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Taken together, a certain closed system and its surroundings make up an isolated system. Answer the following true or false. If false, explain why. (a) No process is allowed in which the entropies of both the system and the surroundings increase. (b) During a process, the entropy of the system might decrease, while the entropy of the surroundings increases, and conversely. (c) No process is allowed in which the entropies of both the system and the surroundings remain unchanged. (d) A process can occur in which the entropies of both the system and the surroundings decrease.

Short Answer

Expert verified
a: False, b: True, c: False, d: False

Step by step solution

01

Understanding the problem

The problem involves determining the truth of statements about entropy changes in an isolated system. An isolated system means no exchange of energy or matter with the surroundings.
02

Analyze statement (a)

Statement (a) says no process is allowed where both the system's and the surroundings' entropies increase. In an isolated system, total entropy can stay the same or increase, but cannot decrease. Since both increasing does not violate this, the statement is false.
03

Analyze statement (b)

Statement (b) suggests that entropy of the system might decrease while that of the surroundings increases, and conversely. This is true because as long as the total entropy increases or remains the same, individual parts can change in opposite directions.
04

Analyze statement (c)

Statement (c) suggests no process is allowed where both system and surroundings' entropies remain unchanged. This is false because reversible processes exist where the total entropy does not change.
05

Analyze statement (d)

Statement (d) claims a process can occur where both system and surroundings' entropies decrease. This is false because in an isolated system, the total entropy cannot decrease.

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Key Concepts

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

Understanding Entropy
Entropy is a fundamental concept in thermodynamics. It's a measure of disorder or randomness in a system. The second law of thermodynamics states that in an isolated system, the total entropy can never decrease over time; it either increases or remains constant in a reversible process. This means that energy will always spread out or become more disordered unless work is done to keep it organized.

For example, if you leave an ice cube in a warm room, it will melt. The molecules in the ice, initially structured, will move around more freely in the water, increasing the system's entropy.

When thinking about entropy changes in processes, remember:
  • The total entropy of an isolated system never decreases.
  • In real-world processes, the entropy usually increases.
A practical tip is to visualize entropy as a measure of energy dispersal. The more spread out the energy, the higher the entropy.
Isolated Systems
An isolated system is a special type of closed system. It does not exchange energy or matter with its surroundings. Because of this, it is often used to study the laws of thermodynamics in a simplified context. The entire universe is considered an isolated system because there is nothing outside of it to exchange energy or matter with.

In isolated systems, a few important points hold:
  • No matter (mass) or energy can enter or leave the system.
  • The total energy of the system remains constant.
  • The total entropy of the system will either increase or stay the same, but never decrease.
These points help us understand why processes in isolated systems behave in predictable ways.

For instance, consider a perfectly insulated container with a hot and a cold object inside. Over time, heat from the hot object will transfer to the cold one until both reach the same temperature. The system has moved to a more probable state of uniform temperature, increasing the total entropy.
Basic Thermodynamics Principles
Thermodynamics is the study of energy, heat, work, and how they interrelate. It is governed by four basic laws which are crucial for understanding physical processes:

1. The Zeroth Law of Thermodynamics states that if two systems are in thermal equilibrium with a third one, they are in thermal equilibrium with each other.

2. The First Law of Thermodynamics, also known as the Law of Energy Conservation, states that energy cannot be created or destroyed, only transferred or converted from one form to another. The equation to describe this is: \[ \text{ΔU} = Q - W \] where \text{ΔU} is the change in internal energy, \text{Q} is the heat added to the system, and \text{W} is the work done by the system.

3. The Second Law of Thermodynamics states that the entropy of an isolated system always increases over time. It implies that natural processes have a preferred direction of progression, often toward more disorder.

4. The Third Law of Thermodynamics states that the entropy of a perfect crystal at absolute zero is exactly zero.

These laws help explain how energy moves and changes form, making them crucial for understanding isolated systems and entropy changes. For practical use, remember that increasing entropy is like energy becoming more scattered and hard to use without inputting extra work to organize it again.

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Most popular questions from this chapter

Steam enters a turbine operating at steady state at a pressure of \(3 \mathrm{MPa}\), a temperature of \(400^{\circ} \mathrm{C}\), and a velocity of \(160 \mathrm{~m} / \mathrm{s}\). Saturated vapor exits at \(100^{\circ} \mathrm{C}\), with a velocity of \(100 \mathrm{~m} / \mathrm{s}\). Heat transfer from the turbine to its surroundings takes place at the rate of \(30 \mathrm{~kJ}\) per kg of steam at a location where the average surface temperature is \(350 \mathrm{~K}\). (a) For a control volume including only the turbine and its contents, determine the work developed, in \(\mathrm{kJ}\), and the rate at which entropy is produced, in \(\mathrm{kJ} / \mathrm{K}\), each per \(\mathrm{kg}\) of steam flowing. (b) The steam turbine of part (a) is located in a factory where the ambient temperature is \(27^{\circ} \mathrm{C}\). Determine the rate of entropy production, in \(\mathrm{kJ} / \mathrm{K}\) per \(\mathrm{kg}\) of steam flowing, for an enlarged control volume that includes the turbine and enough of its immediate surroundings so that heat transfer takes place from the control volume at the ambient temperature. Explain why the entropy production value of part (b) differs from that calculated in part (a).

A system consists of \(2 \mathrm{~m}^{3}\) of hydrogen gas \(\left(\mathrm{H}_{2}\right)\), initially at \(35^{\circ} \mathrm{C}, 215 \mathrm{kPa}\), contained in a closed rigid tank. Energy is transferred to the system from a reservoir at \(300^{\circ} \mathrm{C}\) until the temperature of the hydrogen is \(160^{\circ} \mathrm{C}\). The temperature at the system boundary where heat transfer occurs is \(300^{\circ} \mathrm{C}\). Modeling the hydrogen as an ideal gas, determine the heat transfer, in \(\mathrm{kJ}\), the change in entropy, in \(\mathrm{kJ} / \mathrm{K}\), and the amount of entropy produced, in \(\mathrm{kJ} / \mathrm{K}\). For the reservoir, determine the change in entropy, in \(\mathrm{kJ} / \mathrm{K}\). Why do these two entropy changes differ?

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, \(25^{\circ} \mathrm{C}\).

Steam at \(0.7 \mathrm{MPa}, 355^{\circ} \mathrm{C}\) enters an open feedwater heater operating at steady state. A separate stream of liquid water enters at \(0.7 \mathrm{MPa}, 35^{\circ} \mathrm{C}\). A single mixed stream exits as saturated liquid at pressure \(p\). Heat transfer with the surroundings and kinetic and potential energy effects can be ignored. (a) If \(p=0.7 \mathrm{MPa}\), determine the ratio of the mass flow rates of the incoming streams and the rate at which entropy is produced within the feedwater heater, in \(\mathrm{kJ} / \mathrm{K}\) per \(\mathrm{kg}\) of liquid exiting. (b) Plot the quantities of part (a), each versus pressure \(p\) ranging from \(0.6\) to \(0.7 \mathrm{MPa}\).

Air enters a compressor operating at steady state with a volumetric flow rate of \(8 \mathrm{~m}^{3} / \mathrm{min}\) at \(23^{\circ} \mathrm{C}, 0.12 \mathrm{MPa}\). The air is compressed isothermally without internal irreversibilities, exiting at \(1.5 \mathrm{MPa}\). Kinetic and potential energy effects can be ignored. Evaluate the work required and the heat transfer, each in \(\mathrm{kW}\).

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