat flow more difficult the more resistances it encounters.

Parallel Thermal Resistances

On the other hand, parallel thermal resistances involve heat dividing its path, flowing through multiple resistances simultaneously from the same initial to the same final point. A good analogy would be a road branching into multiple lanes; they start and end at the same points, but vehicles (heat) can take different routes. In such configurations, the total resistance is not merely a sum but is instead decreased because there are additional paths for the heat to take, effectively allowing more heat to pass through in a given amount of time.
Calculating Thermal Resistances
Performing the thermal resistances calculation is key to predicting how effectively heat will be transferred in a system. As laid out in the exercise solutions, the calculations for series and parallel arrangements follow specific formulas, akin to their electrical counterparts.

For series-connected thermal resistances, the total thermal resistance (\(R_{total}\)) is simply the sum of the individual resistances (\(R_{1}\) and \(R_{2}\)). This reflects the additive nature of resistance in a single pathway for heat flow.

In a parallel connection, however, the heat has the option to pass through multiple routes, and so the total resistance is less than each individual resistance. The formula for parallel thermal resistance involves taking the inverse of the sum of the inverses of each resistance, as shown in the solution. Ensuring a proper understanding of these formulas is crucial for students tackling heat transfer problems as it allows them to quantify each component's impact on the system's overall thermal performance and make informed decisions in design, material selection, and system analysis.

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Most popular questions from this chapter

The heat transfer surface area of a fin is equal to the sum of all surfaces of the fin exposed to the surrounding medium, including the surface area of the fin tip. Under what conditions can we neglect heat transfer from the fin tip?

Circular cooling fins of diameter \(D=1 \mathrm{~mm}\) and length \(L=25.4 \mathrm{~mm}\), made of copper \((k=400 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\), are used to enhance heat transfer from a surface that is maintained at temperature \(T_{s 1}=132^{\circ} \mathrm{C}\). Each rod has one end attached to this surface \((x=0)\), while the opposite end \((x=L)\) is joined to a second surface, which is maintained at \(T_{s 2}=0^{\circ} \mathrm{C}\). The air flowing between the surfaces and the rods is also at \(T_{\infty}=0^{\circ} \mathrm{C}\), and the convection coefficient is \(h=100 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). (a) Express the function \(\theta(x)=T(x)-T_{\infty}\) along a fin, and calculate the temperature at \(x=L / 2\). (b) Determine the rate of heat transferred from the hot surface through each fin and the fin effectiveness. Is the use of fins justified? Why? (c) What is the total rate of heat transfer from a \(10-\mathrm{cm}\) by 10 -cm section of the wall, which has 625 uniformly distributed fins? Assume the same convection coefficient for the fin and for the unfinned wall surface.

What is the value of conduction shape factors in engineering?

A cylindrical pin fin of diameter \(0.6 \mathrm{~cm}\) and length of \(3 \mathrm{~cm}\) with negligible heat loss from the tip has an efficiency of 0.7. The effectiveness of this fin is (a) \(0.3\) (b) \(0.7\) (c) 2 (d) 8 (e) 14

Hot- and cold-water pipes \(8 \mathrm{~m}\) long run parallel to each other in a thick concrete layer. The diameters of both pipes are \(5 \mathrm{~cm}\), and the distance between the centerlines of the pipes is \(40 \mathrm{~cm}\). The surface temperatures of the hot and cold pipes are \(60^{\circ} \mathrm{C}\) and \(15^{\circ} \mathrm{C}\), respectively. Taking the thermal conductivity of the concrete to be \(k=0.75 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\), determine the rate of heat transfer between the pipes.

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