Відео

Love this info, amazing resource and available for *free!* Thank you!!

Very nice summary presentation. A few minor critiques: 1. When discussing batching the at atmospheric conditions present above the glass melt should also be considered. For instance organic fuels can be a source of redox, contamination in fuel sources can enter the glass melt, and oxygen or hyderogen combustion can even infulence glass forming with generation of non-bridged oxygens. 2.When discussing gaseous defects sources such as refractory transperated gases/reactions or electochemical reactions with electrodes can generate seeds/blisters as well. 3.When discussing melting and fining the assumtion standard pressure is made in this presentation, this is rarely the case. Positive pressure in melting or negative pressure in fining can have a major influence. Small critiques overall but as a broad brief overview this is an excellent presentation. Looking forward to more similar content.

Amazing lecture

Perfect!

REAL💥💥🔥🔥

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very generous of you to upload this I just watched your series on crystallization which was absolutely amazing.

Fantastic John! Onward and upward!

Well-potential glass explorations 🔍Impact Research@John Mauro # great to see you💦💨🥳

Sir all your videos is useful to me I studying MSc physics in india and I am indian. my seminar topic is vitreous silica and sio2 glasses that's why I watched many times to understand the concept however done my seminar last week thank you thankyou so much sir...

Great lecture. Loved the Jurassic Park reference 😊

As a trained Glassblower, i really enjoyed this video :)

At 17:29 FQ the affinity associated with internal energy is defined to be 1/T. Later at 24:30 FQ is given as d/dx(1/T). Why are these different?

Thank you Professor! Great content!

Found this lecture a bit more hard going. Pair distribution function is a new concept to me though so I will need to read a bit more around that I think

Thank you very much, professor.

Nicely done!

Dear Prof Mauro, thanks for making these wonderful videos available. They go so perfectly with your excellent book. I was wondering for multicomponent systems, such as binary glasses, would we solve the constraint equation independently for each locally rigid structural unit (former) to get the relative proportions? Thanks again.

what a wonderful world!! i'm really honor to your lecture. from KOREA

Thank you for the great lecture, professor!

@29:55 correction: amorphous silicon is a very small fraction of the PV market. The vast majority is crystalline silicon

@29:55 correction: amorphous silicon is a very small fraction of the PV market. The vast majority is crystalline silicon

How did I not know you were doing this?? Excited for class 😎🎉

Dr. Mauro makes Glassy States FUN! yay💖

Thanks a lot for the really interesting lectures. I was just wondering if we can have access to the slides?

Very well explained. Thanks for sharing.

Thank you so much for this series! I find these topics to be ones that always benefit from reviewing regularly and these videos are invaluable for brushing up on a lot of these concepts!

Babe, wake up! Part two of the glass lecture dropped.

Thank you, Professor, for all your invaluable efforts.

Great news! I'm excited that you'll be lecturing on the glass book, just like you did with the kinetics book. Fantastic!

People with trypophobia might have difficulty with the cover page.

Congratulations professor John Mauro for this great opportunity to study glass science!

thank you for your lecture professor

Just like Boltzmann you are also a great teacher.

What I dont understand is how you compute the w_{\apha \beta} in applications, if you requere to now what you are looking for in the first place (that is f_{\apha} the probability )

The transition between metabasins w_{\alpha \beta} depend on the probability of the metabasin f_{\alpha} wich depend on time t. Then how this simplifies the problem if now you have coeffcients which depend on time? we start with transition that not depend on time (for temperature T constant)

My paper was just rejected by JAcerS, can I resubmit it, professor?

Lord❤❤❤❤❤❤❤

Thanks Dr. Mauro. The video lectures have been a great help.

Beautiful god again❤❤❤

I love birds are happy about the eclipse for they are singing away!!!!❤❤❤❤❤😊😊😊😊😊😊😊

Thank you for the excellent lecture; it was very informative. You mentioned non-viscous relaxation; is it possible to delay Beta relaxation? For instance, regarding gorilla glass, I understood from your discussion that excluding potassium from the parent glass composition is advantageous, suggesting that managing secondary relaxation largely involves compositional adjustments.

So useful lecture, Dr. Mauro. Thank you

Thank you for this amazing advice!

This is really good stuff John. For those looking to publish - this is very concise and well stated.

What an amazing summary! Professor, Do you have time to create a video presentation on the applications of AI and machine learning in materials research?😁

Thank you for the insightful lecture. I don't know if this is a suitable place to ask this question, but I hope so. you have mentioned the importance of the interior tension, and I am curious about the possibilities of manipulating or engineering the central tension. Is there an approach to achieving this? Additionally, the depiction of central tension as a straight line in figure 12.5 prompts me to ask whether this representation is exclusive. Can central tension adopt different shapes, perhaps akin to what I would describe as a "cat head-like shape"? I mean, doesn't it reach its peak immediately following the transition from compression to tension?

I sincerely appreciate your efforts and thank you for the lectures.

It is another great lecture from a nice book! Congratulations professor John Mauro🎉!

Thanks for uploading the amazing lecture!