• So for the reversible process, the work done is the integral under the pressure volume state function, the function of state.

    对可逆过程,做的功,是压强体积态函数曲线下,的积分面积。

    麻省理工公开课 - 热力学与动力学课程节选

  • get back to the initial point is going to require some input from outside, like heat or extra work or extra heat or something because you've done an irreversible process.

    如果要逆转它,回到初始点,就需要外界的投入,比如额外的功,额外的热量等等,因为你进行了一个不可逆过程。

    麻省理工公开课 - 热力学与动力学课程节选

  • In that process there is a metabolic engine at work, and some people have an efficient engine so that the calories in get banked in the fat, other people have an inefficient engine, that is the calories get wasted as body heat and things like that, and they tend not to gain weight.

    这过程中人体内有个工作着的代谢引擎,有些人的代谢引擎效率很高,热量便转化为脂肪储存起来,另一些人的效率低下,能量就以体温等形式被浪费了,因此他们就不容易发胖

    耶鲁公开课 - 关于食物的心理学、生物学和政治学课程节选

  • When I flail my arms around I generate work and heat. This is not a constant volume process.

    这不是一个恒容过程,但如果我是一个系统,当我做这些的时候。

    麻省理工公开课 - 热力学与动力学课程节选

  • And we had the similar statement by Kelvin about the heat engine that required that some heat gets dumped into a cold reservoir in the process of converting the heat from the hot reservoir into work.

    相同的陈述,同样的有开尔文表述:,把热量完全从高温热源,转移至低温热源的过程中,必然有功的输出。

    麻省理工公开课 - 热力学与动力学课程节选

  • Anyway, the work associated with process number two is described by this box.

    好,刚才那个过程的功,由这个矩形描述。

    麻省理工公开课 - 热力学与动力学课程节选

  • There's no change in them, and then we also looked at some at non-state functions, work and heat, and saw that those aren't zero going around a cycle. Of course you can do work in a cyclic process, and heat can be exchanged with the environment at the same time.

    它们不会有变化,然后我们研究了,一些非态函数,功和热量,并看到,沿着循环行进一周的话,它们并不是零,当然你可以在,一个循环过程中做功,而同时热量可以在系统,与外界环境之间进行交换。

    麻省理工公开课 - 热力学与动力学课程节选

  • So w, the work is less for the irreversible process than the reversible process.

    不可逆过程中系统对外界,做的功要比可逆过程时小。

    麻省理工公开课 - 热力学与动力学课程节选

  • So, the work for this process is the integral, pdv or minus the integral, V1, V2, p dV.

    此过程中的做功等于负的积分,从v1到v2,外部。

    麻省理工公开课 - 热力学与动力学课程节选

  • If it's a reversible process, we know the work is the area under the curve.

    对可逆过程,功等于p-V图上。

    麻省理工公开课 - 热力学与动力学课程节选

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