Fistum 5-schoedinger

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Fistum 5-schoedinger

Pertemuan 5 Fisika Kuantum Bab V Persamaan Schrödinger Bambang Heru Iswanto, Dr.rer.nat M.Si ,[object Object],[object Object]

Latar Belakang ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

Persamaan Schrödinger ,[object Object],[object Object],PERSAMAAN SCHROEDINGER 10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

Struktur matematis pers. Schrödinger ,[object Object],[object Object],[object Object],[object Object],10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

Perubahan Nilai Harap Terhadap Waktu 10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

[object Object],10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

Rapat Arus Peluang 10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

Persamaan Schrödinger Bebas Waktu Ini solusi pers. Schoedinger bebas waktu, yakni jika V = V(x ) Disebut fungsi gelombang stasioner Dimana P tidak bergantung waktu dan  E=0 10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

[object Object],[object Object],[object Object],Keadaan Stasioner 10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

Persamaan Fungsi Eigen ,[object Object],[object Object],[object Object],10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

TERIMA KASIH 10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

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Fistum 5-schoedinger

1.

2.

3.

4.

5. Perubahan Nilai Harap Terhadap Waktu 10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

6.

7. Rapat Arus Peluang 10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

8. Persamaan Schrödinger Bebas Waktu Ini solusi pers. Schoedinger bebas waktu, yakni jika V = V(x ) Disebut fungsi gelombang stasioner Dimana P tidak bergantung waktu dan  E=0 10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |

9.

10.

11. TERIMA KASIH 10/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |