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関連する概念動画

Phase Transitions: Vaporization and Condensation02:39

Phase Transitions: Vaporization and Condensation

The physical form of a substance changes on changing its temperature. For example, raising the temperature of a liquid causes the liquid to vaporize (convert into vapor). The process is called vaporization—a surface phenomenon. Vaporization occurs when the thermal motion of the molecules overcome the intermolecular forces, and the molecules (at the surface) escape into the gaseous state. When a liquid vaporizes in a closed container, gas molecules cannot escape. As these gas phase molecules...
Vapor Pressure02:34

Vapor Pressure

When a liquid vaporizes in a closed container, gas molecules cannot escape. As these gas phase molecules move randomly about, they will occasionally collide with the surface of the condensed phase, and in some cases, these collisions will result in the molecules re-entering the condensed phase. The change from the gas phase to the liquid is called condensation. When the rate of condensation becomes equal to the rate of vaporization, neither the amount of the liquid nor the amount of the vapor...
Enthalpy and Heat of Reaction02:12

Enthalpy and Heat of Reaction

Combustion, commonly known as burning, is a reaction in which a substance reacts with an oxidizing agent, which in most cases is molecular oxygen, to liberate energy in the form of heat, light, or sound. The heat of combustion is also known as the enthalpy of combustion. The energy released when one mole of a substance undergoes complete combustion at constant pressure is called molar heat of combustion. Combustion reactions are exothermic; that is, they release energy, and their ΔH sign...
Heat and Free Expansion01:24

Heat and Free Expansion

The work done by a thermodynamic system depends not only on the initial and final states but also on the intermediate states—that is, on the path. Like work, when heat is added to a thermodynamic system, it undergoes a change of state, and the state attained depends on the path from the initial state to the final state. Consider an ideal gas cylinder fitted with a piston. When the cylinder is heated at a constant temperature, the gas molecules absorb energy and expand slowly in a controlled...
The Joule and Joule–Thomson Experiments01:23

The Joule and Joule–Thomson Experiments

Consider an adiabatic system composed of two chambers, A and B, designed such that no heat flows into or out of the system. Initially, chamber A is filled with a gas at a fixed temperature T1, pressure p1, and volume V1, while chamber B is evacuated. The gas is then gradually forced through a rigid, porous barrier to chamber B, ultimately reaching temperature T2, pressure p2, and volume V2. A piston on the right side maintains a constant pressure (p2), which is lower than p1. The significant...
Perfect Gases and the First Law01:29

Perfect Gases and the First Law

A perfect gas obeys the equation of state pV = nRT. The internal energy of a perfect gas remains unaffected by volume alterations. Therefore, the internal energy of a perfect gas is solely dependent on temperature.Consider an ideal gas enclosed in a cylinder situated within a substantial constant-temperature bath. In an isothermal process, where the temperature remains constant, the change in internal energy equates to zero. Thus, according to the first law of thermodynamics, heat absorbed (q)...

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関連する実験動画

Updated: Jun 29, 2026

Laser-heating and Radiance Spectrometry for the Study of Nuclear Materials in Conditions Simulating a Nuclear Power Plant Accident
09:18

Laser-heating and Radiance Spectrometry for the Study of Nuclear Materials in Conditions Simulating a Nuclear Power Plant Accident

Published on: December 14, 2017

蒸気相爆発:基本的な爆発?

G R Fowles

    Science (New York, N.Y.)
    |April 13, 1979
    PubMed
    まとめ
    この要約は機械生成です。

    過熱した液体は,化学爆発物と同様の爆発を引き起こす可能性があります. 液体メタンは,過熱すると,かなりのエネルギーを放出し,液体蒸気爆発に関する新しい視点を提供します.

    さらに関連する動画

    Minimum Burning Pressures of Water-based Emulsion Explosives
    08:35

    Minimum Burning Pressures of Water-based Emulsion Explosives

    Published on: October 31, 2017

    Combustion Chemistry of Fuels: Quantitative Speciation Data Obtained from an Atmospheric High-temperature Flow Reactor with Coupled Molecular-beam Mass Spectrometer
    07:24

    Combustion Chemistry of Fuels: Quantitative Speciation Data Obtained from an Atmospheric High-temperature Flow Reactor with Coupled Molecular-beam Mass Spectrometer

    Published on: February 19, 2018

    関連する実験動画

    Last Updated: Jun 29, 2026

    Laser-heating and Radiance Spectrometry for the Study of Nuclear Materials in Conditions Simulating a Nuclear Power Plant Accident
    09:18

    Laser-heating and Radiance Spectrometry for the Study of Nuclear Materials in Conditions Simulating a Nuclear Power Plant Accident

    Published on: December 14, 2017

    Minimum Burning Pressures of Water-based Emulsion Explosives
    08:35

    Minimum Burning Pressures of Water-based Emulsion Explosives

    Published on: October 31, 2017

    Combustion Chemistry of Fuels: Quantitative Speciation Data Obtained from an Atmospheric High-temperature Flow Reactor with Coupled Molecular-beam Mass Spectrometer
    07:24

    Combustion Chemistry of Fuels: Quantitative Speciation Data Obtained from an Atmospheric High-temperature Flow Reactor with Coupled Molecular-beam Mass Spectrometer

    Published on: February 19, 2018

    科学分野:

    • 熱力学は熱力学である.
    • 物理化学 物理化学
    • 爆発科学とは,爆発の科学である.

    背景:

    • 液体蒸気爆発は一般的な現象です.
    • 発症と拡散のメカニズムは未だに十分に理解されていない.
    • 既存の理論は,これらの爆発的な出来事を完全に説明できません.

    研究 の 目的:

    • 超熱した液体が爆発を支える熱力学的可能性を調査する.
    • 化学爆発物と同様の液体蒸気爆発の可能性を調査する.
    • 超熱した液体メタンの爆発エネルギーを定量化するために.

    主な方法:

    • 超熱した液体の状態の熱力学分析.
    • 液体蒸気爆発エネルギーと化学爆発物の比較.
    • 超高温状態での液体メタンの実験的または理論的モデリング.

    主要な成果:

    • 熱力学は,過熱した液体が爆発を起こすことを可能にします.
    • 液体メタンは沸騰点より50K超熱すると,爆発的可能性を示します.
    • 超熱した液体メタンの計算された爆発エネルギーは,TNTの2-3%です.

    結論:

    • 超熱した液体は,爆発のための有効な熱力学的経路を示します.
    • 液体メタンは,これらの現象を理解するためのモデルシステムとして機能します.
    • 液体蒸気爆発の発生と拡散を完全に解明するには,さらなる研究が必要である.