As you were going through the derivation, i could hear my classical mechanics professor's voice. Ghost from 50 years ago. Fascinating - to quote a certain Vulcan
In my first year in physics 1 course, my teacher tried to give an overview on Lagrangian Mechanics, but he used a lot math tools that i didn't know at the time, for exemple a Taylor Series with two variables. So, I don't need to say that i didn't get anything that he said. But your video can give a very good overview of Lagrangian for a first year!. Good Job! I want a Series!
Hey, if you want a complete course on Lagrangian Mechanics ( with problem solving sessions) , then here I am sharing a playlist with you, I created this series of videos to introduce LAGRANGIAN mechanics in a simple and exciting way, yet retaining the rigour of the subject. Hope you enjoy it ! THIS IS THE LINK TO MY PLAYLIST : ruclips.net/p/PLZumX0a4ZsO0MSJ5Qujht8TOxm-w5XbBf
Whenever I see T used for kinetic, I usually also see V for potential. In Newtonian physics, U is used for potential and K for kinetic. V is used for electric potential per unit charge (voltage), so I appreciate the U to avoid that confusion. I still prefer K for kinetic, as T is often used for time period or for tension, depending on context.
I always assumed it came from the word for work in European languages, which mostly start with "T", because there is a theorem that states that the total work is equal to variation of kinetic energy
After watching you video, I felt Lagrangian mechanics is a very smart way to do it. This feeling is like there is a house, front door is closed. Backdoor is opened but people don't know there has a back door in this house. When try to open the door and into the house, Newtonian mechanics try very hard use force to breaching the door, and Lagrangian mechanics just into the house from back door.
maths and even problem solving in general is poking on all sides until you see some give. then poke there more, rinse, repeat. and if you see similarities to another house, then it makes things even easier ofc every problems has tools that make it easier or harder. but often, differentiation is much easier than integration, hence the Lagrangian comes in handy.
This is such a great breakdown of what's going on. I'm in a 700 level mechanics course and this is pretty much on par with what we've been reading (Goldstein)
Nice introduction to LM ... An important point which was overlooked is the way in which LM can incorporate generalized forces (which would appear as extra terms in the E-L equation). Such forces must be taken into account when some physical forces acting on the system are not conservative (and therefore not expressible via potential energy). Such forces also are especially convenient/useful for assessing relevant constraint forces.
This is amazing man. I've always had a lot of problems with parametrization, and although that was not the core of the video you made me see it in a different way. Keep it up
For people that can't simply get over using the equation without knowing where did it come from (god knows I can't), video from Eugen Khutoryansky gives a rather satisfying explanation of Euler-Lagrange equation derivation.
I can't let it go ever in any instance. I can't shutup and calculate. I need to know the derivation, and why, and how, and inside and out. How else will I fundamentally understand the things I'm doing?
At 13:14, the derivative should be positive because you defined y as -l*cos(theta). Although it doesn't affect the result as you are squaring it later!
T can be calculated- using resolution of vectors resolute T in vectors components as Tcosx (theta=x) and Tsinx. Tcosx and mg gets neutralized and we are left with Tsinx. Since, bob is moving in circular trajectory it implies we can equate Tsinx= mR(dx/dt)^2 where R is radius Therefore,. T= mR(dx/dt)^2/sinx
It's been a long time since I studied multi variable calculus. Can you remind me why you can assume ydot doesn't depend on y? When taking the partial of ydot with respect to y my first thought is that ydot could possibly be equal to a function of y so I wouldn't assume the ydot term would be zero.
I'm new to this but I think its more to do with the lagrangian itself, to predict an objects motion it requires an initial velocity and position which are not dependent on each other in configuration space?
This video deserves to be prefaced with links to the sources for related and assumed knowledge, so people can get the pre-requisite knowledge required to understand and appreciate this video.
I'm happy you found this useful (but not happy your instructor isn't useful). Here's my current course in classical mechanics (but we aren't yet to the Lagrangian). ruclips.net/p/PLWFlMBumSLSbZvcPMA0nH60x1ebX4XSqB
It gets fixed while adding their square if you have noticed it, even if it is fixed by mistake. 😂😂 I mean because of squaring and getting the right answer 😁
Same here. I'm guessing that was a lot of development by different mathematicians, maybe spanning years, to arrive at L = T - U. The teachers don't go into the history.
