A material is found to have a thermal expansivity \(\alpha_{P}=R / P v+a / R T^{2} v\) and an isothermal compressibility \(K_{T}=1 / v(T f(P)+(b / P))\) where \(v=V / n\) is the molar volume. (a) Find \(f(P)\). (b) Find the equation of state. (c) Under what conditions is this material mechanically stable?

Short Answer

Expert verified
Function \(f(P)\): \(f(P)=\frac{1}{T}\left( -\frac{1}{Pv}\left(\frac{\partial v}{\partial P}\right)_T- \frac{b}{P}\right)\). Equation of state: \(Pv=RT+\frac{a}{T}\). Stability: \(T f(P)+\frac{b}{P}>0\).

Step by step solution

01

Understand the given formulas

Identify given expressions for thermal expansivity \ \( \alpha_{P}=\frac{R}{Pv} + \frac{a}{RT^{2}v} \) and isothermal compressibility \ \( K_{T} = \frac{1}{v(T f(P)+(b/P))} \). Note that \(v = V/n\) is the molar volume.
02

Define and Relate Variables

Recognize that \( \alpha_{P} = \frac{1}{v} \left( \frac{\partial v}{\partial T} \right)_P \) and \( K_{T} = - \frac{1}{v} \left( \frac{\partial v}{\partial P} \right)_T \). Identify terms to find functions for pressure and volume.
03

Find Expression for f(P) [Part (a)]

Solve function \(f(P)\) using relation between \(K_{T}\) and partial derivatives of volume with respect to pressure. Simplifying: \ \( K_{T} = - \frac{1}{v} \left( \frac{\partial v}{\partial P} \right)_T = \frac{1}{v(T f(P)+(b/P))} \). Rearrange: \ \( - \left( \frac{\partial v}{\partial P} \right)_T = \frac{1}{(Tf(P) + b/P)} \). Adjust to isolate for \(f(P)\). Solution: \ \( f(P) = \frac{1}{T} \left( - \frac{1}{Pv} \left( \frac{\partial v}{\partial P} \right)_T - \frac{b}{P} \right) \).
04

Find the Equation of State [Part (b)]

Rearrange given expressions to obtain an equation of state that includes \(T\), \(P\), and \(v\). Integrate or substitute as necessary to derive: Equation of state: \ \[(Pv)=RT+ \frac{a}{T} \].
05

Determine Mechanical Stability Conditions [Part (c)]

Assess mechanical stability using criteria derived from physical laws including the dependency on volume and pressure. Specifically, stability condition for isothermal compressibility \(K_{T}>0\) implies \ \( T f(P)+ \frac{b}{P}>0 \). Analyze terms ensuring function remains positive.

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Key Concepts

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

thermal expansivity
Understanding thermal expansivity is crucial in statistical physics. Thermal expansivity, often represented by the symbol \( \alpha_{P} \), measures how much the volume of a material changes in response to a change in temperature, while keeping the pressure constant. Mathematically, it's defined as:\( \alpha_{P} = \frac{1}{v} \left( \frac{\partial v}{\partial T} \right)_{P} \) In the given exercise, thermal expansivity is expressed as:\( \alpha_{P} = \frac{R}{Pv} + \frac{a}{RT^{2}v} \) Here, \( R \) stands for the gas constant, \( P \) is the pressure, \( v \) is the molar volume, \( T \) is the temperature, and \( a \) is a constant. This relation shows us how both pressure and temperature impact the volume of the material.
isothermal compressibility
Isothermal compressibility, denoted as \( K_{T} \), tells us how the volume of a material changes with pressure, while the temperature remains constant. It's defined by the formula:\( K_{T} = - \frac{1}{v} \left( \frac{\partial v}{\partial P} \right)_{T} \) For our exercise, it's given as:\( K_{T} = \frac{1}{v(T f(P) + \frac{b}{P})} \) This implies the relationship between compressibility, pressure, volume, and an additional function \( f(P) \), dependent on pressure. Here, \( b \) is another constant. The presence of \( f(P) \) indicates a unique dependency of compressibility on pressure and temperature.
molar volume
Molar volume, represented by \( v \), is the volume occupied by one mole of a substance. It's related to the material's density and is expressed as:\( v = \frac{V}{n} \) where \( V \) is the total volume and \( n \) is the number of moles. In the context of the given problem, molar volume appears in both the thermal expansivity and isothermal compressibility equations. It acts as a bridge linking the amount of substance, its volume, temperature, and pressure. These relationships are essential in deriving both \( f(P) \) and the equation of state.
equation of state
An equation of state is a mathematical equation connecting the state variables such as pressure \( P \), volume \( V \), and temperature \( T \) of a material. For the given exercise, we derive the equation of state as:\( Pv = RT + \frac{a}{T} \) This equation explains how the pressure, volume, and temperature are interrelated for the material. The term \( \frac{a}{T} \) introduces a correction factor based on temperature, distinguishing this from the ideal gas law \( Pv = nRT \). Such equations are fundamental in understanding how materials behave under different physical conditions.
mechanical stability
Mechanical stability refers to the tendency of a material to maintain its structure without changing its volume indefinitely. For a system to be mechanically stable, the isothermal compressibility must be positive:\( K_{T} > 0 \) This implies that \( T f(P) + \frac{b}{P} > 0 \) in our exercise. This condition ensures that the material does not collapse or expand uncontrollably under constant temperature and varying pressure. Stability is crucial for practical applications, as it ensures that a material can withstand external pressures without deforming beyond acceptable limits.

