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Kelvin Xie MSEN TAMU
Добавлен 15 май 2019
My name is Kelvin Xie and I am an Assistant Professor in the Department of Materials Science and Engineering at the Texas A&M University.
I am using this channel to share some of my teaching materials with students and other researchers who are interested in microscopy and materials science.
I am using this channel to share some of my teaching materials with students and other researchers who are interested in microscopy and materials science.
Eli Norris - Unsupervised learning-aided extrapolation for accelerated design of superalloys
The paper was published by Liao, et al. in njp Computational Materials (2024)
Просмотров: 46
Видео
High strain rate indentation response of NiCoV equi-atomic medium entropy alloy (TMS 2024)
Просмотров 12728 дней назад
The work was supported by ARO. The slides were presented at TMS 2024. The content was published in MSEA: www.sciencedirect.com/science/article/pii/S0921509324010220?STMJ_219742_AUTH_SERV_PA&SIS_ID=&dgcid=STMJ_219742_AUTH_SERV_PA&CMX_ID=&DM499035&AC_
Reconstruct and index Auto CLAHE processed datasets
Просмотров 170Год назад
The video was created with the help of Jiaqi Dong
Auto-CLAHE Video Tutorial by Luke Wang
Просмотров 403Год назад
This video explains how to use our Auto-CLAHE algorithm to enhance the diffraction pattern signal in the PED data to achieve better indexing quality. Our source code can be found at github.com/lukewang05/Auto-CLAHE. The work was supported by the National Science Foundation (NSF-DMR, grant number: 2144973, Program Manager: Dr. Jonathan Madison).
Crystallographic Variant Mapping Tutorial by Marcus Hansen
Просмотров 289Год назад
The code automates the identification of martensitic variants in materials by analyzing diffraction patterns in the precession electron diffraction (PED) data acquired using the NanoMEGAS system. The method is also termed "similarity mapping." The video was prepared by Marcus Hansen. The code used for our algorithms can be found on GitHub (github.com/TAMU-MHansen/PED-Similarity-Mapping).
5.2: TRIP steel and shape memory alloys
Просмотров 685Год назад
5.2: TRIP steel and shape memory alloys
5.1: Martensitic transformation: characteristics, nucleation, and growth
Просмотров 1,5 тыс.Год назад
5.1: Martensitic transformation: characteristics, nucleation, and growth
4.2: TTT diagrams and phases in steels (pearlite, bainite, martensite, and more)
Просмотров 6 тыс.Год назад
4.2: TTT diagrams and phases in steels (pearlite, bainite, martensite, and more)
TMS 2021 presentation on shear banding in cp-Ti
Просмотров 719Год назад
TMS 2021 presentation on shear banding in cp-Ti
4.1: Diffusional transformation and spinodal decomposition
Просмотров 1,6 тыс.Год назад
4.1: Diffusional transformation and spinodal decomposition
3.4: Casting - sand casting, continuous casting, investment casting, and melt spinning
Просмотров 4622 года назад
3.4: Casting - sand casting, continuous casting, investment casting, and melt spinning
3.3: Solidification of binary systems
Просмотров 4692 года назад
3.3: Solidification of binary systems
PED strain mapping sanity check video by Ainiu Luke Wang
Просмотров 6992 года назад
GitHub link: github.com/TAMU-Xie-Group/PED-Strain-Mapping
PED strain mapping tutorial video by Marcus Hansen
Просмотров 3772 года назад
PED strain mapping tutorial video by Marcus Hansen
3.2: Growth, dendrite formation, and hot cracking
Просмотров 9242 года назад
3.2: Growth, dendrite formation, and hot cracking
3.1: Homogeneous and heterogeneous nucleations
Просмотров 4,9 тыс.2 года назад
3.1: Homogeneous and heterogeneous nucleations
1.8: Binary phase diagrams of systems with limited solubility
Просмотров 2,2 тыс.2 года назад
1.8: Binary phase diagrams of systems with limited solubility
1.7: Phase seperation in phase diagrams
Просмотров 1 тыс.2 года назад
1.7: Phase seperation in phase diagrams
1.5: Binary phase diagrams of systems with full solubility
Просмотров 3,8 тыс.2 года назад
1.5: Binary phase diagrams of systems with full solubility
1.4: Gibbs free energy of binary systems
Просмотров 3 тыс.2 года назад
1.4: Gibbs free energy of binary systems
1.3: Effect of temperature and pressure on Gibbs free energy in single-component systems
Просмотров 2,3 тыс.2 года назад
1.3: Effect of temperature and pressure on Gibbs free energy in single-component systems
1 2: Gibbs free energy and equilibrium
Просмотров 1,7 тыс.3 года назад
1 2: Gibbs free energy and equilibrium
6.7: Convolution and Laplace Transform
Просмотров 1353 года назад
6.7: Convolution and Laplace Transform
Great Video with a lot of information............... Thank You So much
I thought austerity couldn't exist at a temperature below critical temperature, how is it existing at 300 degree Celsius
Hello Sir, How can I confirm if one phase has superlattice or not ? thank you
Thank you for the video, it was such a delight to watch.
what is the criterion for the screw dislocations, if we have a mixed dislocation, then the burgers vector is parallel to the g, so we still can find the dislocations in TEM right?
