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|
| Line 3: |
Line 3: |
| <math> | | <math> |
| \mathcal{L} = \sum{i=1}^{N} \frac{m_{i}}{2} s^{2} \bold{r}_{i}^{2}. | | \mathcal{L} = \sum{i=1}^{N} \frac{m_{i}}{2} s^{2} \bold{r}_{i}^{2}. |
| | </math> |
| | |
| | <math> |
| | 5+3=4. |
| </math> | | </math> |
|
| |
|
Revision as of 14:15, 29 May 2019
In the approach by Nosé and Hoover[1][2][3] an extra degree of freedom is introduced in the Hamiltonian. The heat bath is considered as an integral part of the system and has a fictious coordinate 
which is introduced into the Lagrangian of the system. This Lagrangian for an 
is written as
References
