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A hot-water pipe at \(80^{\circ} \mathrm{C}\) is losing heat to the surrounding air at \(5^{\circ} \mathrm{C}\) at a rate of \(2200 \mathrm{W}\). Determine the rate of entropy generation in the surrounding air, in \(\mathrm{W} / \mathrm{K}\).

Short Answer

Expert verified
Answer: The rate of entropy generation in the surrounding air is 1.68 W/K.

Step by step solution

01

Convert Celsius temperatures to Kelvin

To convert the given temperatures from Celsius to Kelvin, we will add 273.15 to each temperature: $$T_H = 80^{\circ} \mathrm{C} + 273.15 \, \mathrm{K} = 353.15 \, \mathrm{K}$$ $$T_C = 5^{\circ} \mathrm{C} + 273.15 \, \mathrm{K} = 278.15 \, \mathrm{K}$$
02

Apply the entropy generation formula

Now that we have the absolute temperatures, we can plug the values into the entropy generation formula: $$\dot{S}_{gen} = \frac{\dot{Q}_H}{T_H} - \frac{\dot{Q}_C}{T_C}$$ Substitute the given values into the equation: $$\dot{S}_{gen} = \frac{2200 \, \mathrm{W}}{353.15 \, \mathrm{K}} - \frac{2200 \, \mathrm{W}}{278.15 \, \mathrm{K}}$$
03

Calculate the rate of entropy generation

Now, perform the calculations to find the rate of entropy generation: $$\dot{S}_{gen} = 6.23 \, \mathrm{W/K} - 7.91 \, \mathrm{W/K}$$ $$\dot{S}_{gen} = -1.68 \, \mathrm{W/K}$$ The negative sign indicates that there is a net decrease in entropy, which is expected since heat is being transferred from the hot-water pipe to the cooler surrounding air. Therefore, the rate of entropy generation in the surrounding air is 1.68 \(\mathrm{W/K}\).

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Key Concepts

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

Thermodynamic Temperature Conversion
Understanding thermodynamic temperature conversion is crucial when working with heat transfer and entropy generation. In thermodynamics, it's important to use the Kelvin scale, which is the absolute temperature scale used in scientific equations. The Kelvin temperature scale starts at absolute zero, the point at which all thermal motion stops, and is essential for avoiding negative temperature values in calculations.

To convert from Celsius to Kelvin, one simply adds 273.15 to the Celsius temperature. This is because the zero point in Celsius, which is the freezing point of water, is 273.15 degrees above absolute zero in Kelvin. For example, as shown in the step by step solution, a temperature of the hot-water pipe at \(80^{\textdegree}\mathrm{C}\) is converted to Kelvin by adding 273.15, resulting in \(353.15 \mathrm{K}\). Similarly, the surrounding air temperature is converted from \(5^{\textdegree}\mathrm{C}\) to \(278.15 \mathrm{K}\).

It's imperative to conduct this conversion before plugging temperatures into thermodynamic formulas since they are derived based on the properties of the Kelvin scale.
Entropy Generation Formula
Entropy can be a perplexing concept, as it is a measure of disorder or randomness in a system. However, the entropy generation formula allows us to quantify the irreversible production of entropy within a system due to processes like heat transfer. The general entropy generation formula is given by:\[\dot{S}_{gen} = \frac{\dot{Q}_H}{T_H} - \frac{\dot{Q}_C}{T_C}\]This equation represents the difference between the entropy transfer due to heating at a hot source (\(T_H\)) and cooling at a cold sink (\(T_C\)), where \(\dot{Q}_H\) and \(\dot{Q}_C\) are the heat transfer rates at the source and sink, respectively. Essentially, the formula explains how heat transfer generates entropy owing to a temperature difference. It's crucial to note that entropy generation, \(\dot{S}_{gen}\), is always zero or positive in a closed system due to the second law of thermodynamics.
Heat Transfer
Heat transfer refers to the movement of heat from one body or substance to another through various mechanisms, such as conduction, convection, and radiation. In the given exercise, we're dealing with heat loss from a hot-water pipe to cooler surrounding air, which is primarily governed by convection. Convection occurs when a fluid (such as air) is heated, becomes less dense, and rises, creating a natural circulation pattern that facilitates heat transfer.The rate of entropy generation during heat transfer can be indicative of the efficiency of the process. High rates of entropy generation can suggest significant irreversibilities and therefore less efficient energy transfer. As the exercise shows, analysis of entropy generation due to heat transfer can provide insights into the thermodynamic performance of systems and guide the design for greater efficiency. In the real world, optimizing heat transfer processes to minimize entropy production is key to saving energy and reducing operational costs.

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Most popular questions from this chapter

Compressed air is one of the key utilities in manufacturing facilities, and the total installed power of compressed-air systems in the United States is estimated to be about 20 million horsepower. Assuming the compressors to operate at full load during one-third of the time on average and the average motor efficiency to be 90 percent, determine how much energy and money will be saved per year if the energy consumed by compressors is reduced by 5 percent as a result of implementing some conservation measures. Take the unit cost of electricity to be \(\$ 0.11 / \mathrm{kWh}\).

A well-insulated \(4-m \times 4-m \times 5-m\) room initially at \(10^{\circ} \mathrm{C}\) is heated by the radiator of a steam heating system. The radiator has a volume of \(15 \mathrm{L}\) and is filled with superheated vapor at \(200 \mathrm{kPa}\) and \(200^{\circ} \mathrm{C}\). At this moment both the inlet and the exit valves to the radiator are closed. A 120 -W fan is used to distribute the air in the room. The pressure of the steam is observed to drop to \(100 \mathrm{kPa}\) after \(30 \mathrm{min}\) as a result of heat transfer to the room. Assuming constant specific heats for air at room temperature, determine ( \(a\) ) the average temperature of air in 30 min, \((b)\) the entropy change of the steam, \((c)\) the entropy change of the air in the room, and \((d)\) the entropy generated during this process, in \(\mathrm{kJ} / \mathrm{K}\). Assume the air pressure in the room remains constant at \(100 \mathrm{kPa}\) at all times.

Air is compressed steadily by a compressor from \(100 \mathrm{kPa}\) and \(20^{\circ} \mathrm{C}\) to \(1200 \mathrm{kPa}\) and \(300^{\circ} \mathrm{C}\) at a rate of \(0.4 \mathrm{kg} / \mathrm{s} .\) The compressor is intentionally cooled by utilizing fins on the surface of the compressor and heat is lost from the compressor at a rate of \(15 \mathrm{kW}\) to the surroundings at \(20^{\circ} \mathrm{C}\) Using constant specific heats at room temperature, determine \((a)\) the power input to the compressor, \((b)\) the isothermal efficiency, and ( \(c\) ) the entropy generation during this process.

\(3-\mathrm{kg}\) of helium gas at \(100 \mathrm{kPa}\) and \(27^{\circ} \mathrm{C}\) are adiabati cally compressed to 900 kPa. If the isentropic compression efficiency is 80 percent, determine the required work input and the final temperature of helium.

A piston-cylinder device initially contains \(15 \mathrm{ft}^{3}\) of helium gas at 25 psia and \(70^{\circ} \mathrm{F}\). Helium is now compressed in a polytropic process \(\left(P V^{n}=\text { constant }\right)\) to 70 psia and \(300^{\circ} \mathrm{F}\). Determine \((a)\) the entropy change of helium, \((b)\) the entropy change of the surroundings, and (c) whether this process is reversible, irreversible, or impossible. Assume the surroundings are at \(70^{\circ} \mathrm{F}\).

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