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Derive the ideal gas law, Eq. ( 10 ). Begin with the pressure integral (Eq. 9 ) and the Maxwell-Boltzmann velocity distribution functio, $$n_{v} d v=n\left(\frac{m}{2 \pi k T}\right)^{3 / 2} e^{-m v^{2} / 2 k T} 4 \pi v^{2} d v$$ $$\begin{aligned}&P_{g}=n k T\\&P=\frac{1}{3} \int_{0}^{\infty} m n_{v} v^{2} d v\end{aligned}$$

   Derive the ideal gas law, Eq. ( 10 ). Begin with the pressure integral (Eq. 9 ) and the Maxwell-Boltzmann velocity distribution functio,
$$n_{v} d v=n\left(\frac{m}{2 \pi k T}\right)^{3 / 2} e^{-m v^{2} / 2 k T} 4 \pi v^{2} d v$$
$$\begin{aligned}&P_{g}=n k T\\&P=\frac{1}{3} \int_{0}^{\infty} m n_{v} v^{2} d v\end{aligned}$$
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An Introduction to Modern Astrophysics
An Introduction to Modern Astrophysics
Bradley W. Carroll,… 2nd Edition
Chapter 11, Problem 5 ↓

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This gives us: $$P=\frac{1}{3} \int_{0}^{\infty} m n\left(\frac{m}{2 \pi k T}\right)^{3 / 2} e^{-m v^{2} / 2 k T} 4 \pi v^{4} d v$$  Show more…

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Derive the ideal gas law, Eq. ( 10 ). Begin with the pressure integral (Eq. 9 ) and the Maxwell-Boltzmann velocity distribution functio, $$n_{v} d v=n\left(\frac{m}{2 \pi k T}\right)^{3 / 2} e^{-m v^{2} / 2 k T} 4 \pi v^{2} d v$$ $$\begin{aligned}&P_{g}=n k T\\&P=\frac{1}{3} \int_{0}^{\infty} m n_{v} v^{2} d v\end{aligned}$$
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Key Concepts

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Integration in Statistical Mechanics
Integration techniques in statistical mechanics are used to sum over the contributions of all possible molecular speeds or states to obtain macroscopic thermodynamic quantities. In the derivation of the ideal gas law, the integration of the Maxwell-Boltzmann velocity distribution is crucial. By integrating the squared velocity weighted by the distribution, one obtains the average kinetic energy which directly relates to the pressure of the gas.
Equipartition Theorem
The equipartition theorem states that energy is equally distributed among all available degrees of freedom in a system at thermal equilibrium. For gases, this means that each translational degree of freedom contributes equally to the total kinetic energy. This concept links temperature to the average kinetic energy per molecule, providing a basis for deriving expressions for pressure and temperature from molecular motion.
Maxwell-Boltzmann Distribution
The Maxwell-Boltzmann distribution describes the statistical distribution of speeds (or velocities) of particles in an ideal gas in thermal equilibrium. It provides the probability of finding a particle with a given speed in terms of the mass of the particle, the temperature of the system, and fundamental constants. This distribution is essential in kinetic theory for deriving macroscopic properties like pressure and temperature.
Ideal Gas Law
The Ideal Gas Law is a fundamental equation of state for gases that relates the pressure, volume, and temperature of an ideal gas. It is typically expressed as PV = nRT (or PV = NkT when using the number of molecules), assuming that the particles do not interact except through elastic collisions. This law is a bridge between microscopic molecular behavior and macroscopic observable properties.
Kinetic Theory of Gases
The kinetic theory of gases explains macroscopic gas properties by considering the motions and collisions of individual molecules. It establishes that gas pressure results from molecules repeatedly colliding with the walls of a container, with each collision imparting momentum. By integrating contributions from molecules moving at different speeds, one can relate the microscopic kinetic energy of particles to the macroscopic pressure of the gas.

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