Einstein's General Theory of Relativity | Lecture 2
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- Опубліковано 21 січ 2009
- In this lecture, Professor Leonard Susskind of the Stanford University Physic's Department discusses dark energy, the tendency of it to tear atoms apart, and Gauss's Law.
Einstein's Theory (PHY 27) discusses the different applications of Einstein's Theory of Relativity in particle physics, including Newtonian, Galilean, and Guassian laws; particle attraction and repulsion; gravitational fields; and dark energy.
Physics Department at Stanford University:
www.physics.stanford.edu/
Stanford University:
www.stanford.edu/
Stanford University Channel on UA-cam:
/ stanford
[Dark energy - not related to the course]; Del operator 15:00; Gravitational field and Gauss law 21:00; Gauss theorem 32:00; Equivalence Principle 59:30; Galilean transformation 1:09:00; Accelerating frame of reference 1:12:00; Light motion in accelerating frame 1:18:00; Tidal forces 1:32:00; Curvature 1:37:00
For all of you who say these students ask stupid questions:
"We must know. We will know." - David Hilbert
Asking questions is never stupid. Not asking questions for fear of sounding stupid. Now, that's really stupid.
morani789 that’s such a moronic position, most questions are extremely stupid and shouldn’t be entertained in a serious environment
morani789, those students are not prepared for this class, and the level of this class is not high, but their level is low.
I think they approach it from an opposite direction in perceiving the concept'sas myself . I see a concept in my mind and attempt to put the math to it. Others with a more mathematics background I think may see the equation and from that derived the image in the mind.
I thought the same at first but I was a 4.0 physics major, not mathematics. I can't expect others to see the concept's presented as quickly. That doesn't lesson their questions however. Koodos to the students. It a challenging concept to truly grasp.
I think if we look at it as people just discussing things instead of as a “physics lecture”, then we won’t be so annoyed by the questions :)
Stop defending the indefensible. Some of these questions are atrocious. Really dumb.
This professor is SUPREMELY patient. The student asking the questions over and over again is justified in asking. He paid for the course. He has every right. But he also needs to be getting his notes out and trying to solve on his own. Otherwise, he's just asking for the prof to do his work for him.
Point well taken....I must agree with you here.
Totally agree... but I'm thinking of the other tuition paying students; it does get annoying.
It just disappoints me that they are paying for this class and aren't even enjoying his great physics puns.
visnevskiscom "Information presented in a particular way" is, by definition, a service. But also, it was a joke.
The student was looking at his notes but must have not paid attention when the professor canceled the 4pi, the when he looked at his notes to catch up.he was like, but wait professor ☝
Thanks Stanford University for posting these lectures
I know.....students pay a lot to be at this seat of learning....so to give this away for free is generous.
All this to disprove the flat earth
10 year old comment jesus christ
@@mattwooten830 you are on the good drugs
All they know the Einstein's stuff is just a HUGE HOAX that has been devealed at: numbermusicrevolution.com/srt/ Indeed, Einstein's lies allowed many institutions and scholars to rise so much funds rising, so they are not willing to kill that Golden Chicken. Notwithstanding, all this hoax has to come to and end, sooner or later, and many people will have to face justice.
he is so patient and calm while giving lecture
I can’t get enough, this is my idea of finding the bright side of life. Free class at a university I couldn’t afford. I’m loving it🤭😍🥳
The finishing sentence of this lecture gave me a real breakthrough in understanding. In all of these series of lectures, how can anyone thank Prof. Susskind enough for his generosity of spirit?
Robin Betts One of his books (forget which) mentions the great pleasure he gets from teaching physics , for which I'm eternally grateful.
Seriously this guy is great!
Do you mean his line that curvatures in spacetime are equivalent to tidal forces? Or a different line?
@@andrewmartin3671 1:47:16
@Andrew Martin
Not sure what Robin Betts meant, but yeah, that was an enlightening insight right there for me. Or at least it makes me feel like I understand something important which I previously did not.
I admire the clarity with which Prof. Susskind can gauge the right moment to feed such illustrative central points of insight to the audience so they can make the connection. Even when he's getting tired.
A great teacher!
Heartfelt thanks to Professor Susskind and Stanford for making these beautiful ideas available to me. I am following all of the series.
life passes by as i try to understand this 'introduction'
This is an advanced undergraduate or early graduate course, to be able to grasp the concepts you need a foundation of college level calculus of several variables.
