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The Chinese Physicist Who Turned Force Into Geometry In 1954, Chinese physicist Chen-Ning Yang, together with Robert Mills, introduced a new idea that changed modern physics: Maybe a force is not just something that pushes or pulls. Maybe a force can come from geometry. In Yang-Mills Theory, every point... in space carries a hidden internal direction. As you move through space, that direction can twist. If you go around a closed loop and the direction does not return exactly the same, the field has curvature. That curvature is what we see as force. In this animation, the glowing surface shows where the gauge field is strongest. The changing colours show how the hidden internal direction varies across space. The moving rectangular loops are Wilson loops. They travel through the field and measure how much the internal direction changes after completing a closed path. The key equation behind the scene is Fₓᵧ = ∂ₓAᵧ - ∂ᵧAₓ + Aₓ × Aᵧ. The final term, Aₓ × Aᵧ, is the special part. It means the field can interact with itself. That self-interaction is one reason Yang-Mills theory became one of the foundations of particle physics. #China #ChinesePhysics #YangMills #GaugeTheory #QuantumFieldTheory #NonAbelianGeometry #WilsonLoops #ModernPhysics #STEMshow more

Mathelirium

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Why String Theory Won't Die The string theory idea refuses to die because it's one of the few frameworks that forces a quantum object and spacetime geometry into the same picture. In the render, a closed string isn’t just a loop doing pretty vibrations. Its internal phase pattern is a quantum degree of freedom, shown as color. At the same time, its motion stirs ripples in the surrounding metric, shown as the fabric below. One object, two roles. A wave-like state living on the string, and a curvature-like response spreading through the background. You can literally watch quantum stuff and gravity stuff talk to each other in the same scene. #StringTheory #Physics #QuantumMechanics #GeneralRelativity #MathematicalPhysics #SciComm

Why String Theory Won't Die The string theory idea refuses to die because it's one of the few frameworks that forces a quantum object and spacetime geometry into the same picture. In the render, a closed string isn’t just a loop doing pretty vibrations. Its internal phase pattern is a quantum degree of freedom, shown as color. At the same time, its motion stirs ripples in the surrounding metric, shown as the fabric below. One object, two roles. A wave-like state living on the string, and a curvature-like response spreading through the background. You can literally watch quantum stuff and gravity stuff talk to each other in the same scene. #StringTheory #Physics #QuantumMechanics #GeneralRelativity #MathematicalPhysics #SciComm

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Mathelirium

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Zyron

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Most people learned physics starting with particles. Tiny things. Moving through empty space. Forces pushing them around. Many engineers already know something different. Pixels don’t contain the image. Droplets don’t contain the pattern in a fountain display. Radio circuits don’t contain the music. In every case: individual events → timed in relation → repeating into stable patterns The structure isn’t in the components. It shows up through their coordination. Now follow that one step further. If patterns appear when events coordinate in phase, then what we call an object is a stabilized pattern of relations in a deeper field. That shift flips the usual physics story. Instead of starting with tiny parts and trying to glue the universe together, the demonstration in this video starts from global closure of the field itself. From that closure: • geometry is understood as the field closing on itself • forces and shapes arise as conjugate projections • quantum randomness is understood as information lost at measurement • particles show up as compressed views of coherent field structure Even “gravity” looks different. When geometry is understood as the signature of electromagnetic field closure, gravity is understood as large-scale nested electromagnetic interaction. Space itself is the field’s geometry responding to closure. And the same principle scales everywhere. Atoms close → molecules stabilize. Molecules close → cells stabilize. Each layer becomes the substrate for the next. So here’s the question worth sitting with: How does physics show up when we start from the field itself instead of the particles we measure inside it? 🔗 Link: Zenodo archive with The Grammar of Projection (formal articulation), it's conjugate, The Grammar of Persistence, nearly 500 pages of rigorous canonical derivations starting from global closure, and a couple supplemental documents. The description in the archive indexes the papers well. The recursion holds. 🌀

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Can Spacetime Move Faster Than Light? In 1994, Miguel Alcubierre proposed a strange solution to Einstein’s field equations: A Spacetime geometry where a compact region could be transported without the object inside locally breaking the speed of light. The idea is not that a ship accelerates through space faster than light. The local interior remains comparatively calm. The violent part is the surrounding geometry. Space contracts in front of the bubble, expands behind it, and forms a moving transport shell that carries the interior region forward. A simplified form of the Alcubierre metric is ds² = −dt² + [dx − vₛ f(rₛ)dt]² + dy² + dz² where f(rₛ) shapes the warp bubble and vₛ describes the motion of its centre. The physics is still highly speculative, especially because the original construction requires exotic stress-energy, but the mathematical idea is powerful. #GeneralRelativity #AlcubierreDrive #WarpDrive #Spacetime #EinsteinEquations #Relativity #Physics #Astrophysics #Cosmology

