A room at \(20^{\circ} \mathrm{C}\) air temperature is loosing heat to the outdoor air at \(0^{\circ} \mathrm{C}\) at a rate of \(1000 \mathrm{~W}\) through a \(2.5\)-m-high and 4 -m-long wall. Now the wall is insulated with \(2-\mathrm{cm}\) thick insulation with a conductivity of \(0.02 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). Determine the rate of heat loss from the room through this wall after insulation. Assume the heat transfer coefficients on the inner and outer surface of the wall, the room air temperature, and the outdoor air temperature to remain unchanged. Also, disregard radiation. (a) \(20 \mathrm{~W}\) (b) \(561 \mathrm{~W}\) (c) \(388 \mathrm{~W}\) (d) \(167 \mathrm{~W}\) (e) \(200 \mathrm{~W}\)

Short Answer

Expert verified
Answer: The new rate of heat loss after adding the insulation is approximately 20 W.

Step by step solution

01

Find the temperature difference between indoor and outdoor air

We are given the temperature of indoor and outdoor air. To find the temperature difference, subtract the outdoor air temperature from the indoor air temperature: \(\Delta T = T_{indoor} - T_{outdoor} = 20^{\circ} C - 0^{\circ} C = 20^{\circ} C\)
02

Calculate the area of the wall

To calculate the area of the wall, multiply the height and length of the wall: \(A = height \times length = 2.5 \mathrm{m} \times 4 \mathrm{m} = 10 \mathrm{m^2}\)
03

Determine the thermal resistance of the insulation

The thermal resistance of the insulation can be calculated using the formula: \(R_{insulation} = \frac{thickness}{k} = \frac{0.02 \mathrm{m}}{0.02 \mathrm{W/m \cdot K}} = 1 \mathrm{K/W}\)
04

Calculate the total thermal resistance

We're given that the rate of heat loss (without the insulation) is 1000 W. So, we can calculate the total thermal resistance of the wall without insulation: \(R_{total} = \frac{\Delta T}{Q} = \frac{20 \mathrm{K}}{1000 \mathrm{W}} = 0.02 \mathrm{K/W}\) Now that we've found the insulation's thermal resistance, we can add we add the thermal resistance value of the insulation to find the total thermal resistance of the wall with insulation: \(R_{total}^{'} = R_{total} + R_{insulation} = 0.02 \mathrm{K/W} + 1 \mathrm{K/W} = 1.02 \mathrm{K/W}\)
05

Calculate the new rate of heat loss

Now we can use the new total thermal resistance to calculate the new rate of heat loss: \(Q^{'} = \frac{\Delta T}{R_{total}^{'}} = \frac{20 \mathrm{K}}{1.02 \mathrm{K/W}} = 19.61 \mathrm{W}\) The result is approximately 20 W, which corresponds to the answer (a) \(20 \mathrm{W}\).

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Key Concepts

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

Understanding Thermal Resistance
Thermal resistance is a concept that measures the ability of a material to resist the flow of heat. It is especially useful in the context of insulation and building design, because it helps determine how effectively a material can prevent heat exchange between different areas. To put it simply, thermal resistance is to heat transfer what electrical resistance is to electrical current.

Let's use the example given in the exercise. In this scenario, the insulation added to the wall has a thermal resistance calculated by dividing its thickness by its thermal conductivity, resulting in a value of 1 K/W. This number represents how much temperature difference (in Kelvin) would cause one watt of heat to flow through the insulator per second. The higher the thermal resistance, the less heat is lost, as there is more resistance to the heat flow.

In a practical sense, when you add insulation to a wall, the total thermal resistance of the wall increases. It's like adding an extra layer of clothing on a cold day—it slows down the rate at which your body loses heat to the environment. Hence, to improve the heat efficiency of a room or any enclosed space, one should aim to increase the overall thermal resistance of the enclosure. This concept is why we often seek materials with high thermal resistance for insulation purposes.
The Role of Thermal Conductivity in Heat Loss
Thermal conductivity is a measure of a material's ability to conduct heat. It represents how easily heat can pass through a material, with high values indicating that a material is a good heat conductor, like metal, and lower values indicating a poor heat conductor, such as foam insulation.

The exercise provided gives us the thermal conductivity of the wall insulation (0.02 W/m·K), which is a crucial piece of data for calculating how much heat will be lost through the wall. A key point in understanding thermal conductivity is that it's an intrinsic property of the material itself, and not affected by its dimensions or shape. However, when it comes to a physical installation, the size, shape, and thickness of the material will determine how much heat is transferred – which brings us back to thermal resistance, which does take into account the material’s dimensions.

Generally, in building and home improvement, materials with low thermal conductivity are sought for insulation to minimize heat transfer and therefore energy usage. The challenge lies in balancing good insulation while also addressing factors like cost, durability, and other structural needs.
Heat Transfer Coefficient's Impact on Insulation
The heat transfer coefficient is an indicator of how well heat is transmitted from a material to its surroundings (like air or water). In technical terms, it quantifies the amount of heat that passes through a unit area of a material, for a given temperature difference between the material and its environment. Higher coefficients mean that heat is transferred more efficiently, and vice versa. Its role in our context is passive, yet it's an essential part of the whole system that determines how much energy is lost to the surroundings.

In the exercise, we are asked to assume the heat transfer coefficients on the inner and outer surface of the wall remain constant. The significance of this assumption can't be overstated. It allows a straightforward calculation by ignoring the complex nature of how different materials might alter these coefficients. For further heat loss calculations, understanding the heat transfer coefficient can help in selecting the right materials for a building's exterior that will interface effectively with the environment.

