正在加载视频...

视频加载失败

加载此视频时出现问题。这可能是由于临时网络问题，或视频可能不可用。

Introducing: Ecliptica_Veil_Refrain Step into the latest marvel of #Trinity’s AI simulation universe: Ecliptica_Veil_Refrain. {"RENDERER_STATE":{"Nraymarch":64,"spp_per_frame":1,"max_spp":32,"show_bounds":false,"skyColor":[0,0,0],"sunColor":[0.5489273590657855,0.5489273590657855,0.5489273590657855],"sunPower":1.367144516090617,"sunLatitude":76.73485298771871,"sunLongitude":138.94571082309892,"colliderSpec":[0.6666666666666667,0.6013071895424837,0.6013071895424837],"colliderDiffuse":[0.06666666666666667,0.3607843137254902,0.8980392156862745],"colliderRoughness":0.341872424239417,"exposure":0.3664541543565143,"gamma":1.5549681231534773,"saturation":1.2470158685577861,"anisotropy":0.5438412313677659,"extinctionScale":-0.4726864204465695,"emissionScale":1.0281427174005486,"blackbodyEmission":-11.619147601146414,"TtoKelvin":0.9924693630221351},"SOLVER_STATE":{"timestep":1,"NprojSteps":16,"vorticity_scale":0.43671445160906175,"Nx":160,"Ny":160,"Nz":160,"max_timesteps":500,"expansion":0.1},"SIMULATION_STATE":{"gravity":0.029775985336981482,"buoyancy":0.009925328445660495,"radiationLoss":0.9970476559131248,"blast_height":0.13595000702148574,"blast_radius":0.1583940602227418,"blast_velocity":48.523827956562414,"blast_heat_flux":49.62664222830247,"animation_period":13.233771260880658,"dust_inflow_rate":4.962346815110676,"dust_absorption":[0.8980392156862745,0.5843137254901961,0.06274509803921569],"dust_scattering":[0.011764705882352941,0.011764705882352941,0.9372549019607843],"TtoKelvin":52.93508504352263},"CAMERA_STATE":{"pos":[428.5065222671221,231.18004269182862,-137.9063177523132],"tar":[95.47877293559753,48.26456077993378,85.76052711016654],"near":1,"far":20000},"GUI_STATE":{"visible":true},"EDITOR_STATE":{"common_glsl":"//////////////////////////////////////////////////////////////////////////////////////////////////////\n// Bind UI parameters to uniforms used in the various programs\n//////////////////////////////////////////////////////////////////////////////////////////////////////\n\n// \"Physics\"\nuniform float gravity; // {\"name\":\"gravity\", \t \"min\":0.0, \"max\":0.1, \"step\":0.001, \"default\":0.05}\nuniform float buoyancy; // {\"name\":\"buoyancy\", \"min\":0.0, \"max\":0.1, \"step\":0.001, \"default\":0.5}\nuniform float radiationLoss; // {\"name\":\"radiationLoss\", \"min\":0.9, \"max\":1.0, \"step\":0.01,... \"default\":0.999}\n\n// Blast geometry \nuniform float blast_height; // {\"name\":\"blast_height\", \"min\":0.1, \"max\":0.9, \"step\":0.001, \"default\":0.25}\nuniform float blast_radius; // {\"name\":\"blast_radius\", \"min\":0.0, \"max\":0.3, \"step\":0.001, \"default\":0.1}\nuniform float blast_velocity; // {\"name\":\"blast_velocity\", \"min\":0.0, \"max\":100.0, \"step\":0.1, \"default\":50.0}\nuniform float blast_heat_flux; // {\"name\":\"blast_heat_flux\", \"min\":0.0, \"max\":100.0, \"step\":1.0, \"default\":100.0}\nuniform float animation_period; // {\"name\":\"animation_period\", \"min\":0.0, \"max\":100.0, \"step\":1.0, \"default\":100.0}\n\n// Dust\nuniform float dust_inflow_rate; // {\"name\":\"dust_inflow_rate\", \"min\":0.0, \"max\":10.0, \"step\":0.01, \"default\":1.0}\nuniform vec3 dust_absorption; // {\"name\":\"dust_absorption\", \"default\":[0.5,0.5,0.5], \"scale\":1.0}\nuniform vec3 dust_scattering; // {\"name\":\"dust_scattering\", \"default\":[0.5,0.5,0.5], \"scale\":1.0}\n\n// Rendering\nuniform