Math for Physics
Math for Physics
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วีดีโอ

Smooth Manifolds ep. 8 - Smooth Maps on Manifolds
มุมมอง 1.6K3 ปีที่แล้ว
The date went well
Smooth Manifolds ep. 7 - Proving S1 is a Smooth Manifold
มุมมอง 3.9K3 ปีที่แล้ว
Smooth Manifolds ep. 7 - Proving S1 is a Smooth Manifold
Smooth Manifolds ep. 6 - Proving Rn is a Smooth Manifold
มุมมอง 1.6K3 ปีที่แล้ว
Smooth Manifolds ep. 6 - Proving Rn is a Smooth Manifold
Smooth Manifolds ep. 5 - What is a Smooth Manifold?
มุมมอง 3.3K4 ปีที่แล้ว
Smooth Manifolds ep. 5 - What is a Smooth Manifold?
Smooth Manifold ep 4 - Atlases
มุมมอง 3.2K4 ปีที่แล้ว
Smooth Manifold ep 4 - Atlases
Smooth Manifolds ep. 3 - Compatible Charts and Transition Functions
มุมมอง 1.8K4 ปีที่แล้ว
Smooth Manifolds ep. 3 - Compatible Charts and Transition Functions
Smooth Manifolds ep. 2: Co-ordinate Charts
มุมมอง 2.2K4 ปีที่แล้ว
Smooth Manifolds ep. 2: Co-ordinate Charts
Smooth Manifolds Ep. 1 - Topological Manifolds
มุมมอง 2.2K4 ปีที่แล้ว
Smooth Manifolds Ep. 1 - Topological Manifolds
Discrete Representation Theory Ep. 12 - Examples of Group Algebras and Regular Representations
มุมมอง 3534 ปีที่แล้ว
Discrete Representation Theory Ep. 12 - Examples of Group Algebras and Regular Representations
Discrete Representation Theory Ep. 11 - The Regular FG-Module (Regular Representations)
มุมมอง 4594 ปีที่แล้ว
A more rigorous proof of faithfulness is left as an exercise to the viewer, because I saw all the holes in my proof while editing, but didn't care enough to re-film it
Discrete Representation Theory Ep. 10 - Group Algebras
มุมมอง 2624 ปีที่แล้ว
a longer aside before returning to representation theory
Discrete Representation Theory Ep. 9 - What the heck is an algebra?
มุมมอง 2334 ปีที่แล้ว
a quick aside
Discrete Representation Theory Ep. 8 - Reducibility
มุมมอง 4094 ปีที่แล้ว
Let's turn big matrices into smaller matrices
Discrete Representation Theory Ep. 7 - Permutation Modules
มุมมอง 6025 ปีที่แล้ว
This video looks at permutation modules, and shows how to use them to construct permutation representations.
Discrete Representation Theory Ep. 6 - FG-Modules to Reps, and Equivalent Reps in FG-Modules
มุมมอง 6575 ปีที่แล้ว
Discrete Representation Theory Ep. 6 - FG-Modules to Reps, and Equivalent Reps in FG-Modules
Discrete Representation Theory Ep. 5 - Intro to FG-Modules
มุมมอง 8955 ปีที่แล้ว
Discrete Representation Theory Ep. 5 - Intro to FG-Modules
Discrete Representation Theory Ep. 4 - Reps of (Sick)lic groups
มุมมอง 3045 ปีที่แล้ว
Discrete Representation Theory Ep. 4 - Reps of (Sick)lic groups
Discrete Representation Theory Ep. 3 - Faithful Representations
มุมมอง 5965 ปีที่แล้ว
Discrete Representation Theory Ep. 3 - Faithful Representations
Discrete Representation Theory Ep. 2 - Equivalent Representations
มุมมอง 7415 ปีที่แล้ว
Discrete Representation Theory Ep. 2 - Equivalent Representations
Discrete Representation Theory Ep. 1 - Introduction to Representations of Discrete Groups
มุมมอง 1.1K5 ปีที่แล้ว
Discrete Representation Theory Ep. 1 - Introduction to Representations of Discrete Groups
Corrections to Newton's 2nd Law using Quantum Mechanics
มุมมอง 4356 ปีที่แล้ว
Corrections to Newton's 2nd Law using Quantum Mechanics
Deriving Newton's 2nd Law (the fast way, with Ehrenfest)
มุมมอง 4646 ปีที่แล้ว
Deriving Newton's 2nd Law (the fast way, with Ehrenfest)
Deriving Newtons 2nd Law with Quantum Mechanics
มุมมอง 6K10 ปีที่แล้ว
Deriving Newtons 2nd Law with Quantum Mechanics
Deriving the Momentum Operator (Quantum Mechanics)
มุมมอง 33K10 ปีที่แล้ว
Deriving the Momentum Operator (Quantum Mechanics)
Dirac Delta (not) Function - for Dani
มุมมอง 1.1K10 ปีที่แล้ว
Dirac Delta (not) Function - for Dani

