@StudyAcademic You obviously don't understand relativity then. The fact that GR distinguishes between proper time and coordinate time is one of its central relativistic features. All of SR applies in local inertial frames in GR.
@ozkansafak I'm not sure if I've got this right, but I think the ordinary derivative describes the change of a tensor relative to a particular coordinate system. The gammas describe how that coordinate system changes relative to the metric. So if the metric causes the coordinates to change, that will change the tensor, which should remain invariant. So you have the gammas to account for any change to the coordinates due to the metric.
Of course, I could be totally wrong about all that.
@SpiritualAtheist The christoffel symbols account for the change in the bases for the particular coordinate system. In Euclidean 4 - space one does not need to worry about this because the bases are orthonormal but this is not true in general such as in spherical polar coordinates. Therefore, the covariant derivative accounts for the relative change of the basis vectors and/or dual basis vectors.
@ozkansafak Because its the change of the Tensor's components relative to the coordinates. If it was a Tensor then it should be 0 in all coordinate systems if its 0 in one. However a Tensor that is constant in one coordinate system could be varying in a different coordinate system simply because the axes are varying.
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@oringent You can't jump into maxwell's equations without knowing what divergence and curl are. You can't jump into quantum mechanics without knowing what wave equations are. You can't jump into general relativity without knowing how tensors work.
He might have been operating with affine connections which are the negative of the ones you would normally see. However at 1:10:00 he uses the usual sign for the Christoffel Symbols. Therefore I guess Susskind made a small error. All the same he is a great lecturer.
All of my tensor calculus books state the covariant derivative of a covariant tensor has a negative sign in front of the gamma and the covariant derivative of a contravariant tensor has a positive sign. So did Susskind make a small error when he wrote down that version or am I just misunderstanding?
FYI. Whats important to note here is that the Christoffel symbols represent the forces, not just gravitation, ergo the many different symbols with set values attached to each. So the symbols (values) may remain constant, even though spacetime (the metric) around it may be changing. The term connection symbolizes the constancy whether in flat space or curved space. Laws are universal, gravity fields change.
Just so you know, over the 5 lessons so far, we have covered Gauss (extrinsic geometry), Riemann (the metric), Minkowski (d(tau)^2 products), Ricci-Curbastro/Levi-Civita (covariant calculus) and now Christoffel (forces in tensors). Einstein has yet to rate a mention. The field equations (later) came from Hilbert who was himself working on gravitation.
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True but my case is not against women but rather my case is that we often dismiss what we do not understand as "boring". We value what is instantaneously stimulating more than patience and learning and self discovery.
wow....these are most excellent!!! I wish I saw these at the beginning of the year....sitting my relativity exam next week!! thankyou prof susskind!! excellent.....everyone should know about these lectures!!!
I'm confused about one point. He says that the word covariant in covariant derivative has nothing to do with covariance as in covariant tensor. But I understand that taking the covariant derivative of a tensor yields a tensor with one more covariant indice; increasing the rank of the tensor by one. He has totally avoided this notion by using del ?? I am used to the comma notation.
Thank you for giving me a view into a world I've had an interest in since my undergraduate days but have never had the time to study seriously. Your Physics Videos are a real joy and I might add, a powerfull motivator. Thanks again.
Thank you for posting these. I have been learning this on my own and missed some of the basic ideas. Please post the rest, I really thank you for posting these.
The few ideas I missed by learning on my own were conceptual Ideas that really make a big change in how I Understand GR.
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Kicks ass just by listening to it.
grunder20 1 month ago
I get a kick everytime he says "everwheres"
sssandhu78 1 month ago
nice one! thanks
adelle0001 2 months ago
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My head hurts, but I'm letting it be because this is Einsteins work!!!
grunder20 2 months ago
Einstein id my idol. I bet he's the professors idol too. LOL
agapitoflores001 2 months ago
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I want my mommy.
csmcmillion 4 months ago
I got an A- in this course.
EinsteinsApprentice1 5 months ago
Susskind drinking game: take a shot every time he says "everywheres"
necroforest 6 months ago
Views decrease as the no. of lecture increases!
gikiian 6 months ago 4
Which textbook does he use?
gikiian 6 months ago
Comment removed
csmcmillion 4 months ago
@gikiian None. He gives the class copies of his notes.
csmcmillion 4 months ago
Ha ha, the crowd is still. That's Funny :) (in some way)
jpknie 6 months ago
what is gamma?
