Title | : | Euler-Lagrange equation explained intuitively - Lagrangian Mechanics |
Lasting | : | 18.22 |
Date of publication | : | |
Views | : | 361 rb |
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Please change or remove the music altogethernot useful nor is the graph useful Comment from : Marion Deleon |
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“Let’s consider the slope of a line on this graph”brPlease No Don’tbr“We need to consider the partial derivative”brANYTHING BUT THE CALCULUSbr*starts calculating the derivative of a partial derivative *brNOOOOOOOOOOOOOOOOOO Comment from : Phrygian Phreak |
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Hard to focus on this video with a banger like Liszt’s Hungarian Rhapsody no 2 playing in the background Comment from : Benjamin Graziano |
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More confused after than before, but I really wanna touch that graph 😂 Comment from : Yung Jwall |
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Totally love these videos Narrating excellent too brCan see a lot of work has gone into explaining the concept brGreat stuff as usual! Comment from : Irigima |
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Eles complicam a equação para não entenderem , é natural que isso seja assim , Comment from : Osvaldimar dos Santos |
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Take physics from YouTube it's very very and a Very Bad, br __go to library and there Whole better Scientist of 1000 years Best of best books, br Best Understanding of MechanicbrErnst Mach: Critique of Mechanic Comment from : Hannibaal Barça |
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힘내주세요 포기하지말아요 이 동영상은 아주 멋져요 도와주셔서 고마워요❤ Comment from : 그여름날의추억 |
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nothing understandable in this video demonstration is bad, not intuitive i am sorry u make easy thing difficult Comment from : Natural Learning insaan |
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it's just amazing thank you so much Comment from : Mohamed Mouh |
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Wow, clear as mud 😆 Comment from : Robert Brandywine |
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This video is basically "let's do ___" without explaining why Comment from : Gabe Darrett |
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So, you are telling change rate is the amount changed? Doesn't make sense? Comment from : Gytoser |
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It would be fine if there were Chinese editions Comment from : li jack |
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This is a tough one 😂 Comment from : Peeper |
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I want physical meaning of Euler-Lagrange equation and Lagrangian density can you help me and write me that? Comment from : M_aa |
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Thanks for the video Does anyone know what the names of the first songs are? Comment from : Rebecca Herr |
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Nl entendí na Comment from : Rodrigo Cordoba |
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The beautiful music become a big drag here ! Comment from : Zack 120 |
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music with explanation is very bad and annoying Comment from : Lonely Shepherd |
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Great visualisation! Thank you very much Can anyone tell me the name of the background music of this video? I can't remember it and it stuck with me Comment from : Yorick Zeschke |
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manyak manyak işler Comment from : murathan karatmanlı |
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Really nice video People may need to watch it a few times while making notes, but everything is there Comment from : W R |
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From D'Alambert to Hamilton youtube/IKDI5uFKp2Y Comment from : Stephan Kocher |
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Brilliant This is worth saving in my playlist Comment from : Batman Fan |
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Wow there are a lot of smart people in the world I never know this way to understand Euler Lgrangian equation geometrically Comment from : HY Prk |
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I have no idea how many times I've watched this by now, but I love it Thanks Comment from : Migo Narvo |
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Absolutely amazing, thank you for such a wonderful animated explanation Will rewatch and make some proper notes, that was excellent :D Comment from : Malcolm Akner |
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loved your work as always but i think the we need a bit more intuition, something on lines of why the formulation is this particular one and not others seemingly giving similar results Comment from : Sujit Sadhnani |
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Tom and Jerry flashbacks from music Comment from : R J |
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Didnt get the math, but enjoyed the Hungarian Rhapsody Comment from : copernicus633 |
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안녕하세요 에브입니다 Comment from : 훙훙훙 |
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Awesome understanding but just one suggestion Please do not put music Its kind of distracting not able to focus completely on the explanation Comment from : Karan Tamboli |
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6:08 I don't get why this is true Comment from : Rodrigo Appendino |
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Instant subscribe As someone who is struggling through learning lagrangian mechanics right now, this video was invaluable, especially the explanation of 14:28 of why one must take the derivative with respect to time of the second term Comment from : Aeden Gasser-Brennan |
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Subbed :) Comment from : Rovsau |
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Nice visual representation of the Lagrangian, which is a very difficult topic! Comment from : David Terr |
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Евгений привет еще раз здрасте,brДля визализации Вы пользуетесь Графическим пакетом iClone?? Comment from : Ko Prometheus |
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Привет,brВы говорили, что Визуализация квантового поля будет в другом видеоbrПодскажите где это видео можно найти?? Comment from : Ko Prometheus |
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The animations here made me think of gummi worms a lot Comment from : Jeffris (Suspicious Manifold) |
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This video sponsored by the World Colonoscopists Association Comment from : IncompleteTheory |
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Nice 👍 Comment from : brenda williams |
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Normally I LOVE these videos, but the plot of the action just looked like intestines … Comment from : Jack Stewart |
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From my first years as an undergrad, to me now pursuing my MSc, you have always been there when I needed you the most Thank you Eugene Khutoryansky Comment from : Arvin T |
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Eugene , How you make these animation video ? Pls tell me 😊 Comment from : Ankur kumar |
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Thank you for your amazing teaching video brI'm wondering if there is proof for more independent variables brI've searched on the internet but don't find the full proof Thank you in advance Comment from : Jimmy |
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👍🏻 Comment from : Civil Ideas |
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This is a showoff of animation but not a good explanation of Lagrangian for beginner Comment from : Guiwen Luo |
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그래 이게 오일러 라그랑주 방정식의 물리적의미지 Comment from : 林·님太:ᄐᆡᇰ成셔ᇰ |
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best video Comment from : Tanvir Farhan |
