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Answer the following true or false. If false, explain why. A process that violates the second law of thermodynamics violates the first law of thermodynamics. (b) When a net amount of work is done on a closed system undergoing an internally reversible process, a net heat transfer of energy from the system also occurs. (c) One corollary of the second law of thermodynamics states that the change in entropy of a closed system must be greater than zero or equal to zero. (d) A closed system can experience an increase in entropy only when irreversibilities are present within the system during the process. (e) Entropy is produced in every internally reversible process of a closed system. (f) In an adiabatic and internally reversible process of a closed system, the entropy remains constant. (g) The energy of an isolated system must remain constant, but the entropy can only decrease.

Short Answer

Expert verified
a) False. b) False. c) True. d) False. e) False. f) True. g) False.

Step by step solution

01

- Analyze statement (a)

The second law of thermodynamics states that entropy of an isolated system always increases over time. The first law of thermodynamics states that energy cannot be created or destroyed. A process that violates the second law does not necessarily violate the first law. Therefore, the statement is false.
02

- Analyze statement (b)

For a closed system undergoing an internally reversible process, net work done on the system implies a change in energy, which could result in heat transfer. However, a net heat transfer out of the system is not a requirement, making the statement false.
03

- Analyze statement (c)

One corollary of the second law of thermodynamics does indeed state that the change in entropy of a closed system must be greater than or equal to zero. Hence, this statement is true.
04

- Analyze statement (d)

Entropies in closed systems can increase due to heat transferred into the system even in the absence of irreversibilities. Thus, this statement is false.
05

- Analyze statement (e)

In internally reversible processes, entropy is conserved and not produced. Therefore, the statement is false.
06

- Analyze statement (f)

During an adiabatic, internally reversible process, no heat is transferred, and entropy remains constant. Thus, this statement is true.
07

- Analyze statement (g)

The energy of an isolated system must remain constant, but the entropy can only increase or remain constant as per the second law. Therefore, the statement is false.

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Key Concepts

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

Second Law of Thermodynamics
The second law of thermodynamics is a fundamental principle describing how energy transitions occur in isolated systems. It states that in any natural thermodynamic process, the total entropy of an isolated system will either increase or remain constant over time—it never decreases.
Entropy, which is a measure of the disorder or randomness in a system, dictates that energy transformations have a preferred direction. This law explains why certain processes, such as heat spontaneously flowing from a hot object to a cold one, occur naturally.
Some points to remember about the second law of thermodynamics:
  • This law is crucial for understanding processes like heat engines and refrigerators.
  • While energy remains constant due to the first law, entropy ensures that energy transforms in a specific direction.
  • It indicates that perpetual motion machines of the second kind are impossible due to an inevitable increase in entropy.
In essence, the second law describes a tendency towards equilibrium and the natural progression towards increased entropy.
First Law of Thermodynamics
The first law of thermodynamics is synonymous with the principle of conservation of energy. It states that energy cannot be created or destroyed, only transformed from one form to another. The mathematical representation of this law is: \[ \Delta U = Q - W \] where:
  • \( \Delta U \): Change in internal energy of the system
  • \( Q \): Heat added to the system
  • \( W \): Work done by the system
This principle is important for many applications, such as calculating the energy balance in engines, refrigerators, and various other systems.
Some key aspects of the first law of thermodynamics include:
  • Energy can change forms, such as from potential energy to kinetic energy or thermal energy.
  • In closed systems, where no mass enters or leaves, the total energy remains constant.
  • This law forms the foundation for all energy analysis in thermodynamics.
Essentially, the first law underscores that the combined energy within an isolated system remains constant, thereby setting a groundwork for analyzing energy transformations and exchanges.
Entropy Change
Entropy is a central concept in thermodynamics, representing the degree of disorder or randomness in a system. The change in entropy gives insight into the direction and feasibility of thermodynamic processes. The second law of thermodynamics comes into play here, highlighting that for any spontaneous process, the total entropy of a system and its surroundings always increases.
Entropy changes can be understood as follows:
  • In an irreversible process, the system's entropy increases because of internal irreversibilities like friction or unrestrained expansion.
  • During a reversible process, entropy change can be calculated using the formula: \[ \Delta S = \int \frac{dQ_{rev}}{T} \] where \( \Delta S \) is the change in entropy, \( dQ_{rev} \) represents the infinitesimal heat added reversibly, and \( T \) is the temperature.
  • Entropy can remain constant in an adiabatic reversible process, as no heat transfer occurs (adiabatic) and no irreversibilities are present.
Clarifying these aspects, entropy change helps in understanding the efficiency and limitations of various thermodynamic cycles, processes, and systems. It's a key factor in determining whether a process can occur naturally and what the potential impact on energy distribution will be.