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37,986 views • 1 month ago

String Theory Lecture 1 A String Does Not Move Like a Point A point particle traces a line through spacetime. A string traces a surface. This is the first geometric shift in String Theory. Particle mechanics asks where one object is at time t, so its history is a curve. String Theory asks where every point of an extended object is at worldsheet time τ, so we need another coordinate telling us where we are along the string. For a point particle x(t) So, for one input of time we get a position in Spacetime. For a string Xᵘ(τ,σ) Here τ plays the role of time on the worldsheet, while σ labels position along the string. Freeze τ and vary σ, and you see the string at one instant. Let τ move, and that curve sweeps out a two-dimensional surface... the worldsheet. The same comparison appears in the action. For a relativistic point particle, the geometric action measures worldline length S = −m ∫ ds If we parameterize the path by t, the action has one integral, one parameter, and one tangent vector dxᵘ/dt For a string, the same idea grows by one dimension. The action measures area, not length. In Nambu-Goto form, S = −T ∫ dτ dσ √[−det hₐᵦ] Here T is the string tension. It plays a role similar to mass, but for an extended object. It weights the area of a surface rather than the length of a line. The particle action has ∫ dt because the history is one-dimensional. The string action has ∫ dτ dσ because the history is two-dimensional. We are no longer summing along a path, we are summing over a surface. The geometry changes for the same reason. For the particle, one derivative is enough dxᵘ/dt For the string, the geometry is built from two derivatives: ∂τXᵘ and ∂σXᵘ The first tells you how the string changes as worldsheet time flows. The second tells you how the embedding changes as you move along the string. Together they define the induced worldsheet metric hₐᵦ = ∂ₐXᵘ ∂ᵦXᵤ In plain terms, hₐᵦ measures tangent lengths and tangent angles on the worldsheet. From it, the area element is dA = dτ dσ √[−det hₐᵦ] This, the Nambu-Goto action is the direct analogue of the point-particle length action. The point particle extremizes length and the string extremizes area. For calculations, people usually switch to the Polyakov action: S = −(T/2) ∫ dτ dσ √[−γ] γᵃᵇ ∂ₐXᵘ ∂ᵦXᵤ This describes the same classical string dynamics, but the algebra is cleaner. After choosing conformal gauge, varying with respect to Xᵘ gives (∂²/∂τ² − ∂²/∂σ²) Xᵘ = 0 This is the first real dynamical payoff... a two-dimensional wave equation on the worldsheet. For a point particle, the equation of motion tells you how one position evolves along one path. For a string, it tells you how an entire curve evolves, with waves traveling along it. The term ∂²Xᵘ/∂τ² measures acceleration in worldsheet time, while ∂²Xᵘ/∂σ² measures curvature along the string. The time evolution is balanced by how the string bends along its own length. This is why strings have oscillation modes. A point particle has one trajectory. A string has many possible vibration patterns, each one a normal mode of the worldsheet wave equation. For a closed string, σ wraps around the loop Xᵘ(τ, σ + 2π) = Xᵘ(τ, σ) For an open string, one standard free-end condition is ∂σXᵘ = 0 at the endpoints. Solving the wave equation gives waves moving in opposite directions along the string Xᵘ(τ,σ) = Fᵘ(τ + σ) + Gᵘ(τ − σ) A function of τ + σ moves one way. A function of τ − σ moves the other. Therefore, a particle has a worldline, its action measures length, and its geometry uses one tangent. The string has a worldsheet, its action measures area, and its geometry uses two tangent directions. #StringTheory #TheoreticalPhysics #MathematicalPhysics #Physics #Spacetime

