Choose the substance which has higher possible entropy (per mole) at a given temperature. (a) solid carbon dioxide (b) nitrogen gas at 1 atm (c) nitrogen gas at \(0.01\) atm (d) nitrogen gas at \(0.00001\) atm

Short Answer

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Nitrogen gas at 0.00001 atm (d) has the highest possible entropy per mole at a given temperature.

Step by step solution

01

Understanding Entropy

Entropy is a measure of the degree of disorder or randomness in a system. Generally, for the same substance, the entropy increases with the phase change from solid to liquid to gas because the particles have more freedom of movement and thus more possible microstates in the gaseous state. Also, at higher temperatures or lower pressures, gases will have more entropy because the particles are further apart and have more possible positions and velocities.
02

Comparing States of Matter

Solid carbon dioxide (a), also known as dry ice, has its particles in a fixed lattice with very little movement or freedom, which makes its entropy lower than that of a gas. Nitrogen gas (b, c, and d), being in the gaseous state, has particles that are free to move around and spread out, giving it a higher entropy than the solid carbon dioxide.
03

Comparing Gas Samples

Between samples of nitrogen gas at different pressures, the sample with the lowest pressure has the highest entropy. This is because lower pressure allows gas particles to have more volume to occupy and more possible microstates. Therefore, nitrogen gas at 0.00001 atm (d) has a higher possible entropy than the same gas at 0.01 atm (c) and at 1 atm (b).

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Key Concepts

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

Thermodynamics
Thermodynamics is a branch of physics that deals with the relationships between heat, work, temperature, and energy in a system. This field is crucial for understanding how energy is converted in chemical reactions and physical changes. One of the central concepts in thermodynamics is entropy, which is used to measure the disorder or randomness in a system. The second law of thermodynamics states that in any spontaneous process, the total entropy of the system and its surroundings always increases, leading to the notion that systems naturally progress toward a state of maximum entropy. This explains why heat flows from hot to cold and why gases expand to fill their containers.
States of Matter
The three traditional states of matter are solid, liquid, and gas. Each state is distinguished by particle arrangement, energy, and movement. In solids, atoms or molecules are tightly packed in a structured pattern, with little movement besides vibration. Solids have a definite shape and volume. Liquids have a definite volume but take the shape of their container, as their particles have more freedom to move than in solids. Gases have neither a fixed volume nor shape and will expand to fill their container. Particles in a gas move rapidly and are widely spaced apart, which often results in higher entropy compared to solids and liquids at the same temperature.
Entropy and Pressure
Entropy in a system is greatly affected by pressure. In a gaseous system, reducing pressure allows gas molecules to spread out over a larger volume, thereby increasing the number of possible configurations or microstates the system can occupy. This increases the entropy of the system, reflecting a higher degree of randomness. Conversely, when pressure is increased, the gas molecules are compressed into a smaller volume, reducing the number of possible microstates and, consequently, decreasing entropy. Thus, pressure and entropy are inversely related in gases; as one decreases, the other increases, and vice versa.
Microstates
A microstate is a specific configuration that a system can assume based on the arrangement and states of its individual particles. In simple terms, each microstate represents a unique way in which the system's particles can be distributed in terms of position and energy. In the realm of thermodynamics, entropy can be thought of as the logarithm of the number of microstates (W) available to a system at a given energy. The more microstates available, the higher the entropy, indicating a larger amount of disorder. In the context of our gaseous nitrogen example, a sample at a lower pressure has a greater volume to spread out, leading to many more microstates and therefore a higher entropy.

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Most popular questions from this chapter

A definite mass of a monoatomic ideal gas at 1 bar and \(27^{\circ} \mathrm{C}\) expands against \(\begin{array}{llll}\text { vacuum } & \text { from } & 1.2 \mathrm{dm}^{3} & \text { to } & 2.4 \mathrm{dm}^{3} \text { . }\end{array}\) The change in free energy of the gas, \(\Delta G\), is \((R=0.08\) bar- \(\mathrm{L} / \mathrm{K}-\mathrm{mol}, \ln 2=0.7)\) (a) 0 (b) \(-64\) bar- 1 (c) \(+84 \mathrm{~J}\) (d) \(-84 \mathrm{~J}\)

Inversion temperature is defined as the temperature above which a gas gets warm up and below which, the gas become cooler, when expanded adiabatically. Boyle temperature for a gas is \(20^{\circ} \mathrm{C}\). What will happen to the gas if it is adiabatically expanded at \(50^{\circ} \mathrm{C}\) ? (a) Heating (b) Cooling (c) Neither heating nor cooling (d) First cooling then heating

One mole of an ideal monoatomic gas undergoes adiabatic free expansion from 2 to \(20 \mathrm{dm}^{3}, 300 \mathrm{~K}\). The value of \(\Delta S\) for the gas is (a) 0 (b) \(+R \ln 10\) (c) \(-R \ln 10\) (d) \(+1.5 R \ln 10\)

The solubility of \(\mathrm{NaCl}(\mathrm{s})\) in water at \(298 \mathrm{~K}\) is about 6 moles per litre. Suppose you add 1 mole of \(\mathrm{NaCl}(\mathrm{s})\) to a litre of water. For the reaction: \(\mathrm{NaCl}(\mathrm{s})+\mathrm{H}_{2} \mathrm{O}\) \(\rightarrow \mathrm{NaCl}(\mathrm{aq})\) (a) \(\Delta G>0, \Delta S>0\) (b) \(\Delta G<0, \Delta S>0\) (c) \(\Delta G>0, \Delta S<0\) (d) \(\Delta G<0, \Delta S<0\)

A system undergoes a process in which the entropy change is \(+5.51 \mathrm{JK}^{-1}\). During the process, \(1.50 \mathrm{~kJ}\) of heat is added to the system at \(300 \mathrm{~K}\). The correct information regarding the process is (a) the process thermodynamically reversible. (b) the process is thermodynamically irreversible. (c) the process may or may not be thermodynamically reversible. (d) the process must be isobaric.

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