Wolfram Demonstrations Project
Materials Science
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Demonstrations 21 - 40 of 244
Mohr's Arbelos and Lamé's EllipsoidsElectronic Structure of 1D and 2D Quasiperiodic SystemsCahn-Hilliard Equation for Phase SeparationThe 14 3D Bravais LatticesThe Structure of Diamond
Mohr's Arbelos and Lamé's Ellipsoids
Electronic Structure of 1D and 2D Quasiperiodic Systems
Cahn-Hilliard Equation for Phase Separation
The 14 3D Bravais Lattices
The Structure of Diamond
Coloring 2D Metallic-Mean Quasicrystal Tilings with a Mesh-Based MethodSpectral Properties of 1D Fibonacci QuasicrystalsEigenvalues and Eigenfunctions for Angular Double-Well PotentialPhosphorene Quantum DotsSolubilization Model for Ionic Compounds
Coloring 2D Metallic-Mean Quasicrystal Tilings with a Mesh-Based Method
Spectral Properties of 1D Fibonacci Quasicrystals
Eigenvalues and Eigenfunctions for Angular Double-Well Potential
Phosphorene Quantum Dots
Solubilization Model for Ionic Compounds
Motion of Three Magnetic VorticesFlory-Huggins Model for Gibbs Free Energy of Mixing in Polymer SolutionsDistribution of End-to-End Distances in Linear Substituted PolymethylenesEvaporative Crystallization with RecycleMass Balances in Evaporative Crystallization
Motion of Three Magnetic Vortices
Flory-Huggins Model for Gibbs Free Energy of Mixing in Polymer Solutions
Distribution of End-to-End Distances in Linear Substituted Polymethylenes
Evaporative Crystallization with Recycle
Mass Balances in Evaporative Crystallization
Spectral-Temporal Distribution of Biphotons from a Spontaneous Parametric Down Conversion (SPDC) ProcessNucleation Rates for Cd-Se NanoparticlesOn the Ewing Model of MagnetismFour Kinds of Rhombic PolyhedraSimple Crystal Structures and Miller Indices
Spectral-Temporal Distribution of Biphotons from a Spontaneous Parametric Down Conversion (SPDC) Process
Nucleation Rates for Cd-Se Nanoparticles
On the Ewing Model of Magnetism
Four Kinds of Rhombic Polyhedra
Simple Crystal Structures and Miller Indices

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