ความคิดเห็น

  • @math_time7984
    @math_time7984 29 วันที่ผ่านมา

    Thank you very much.

  • @quantaali543
    @quantaali543 2 หลายเดือนก่อน

    We don't drive it. We define it. Just like we have defined the energy operator, right in the Schrödinger equation. The easiest way to get to the definition is to take a wave functions ψ=Ae ^i(xp-Εt) and differentiate it wrt x. Then, you'll immediately see how the momentum operator pops out.

  • @PaulaBlazer-n7l
    @PaulaBlazer-n7l 2 หลายเดือนก่อน

    Physics is fun😊

  • @geneyoungdho
    @geneyoungdho 3 หลายเดือนก่อน

    I wish you reply p,x’s poisson relation with ih.

  • @ChaineYTXF
    @ChaineYTXF 3 หลายเดือนก่อน

    C^k means defined and continuous, doesn't it? Not just defined

  • @forheuristiclifeksh7836
    @forheuristiclifeksh7836 4 หลายเดือนก่อน

    1:00

  • @JohnJoss1
    @JohnJoss1 5 หลายเดือนก่อน

    Yes! Thank you very much. I did look at a few videos on the momentum operator but none were as clear as this one. A bit cranky and untidy but that’s part of the fun 🎉 . Dr-J

  • @yldzulkutunc6931
    @yldzulkutunc6931 5 หลายเดือนก่อน

    Thank you !

  • @GiovannaIwishyou
    @GiovannaIwishyou 6 หลายเดือนก่อน

    When it comes to faithful homomorphisms (including group actions) somehow it clicked for me when my professor said - that homomorphism has no kernel (meaning the only element in the kernel is just a neutral element).

  • @GiovannaIwishyou
    @GiovannaIwishyou 6 หลายเดือนก่อน

    "I happen to have a linear map here." - pulls out toilet paper tube 🤣 (I might try that during my thesis defense)

  • @elkronnie6500
    @elkronnie6500 7 หลายเดือนก่อน

    Thank you so much 😭 This video was really helpful

  • @slog656
    @slog656 8 หลายเดือนก่อน

    based

  • @JBudOner
    @JBudOner 8 หลายเดือนก่อน

    Really appreciate you taking the over pedantic description out of your explanation, super easy to follow along

  • @samiachiba2577
    @samiachiba2577 10 หลายเดือนก่อน

    Please exercises

  • @D-Brow
    @D-Brow 10 หลายเดือนก่อน

    I could not find any other source or reference that describes the maximum or net force of the impact in terms or Fi + Fg... rather all of them say the F = m*a*(h/d)... Can you provide another source that talks about this inertial frame of reference with respect to a falling object?

  • @ernestschoenmakers8181
    @ernestschoenmakers8181 ปีที่แล้ว

    Newton's 2nd law can also be derived from the Euler-Lagrange equations where IBP is also involved.

  • @sarahkhan7875
    @sarahkhan7875 ปีที่แล้ว

    Bro why did you stop making videos for this playlist it is a life saver please continue the playlist please 🙏🥺