float TtoKelvin; // {\"name\":\"TtoKelvin\", \"min\":0.0, \"max\":300.0, \"step\":0.01, \"default\":10.0}\n\n/******************************************************/\n/* mandatory function /\n//\n\nfloat Tambient;\nfloat M_PI = 3.141592;\n\nvoid init()\n{\n\t// Any global constants defined here are available in all functions\n \tTambient = 1.0;\n}","initial_glsl":"///////////////////////////////////////////////////////////////////////////////////////////////////////\n// Specify the initial conditions for the simulation (velocity, temperature, and medium density/albedo)\n// at time 0.0 (if unspecified, all quantities default to zero).\n///////////////////////////////////////////////////////////////////////////////////////////////////////\n\n//\n/ mandatory function /\n//\n\nvoid initial_conditions(in vec3 wsP, // world space center of current voxel\n in vec3 L, in float dL, // world-space extents of grid, and voxel-size\n inout vec3 v, // initial velocity\n inout vec4 T, // initial temperature\n inout vec3 medium, // initial per-channel medium density (extinction)\n inout vec3 mediumAlbedo) // initial per-channel medium albedo\n{\n v = vec3(0.0);\n T = vec4(Tambient);\n medium = vec3(0.0);\n mediumAlbedo = vec3(0.0);\n}\n","inject_glsl":"//////////////////////////////////////////////////////////////////////////////////////////////////////\n// Update the velocity, temperature via either:\n// - specification of volumetric inflow/outflow rate due to sources/sinks (vInflow, Tinflow)\n// - modification in-place, i.e. Dirichlet boundary conditions (v, T)\n// Also specify the injected medium density inflow rate, and its scattering albedo.\n//////////////////////////////////////////////////////////////////////////////////////////////////////\n\n//\n/ mandatory function */\n/******************************************************/\n\nvoid inject(in vec3 wsP, // world space center of current voxel\n in float time, // time\n in vec3 L, in float dL, // world-space extents of grid, and voxel-size\n inout vec3 v, // modify velocity in-place (defaults to no change)\n inout vec3 vInflow, // velocity inflow rate (defaults to zero)\n inout vec4 T, // modify temperature in-place (defaults to no change)\n inout vec4 Tinflow, // temperature inflow rate (defaults to zero)\n inout vec3 mediumInflow, // medium density (extinction) inflow rate (defaults to zero)\n inout vec3 mediumAlbedo) // medium albedo\n{\n float phase = 0.05M_PItime/animation_period;\n vec3 blast_center = 0.5L + 0.5vec3(0.5L.xsin(13.0phase),\n 0.5L.ysin(17.0phase),\n 0.5L.zsin(19.0phase));\n \n vec3 dir = wsP - blast_center;\n float r = length(dir);\n dir /= r;\n float rt = r/(blast_radiusL.y);\n if (rt <= 1.0)\n {\n // Within blast radius: inject velocity and temperature\n float radial_falloff = max(0.0, 1.0 - rtrt(3.0 - 2.0rt));\n vInflow = dir blast_velocity * radial_falloff;\n Tinflow.r = blast_heat_flux * radial_falloff;\n\n \t// Also inject absorbing/scattering \"dust\"\n vec3 dust_extinction = dust_absorption + dust_scattering;\n mediumInflow = dust_extinction * dust_inflow_rate * radial_falloff;\n mediumAlbedo = dust_scattering / dust_extinction;\n }\n \telse\n \t{\n // Apply thermal relaxation due to \"radiation loss\" \n T.r *= radiationLoss;\n }\n}\n","influence_glsl":"//////////////////////////////////////////////////////////////////////////////////////////////////////\n// Apply