I think Hamilton cared for the fact that momentum is a covector, so when you differentiate something with respect to its components, indices 'flip' and you get a vector, and vice versa. So it made sense to formulate Hamiltonian mechanics with a vector and a covector: you differentiate the Hamiltonian with respect to one and get another.
@noobyfromhell Well, eh, that is true with Hamiltonian dynamics. The momentum is defined to be a vector in the cotangent space of the configuration manifold (the manifold of possible spatial configurations). However, I don't think that your reasoning can be applied to Lagrangian mechanics in which the generalized velocities are simply elements of the tangent space.
Anybody who eats cookies and gives lectures on physics is one cool mofo. I can't get enough of these lectures. I wish they'd arrange them all a little better and add the missing ones.
I would imagine that Hamilton's purpose was twofold. First, the canonical equations of motion tend to take the form of a system of first order ODEs instead of second order. Second, because the canonically conjugate momenta tend to be conserved quantities, the equations of motion will tend to take a more obviously simple form.
What's more, there is something of a preference for energies, or Hamiltonians, over Lagrangians which don't seem to have meaning outside of deriving equations of motion.
These are great lectures and Susskind is a great teacher. It's too bad they didn't get a competent cameraman to work with him. Often the camera needlessly moves away from important equations on the board. Nevertheless, Susskind makes these the best physics lesson I'ver ever seen, in any format.
if you knew that at time t the pendulum's energy was 0 and its theta was pi (the pendulum is stuck vertically upright), then how could you know whether it was pushed clockwise or counterclockwise to get to that position? aren't classical systems supposed to be deterministic into the past?
I think that on a y/t graph, the path of bob is given by a vertical straight line (y does not change, t does)
Since d energy is 0,its more like a ball of mass in space,with no forces on it(T n U both r 0).In such a case,the path is well just the vertical line frm - infinity to +infinity.Hence d path is deterministic.
If what u meant was dat T alone is 0,then its more like a pendulum on earth,at rest.Path again is fixed, being a vertical line on t-y.determinism is therefore given
For determinism we need to know both q and q-dot (velocity). If we know both these quantities for your setup, you will see that you can easily predict the path.
You can follow the equations back in time in that case, and you will find that it was always balanced at the top. In the case where the pendulum is swung with just enough energy to never fall down, it approaches the top asymptotically, so there's always a small displacement from the top, with a correspondingly small amount of velocity toward the top - and in that case you can work out which way (and when) it was swung. In either case determinism is intact :)
i enjoyed this vid
jayejayeee 2 days ago
love the video really good
staranjela 4 days ago
love the video man
grisgrisy 1 week ago
love the video really good
SuperDogbrown 1 week ago
1:42:05
I think that peeve in the audience asked a question so necessary they had to cut the sound out.
awsomenesscaleb 1 month ago
An instructor who knows what he's doing. Good man.
grunder20 2 months ago
a person who understands and masters physics is a great teacher, even if he is a peacful guy
edy141000 3 months ago
balancing the pendulum on the top is a standard trick for robotics
SalsaTiger83 4 months ago
I think Hamilton cared for the fact that momentum is a covector, so when you differentiate something with respect to its components, indices 'flip' and you get a vector, and vice versa. So it made sense to formulate Hamiltonian mechanics with a vector and a covector: you differentiate the Hamiltonian with respect to one and get another.
noobyfromhell 9 months ago
@noobyfromhell Well, eh, that is true with Hamiltonian dynamics. The momentum is defined to be a vector in the cotangent space of the configuration manifold (the manifold of possible spatial configurations). However, I don't think that your reasoning can be applied to Lagrangian mechanics in which the generalized velocities are simply elements of the tangent space.
MichaelKovarik 7 months ago
What is that "feida DOT"? Why does he put the dot over the Greek letter which corresponds as an angle?
Gytax0 10 months ago
@Gytax0 It's theta and dot means 'derivative with respect to time'.
noobyfromhell 9 months ago
@noobyfromhell Thank you.
Gytax0 9 months ago
Anybody who eats cookies and gives lectures on physics is one cool mofo. I can't get enough of these lectures. I wish they'd arrange them all a little better and add the missing ones.
1isaacmusic 11 months ago
This has been flagged as spam show
Think about your marriage and get a trusted women rockmycity.info
shasikamalika 1 year ago
Leonard Susskind is just unbelievable, he should be treasured lol. I love him.
paulojunior201 1 year ago
I would imagine that Hamilton's purpose was twofold. First, the canonical equations of motion tend to take the form of a system of first order ODEs instead of second order. Second, because the canonically conjugate momenta tend to be conserved quantities, the equations of motion will tend to take a more obviously simple form.
What's more, there is something of a preference for energies, or Hamiltonians, over Lagrangians which don't seem to have meaning outside of deriving equations of motion.
odysseus9672 1 year ago 2
Bob & Herman 26:50 :)
TheBobathon 1 year ago
These are great lectures and Susskind is a great teacher. It's too bad they didn't get a competent cameraman to work with him. Often the camera needlessly moves away from important equations on the board. Nevertheless, Susskind makes these the best physics lesson I'ver ever seen, in any format.
thyorison 1 year ago
if you knew that at time t the pendulum's energy was 0 and its theta was pi (the pendulum is stuck vertically upright), then how could you know whether it was pushed clockwise or counterclockwise to get to that position? aren't classical systems supposed to be deterministic into the past?
andrew11235 2 years ago
i guess you could say that's because it's a symmetry? anyone know?
andrew11235 2 years ago
Good question.. Am stuck on that too..or may be am just too stupid.
rahulilrplac 2 years ago
I think that on a y/t graph, the path of bob is given by a vertical straight line (y does not change, t does)
Since d energy is 0,its more like a ball of mass in space,with no forces on it(T n U both r 0).In such a case,the path is well just the vertical line frm - infinity to +infinity.Hence d path is deterministic.
If what u meant was dat T alone is 0,then its more like a pendulum on earth,at rest.Path again is fixed, being a vertical line on t-y.determinism is therefore given
Just my thought.
rahulilrplac 2 years ago
Also, let's say we are at angle pi.
For determinism we need to know both q and q-dot (velocity). If we know both these quantities for your setup, you will see that you can easily predict the path.
Does that answer your question?
rahulilrplac 2 years ago
You can follow the equations back in time in that case, and you will find that it was always balanced at the top. In the case where the pendulum is swung with just enough energy to never fall down, it approaches the top asymptotically, so there's always a small displacement from the top, with a correspondingly small amount of velocity toward the top - and in that case you can work out which way (and when) it was swung. In either case determinism is intact :)
nathanielvirgo 2 years ago 2
ah, of course! thanks.
andrew11235 2 years ago
Comment removed
maxschmeling666 2 years ago
Comment removed
rmnbrw 2 years ago
Comment removed
fielsjd 2 years ago
Comment removed
asscork 2 years ago
This guy is really helpful, and a great teacher, I can't believe I'm watching University lectures for free.
ogirv101 2 years ago 21
@ogirv101
Welcome to the age of the internet where great things are possible.
ethositachi 1 year ago
@ogirv101
Leonard Susskind truly is a man among men!
HelloIAmDaniel 1 year ago
Good instructor!
chile1231 3 years ago 5
lol, this guy is no ordinary physics instructor
mrunzi76 2 years ago 18
Comment removed
rmnbrw 2 years ago
@mrunzi76 this guy is no ordinary physicist - he's the guy who bitch slapped Hawking.
csmcmillion 5 months ago