I just wanted to take a moment and express my gratitude on how concise, thorough and clear this whole series has been. I happen to be a math professor who is NOT an expert on the subject so this has been an excellent guide to the the main definitions and results of mathematical physics related to GR. I should also point out that your humility is a testament to your greatness. Keep up the good work and thank you for simplifying our lives!
We were all living in darkness, then one day God saw us, listened to our prayers and then He sent us eigenchris to shed some light and teach us what we could not see through the darkness.
Just completed Both your playlists on Tensors and Tensor calculus. It was a very intuitive and logical dive into the world of Tensors - something that can really help many trying to understand General Relativity. A proper understanding of Tensors can help many get a better grasp of GR. I really appreciate all the effort that you have put in making this series .
Overall impressions of the whole series of videos. I finally reached the end of the series of videos.
I can't believe I ate the whole thing ... like sitting alone in front of a large empty pizza box ...
Yes, I even plowed through the "long boring proof" of the second Bianchi identity of lecture 26 from [10:23] to [16:38]. I found value in seeing a double Lie bracket and using the Lie bracket as one of the inputs of the Riemann tensor. (It remains beyond me how anyone could have managed to establish such a complicated proof.)
A year ago, I was very excited with the first few videos on tensor algebra. So clearly and brilliantly explained. The occasional comment about "some of you might wonder why" came exactly when I was indeed wondering why - as if the teacher was witnessing incomprehension developing ... The explanation of the why was most welcome.
A sense of being overwhelmed started to develop when I realized how much more material there was yet to view. But I persevered, taking notes.
There was a promise of being led to General Relativity.
There was a sort of epiphany when the unit basis vectors where shown to be the same as the directional derivatives. Wow ! And a clear explanation of the infamous λ parameter of parametrized curves with the use of speed and acceleration. Wow again !
I finally caught up on the backlog of videos.
Next, a sense of a loss occurred when no new video was appearing for months.
The level of mathematical complexity picked up but video 25 dealing with the derivative of the volume form really yanked me out of my comfort zone. It really was a nice touch advising that video 26 was the last one of the series. I had been sort of discouraged by the ugliest of all ugly formulas, regarding the volume form. That one truly is ugly as sin.
The sneak preview of the GR field equations was very interesting.
I am not too concerned with the delay to 2020 for the GR series. First of all, this will give me time to review at least the last 10 or so videos - glad I kept such meticulous notes.
And 2020 is now really just around the corner.
In the meantime, I'll also be busy boning up on the Arduino and Raspberry pi.
What a wonderful experiment this all was. A stellar teacher who understands the difference between teaching and mere telling.
Thanks for your detailed feedback. I agree a lot of the Ricci tensor stuff is ugly... but quite a number of sources in physics only leave about 1 paragraph explaining the Ricci tensor and don't explain where it comes from. I found it very very hard to track down sources that explained it. I got about 80% of the way to understanding it and then gave up and posted the videos anyway, since I had already been struggling with it for months and didn't want to waste more time on it. I sometimes wonder if there are any humans still alive who understand it. I hope at least I did more good than harm.
Fifteen years ago, I was a physics major, but I couldn't wrap my head around General Relativity, so I switched to experimental physics. Unfortunately, I found experimental physics to be rather dull, and I eventually ended up as a software engineer. I attended a prestigious high school and then went on to the top engineering university in my country. My best friend from high school, the smartest student in our class, even won a silver medal at the World Physics Olympiad. But even he was baffled by General Relativity and gave up physics to become a dentist. Had eigenchris been around when I was a student, I'm convinced that we both would have stuck with physics. Less money but maybe more happy.
This truly does feel like the end of a journey. I am happy that TH-cam brought me to your channel recently. I just watched a few of your videos, and got interested in the subject. Then, I decided I actually want to watch the whole series, and take notes. So I did. I religiously watched 1-3 videos per day, taking notes. During the proof of the second Bianchi identity, I started to question that decision. I almost gave in to the temptation of not writing an arrow over my vectors. But I did not. I am incredibly grateful that you made this video series. It inspired me, along with a few other factors, to change the direction of my undergraduate degree from Statistics to Geometry/Mathematical Physics.
@@canyadigit6274 It's going quite well, thank you for asking. This was meant to be my final year, but I will take one more year to catch up on Geometry/physics courses. Thanks for the kinds words, best wishes to you as well.
What a delicious video series from our beloved Eigenchris! Twenty-sex in-depth video lectures on tensor calculus? On youtube? For free? What a delight. Thank you Eigenchris, you are an educational maharishi.
@@joabrosenberg2961 I have an undergrad degree in "Engineering Physics". I work as a software developer. I don't teach anywhere. I never took GR in undergrad, so I decided to try learning it in my free time, but was pretty horrified at some of the explanations and thought maybe I wasn't smart enough to learn it. I tried to learn GR several times over the years, often giving up, taking a break, and then having to re-learn things after I decided to try again. Once in a while, I found "good" explanations for the various concepts scattered over the internet (I've forgotten most of the sources now) and eventually things started to "click". I realized a huge problem is that a lot of GR texts teach tensors using tensor calculus and tensor fields first instead of teaching basis tensor algebra first. I decided to make 5-10 videos on tensors without calculus. In a couple months I had gained about 100 subscribers, so I just kept making more videos, and I've been doing that ever since.
Been making notes on Tensor algebra and have just made it to the end of Tensor Calculus. I am about to go through the relativity playlist but before I do I just want to take some time to give my sincerest gratitude to Chris. I am about to embark on postgraduate studies in September and I will be studying this stuff more formally. This series has really helped me to better understand all the big ideas in an intuitive way. I feel more confident going into my postgrad studies now. Even Andrew Dotson has rated these videos (especially the Riemann curvature video which was just amazingly explained). You have done a great service to the physics/maths community in making these videos Chris. I give you my most sincere gratitude for going through the hard work of understanding this and arranging it in such a graphic and intuitive way.
I am deeply impressed by this lecture series. I will return to these lectures over the next couple of months, not only to refresh some of the concepts presented here, but also to take note of how the course is structured and in what ways it outshines most university lectures. Apart from being helpful to students, this is an absolute masterclass in how to construct a lecture series that is both engaging and informative! There is so much more I'd like to write about the ways in which I appreciated this series, but that would be better expressed in an essay rather than in the youtube comment section.
You should write a textbook on tensors! In all the years since dropping out of my Ph.D. program in chemistry, I had struggled with understanding tensors. Your video series cured that. I can’t wait to see you general relativity series, and I may just go crack open my old copy of Misner, Thorne, and Wheeler!
at '23 end i finished this series and was middle of relativity it kinddled some kind of fire in me, idk, im not trying to flex or anythinig, but from april 24 i started doing analysis, algebra and some topology now im going through langs and rotmanns for modules and tensors, loving each problems from those texts, im just a vehicle and the path is already there, hopefully im gonna learn some more algebra and topology over the next months and years and decades. such is the quest, but this channel was a massive influence to my journey so imm more than thankful, just a quote to finish it off "an unitary associative R-algebra is an R module which also has a ring structure" this is hymn
Hey man you are a gem to the world !helping the self learners like me. I would be so grateful if you could provide the notes to these lectures as well like the zip file you provided for 'Tensors for beginners' series.
