6 V O L . 1 3 , D O C . 3 8 2 a C A L C U L A T I O N S
Vol. 13, 382a. Calculations
[On board SS Kitano Maru, on or after 7 October
1922][1]
td )
δ(³2L
0 Bed δE 0 = =

·
λ--------¹
∂E
∂qν
–+
©
§ ·
δqν
·
λ--------¹
∂E
∂pν

©
§ ·
δpν + dt 0 =
Statistik σ Phasendichte Teilungen E'
invariant varirt. Dann

·
λ1--------
∂E'
∂qν
–=

·
λ1--------
∂E'
∂pν
=
∂E
∂pν
-------- λi©
∂E
∂qν
--------qν
·
--------pν¹·E∂∂pν
·
+
§
+
∂E
∂pν
--------
0
∂σpν
·
∂pν
------------
∂σqν
·
∂qν
------------ +

∂pν©
--------§
σλi∂qν¹
∂Ei
--------·


∂qν©
--------§
σλi∂pν¹·iE∂--------
+ = =
0
∂σλi
∂pν
------------------- -
∂Ei
∂qν

∂pν
-------------------iEi∂-∂σλ
∂pν
+ =
λiFunkt von E' allein
Dann reduziert sich Formel auf
λi------
dE
dt
- 0 =

·
λ--------
∂E
∂qν
–=

·
λ--------
∂E
∂pν
=
E konst =
Previous Page Next Page