Chapter 22: Problem 14
Temperature-dependent dielectric constants. Show that Coulombic interactions between charges in liquids can have an entropic component if the dielectric constant \(D\) depends on temperature.
Short Answer
Expert verified
Coulombic interactions have an entropic component if the dielectric constant depends on temperature, as the interaction energy includes an entropic term \(TS\).
Step by step solution
01
Understand Coulombic interactions
Coulombic interactions refer to the force between two charges. The force is given by Coulomb's law: \[ F = \frac{q_1 q_2}{4 \pi \epsilon_0 D r^2} \] Here, \(q_1\) and \(q_2\) are the charges, \(r\) is the distance between the charges, \( \epsilon_0\) is the vacuum permittivity, and \(D\) is the dielectric constant of the medium.
02
Express energy of interaction
The potential energy \(U\) of the interaction between two charges in a medium with a dielectric constant \(D\) is given by: \[ U = \frac{q_1 q_2}{4 \pi \epsilon_0 D r} \] This energy is dependent on \(D\) which may vary with temperature.
03
Identify entropic component
Entropy \(S\) is a measure of the number of specific ways in which a system may be arranged, often taken to be a measure of disorder. If the dielectric constant \(D\) depends on temperature \(T\), then changes in temperature can influence the system's entropy. The entropic component of energy is given by: \[ TS \] where \(T\) is temperature in Kelvin and \(S\) is entropy.
04
Relate dielectric constant to temperature
The dielectric constant \(D\) can be expressed as a function of temperature: \[ D = f(T) \] Here, any change in \(T\) will affect \(D\), which in turn affects the Coulombic interaction energy.
05
Differentiate entropic and energetic components
The total free energy \(F\) in a system that includes both energetic and entropic components is given by: \[ F = U - TS \] Since \(U\) depends on \(D\) which is a function of \(T\), the change in energy can also have an entropic component linked to the temperature dependency of \(D\). Therefore, Coulombic interactions in such a system can indeed have an entropic component when the dielectric constant depends on temperature.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Coulomb's Law
Coulomb's law describes how the force between two charged objects depends on the magnitude of their charges and the distance between them. The mathematical formula is given by: F = \frac{q_1 q_2}{4 \pi \epsilon_0 D r^2} Here, let’s break down what each symbol means: \(q_1\) and \(q_2\) are the amounts of charge on the two objects, \epsilon_0 \text{ is the vacuum permittivity, } D \text{ is the dielectric constant of the medium, } and r \text{ is the distance between the charges. } The dielectric constant, \(D\), is a measure of a material's ability to reduce the effective electrostatic force between two charges. As \(D\) increases, the force \(F\) decreases. The force can either be attractive or repulsive depending on whether the charges are opposite or similar (opposite charges attract, like charges repel). Understanding Coulomb's law is fundamental to grasping how forces act at a distance in many physical systems, including in liquids with varying dielectric constants.
Entropy
Entropy, commonly represented by \(S\), is a measure of disorder or randomness in a system. In thermodynamics, it's used to quantify the number of possible ways the system can be arranged. A higher entropy indicates more disorder.Entropy plays a crucial role in determining the spontaneity of a process. According to the second law of thermodynamics, the total entropy of an isolated system can never decrease over time. It always either increases or remains constant. When you have a temperature-dependent dielectric constant, changes in temperature impact the system’s entropy. If the dielectric constant \(D\) relies on temperature, fluctuations in temperature will alter the system's arrangement and therefore its entropy. This is important for understanding Coulombic interactions in such systems where the dielectric constant is not constant but is instead influenced by the surrounding environment.
Dielectric Constant Dependency on Temperature
The dielectric constant \(D\) is a property of materials that measures their ability to reduce the electrostatic forces between charges. In many materials, the dielectric constant is not static but varies with temperature. This temperature dependency is crucial in thermodynamics and electrostatics.The dielectric constant can be expressed as a function of temperature: D = f(T) Changes in temperature \(T\) can lead to variations in \(D\). These changes affect how much the material can insulate electrical charge. For example, in many liquids, as the temperature increases, the dielectric constant decreases, reducing the material's insulating properties.Temperature-dependent dielectric constants introduce additional complexity in understanding how Coulombic interactions behave in different conditions. When \(D\) varies, the electrostatic potential energy between charges also varies, leading to potential changes in the system’s entropy.
Free Energy in Thermodynamic Systems
Free energy, often represented by \(F\), in a thermodynamic system is the energy available to do work. It combines both the internal energy (potential energy) and the temperature-entropy product. The total free energy \(F\) is given by: F = U - TS Here, \(U\) is the internal or potential energy, \(T\) is the temperature, and \(S\) is the entropy. \(T\) and \(S\) influence the system's ability to do work.When dealing with temperature-dependent dielectric constants, the potential energy \(U\) depends on \(D\), which in turn depends on temperature \(T\). Thus, changes in temperature directly impact both the energetic (internal energy) and entropic components of the free energy. This understanding helps us see that systems involving Coulombic interactions in materials where the dielectric constant is dependent on temperature will have an entropic component as well as an energetic part in their free energy calculation.