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Answer the following true or false. If false, explain why. (a) The change of entropy of a closed system is the same for every process between two specified states. (b) The entropy of a fixed amount of an ideal gas increases in every isothermal compression. (c) The specific internal energy and enthalpy of an ideal gas are each functions of temperature alone but its specific entropy depends on two independent intensive properties. (d) One of the \(T d s\) equations has the form \(T d s=d u-p d v\). (e) The entropy of a fixed amount of an incompressible substance increases in every process in which temperature decreases.

Short Answer

Expert verified
(a) True. (b) False - entropy decreases in isothermal compression. (c) True. (d) True. (e) False - entropy decreases with temperature decrease.

Step by step solution

01

- Analyze statement (a)

The change of entropy for a closed system between two specified states is a property change, which depends only on the initial and final states and not on the process path. This statement is true.
02

- Analyze statement (b)

For an isothermal compression of an ideal gas, the volume decreases while temperature remains constant. According to the entropy change formula for an ideal gas, \[\frac{\text{d}S}{\text{d}V} = \frac{C_v}{T} - \frac{R}{V}\], since the volume decreases, the entropy change \(\text{d}S\) is negative. Thus, the entropy of an ideal gas decreases in isothermal compression. This statement is false.
03

- Analyze statement (c)

Specific internal energy \(u\) and enthalpy \(h\) of an ideal gas are only functions of temperature according to these relations: \(u = u(T)\) and \(h = h(T)\). However, entropy \(s\) is a function of both temperature and volume or temperature and pressure, i.e., \(s = s(T, V)\) or \(s = s(T, P)\). This statement is true.
04

- Analyze statement (d)

The T d s equation is derived from first and second laws of thermodynamics. One form of the \(T d s\) equation for a reversible process is \(T d s = d u + p d v\). This matches the form given in the statement, so this statement is true.
05

- Analyze statement (e)

For incompressible substances, changes in entropy are largely dependent on temperature because they do not change volume under pressure. When temperature decreases for an incompressible substance, the randomness or disorder typically decreases, hence entropy decreases. This statement is false.

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Key Concepts

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

entropy change
Entropy change in thermodynamics is a crucial aspect of understanding how systems evolve. Entropy can be thought of as a measure of disorder or randomness within a system.
For a closed system, the change in entropy depends only on the initial and final states, meaning it is a state function. This implies it does not depend on the path taken to reach from one state to another.
For example, whether you compress a gas abruptly or slowly to the same final state, the entropy change will remain identical if the initial and final states are the same.
This fundamental concept is crucial for solving many problems in thermodynamics and provides insight into the principles governing energy transfer and efficiency.
ideal gas properties
Ideal gases follow specific laws and properties which simplify their analysis. Key among these is the ideal gas law stated as \(\text{PV = nRT}\), where *P* is pressure, *V* is volume, *n* is the number of moles, *R* is the universal gas constant, and *T* is temperature.

The internal energy \(u\) and enthalpy \(h\) of an ideal gas are solely functions of temperature: \(u = u(T)\) and \h = h(T). \ The state functions depend on temperature independent of pressure or volume.
Entropy \s, however, depends on both temperature and another independent variable such as volume or pressure: \(s = s(T, V)\) or \(s = s(T, P)\).
For an isothermal process involving an ideal gas, when compressed, the volume of the gas decreases and since the temperature remains the same, the entropy decreases.
TdS equations
The T dS equations form the foundation for understanding entropy changes in thermodynamics. These equations combine the first and second laws of thermodynamics to link entropy change with other properties. One commonly used form is \(T dS = du + p dV\), applicable to reversible processes.

Here, *T* represents temperature, *dS* is the change in entropy, *du* is the change in internal energy, *p* is pressure, and *dV* is the change in volume.
These relationships help in computing the entropy change for varying thermodynamic processes. By integrating these equations, we can derive expressions for entropy changes based on measurable properties like temperature, pressure, and volume.
incompressible substances
Incompressible substances, like liquids and solids, retain constant volume regardless of pressure changes. This characteristic makes their analysis somewhat simpler compared to gases.
For incompressible substances, entropy change is predominantly influenced by temperature changes.

