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Closed Brayton power systems, receiving their energy input from radioisotopes, nuclear reactors, or solar collectors, have been suggested for meeting space vehicle power requirements. What are the advantages and disadvantages of closed Brayton cycles for spaceflight applications? What missionspecific design criteria might determine the selection of the system and the energy source?

Short Answer

Expert verified
Advantages: high efficiency, vacuum operation, long life. Disadvantages: complexity, mechanical failure, need for heat sink. Criteria: duration, energy needs, thermal management.

Step by step solution

01

Identify Advantages

List and explain the advantages of closed Brayton cycles for spaceflight applications. Examples include high efficiency, ability to operate in a vacuum, and long operational life.
02

Identify Disadvantages

List and explain the disadvantages of closed Brayton cycles for spaceflight applications. Examples include complexity, potential for mechanical failure, and the need for a heat sink.
03

Determine Mission-Specific Criteria

Identify design criteria that might affect the choice of a closed Brayton cycle system and the energy source. Such criteria include mission duration, energy requirements, thermal management, and the specific environment of the space mission.
04

Evaluate Energy Sources

Discuss the merits and limitations of different energy sources, such as radioisotopes, nuclear reactors, and solar collectors, when used in conjunction with a closed Brayton cycle in space.
05

Summarize Findings

Summarize the advantages and disadvantages of closed Brayton cycles and discuss how the mission-specific criteria and the selection of an energy source can impact the decision-making process for spaceflight applications.

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Key Concepts

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

space vehicle power requirements
Space missions often require robust and reliable power systems. The needs vary depending on mission objectives, durations, and environments encountered in space. For instance, power requirements for a satellite are different from those for manned missions to Mars.
  • Continuous Power Supply: Space vehicles need a reliable power source to support critical operations, like instrument functionality, communications, and life support systems.

  • High Efficiency: High efficiency is crucial as it reduces fuel and resource consumption, which is vital since resupply in space is not feasible.

  • Portability and Compactness: Power systems must be lightweight and compact to fit the space vehicle's limited size constraints.

The selection of power systems affects mission success significantly. Engineers must balance efficiency, durability, and size while adhering to mission-specific requirements.
nuclear reactors
Nuclear reactors have been considered a potential energy source for space vehicles.

  • High Energy Output: Nuclear reactors can generate substantial energy, making them suitable for high-demand missions such as deep-space exploration.

  • Long Operational Life: They have the ability to provide continuous power over extended periods without refueling, ideal for long-duration missions.

  • Weight and Safety Concerns: Despite their benefits, nuclear reactors are heavy and come with significant safety concerns. Radiation shielding is necessary to protect spacecraft and crew, which adds to the overall weight.

The pros and cons of nuclear reactors must be carefully weighed to suit specific mission needs. They are ideal for long voyages but come with stringent safety and design requirements.
solar collectors
Solar collectors are another energy source for space vehicles, particularly effective for missions within the inner solar system.

  • Renewable Energy: Solar collectors harness energy from the sun, providing a sustainable power source as long as the spacecraft remains within sunlight reach.

  • Lightweight: Solar panels are relatively lightweight and can be deployed large enough to capture adequate sunlight, advantageous for reduced mass and cost.

  • Dependence on Sunlight: These collectors are less effective in deep space or shadowed regions of celestial bodies. Their effectiveness decreases as the distance from the sun increases.

While solar collectors offer advantages for near-Earth missions, their limitations must be considered when planning missions further from the sun.
radioisotopes
Radioisotope power systems (RPS) provide another viable energy source for space missions.

  • Consistent Power Output: Radioisotopes generate electricity through decay, providing a steady power supply irrespective of the space environment.

  • Compact and Reliable: These systems are compact, reliable, and can function in harsh conditions, including deep space and shaded regions.

  • Limited Power Levels: The power output is generally lower than that of nuclear reactors, making radioisotopes suitable for missions with lower energy demands.

Radioisotope power systems are widely used in space exploration where other energy sources may falter. They are ideal for missions requiring long-lasting and low-maintenance power.

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Most popular questions from this chapter

Air enters the compressor of a gas turbine at \(100 \mathrm{kPa}\), \(300 \mathrm{~K}\). The air is compressed in two stages to \(900 \mathrm{kPa}\), with intercooling to \(300 \mathrm{~K}\) between the stages at a pressure of \(300 \mathrm{kPa}\). The turbine inlet temperature is \(1480 \mathrm{~K}\) and the expansion occurs in two stages, with reheat to \(1420 \mathrm{~K}\) between the stages at a pressure of \(300 \mathrm{kPa}\). The compressor and turbine stage efficiencies are 84 and \(82 \%\), respectively. The net power developed is \(1.8 \mathrm{MW}\). Determine (a) the volumetric flow rate, in \(\mathrm{m}^{3} / \mathrm{s}\), at the inlet of each compressor stage. (b) the thermal efficiency of the cycle. (c) the back work ratio.

An air-standard Otto cycle has a compression ratio of \(8.5\). At the beginning of compression, \(p_{1}=100 \mathrm{kPa}\) and \(T_{1}=300 \mathrm{~K}\). The heat addition per unit mass of air is \(1400 \mathrm{~kJ} / \mathrm{kg}\). Determine (a) the net work, in \(\mathrm{kJ}\) per \(\mathrm{kg}\) of air. (b) the thermal efficiency of the cycle. (c) the mean effective pressure, in \(\mathrm{kPa}\). (d) the maximum temperature in the cycle, in \(\mathrm{K}\). (e) To investigate the effects of varying compression ratio, plot each of the quantities calculated in parts (a) through (d) for compression ratios ranging from 1 to 12 .

The ideal Brayton and Rankine cycles are composed of the same four processes, yet look different when represented on a \(T-s\) diagram. Explain.

If the inlet state and the exit pressure are specified for a twostage turbine with reheat between the stages and operating at steady state, show that the maximum total work output is obtained when the pressure ratio is the same across each stage. Use a cold air-standard analysis assuming that each compression process is isentropic, there is no pressure drop through the reheater, and the temperature at the inlet to each turbine stage is the same. Kinetic and potential energy effects can be ignored.

Using Interactive Thermodynamics: \(I T\), generate tables of the same normal shock functions as in Table \(9.2\) for specific heat ratios of \(1.2,1.3,1.4\), and \(1.67\) and Mach numbers ranging from 1 to 5

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