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Ana Sayfaya Dön

before i forget this is a quick particle demonstration the first is a brap barrage you use for smaller farts and don't want to copy paste the same particle over and over. there's one fart every second the second is for huge farts. very huge farts that air out... show more

Shokiekins (COMM SLOTS: 3/3) 🐾

4,986 subscribers

35,655 görüntüleme • 1 yıl önce •via X (Twitter)

Anya Rossi• Live Now

Private livecam show

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NormHal HueMann profil fotoğrafı

NormHal HueMann1 yıl önce

Small toots that indicates the timer on the curry-shaped bomb in her system is tickin' down

she oneesan on my skunk til i kusai (heehee) profil fotoğrafı

she oneesan on my skunk til i kusai (heehee)1 yıl önce

erm oomf just dropped peak?

Birdy~ profil fotoğrafı

Birdy~1 yıl önce

Oomf needs to animate more often🥹

Strikerkb12 profil fotoğrafı

Strikerkb121 yıl önce

Nice work, love rapid fire farts

Homino profil fotoğrafı

Homino1 yıl önce

I freaking love it ~~~ 🥵🤤🥵🤤🥵🤤

Mango profil fotoğrafı

Mango1 yıl önce

Personally i would NOT stand behind her.....

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This is what happens when thinking about Trump consumes every second of your life. Don’t do this. If you do, you’ll turn into James Carville. Turn on the sound for 5 seconds, and it becomes undeniable that this man has completely lost his mind. He’s now yelling at Trump for “smelling [his] own farts” and to let Lindsey Graham smell them instead. “I want you to call Lindsey and be sure that he has the fart ringtone so he knows to get down to the White House quickly to get his nose up your ass and so you can fart in his face!” “Stop smelling your own farts, you son of a b*tch!” “That’s Lyndsey’s job.”

This is what happens when thinking about Trump consumes every second of your life. Don’t do this. If you do, you’ll turn into James Carville. Turn on the sound for 5 seconds, and it becomes undeniable that this man has completely lost his mind. He’s now yelling at Trump for “smelling [his] own farts” and to let Lindsey Graham smell them instead. “I want you to call Lindsey and be sure that he has the fart ringtone so he knows to get down to the White House quickly to get his nose up your ass and so you can fart in his face!” “Stop smelling your own farts, you son of a b*tch!” “That’s Lyndsey’s job.”

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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

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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

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FAMILY FIRST: VP Vance shares the joyful update that Second Lady Usha Vance is pregnant with their fourth child: "Every single one of those specific policy wins is about a simple fact — reinvesting in you and ensuring that your family has the same great shot at the American dream that I had. This is very personal to me." "Our wonderful second lady is pregnant with our fourth child and I'm very, very happy about that."

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The unconstitutional and archaic tax on the Second Amendment is one step closer to being a thing of the past.🔥 This is a HUGE victory for the gun community and a blow to the gun control agenda. THANK YOU to all members and supporters who helped us get this far.🙏

The unconstitutional and archaic tax on the Second Amendment is one step closer to being a thing of the past.🔥 This is a HUGE victory for the gun community and a blow to the gun control agenda. THANK YOU to all members and supporters who helped us get this far.🙏

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Another reason why my farts are so big - I hold them and build up pressure for one huge rip. This is me *not* holding them. Pressing record every time i felt one coming. This is in the span of about 45min. Now i try and sleep. Im still farting as i post this.

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Another reason why my farts are so big - I hold them and build up pressure for one huge rip. This is me not holding them. Pressing record every time i felt one coming. This is in the span of about 45min. Now i try and sleep. Im still farting as i post this.

⚠️ᴄᴏɴᴛᴇɴᴛꜱ ᴜɴᴅᴇʀ ᴘʀᴇꜱꜱᴜʀᴇ ⚠️

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Particle is not a "wave", particle is a "knight". In chess knight moves two squares vertically and one square horizontally, or two squares horizontally and one square vertically. Average behaviour for 1000 knights looks like normal distribution. In physics such behaviour is called "particle behaviour". At the same time if knight can move only two squares horizontally and one square vertically, average behaviour looks like a sequence of vertical lines. In physics such behaviour is called "wave behaviour". What I want to say is that particle does not have to be any kind of wave, does not have to pass through 2 slits for wave behaviour to appear.. Everything might be much simpler.. Particle algorithm can lead to different outcomes depending on conditions.

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Aryeh (R-Yay) ⏸️ ⏹️

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don't forget to help the timerangers wash v-rex together before the holidays are over (this is a very important scene)

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CW-FARTS/VOICE Pov- your date finds out your secret turn on~ (this is my first time uploading fart content, i know some of you aren't into that and that's ok but i have had a few request to post something lie this~! full video over you know where~! 🩵)

CW-FARTS/VOICE Pov- your date finds out your secret turn on~ (this is my first time uploading fart content, i know some of you aren't into that and that's ok but i have had a few request to post something lie this~! full video over you know where~! 🩵)

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Two videos. The first is a collection of the reactions to Trump's immigration policies during his first term. Spoiler alert. The phonies are using the same lines almost verbatim again during his second term. The second video is a look at the pain and suffering that Biden's immigration policies caused to migrants. Every single person who was crying and whining in the first video remained completely silent for the four years that this was going on. Spoiler alert. They will go back to being completely silent once a Democrat is back in the White House again. It's a shame that the country has to go through this game over and over again.

Two videos. The first is a collection of the reactions to Trump's immigration policies during his first term. Spoiler alert. The phonies are using the same lines almost verbatim again during his second term. The second video is a look at the pain and suffering that Biden's immigration policies caused to migrants. Every single person who was crying and whining in the first video remained completely silent for the four years that this was going on. Spoiler alert. They will go back to being completely silent once a Democrat is back in the White House again. It's a shame that the country has to go through this game over and over again.

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THE “GOD PARTICLE” THAT MAKES EVERYTHING HAVE MASS The Higgs boson is the tiny particle that gives all other particles their mass, and scientists chased it for decades. To find it, CERN built the Large Hadron Collider, a 17 mile underground ring that smashes protons together at crazy speeds. In 2012, two huge experiments finally spotted it, proving one of physics’ biggest theories. Source: glamour_physics

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