  • @yaze-uw3hd
    @yaze-uw3hd ปีที่แล้ว

    I DO NOT BELIEVE THAT, the RATIO of. " h / d " is the. REAL CORRELATION OF NET IMPACT .. . THAT. IS. ONLY. A. FANCY. EQUATION, that gives unTRUE RESULTS .. . I MADE MY OWN RESEARCH ABOUT. THE " CODES OF ENERGY TRANSFORMATION ", TO ACCURATELY DERIVE THE TRUE IMPACT ,, , coz everytime I drop the ball I get different values of " d " from the same height and same amount of Mass.. . That is why using the REBOUND DISTANCE ( d ) is not an APPROPRIATE CORRELATION TO HAVE EXACT AMOUNT OF ENERGY. THE ENERGY OF POTENTIAL WORK AT REBOUND DISTANCE ( d ) , ,, IS NOT A COMPLETE TASK BECAUSE THAT ENERGY OF WORK in that TRANSFORMATION HAS EXPERIENCING ENERGY DISSIPATION coz some Shocks of IMPACT WAS DIRECTLY ABSORBED BY THE GROUND OR FLEBILITY OR RIGIDITY OF OBJECT BEING DROP ... TAKE NOTE THAT EVERYTHING WAS CREATED BY GOD WAS CLOTHE WITH THE " ENERGY ", AND THE ENERGY IS THE STRENGTH AND SHIELD OF PROTECTION OF THE MATTER TO SUSTAIN ITSELF OF ITS EXISTENCE, AS LONG AS THE STRENGTH OF THE OBJECT DID NOT MATCH THE EXTERNAL FORCES THAT CAN DESTROY IT, IT WILL NOT FACE ITS EXTINCTION .. . AND PERFECT WAY TO MEASURE THE ENERGY OF IMPACT THRU POTENTIAL WORK, IS TO MEASURE THE DEFORMATION OF THE GROUND .. . AND REMODEL THE SCALE OF IMPACT USING WEIGHING SCALE THAT WILL YIELD SAME SETTLEMENT OR DEFORMATION THAT WILL BE LOADED BY EQUIVALENT MASS OF GROSS IMPACT... OR REMODEL THE DEFORMATION OF OBJECT BEING DROPPED.. . IF YOU DRAW THE ACTUAL CURVE OF IMPACT DONE BY TEST EXPERIMENTS, IT IS NOT A LINEAR EQUATION, BUT IT IS SOMETHING LIKE A PARABOLIC OR 2ND DEGREE EXPONENTIAL CURVE ... AND I ALREADY DERIVE THAT PERFECT FORMULA FOR CURVE OF IMPACT FORCE .. .

  • @catdanceable
    @catdanceable ปีที่แล้ว

    to much hand waving then again your catering to physicist

  • @raelerminy1859
    @raelerminy1859 ปีที่แล้ว

    Amazing video. You got a new subscriber.

  • @renuchauhan3102
    @renuchauhan3102 ปีที่แล้ว

    Sir upload more video

  • @one4runner435
    @one4runner435 ปีที่แล้ว

    Awesome series. Really enjoying it so far. I don't know if I'll be able to keep the smirk off my face the next time my prof says unfaithful representation.

  • @sachinmore448
    @sachinmore448 ปีที่แล้ว

    thank you but i think you messed the thing more

  • @crashhappy7296
    @crashhappy7296 ปีที่แล้ว

    Thank you for this. Deriving this was a homework question on our first ever QM hw assignment (it wasn't even hinted at in the book). I never would have figured this out on my own.

  • @JimKasper1
    @JimKasper1 ปีที่แล้ว

    I have never heard of stopping distance = 1ft. This seems incredibly facile, at best. To me, the whole equation falls to pieces when you make generalizations like this. SO many factors are playing around with each other when a body (be it yours or your friend's or a length of wood being rigged) comes to a stop, I can't see working with numbers that make such recklessly static assumptions. Where's rope stretch? Diameter? Systemic friction? Materials present? This topic is interesting, but not at all useful pragmatically for a practicing arborist. Theory versus praxis.

  • @ritalungu3396
    @ritalungu3396 ปีที่แล้ว

    i think am gonna pass manifolds course after watching this video

  • @chuyzepeda835
    @chuyzepeda835 ปีที่แล้ว

    What is the difference between velocity and speed in this context?

  • @An-xz1hj
    @An-xz1hj 2 ปีที่แล้ว

    How the hell does the integral of psi*psi goes from negative infinity to positive infinity goes to zero when for a normalised psi when it's literally defined as equal to 1 for a normalised function as the probability of finding a particle from positive to negative infinity is one .. this makes no sense and its driving me crazy ughh 🤬🤬

  • @poopyfarts42069
    @poopyfarts42069 2 ปีที่แล้ว

    Thanks it really helped me out :D

  • @onefortrees
    @onefortrees 2 ปีที่แล้ว

    So cool. New climber but I've worked under my father, who's been a climber for 30+ years, for about 4 or 5 years total now. I've been roping all that time. He's a master arborist and has always stressed that physics is vital to a safe take down. Thanks for the video!