For instance, glass has a different heat transfer coefficient compared to brick. When designing or improving a building’s energy efficiency, this coefficient is pivotal. One could theoretically use materials that inherently have a lower heat transfer coefficient to reduce heat loss or gain without significantly altering the structure's thermal resistance.

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Most popular questions from this chapter

Two plate fins of constant rectangular cross section are identical, except that the thickness of one of them is twice the thickness of the other. For which fin is the \((a)\) fin effectiveness and \((b)\) fin efficiency higher? Explain.

A row of 3 -ft-long and 1-in-diameter used uranium fuel rods that are still radioactive are buried in the ground parallel to each other with a center-to- center distance of 8 in at a depth of \(15 \mathrm{ft}\) from the ground surface at a location where the thermal conductivity of the soil is \(0.6 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft} \cdot{ }^{\circ} \mathrm{F}\). If the surface temperature of the rods and the ground are \(350^{\circ} \mathrm{F}\) and \(60^{\circ} \mathrm{F}\), respectively, determine the rate of heat transfer from the fuel rods to the atmosphere through the soil.

An 8-m-internal-diameter spherical tank made of \(1.5\)-cm-thick stainless steel \((k=15 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) is used to store iced water at \(0^{\circ} \mathrm{C}\). The tank is located in a room whose temperature is \(25^{\circ} \mathrm{C}\). The walls of the room are also at \(25^{\circ} \mathrm{C}\). The outer surface of the tank is black (emissivity \(\varepsilon=1\) ), and heat transfer between the outer surface of the tank and the surroundings is by natural convection and radiation. The convection heat transfer coefficients at the inner and the outer surfaces of the tank are \(80 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) and \(10 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), respectively. Determine \((a)\) the rate of heat transfer to the iced water in the tank and \((b)\) the amount of ice at \(0^{\circ} \mathrm{C}\) that melts during a 24 -h period. The heat of fusion of water at atmospheric pressure is \(h_{i f}=333.7 \mathrm{~kJ} / \mathrm{kg}\).

A 0.3-cm-thick, 12-cm-high, and 18-cm-long circuit board houses 80 closely spaced logic chips on one side, each dissipating \(0.04 \mathrm{~W}\). The board is impregnated with copper fillings and has an effective thermal conductivity of \(30 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). All the heat generated in the chips is conducted across the circuit board and is dissipated from the back side of the board to a medium at \(40^{\circ} \mathrm{C}\), with a heat transfer coefficient of \(40 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). (a) Determine the temperatures on the two sides of the circuit board. (b) Now a \(0.2\)-cm-thick, 12-cm-high, and 18-cmlong aluminum plate \((k=237 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) with 864 2-cm-long aluminum pin fins of diameter \(0.25 \mathrm{~cm}\) is attached to the back side of the circuit board with a \(0.02\)-cm-thick epoxy adhesive \((k=1.8 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\). Determine the new temperatures on the two sides of the circuit board.

We are interested in steady state heat transfer analysis from a human forearm subjected to certain environmental conditions. For this purpose consider the forearm to be made up of muscle with thickness \(r_{m}\) with a skin/fat layer of thickness \(t_{s f}\) over it, as shown in the Figure P3-138. For simplicity approximate the forearm as a one-dimensional cylinder and ignore the presence of bones. The metabolic heat generation rate \(\left(\dot{e}_{m}\right)\) and perfusion rate \((\dot{p})\) are both constant throughout the muscle. The blood density and specific heat are \(\rho_{b}\) and \(c_{b}\), respectively. The core body temperate \(\left(T_{c}\right)\) and the arterial blood temperature \(\left(T_{a}\right)\) are both assumed to be the same and constant. The muscle and the skin/fat layer thermal conductivities are \(k_{m}\) and \(k_{s f}\), respectively. The skin has an emissivity of \(\varepsilon\) and the forearm is subjected to an air environment with a temperature of \(T_{\infty}\), a convection heat transfer coefficient of \(h_{\text {conv }}\), and a radiation heat transfer coefficient of \(h_{\mathrm{rad}}\). Assuming blood properties and thermal conductivities are all constant, \((a)\) write the bioheat transfer equation in radial coordinates. The boundary conditions for the forearm are specified constant temperature at the outer surface of the muscle \(\left(T_{i}\right)\) and temperature symmetry at the centerline of the forearm. \((b)\) Solve the differential equation and apply the boundary conditions to develop an expression for the temperature distribution in the forearm. (c) Determine the temperature at the outer surface of the muscle \(\left(T_{i}\right)\) and the maximum temperature in the forearm \(\left(T_{\max }\right)\) for the following conditions: $$ \begin{aligned} &r_{m}=0.05 \mathrm{~m}, t_{s f}=0.003 \mathrm{~m}, \dot{e}_{m}=700 \mathrm{~W} / \mathrm{m}^{3}, \dot{p}=0.00051 / \mathrm{s} \\ &T_{a}=37^{\circ} \mathrm{C}, T_{\text {co }}=T_{\text {surr }}=24^{\circ} \mathrm{C}, \varepsilon=0.95 \\ &\rho_{b}=1000 \mathrm{~kg} / \mathrm{m}^{3}, c_{b}=3600 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}, k_{m}=0.5 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K} \\ &k_{s f}=0.3 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, h_{\text {conv }}=2 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}, h_{\mathrm{rad}}=5.9 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K} \end{aligned} $$

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