String Theory Lecture 1 A String Does Not Move Like a Point A point particle traces a line through spacetime. A string traces a surface. This is the first geometric shift in String Theory. Particle mechanics asks where one object is at time t, so its history is a curve. String Theory asks where every point of an extended object is at worldsheet time τ, so we need another coordinate telling us where we are along the string. For a point particle x(t) So, for one input of time we get a position in Spacetime. For a string Xᵘ(τ,σ) Here τ plays the role of time on the worldsheet, while σ labels position along the string. Freeze τ and vary σ, and you see the string at one instant. Let τ move, and that curve sweeps out a two-dimensional surface... the worldsheet. The same comparison appears in the action. For a relativistic point particle, the geometric action measures worldline length S = −m ∫ ds If we parameterize the path by t, the action has one integral, one parameter, and one tangent vector dxᵘ/dt For a string, the same idea grows by one dimension. The action measures area, not length. In Nambu-Goto form, S = −T ∫ dτ dσ √[−det hₐᵦ] Here T is the string tension. It plays a role similar to mass, but for an extended object. It weights the area of a surface rather than the length of a line. The particle action has ∫ dt because the history is one-dimensional. The string action has ∫ dτ dσ because the history is two-dimensional. We are no longer summing along a path, we are summing over a surface. The geometry changes for the same reason. For the particle, one derivative is enough dxᵘ/dt For the string, the geometry is built from two derivatives: ∂τXᵘ and ∂σXᵘ The first tells you how the string changes as worldsheet time flows. The second tells you how the embedding changes as you move along the string. Together they define the induced worldsheet metric hₐᵦ = ∂ₐXᵘ ∂ᵦXᵤ In plain terms, hₐᵦ measures tangent lengths and tangent angles on the worldsheet. From it, the area element is dA = dτ dσ √[−det hₐᵦ] This, the Nambu-Goto action is the direct analogue of the point-particle length action. The point particle extremizes length and the string extremizes area. For calculations, people usually switch to the Polyakov action: S = −(T/2) ∫ dτ dσ √[−γ] γᵃᵇ ∂ₐXᵘ ∂ᵦXᵤ This describes the same classical string dynamics, but the algebra is cleaner. After choosing conformal gauge, varying with respect to Xᵘ gives (∂²/∂τ² − ∂²/∂σ²) Xᵘ = 0 This is the first real dynamical payoff... a two-dimensional wave equation on the worldsheet. For a point particle, the equation of motion tells you how one position evolves along one path. For a string, it tells you how an entire curve evolves, with waves traveling along it. The term ∂²Xᵘ/∂τ² measures acceleration in worldsheet time, while ∂²Xᵘ/∂σ² measures curvature along the string. The time evolution is balanced by how the string bends along its own length. This is why strings have oscillation modes. A point particle has one trajectory. A string has many possible vibration patterns, each one a normal mode of the worldsheet wave equation. For a closed string, σ wraps around the loop Xᵘ(τ, σ + 2π) = Xᵘ(τ, σ) For an open string, one standard free-end condition is ∂σXᵘ = 0 at the endpoints. Solving the wave equation gives waves moving in opposite directions along the string Xᵘ(τ,σ) = Fᵘ(τ + σ) + Gᵘ(τ − σ) A function of τ + σ moves one way. A function of τ − σ moves the other. Therefore, a particle has a worldline, its action measures length, and its geometry uses one tangent. The string has a worldsheet, its action measures area, and its geometry uses two tangent directions. #StringTheory #TheoreticalPhysics #MathematicalPhysics #Physics #Spacetime

Mathelirium

31,560 views • 3 months ago

String Theory is one of the few frameworks that tries to describe Quantum Physics and Gravity in the same mathematical language. In this animation, the glowing loop is the string, the shifting color along it represent its quantum vibration modes, and the surrounding fabric is a proxy for Spacetime responding. When you quantize a string, one of its vibration modes behaves like a graviton. So, geometry shows up as part of the same quantum system. #StringTheory #QuantumGravity #GeneralRelativity #QuantumPhysics #TheoreticalPhysics #PhysicsVisualization

String Theory is one of the few frameworks that tries to describe Quantum Physics and Gravity in the same mathematical language. In this animation, the glowing loop is the string, the shifting color along it represent its quantum vibration modes, and the surrounding fabric is a proxy for Spacetime responding. When you quantize a string, one of its vibration modes behaves like a graviton. So, geometry shows up as part of the same quantum system. #StringTheory #QuantumGravity #GeneralRelativity #QuantumPhysics #TheoreticalPhysics #PhysicsVisualization

Mathelirium

42,172 views • 5 months ago

Ever Heard of a Metric in Differential Geometry? How About a Geodesic? These two ideas are central to how Mathematics and Physics describe Spacetime. A metric is how a surface measures distance and angle. A geodesic is the path that counts as "straight" after that measuring rule is chosen. Once the metric changes from point to point, straightness is no longer something you judge by eye. On a curved surface, the shortest paths are geodesics. They are chosen by the metric. Take a surface written as r(x,y) = (x, y, f(x,y)) Its metric is gᵢⱼ = ∂ᵢr · ∂ⱼr A geodesic q(t) = (x(t), y(t)) obeys q̈ᵏ + Γᵏᵢⱼ q̇ᶦq̇ʲ = 0 where Γᵏᵢⱼ are the Christoffel symbols of the surface metric. Launch many almost-parallel paths. At the start, they look like a clean beam until curvature takes over. Some paths focus, others separate and some slide around ridges. The surface is essentially the rulebook for motion. The shortest path is local. The geometry remembers everything. #DifferentialGeometry #Geodesics #RiemannianGeometry #MathematicalPhysics #Curvature #TensorCalculus #AppliedMathematics #Geometry #ScienceAnimation