  • @spelunkerd
    @spelunkerd 2 ปีที่แล้ว

    I spent some time this week trying to derive the 20% rule for dismantling a spar. ie when an arborist cuts down a spar, each piece should be 20% of the total height of the spar for it to land flat after a 3/4 rotation. I got height of last cut off the ground (s) is 4.45X length of the log(l), which is pretty close to the ideal 4.0, but I wonder if I did it correctly. I used total energy available in the first 90 deg, turning that into the rotational energy of a log spinning from one end PLUS the kinetic energy of the center of mass moving downward. I got w=sqrt((12g)/7l). That gave me angular velocity (w in radians), and downward velocity was wl/2 when the log was at 90 degrees, where l is length of log. From there I calculated how high the arborist has to be to allow another pi radians of rotation, which worked out to s=l*((7pi^2/24)+pi/2). I'm wondering whether at liftoff I should have made note that the moment of inertia changes from (ml^2)/3 to (ml^2)/12, but when I tried that I got a completely wrong answer. Reason? When the log leaves the stump, it should instantly begin to rotate about its center axis, so angular velocity should increase to conserve momentum, like a skater who pulls her arms in. Why doesn't that work out?

  • @akrishna1729
    @akrishna1729 2 ปีที่แล้ว

    this is such a great vid, thanks so much!

  • @Phountainhead
    @Phountainhead 2 ปีที่แล้ว

    Which sources did you use as research material?

  • @Phountainhead
    @Phountainhead 2 ปีที่แล้ว

    What a great playlist, I can't believe it has so little views. I feel like I found the holy grail since I need to prepare a 90 minute talk about this. Thanks!

  • @jpcgandre
    @jpcgandre 2 ปีที่แล้ว

    One comment: the Eg = mgh more accurately is Eg=mg(h+d). And you are assuming objects are rigid. I think the force you feel on impact if Fi, not Fnet. Otherwise when you place an object on top of your head and this is in static state you wouldn't feel any force (Fnet is 0).

  • @omar281997
    @omar281997 2 ปีที่แล้ว

    I believe there is a mistake at the equation at time 03:47 Instead of phi inverse on the LHS it should be psi inverse. The idea of this is to show that smoothness is independent of chart.

  • @nackle_k
    @nackle_k 2 ปีที่แล้ว

    dang I know next to nothing about topology and even I almost understood this, nicely done!

  • @danielng8699
    @danielng8699 2 ปีที่แล้ว

    This is simply a consistency check.

  • @stipepavic843
    @stipepavic843 2 ปีที่แล้ว

    instantly subbed, thankkks!!

  • @jomajsable
    @jomajsable 2 ปีที่แล้ว

    Love how entertaining you've made this (on top of representation theory already being a blast, obviously). Thanks!

  • @GCKteamKrispy
    @GCKteamKrispy 2 ปีที่แล้ว

    You did it, you son of a b****😂

  • @deepak73008
    @deepak73008 2 ปีที่แล้ว

    Thank u

  • @flofe2607
    @flofe2607 2 ปีที่แล้ว

    Me: "Why is that definition so over the top and complicated?" Him: "and we know how maps work from R^n to R^k" Me: "Ahhhhh" Well thank you Sir! :D

  • @same-shivacademyofmechanic294
    @same-shivacademyofmechanic294 3 ปีที่แล้ว

    Excellent

  • @sawmill035
    @sawmill035 3 ปีที่แล้ว

    Wow, for only ~350 views, this video is extremely well done. Nice work for the vid, and apparently nice work that night too. ;) P.S. When you said "When someone gives me this, I'm like... what?" I felt that.

  • @jaredaitken1260
    @jaredaitken1260 3 ปีที่แล้ว

    Dude, wonderful video. Thanks so much

  • @sadhbhryan3510
    @sadhbhryan3510 3 ปีที่แล้ว

    You sir are a hero :) thank you so much <3

  • @xwyl
    @xwyl 3 ปีที่แล้ว

    Super short videos are super good compared with the half an hour videos

  • @xwyl
    @xwyl 3 ปีที่แล้ว

    The extra explanations (which textbooks lack) is good for understanding.

  • @petterbrandt786
    @petterbrandt786 3 ปีที่แล้ว

    Yes! Physics for Arborists that's great! when using this formula for negative rigging - would "h" be the distance of free fall or the total distance until completely stopped? I've been thinking a bit about physics and negative rigging lately, since the distance is measured from the piece's center of gravity - a long piece would fall a longer distance before the rope can stop it, but I don't really have a good understanding of how to calculate forces in a tipping motion, have you ever thought of this?