We're coming into a new era with the internet education. Susskind is one of the greatest teachers available, togehter with a handful others, and I'm very grateful that his lectures are freely available online.
I'm 40 yo, regrettably didn't find physics back in the school days, but I've had an exploding interest in physics the last 3-4 years. Now there's the math barrier - luckily, I've taken all the required maths during my education, so some refreshment is needed.
This is some hardcore stuff. I feel so humbled watching this haha. I think I can barely understand it but man its a mindfuck. Its very warming to see that people like the professor not only understand it, but can teach it. And this is only an introduction to relativity!
The depth of questions that Professor Susskind has to bare and answer is.. nerve-challenging. Hats up for this remarkable professor for his beautiful mind and personality.
Thank yo u to Leonard Susskind for these lectures. I wish that my physics lecturers 40 years ago at Oxford had covered this!
Thanks for posting these lectures by Dr. Susskind
Alternative form of the calculation of gravitational acceleration at a point inside a spherical mass.
A = m G / r^2 which in terms of whole sphere is: A = n M G / R^2
R : Radius to point on surface of sphere
r : Radius to point inside radius of sphere
n : Ratio of r to R
I want this guy as my professor.
Haha... I'm a MSc student now and I'm planning to apply for my PhD. But I'm not a physicist, so he won't be my professor either way I look at it.
not a problem - 75 000 USD per year and you in Stanford.
If you continue watching this series... Than he is your prof.
Is he still teach at Stanford, I really want to meet him, just once time =)
You're not alone.
the presentation is well organised and the lecturer too, i think he deals well with his students. i like the way he handle question, is been enlightening lecture.on relativity.theory.
The case where red sphere is inside A question in the class is that a 4*pi is missing from the equation. I think the reason for this would be like this:
by dissolving guass theorem we get- 4 * pi *G * integral(rho * cube(dx))=Aperpendicular*- 4* pi * R2.
Now as explained by the sir this case has a unit mass density uniformly distributed. so the equation can be written,
=> 4 * pi *G* rho* integral(cube(dx))=Aperpendicular* -4* pi * R2. As you can see that rho in the integral is taken out of the integral.
the remaining integral would be volume of the red sphere. so,
=> 4 * pi *G* rho* 4/3 * pi * R3=Aperpendicular* -4* pi * R2
=> 4* pi * G* rho * R/3 = -Aperpendicular.
Now if you check this equation with the one on the right board these would match and no extra pi is missing.
Outside sphere
AHHHHHHHHH! God I’m dumb. I figured that he was right and that the students were wrong because he’s saying that the conditions are different. I didn’t understand how he got his answer until you explained it. A uniform ρ means that it’s constant and can be left out of the integral. So it’s just -4πGρ on the left side. So I’m assuming then, that means the integral of d^3x is actually the volume of the sphere, right? So if you evaluated it, you’d get (-4πGρ)(4πR^3/3) = 4πR^2. You’d cancel the 4π on either side and be left with (-4πGρ)R^3/3 = R^2. Then you cancel again which gives you -4πGpR/3. That is equivalent to Newton’s equation.
He got the wrong answer because he left out the initial -4π.
Dr Susskind is a national treasure!
Thanks to UA-cam and Stanford for posting these awesome videos :-)..........really worthwhile!.....oh and thanks to Prof Susskind for his lectures
It is an honor to be taught by this gentleman. He has full command over what he is talking about. Thanks a lot Prof. Susskind.
it is my first mathematical lecture on general theory.... its very use full to me..😊
PRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONGPRANK GONE WRONG
I love this stuff I could listen to it all day
PRANK GONE WRONG
So could i. But i still wouldnt understand
What an amazing lecture!
Leonard is my absolutely favorite contemporary physicist.
These lectures are incredible.
My maths is so damned rusty..Yet, Professor Susskind makes lecture's substance sound very easy... Thoroughly enjoyable and interesting stuff.