How does the problem change when you have a pendulum in 3D space? when I plug my z value in, is it also lcos(theta)(theta-dot)? Or would the angle be different when referring to z? And then how does that affect the rest of the process??
Will it not be Theta double dot =- g sin Theta/ Lower case L rather than capital L in the denominator? Also del L/ Del theta dot is zero in the first term because Theta dot is a function of time and not Theta. Am I right?
Very clear explanation of how to do problems using lagrangian dynamics, but I still wonder where it comes from. Why did someone define L=T-U in the first place, etc. Great video!
I think, like many concepts in physics, we use the Lagrangian just because it works. Lagrange showed that if you defined L, then the action integral would be the same as the actual trajectory. It's crazy.
_"Great video!"_ _"but I still wonder where it comes from"_ Isn't that some kind of contradiction? If you can't understand it from the video, probably it's a bad video. We would not have to bother, but this guy is stealing our time.
Not sure about the right hand plot at 5:39. S, as defined by the integral, is a just a constant for each path, since y is a function of t, and we are integrating wrt t. So any plot S should be against "path". How is that represented by the horizontal axis?
Afte practising so many questions, I have seen making mistakes due to writing x prime or x dot to show the velocity in x direction and it's not so efficient to always write like those old books, I do not make mistakes in differentiation or calculus, I make mistakes in distinguishing between velocity and coordinate. So I start writing Vx or Vy or Vz or Vi to show velocity XD
Hi, Dot physics I have two question and im seeking my answer for long time never satisfied with any.1) why lagrangian are defined like L=T-U??? Why not any otjer form like L= sin T- log U or amy othe rkind of weired combination??? Dpes lagrange derrive this perticuler form from Anywhere or he got it in his dream??? 2) if a system is in motion with non conservative force, only like friction can we still define Lagrangian??? How???
The Lagrangian takes different forms depending upon the theory in question - and yes he dreamt it in just the way Newton dreamt F=ma. It's a guess that can be compared with reality.
Could you explain why L is defined as T - U? Also when you were doing the partials around @10:00, even though y dot and y are different variables, isn't y dot still dependent on y and vice versa? So if you are doing the partial of one variable, wouldn't the other be affected as well, in other words when you are doing the partial of y the y dot is moving and vice versa so that the results are not clean? Help me if I am over thinking or there is something to this.
Thats like asking why is newtonian Force defined as the product of mass and acceleration. These are just definitions invented to make calculation possible. you can invent a new definition yourself but the difficult part is to come up with a definition that is useful in calculation
@@maalikserebryakov Net force being equal mass times acceleration is not “a definition invented “ it’s a fact about the natural world transcribed in mathematical term. L=T-U is however purely definitional, and useless considered by itself; However, the Lagrangian EQUATION, is a statement about the physical world.
Nice reintroduction to the Lagrangian - it's been 50 years since I played with this.
Still beautiful! isn't it?
@@rohitjha8626 Yep!
As you were going through the derivation, i could hear my classical mechanics professor's voice. Ghost from 50 years ago. Fascinating - to quote a certain Vulcan
So u never used it in 50yrs??
What's the purpose of knowledge is u rnt gonna use it?
In my first year in physics 1 course, my teacher tried to give an overview on Lagrangian Mechanics, but he used a lot math tools that i didn't know at the time, for exemple a Taylor Series with two variables. So, I don't need to say that i didn't get anything that he said. But your video can give a very good overview of Lagrangian for a first year!. Good Job! I want a Series!
ruclips.net/video/XPCgGT9BlrQ/видео.html 👍💐
Hey, if you want a complete course on Lagrangian Mechanics ( with problem solving sessions) , then here I am sharing a playlist with you, I created this series of videos to introduce LAGRANGIAN mechanics in a simple and exciting way, yet retaining the rigour of the subject. Hope you enjoy it ! THIS IS THE LINK TO MY PLAYLIST :
ruclips.net/p/PLZumX0a4ZsO0MSJ5Qujht8TOxm-w5XbBf
@@suddhasattasaha4793thank you
In french "kinetic energy" is "énergie cinétique". There is no "T" in that. But it could come from the word "travail" which means "work" in french.
of course there is a 't,' it is right there: cineTique
I thought it’s because T is before U, so they used T.
