The spherical triple integral builds the sphere’s volume slice by slice, ρ² sinφ dρ dθ dφ guiding every infinitesimal shell.Red dots tracing the radius, blue sector sweeping the angle, green base anchoring height; lands exactly on 4/3πR³.
1:06
x.comMathematica
The spherical triple integral builds the sphere’s volume slice by slice, ρ² sinφ dρ dθ dφ guiding every infinitesimal shell.Red dots tracing the radius, blue sector sweeping the
Mathematica (@mathemetica). 9 replies. The spherical triple integral builds the sphere’s volume slice by slice, ρ² sinφ dρ dθ dφ guiding every infinitesimal shell.Red dots tracing the radius, blue sector sweeping the angle, green base anchoring height; lands exactly on 4/3πR³.
56.2K views2 months ago
Mathematica Tutorial
Mathematica Tutorial: Getting Started for Absolute Beginners
42:50
Mathematica Tutorial: Getting Started for Absolute Beginners
YouTubeLeandro Junes
70.8K viewsAug 7, 2020
Mathematica Essentials: Intro & Overview (Wolfram Language)
10:23
Mathematica Essentials: Intro & Overview (Wolfram Language)
YouTubeSocratica
179.5K viewsAug 16, 2021
Mathematica For Beginners: The Basics
54:06
Mathematica For Beginners: The Basics
YouTubeRichard Southwell
299.6K viewsMar 29, 2014
Top videos
Ripplegraphy – Mesmerizing 3D mathematical ripplesA dynamic 3D surface plot showing concentric waves radiating outward, like a pebble dropped in a pond. Formula:f(x, y) = sin(10 × ((x/d)² + (y/d)²)) / 5
0:08
Ripplegraphy – Mesmerizing 3D mathematical ripplesA dynamic 3D surface plot showing concentric waves radiating outward, like a pebble dropped in a pond. Formula:f(x, y) = sin(10 × ((x/d)² + (y/d)²)) / 5
x.comMathematica
2.9K views3 weeks ago
3D visualization of Euler’s formula: e^{jθ} = cos(θ) + j sin(θ).A point traces the unit circle in the complex plane while red, green, and blue curves project the cosine, sine, and exponential paths along the θ-axis.
1:27
3D visualization of Euler’s formula: e^{jθ} = cos(θ) + j sin(θ).A point traces the unit circle in the complex plane while red, green, and blue curves project the cosine, sine, and exponential paths along the θ-axis.
x.comMathematica
219.7K views3 months ago
Watch points instantly snap to their nearest neighbor center; arrows show the magnetic pull in real time!Local greedy rule produces macroscopic order; perfect swirling dipoles one moment, full turbulence the next.
0:18
Watch points instantly snap to their nearest neighbor center; arrows show the magnetic pull in real time!Local greedy rule produces macroscopic order; perfect swirling dipoles one moment, full turbulence the next.
x.comMathematica
32.8K views3 months ago
Mathematica Projects
Getting Started with Mathematica
38:40
Getting Started with Mathematica
YouTubeChristopher Lum
138.1K viewsSep 28, 2018
Mathematica Basics
12:25
Mathematica Basics
YouTubeWolfram
136.3K viewsSep 2, 2010
Basic Things You Need To Know To Start With MATHEMATICA | Tutorial-1(ENG)
19:51
Basic Things You Need To Know To Start With MATHEMATICA | Tutorial-1(ENG)
YouTubePhyLosophy
107.3K viewsJun 9, 2020
Ripplegraphy – Mesmerizing 3D mathematical ripplesA dynamic 3D surface plot showing concentric waves radiating outward, like a pebble dropped in a pond. Formula:f(x, y) = sin(10 × ((x/d)² + (y/d)²)) / 5
0:08
Ripplegraphy – Mesmerizing 3D mathematical ripplesA dynamic 3D surface plot showing concentric waves radiating outward, like a pebble dropped in a pond. Formula:f(x, y) = sin(10 × ((x/d)² + (y/d)²)) / 5
2.9K views3 weeks ago
x.comMathematica
3D visualization of Euler’s formula: e^{jθ} = cos(θ) + j sin(θ).A point traces the unit circle in the complex plane while red, green, and blue curves project the cosine, sine, and exponential paths along the θ-axis.
1:27
3D visualization of Euler’s formula: e^{jθ} = cos(θ) + j sin(θ).A point traces the unit circle in the complex plane while red, green, and blue curves project the cosine, sine, and exponential paths along the θ-axis.
219.7K views3 months ago
x.comMathematica
Watch points instantly snap to their nearest neighbor center; arrows show the magnetic pull in real time!Local greedy rule produces macroscopic order; perfect swirling dipoles one moment, full turbulence the next.
0:18
Watch points instantly snap to their nearest neighbor center; arrows show the magnetic pull in real time!Local greedy rule produces macroscopic order; perfect swirling dipoles one moment, full turbulence the next.
32.8K views3 months ago
x.comMathematica
Discrete topology meets nonlinear dynamics in this higher-order nodal network. Irrotational and solenoidal flows synchronize, diffuse, and self-organize into emergent collective states.The quiet mathematics powering next-gen ML and neural rhythms.