@@ahmedabdeltawab8408 I took 2 quantum classes and I still struggle to understand basic things like why the momentum operator is -i*hbar*d/dx. The axioms of quantum just seem like nonsense to me. I suppose I could do the math but I have very little clue what it means.
I started seing you series on linear tensors in the first half of 2020, then i wanted to begun this but i didnt haved enought knowledge and needed to focus on my tests to get into university, after the first classes in university i begun reading throw the books and at some point i remenbered this series and realized i already haved the knowledge to see it. Now after a few months of using this as study material i have finaly ended, i cant say enought thanks to you for how much you chaneel helped me learn. I an not kiding when i say that i learned more from you than from any of my uni teatchers until now. The proff is from my notebooks from college the only one that has a similar amount of pages to yours is the Linear algebra and analytic geometry one, and that one i studied almost solo due to corona.
I watched this video series over and over again till I have some kind of intuition on abstract concepts of tensor calculus. Without this series, I have no idea how to find a route to climb up the Mt. Everest of General Relativity theory. On these days, I am also watching your relativity series. It Is A Great Pleasure To Meet Your New Uploaded Video. But I recommend you not to hurry - never hurry. I believe your job is already outstanding. You don't need to hurry up or make yourself overloaded to prove that your job is outstanding. Your job is worth to wait. If somebody complaints that Christopher Nolan or James Cameron are not not so diligent to make a movie every month, It's not their problem. So, please take your time. from South Korea
"But I recommend you not to hurry - never hurry.". Thanks. I often feel pressure to produce videos. But I am glad you want me to take my time to ensure they are good.
I am a computer science student and I found this series so useful and I am already thinking how can I solve certain problems with this new toolbox, thank you so much!
Just coming to the end of this series, thank you so much for taking us on this journey! The clarity of your explanations is really exemplary, your course is a gem! And with respect to the somewhat more complex proofs towards the end of the series - with a physics background myself I can live live with proofs that work “in almost all situations”, especially anything that is encountered in the real world, whilst I trust that mathematicians will have put the rare exceptions and extreme cases on a solid foundation. I can only encourage you to keep going where your curiosity takes you, and continue sharing your learnings! The following comments may perhaps be useful for some viewers - at some points of the series I used additional resources as a change of perspective helps my learning. There are 2 recent books that I found particularly helpful to complement the series: The first book would be “A visual introduction to differential forms and calculus on manifolds” by Jon Pierre Fortney with excellent illustrations and step-by-step derivations of the math foundations for differential geometry. The second book is “Visual Differential Geometry and Forms” by Tristan Needham. This book uses a somewhat different mathematical notation that is geometrically inspired and goes back to Newton’s Principia, so this takes some getting used to. However, the practical examples of constructing geodesics or doing parallel transport on the peel of various fruits are really fun and helped me visualise some concepts better. The history excursions are fun, too.
Wow! This was tough staff, but you made it comprehensible and enjoyable (without compromising rigour). Quite a feat. Looking fwd to watching the GR videos!
I'm really grateful to you for this series. I've always been fascinated by General Relativity, unfortunately many people always that one needs a really deep mathematical background, which is not my strong point, to understand this theory. But after watching your videos, I realized that while it does require some mathematical knowledge, it's not as complicated as people say (at least the basic concept). And this series will definitely help me in my exam next month. For this I would like to thank you once again
I've come this far from Functions in 8 months. I don't know if it's a big job or a small job, but I thank everyone who helped. Exist. Now we are one step closer to our goal. There is no stopping until we reach our goal. Shame on those who do not stop. IN DURDURANA
You have already so many gratifying comments, but I can't help adding mine: for both algebra and calculus you made a VERY VERY WELL DONE JOB! I never had such a clear explanation of vector spaces and all the attached stuff. Thanks a lot. Looking forward your GR video series...
Wonderfull work! This is the best tensor lessons to understand what it really is and to use it. I tried by reading some books some years ago but I've never get the essence before seing your channel. Thanks!
@@GeminiAnu I'm not really sure what the scope of your thesis would be. One of the main applications of tensor calculus in physics is general relativity. You could do something about that. I'd probably as one of your professors for advice.
Great series man.. I was struggling in understanding tensor calculus for two years.. Now it becomes clear to me. Thanks for this. Waiting for General relativity series..
Suggestion for your upcoming series on GR : an explanation of the Mars perihelion and how GR solves it. And no, you definitely do not have to be concerned with how much time you need to create the new series. You are the master of your own time and we'll get what you give when it is good and ready, period.
Yes this is what I meant - I should have been more careful writing this.The importance I gave it is that it was mentioned in a TV series when Einstein stated something like "it also explains the precession of the Mars perihelion and the theory is complete".The answer is that solving the field equations creates a new term in the standard Newtonian equation for the Mars orbit. I would love to see this derivation explained in detail.
lots to consider here.. but glad i completed the series! gonna do some light courses on spinors… maybe one day soon i’ll be able to implement something cool with all this knowledge of tensor calculus!
9:16,how do you know which connection coefficient relates to point P? Similarly,at 9:36,how come some of the connection coefficients reduced to zero and others didn't? How do you distinguish?????
Everyone here is a genius! You and I are the only dummies who have asked this question. Perhaps, however, I have understood. At point p, the gamma connection coefficients are zero, but the derivatives of the gamma are not zero, since the value of a variable at a point is one thing, the variation of that variable at that point is quite another. In fact, the gamma are zeroed when they are factors, not when they are arguments of derivatives. Someone please tell me how much nonsense I have written!
Hi Chris. At 20:00, why can you raise & lower indices on the right side of the semi colon? I see why you can do it on indices to the left of the semicolon as you showed earlier in the video. Thanks in advance!! EDIT: Sorry, not raise & lower, but just change letters via kronecker delta. Question still remains - why can you apply kronecker delta to the basis vector direction on which the covariant derivative is acting on R?