Whenever I see T used for kinetic, I usually also see V for potential.
In Newtonian physics, U is used for potential and K for kinetic. V is used for electric potential per unit charge (voltage), so I appreciate the U to avoid that confusion. I still prefer K for kinetic, as T is often used for time period or for tension, depending on context.
Exactly. Travail mécanique...
I always assumed it came from the word for work in European languages, which mostly start with "T", because there is a theorem that states that the total work is equal to variation of kinetic energy
After watching you video, I felt Lagrangian mechanics is a very smart way to do it. This feeling is like there is a house, front door is closed. Backdoor is opened but people don't know there has a back door in this house. When try to open the door and into the house, Newtonian mechanics try very hard use force to breaching the door, and Lagrangian mechanics just into the house from back door.
maths and even problem solving in general is poking on all sides until you see some give. then poke there more, rinse, repeat. and if you see similarities to another house, then it makes things even easier
ofc every problems has tools that make it easier or harder. but often, differentiation is much easier than integration, hence the Lagrangian comes in handy.
Absolutely right
Or can use brute force computational physics and take all the nails and bolts out and lift off the roof.
Really cool! I'm planning on getting a Physics degree and this just keeps me motivated.
Don’t do it until covid is cured. Trust me I’m dying
ruclips.net/video/XPCgGT9BlrQ/видео.html 👍💐
@@bockminster7474 glad to know I'm not alone xd
just don't
@@bockminster7474 Facts man, me too... What year are you? (Senior coming into Fall semester for me). Things have been super tough during COVID
Your teaching levels of physics is very good and it makes me to listen to your teaching
This is such a great breakdown of what's going on. I'm in a 700 level mechanics course and this is pretty much on par with what we've been reading (Goldstein)
700 level ?
@@kingplunger1grad school
Nice introduction to LM ... An important point which was overlooked is the way in which LM can incorporate generalized forces (which would appear as extra terms in the E-L equation). Such forces must be taken into account when some physical forces acting on the system are not conservative (and therefore not expressible via potential energy). Such forces also are especially convenient/useful for assessing relevant constraint forces.
This is amazing man. I've always had a lot of problems with parametrization, and although that was not the core of the video you made me see it in a different way. Keep it up
Thank you so much for posting this! The explanation is super clear and very helpful for me to understand this topic which is entirely new to me!
Please keep making videos on Lagrangian mechanics 🙏
you know it.
Very clear, and this subject is often presented poorly. Thank you!
I wonder sometimes, how can something be explained this good. Thanksssss
Oh. That’s nice. Thanks!!
For people that can't simply get over using the equation without knowing where did it come from (god knows I can't), video from Eugen Khutoryansky gives a rather satisfying explanation of Euler-Lagrange equation derivation.
I can't let it go ever in any instance. I can't shutup and calculate. I need to know the derivation, and why, and how, and inside and out. How else will I fundamentally understand the things I'm doing?
@@SolidSiren I feel you brother. That is why I warmly recommend this one. Also 'Physics with Eliot' channel has amazing resources on this.
At 13:14, the derivative should be positive because you defined y as -l*cos(theta). Although it doesn't affect the result as you are squaring it later!
T can be calculated- using resolution of vectors resolute T in vectors components as Tcosx (theta=x) and Tsinx. Tcosx and mg gets neutralized and we are left with Tsinx. Since, bob is moving in circular trajectory it implies we can equate Tsinx= mR(dx/dt)^2 where R is radius
Therefore,. T= mR(dx/dt)^2/sinx
This was a really good video, Physics is very interesting subject, although a little complicated.
Every indian jee adv aspirant is kinda junior physicist lol... (me😭)
@@kamalenduhaldar5805 🗿
This video is really helpful, but I think the diagram at 4:45 could use a redraw of sorts ;)
I finally get this comment. I feel stupid now.
should the y_double_dot on 10:37 be minus g because it is acting downwards or I am missing something
You are right 👍🏽
Yep
ye its -g
He lost a minus when solving the last equation.
I noticed this flaw too. Fortunately, someone had described this problem earlier, so my worries quickly disappeared.
Thank you so much Sir for this wonderful video. I am starting this topic in my 1st year. It is very helpful .
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Exceptional introduction- THANK YOU
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Excellent straightforward explanation
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I just realized how important is this when I saw the "LAGRANGIAN" is so big. !