0:20
Discrete topology meets nonlinear dynamics in this higher-order nodal network. Irrotational and solenoidal flows synchronize, diffuse, and self-organize into emergent collective states.The quiet mathematics powering next-gen ML and neural rhythms.
15.6K views3 months ago
x.comMathematica
Touch a bowl of water to excite a superposition of symmetric surface wave modes with different frequencies. Sunlight refracts through ripples into caustics below. Absent energy dissipation, these waves would theoretically reconstruct original shape.
0:24
Touch a bowl of water to excite a superposition of symmetric surface wave modes with different frequencies. Sunlight refracts through ripples into caustics below. Absent energy dissipation, these waves would theoretically reconstruct original shape.
1.7K views3 months ago
x.comMathematica
∑ Δ_i² = 0Jingdiao CNC nulls every term in the tolerance stack. RMS deviation hits machine epsilon; kinematic pairs close with exact constraint equations, zero residual DOF.Applied in aerospace gyros and EUV lithography stages.
0:59
∑ Δ_i² = 0Jingdiao CNC nulls every term in the tolerance stack. RMS deviation hits machine epsilon; kinematic pairs close with exact constraint equations, zero residual DOF.Applied in aerospace gyros and EUV lithography stages.
20K views2 months ago
x.comMathematica
The most underrated math theorem but Google secretly used it to change the world.Perron-Frobenius Theorem (positive matrix version): Let A be an n×n matrix with every entry a_{ij} > 0. Then there exists a unique positive real number λ > 0 (the Perron root) and a unique (up to scaling) positive vector x > 0 such that:A x = λ xMoreover:λ = ρ(A) (spectral radius of A)λ > |μ| for every other eigenvalue μλ is simple (algebraic multiplicity = 1)Your search results aren't just a list; they are the coor
0:06
The most underrated math theorem but Google secretly used it to change the world.Perron-Frobenius Theorem (positive matrix version): Let A be an n×n matrix with every entry a_{ij} > 0. Then there exists a unique positive real number λ > 0 (the Perron root) and a unique (up to scaling) positive vector x > 0 such that:A x = λ xMoreover:λ = ρ(A) (spectral radius of A)λ > |μ| for every other eigenvalue μλ is simple (algebraic multiplicity = 1)Your search results aren't just a list; they are the coor
22.3K views1 month ago
x.comMathematica
0:15
The wave equation in spherical coords: ∇²Φ = (1/c²)∂²Φ/∂t² drives these levitated droplets into pure l=3 & l=4 modes. Watching a water drop morph into perfect triangular stars & quadrupolar symmetry at ultrasonic resonance is pure fluid poetry.
100.9K views2 months ago
x.comMathematica
0:21
Watch this fractal binary tree grow iteratively. It's incredible how simple recursive algorithms can generate such lifelike complexity.
8.5K views1 month ago
x.comMathematica
0:37
RT @mathemetica: When four simple periodic grids in CMYK phase-shift you get this.Beat frequencies, moiré patterns, and full-spectrum hal…
328K views3 months ago
x.comMathematica
0:29
∑ F_i = M a∑ τ_i = I αWatching individual ants with near-zero global visibility cooperatively transport a large rigid payload through a constrained T-shaped aperture using purely local force and torque interactions. This is a live demonstration of emergent coordination via distributed physics-based optimization. No central controller or lead architect: just local sensing, attachment forces, stochastic adjustments, and collective "noise" enabling the group to discover viable rotation-translation
17.7K views2 months ago
x.comMathematica
1:23
Linear dynamics x' = Ax in ℝ³, ruled by the eigenvalues of A. Real λ → flows along eigendirections. Complex pair → spirals. Triple repeated λ (defective) → it tries to spiral but can’t quite.
21.4K views3 months ago
x.comMathematica
0:17
F = ma meets a² + b² = c²Three strings. Three masses: 3m, 4m, 5m.Pulleys, gravity, equilibrium.The tensions balance perfectly only when the angles form a right triangle; because the vector sum closes exactly when the sides satisfy 3² + 4² = 5².You don't just see the theorem.You feel the forces prove it in real time. The strings go slack or snap out of balance the instant you break the ratio.This is why your bridge doesn't collapse, why your rocket hits orbit, and why the Pythagorean theorem isn'
114.2K views2 months ago
x.comMathematica
0:59
Mathematica (@mathemetica) on X
8.8K views2 months ago
x.comMathematica
0:41
5×5 lattice. One node perturbed. The discrete heat equation unfolds in real time: ∂u/∂t = αΔu, solved via finite differences. A single thermal impulse diffuses outward, colors bleeding through the grid like living eigenvectors.
13.3K views3 months ago
x.comMathematica
1:18
(1/n) ∑_{i=0}^{n-1} f(T^i x) → ∫_X f dμWatching Maryam Mirzakhani command the blackboard like this; unique ergodicity, the convergence of invariant measures, the rhythmic tap of the chalk: it hits different. The absolute fluid motion, the focus, the way she translates the chaotic dance of orbits into a singular, elegant truth.This is pure dynamical magic: where the statistical history of a single point dictates the behavior of the entire space. It’s the bridge between simple iterations and the d
25.4K views2 months ago
x.comMathematica
See more
Static thumbnail place holder