٩ة٩٩خخت٩نت٩ةنك٩٩٩و٩٩٩خ٩٩٩٩٩٩ة٩و٩٩٩٩٩٩٩٩ة٩٩ت٩و٩٩٩ وننتظرن وون تت٩ ت٩ ن تت ٠ت ٩ ههههه ٩تو ت٩ خ٩ةتة٩ تت تتت تنخ٩ اه ٩٠نحت اه ٠ون٠٠ تت نن ٠٩٩ت٠٩ت نن نت٩ت٠تن٩٠٠ ٠ن٩٩٠ ٠ون٩
this are these these vids that you see in your watch history when you wake up
for the field to be inside on the left hand side it should be--
(-4/3 πR^3 4πρG)=4πR^2 A(perpendicular)
then the missing pi can be located and the equation will become appropriate
+Tarun Kumar the field is worked out by volume? I thought surface area;4pir^3(as he explained it)
+deadmeat1471
p = m/v
m = pv
v_sphere = (4/3)πr^3
m = p((4/3)πr^3)
For the equations to be consistent with each other, the "m" on the right board should be able to be replaced with the "pv" equivalent expression above, resulting in "A_perp = -(4π*r^3*p*G)/(3*r^2) = -(4π*p*G/3)*r" but instead the left board only shows "A_perp = -(p*G/3)*r". That's where the 4π is missing on the left (assuming the right was derived correctly)
The error was in the right side of the equation on the left board. He equated A_perp*4pi*R^2 with the total mass inside the sphere (multiplied with G) and then expressed that as the volume of the sphere times the mass density.
The correct way to apply Gauss' theorem would have been to equate the left side of this equation with the volume of the sphere V times the divergence inside, which is according to Gauss' law -4pi*rho*G. Thr final equation looks like this:
A_perp*4pi*R^2=-4pi*rho*G*V
and using V=(4/3)*pi*R^3:
A_perp*4pi*R^2=-4pi*rho*G*(4/3)*pi*R^3
which has an additional factor of 4pi on the right side.
deadmeat1417 use "dimensional analysis" to know you are wrong here. 4pi is dimensionless, so 4pi r^3 has dimension (length)^3. So its a volume, not an area.
It takes an incredibly well prepared lecturer to throw out derivations on demand.
Austin Fahrenheit
or a very smart and passionate one
not discredit Pr Susskind here, but anyone with basic school knowledge about differentiating could do derivations
To follow them and understand them yes, but to remember where the equations came from takes an incredibly well prepared lecturer.
I suspect Austin is talking about derivations of phyical formulae not about derivations of mathematical functions a.k.a. derivatives.
I recommend to read Professor Susskind's books as well (the Theoretical Minimum Series), in my opnion before looking the lectures. I t is a big luck that a first class, premium, five star scientist with such a reputation obviously has fun and an excellent ability to teach his stuff. Thank you for making this publicly available. Kind regards from Germany!
Bro I am read
Bro I am read
i absolutely appreciate your videos they are amazingly useful
good to see math kids all disagreeing with each other and one of the worlds best physicists, Gives innumerate biology students like me, hope!
Just love this guys voice and accent
I'm not a student, I am just fascinated with physics and I love watching these to try to learn anything I can. Very good lectures!
Is cosmological constant sort of like the inverse of gravity or something? Gravity is very weak but gets very strong with mass, cosmological constant is very weak but gets very strong with distance. So, in order to live in a universe (or to find ourselves in one from the anthropic principle) in which matter is being held together due to gravity, you would ultimately have to have the repulsion, otherwise it'd collapse on itself, and as the universe gets bigger and bigger, faster and faster, the surface area and distances of it is larger therefore enacting the cosmological constant to grow larger?
Does that have anything to do with the formation of voids like Bootes void? To me it seems like that's why you get a filament or sponge like structure if you could zoom out on the universe as a whole.. all of the mass coalescing into valleys of spacetime, and voids bubbling up in relatively empty regions, which pushes matter out toward the valleys?
Sorry, I'm sure these are really dumb questions, just trying to figure it out!
I don't know, but I think that he said dark energy is a constant, so it doesn't get stronger.
@@itchyandscratchy7350 The cosmological constant would get stronger as the time passes, I think Prof. Susskind explained it pretty clearly in the beginning.
Also, it's not really getting stronger by the distance but due to its extremely small value, the equation would only sums up into a considerable number when it's multiplied by a huge distance, hence it only matter when you accounted the entire universe for it, but not so much in an astronomical scale or even in global scale.
Calling it an inverse gravity is pretty much inaccurate because it's not exactly a force. Let alone a force that repulse each matter or particle from each other, it's something that drive the particle grow apart from each other.
@@Vandalgia
6:20
Professor Susskind tells that the theory on the "Big Rip" describes the cosmological constant to be time-dependant, therefore growing with time. As Professor Susskind reminds, however, that is not true ; the theory on the "Big Rip" violates all principles of physics, and so it is not true based on the given principles of physics.