Thank you so much 😘
From vietnam with love
11:57
The Potential energy is mglsin theta since the restoring force is mg sine theta
In your final solution for the pendulum problem you have upper case L in the denominator. It should be lower case.
Mr physics explained make more video on Lagrangian principle it's so helpful for me👍🏻
I can see this is a BIG DEAL!
Thanks for the super tutorial! (Last formular of the pendulum: instead of "L" should be "l" [length of pendulum])
Extremely wonderful video 👏.
simple and easy to understand, thank you!!!!
Good video and great explanation.
ruclips.net/video/XPCgGT9BlrQ/видео.html 👍💐
Great content
Mewton: force
LaGrange: energy
T was chosen by the person who introduced the concept of kinetic energy. It stands for "translational" cause it's the energy of movement
Amazing intro to lagrangian.
thanks!
Thank u sir for this nice explanation 👍🏻👏🙏
Came here from the subreddit
Awesome video, liked and subscribed
This video was really helpful!
ruclips.net/video/XPCgGT9BlrQ/видео.html 👍💐
I like the introduction series
ruclips.net/video/XPCgGT9BlrQ/видео.html 👍💐
So simply explained thanks ❤️
Glad it was helpful!
It's been a long time since I studied multi variable calculus. Can you remind me why you can assume ydot doesn't depend on y? When taking the partial of ydot with respect to y my first thought is that ydot could possibly be equal to a function of y so I wouldn't assume the ydot term would be zero.
I'm new to this but I think its more to do with the lagrangian itself, to predict an objects motion it requires an initial velocity and position which are not dependent on each other in configuration space?
they're taking the partial of L wrt y, and L is a function y, ydot, and t. so we ignore the ydot and t if taking the partial wrt y
i love this channel
Perfect
Great lecture!! Thanks
Glad it was helpful!
Wow, u made it easier
At time stamp 10:30, shouldn't it be mg = -my dot?
Many thanks! There is an obvious mistake at 10:25 . You've lost te sign. There y double dots should be equal to minus g
You missed a minus at 10:23. As a result you got y''=g, which is obviously wrong, as the acceln due to gravity is DOWNWARDS!
This is great! Thank you! Does someone learn this as an engineer? Because I study Civil but have never seen this.
For civil engineering - you might not get to this stuff.
Mechanical engineering - vibration, yeah
@@diatlemaboe9942 yess I'm taking a class in vibrations and you see this stuff
This video deserves to be prefaced with links to the sources for related and assumed knowledge, so people can get the pre-requisite knowledge required to understand and appreciate this video.
thanks for a great video!
Glad you liked it!
That 'identical' caught me off guard.. 🤣🤣🤣
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Ah yes I should clearly be learning this going to 10th grade
@ 10:36 its negative g.
great video!
Aahh yeah this man needs more than just one like
Thanks a lot, my lecturer sucks at this😫
I'm happy you found this useful (but not happy your instructor isn't useful). Here's my current course in classical mechanics (but we aren't yet to the Lagrangian).
ruclips.net/p/PLWFlMBumSLSbZvcPMA0nH60x1ebX4XSqB
didnt know cheatcode existed irl💀💀
Very good explanation !!
nicely explained !
This is a really amazing video!. Actually I was a little bit confused in 13:11, why y' is d/dt(lcos(theta))? it shouldn't by d/dt(-lcos(theta))?
I´d like to know as well
It gets fixed while adding their square if you have noticed it, even if it is fixed by mistake. 😂😂
I mean because of squaring and getting the right answer 😁
I was following along until i got to the ball and shaft problem and i had to pause and reevaulate if i should laugh or cry
T stands for travaille i think. Which means work
GOOD JOB with this movie... Now I will check with others u movies. Maybe this channel is worth to recommend to others. :-)
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Nice Explanation
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Great video, helped a lot. Also, would you happen to know why we use T-U as the lagrangian? I can't seem to find a good answer anywhere
Same here. I'm guessing that was a lot of development by different mathematicians, maybe spanning years, to arrive at L = T - U. The teachers don't go into the history.
Thank you so much
AMAZING ! , SUSCRIBED INMEDIATLY
Great video and great explanation!!! I'm becoming a fan.
excellent teaching sir. But just one doubt, in potential energy, for Y we have to substitute (l - l cos(theta)) right??
aha at 10:38 it's y''=-g not y''=g, since we defined the ground to be 0 and the sky to be positive.