any external forces to the fluid\n//////////////////////////////////////////////////////////////////////////////////////////////////////\n\n/******************************************************/\n/* mandatory function */\n/******************************************************/\n\nvec3 externalForces(in vec3 wsP, // world space center of current voxel\n in float time, // time\n in vec3 L, in float dL, // world-space extents of grid, and voxel-size\n in vec3 v, in float P, in vec4 T, // velocity, pressure, temperature at current voxel\n in vec3 medium) // medium density (extinction) at current voxel\n{\n // Boussinesq approximation (a la Fedkiw & Stam)\n float densityAvg = (medium.r + medium.g + medium.b)/3.0;\n float buoyancy_force = -densityAvggravity + buoyancy(T.r - Tambient);\n return vec3(0.0, buoyancy_force, 0.0);\n}","collide_glsl":"//////////////////////////////////////////////////////////////////////////////////////////////////////\n// Specify regions which contain impenetrable collider material\n//////////////////////////////////////////////////////////////////////////////////////////////////////\n\n/******************************************************/\n/* mandatory function /\n//\n\nfloat collisionSDF(in vec3 wsP, // world space center of current voxel\n in float time, // time\n in vec3 L, in float dL) // world-space extents of grid, and voxel-size\n{\n // Regions which are solid obstacles have SDF < 0.0\n return 1.0e6;\n}","render_glsl":"//////////////////////////////////////////////////////////////////////////////////////////////////////\n// Specify the fluid emission field \n//////////////////////////////////////////////////////////////////////////////////////////////////////\n\n// Approximate map from temperature in Kelvin to blackbody emiss\n// Valid from 1000 to 40000 K (and additionally 0 for pure full white)\nvec3 colorTemperatureToRGB(const in float temperature)\n{\n // Values from: \n mat3 m = (temperature <= 6500.0) ? mat3(vec3(0.0, -2902.1955373783176, -8257.7997278925690),\n\t vec3(0.0, 1669.5803561666639, 2575.2827530017594),\n\t vec3(1.0, 1.3302673723350029, 1.8993753891711275)) : \n\t \t\t\t\t\t\t\t\t mat3(vec3(1745.0425298314172, 1216.6168361476490, -8257.7997278925690),\n \t vec3(-2666.3474220535695, -2173.1012343082230, 2575.2827530017594),\n\t vec3(0.55995389139931482, 0.70381203140554553, 1.8993753891711275)); \n return mix(clamp(vec3(m[0] / (vec3(clamp(temperature, 1000.0, 40000.0)) + m[1]) + m[2]), vec3(0.0), vec3(1.0)), \n vec3(1.0), \n smoothstep(1000.0, 0.0, temperature));\n}\n\n\n//\n/ mandatory functions */\n/******************************************************/\n\n// Specify how the temperature is mapped to the local emission radiance\nvec3 temperatureToEmission(in vec4 T)\n{\n vec3 emission = colorTemperatureToRGB(T.r * TtoKelvin) * pow(T.r/100.0, 4.0);\n \treturn emission;\n}\n\n// Optionally remap the medium density (extinction) and albedo\nvoid mediumRemap(inout vec3 medium,\n inout vec3 mediumAlbedo)\n{}\n\n// Specify the phase function of the scattering medium\nfloat phaseFunction(float mu, // cosine of angle between incident and scattered ray\n float anisotropy) // anisotropy coefficient\n{\n const float pi = 3.141592653589793;\n float g = anisotropy;\n float gSqr = gg;\n return (1.0/(4.0pi)) * (1.0 - gSqr) / pow(1.0 - 2.0gmu + gSqr, 1.5);\n}\n"}}show more