I hope that clarifies Professor Susskind's point about the constant.
@@powahfulgameplayer Yeah, "stronger" might not be the correct word to describe this. As you stated it, it's more like, it changes as the time passes.
Session starts at 14.20
PRANK GONE WRONG
14:20
Dr. Leonard is enjoying himself when students question him.
Thanks very much for this lecture.
I accedentally fell asleep when watching youtube, woke up and had watched the whole lecture one and was at the end of this one. Am I gonna be a genius now?
Thanks a lot to Standford University, it's dificult to find the RG theory...
thanks from Peru. Greetings
Thank you Stanford!!
That disagreement from 45:00 to 52:00, the student was 100% right, the professor got it wrong. He left out a factor of 4pi from the right hand side. Gauss's Law&Theorem state that Aperp*surf. area == -4piGM.
So, at 45:00, the surface area is 4piR^2.
And the mass of the sphere is the volume of the sphere * rho.
The volume of the sphere is 4pi/3 * R^3.
Plug all that in, you get:
Aperp * 4piR^2 = -4pi * G * 4pi/3 * R^3 * rho. See the problem? When he wrote it down at 45:00, he forgot the first 4pi. He wrote down simply -GM rather than -4piGM. The student was right. After cancelling the 4pis from each side, you end up with:
Aperp * R^2 = -G * 4pi/3 * R^3 * rho.
So, Aperp = -4pi/3 * rho * G * R.
If you changed that back to mass instead of rho, you'd get back to the original Gauss equation:
Aperp = -GM/R^2.
greg55666 That is correct. The student was right to be confused by the result Dr. Susskind came to on the left board because M=V*rho. For A perp = -MG/R^2 as on the right board the equation should read -{[(4pi/3)*R^3]*rho*G}/R^2. The (4pi/3)*R^3 is the volume of the sphere so when you multiply the volume by rho you get Mass or M=V*rho. Now all you need to do is substitute V*rho for M in the equation A perp = -MG/R^2 and cancel out the R^2 in the denominator with the R^3 in the numerator. That leaves A perp = (4pi/3)*rho*R*G. I think the confusion here is that the student asking the question had no idea how to articulate the correction he was attempting to point out. Had he been able to say "I can't seem to make the 4pi cancel out like you did due to the 2 equations you set up not being equivalent between the left and right boards. I think you unnecessarily added a 4pi to the L.H.S of the equation on the left board." then I think Dr. Susskind would have immediately realized the error and corrected it. The fact that there were so many conflicting voices in the room and nobody was making any sense led him to just leave it as it was.
@@dylanhaymore608 in student’s defense, he was constantly interrupted by sycophants. I’ve watched this maybe 10x trying to find the error. These posts helped Ty
@@paulodonnell753 I'm glad I was able to help you understand. This material is already difficult to learn so it's even harder to notice when there are errors from the instructor. Good luck on your journey for knowledge!
Best course ever
At 1:13:13, it givs x = (1/2)g*t^2 as a formula for position of a (uniformly) accelerated object. That formula is only strictly applicable if the object started out at rest.
I thought this was the final part of the explanation as I had simply opened this video, not the playlist, and UA-cam hadn't recommended any part 3 or bigger on the suggestions. :(
I tend to believe that the Felix Bloch professor of theoretical physics at Stanford University and his considerable contribution to string theory probably deserves a little more respect then that.. it is a privilege to watch this and thanks to him for his dedication to education.
Thanks for taking the trouble to clear that up for me.
37:09 - a piece of art work: a little sitting bear he has candidly drawn 😊
It just make me smile every time Prof. Susskind call the white board "black board". Other than that he's such a great educator. I wish i can attend his classes one day.
the description has: "discusses dark energy, the tendency of it to tear atoms apart" Susskind would be so pissed. He only spent about 15 minutes of the class explaining how unlikely it is for dark energy to rip apart atoms.
Well tendency can mean tendency not to. Still, kind of misleading.
35:08
Fatality
Must be quite an honor to actually be on lectures of that guy.
About 26:35 into the video, he mentions unit vectors. Good. A very useful concept.
