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[
{
"slide": 1,
"fragments": [
{
"fragment_index": -1,
"text_description": "Kinetic Theory of Gases\nWhere restless particles shape every puff of air.",
"image_description": ""
}
]
},
{
"slide": 2,
"fragments": [
{
"fragment_index": 1,
"text_description": "What is Kinetic Theory?",
"image_description": ""
},
{
"fragment_index": 2,
"text_description": "Kinetic Theory",
"image_description": ""
},
{
"fragment_index": 3,
"text_description": "A gas is a swarm of tiny particles in nonstop, random, straight-line motion. Their collisions with container walls produce the observed gas pressure.",
"image_description": ""
},
{
"fragment_index": 4,
"text_description": "Quick check → Gas pressure arises from: (A) gravity, (B) particle collisions, or (C) magnetic forces?",
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}
]
},
{
"slide": 3,
"fragments": [
{
"fragment_index": -1,
"text_description": "Ideal Gas Model",
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{
"fragment_index": 1,
"text_description": "Ideal Gas\nA theoretical gas whose molecules have zero size and interact only through perfectly elastic collisions.\nKey Assumptions:\nMolecules are point particles; their own volume is negligible.\nNo attractive or repulsive forces except during impact.\nCollisions are perfectly elastic, conserving kinetic energy.\nA large number of molecules move randomly in all directions.",
"image_description": ""
}
]
},
{
"slide": 4,
"fragments": [
{
"fragment_index": -1,
"text_description": "How Pressure Happens",
"image_description": ""
},
{
"fragment_index": 0,
"text_description": "Follow one molecule, then many, to see pressure grow.",
"image_description": ""
},
{
"fragment_index": 1,
"text_description": "1\nOne Hit\nA single molecule strikes the wall and gives it a tiny push.",
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},
{
"fragment_index": 2,
"text_description": "2\nMillions of Hits\nCountless molecules collide each second; their pushes add together.",
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},
{
"fragment_index": 3,
"text_description": "3\nForce on Wall\nAll impulses merge into a steady force \\(F\\) pressing outward.",
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},
{
"fragment_index": 4,
"text_description": "4\nForce Becomes Pressure\nPressure forms: \\(P = \\\\frac{F}{A}\\\\). Faster motion or more particles raises \\(F\\) and so \\(P\\).",
"image_description": ""
},
{
"fragment_index": 5,
"text_description": "Pro Tip:\nPressure equals the combined momentum change delivered during molecular collisions.",
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}
]
},
{
"slide": 5,
"fragments": [
{
"fragment_index": -1,
"text_description": "Energy ∝ Temperature",
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},
{
"fragment_index": 1,
"text_description": "",
"image_description": "https://asset.sparkl.ac/pb/sparkl-vector-images/img_ncert/kys3FAXTPg2OQResr82DFFdEFuzzd7lgAfhNycDL.png"
},
{
"fragment_index": 2,
"text_description": "Average kinetic energy rises linearly with absolute temperature.\nIn an ideal gas, each molecule’s kinetic energy increases directly as the Kelvin temperature increases.",
"image_description": ""
},
{
"fragment_index": 3,
"text_description": "Key Points:\n\\( \\langle E_k \\rangle = \\frac{3}{2}k_B T \\)\nDouble \\(T\\) → double average kinetic energy.\nStraight-line graph passes through the origin; slope \\( \\frac{3}{2}k_B \\).",
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}
]
},
{
"slide": 6,
"fragments": []
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{
"slide": 7,
"fragments": [
{
"fragment_index": -1,
"text_description": "Key Takeaways",
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{
"fragment_index": 1,
"text_description": "Particles in constant motion\nGas molecules move randomly at every instant.",
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},
{
"fragment_index": 2,
"text_description": "Pressure from wall impacts\nEach molecular hit on the container wall exerts force, producing pressure.",
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},
{
"fragment_index": 3,
"text_description": "Ideal-gas model\nWe treat molecules as non-interacting points to simplify theory.",
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},
{
"fragment_index": 4,
"text_description": "Energy ↔ temperature\nAverage kinetic energy is directly proportional to absolute temperature, \\(E_k \\propto T\\).",
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}
]
}
]