Maxwell-Boltzmann distribution

(noun)

A distribution describing particle speeds in gases, where the particles move freely without interacting with one another, except for very brief elastic collisions in which they may exchange momentum and kinetic energy.

Related Terms

  • disorder

Examples of Maxwell-Boltzmann distribution in the following topics:

  • Speed Distribution of Molecules

    • A gas of many molecules has a predictable distribution of molecular speeds, known as the Maxwell-Boltzmann distribution.
    • Maxwell-Boltzmann distribution is a probability distribution.
    • The Maxwell–Boltzmann distribution for the speed follows immediately from the distribution of the velocity vector, above.
    • The Maxwell-Boltzmann distribution of molecular speeds in an ideal gas.
    • Describe the shape and temperature dependence of the Maxwell-Boltzmann distribution curve
  • Distribution of Molecular Speeds and Collision Frequency

    • The Maxwell-Boltzmann Distribution describes the average molecular speeds for a collection of gas particles at a given temperature.
    • In theory, this energy can be distributed among the gaseous particles in many ways, and the distribution constantly changes as the particles collide with each other and with their boundaries.
    • This results in an asymmetric curve, known as the Maxwell-Boltzmann distribution.
    • Velocity distributions are dependent on the temperature and mass of the particles.
    • When we plot this, we see that an increase in temperature causes the Boltzmann plot to spread out, with the relative maximum shifting to the right.
  • Overview of Temperature and Kinetic Theory

    • The distribution of the speeds (which determine the translational kinetic energies) of the particles in a classical ideal gas is called the Maxwell-Boltzmann distribution.
    • (k: Boltzmann's constant).
  • Stastical Interpretation of Entropy

    • The most likely conditions (or macrostate) for the gas are those we see all the time—a random distribution of atoms in space with a Maxwell-Boltzmann distribution of speeds in random directions, as predicted by kinetic theory as shown in (a).
    • (a) The ordinary state of gas in a container is a disorderly, random distribution of atoms or molecules with a Maxwell-Boltzmann distribution of speeds.
  • The Arrhenius Equation

    • The equation combines the concepts of activation energy and the Boltzmann distribution law into one of the most important relationships in physical chemistry:
    • Recall that the exponential part of the Arrhenius equation ($e^{\frac{-E_a}{RT}}$) expresses the fraction of reactant molecules that possess enough kinetic energy to react, as governed by the Maxwell-Boltzmann distribution.
  • Order to Disorder

    • This notion was initially postulated by Ludwig Boltzmann in the 1800s.
    • Rather than having two masses at different temperatures and with different distributions of molecular speeds, we now have a single mass with a uniform temperature.
  • Variation of Pressure With Depth

    • Since, for gases and liquids, the force acting on a system contributing to pressure does not act on a specific point or particular surface, but rather as a distribution of force, analyzing pressure as a measure of energy per unit volume is more appropriate.
    • Thus the force contributing to the pressure of a gas within the medium is not a continuous distribution as for liquids and the barometric equation given in must be utilized to determine the pressure exerted by the gas at a certain depth (or height) within the gas (p0 is the pressure at h = 0, M is the mass of a single molecule of gas, g is the acceleration due to gravity, k is the Boltzmann constant, T is the temperature of the gas, and h is the height or depth within the gas).
    • The force contributing to the pressure of a gas within the medium is not a continuous distribution as for liquids and the barometric equation given in this figure must be utilized to determine the pressure exerted by the gas at a certain depth (or height) within the gas (p0 is the pressure at h = 0, M is the mass of a single molecule of gas, g is the acceleration due to gravity, k is the Boltzmann constant, T is the temperature of the gas, and h is the height or depth within the gas)
  • Particle-Wave Duality

    • In 1861, James Clerk Maxwell explained light as the propagation of electromagnetic waves according to the Maxwell's equations.
    • The standard interpretation is that the act of measurement causes the set of probabilities, governed by a probability distribution function acquired from a "wave", to immediately and randomly assume one of the possible values, leading to a "particle"-like result.
  • Radiation

    • The radiated energy depends on its intensity, which is represented by the height of the distribution .
    • The rate of heat transfer by emitted radiation is determined by the Stefan-Boltzmann law of radiation:
    • where =5.67×10−8 J s-1⋅m-2⋅K-4 is the Stefan-Boltzmann constant, A is the surface area of the object, and T is its absolute temperature in kelvin.
  • The Importance of Sociocultural Differences

    • Maxwell House advertised itself as the "great American coffee" in Germany.
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