R; _n is just like a row vector whose column entry is denoted by the "n" index. The kronecker delta δ^n_l is just like an identity matrix. We're basically multiplying a row vector by an identity matrix. And since the index letters are arbitrary, we're always free to change them. Does that make sense?
first thanks for all your effort and hard work you have done at this course i want to know from you the name of a best textbook that you see in your opinion is good and explain easy as your style of explaning at tensor calculs i trust your opinion very much thank you sir very much ❤
A question about the proof of the second bianchi identity. You proved it at first in local inertial frame and after in a general case. But since these are tensorial relations, proving them in one coordinate system shouldn’t be enough to be true in any coordinate system, since tensorial relationship shouldn’t change changing coordinate system?
i feel like sometimes that field equations are dimensionally inconsistent...because on left we have curvture and on the other side we have energy....dont both have different dimensions? i know i am wrong ...correct me(by the way....very nice vedio)
Yeah, curvature (Einstein tensor specifically) has dimensions of m⁻², while energy-momentum tensor has dimensions of energy per volume (J⋅m⁻³), but we have another constant factor of 8πG/c⁴, which has dimensions of m³⋅kg⁻¹⋅s⁻² / (m⋅s⁻¹)⁴ = m³⋅kg⁻¹⋅s⁻² ⋅ m⁻⁴⋅s⁴ = m⁻¹kg⁻¹s² = m⋅J⁻¹, so actual equation reads m⁻² = m⋅J⁻¹ * J⋅m⁻³, which is certainly true
Hi eigenchris, I really enjoyed watching your tensor calculus videos and learned a lot and new concepts on how to look on already familiar things. May I propose an Idea to you: In the end and sometimes inmidst of your videos you have these nice summary slides. Could you make them available to your audience (not just for me of course) in PDF format or something similar? Now that I am learning GRT in master courses I wish I had your formulas summed up. Since this is a lot to ask for and will cost you extra working time, I'd definitely drop you another cups of Coffee for that. Even if you dont like that proposal or dont even have time for that, still thanks a lot for these high quality lectures. :)
I have the slides from the fist 20 video here: github.com/eigenchris/MathNotes (in Microsoft Office .pptx form, but those can be exported to .pdf). The slides for the last 6 videos are scattered around in old drives so I'll have to take some time to get them together.
How do I linearize the Ricci tensor according to the metric? When it comes to gravitational waves in flat space, Einstein's field equation is rearranged according to the Ricci tensor. Then you assume that you are in a vacuum and therefore the energy-momentum tensor = 0. So you get Ricci-Tensor=0. Now we linearize this at the point of the Minkowski metric and obtain D`Alembert operator of the metric tensor =0 and thus a linear wave equation. I have not found anywhere how to do this. I would like to know how to linearize the Ricci tensor in other metrics. For example, when gravitational waves propagate in the Schwarzschild metric.
Hey Eigenchris, Thanks again for uploading such a clear and well-presented course! I was just wondering - what sources did you find most useful in learning about Tensors and Tensor calculus? I have been looking for a good resource for intuition on the push back/pull forward and the wedge and double wedge product and was wondering if you had come across any whilst making your videos!
I think this playlist by David Metzler is the best introduction to those topics that I've come across: th-cam.com/video/M5wrnwlm8lw/w-d-xo.html. It's a bit on the longer side, but he does go through lots of examples. (Though I'll say I've never heard of the double wedge product and I don't think he covers that). I'm hoping to do videos on the wedge product and exterior derivative before the end of 2020, myself. As for how I learned... I basically just googled nonstop until I felt I understood it. I think I left some links in the description to some PDFs that helped me. I've never gone through a textbook cover-to-cover. I tend to just skip to parts I want to learn about and see if it helps, and if not, toss it and look for something new. You can also check my "About" page for additional links.
@@eigenchris Great! Thank you I will look into those! Yes - definitely looking forward to those videos! This is definitely the best and clearest course I have come across on Tensor calculus by far!
I don't have plans to in the near future. It seems pretty complicated and I don't feel like investing time in learning it right now since it isn't needed for the basics of general relativity.
When contracting the Ricci Tensor, this is a 2 times covariant tensor, right? Thus. before contraction we need to use the metric tensor to transfrom it to a 1,1 Tensor. What is the correct formula for the resulting scalar (Ricci scalar) ? For 2 dimensions: R11*g11 + R21*g21 + R12*g12 + R22*g22 ? We need to multiply the "row of rows" (Ricci Tensor) with a "column of columns" (metric tensor), right? It should be the trace of "the matrix", but I'm too dumb to find the correct answer. Could you please enlight me? THANK YOU!!
Hah :) Some time ago I wasn't sure if I would go through this playlist... thought the tensor algebra would be enough. But here I am. And I'm certainly moving to the general relativity playlist. Woo-hoo!
Many little gems of insight here! Thank you. Do you suppose that the conservation laws for T was a key element in Einstein's search for the modification of R that would also have zero covariant derivative?
As far as I know, Einstein's original publication of the Einstein Field Equations did not have a "modified R" term. It was just R_uv = 8πG/c^4 T_uv. He was able to use this to calculate the perihelion advance of Mercury's orbit (since the extra "modified R" term conveniently went to zero in that special case). But it was later pointed out to Einstein that his equation violated conservation of energy, and so he added the "modified R" term to fix that. I also have a playlist on Relativity that covers this in a video called "Relativity 107f" if you're interested.
Your question is one that I had for some time. Eigenchris points out (indirectly) in his reply to your question that Einstein was alerted (I understand it was by David Hilbert) that Energy was not conserved in his original formulation of GR. So, noting the Bianchi Identity, Einstein added the Ricci Scaler term which then satisfies Energy Conservation. Much later, I realized that in study of Cosmology that photons loose energy during the expansion of the Universe. WHAT? Turns out that Energy is only conserved Locally not Globally in GR. Eigenchris's work here and much later in his Cosmology videos, I have found just how valuable his videos are, how well they are produced (few mistakes) and how well he explains his subjects.
@@eigenchris Yes, this is a correct understanding. Yet, as I have commented below, Energy Conservation guided Einstein to a correct formulation of GR yet Energy is not globally conserved in GR - as in the Expansion of the Universe.
Wow what a great series. Just one question. I found the choice of indices somewhat confusing at parts. I watched the whole series and the tensor algebra but I'm still confused about how to choose the indices of the terms confusing especially when multiplying by new terms. would you mind referring to a text or source for clarification?
@@eigenchris ok so I guess just to use 2 instances that I remember. in Tensor for beginner part 8 at 3:17 you derived how the linear operator transforms under the change of basis. first starting with the telda basis then replacing each term until you get the FLB for the order of the operators. If i understand correctly, each time the top index of the operator matched the index of the basis it was acting on. The order in which we do this gave us FLB and the lower index of each operator matches the next operator's top index however you wrote down BLF. If i understood correctly the top index represents row of operator and bottom represents column and since for matrix multiplication we do row of the left operator times the column of the right operator shouldn't the correct order be FLB to find L_telda? If i'm not mistaken the order does not matter in index notation since they just represent the entries of the matrices but given we wanted to perform matrix operations to find L_telda it should be equal to FLB correct? Similarly in another instance in tensor calculus series part 17.5 at 9:00 you start with the expression of the covariant derivative and on the 2nd line you perform chain-rule on terms on both sides of the equation. the index for p in the left and right hand side are "n" and "m" but I'm not quite sure why they have to be different or why they couldnt have been another one of the existing indices. In general i'm confused when having a different index means we are referring to another term and when it represents that we are summing over that index. sorry about the long comment
you keep calling R superscript mn the Ricci Tensor.But i thought Ricci Tensor should be subscripeted?The superscripted version should be the Ricci Tensor that’s raised to superscript by virtue of the Inverse Metric Tensor. So is it just colloquialism?