$TRINiTY

1,309 subscribers

19,625 次观看 • 1 年前 •via X (Twitter)

游戏科学技术教育 #Trinity

Anya Rossi• Live Now

Private livecam show

10 条评论

Prim 的头像

Prim1 年前

Same guys as on Cyborgism, take a look at their chart on what's next ;) Stay safe fam

Tyler Seregely 的头像

Tyler Seregely1 年前

Scam chart because the insiders buy and manipulate to make higher lows to fool you and then eventually cash everything out. Scammers need investigated by @FBI

Kamal 的头像

Kamal1 年前

When will launch in Coin Market Cap?

SAMMY ARTIST 的头像

SAMMY ARTIST1 年前

@Trinitytoken_AI I have been following your project for a while on space and I will love to connect with you. Can I know when we can discuss?

Gero Seratto 的头像

Gero Seratto1 年前

This is mi nd-blowing! Shoot me a DM so we can discuss further! 📨

Vixo ⛩️ 的头像

Vixo ⛩️1 年前

I love this 🧡 Let’s collab 🤝 DM me 💌

𝙂𝙀𝙈𝙎💎𝙋𝙍𝙊𝙈𝙊 𝙈𝘼𝙎𝙏𝙀𝙍 的头像

𝙂𝙀𝙈𝙎💎𝙋𝙍𝙊𝙈𝙊 𝙈𝘼𝙎𝙏𝙀𝙍1 年前

Hi, let's go big 🚀🚀 DM me for collaboration

M2thaK 的头像

M2thaK1 年前

hmu fam

Majime Tanaka 🏯 的头像

Majime Tanaka 🏯1 年前

Your project looks promising! 👌🏻

Alvin Eth 的头像

Alvin Eth1 年前

Hey there, contact me to set up a marketing plan. 🔥

相关视频

Thanks for 20k! vec3 p,c;for(float i,z,d,n=6.5*PI*(1.-cos(t*.2));max(i++,z/n)<1e2;o+=(cos(dot(sin(c/=19.),cos(c.yzx))*9.+vec4(0,.6,1,3)+t)+1.)/(2e2+.1*d*d))z+=d=length(sin(c=clamp(p=(z*(FC.rgb*2.-r.xyy)/r.y+vec3(0,0,n)/.4)*rotate3D(n/3e1,c/c),-n,n))+p-c)-.5;

Thanks for 20k! vec3 p,c;for(float i,z,d,n=6.5PI(1.-cos(t.2));max(i++,z/n)<1e2;o+=(cos(dot(sin(c/=19.),cos(c.yzx))9.+vec4(0,.6,1,3)+t)+1.)/(2e2+.1dd))z+=d=length(sin(c=clamp(p=(z(FC.rgb2.-r.xyy)/r.y+vec3(0,0,n)/.4)*rotate3D(n/3e1,c/c),-n,n))+p-c)-.5;

Xor

22,276 次观看 • 1 年前

for(float i,k,j,g,e,s,n=15.;i++<1e2;o.rgb+=hsv(s=log(s)/n,.5,s/2e2*k)+FC.zww*g*k/6e4){vec3 q,p=vec3((FC.xy-.5*r)/r.y*g-9.,g)+n;p.zx*=rotate2D(t/n);s=j=3.;k=s+snoise3D(vec3(p.xz*.1,t));for(q=p;j++<23.;p=vec3(0,4,-1)-abs(abs(p)*e-vec3(3,4,3)))s*=e=n/dot(p,p);g+=min(30.-q.y,p.y/s);}

for(float i,k,j,g,e,s,n=15.;i++<1e2;o.rgb+=hsv(s=log(s)/n,.5,s/2e2k)+FC.zwwg*k/6e4){vec3 q,p=vec3((FC.xy-.5r)/r.yg-9.,g)+n;p.zx=rotate2D(t/n);s=j=3.;k=s+snoise3D(vec3(p.xz.1,t));for(q=p;j++<23.;p=vec3(0,4,-1)-abs(abs(p)e-vec3(3,4,3)))s=e=n/dot(p,p);g+=min(30.-q.y,p.y/s);}

yonatan

100,369 次观看 • 1 年前

//#つぶやきProcessing float n=1,t,r; void setup(){ size(800,800); } void draw(){ background(0); stroke(255,255-t*2,255-t*5,256-t*3); translate(400,400); for(r=0;r<TAU;r+=PI/n) line(n*sin(r*t),n*cos(r*t),(400-n)*sin(r),(400-n)*cos(r)); t+=.05; n+=.5; }

//#つぶやきProcessing float n=1,t,r; void setup(){ size(800,800); } void draw(){ background(0); stroke(255,255-t2,255-t5,256-t3); translate(400,400); for(r=0;r<TAU;r+=PI/n) line(nsin(rt),ncos(rt),(400-n)sin(r),(400-n)*cos(r)); t+=.05; n+=.5; }

ひさだん

41,372 次观看 • 11 个月前

🐻‍❄️: J A S O N N N N N N N N N N N !!!!!!!!!!!! #f0rsakeN #t3xture [ขออนุญาตโควทคั้บ]

🐻‍❄️: J A S O N N N N N N N N N N N !!!!!!!!!!!! #f0rsakeN #t3xture [ขออนุญาตโควทคั้บ]

kiwi

121,138 次观看 • 1 年前

Hey World Mobile, how's this for a math problem? 1000 + E + N + N + F + T + S = M 1 N T 1 N G / N 0 W 🙃 $WMT #WorldMobile #ENNFT #CardanoCommunity #Cardano #NFT #NFTCommunity

Hey World Mobile, how's this for a math problem? 1000 + E + N + N + F + T + S = M 1 N T 1 N G / N 0 W 🙃 $WMT #WorldMobile #ENNFT #CardanoCommunity #Cardano #NFT #NFTCommunity

World Mobile Chain

25,558 次观看 • 3 年前

A N A T I O N I S N O T A N I D E A

A N A T I O N I S N O T A N I D E A

National Revival

228,134 次观看 • 1 年前

K A F T A N C O N N E C T 🇳🇬

K A F T A N C O N N E C T 🇳🇬

kc

298,715 次观看 • 5 个月前

g ö n l ü n ü g ü n e d e n i s e v m e z s e v d a i s t e r h e p o n u ü z e n i

g ö n l ü n ü g ü n e d e n i s e v m e z s e v d a i s t e r h e p o n u ü z e n i

nerde o eski şarkılar

524,092 次观看 • 3 年前

I N C A N T A T I O N REZZ x FKNSYD Friday.

