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What are some of the principal irreversibilities present during operation of (a) an automobile engine, (b) a household refrigerator, (c) a gas-fired water heater, (d) an electric water heater?

Short Answer

Expert verified
The principal irreversibilities are: (a) combustion, friction, and heat loss; (b) heat transfer, compressor friction, throttling; (c) heat loss, incomplete combustion, friction; (d) heat transfer, electrical resistance, heat loss.

Step by step solution

01

- Identify irreversibilities in an automobile engine

Consider the main sources of inefficiency in an automobile engine. The principal irreversibilities include combustion irreversibility, friction between moving parts, and heat loss to the surroundings.
02

- Identify irreversibilities in a household refrigerator

For a household refrigerator, the main irreversibilities are heat transfer losses, friction in the compressor, and the irreversibility associated with throttling in the expansion valve.
03

- Identify irreversibilities in a gas-fired water heater

A gas-fired water heater experiences irreversibilities primarily due to heat losses to the surroundings, incomplete combustion of the fuel, and frictional losses in the flow of water and exhaust gases.
04

- Identify irreversibilities in an electric water heater

In an electric water heater, the principal irreversibilities include heat transfer losses to the surroundings, electrical resistance losses in the heating element, and heat losses from the water tank to the surroundings.

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Key Concepts

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

automobile engine irreversibilities
Automobile engines are complex systems filled with various inefficiencies. One of the primary irreversibilities in an automobile engine is **combustion irreversibility**. This occurs because combustion in the engine is never perfectly efficient. There are always some fuel molecules that do not completely combust, leading to energy losses.

Another significant source of energy loss is **friction** between moving parts such as the pistons and the crankshaft. This friction not only wastes energy but also generates unwanted heat.

Lastly, **heat loss to the surroundings** is a major irreversibility. No engine is entirely insulated. The heat produced during combustion often escapes into the environment instead of being used for work.

To minimize these irreversibilities, engineers focus on improving combustion efficiency, reducing friction through better lubrication, and insulating the engine better to prevent heat loss.
household refrigerator inefficiencies
Household refrigerators are designed to keep food cold, but they also suffer from several inefficiencies. The most significant is **heat transfer loss**. This mainly occurs due to poor insulation and frequent opening and closing of the refrigerator door, allowing warm air to enter.

Another source of inefficiency is **friction in the compressor**. The compressor is responsible for circulating the refrigerant but loses energy due to friction between its moving parts.

Finally, there is **irreversibility due to throttling in the expansion valve**. This process is not perfectly efficient and results in some energy being lost.

To reduce these inefficiencies, you can improve insulation around the refrigerator, ensure the door seals properly, and consider technology improvements in compressor design.
gas-fired water heater losses
Gas-fired water heaters are common in many homes but are prone to several inefficiencies. One of the main irreversibilities is **heat loss to the surroundings**. Despite the insulation, some heat always escapes from both the heater and the water tank.

**Incomplete combustion of the fuel** is another major inefficiency. Not all the fuel burns completely, which means some of the chemical energy is not converted to heat.

Additionally, there are **frictional losses in the flow of water and exhaust gases**. As water and exhaust gases move through pipes and vents, friction reduces the overall energy efficiency.

Improving these systems involves better insulation, more efficient combustion technologies, and minimizing friction losses through design modifications.
electric water heater inefficiencies
Electric water heaters, though highly effective, still experience inefficiencies. A primary irreversibility is **heat transfer losses to the surroundings**. Even with good insulation, heat will inevitably escape from the heater to the surrounding environment.

**Electrical resistance losses in the heating element** are another inefficiency. Electrical energy passes through the heating element, generating heat, but this process is not perfectly efficient.

Furthermore, **heat losses from the water tank to the surroundings** further reduce the system's overall efficiency. Despite insulation, some warmth will always escape.

To reduce these inefficiencies, enhancing the insulation of the water heater and using more efficient heating elements are often effective solutions.

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Most popular questions from this chapter

A heat pump operating at steady state is driven by a \(1-\mathrm{kW}\) electric motor and provides heating for a building whose interior is to be kept at \(20^{\circ} \mathrm{C}\). On a day when the outside temperature is \(0^{\circ} \mathrm{C}\) and energy is lost through the walls and roof at a rate of \(60,000 \mathrm{~kJ} / \mathrm{h}\), would the heat pump suffice?

At steady state, a power cycle having a thermal efficiency of \(38 \%\) generates \(100 \mathrm{MW}\) of electricity while discharging energy by heat transfer to cooling water at an average temperature of \(70^{\circ} \mathrm{F}\). The average temperature of the steam passing through the boiler is \(900^{\circ} \mathrm{F}\). Determine (a) the rate at which energy is discharged to the cooling water, in Btu/h. (b) the minimum theoretical rate at which energy could be discharged to the cooling water, in Btu/h. Compare with the actual rate and discuss.

For each \(\mathrm{kW}\) of power input to an ice maker at steady state, determine the maximum rate that ice can be produced, in \(\mathrm{kg} / \mathrm{h}\), from liquid water at \(0^{\circ} \mathrm{C}\). Assume that \(333 \mathrm{~kJ} / \mathrm{kg}\) of energy must be removed by heat transfer to freeze water at \(0^{\circ} \mathrm{C}\), and that the surroundings are at \(20^{\circ} \mathrm{C}\).

The preliminary design of a space station calls for a power cycle that at steady state receives energy by heat transfer at \(T_{\mathrm{H}}=600 \mathrm{~K}\) from a nuclear source and rejects energy to space by thermal radiation according to Eq. 2.33. For the radiative surface, the temperature is \(T_{\mathrm{C}}\), the emissivity is \(0.6\), and the surface receives no radiation from any source. The thermal efficiency of the power cycle is one- half that of a reversible power cycle operating between reservoirs at \(T_{\mathrm{H}}\) and \(T_{\mathrm{C}}\) - (a) For \(T_{\mathrm{C}}=400 \mathrm{~K}\), determine \(\dot{W}_{\text {cycle }} / \mathrm{A}\), the net power developed per unit of radiator surface area, in \(\mathrm{kW} / \mathrm{m}^{2}\), and the thermal efficiency. (b) Plot \(\dot{W}_{\text {cycle }} / \mathrm{A}\) and the thermal efficiency versus \(T_{\mathrm{C}}\), and determine the maximum value of \(\dot{W}_{\text {cycle }} / \mathrm{A}\). (c) Determine the range of temperatures \(T_{\mathrm{C}}\), in \(\mathrm{K}\), for which \(\dot{W}_{\text {cycle }} / \mathrm{A}\) is within 2 percent of the maximum value obtained in part (b). The Stefan-Boltzmann constant is \(5.67 \times 10^{-8} \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}^{4}\).

A heat pump maintains a dwelling at \(20^{\circ} \mathrm{C}\) when the outside temperature is \(0^{\circ} \mathrm{C}\). The heat transfer rate through the walls and roof is \(3000 \mathrm{~kJ} / \mathrm{h}\) per degree temperature difference between the inside and outside. Determine the minimum theoretical power required to drive the heat pump, in \(\mathrm{kW}\).

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