😂😂😂😂😂
Unbelievable. I have had very little formal education, a lifetime of professional experience traveling and living around the world. Mind blowing knowledge - FOR FREE - presented by a world class professor. It's troubling UA-cam algorithm does not push this content and knowledge More; esp the younger generation. I remember visiting a tiny all girls(K-8th) school started by Irish nuns over a century ago in Peshawar a few years ago; an entire classroom of 6th grade girls were doing Calculus on a true blackboard. I didn't understand a lick of it. Mean while in US, my 5th grade son has not come near Algibra much less Calculus. I'm not complaining, just comparing. Kids living in extreme poverty in a extremely dense ancient city, non stop extreme violence all around, yet they can focus their young minds to unbelievable levels academically. Our kids are distracted by countless electronic devices, social media, video games. Yet it is on those devices and media that you can find a world class education 🤷♂️.
To be onest he is real good teacher. Turning complex things to real simple (making it dumb) is high skill. Explaining something complex in a complex way is easy. What hard is turning complex things into a "cosmological constant" dumb level,requires high amount of experience and capeability.
Btw : the students having problem with perpendicular A is the mistake that the both examples are different and the perpendicular A is example specific. there are two different A not equal :)
but when we replace density by M/v= mass to volume ratio
thn we get A is inversely proportional to R (not directly, plz correct me if i m wrong
the correct formula for the acceleration inside a body is a(R)=4*π*ρ*R/3 , the 4*π should exist on the formula @46.27
good lecture
It is the sin(x) = 2MG/Rc^2 with x=2MG/Rc^2 that is used for the aproximation, also there is other aproximation, that for the elapsed time delta t, it is taken as the horizontal component of speed of light is the same c, that can be appear as a logic circle (that is not), since for this is used the a posteriori known fact that the angle is too small, and in the former the use of values of G and c are used to aproximate sinx =x.
The 4pi is lost when he subs into Gauss's Theorem at 44:43. The right-hand side was previously calculated to be -4piGM (at 38:55), but he only subs into -GM, losing the 4pi.
45:20 He remembers the G but forgets the original 4pi from Gauss' Law.
45:20
Time 50:00 min
4π is also there in the formula on right side when particle is inside sphere
The reason he messed up at 0:45:24 is that he is missing an additional factor of 4pi on the right hand side from Gauss' law: Del.A = G rho 4pi. Integrating this expression over the volume of a sphere leads to 4/3 pi r^3 * G rho 4 pi
Thank you!! The good professor goofed a few times in this lecture.
BTW the last half hour of this video is freaking cool.
Hi, wonderful video. but a question: there is a book for follow this lectures?
i want to have also a book for Einstein relativity Special and general.
Thanks all and regards from Italy :-)
there is one called Special Relativity and Classical Field Theory: The Theoretical Minimum . It is coming out in September. Susskind wrote other books such as 'Quantum Mechaniics'
as of this writing
Lecture 1: 5,504,000 views
Lecture 2: 938,000 views
But does that suggest that the divergence is a relative scalar?
Am I the only one that get's extremely satisfied when he erases every marker trail instead of just leaving it be
You are not alone.
thank u so much for the videos..:)
Thank you professor..... One question was : why the effect of mass outside the Gauss surface inside the spherical mass be neglected or canceled ....my answer is I think that the mass is not neglected as you see the density of the field (the gravitation density g) be reduced by reducing the (r) to becomes zero in the centre of sphere which means that the effect of the outside mass which also cause (g) can be considered as superposition summation for the (g) vector at the center and that summation becomes zero when (r) become zero so the disappear of the (g) in the center due to the opposite directions of (g) , from the general relativity point of view also we can understand that the distortion of the metric tensor curvature outside the mass (density of energy) is totally different than when it passes through the it ...thank you
Awesome....physics for free
Wow such understanding and superior explanation, compared to my "professers"
It is impossible to overrate the quality of this lecture.
Take note that in the discussion of the gravitational field at some radius R inside the earth taken from the center of the earth, that Leonard had dropped a 4pi. Perhaps you may have caught this. So, the g field at radius R inside the earth is actually: G*p*pi*R*4/3
At 1.18 Susskind describes how a light beam would cross an accelerating elevator -- noting that the observer in the elevator would see a downward curving light beam (and an external ,stationary , observer , presumably seeing the light beam travelling straight and horizontally ).
And yet had the elevator been travelling at a constant speed (SR), the observer in the elevator would see the beam travelling horizontally within the elevator, and the external observer would see it travelling diagonally upwards.
Why does the external observer ,say, see the light beam being affected by the elevator's frame of reference in the SR case , but not in the GR case. ?.
