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Boltzmann distribution
A formula describing the statistical distribution of particles in a system among different energy levels.
Applications of the Boltzmann-distribution I.: Nernst equation
- P.E = Charge * Voltage
- Has long formula
Applications of the Boltzmann-distribution II.: equilibrium and rate of chemical reactions. (The Arrhenius plot)
- In chemical reactions atoms must transition from one energy state A, to state B.
- In equilibrium the distribution between the states can be calculated with formula.
- na/nb = K (equi. Constant)
- Arrhenius plot, Graph K / 1/t and the slope gibes the energy distribution between 2 states.
Applications of the Boltzmann-distribution III.: barometric formula
- In thermal equilibrium we can measure decreases in atmospheric density vs altitude by this formula.
Applications of the Boltzmann-distribution IV. electric conductivity of semiconductors.
- Depends on number of electrons which are able to transition from valence band through gap to the conduction band.
- Number increases with T.
- Using Boltzmann distribution we can calculate fraction of electrons that are able to cross the gap.
(Delta e)
Macrostate and microstate in thermodynamics
- Microstate: Examination of molecular state of system and instant state. (Location of particles, velocity of particles, momentum)
- Macrostate: Examine whole system (Pressure, Temperature)
- In Thermal equilibrium the macro states stay constant whole microstate always changes.
Boltzmann’s definition of entropy
S = k * ln
S = entropy (extensive quantity of heat)
- Number of micro states which belong to a macrostate
Kinetic gas theory
- Particles are small compared to volume
- Constant random motion
- Collision of particles is elastic
- Particles exert pressure when colliding with container wall
- Molecular speed is proportional to temperature
Maxwell-Boltzmann velocity distribution
- Upon increasing temperature, average absolute value of molecular speed increases
- Width of distribution increases due to increase in interactions between molecules
The Ideal gas
- Non realistic gas
- Composed of molecules which follow the kinetic gas theory
- Pv = nrt
The real gas
- Contrary to ideal gas
- Particles are not point like
- Volume is not negligible
- Less volume available for motion
- Interaction between particles arise and pressure becomes reduced
- Explains possibility of condensartion
State equation of real gases
() () = nkt
Pressure of ideal gases
Pv=nRt
The crystalline state (unit cell, crystal defects)
- Unit cells arrange to form crystal lattice.
- Ideal crystals: Infinite periodic spatial sequences of identical structural elements.
- Real crystals: Microcrystaline, keep their identical spatial sequence only in microscopic scale and instead have various sizes and orientations in structure.
- Defects: Point defect, Line defect, Surface defect
Optical properties of crystalline materials
Anisotropic, their physical properties are dependent on direction of measurement related to orientation of atoms in the crystal.