Confinement and Quantization: Part 1

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  • Опубліковано 19 вер 2011
  • Physics of Materials by Dr. Prathap Haridoss,Department of Metallurgical & Materials Engineering,IIT Madras. For more details on NPTEL visit nptel.iitm.ac.in
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КОМЕНТАРІ • 12

  • @wisanuboonrawd6689
    @wisanuboonrawd6689 8 років тому +2

    Great lecture. Very clear to understand from fundamental.

  • @newtonbarbosa2730
    @newtonbarbosa2730 5 років тому

    Congratulations Professor. Very nice class!!!

  • @MrMGA06
    @MrMGA06 11 років тому +2

    you are simply awesome... thanks.

  • @Ravikumar-dl5wg
    @Ravikumar-dl5wg 5 років тому

    Excellent analogy to explain Quantization in potential well

  • @dhanabalshanmugam7559
    @dhanabalshanmugam7559 Рік тому

    Fantastic explanation Professor!! Thank you!!!

  • @chaudry123
    @chaudry123 3 роки тому

    Absolutely awesome

  • @dilawarabbas1469
    @dilawarabbas1469 3 роки тому

    Outclass lecture

  • @MrSfchin
    @MrSfchin 7 років тому

    what constitutes a potential well in atoms ? and how to calculate the width of a potential well ?

    • @mrinmoymandal2695
      @mrinmoymandal2695 6 років тому

      soon fatt Chin follow quantum mechanics by H.C.Verma

  • @alokkumar3703
    @alokkumar3703 4 роки тому

    fermi energy is define at 0 k.but u r showing here for non zero temperature.how?
    at 0 k, there will not be any free e lectron .

    • @rajatkamboj230
      @rajatkamboj230 6 місяців тому

      The situation he is explaining is at 0 K.
      The nearly free electrons are filled up to fermi energy. Point to keep in mind is that at 0 K these nearly free electron are also freezed.

  • @mrinmoymandal2695
    @mrinmoymandal2695 6 років тому +1

    Proff.repeating one line again and again.. #**#