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Most popular questions from this chapter

Employing the ideal gas model, determine the change in specific entropy between the indicated states, in \(\mathrm{kJ} / \mathrm{kg} \cdot \mathrm{K}\). Solve three ways: Use the appropriate ideal gas table, \(I T\), and a constant specific heat value from Table A-20. (a) air, \(p_{1}=100 \mathrm{kPa}, T_{1}=20^{\circ} \mathrm{C}, p_{2}=100 \mathrm{kPa}, T_{2}=\) \(100^{\circ} \mathrm{C} .\) (b) air, \(p_{1}=1\) bar, \(T_{1}=27^{\circ} \mathrm{C}, p_{2}=3\) bar, \(T_{2}=377^{\circ} \mathrm{C}\). (c) carbon dioxide, \(p_{1}=150 \mathrm{kPa}, T_{1}=30^{\circ} \mathrm{C}, p_{2}=300 \mathrm{kPa}\), \(T_{2}=300^{\circ} \mathrm{C}\) (d) carbon monoxide, \(T_{1}=300 \mathrm{~K}, v_{1}=1.1 \mathrm{~m}^{3} / \mathrm{kg}, T_{2}=500 \mathrm{~K}\), \(v_{2}=0.75 \mathrm{~m}^{3} / \mathrm{kg}\) (e) nitrogen, \(p_{1}=2 \mathrm{MPa}, T_{1}=800 \mathrm{~K}, p_{2}=1 \mathrm{MPa}\), \(T_{2}=300 \mathrm{~K}\)

A well-insulated rigid tank of volume \(10 \mathrm{~m}^{3}\) is connected by a valve to a large-diameter supply line carrying air at \(227^{\circ} \mathrm{C}\) and 10 bar. The tank is initially evacuated. Air is allowed to flow into the tank until the tank pressure is \(p\). Using the ideal gas model with constant specific heat ratio \(k\), plot tank temperature, in \(\mathrm{K}\), the mass of air in the tank, in \(\mathrm{kg}\), and the amount of entropy produced, in \(\mathrm{kJ} / \mathrm{K}\), versus \(p\) in bar.

Carbon dioxide \(\left(\mathrm{CO}_{2}\right)\) enters a nozzle operating at steady state at 28 bar, \(267^{\circ} \mathrm{C}\), and \(50 \mathrm{~m} / \mathrm{s}\). At the nozzle exit, the conditions are \(1.2\) bar, \(67^{\circ} \mathrm{C}, 580 \mathrm{~m} / \mathrm{s}\), respectively. (a) For a control volume enclosing the nozzle only, determine the heat transfer, in \(\mathrm{kJ}\), and the change in specific entropy, in \(\mathrm{kJ} / \mathrm{K}\), each per \(\mathrm{kg}\) of carbon dioxide flowing through the nozzle. What additional information would be required to evaluate the rate of entropy production? (b) Evaluate the rate of entropy production, in \(\mathrm{kJ} / \mathrm{K}\) per \(\mathrm{kg}\) of carbon dioxide flowing, for an enlarged control volume enclosing the nozzle and a portion of its immediate surroundings so that the heat transfer occurs at the ambient temperature, \(25^{\circ} \mathrm{C}\).

Water is to be pumped from a lake to a reservoir located on a bluff \(290 \mathrm{ft}\) above. According to the specifications, the piping is Schedule 40 steel pipe having a nominal diameter of 1 inch and the volumetric flow rate is \(10 \mathrm{gal} / \mathrm{min}\). The total length of pipe is \(580 \mathrm{ft}\). A centrifugal pump is specified. Estimate the electrical power required by the pump, in \(\mathrm{kW}\). Is a centrifugal pump a good choice for this application? What precautions should be taken to avoid cavitation?

Methane gas \(\left(\mathrm{CH}_{4}\right)\) at \(280 \mathrm{~K}, 1\) bar enters a compressor operating at steady state and exits at \(380 \mathrm{~K}, 3.5\) bar. Ignoring heat transfer with the surroundings and employing the ideal gas model with \(\bar{c}_{p}(T)\) from Table A-21, determine the rate of entropy production within the compressor, in \(\mathrm{kJ} / \mathrm{kg} \cdot \mathrm{K}\).

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