First of, great series! Truly outstanding. Secondly, would it be possible for you to maybe upload these slides, so we can download them. I know there are some of them already on you Github page, but I am talking about the rest. Thank you!
The problem is that the presentations are in pieces on my laptop due to multiple versions and edits.. and I need to reassemble them. If you have any favourite videos, I can focus on those first, but it will take time to get them all.
@@eigenchris Oh, that's too bad. As for 'favourite' videos, not paticularly. In this case I guess it would make the most sense to just continue doing them in order. Thank you for your response!
A big weakness of mine is that I do very few exercises and just look at proofs/examples to makes these videos. I read parts of Gravitation by Misner, Thorne amd Wheeler to learn about tensors and I know that book has exercises, but I can't say if they are any good.
I don't want to get your hopes up too much. I will not start work on these until 2020. But my rough plan is: Intro (1 video), tensor algebra reveiw (1), special relativity (1), differential geometry review (2), assumptions of GR and einstein equations (1), schwarzschild metric and black holes (2, maybe 3), expansion of the universe and cosmological constant (1), gravity waves (1).
Hello, Your series is very helpfull! I would like to ask if you can recommand me a book about GR to understand it in a deeper level. Thank you for your time!
There is Gravitation by Misner, Thorne and Wheeler, but it is very thick and very detailed, perhaps hard for a beginner. Professor Sean Caroll has notes from his General Relativity course online.
Hello Chris, I plan on writing some tensor calculus notes and would like to use your videos as a source, giving full credit, both in the document and in the page linking to them. Is that okay? I could not find any other way to contact you. Thanks for the great videos!
I've been kind of misled by the assumptions that we can equalize G_mn and T_mn based on the fact that theyr's both derivatives are 0. Following this logic we actually can equalize any other things that has 0 derivative. Why can't we equalize g to T_mn?
I have a video called "Relativity 107f" which does a more thorough derivation of Einstein's equations. The idea is to generalize Poisson's Equation, which says "△φ = 4πG ρ". This says the Laplacian of the potential φ is proportional to the mass density ρ. But these are not lorentz-invariant quantities. If I Lorentz transform to a frame with a different velocity, the density ρ will be different in that new frame. To make it relavitistically invariant, we replace △φ with Ruv and replace ρ with Tuv. This gives us Ruv = 4πG Tuv, which is almost right. However, the divergence of Tuv is zero, and the divergence of Ruv is non-zero. So we add the extra 1/2 R guv term to make both sides have zero divergence. I'm not trying to say any rank 2 tensors with zero divergence are equal.. The idea of making Ruv and Tuv equal (or "almost equal") comes from Newtonian gravity.
I normally see the Einstein Field Equations written wity covariant tensors. But you can always raise or lower thr indices using the metric tensor. Does that answer your question?
Dark Energy and dark matter are very controversial in theoretical physics as to date there has been no empirical detection of the same. The recent Null-experiments to empirically detect SUSY WIMPS and Axions has sent theoretical physics back to the drawing board regarding the physical explanation of dark matter. Obviously, there exists a principle which theoretical physics has not yet imagined nor discovered.
one of the methods for controling nonlinear systems is feedback linearization and lie derivatives used to linearize the system feedback it is robotic and aerospace applications I had spent months studying differential geometry as fundamental concepts for geometric control and your classes are so helpful thank you very much
I just wanted to take a moment and express my gratitude on how concise, thorough and clear this whole series has been. I happen to be a math professor who is NOT an expert on the subject so this has been an excellent guide to the the main definitions and results of mathematical physics related to GR. I should also point out that your humility is a testament to your greatness. Keep up the good work and thank you for simplifying our lives!
Thanks. I'm really glad to hear these videos were able to get you up to speed on the math needed for GR.
We were all living in darkness, then one day God saw us, listened to our prayers and then He sent us eigenchris to shed some light and teach us what we could not see through the darkness.
You need sex education 😂
@@catmatism Probably
Just completed Both your playlists on Tensors and Tensor calculus.
It was a very intuitive and logical dive into the world of Tensors -
something that can really help many trying to understand
General Relativity. A proper understanding of Tensors can help many get a better grasp of GR.
I really appreciate all the effort that you have put in making this series .
Thanks. My relativity series is moving forward, albeit slowly.
@@eigenchris Looking forward to it.
I can’t wait for your general relativity series
Overall impressions of the whole series of videos.
I finally reached the end of the series of videos.
I can't believe I ate the whole thing ... like sitting alone in front of a large empty pizza box ...
Yes, I even plowed through the "long boring proof" of the second Bianchi identity of lecture 26 from [10:23] to [16:38]. I found value in seeing a double Lie bracket and using the Lie bracket as one of the inputs of the Riemann tensor. (It remains beyond me how anyone could have managed to establish such a complicated proof.)
A year ago, I was very excited with the first few videos on tensor algebra. So clearly and brilliantly explained. The occasional comment about "some of you might wonder why" came exactly when I was indeed wondering why - as if the teacher was witnessing incomprehension developing ... The explanation of the why was most welcome.
A sense of being overwhelmed started to develop when I realized how much more material there was yet to view. But I persevered, taking notes.
There was a promise of being led to General Relativity.
There was a sort of epiphany when the unit basis vectors where shown to be the same as the directional derivatives. Wow ! And a clear explanation of the infamous λ parameter of parametrized curves with the use of speed and acceleration. Wow again !
I finally caught up on the backlog of videos.
Next, a sense of a loss occurred when no new video was appearing for months.
The level of mathematical complexity picked up but video 25 dealing with the derivative of the volume form really yanked me out of my comfort zone. It really was a nice touch advising that video 26 was the last one of the series. I had been sort of discouraged by the ugliest of all ugly formulas, regarding the volume form. That one truly is ugly as sin.
The sneak preview of the GR field equations was very interesting.
I am not too concerned with the delay to 2020 for the GR series. First of all, this will give me time to review at least the last 10 or so videos - glad I kept such meticulous notes.
And 2020 is now really just around the corner.
In the meantime, I'll also be busy boning up on the Arduino and Raspberry pi.
What a wonderful experiment this all was. A stellar teacher who understands the difference between teaching and mere telling.
Thanks for your detailed feedback. I agree a lot of the Ricci tensor stuff is ugly... but quite a number of sources in physics only leave about 1 paragraph explaining the Ricci tensor and don't explain where it comes from. I found it very very hard to track down sources that explained it. I got about 80% of the way to understanding it and then gave up and posted the videos anyway, since I had already been struggling with it for months and didn't want to waste more time on it. I sometimes wonder if there are any humans still alive who understand it. I hope at least I did more good than harm.
You took the words out of my mouth!
@@eigenchrisyou did ….and,still,do.
Fifteen years ago, I was a physics major, but I couldn't wrap my head around General Relativity, so I switched to experimental physics. Unfortunately, I found experimental physics to be rather dull, and I eventually ended up as a software engineer.