StudyAcademic 7 months ago
General Relativity is all about Calculus and Tensor Calculus...no relativity at all
StudyAcademic 7 months ago
@StudyAcademic You obviously don't understand relativity then. The fact that GR distinguishes between proper time and coordinate time is one of its central relativistic features. All of SR applies in local inertial frames in GR.
floopsie666 7 months ago
@floopsie666
I know but it's 5th lecture and all he talks is some tricky mathematics. He doesn't talk about relativity at all.
I've got a question: why time slows as you move faster? how can time slow down or stop?
StudyAcademic 7 months ago
@StudyAcademic it slows to protect the cosmic "speed limit" what is the speed of light, so it slows down so u cant go over that
bigbobgotu 3 months ago
Do they have lectures past Lec. 7?
ClamCrunchy 8 months ago
why is the ordinary derivative of a tensor not a tensor ?!? Didn't get it..
ozkansafak 9 months ago
@ozkansafak I'm not sure if I've got this right, but I think the ordinary derivative describes the change of a tensor relative to a particular coordinate system. The gammas describe how that coordinate system changes relative to the metric. So if the metric causes the coordinates to change, that will change the tensor, which should remain invariant. So you have the gammas to account for any change to the coordinates due to the metric.
Of course, I could be totally wrong about all that.
SpiritualAtheist 8 months ago
@SpiritualAtheist The christoffel symbols account for the change in the bases for the particular coordinate system. In Euclidean 4 - space one does not need to worry about this because the bases are orthonormal but this is not true in general such as in spherical polar coordinates. Therefore, the covariant derivative accounts for the relative change of the basis vectors and/or dual basis vectors.
floopsie666 7 months ago
@ozkansafak Because its the change of the Tensor's components relative to the coordinates. If it was a Tensor then it should be 0 in all coordinate systems if its 0 in one. However a Tensor that is constant in one coordinate system could be varying in a different coordinate system simply because the axes are varying.
GammahooX 7 months ago
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ozkansafak 9 months ago
Comment removed
ozkansafak 9 months ago
If the theta component is 0, the (unit) vector should lie on the x axis.
wizardofmadness 9 months ago
lol How these students concentrate for almost 2hrs sitting in a Lecture. A BIT TOO MUCH I Recon.
gur0004 1 year ago
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REAL Free energy technology exists!But the powerfull Oil business won't alow common ppl to know this,Find a motor that needs no fuel or input at LT-MAGNET-MOTORdotCOM ,Big change is comming soon!
urgencyharviefcem 1 year ago
He's a fantastic teacher!
bhigr 1 year ago 2
lol 5 lectures on general relativity without any general relativity
oringent 1 year ago
@oringent You can't jump into maxwell's equations without knowing what divergence and curl are. You can't jump into quantum mechanics without knowing what wave equations are. You can't jump into general relativity without knowing how tensors work.
floopsie666 1 year ago 2
@floopsie666
Well said. To study general relativity usually means one has to study tensor calculus first.
lukequixotesanjose 1 year ago
most questions asked are not really questions.
SpecterReflector 1 year ago
omg this is the longest video i ever seen!
keycomedy 1 year ago
@keycomedy You mean you've never seen The Return of the King? You poor thing! :P
fermista 1 year ago
He might have been operating with affine connections which are the negative of the ones you would normally see. However at 1:10:00 he uses the usual sign for the Christoffel Symbols. Therefore I guess Susskind made a small error. All the same he is a great lecturer.
EsatBrahimLodi 2 years ago
All of my tensor calculus books state the covariant derivative of a covariant tensor has a negative sign in front of the gamma and the covariant derivative of a contravariant tensor has a positive sign. So did Susskind make a small error when he wrote down that version or am I just misunderstanding?
ExhumedANDConsumed 2 years ago
@ExhumedANDConsumed
So your connection coeffincents are minus his coefficients;). That doesn't change the math;)
Cheers
grootkanoniek 2 years ago
And mathematics isn't reality either! Of course they're not THE forces.
