Wolfram Demonstrations Project
Statistical Mechanics
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Demonstrations 221 - 240 of 265
Unsteady-State Interphase DiffusionResidence Time Distribution Function of a Stirred-Tank Cascade (E-Curve)Penetration of Potential in a Semi-Infinite RegionDerivation of Thermodynamic Derivatives Using JacobiansPhase Transitions in 2D Cellular Automata--A 3D View
Unsteady-State Interphase Diffusion
Residence Time Distribution Function of a Stirred-Tank Cascade (E-Curve)
Penetration of Potential in a Semi-Infinite Region
Derivation of Thermodynamic Derivatives Using Jacobians
Phase Transitions in 2D Cellular Automata--A 3D View
Hopf Bifurcation in the BrusselatorHeat Conduction in Some Standard SolidsThe Maxwell Speed DistributionConstruction of the Rate-Conversion-Temperature Chart from Kinetic DataLava Lamp
Hopf Bifurcation in the Brusselator
Heat Conduction in Some Standard Solids
The Maxwell Speed Distribution
Construction of the Rate-Conversion-Temperature Chart from Kinetic Data
Lava Lamp
Einstein SolidDiffusion-Limited Aggregation: A Real-Time Agent-Based SimulationCarnot Cycle on Ideal GasReactor Steady StatesMolecular Dynamics of Lennard-Jones Particles Using the Velocity Verlet Algorithm
Einstein Solid
Diffusion-Limited Aggregation: A Real-Time Agent-Based Simulation
Carnot Cycle on Ideal Gas
Reactor Steady States
Molecular Dynamics of Lennard-Jones Particles Using the Velocity Verlet Algorithm
Equivalent Isothermal Time at a Reference Temperature as a Function of TimeBose-Einstein, Fermi-Dirac, and Maxwell-Boltzmann StatisticsLog Survival Ratio as a Function of TimeWeibullian Inactivation Rate as a Function of TimeWeibullian Inactivation Rate as a Function of Temperature
Equivalent Isothermal Time at a Reference Temperature as a Function of Time
Bose-Einstein, Fermi-Dirac, and Maxwell-Boltzmann Statistics
Log Survival Ratio as a Function of Time
Weibullian Inactivation Rate as a Function of Time
Weibullian Inactivation Rate as a Function of Temperature

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