I attended a prestigious high school and then went on to the top engineering university in my country. My best friend from high school, the smartest student in our class, even won a silver medal at the World Physics Olympiad. But even he was baffled by General Relativity and gave up physics to become a dentist.
Had eigenchris been around when I was a student, I'm convinced that we both would have stuck with physics. Less money but maybe more happy.
This truly does feel like the end of a journey. I am happy that TH-cam brought me to your channel recently. I just watched a few of your videos, and got interested in the subject. Then, I decided I actually want to watch the whole series, and take notes. So I did. I religiously watched 1-3 videos per day, taking notes. During the proof of the second Bianchi identity, I started to question that decision. I almost gave in to the temptation of not writing an arrow over my vectors. But I did not.
I am incredibly grateful that you made this video series. It inspired me, along with a few other factors, to change the direction of my undergraduate degree from Statistics to Geometry/Mathematical Physics.
How’s that degree going? And good luck! Wish you the best 👍
@@canyadigit6274 It's going quite well, thank you for asking. This was meant to be my final year, but I will take one more year to catch up on Geometry/physics courses.
Thanks for the kinds words, best wishes to you as well.
I was enthralled from beginning to end of the series. You are a master of exposition. Mega thank you.
Thanks. I'm glad these videos were able to able to help you out.
What a delicious video series from our beloved Eigenchris! Twenty-sex in-depth video lectures on tensor calculus? On youtube? For free? What a delight. Thank you Eigenchris, you are an educational maharishi.
My "Relaltivty" playlist (Special and General) is here:
th-cam.com/video/bEtBncTEc6k/w-d-xo.html
Your videos have changed my life. Thank you for all the hard work you put into them
Great Stuff. Looking forward to the GR course. As Einstein said: “Everything should be made as simple as possible, but no simpler”
Can you something about who you are and what is your background? Where do you teach?
@@joabrosenberg2961 I have an undergrad degree in "Engineering Physics". I work as a software developer. I don't teach anywhere. I never took GR in undergrad, so I decided to try learning it in my free time, but was pretty horrified at some of the explanations and thought maybe I wasn't smart enough to learn it. I tried to learn GR several times over the years, often giving up, taking a break, and then having to re-learn things after I decided to try again. Once in a while, I found "good" explanations for the various concepts scattered over the internet (I've forgotten most of the sources now) and eventually things started to "click". I realized a huge problem is that a lot of GR texts teach tensors using tensor calculus and tensor fields first instead of teaching basis tensor algebra first. I decided to make 5-10 videos on tensors without calculus. In a couple months I had gained about 100 subscribers, so I just kept making more videos, and I've been doing that ever since.
These are special relativity... When will you be making general relativity?
Been making notes on Tensor algebra and have just made it to the end of Tensor Calculus. I am about to go through the relativity playlist but before I do I just want to take some time to give my sincerest gratitude to Chris.
I am about to embark on postgraduate studies in September and I will be studying this stuff more formally. This series has really helped me to better understand all the big ideas in an intuitive way. I feel more confident going into my postgrad studies now. Even Andrew Dotson has rated these videos (especially the Riemann curvature video which was just amazingly explained). You have done a great service to the physics/maths community in making these videos Chris. I give you my most sincere gratitude for going through the hard work of understanding this and arranging it in such a graphic and intuitive way.
Sir, you have done a very noble service for mankind. thank you.
I am deeply impressed by this lecture series. I will return to these lectures over the next couple of months, not only to refresh some of the concepts presented here, but also to take note of how the course is structured and in what ways it outshines most university lectures. Apart from being helpful to students, this is an absolute masterclass in how to construct a lecture series that is both engaging and informative!
There is so much more I'd like to write about the ways in which I appreciated this series, but that would be better expressed in an essay rather than in the youtube comment section.
Finished the series, Eigenchris. Many thanks on your fine work.
You should write a textbook on tensors! In all the years since dropping out of my Ph.D. program in chemistry, I had struggled with understanding tensors. Your video series cured that. I can’t wait to see you general relativity series, and I may just go crack open my old copy of Misner, Thorne, and Wheeler!
at '23 end i finished this series and was middle of relativity
it kinddled some kind of fire in me, idk, im not trying to flex or anythinig, but from april 24 i started doing analysis, algebra and some topology
now im going through langs and rotmanns for modules and tensors, loving each problems from those texts,
im just a vehicle and the path is already there, hopefully im gonna learn some more algebra and topology over the next months and years and decades. such is the quest, but this channel was a massive influence to my journey so imm more than thankful,
just a quote to finish it off
"an unitary associative R-algebra is an R module which also has a ring structure"
this is hymn
Hey man you are a gem to the world !helping the self learners like me.
I would be so grateful if you could provide the notes to these lectures as well like the zip file you provided for 'Tensors for beginners' series.
Notes are here: github.com/eigenchris/MathNotes
Can’t wait for the GR series! Great work!
i would be awesome seeing almighty eigenchris teaching us mathematics of QM..........
I don't think that will happen anytime soon, unfortunately. I don't understand QM very well.
There is no "mathematics of qm" just a shitton of linear algebra.
eigenchris you’d grasp it pretty fast. Look into the canonical quantization.
@@eigenchris i think the mathematics of QM is much easier than of GR but some concepts of QM is very increidable
@@ahmedabdeltawab8408 I took 2 quantum classes and I still struggle to understand basic things like why the momentum operator is -i*hbar*d/dx. The axioms of quantum just seem like nonsense to me. I suppose I could do the math but I have very little clue what it means.
I started seing you series on linear tensors in the first half of 2020, then i wanted to begun this but i didnt haved enought knowledge and needed to focus on my tests to get into university, after the first classes in university i begun reading throw the books and at some point i remenbered this series and realized i already haved the knowledge to see it. Now after a few months of using this as study material i have finaly ended, i cant say enought thanks to you for how much you chaneel helped me learn.
I an not kiding when i say that i learned more from you than from any of my uni teatchers until now. The proff is from my notebooks from college the only one that has a similar amount of pages to yours is the Linear algebra and analytic geometry one, and that one i studied almost solo due to corona.
I watched this video series over and over again till I have some kind of intuition on abstract concepts of tensor calculus.
Without this series, I have no idea how to find a route to climb up the Mt. Everest of General Relativity theory.
On these days, I am also watching your relativity series.
It Is A Great Pleasure To Meet Your New Uploaded Video.
But I recommend you not to hurry - never hurry.
I believe your job is already outstanding.
You don't need to hurry up or make yourself overloaded to prove that your job is outstanding.
Your job is worth to wait.
If somebody complaints that Christopher Nolan or James Cameron are not not so diligent to make a movie every month,
It's not their problem.
So, please take your time.
from South Korea
"But I recommend you not to hurry - never hurry.". Thanks. I often feel pressure to produce videos. But I am glad you want me to take my time to ensure they are good.
Man these videos must take a lot of effort to make. Thanks for the great job Eigenchris.