Ever Heard of a Metric in Differential Geometry? How About a Geodesic? These two ideas are central to how Mathematics and Physics describe Spacetime. A metric is how a surface measures distance and angle. A geodesic is the path that counts as "straight" after that measuring rule is chosen. Once the metric changes from point to point, straightness is no longer something you judge by eye. On a curved surface, the shortest paths are geodesics. They are chosen by the metric. Take a surface written as r(x,y) = (x, y, f(x,y)) Its metric is gᵢⱼ = ∂ᵢr · ∂ⱼr A geodesic q(t) = (x(t), y(t)) obeys q̈ᵏ + Γᵏᵢⱼ q̇ᶦq̇ʲ = 0 where Γᵏᵢⱼ are the Christoffel symbols of the surface metric. Launch many almost-parallel paths. At the start, they look like a clean beam until curvature takes over. Some paths focus, others separate and some slide around ridges. The surface is essentially the rulebook for motion. The shortest path is local. The geometry remembers everything. #DifferentialGeometry #Geodesics #RiemannianGeometry #MathematicalPhysics #Curvature #TensorCalculus #AppliedMathematics #Geometry #ScienceAnimation

Mathelirium

22,170 views • 1 month ago

🚨 NOW: President Trump takes huge VICTORY LAP on the success of Space Force — which some Democrats MOCKED Space Force is now vastly improving the accuracy of our weapons on the ground. And we're leading China and Russia, easily 🔥 "I'm very proud of the Space Force because that was a branch that a new one that came up, and we were losing to Russia and to China in space." "Space Force is now leading the other countries, China, Russia, and there is no fourth, really, and leading them by, we saw numbers the other day, leading, we're leading in space by so much it's, we're never going to be caught. So I'm very proud of Space Force!" "I think it's going to be one of our most important as time goes by. A lot of the things that you see, a lot of the accuracy of the weapons is caused because of what we created with Space Force, so we're very proud of that."

🚨 NOW: President Trump takes huge VICTORY LAP on the success of Space Force — which some Democrats MOCKED Space Force is now vastly improving the accuracy of our weapons on the ground. And we're leading China and Russia, easily 🔥 "I'm very proud of the Space Force because that was a branch that a new one that came up, and we were losing to Russia and to China in space." "Space Force is now leading the other countries, China, Russia, and there is no fourth, really, and leading them by, we saw numbers the other day, leading, we're leading in space by so much it's, we're never going to be caught. So I'm very proud of Space Force!" "I think it's going to be one of our most important as time goes by. A lot of the things that you see, a lot of the accuracy of the weapons is caused because of what we created with Space Force, so we're very proud of that."

Eric Daugherty

15,034 views • 3 months ago

Desveaux’s Theory of Helix Fields Tweet 1 of 2 For decades, we treated the universe like a giant stage where particles act out their lives. What if the stage itself isn't empty? What if the "void" of space is a structured, rotating medium that is constantly twisting & turning? We have been looking at the pieces of the puzzle, but ignoring the board they sit on. It’s been hiding in plain in sight? My idea on Helix Fields suggests everything we see, from the smallest atom to the largest galaxy, is actually a "corkscrew" in the fabric of reality. In standard physics, we think of particles like tiny billiard balls. In Helix Field Theory, we rethink them as solitons - essentially stable, high-energy "whirlpools" or "corkscrews" made of space itself. Imagine a ribbon. If you pull it straight, it’s flat and simple. But if you twist it, you create a spiral. That twist is what we call Torsion. My theory says that what we perceive as "matter" is simply a place where the vacuum of space is rotating so tightly that it creates a "density core." To explain how this all works, we use a mathematical roadmap called a Lagrangian. Think of it as a master recipe or cookbook for the universe. It combines four key ingredients: 1. Electricity and Magnetism: How light and energy move. 2. Scalar Fields: The underlying "pressure" of the vacuum in space itself 3. Matter: The physical "stuff" we can touch. 4. Torsion: The "twist" or rotational force of space. By looking at the universe through this "helix" lens, we can solve two of the biggest headaches in modern science: The Hubble Tension - Astronomers are currently arguing over how fast the universe is expanding because different measurements give different answers. My theory suggests this "tension" exists because we haven't accounted for the universal rotation (torsion) affecting our measurements. The Dark Sector - We know there is "Dark Matter" and "Dark Energy" out there, but we can't find it. Helix Field Theory suggests these aren't invisible particles, but rather geometric artifacts - ripples and shadows created by the rotating vacuum itself. We are moving away from a universe of "things" and toward a universe of geometry and motion. If the vacuum of space is a structured, rotating medium, then we aren't just living in the universe - we are part of its physical rotation. The "Quantum Substratum" isn't just a theory; it’s a new way to understand the very "twist" of existence. - Protons: tiny rotating black hole-like cores anchoring the scalar field - Neutrons: stabilisers that prevent proton cores from decaying - Quarks & Gluons: the deepest torsion knots; the strong force is intrinsic torsion - Electrons: corkscrew-shaped solitons producing microscopic magnetic vortices - Neutrinos: ultra-light messenger waves traveling along the field’s “communication lines.” - Photons: instruction ripples traveling at light speed - Dark Photons: the “torsion messengers” of the Helix Field. They carry the twist, regulate the twist, and stabilize the twisting motion - W and Z bosons: on/off switches and stabilising nodes in the neutrino network - Higgs field: the local density of the scalar field, giving solitons their effective mass - Dark energy: the gentle outward push caused by the field’s overall rotation - Entropy: friction in that rotation, giving time its arrow - Cosmic Microwave Background: the universal “sustain pedal” like on a guitar or piano, keeping the field’s vibrations in phase. In this vision, dark matter isn’t missing matter - it’s the gravitational echo of the scalar field itself. Exploring antiparticles further: they may regulate the flow of time itself. In a rotational and torsional universe Time is a neutral observer: the past and future are fixed, but the present - our free will - is the point where choices echo into fate. Time is the “God” of the universe: ever-present, ever-aware, never interfering - just watching, as we decide which thread to follow.