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I generally believe that your videos are very informative and easy to understand I can't say this is the case for this video Sorry!!! Comment from : thanasis constantinou |
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this is a test 2 Comment from : Ryan Nordquist |
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thank you so much! thanks to this video, I understood Lagrangian more accurately Comment from : Ethan |
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Beautiful videos Just too complex for me to comprehend :D Comment from : Mairis Bērziņš |
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He starts saying about 3D path of a particle, and suddenly changes to explain the Lagrangian in 1D space, which the path is just a straight line Even though the Lagrangian changes in 1D path After all, he changes again to the time domain to explain the concept of action (which is the integral of the Lagrangian) Very confusing and misleading Comment from : Leonardo Santos |
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Can you please explain why the slope of the action/change in path graph has to be 0 for the actual path if the work done depends only on the initial and final state (6:11)? Comment from : Wilf Ashworth |
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Да сфигали? С какой стати 20 мин? Люди минимум семестр на это тратят А то и два! Спасибо Comment from : Николай Николаев-Потапов |
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Khutoryansky teaching philosophy: You never really learn something until you make a full-color computer graphics animation of it set to classical music Comment from : The Ultimate Reductionist |
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The video is for chess players to understand its quantum system Comment from : Mr Goldie |
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6:01 - Maybe this state could be elaborated a bit further Why conservative forces implies stationary action? Not obvious to me Comment from : Giuseppe Papari |
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wow this is heavy! it's hard to digest Comment from : incognegro mode |
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I don't know who chose the music for this video, but it makes my anxiety SKYROCKET Comment from : SuperKimxD |
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I'm just picturing a cat & a mouse beating the crap out of each other at a piano Comment from : Massimo OKissed |
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What the hell Why is this video SO good Goddamn Came to the comments section to literally complain about what incredible quality this video is when surprise comment by Michael Stevens! Always a pleasure to see that Comment from : Kaiden Schmidt |
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At 2:45, the Lagrangian looks like a pair of boobs Comment from : somuboy |
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Bro I just started learning Lagrangian Mechanics and this video blows my mind, greetings from Berlin!! Comment from : Leon_Noel |
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Can someone explain the assertion made at 5:56 where the true path of the system must be when the action of the system is zero? I get that work is a state function, but how does that relate to the action and it being related to the derivative being zero? Comment from : Mickel Ross |
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Dear madam, br[1] could you please describe why Lagrangian is described as (KE - PE) ?br[2] While taking derivative in animated plot, why you change colored balls position according to its color?brTIA Comment from : Sayanjit Banerjee |
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Why does the video choose to show the change in x(t) as increasing the action, while the corresponding changes in x'(t) decrease the action? It seems equally possible to me that both changes can cause an increase in the action For example, what's stopping the Lagrangian from having the opposite of the slopes you showed at 14:50? In that case, the action would increase overall from the small change in the path Comment from : Alexander Pleava |
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I don't get where that d/dt came from in Euler-Lagrange equation? Also why is change in action equal to change in Lagrangian? And why is there a minus sign in E-L? As far as I get part with partial derivative with respect to path should be equal to time derivative of partial derivative with respect to velocity but is seems like it's just tautology, how can we get anything meaningful out of that? Comment from : Matej Pavlović |
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Нихуя не не понял, но очень интересно (с) Comment from : Adrenalin |
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I would need more on the calculus of variations, Euler lagrange solutions and the application to complex problems in computational geotechnics For example, the gain in compressive strength of compacted treated/modified/cemented soil against time of curing in days This system is constrained for a start, between 7 and 28 days when cemented components are expected to gain initial strength and around 70-80 of total strength respectively Experimental experience has shown that the typical behavior of the graph is semi-parabolic and in some cases parabolic Any insights can help I am assiduously working on this If you dont mind, you can send any insights you have to konyelowe@gmailcom Much appreciated Comment from : Kennedy Onyelowe |
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I sincerely wish to thank you Eugene for this thoughtful and inspiring video visualization lecture It is right on time Comment from : Kennedy Onyelowe |
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I have master in physics but still do not understand why the statement at 06:03 is true Comment from : MH Yip |
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Can you do a video on the Hamiltonian Comment from : Cameron Spalding |
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This video is very interesting but some steps, not formally proved, remain unclear for me In particular at time 11min24s of this video this (very important) assertion is given: for the slope of the blue line to be zero (slope of a map whose domain is the set of all possibles pathes and whose codomains is the set R of the action values) this expression (namely: dL/dx - d/dt (dL/ dx') must also be zero As one function is defined over pathes and the other over the time, their relation (or their dependancy) is really not clear for mebrIt is also not clear if one should consider that two pathes of the set of all pathes are supposed to have the same time domain or not brfor short: it would be nice if you could provide a formal proof of the assertion given at time 11min24s Comment from : N R |
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What’s the name if the song? Comment from : Drag |
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T💗🥦💕🧠👩❤️👨🦄💕🥦💗Ttt99💕💕🥦🥦 Comment from : Omega79 Theta79 |
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secular academics and logical mathematics and love and kindness and peace Comment from : Omega79 Theta79 |
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Thank you Comment from : Mahxy Lim |
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you deserve much more views and subscribers Comment from : Sophile |
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thanks for the video Comment from : Sophile |
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I am back for round 2 after about a month I first watched this I hope this time I will understand half of what is in this video Comment from : Wil Ts |
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Я ничего не понял, но зато я теперь увидел как выглядит заворот кишок Comment from : Шум Шумов |
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What's the music in the background Comment from : darkmath100 |
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I'm dumb ): Comment from : fjoa123 |
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Which animation tool did you use to make this? Comment from : Unver Ozkol |
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