The Figure Shows a Reversible Cycle Through Which Energy Transformations Occur

The figure shows a reversible cycle through which energy transformations occur, providing a visual representation of the thermodynamic processes involved. This cycle consists of four distinct stages, each characterized by specific energy changes and transformations.

The first stage is an isothermal expansion, where the system expands while maintaining a constant temperature. During this stage, heat is absorbed by the system, resulting in an increase in volume and a decrease in pressure. The second stage is an adiabatic expansion, where the system expands without any heat exchange with the surroundings.

As the system expands, its internal energy decreases, causing a drop in both temperature and pressure.

Cycle Overview

This reversible cycle is designed to provide a comprehensive understanding of the energy transformations that occur within a thermodynamic system. It consists of four distinct stages, each characterized by specific energy exchanges and state changes.

The cycle begins with the system in a state of equilibrium. Stage 1 involves the addition of heat to the system, causing an increase in its internal energy and a change in state. In Stage 2, the system undergoes an isothermal expansion, where its volume increases while its temperature remains constant.

This expansion results in the conversion of internal energy into work.

Stage 3

In Stage 3, heat is removed from the system, leading to a decrease in its internal energy and a change in state. This heat removal is followed by an isothermal compression in Stage 4, where the system’s volume decreases while its temperature remains constant.

This compression converts work back into internal energy, completing the cycle and returning the system to its initial equilibrium state.

Thermodynamics of the Cycle: The Figure Shows A Reversible Cycle Through Which

The first law of thermodynamics states that energy cannot be created or destroyed, only transferred or transformed. In the context of the cycle, this means that the total energy of the system remains constant throughout the cycle.

During the cycle, there are changes in internal energy, heat, and work. Internal energy is the energy of the system due to its temperature and molecular motion. Heat is the transfer of thermal energy between objects or systems at different temperatures.

Work is the transfer of energy by a force acting through a distance.

Changes in Internal Energy, The figure shows a reversible cycle through which

Internal energy increases during the heating process (A to B) and decreases during the cooling process (C to D).

Changes in Heat

Heat is added to the system during the heating process (A to B) and removed from the system during the cooling process (C to D).

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Changes in Work

Work is done by the system during the expansion process (B to C) and on the system during the compression process (D to A).

Entropy

Entropy is a measure of the disorder of a system. In the context of the cycle, entropy increases during the heating process (A to B) and decreases during the cooling process (C to D).

Graphical Representation

The figure shows a reversible cycle through which

The cycle’s pressure-volume (P-V) diagram provides a graphical representation of the changes in pressure and volume as the system undergoes the various processes. It is a useful tool for visualizing the cycle and understanding the work done by the system.

The P-V diagram for the cycle is shown in the table below. The diagram shows the four processes that make up the cycle: isothermal expansion, adiabatic expansion, isobaric compression, and adiabatic compression.

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Key Features of the P-V Diagram

  • The isothermal expansion process is shown by the line from point A to point B. During this process, the temperature of the system remains constant, and the pressure decreases as the volume increases.
  • The adiabatic expansion process is shown by the line from point B to point C. During this process, no heat is transferred to or from the system, and the temperature decreases as the volume increases.
  • The isobaric compression process is shown by the line from point C to point D. During this process, the pressure remains constant, and the temperature increases as the volume decreases.
  • The adiabatic compression process is shown by the line from point D to point A. During this process, no heat is transferred to or from the system, and the temperature increases as the volume decreases.

Determining the Work Done by the Cycle

The work done by the cycle is equal to the area enclosed by the P-V diagram. In this case, the work done by the cycle is positive, which means that the system does work on the surroundings.

Applications of the Cycle

The reversible cycle, also known as the Carnot cycle, is a theoretical thermodynamic cycle that describes the most efficient way to convert heat into work. It is used as a benchmark for comparing the efficiency of real-world heat engines.In practice, the reversible cycle is used in a variety of applications, including:

  • Power plants:The reversible cycle is used in power plants to generate electricity from heat. The heat source can be from fossil fuels, nuclear reactions, or renewable energy sources such as solar or geothermal energy.
  • Refrigerators and air conditioners:The reversible cycle is used in refrigerators and air conditioners to remove heat from a cold reservoir and transfer it to a hot reservoir. This process cools the cold reservoir and heats the hot reservoir.
  • Heat pumps:The reversible cycle is used in heat pumps to transfer heat from a cold reservoir to a hot reservoir. This process heats the hot reservoir and cools the cold reservoir.

The reversible cycle has a number of advantages over other thermodynamic cycles. These advantages include:

  • High efficiency:The reversible cycle is the most efficient way to convert heat into work.
  • Reversibility:The reversible cycle can be reversed, which means that it can be used to either generate electricity or remove heat.
  • Simplicity:The reversible cycle is a simple cycle that is easy to understand and analyze.

However, the reversible cycle also has some limitations. These limitations include:

  • Idealization:The reversible cycle is an idealization that does not exist in the real world. Real-world heat engines are always less efficient than the reversible cycle.
  • Cost:The reversible cycle is more expensive to build and operate than other thermodynamic cycles.
  • Complexity:The reversible cycle is more complex than other thermodynamic cycles, which makes it more difficult to design and build.

Overall, the reversible cycle is a powerful tool for understanding the conversion of heat into work. It is used in a variety of applications, and it has a number of advantages over other thermodynamic cycles. However, the reversible cycle also has some limitations, which make it less practical for some applications.

Last Word

The figure shows a reversible cycle through which

In conclusion, the figure provides a comprehensive overview of a reversible cycle, highlighting the energy transformations that occur during each stage. The cycle’s graphical representation allows for a clear understanding of the thermodynamic processes involved, making it a valuable tool for analyzing and understanding energy conversion systems.

FAQ Compilation

What is the purpose of a reversible cycle?

A reversible cycle is a theoretical construct that represents an idealized thermodynamic cycle in which all processes are reversible, meaning they can be reversed without any loss of energy. It serves as a benchmark for comparing the efficiency of real-world cycles.

What are the key features of a P-V diagram?

A P-V diagram is a graphical representation of the pressure-volume relationship of a system undergoing a thermodynamic cycle. It consists of four distinct regions: isothermal, adiabatic, isobaric, and isochoric processes. These regions provide insights into the energy transformations occurring during each stage of the cycle.

What is the significance of entropy in a reversible cycle?

Entropy is a measure of the disorder or randomness of a system. In a reversible cycle, the total entropy change over the entire cycle is zero, indicating that the system returns to its initial state without any net change in entropy.

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