Desveaux’s Theory of Helix Fields Tweet 1 of 2 For decades, we treated the universe like a giant stage where particles act out their lives. What if the stage itself isn't empty? What if the "void" of space is a structured, rotating medium that is constantly twisting & turning? We have been looking at the pieces of the puzzle, but ignoring the board they sit on. It’s been hiding in plain in sight? My idea on Helix Fields suggests everything we see, from the smallest atom to the largest galaxy, is actually a "corkscrew" in the fabric of reality. In standard physics, we think of particles like tiny billiard balls. In Helix Field Theory, we rethink them as solitons - essentially stable, high-energy "whirlpools" or "corkscrews" made of space itself. Imagine a ribbon. If you pull it straight, it’s flat and simple. But if you twist it, you create a spiral. That twist is what we call Torsion. My theory says that what we perceive as "matter" is simply a place where the vacuum of space is rotating so tightly that it creates a "density core." To explain how this all works, we use a mathematical roadmap called a Lagrangian. Think of it as a master recipe or cookbook for the universe. It combines four key ingredients: 1. Electricity and Magnetism: How light and energy move. 2. Scalar Fields: The underlying "pressure" of the vacuum in space itself 3. Matter: The physical "stuff" we can touch. 4. Torsion: The "twist" or rotational force of space. By looking at the universe through this "helix" lens, we can solve two of the biggest headaches in modern science: The Hubble Tension - Astronomers are currently arguing over how fast the universe is expanding because different measurements give different answers. My theory suggests this "tension" exists because we haven't accounted for the universal rotation (torsion) affecting our measurements. The Dark Sector - We know there is "Dark Matter" and "Dark Energy" out there, but we can't find it. Helix Field Theory suggests these aren't invisible particles, but rather geometric artifacts - ripples and shadows created by the rotating vacuum itself. We are moving away from a universe of "things" and toward a universe of geometry and motion. If the vacuum of space is a structured, rotating medium, then we aren't just living in the universe - we are part of its physical rotation. The "Quantum Substratum" isn't just a theory; it’s a new way to understand the very "twist" of existence. - Protons: tiny rotating black hole-like cores anchoring the scalar field - Neutrons: stabilisers that prevent proton cores from decaying - Quarks & Gluons: the deepest torsion knots; the strong force is intrinsic torsion - Electrons: corkscrew-shaped solitons producing microscopic magnetic vortices - Neutrinos: ultra-light messenger waves traveling along the field’s “communication lines.” - Photons: instruction ripples traveling at light speed - Dark Photons: the “torsion messengers” of the Helix Field. They carry the twist, regulate the twist, and stabilize the twisting motion - W and Z bosons: on/off switches and stabilising nodes in the neutrino network - Higgs field: the local density of the scalar field, giving solitons their effective mass - Dark energy: the gentle outward push caused by the field’s overall rotation - Entropy: friction in that rotation, giving time its arrow - Cosmic Microwave Background: the universal “sustain pedal” like on a guitar or piano, keeping the field’s vibrations in phase. In this vision, dark matter isn’t missing matter - it’s the gravitational echo of the scalar field itself. Exploring antiparticles further: they may regulate the flow of time itself. In a rotational and torsional universe Time is a neutral observer: the past and future are fixed, but the present - our free will - is the point where choices echo into fate. Time is the “God” of the universe: ever-present, ever-aware, never interfering - just watching, as we decide which thread to follow.

Clinton Desveaux

23,492 views • 7 months ago

The Hidden Flow Inside Schrödinger’s Equation Once you define ρ = |ψ|² and differentiate it, Schrödinger equation rearranges into a continuity law, ∂ρ/∂t + ∇·j = 0, with j = (1/m)Im(ψ*∇ψ). Which means that probability is not just sitting there, it flows. Write ψ = r e^(iθ), and the current becomes j = (ρ/m)∇θ. So, the phase gradient is the steering field. When the phase winds by 2πn around a loop, the circulation is quantized, and the cores appear where ρ collapses so the phase can go undefined. In the animation, the ribbons trace that current, the color field shows phase, and the curls in the streamlines mark quantized vortex defects.

