Quote:
Originally Posted by zzzoak 1)
Consider gas at temperature T, wall at temperature T.
The impulse going to the wall is mv(T),
the impulse going from the wall is -mv(T).
The impulse difference is
mv(T)-(-mv(T))=2mv(T).
Number of particles going to the wall n~v(T).
Pressure p(T)~mv(T)^2
The first member of impulse gives to pressure p(T)/2 and the second also p(T)/2,
so total pressure is p(T).
2)
Consider gas at temperature T, wall at temperature T1, time t=0 s.
The impulse going to the wall is mv(T),
the impulse going from the wall is -mv(T1).
The impulse difference is mv(T)+mv(T1).
Number of particles going to the wall n~v(T).
Pressure p(T1)(t=0)~mv(T)^2+mv(T1)v(T)=(1+v(T1)/v(T))p(T)/2.
If T1>T the pressure is higher p(T1)>p(T).
While heating member v(T) tends to v(T1) and finally total pressure becomes ~2mv(T1)^2. |
That was very informative to me. I have a question though. In both cases (i.e. for T of the wall =T and T1>T), the impulse going to the wall is the same, namely mv(T) because the gas is at the same temperature. I understand the impulse difference is greater in the case the wall is hotter, but can you say that
the gas exerts more pressure onto the wall in the case the wall is at T1>T compared to T?
I believe so... Nice explanation.