Thank you sir, for valuable lectures. can you please explain further how to measure the burgers vector?
Hello, do you still do research regarding phase transformations in metals?
quick question (3 years late) but in which scenario would you use the third case? the one e^(-as) laplace{f(t+a)}
thanks bro
ruclips.net/video/o7mIX_FqMC4/видео.html
Banger, thanks man
thx
I would like a more detailed demonstration of the Pierel stress, it is a doubt that I have had for a while :(
Thanks for your lectures. I see some worm-like pattern when I image a 5nm ferroelectric sample with HIM. With SEM, I only see the pattern when I use EsB detector. The inlens and SE detector doesn't see the pattern. What do you think is the contrast mechanism for the worm like pattern?
I love this lecture. Thank you very very much from Korea. Have a nice day~!
thanks a lot , this is one of the best explanation of the concept I have come across on RUclips.. 👍
nice and useful series, please upload more practical sessions.
what is the spot size ? we can control the aperture and condenser lenses to change the beam intensity and size (converge and diverge), then how the spot size is being controlled?
Well done! 👍
the least knobby dot to you too
Can you give me the link of website please?
I'm Vietnamese student thank you so much for sharing your knowledge
Thank you for your lectures. Unfortunately, I can't understand how to match the provided stress field diagrams with the 3D figures of the edge and screw dislocations. Could you please provide some additional sources where I can find the explanation or give me advice on how to understand that?
great lecture, but someone take this man out to the night club!
Hello Pfofessor, very beautiful analogy. Thank you for sharing. Best wishes.
Thanks for your helpful video. i am confused about the equation of calculating Si. the delta θ and θB is a angle parameter. why could we measure the distance (as marked in the video) to indicate the angle. what's the relationship between the θ and distance of fringe?
I'm confused, shouldn't you multiply S(theta) to the homogeneous critical energy instead of the heterogeneous one? SInce it's supposed to have higher critical gibbs energy
Tnx
very well explained , i am student of IIT VARANASI( BHU)
why enthalpy equals to 0 when the T equals to 25C or 298K?
Can you please explain the difference between gun shift and beam shift?
Do we have liquidus and solidus on ternary diagram?
Thank you so much! In the "angle of scattering ", I guess Elastically and inelastically should be vice versa
Kindly write good hand writing Sir its not clear for us
How metric A comes from sir? 😢
Very nice explanation, thx!
Very helpful, thanks sir...!!!
Dear Prof. Xie, It is interesting what you have done, making this amazing TEM imaging series. My question is how can we determine which g-vector to use in order to get a suitable micrograph of my dislocations? Can I predict my g-vectors before I start doing TEM? I have a dual-phase alloy contains FCC and BCC phases.
Sir is this a free software? What's the raw format? Can it accept dm3 or dm4
The traditional Japanese sword makers coated the sword in a clay mix on the back of the blade (the blunt side), and left the sharp side uncovered. They heated the sword and judged the right temperature by the colour, then quenched it. The sharp edge had no clay on it so it cooled immediately, the spine of the blade had clay on it so it cooled much slower. The end result was a sword with a tough flexible spine and a hard sharp edge.
My ex mother was the spine
The effect of dislocation line direction, in the third case when the dislocation line is parallel to the beam direction, are the points still seen if the g.b invisibility criteria is satisfied?
You are correct. The contrast is weak though and it is referred as the residual contrast.
The key take away from this class: Propose with graphite ring
graphite is forever🤣🤣, excellent lecture.
Is it supposed to be gamma square or gamma cube? In that formula for critical Energy
Pretty sure it's gamma cube
感谢教授,祝各位早日做出杰出贡献😁
This is what, I was precisely looking for. Finally found amazing piece of information with lot of contents , 👍
Neat!
Hi Prof. Xie, thanks a lot for the nice video, may I know how to distinguish partial and perfect dislocations using tem?
Hi, in theory, there is no perfect dislocation. All dislocations are partial. For large dislocation dissociation, you can use weak-beam dark-field to resolve them. For small dissociation, you need to use HRTEM.
Thanks a lot for the reply@@kelvinxiemsentamu6890
Do you have your code available on an open source repository?
Yes. They are on GitHub and the links are provided in the descriptions of the videos.
Sorry, I thought I had included the link in the description. Here it is: Our source code can be found at github.com/lukewang05/Auto-CLAHE.
You are blessed. You saved me!