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Most popular questions from this chapter

A stochastic process, involving three fluctuating quantities, \(x_{1}, x_{2}\), and \(x_{3}\), has a probability distribution $$ P\left(x_{1}, x_{2}, x_{3}\right)=C \exp \left[-\frac{1}{2}\left(2 x_{1}^{2}+2 x_{1} x_{2}+4 x_{2}^{2}+2 x_{1} x_{3}+2 x_{2} x_{3}+2 x_{3}^{2}\right)\right] $$ where \(C\) is the normalization constant. (a) Write probability distribution in the form \(P\left(x_{1}, x_{2}, x_{3}\right)=C \exp \left(-1 / 2 x^{T} \cdot g+x\right)\), where \(g\) is a \(3 \times 3\) symmetric matrix, \(x\) is a column matrix with matrix elements \(x_{i}, i=1,2,3\), and \(x^{T}\) is its transpose. Obtain the matrix \(\boldsymbol{g}\) and its inverse \(g^{-1}\). (b) Find the eigenvalues \(\lambda_{i}(i=1,2,3)\) and orthonormal eigenvectors of \(\boldsymbol{g}\) and obtain the \(3 \times 3\) orthogonal matrix \(\boldsymbol{O}\) that diagonalizes the matrix \(\boldsymbol{g}\) (get numbers for all of them). Using this orthogonal matrix, we can write \(x^{\mathrm{T}} \cdot g \cdot x=x^{\mathrm{T}} \cdot \boldsymbol{O}^{\mathrm{T}} \cdot \boldsymbol{O} \cdot g \cdot \boldsymbol{O}^{\mathrm{T}} \cdot \boldsymbol{O} \cdot \boldsymbol{x}=\boldsymbol{a}^{\mathrm{T}} \cdot \bar{\Lambda} \cdot \boldsymbol{a}=\sum_{i=1}^{3} \lambda_{i} a_{i}^{2}\) where \(\boldsymbol{O} \cdot g \cdot \boldsymbol{O}^{\mathrm{T}}=\bar{\Lambda}\) is a \(3 \mathrm{x}\) 3 diagonal matrix with matrix elements \((\bar{A})_{i, j}=\lambda_{i} \delta_{i, j}\) and \(\boldsymbol{O} \cdot \boldsymbol{x}=\boldsymbol{a}\) is a column matrix with elements, \(a_{i}(i=1,2,3)\). (c) Compute the normalization constant, C. (d) Compute the moments \(\left(x_{i}\right)(i=1,2,3),\left\langle x_{i} x_{j}\right\rangle(i=1,2,3, j=1,2,3)\left(x_{1}^{2} x_{2} x_{3}\right)\) and \(\left\langle x_{1} x_{2}^{2} x_{3}\right\rangle+\) (Note that Exercises \(\mathrm{A.7}\) and \(\mathrm{A} .8\) might be helpful.)

A Carnot engine uses a paramagnetic substance as its working substance. The equation of state is \(M=n D H / T\), where \(M\) is the magnetization, \(H\) is the magnetic field, \(n\) is the number of moles, \(D\) is a constant determined by the type of substance, and \(T\) is the temperature. (a) Show that the internal energy \(U\), and therefore the heat capacity \(C_{M}\), can only depend on the temperature and not the magnetization. Let us assume that \(C_{M}=C=\) constant. (b) Sketch a typical Carnot cycle in the \(M-H\) plane. (c) Compute the total heat absorbed and the total work done by the Carnot engine. (d) Compute the efficiency of the Carnot engine.

Compute the heat capacity at constant magnetic field \(C_{H, n}\), the susceptibilities \(X_{T}, \mathrm{n}\) and \(X_{S, n}\) ' and the thermal expansivity \(\alpha_{H, n}\) for a magnetic system, given that the mechanical equation of state is \(M=\mathrm{n} D H / T\) and the heat capacity is \(C_{M, n}=\pi c_{\prime}\) where \(M\) is the magnetization, \(H\) is the magnetic field, \(\mathrm{n}\) is the number of moles, \(D\) is a constant, \(c\) is the molar heat capacity, and \(T\) is the temperature.

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