00:07
Expansion isothermal expansion the temperature will be constant along this process after then second we have adiabetic expansion in adiabatic expansion the temperature of the function of v inverse v gamma inverse the temperature is the function of v gamma minus one hence in isothermal process i isothermal compression, which is ab, this one is b, c, after then is isothermal compression, which is cd.
01:05
The temperature will be constant along this process, temperature constant, after then 4.
01:13
We have adiabatic compression along d, a, the temperature is the function of b gamma minus 1.
01:29
Note that tb gamma minus 1, t b gamma minus 1 is constant in adiabatic process.
01:38
It's constant.
01:40
Now we can find the value of p which is constant upon b gamma minus 1.
01:53
Second, we can find the curve temperature in calvin b a here.
02:27
One is expansion, isothermal expansion, isothermal, process.
02:34
Second is extension adiabetic process...
