7.1 | MSE104 - Diffusion, Nucleation and Growth

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  • Опубликовано: 2 авг 2024
  • Lecture 7. Diffusion and homogenisation. Nucleation and growth of precipitates - the nucleation energy barrier.
    Course webpage with notes: dyedavid.com/mse104
    Lecturer: Dr David Dye.
    Licence: Creative Commons
    Department of Materials, Imperial College, London, UK

Комментарии • 24

  • @mcleanb981
    @mcleanb981 2 года назад +3

    Im in my final semester of my program, and this is the first time I've ever received a good lecture on this. Your lectures are fantastic and your students are lucky to have you.

  • @sdanielmcarthur8613
    @sdanielmcarthur8613 Год назад

    Amazing explanation, understood the concept clearly. Loved it!

  • @PersonWeird
    @PersonWeird 6 лет назад +2

    This video saved my life thank you so much you're a great teacher!

  • @MoeMoeStudio
    @MoeMoeStudio 6 лет назад +2

    How can you not like this guy??

  • @alexandernellessen4398
    @alexandernellessen4398 3 года назад

    simply love listening to you...

  • @simonepujatti4414
    @simonepujatti4414 7 лет назад +1

    A quick remark: in the Arrhenius expression of diffusivity D=Do*exp(-Q/RT), Do is not the diffusivity at the absolute 0, it is instead the maximum diffusivity that you obtain when temperature approaches an infinite value

  • @Selma-im9er
    @Selma-im9er 2 года назад

    you video saved my semester

  • @moyovelaphi8031
    @moyovelaphi8031 7 лет назад +4

    may we please have some lectures , we really like the methodology used .....proudly NUST students

  • @GaDaoud
    @GaDaoud 11 лет назад

    Thank you so much!

  • @gsmysteries223
    @gsmysteries223 4 года назад

    Thank u sir for making me clear🙏

  • @laughtale1181
    @laughtale1181 7 лет назад

    thank u really helped

  • @icocryptocurrencyvn.videos1564
    @icocryptocurrencyvn.videos1564 9 лет назад +1

    very good explanation...

  • @yjasper8411
    @yjasper8411 6 лет назад +1

    you explained that so much better than my professor :(

  • @bksaif
    @bksaif 11 лет назад

    In 28.18 and 28.27, Prof. Dye actually means to say w* goes up -- not down.

  • @keremkansu4756
    @keremkansu4756 6 лет назад +1

    hocam sizi allah gonderdi sevgileerr love from turkey

  • @yuangfu5023
    @yuangfu5023 6 лет назад

    is there a mistake in this video that the added strain energy should increase the W* rather than decrease?

  • @noondonporn9710
    @noondonporn9710 5 лет назад

    Your lecture is so good. I want to study master degree with you

  • @bksaif
    @bksaif 11 лет назад

    In 5.43, l_ave ~ sqrt(D*t)..... Isn't D that depends on the jump or frequency rate, and not t ?

  • @iPlayZone
    @iPlayZone 10 лет назад +1

    W = + 4/3*pi*r³*delta_G_v+4*pi*r²*sigma, Delta_G_v = G_solid - G_liquid < 0 hence negative! Also r* = - 2*sigma/delta_G_v. W* is right, but only because you copied the right answer :D.

  • @nagoenes
    @nagoenes 5 лет назад

    Why is gas constant here? There is nothing about gases but it appears in equations anyway.

  • @sunilgavade2293
    @sunilgavade2293 3 года назад

    Steel Making process

  • @burcmm
    @burcmm 10 лет назад

    Actually, does not strain energy add to the total nucleus energy? Then this will make the stabilization of a nucleus even more difficult, yielding a larger critical radius (with the assumption that all the strain energy is accumulated in the nucleus). Thanks.

  • @moyovelaphi8031
    @moyovelaphi8031 7 лет назад

    *more*