ShootBigBird 2 years ago
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this is great period!
elliottc2001 2 years ago
lol that dude asking questions is a total tard
ibreakkidslegs 2 years ago 5
There's always one tard asking stupid questions.
mizantrop12 2 years ago
yea i noticed. im auditing a GR course this year and we have an old tard asking stupid questions
ibreakkidslegs 2 years ago
This guy is a fucking great teacher.
greg5566 2 years ago 6
hes brutal at putting equal signs where they shouldnt be
ibreakkidslegs 2 years ago
FYI. Whats important to note here is that the Christoffel symbols represent the forces, not just gravitation, ergo the many different symbols with set values attached to each. So the symbols (values) may remain constant, even though spacetime (the metric) around it may be changing. The term connection symbolizes the constancy whether in flat space or curved space. Laws are universal, gravity fields change.
ShootBigBird 2 years ago
Just so you know, over the 5 lessons so far, we have covered Gauss (extrinsic geometry), Riemann (the metric), Minkowski (d(tau)^2 products), Ricci-Curbastro/Levi-Civita (covariant calculus) and now Christoffel (forces in tensors). Einstein has yet to rate a mention. The field equations (later) came from Hilbert who was himself working on gravitation.
ShootBigBird 2 years ago
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TruthLogic 2 years ago
This comment has received too many negative votes show
the staement fucks up.
i can it better
winfriedstar 2 years ago
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so boring...
someuser91 2 years ago
Anything we don't understand is boring. It's the same reason that a lot of women don't like football.
forgotaboutbre 2 years ago
women understand football. they just don't see any sence in watching it.
12elza12 2 years ago
True but my case is not against women but rather my case is that we often dismiss what we do not understand as "boring". We value what is instantaneously stimulating more than patience and learning and self discovery.
forgotaboutbre 2 years ago
wow....these are most excellent!!! I wish I saw these at the beginning of the year....sitting my relativity exam next week!! thankyou prof susskind!! excellent.....everyone should know about these lectures!!!
listminusv 2 years ago 7
I'm confused about one point. He says that the word covariant in covariant derivative has nothing to do with covariance as in covariant tensor. But I understand that taking the covariant derivative of a tensor yields a tensor with one more covariant indice; increasing the rank of the tensor by one. He has totally avoided this notion by using del ?? I am used to the comma notation.
sodiumcrapolate 2 years ago
methinks del is the same as using the comma
listminusv 2 years ago
This is really a very generous gift to the community of those interested in learning. Thank you for posting these videos, professor!
KinStrategy 2 years ago 50
mez lernd lots tank ya vry moch!
djwalsh101 2 years ago
lol...I thought the tracker was broken...o.o Because the video is so long. xD
xCookiex3 2 years ago
Is it true, that you can actually represent any visual object as a mathematical equation???
EuroCarfan00 2 years ago
i think this is stupid question...
cr3rzemJest 2 years ago
THANKS FOR THESE VIDEOS
elmeromero123456789 2 years ago 2
He sounds like Christopher Walken!!!
SixFt12 2 years ago
thanks 4 postin' these videos
irfaanfr9 2 years ago 7
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fuck school nigga, im a be a dope dillah!
eigilmus 2 years ago
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fuck school,edu,learning,univerity and usa
enahurr 2 years ago
Thank you for giving me a view into a world I've had an interest in since my undergraduate days but have never had the time to study seriously. Your Physics Videos are a real joy and I might add, a powerfull motivator. Thanks again.
dickbeck 2 years ago 4
are you nuts?there is a on hour video!
rusurazvan 2 years ago 2
Thank you for posting these. I have been learning this on my own and missed some of the basic ideas. Please post the rest, I really thank you for posting these.
The few ideas I missed by learning on my own were conceptual Ideas that really make a big change in how I Understand GR.
Thanks again !!!!
russelljbarry15 2 years ago 3
thank you for these videos, could you please please please please upload the rest. thanks once again
clearview007 2 years ago 8
I'm looking forward to seeing the remaining videos once they get uploaded!
1234spankymc 2 years ago 16
Can you please upload the rest of the lecture series? I am really enjoying these videos. Thanks.
1234spankymc 2 years ago 7