12:05 Potential energy is not - mgl cos@ but mgl (1 - cos@)
Awesome video 😍
Thanks 🤗
I don't think the T has a particular meaning in french either...
One day I'm gonna study them
I came again
How does the problem change when you have a pendulum in 3D space? when I plug my z value in, is it also lcos(theta)(theta-dot)? Or would the angle be different when referring to z? And then how does that affect the rest of the process??
The Langrangian is the excess of kinetic energy over the potential energy of a system.
ref: Lanczos
Great Videos keep it up!
At 10:28 acceleration should be -g
Travail = Work
Great vid!
Thank you sir
Will it not be Theta double dot =- g sin Theta/ Lower case L rather than capital L in the denominator? Also del L/ Del theta dot is zero in the first term because Theta dot is a function of time and not Theta. Am I right?
Amazing
I'll admit, a bit of a dry topic, but it's nice to hear Duncan Trussel branching out.
How will we obtain the Lagragian for an object sliding under the influence of force 'F' on a frictional surface?
Thank you so much ❤
Interesting problem at 4:45, looks very familiar...
I think something is wrong with me; I keep watching this type of stuff for fun :-)
Kinetic energy translates to "énergie cinétique" in french, so the T probably doesn't come from there ^^
Very clear explanation of how to do problems using lagrangian dynamics, but I still wonder where it comes from. Why did someone define L=T-U in the first place, etc.
Great video!
I think, like many concepts in physics, we use the Lagrangian just because it works. Lagrange showed that if you defined L, then the action integral would be the same as the actual trajectory. It's crazy.
_"Great video!"_
_"but I still wonder where it comes from"_
Isn't that some kind of contradiction? If you can't understand it from the video, probably it's a bad video. We would not have to bother, but this guy is stealing our time.
At minute 9:51 shouldn’t the derivative of why dot the 2MY dot?
Not sure about the right hand plot at 5:39. S, as defined by the integral, is a just a constant for each path, since y is a function of t, and we are integrating wrt t. So any plot S should be against "path". How is that represented by the horizontal axis?
Sorry to say that, but it's an awkward BS diagram as well as an awkward BS explanation. Thumbs down.
that path from 4:47 is something familiar !?
Great one !!!
Should that derivative with respect y be my' * mdy'/dy - mg?
Afte practising so many questions, I have seen making mistakes due to writing x prime or x dot to show the velocity in x direction and it's not so efficient to always write like those old books, I do not make mistakes in differentiation or calculus, I make mistakes in distinguishing between velocity and coordinate. So I start writing Vx or Vy or Vz or Vi to show velocity XD
Hi, Dot physics I have two question and im seeking my answer for long time never satisfied with any.1) why lagrangian are defined like L=T-U??? Why not any otjer form like L= sin T- log U or amy othe rkind of weired combination??? Dpes lagrange derrive this perticuler form from Anywhere or he got it in his dream??? 2) if a system is in motion with non conservative force, only like friction can we still define Lagrangian??? How???
The Lagrangian takes different forms depending upon the theory in question - and yes he dreamt it in just the way Newton dreamt F=ma. It's a guess that can be compared with reality.
Thank u sir.
Could you explain why L is defined as T - U? Also when you were doing the partials around @10:00, even though y dot and y are different variables, isn't y dot still dependent on y and vice versa? So if you are doing the partial of one variable, wouldn't the other be affected as well, in other words when you are doing the partial of y the y dot is moving and vice versa so that the results are not clean? Help me if I am over thinking or there is something to this.
Thats like asking why is newtonian Force defined as the product of mass and acceleration. These are just definitions invented to make calculation possible.
you can invent a new definition yourself but the difficult part is to come up with a definition that is useful in calculation
@@maalikserebryakov Useful for calculation is good enough for me. I thought there was something more deeper.
@@classictutor
yes thats all there is to it nothing deeper at all 👍
@@maalikserebryakov Net force being equal mass times acceleration is not “a definition invented “ it’s a fact about the natural world transcribed in mathematical term.
L=T-U is however purely definitional, and useless considered by itself; However, the Lagrangian EQUATION, is a statement about the physical world.
Thank you! Thank you!