+Metallurgist47 If I understand correctly the difference is in the original vector of the light. With the accelerating frame the assumption is the beam is emitted at the same time the acceleration starts and so it's direction is horizontal. In the constant velocity case, since the velocity is constant, you have to assume that the elevator is in motion at the beginning of the experiment and the beam is emitted from a source inside the elevator and therefore it starts with the upward component already. Also, the curvature is only seen by the observer inside the elevator. To someone outside it travels perfectly horizontally.
Yeah. Well put. Spherical space about the center of mass is the reasonable conclusion. I forgot that the mandatory requirement that all mass be contained within R of the center of mass.
Thanks to Google, UA-cam and the internet technology researchers who made this possible to watch these videos. Otherwise I had no chance to see this lecture series.
alright, thanks mate! :)
If we could have the moons lack of gravity with the Earths atmosphere. Thanks for teaching and posting this!
Well, actually when the gravity field equation is derived, we assume a test particle with mass m different than zero. When the m term appears on both sides of the equation, we divide by that (thus it must be different than zero).
Therefore it is counter-intuitive to suggest that gravity has the same effect on a zero mass particle. On the contrary according to Newton the gravitational force exerted on a zero mass particle is zero.
Inspiring
Would it be correct, trying to combine both equations (inside and outside the planet) to consider the planet as a point in the center with punctual weight equal to the weight of the section of distance less than ||x|| and a shell acquipped with the mass of the section consisting of point at distance between ||x|| and R_planet ?
52:42 The equations in the 2 cases don't match coz a 4pi was accidentally left out which comes from the Gauss's Law
Is the lamda increase due to the dark energy that is added through distance
Great lecture, I think I really understand General Relativity now, but I have one question:
What happens if I just take the stairs?
R u an engineer?
@tonyxon That little round button at the bottom of the Flash display does something called "seeking". Try it out.
woooooooooooooooot i was so excited when he said Cosmological Constant
Fell asleep with UA-cam running and just woke up to Peter Griffin teaching calculus. Is this real life?
Peter Griffin teaching calculus? He's clearly got an accent from the South Bronx instead of Rhode Island. This course is way above normal calculus.
Time = vector quantity (foward)
Clockwise = could be moving to the right like of the normal clock we have but some people do sell clock that move to the left. As long as it is 360 degrees.
So I think there is nothing like 'anti'
Ant = se-mut
A-rah = direction
Jam = clock
What is wise?
Page 1375
-wise adv combining form. 1 indicating direction or manner: clockwise; likewise. 2 with reference to: businesswise. [OE -wisan (italic); see WISE2]
wise1
1
2 prudent; sensible.
3
4
5
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7 Arch. possessing power or magic.
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wise2
n Arch. way, manner, fashion, or respect (esp. in any wise, in no wise) [OE wise (italic) manner]
Since the divergance of the field equation is calculated in terms of Pi does that mean that the mass density can only account for spherical space?
i think some people ask questions just to show how smart they are.
I think half the comments here are for the same reason. :-)
Teachers and students alike like it when students come prepared, or read ahead of the class.
@memyself1125 No. Satelites use it and Particle accelerators use it but until you get to speeds of (lets say 10,000 miles per hour) you do not use it.
That being said there is relative motion, which is helpful to the layman, but not a necessity.
thank you
So there is a newtonian aquivalence Principle( if an object gets pulled by a bigger mass the acceleration is not dependent of the mass of the smaller object) and Einsteins aquivalence princple( when you accelerate a rocket with 9,81m/s^2 it Feels like earth‘s Gravity Field for someone in that rocket )?
Nope, there was a 4pi missing. Should be for
R>R_0: A=-MG/R²
R
00 lol you can 00 lol 00 00 loll 00 like 00000000000000000000000)00 0000lolllll
Does this really follow up lecture 1? It seems there's a break in content between the two
I suppose that this is second year subject, but Student are asking question like they did not complete any university maths, or physics before. Gauss's Law is and Gauss theorem is usually first year mathematics, and they usually had to overcome difficulties with new concepts.
Good lecture. Easy to follow. Btw, as the student said , it missed the 4pi in the equation. :>
14:03 I liked where you were going. 🤷♀️ Nicely handled, though. Every semester, some play on relativity, I assume.
Yes people are asking question like they don't know what they are talking about. And his style is like he is teaching for those who already have some knowledge.