I am a computer science student and I found this series so useful and I am already thinking how can I solve certain problems with this new toolbox, thank you so much!
Just coming to the end of this series, thank you so much for taking us on this journey! The clarity of your explanations is really exemplary, your course is a gem! And with respect to the somewhat more complex proofs towards the end of the series - with a physics background myself I can live live with proofs that work “in almost all situations”, especially anything that is encountered in the real world, whilst I trust that mathematicians will have put the rare exceptions and extreme cases on a solid foundation.
I can only encourage you to keep going where your curiosity takes you, and continue sharing your learnings!
The following comments may perhaps be useful for some viewers - at some points of the series I used additional resources as a change of perspective helps my learning. There are 2 recent books that I found particularly helpful to complement the series:
The first book would be “A visual introduction to differential forms and calculus on manifolds” by Jon Pierre Fortney with excellent illustrations and step-by-step derivations of the math foundations for differential geometry. The second book is “Visual Differential Geometry and Forms” by Tristan Needham. This book uses a somewhat different mathematical notation that is geometrically inspired and goes back to Newton’s Principia, so this takes some getting used to. However, the practical examples of constructing geodesics or doing parallel transport on the peel of various fruits are really fun and helped me visualise some concepts better. The history excursions are fun, too.
Wow! This was tough staff, but you made it comprehensible and enjoyable (without compromising rigour). Quite a feat. Looking fwd to watching the GR videos!
I'm really grateful to you for this series. I've always been fascinated by General Relativity, unfortunately many people always that one needs a really deep mathematical background, which is not my strong point, to understand this theory. But after watching your videos, I realized that while it does require some mathematical knowledge, it's not as complicated as people say (at least the basic concept). And this series will definitely help me in my exam next month. For this I would like to thank you once again
Just finished your video series and I want to say thank you very much! Great explanations.
This video series was too good! Thanks for making such detailed visualisations with examples, it really really helped a lot! THANK YOU!!
Fantastic series! Looking forward to the new series, your method of explaining these concepts is unparalleled!
I've come this far from Functions in 8 months. I don't know if it's a big job or a small job, but I thank everyone who helped. Exist. Now we are one step closer to our goal. There is no stopping until we reach our goal. Shame on those who do not stop. IN DURDURANA
Please take your meds before posting Publix comments
Hi Chris. I think that your general proof of the second Bianchi Identity is totally Heroic! 😅 Thankyou. Dr-J
Thank You so much Chris!! You have explained these concepts in an amazing way. I have learnt a lot from your video series. Keep up the good work.
You have already so many gratifying comments, but I can't help adding mine: for both algebra and calculus you made a VERY VERY WELL DONE JOB! I never had such a clear explanation of vector spaces and all the attached stuff. Thanks a lot. Looking forward your GR video series...
I'm still happy anytime I hear these videos make people's lives easier. Glad they helped.
This series has been wonderful! It really helped me to put pictures and meaning to all the math. I look forward to your general relativity videos! ❤
Wonderfull work!
This is the best tensor lessons to understand what it really is and to use it. I tried by reading some books some years ago but I've never get the essence before seing your channel. Thanks!
Great playlist, I think I understand tensors better now, thank you!
This is really the great works of Tensor calculus and the foundation to GR.
Absolutely well structured and best step by step approach to understanding tensor calculus
Could you please suggest a research topic that builds systematically from the tensor calculus ? That will make it easier for me
What do you mean by "research topic"? For your free time, or for school?
@@eigenchris Hello, i meant by topic for writing a thesis for school, thanks for your reply
@@GeminiAnu I'm not really sure what the scope of your thesis would be. One of the main applications of tensor calculus in physics is general relativity. You could do something about that. I'd probably as one of your professors for advice.
@@eigenchris thank you so much. I'll do as you mentioned.
Great series man.. I was struggling in understanding tensor calculus for two years.. Now it becomes clear to me. Thanks for this. Waiting for General relativity series..
Working on the relativity series now. Starting with Galilean and Special Relativity.
Again, very nice video series. You are the best!
For those who are getting a little impatient, look here for more on General Relativity: th-cam.com/video/7G4SqIboeig/w-d-xo.html
Getting productive! Thanks for the new vid, now I am falling behind.
I actually finished this video before the other two, which is why it came out so fast.
it was really helpful , its worth watching this lecture then going to university every day and wasting time there.
And wasting money there
@@nellvincervantes6233but you ain't gonna get no cert.
Finally completed the series. Great stuff.
Enjoy your videos so much! Also happy with myself to make to your last video in tensor calculus🙂
@eigenchris Hello sir , Plz tell me - at 11:55 what is difference between Nebla z [R ( u,v) w] and
( Nebla z R )( u,v) w notations
Suggestion for your upcoming series on GR : an explanation of the Mars perihelion and how GR solves it. And no, you definitely do not have to be concerned with how much time you need to create the new series. You are the master of your own time and we'll get what you give when it is good and ready, period.
Do you mean the Mercury perihelion precession?
Mercury's precession was the experiment that acted as a test/proof of Einstein's General Relativity.
Yes this is what I meant - I should have been more careful writing this.The importance I gave it is that it was mentioned in a TV series when Einstein stated something like "it also explains the precession of the Mars perihelion and the theory is complete".The answer is that solving the field equations creates a new term in the standard Newtonian equation for the Mars orbit. I would love to see this derivation explained in detail.
lots to consider here.. but glad i completed the series! gonna do some light courses on spinors… maybe one day soon i’ll be able to implement something cool with all this knowledge of tensor calculus!
Thank you so much for this series Chris, this was very useful. Can't wait for your GR series.
9:16,how do you know which connection coefficient relates to point P?
Similarly,at 9:36,how come some of the connection coefficients reduced to zero and others didn't?
How do you distinguish?????
Everyone here is a genius! You and I are the only dummies who have asked this question. Perhaps, however, I have understood. At point p, the gamma connection coefficients are zero, but the derivatives of the gamma are not zero, since the value of a variable at a point is one thing, the variation of that variable at that point is quite another. In fact, the gamma are zeroed when they are factors, not when they are arguments of derivatives.
Someone please tell me how much nonsense I have written!
Awesome series.
Finally come to the end
thank you for your videos !!!
Thanks a lot for your fantastic explanation!!
Hi Chris. At 20:00, why can you raise & lower indices on the right side of the semi colon? I see why you can do it on indices to the left of the semicolon as you showed earlier in the video. Thanks in advance!!
EDIT: Sorry, not raise & lower, but just change letters via kronecker delta. Question still remains - why can you apply kronecker delta to the basis vector direction on which the covariant derivative is acting on R?
R; _n is just like a row vector whose column entry is denoted by the "n" index. The kronecker delta δ^n_l is just like an identity matrix. We're basically multiplying a row vector by an identity matrix. And since the index letters are arbitrary, we're always free to change them. Does that make sense?
