• The whole thing's going to come to some new equilibrium temperature between the products and the oil or whatever's around it, and we're going to measure that.

    生成物和周围的油或,别的什么东西之间,达到某种新的平衡态,我们要测量的就是这个。

    麻省理工公开课 - 热力学与动力学课程节选

  • There's our condition for equilibrium at constant temperature and pressure.

    这就是我们在,恒定温度和压强下的平衡条件。

    麻省理工公开课 - 热力学与动力学课程节选

  • You could take a continuous path, where you have an infinite equilibrium points in between the two, a smooth path, whereyoudrop pressureand temperature simultaneosly in little increments.

    你可以选择光滑的连续路径,在初末态间有,无数个平衡态的点,压强和温度同时一点,一点地下降。

    麻省理工公开课 - 热力学与动力学课程节选

  • And the triple point of water is 16K that temperature and pressure - there's a unique temperature and pressure where water exists in equilibrium between the liquid phase, the vapor phase, and the solid phase.

    与水的三相点,我们定义它为273。,水的三相点,是一个特定的温度和压强,可以使水的液态,气态和固态三相共同达到平衡,三相点是液态。

    麻省理工公开课 - 热力学与动力学课程节选

  • If I look at different points in my container during that path, I'm going to have to use a different value of pressure or different value of temperature That's not an equilibrium state, and that process turns out then to be an irreversible process.

    如果我要研究在路径中容器里的,不同的点,我就得在容器里不同的点上使用,不同的压强值,或不同的温度值,实际上这不是个平衡态,这个过程是,不可逆过程。

    麻省理工公开课 - 热力学与动力学课程节选

  • pV Also A plus pV and G is minimized at equilibrium with constant temperature and pressure.

    同时等于亥姆赫兹自由能A加上,同时在恒定的温度和压强下。

    麻省理工公开课 - 热力学与动力学课程节选

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