The Hidden Flow Inside Schrödinger’s Equation Once you define ρ = |ψ|² and differentiate it, Schrödinger equation rearranges into a continuity law, ∂ρ/∂t + ∇·j = 0, with j = (1/m)Im(ψ*∇ψ). Which means that probability is not just sitting there, it flows. Write ψ = r e^(iθ), and the current becomes j = (ρ/m)∇θ. So, the phase gradient is the steering field. When the phase winds by 2πn around a loop, the circulation is quantized, and the cores appear where ρ collapses so the phase can go undefined. In the animation, the ribbons trace that current, the color field shows phase, and the curls in the streamlines mark quantized vortex defects.

Mathelirium

26,511 views • 4 months ago

The basic idea behind "UFO physics" is very simple. We can get a strong "upward" force from a fast-spinning magnet (or magnetic flywheel), because it "pushes against space" like a spinning gyroscope. Very easy, if we apply a rotating magnetic field (3 or 5-phase) to that magnet! The problem is that such an "upward" force is accompanied by an equal and opposite "downward" force by Newton's 3rd Law. So we see an increase of gravitational potential, but no loss of total weight ("up" plus "down"), unless that spinning magnet goes into "free fall". How to solve this great problem? The E.T. crop artists have suggested (many times) that we should try to change that "downward" force into another kind of force, which does NOT follow Newton's 3rd Law: namely the Lorentz force of electromagnetism. As shown in a video below, added DC current makes a disc magnet spin rapidly in one direction (by the Lorentz force), while other thin wires which supply that DC current spin in an opposite direction. We can see right away, that the mass of that disc magnet is perhaps 100 times more than the mass of many thin wires which surround it below. Yet they spin in opposite directions at approximately the same speeds! This shows that spin angular momentum (m x v x r) is NOT conserved, due to a peculiar sideways action of the Lorentz force. Does everyone understand so far? In summary, if we can change the "downward" force, for an upward spinning-magnet, into a Lorentz force, then we should have NO real "downward" force, but only a force that goes "up"! So that will be my next experiment. I have had to order some specialized parts to make the trial apparatus correctly, but will try to do it in October, after all needed parts arrive. "The simple is great" (Lao Tzu) 🛸

The basic idea behind "UFO physics" is very simple. We can get a strong "upward" force from a fast-spinning magnet (or magnetic flywheel), because it "pushes against space" like a spinning gyroscope. Very easy, if we apply a rotating magnetic field (3 or 5-phase) to that magnet! The problem is that such an "upward" force is accompanied by an equal and opposite "downward" force by Newton's 3rd Law. So we see an increase of gravitational potential, but no loss of total weight ("up" plus "down"), unless that spinning magnet goes into "free fall". How to solve this great problem? The E.T. crop artists have suggested (many times) that we should try to change that "downward" force into another kind of force, which does NOT follow Newton's 3rd Law: namely the Lorentz force of electromagnetism. As shown in a video below, added DC current makes a disc magnet spin rapidly in one direction (by the Lorentz force), while other thin wires which supply that DC current spin in an opposite direction. We can see right away, that the mass of that disc magnet is perhaps 100 times more than the mass of many thin wires which surround it below. Yet they spin in opposite directions at approximately the same speeds! This shows that spin angular momentum (m x v x r) is NOT conserved, due to a peculiar sideways action of the Lorentz force. Does everyone understand so far? In summary, if we can change the "downward" force, for an upward spinning-magnet, into a Lorentz force, then we should have NO real "downward" force, but only a force that goes "up"! So that will be my next experiment. I have had to order some specialized parts to make the trial apparatus correctly, but will try to do it in October, after all needed parts arrive. "The simple is great" (Lao Tzu) 🛸

Red Collie (Dr. Horace Drew) scientist/inventor

29,769 views • 10 months ago

Some hitters constantly pull off the ball or get spinny. One reason could be related to Motor Shoulder. Every athlete has one shoulder that naturally sits slightly in front of the other. That shoulder often becomes the one that helps drive direction during rotation. In Motor Preferences we commonly see two patterns (with nuance): Back Motor Shoulder Keep the shoulders more in line with the pitcher so the back shoulder can work through and drive direction. Front Motor Shoulder Allow the athlete to load the front shoulder in so when rotation happens they can maintain direction through the middle of the field. The goal isn’t to force the same swing. It’s understanding the ranges of motion the athlete naturally organizes around and coaching toward them. We go deeper on Motor Shoulder and Motor Preferences in the Level 1 Baseball/Softball eCourse.