Thank you eigenchris!
first thanks for all your effort and hard work you have done at this course i want to know from you the name of a best textbook that you see in your opinion is good and explain easy as your style of explaning at tensor calculs i trust your opinion very much thank you sir very much ❤
I don't have any single recommendation. I learned from a number of different sources and webpages.
A question about the proof of the second bianchi identity. You proved it at first in local inertial frame and after in a general case. But since these are tensorial relations, proving them in one coordinate system shouldn’t be enough to be true in any coordinate system, since tensorial relationship shouldn’t change changing coordinate system?
Thank you for making this series.. 👌👍
Bravo! Great series!
i feel like sometimes that field equations are dimensionally inconsistent...because on left we have curvture and on the other side we have energy....dont both have different dimensions? i know i am wrong ...correct me(by the way....very nice vedio)
Yeah, curvature (Einstein tensor specifically) has dimensions of m⁻², while energy-momentum tensor has dimensions of energy per volume (J⋅m⁻³), but we have another constant factor of 8πG/c⁴, which has dimensions of m³⋅kg⁻¹⋅s⁻² / (m⋅s⁻¹)⁴ = m³⋅kg⁻¹⋅s⁻² ⋅ m⁻⁴⋅s⁴ = m⁻¹kg⁻¹s² = m⋅J⁻¹, so actual equation reads m⁻² = m⋅J⁻¹ * J⋅m⁻³, which is certainly true
I never noticed this, but you are right. I'm not sure what the solution is, because the units on either side of the equation disagree.
Great video as always!
YES
Great lecture.
Well done.
when will you upload lectures on general relativity??? will you talk about the energy momentum tensor in your upcoming videos??
They won't start until sometime in 2020. Yes, I will talk about the Energy Momentum tensor.
Hi eigenchris,
I really enjoyed watching your tensor calculus videos and learned a lot and new concepts on how to look on already familiar things.
May I propose an Idea to you:
In the end and sometimes inmidst of your videos you have these nice summary slides. Could you make them available to your audience (not just for me of course) in PDF format or something similar?
Now that I am learning GRT in master courses I wish I had your formulas summed up. Since this is a lot to ask for and will cost you extra working time, I'd definitely drop you another cups of Coffee for that.
Even if you dont like that proposal or dont even have time for that, still thanks a lot for these high quality lectures. :)
I have the slides from the fist 20 video here: github.com/eigenchris/MathNotes (in Microsoft Office .pptx form, but those can be exported to .pdf).
The slides for the last 6 videos are scattered around in old drives so I'll have to take some time to get them together.
@@eigenchris oh yes, thx, what a goldmine
How do I linearize the Ricci tensor according to the metric? When it comes to gravitational waves in flat space, Einstein's field equation is rearranged according to the Ricci tensor. Then you assume that you are in a vacuum and therefore the energy-momentum tensor = 0. So you get Ricci-Tensor=0. Now we linearize this at the point of the Minkowski metric and obtain D`Alembert operator of the metric tensor =0 and thus a linear wave equation. I have not found anywhere how to do this. I would like to know how to linearize the Ricci tensor in other metrics. For example, when gravitational waves propagate in the Schwarzschild metric.
Dear Eigenchris
Will you speak about coordinate basis and non-coordinate basis and tetrad formalism on the next series?
How to derive that "ugly formula" at 1:22 sir?
I explain this is Tensor Calculus videos 22 and 23.
Ok sir thank you. Ill check it
can't wait for the GR series!
Hey Eigenchris, Thanks again for uploading such a clear and well-presented course! I was just wondering - what sources did you find most useful in learning about Tensors and Tensor calculus? I have been looking for a good resource for intuition on the push back/pull forward and the wedge and double wedge product and was wondering if you had come across any whilst making your videos!
I think this playlist by David Metzler is the best introduction to those topics that I've come across: th-cam.com/video/M5wrnwlm8lw/w-d-xo.html. It's a bit on the longer side, but he does go through lots of examples. (Though I'll say I've never heard of the double wedge product and I don't think he covers that). I'm hoping to do videos on the wedge product and exterior derivative before the end of 2020, myself.
As for how I learned... I basically just googled nonstop until I felt I understood it. I think I left some links in the description to some PDFs that helped me. I've never gone through a textbook cover-to-cover. I tend to just skip to parts I want to learn about and see if it helps, and if not, toss it and look for something new. You can also check my "About" page for additional links.
@@eigenchris Great! Thank you I will look into those! Yes - definitely looking forward to those videos! This is definitely the best and clearest course I have come across on Tensor calculus by far!
Thanks for your lecture, enjoy the ko-fi.
Could you do a video on the Weyl tensor? Awesome videos! Keep up the good work!
I don't have plans to in the near future. It seems pretty complicated and I don't feel like investing time in learning it right now since it isn't needed for the basics of general relativity.
as far i am concerned, u dont deserve a coffee...u deserve all the cafè!
When contracting the Ricci Tensor, this is a 2 times covariant tensor, right? Thus. before contraction we need to use the metric tensor to transfrom it to a 1,1 Tensor. What is the correct formula for the resulting scalar (Ricci scalar) ? For 2 dimensions: R11*g11 + R21*g21 + R12*g12 + R22*g22 ? We need to multiply the "row of rows" (Ricci Tensor) with a "column of columns" (metric tensor), right? It should be the trace of "the matrix", but I'm too dumb to find the correct answer. Could you please enlight me? THANK YOU!!
Thanks for all! =)
Hah :) Some time ago I wasn't sure if I would go through this playlist... thought the tensor algebra would be enough. But here I am. And I'm certainly moving to the general relativity playlist. Woo-hoo!
Many little gems of insight here! Thank you.
Do you suppose that the conservation laws for T was a key element in Einstein's search for the modification of R that would also have zero covariant derivative?
As far as I know, Einstein's original publication of the Einstein Field Equations did not have a "modified R" term. It was just R_uv = 8πG/c^4 T_uv. He was able to use this to calculate the perihelion advance of Mercury's orbit (since the extra "modified R" term conveniently went to zero in that special case). But it was later pointed out to Einstein that his equation violated conservation of energy, and so he added the "modified R" term to fix that. I also have a playlist on Relativity that covers this in a video called "Relativity 107f" if you're interested.
@@eigenchris Fascinating!
Your question is one that I had for some time. Eigenchris points out (indirectly) in his reply to your question that Einstein was alerted (I understand it was by David Hilbert) that Energy was not conserved in his original formulation of GR. So, noting the Bianchi Identity, Einstein added the Ricci Scaler term which then satisfies Energy Conservation. Much later, I realized that in study of Cosmology that photons loose energy during the expansion of the Universe. WHAT? Turns out that Energy is only conserved Locally not Globally in GR. Eigenchris's work here and much later in his Cosmology videos, I have found just how valuable his videos are, how well they are produced (few mistakes) and how well he explains his subjects.
@@eigenchris Yes, this is a correct understanding. Yet, as I have commented below, Energy Conservation guided Einstein to a correct formulation of GR yet Energy is not globally conserved in GR - as in the Expansion of the Universe.