As temperature decreases, the molecular motion within the substance slows down, reducing entropy. Conversely, as temperature increases, molecular activity rises, and entropy increases.
Hence, understanding temperature's effect on entropy is vital for analyzing processes involving incompressible substances.
It is important to note that changes in entropy due to pressure for incompressible substances are negligible, making them unique in thermodynamic studies.

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Most popular questions from this chapter

A system undergoes a thermodynamic power cycle while receiving energy by heat transfer from an incompressible body of mass \(m\) and specific heat \(c\) initially at temperature \(T_{\mathrm{H}}\). The system undergoing the cycle discharges energy by heat transfer to another incompressible body of mass \(m\) and specific heat \(c\) initially at a lower temperature \(T_{\mathrm{C}}\). Work is developed by the cycle until the temperature of each of the two bodies is the same, \(T^{\prime}\). (a) Develop an expression for the minimum theoretical final temperature, \(T^{\prime}\), in terms of \(m, c, T_{\mathrm{H}}\), and \(T_{\mathrm{C}}\), as required. (b) Develop an expression for the maximum theoretical amount of work that can be developed, \(W_{\max }\), in terms of \(m, c, T_{\mathrm{H}}\), and \(T_{\mathrm{C}}\), as required. (c) What is the minimum theoretical work input that would be required by a refrigeration cycle to restore the two bodies from temperature \(T^{\prime}\) to their respective initial temperatures, \(T_{\mathrm{H}}\) and \(T_{\mathrm{C}} ?\)

A system executes a power cycle while receiving \(1000 \mathrm{~kJ}\) by heat transfer at a temperature of \(500 \mathrm{~K}\) and discharging energy by heat transfer at a temperature of \(300 \mathrm{~K}\). There are no other heat transfers. Applying Eq. 6.2, determine \(\sigma_{\text {cycle }}\) if the thermal efficiency is (a) \(60 \%\), (b) \(40 \%\), (c) \(20 \%\). Identify the cases (if any) that are internally reversible or impossible.

An electrically-driven pump operating at steady state draws water from a pond at a pressure of 1 bar and a rate of \(40 \mathrm{~kg} / \mathrm{s}\) and delivers the water at a pressure of 4 bar. There is no significant heat transfer with the surroundings, and changes in kinetic and potential energy can be neglected. The isentropic pump efficiency is \(80 \%\). Evaluating electricity at 8 cents per \(\mathrm{kW} \cdot \mathrm{h}\), estimate the hourly cost of running the pump.

Noting that contemporary economic theorists often draw on principles from mechanics such as conservation of energy to explain the workings of economies, \(\mathrm{N}\). Georgescu-Roegen and like-minded economists have called for the use of principles from thermodynamics in economics. According to this view, entropy and the second law of thermodynamics are relevant for assessing not only the exploitation of natural resources for industrial and agricultural production but also the impact on the natural environment of wastes from such production. Write a paper in which you argue for, or against, the proposition that thermodynamics is relevant to the field of economics.

An electric motor operating at steady state draws a current of 10 amp with a voltage of \(220 \mathrm{~V}\). The output shaft rotates at 1000 RPM with a torque of \(16 \mathrm{~N} \cdot \mathrm{m}\) applied to an external load. The rate of heat transfer from the motor to its surroundings is related to the surface temperature \(T_{\mathrm{b}}\) and the ambient temperature \(T_{0}\) by \(\mathrm{hA}\left(T_{\mathrm{b}}-T_{0}\right)\), where \(\mathrm{h}=100 \mathrm{~W} / \mathrm{m}^{2}\). \(\mathrm{K}, \mathrm{A}=0.195 \mathrm{~m}^{2}\), and \(T_{0}=293 \mathrm{~K}\). Energy transfers are considered positive in the directions indicated by the arrows on Fig. P6.51. (a) Determine the temperature \(T_{\mathrm{b}}\), in \(\mathrm{K}\). (b) For the motor as the system, determine the rate of entropy production, in \(\mathrm{kW} / \mathrm{K}\). (c) If the system boundary is located to take in enough of the nearby surroundings for heat transfer to take place at temperature \(T_{0}\), determine the rate of entropy production, in \(\mathrm{kW} / \mathrm{K}\), for the enlarged system.

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