I N C A N T A T I O N REZZ x FKNSYD Friday.

RΞZZ

29,732 次观看 • 10 个月前

S E N H ANT I R L A M A Z S I N B E N U N U T M A M

S E N H ANT I R L A M A Z S I N B E N U N U T M A M

No Context Hayat Bilgisi

28,298 次观看 • 3 年前

K O N S A N T R A S Y O N #AslanGibiSavaş

K O N S A N T R A S Y O N #AslanGibiSavaş

Galatasaray MCT Technic

12,571 次观看 • 8 个月前

$float2 n,q,u=float2(i.uv-.5); float d = dot(u,u),s=9,t=_Time.y,o,j; for (float2x2 m=RM2D(5);j++<16;) { u = mul(m,u);n = mul(m,n); q = u*s+t*4+sin(t*4-d*6)*0.8+j+n; o += dot(cos(q)/s, float2(2,2)); n -= sin(q); s *= 1.2; } return o; #Unity3D #GLSL #VFXFriday$

float2 n,q,u=float2(i.uv-.5); float d = dot(u,u),s=9,t=_Time.y,o,j; for (float2x2 m=RM2D(5);j++<16;) { u = mul(m,u);n = mul(m,n); q = us+t4+sin(t4-d6)0.8+j+n; o += dot(cos(q)/s, float2(2,2)); n -= sin(q); s = 1.2; } return o; #Unity3D #GLSL #VFXFriday

Mirza Beig

627,146 次观看 • 3 年前

$Ex-CERN QUANT applied quantum mechanics to the oil market on Polymarket He trades exclusively oil and made $226K in a week His Harmonic Oscillators model sees structure in the chaos: â†|n⟩ = √(n+1)|n+1⟩ -- growth â|n⟩ = √n|n-1⟩ -- decline Eₙ = ℏω(n + ½) -- energy level N̂|n⟩ = n|n⟩ -- particle number Price discretization: n(t) = ⌊(Rₜ - R_min)/ΔR · (N_L - 1)⌋ Rₜ = Σ r̃_τ/σ Market events: âₜ† = 1_{Δnₜ>0} · |Δnₜ| → buy âₜ = 1_{Δnₜ<0} · |Δnₜ| → sell Result: probability density of the next move: P(n,t) = 1/W · Σ δₙ,ₙτ Oil volatility for everyone is risk, for him it's a signal Check his profile:$

Ex-CERN QUANT applied quantum mechanics to the oil market on Polymarket He trades exclusively oil and made $226K in a week His Harmonic Oscillators model sees structure in the chaos: â†|n⟩ = √(n+1)|n+1⟩ -- growth â|n⟩ = √n|n-1⟩ -- decline Eₙ = ℏω(n + ½) -- energy level N̂|n⟩ = n|n⟩ -- particle number Price discretization: n(t) = ⌊(Rₜ - R_min)/ΔR · (N_L - 1)⌋ Rₜ = Σ r̃_τ/σ Market events: âₜ† = 1_{Δnₜ>0} · |Δnₜ| → buy âₜ = 1_{Δnₜ<0} · |Δnₜ| → sell Result: probability density of the next move: P(n,t) = 1/W · Σ δₙ,ₙτ Oil volatility for everyone is risk, for him it's a signal Check his profile:

sopersone

65,045 次观看 • 2 个月前

🗣️ K O N S A N T R A S Y O N ! #ERZvŞAN

🗣️ K O N S A N T R A S Y O N ! #ERZvŞAN

Erzurumspor FK

14,010 次观看 • 2 年前

S A N A Ç A T L A R C A S I N A İ N A N I Y O R U M

Sensitive content

S A N A Ç A T L A R C A S I N A İ N A N I Y O R U M

B. Eren Savaş

88,986 次观看 • 1 年前