Adiabatic Process绝热过程
An adiabatic process is one in which no heat is gained or lost by the system. The first law of thermodynamics with Q=0 shows that all the change in internal energy is in the form of work done. This puts a constraint on the heat engine process leading to the adiabatic condition shown below. This condition can be used to derive the expression for the work done during an adiabatic process. 绝热过程是指系统不吸收或释放热量的过程。热力学第一定律中Q=0表明,内能的变化全部以做功的形式体现。这对热机过程施加了约束,导致下述的绝热条件。该条件可以用来推导绝热过程中所做的功的表达式。
![]() The ratio of the specific heats γ = CP/CV is a factor in determining the speed of sound in a gas and other adiabatic processes as well as this application to heat engines. This ratio γ = 1.66 for an ideal monoatomic gas and γ = 1.4 for air, which is predominantly a diatomic gas. 比热容比 γ = C_P / C_V 是确定气体中声速以及其它绝热过程的重要因素,也应用于热机。对于理想单原子气体,γ = 1.66;对于空气,γ = 1.4,因为空气主要由双原子气体组成。
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Adiabatic Process绝热过程
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Adiabatic Process绝热过程
(注意:如果初始压力值发生变化,那么将根据上述指定的初始体积和温度计算新的摩尔数。如果您希望限制摩尔数为所输入的值,则需输入该值以及初始体积和温度——所需的压强将被计算。)对于功的计算,指定的初始温度必须以开尔文为单位,因此必须从其他温度尺度转换而来。 中文译文中的待填/计算数值依次对应:1:gam 2:k 3:w 4:wb 5:wp 6:tf2 7:t2 8:tc 9:tf。实际数值以上方原输入框为准。 |
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