Some hitters constantly pull off the ball or get spinny. One reason could be related to Motor Shoulder. Every athlete has one shoulder that naturally sits slightly in front of the other. That shoulder often becomes the one that helps drive direction during rotation. In Motor Preferences we commonly see two patterns (with nuance): Back Motor Shoulder Keep the shoulders more in line with the pitcher so the back shoulder can work through and drive direction. Front Motor Shoulder Allow the athlete to load the front shoulder in so when rotation happens they can maintain direction through the middle of the field. The goal isn’t to force the same swing. It’s understanding the ranges of motion the athlete naturally organizes around and coaching toward them. We go deeper on Motor Shoulder and Motor Preferences in the Level 1 Baseball/Softball eCourse.

Motor Preferences Experts, LLC

11,224 views • 5 months ago

Normalize Working in Phase Space Ordinary space shows where the particle is. Phase space shows its complete state, position and momentum together, revealing the hidden geometry of its motion.

Normalize Working in Phase Space Ordinary space shows where the particle is. Phase space shows its complete state, position and momentum together, revealing the hidden geometry of its motion.

Mathelirium

103,032 views • 28 days ago

NEW PHYSICS! ANY "GENIUSES" OUT THERE WILL HAVE A CHANCE TO PROPOSE THE FIRST THEORY, TO EXPLAIN THESE NOVEL OBSERVATIONS. In many previous videos, I showed you how a permanent disc-magnet spins in the SAME direction as a 3-phase magnetic field (placed below), and rises up. What happens if we use an aluminum disc instead? By itself, an aluminum disc won't spin, because it has no internal magnetic field (which is needed to interact with the 3-phase field below). Yet if we add BOTH an aluminum disc, and also a large wire coil with AC power, then a magnetic field will be induced in that aluminum disc, and it becomes able to spin! The next question becomes: in which DIRECTION does the aluminum disc spin, with its induced magnetic field? Physics "geniuses", please watch this video to find out! Feel free to propose a new theory to explain these strange observations. We find that a large aluminum disc (100 mm diameter) spins clockwise, in the SAME sense as a rotating magnetic field below. Whereas a small aluminum disc (70 mm diameter) spins anti-clockwise, in an OPPOSITE sense to the rotating field below, Why has no one noticed this before? Mainstream physicists today just memorize old equations from textbooks, and could not discover "fleas on a dog".🤡 I suspect that these new data support a "vortex" theory of magnetism, but will let YOU decide! 😀

NEW PHYSICS! ANY "GENIUSES" OUT THERE WILL HAVE A CHANCE TO PROPOSE THE FIRST THEORY, TO EXPLAIN THESE NOVEL OBSERVATIONS. In many previous videos, I showed you how a permanent disc-magnet spins in the SAME direction as a 3-phase magnetic field (placed below), and rises up. What happens if we use an aluminum disc instead? By itself, an aluminum disc won't spin, because it has no internal magnetic field (which is needed to interact with the 3-phase field below). Yet if we add BOTH an aluminum disc, and also a large wire coil with AC power, then a magnetic field will be induced in that aluminum disc, and it becomes able to spin! The next question becomes: in which DIRECTION does the aluminum disc spin, with its induced magnetic field? Physics "geniuses", please watch this video to find out! Feel free to propose a new theory to explain these strange observations. We find that a large aluminum disc (100 mm diameter) spins clockwise, in the SAME sense as a rotating magnetic field below. Whereas a small aluminum disc (70 mm diameter) spins anti-clockwise, in an OPPOSITE sense to the rotating field below, Why has no one noticed this before? Mainstream physicists today just memorize old equations from textbooks, and could not discover "fleas on a dog".🤡 I suspect that these new data support a "vortex" theory of magnetism, but will let YOU decide! 😀