Wow what a great series. Just one question. I found the choice of indices somewhat confusing at parts. I watched the whole series and the tensor algebra but I'm still confused about how to choose the indices of the terms confusing especially when multiplying by new terms. would you mind referring to a text or source for clarification?
Thanks. What do you mean by "choose the indices of the terms"? Can you clarify?
@@eigenchris ok so I guess just to use 2 instances that I remember. in Tensor for beginner part 8 at 3:17 you derived how the linear operator transforms under the change of basis. first starting with the telda basis then replacing each term until you get the FLB for the order of the operators. If i understand correctly, each time the top index of the operator matched the index of the basis it was acting on. The order in which we do this gave us FLB and the lower index of each operator matches the next operator's top index however you wrote down BLF. If i understood correctly the top index represents row of operator and bottom represents column and since for matrix multiplication we do row of the left operator times the column of the right operator shouldn't the correct order be FLB to find L_telda? If i'm not mistaken the order does not matter in index notation since they just represent the entries of the matrices but given we wanted to perform matrix operations to find L_telda it should be equal to FLB correct?
Similarly in another instance in tensor calculus series part 17.5 at 9:00 you start with the expression of the covariant derivative and on the 2nd line you perform chain-rule on terms on both sides of the equation. the index for p in the left and right hand side are "n" and "m" but I'm not quite sure why they have to be different or why they couldnt have been another one of the existing indices.
In general i'm confused when having a different index means we are referring to another term and when it represents that we are summing over that index.
sorry about the long comment
FUCKING UPLOAD ALREADY IM TOO EXCITED
Hi Chris. What books do you recommend on tensor calculus and differential geometry for self-study?
you keep calling R superscript mn the Ricci Tensor.But i thought Ricci Tensor should be subscripeted?The superscripted version should be the Ricci Tensor that’s raised to superscript by virtue of the Inverse Metric Tensor.
So is it just colloquialism?
People tend to say "Ricci Tensor" for any combination of raised/lowered indices. I'm doing the same here.
First of, great series! Truly outstanding.
Secondly, would it be possible for you to maybe upload these slides, so we can download them.
I know there are some of them already on you Github page, but I am talking about the rest.
Thank you!
The problem is that the presentations are in pieces on my laptop due to multiple versions and edits.. and I need to reassemble them. If you have any favourite videos, I can focus on those first, but it will take time to get them all.
@@eigenchris Oh, that's too bad.
As for 'favourite' videos, not paticularly.
In this case I guess it would make the most sense to just continue doing them in order.
Thank you for your response!
Thank you so much! Can you add a video on frame formalism along with Cartan-Riemannian geometry?
Thanks Unfortunately I don't know that geometry so I can't make a video on it.
@@eigenchris okay thanks anyway your videos are priceless
Hey - I was wondering if you had any books with good exercise sets for this and your other series? Thanks!
A big weakness of mine is that I do very few exercises and just look at proofs/examples to makes these videos. I read parts of Gravitation by Misner, Thorne amd Wheeler to learn about tensors and I know that book has exercises, but I can't say if they are any good.
Just to whet our appetite : can you publish a rough outline of the topics your upcoming GR series will cover ? How many videos ?
Regards
I don't want to get your hopes up too much. I will not start work on these until 2020. But my rough plan is:
Intro (1 video), tensor algebra reveiw (1), special relativity (1), differential geometry review (2), assumptions of GR and einstein equations (1), schwarzschild metric and black holes (2, maybe 3), expansion of the universe and cosmological constant (1), gravity waves (1).
Hello,
Your series is very helpfull!
I would like to ask if you can recommand me a book about GR to understand it in a deeper level.
Thank you for your time!
There is Gravitation by Misner, Thorne and Wheeler, but it is very thick and very detailed, perhaps hard for a beginner. Professor Sean Caroll has notes from his General Relativity course online.
Hello Chris, I plan on writing some tensor calculus notes and would like to use your videos as a source, giving full credit, both in the document and in the page linking to them. Is that okay? I could not find any other way to contact you.
Thanks for the great videos!
That's totally fine. Thanks for linking back to the source material.
@@eigenchris Thanks a lot! When it is finished I'll link you to the material, if it ends up being in English.
So all these videos are enough to start studying general relativity ??
I've been kind of misled by the assumptions that we can equalize G_mn and T_mn based on the fact that theyr's both derivatives are 0. Following this logic we actually can equalize any other things that has 0 derivative. Why can't we equalize g to T_mn?
I have a video called "Relativity 107f" which does a more thorough derivation of Einstein's equations. The idea is to generalize Poisson's Equation, which says "△φ = 4πG ρ". This says the Laplacian of the potential φ is proportional to the mass density ρ. But these are not lorentz-invariant quantities. If I Lorentz transform to a frame with a different velocity, the density ρ will be different in that new frame.
To make it relavitistically invariant, we replace △φ with Ruv and replace ρ with Tuv. This gives us Ruv = 4πG Tuv, which is almost right. However, the divergence of Tuv is zero, and the divergence of Ruv is non-zero. So we add the extra 1/2 R guv term to make both sides have zero divergence. I'm not trying to say any rank 2 tensors with zero divergence are equal.. The idea of making Ruv and Tuv equal (or "almost equal") comes from Newtonian gravity.
When can we aspect the new series ?... sir.....
I'm sending a rough draft of my next video to some friends today. I think it's reasonable to expect it on TH-cam by early March.
thinks for this courase; its very great
Could you explain Navier-Stokes equations ?
I can't sorry. I never studied that.
@@eigenchris Okay, no problem
On other sources the indices on all sort of tensors in Field eqn. Are covarient .why?..
I normally see the Einstein Field Equations written wity covariant tensors. But you can always raise or lower thr indices using the metric tensor. Does that answer your question?
You should write a Book! (by the way, if you already have one then I want to buy it)
Thanks. I don't have a book. Maybe one day I'll combine all my videos into a PDF of some kind for downloading.
16:33 w is there...i guess that's not to be, according to 6:43
Dark Energy and dark matter are very controversial in theoretical physics as to date there has been no empirical detection of the same.
The recent Null-experiments to empirically detect SUSY WIMPS and Axions has sent theoretical physics back to the drawing board regarding the physical explanation of dark matter.
Obviously, there exists a principle which theoretical physics has not yet imagined nor discovered.
Can you please explain lie deivatives
I don't really understand Lie derivatives either, unfortunately. I haven't studied them. Is there anything in particular you want to know about them?
one of the methods for controling nonlinear systems is feedback linearization and lie derivatives used to linearize the system feedback it is robotic and aerospace applications I had spent months studying differential geometry as fundamental concepts for geometric control and your classes are so helpful thank you very much
I don't think I'm the right person to talk about that. I don't understand the Lie derivative or its application to feedback linearizattion.
th-cam.com/video/HG3TTsx8PR0/w-d-xo.html
try this link
Awesome
Sir , one example for each new concept.
I made it!