- #1
lokofer
- 106
- 0
System with "big" number of particles..
Let's suppose we have a Hamiltonian of the form:
[tex] H(q_1 ,q_2 ,q_3,..., q_N , p_1,p_2 ,p_3 , ..., p_N ) \Phi (q_1 ,q_2 ,q_3,..., q_N) = E_{n} \Phi (q_1 ,q_2 ,q_3,..., q_N ) [/tex]
but the problem is that N is very "big" , let's say [tex] N \rightarrow \infty [/tex] , so to solve the Schrowedinguer equation becomes a very difficult task... is there a method to deal with this problem?...when you have for example a big number of particles inside a box (gas and similar) to solve SE and get the "Energies" and "Wave functions"?
Let's suppose we have a Hamiltonian of the form:
[tex] H(q_1 ,q_2 ,q_3,..., q_N , p_1,p_2 ,p_3 , ..., p_N ) \Phi (q_1 ,q_2 ,q_3,..., q_N) = E_{n} \Phi (q_1 ,q_2 ,q_3,..., q_N ) [/tex]
but the problem is that N is very "big" , let's say [tex] N \rightarrow \infty [/tex] , so to solve the Schrowedinguer equation becomes a very difficult task... is there a method to deal with this problem?...when you have for example a big number of particles inside a box (gas and similar) to solve SE and get the "Energies" and "Wave functions"?