Red Collie (Dr. Horace Drew) scientist/inventor

26,727 views • 10 months ago

Final Lecture of our Statistical Mechanics Series. Lecture 2 showed how we move from the Full Phase-Space Density ρ(q₁, …, qₙ, p₁, …, pₙ, t) to smaller statistical objects by integrating out variables we do not want to keep. That gives reduced descriptions like the One-Particle Density f₁(q₁,p₁,t) and the Two-Particle Density f₂(q₁,p₁,q₂,p₂,t) This was the simplification. Now comes the catch. If the Full Density obeys Liouville’s Equation, the reduced densities do not evolve independently. The equation for one level depends on the next one and this is referred to as the BBGKY hierarchy. The One-Particle Density depends on the Two-Particle Density. The Two-Particle Density depends on the Three-Particle Density. And the chain keeps going. That happens because particles interact. Once one particle feels the rest, one-particle information is no longer enough. Correlations enter, and the lower level is fed from above. If the full Hamiltonian is H = Σᵢ pᵢ²/(2m) + Σᵢ U(qᵢ) + (1/2) Σᵢ Σⱼ≠ᵢ Φ(qᵢ − qⱼ) then reducing the full density does not make the interaction terms disappear. It leaves behind coupling to higher-order reduced densities. So, schematically, ∂f₁/∂t + transport of one particle = interaction term involving f₂ and more generally the heirarchy is such that ∂fₛ/∂t + s-particle transport = interaction term involving fₛ₊₁ Therefore, Lecture 3 is really about the price of reduction. We simplify the description, but the information we remove comes back as coupling to higher-order correlations. So, how do you actually compute anything if every level depends on the next one? This is the so-called Closure Problem. To make the hierarchy usable, you need an extra assumption that cuts the chain. You replace the exact higher-order object by an approximation in terms of lower-order ones. The most basic example is a factorized closure at the pair level, where the exact correlated Two-Particle Density is replaced schematically by a product of One-Particle Densities: f₂(q₁,p₁,q₂,p₂,t) ≈ f₁(q₁,p₁,t) f₁(q₂,p₂,t) That approximation is not exact. It throws away part of the correlation structure. But it gives you something the raw hierarchy does not... a closed equation for the lower-level description. That is why closure matters so much. Without it, the hierarchy is exact but open. With it, the theory becomes approximate but usable. Thus, the combined point of this final Statistical Mechanics post is simple. First, reduced descriptions are not closed because interactions generate correlations across levels. Second, if you want a workable Kinetic Theory, you must close the hierarchy by approximating those higher-order correlations. It is the bridge from formal many-body mechanics to equations people can actually solve. In the render, that is exactly the story you are seeing. The first part shows the hierarchy itself: one reduced level feeding the next, with lower descriptions inheriting structure from higher ones. The second part shows the closure step where the exact correlated pair level is replaced by a factorized ansatz, and that approximation gives back a closed one-particle description. That is, the animation moves from dependence to approximation, and from approximation to solvability. #StatisticalMechanics #BBGKY #ClosureProblem #KineticTheory #PhaseSpace #ReducedDistribution #HamiltonianMechanics #MathematicalPhysics #Mathematics #Physics

Final Lecture of our Statistical Mechanics Series. Lecture 2 showed how we move from the Full Phase-Space Density ρ(q₁, …, qₙ, p₁, …, pₙ, t) to smaller statistical objects by integrating out variables we do not want to keep. That gives reduced descriptions like the One-Particle Density f₁(q₁,p₁,t) and the Two-Particle Density f₂(q₁,p₁,q₂,p₂,t) This was the simplification. Now comes the catch. If the Full Density obeys Liouville’s Equation, the reduced densities do not evolve independently. The equation for one level depends on the next one and this is referred to as the BBGKY hierarchy. The One-Particle Density depends on the Two-Particle Density. The Two-Particle Density depends on the Three-Particle Density. And the chain keeps going. That happens because particles interact. Once one particle feels the rest, one-particle information is no longer enough. Correlations enter, and the lower level is fed from above. If the full Hamiltonian is H = Σᵢ pᵢ²/(2m) + Σᵢ U(qᵢ) + (1/2) Σᵢ Σⱼ≠ᵢ Φ(qᵢ − qⱼ) then reducing the full density does not make the interaction terms disappear. It leaves behind coupling to higher-order reduced densities. So, schematically, ∂f₁/∂t + transport of one particle = interaction term involving f₂ and more generally the heirarchy is such that ∂fₛ/∂t + s-particle transport = interaction term involving fₛ₊₁ Therefore, Lecture 3 is really about the price of reduction. We simplify the description, but the information we remove comes back as coupling to higher-order correlations. So, how do you actually compute anything if every level depends on the next one? This is the so-called Closure Problem. To make the hierarchy usable, you need an extra assumption that cuts the chain. You replace the exact higher-order object by an approximation in terms of lower-order ones. The most basic example is a factorized closure at the pair level, where the exact correlated Two-Particle Density is replaced schematically by a product of One-Particle Densities: f₂(q₁,p₁,q₂,p₂,t) ≈ f₁(q₁,p₁,t) f₁(q₂,p₂,t) That approximation is not exact. It throws away part of the correlation structure. But it gives you something the raw hierarchy does not... a closed equation for the lower-level description. That is why closure matters so much. Without it, the hierarchy is exact but open. With it, the theory becomes approximate but usable. Thus, the combined point of this final Statistical Mechanics post is simple. First, reduced descriptions are not closed because interactions generate correlations across levels. Second, if you want a workable Kinetic Theory, you must close the hierarchy by approximating those higher-order correlations. It is the bridge from formal many-body mechanics to equations people can actually solve. In the render, that is exactly the story you are seeing. The first part shows the hierarchy itself: one reduced level feeding the next, with lower descriptions inheriting structure from higher ones. The second part shows the closure step where the exact correlated pair level is replaced by a factorized ansatz, and that approximation gives back a closed one-particle description. That is, the animation moves from dependence to approximation, and from approximation to solvability. #StatisticalMechanics #BBGKY #ClosureProblem #KineticTheory #PhaseSpace #ReducedDistribution #HamiltonianMechanics #MathematicalPhysics #Mathematics #Physics

Mathelirium

10,970 views • 3 months ago