Jason Bramburger
Jason Bramburger
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Boundary Reflections in the Wave Equation - Partial Differential Equations | Lecture 41
The previous lecture introduced D'Alembert's solution to the wave equation which decomposes the solution into leftward and rightward travelling components. But what happens if the wave equation is not on an infinite line, but a boundary? In this lecture we study what happens when one of these waves comes up against a boundary and derive mathematically how it can reflect off it. Of course, different boundary conditions can lead to different phenomena and so the viewer is left to experiment with different boundary conditions.
Lectures series on differential equations: th-cam.com/video/UDUH58w4-5w/w-d-xo.html
More information on the instructor: hybrid.concordia.ca/jbrambur/
Follow @jbramburger7 on Twitter for updates.
มุมมอง: 90

วีดีโอ

Characteristics of the Wave Equation - Partial Differential Equations | Lecture 40
มุมมอง 38014 ชั่วโมงที่ผ่านมา
In this lecture we return to the wave equation, but analyze it from a different perspective. We use the method of characteristics to arrive at D'Alembert's solution to the wave equation which decomposes the solution into a leftward and rightward propagating component. We arrive at this solution using the "factoring" of the wave equation from the previous lecture into two first-order PDEs. Lectu...
Method of Characteristics - Partial Differential Equations | Lecture 39
มุมมอง 25319 ชั่วโมงที่ผ่านมา
In this lecture we show that the wave equation can be decomposed into two first-order linear partial differential equations. We further solve these resulting first-order PDEs using the method of characteristics. It is shown that the solutions simply propagate the initial condition left or right in space as time goes on. We then generalize the method to nonlinear systems where now the speed of t...
Scattering and the Schrodinger Equation - Partial Differential Equations | Lecture 38
มุมมอง 342วันที่ผ่านมา
In this lecture we encounter a new PDE: the Schrodinger equation. The Schrodinger equation is a well-studied PDE coming from quantum physics and in this lecture we look at some of its important solutions. In particular, we show that separation of variables results in solutions that oscillate and time and hold fixed profiles based that are solutions of a Sturm-Liouville problem on an infinite li...
Heat Equation on a Semi-Infinite Line - Partial Differential Equations | Lecture 37
มุมมอง 13414 วันที่ผ่านมา
We have now spent some time solving the heat equation on the entire real line. In this lecture we consider it on a semi-infinite line (the positive reals), meaning that a boundary condition must be imposed at the left endpoint x = 0. With Dirichlet boundary conditions the result is a solution written as a superposition of sines. We show that this corresponds to the Fourier Sine Transform, while...
Properties of the Fourier Transform - Partial Differential Equations | Lecture 36
มุมมอง 17314 วันที่ผ่านมา
Now that we have been introduced to the Fourier transform and how it helps to understand the heat equation, we turn to analyzing some of its key properties. In particular, we investigate how the Fourier transform acts on derivatives of functions by applying it to the heat equation. The result is an ordinary differential equation in Fourier space which can be solved using separation of variables...
Fourier Transform and the Heat Equation - Partial Differential Equations | Lecture 35
มุมมอง 38821 วันที่ผ่านมา
In the previous lecture we learned about the Fourier transform. In this lecture we will now apply this knowledge to the heat equation on an infinite line. In particular, we find the Guassian arising naturally in numerous contexts throughout our study: in the influence function, the fundamental solution to the heat equation, and self-similar solutions. Thus, the importance of the Gaussian and Fo...
The Fourier Transform - Partial Differential Equations | Lecture 34
มุมมอง 1K21 วันที่ผ่านมา
In the previous lecture we solved the heat equation on an infinite line to see that the solution is written as an integral over all wave numbers. In this lecture we investigate this integral operator, termed the Fourier transform. We derive the Fourier transform as the limit of a Fourier series as the domain becomes unbounded. As an example we show that Gaussians in physical space are transform...
The Heat Equation on an Infinite Line - Partial Differential Equations | Lecture 33
มุมมอง 15128 วันที่ผ่านมา
For the duration of this lecture series we have looked at PDEs on finite (bounded) domains. Mathematically, we typically study very large domains as being infinite to exclude finite-size effects. However, this infinite domains lead to new issues that have to be carefully dealt with. In this lecture we derive the solution to the heat equation on an infinite line using separation of variables. We...
Eigenfunction Expansions and Resonance - Partial Differential Equations | Lecture 32
มุมมอง 259หลายเดือนก่อน
With our theory of solutions to the Helmholtz equation we are able to apply it to solving inhomogeneous heat and wave equations in higher spatial dimensions. In this lecture we perform an eigenfunction expansion on the PDE model for a vibrating membrane to obtain an explicit series solution. In particular, we focus on the case of a time-periodic forcing applied to the membrane and demonstrate t...
Vibrating Circular Membranes - Partial Differential Equations | Lecture 31
มุมมอง 244หลายเดือนก่อน
In this lecture we apply our study of the Helmholtz equation in the previous lecture to the wave equation in two spatial dimensions. In particular, we solve the PDE of a vibrating circular membrane using separation of variables. Using polar coordinates, we show that the solution can be represented in terms of Bessel functions. Bessel functions are extremely important special functions that aris...
The Helmholtz Equation - Partial Differential Equations | Lecture 30
มุมมอง 386หลายเดือนก่อน
Now that we have mastered Sturm-Liouville theory, we turn to its higher-dimensional analogue. In this lecture we present the Helmholtz equation which naturally arises from separation of variables applied to both the heat and wave equations in more than one spatial dimension. We present a theorem detailing the solutions to the Helmholtz equation which is similar, but contains measurable differen...
Inhomogeneous Boundary Conditions - Partial Differential Equations | Lecture 29
มุมมอง 227หลายเดือนก่อน
In the previous lecture we were introduced to eigenfunction expansions for solving inhomogeneous PDEs. In this lecture we extend the method of eigenfunction expansions to include inhomogeneous, or forced, boundary conditions. It is demonstrated that some care must be taken since the solution expansion can never satisfy the inhomogeneous boundary conditions, but remains valid within the domain a...
Eigenfunction Expansions - Partial Differential Equations | Lecture 28
มุมมอง 357หลายเดือนก่อน
In this lecture we leverage Sturm-Liouville theory to solve inhomogeneous partial differential equations. We demonstrate with a worked example of the heat equation with a space and time dependent heat source. We show that the solution to the PDE can be expanded as an infinite sum of the Sturm-Liouville eigenfunctions from an associated homogeneous problem for which we then obtain ordinary diffe...
Vibrations of a Nonuniform String - Partial Differential Equations | Lecture 27
มุมมอง 1442 หลายเดือนก่อน
With the previous lecture better introducing us to the Rayleigh quotient, we can now put our theories to use to better understand vibrations of a nonuniform string. In this lecture we solve a general wave equation. While the form can only be written abstractly in terms of Sturm-Liouville eigenfunctions that are unknown explicitly, we use the Rayleigh quotient to better understand the eigenvalue...
The Rayleigh Quotient - Partial Differential Equations | Lecture 26
มุมมอง 2412 หลายเดือนก่อน
The Rayleigh Quotient - Partial Differential Equations | Lecture 26
Sturm-Liouville Eigenvalues and Eigenfunctions - Partial Differential Equations | Lecture 25
มุมมอง 3252 หลายเดือนก่อน
Sturm-Liouville Eigenvalues and Eigenfunctions - Partial Differential Equations | Lecture 25
Heat Flow in a Nonuniform Rod - Partial Differential Equations | Lecture 24
มุมมอง 4652 หลายเดือนก่อน
Heat Flow in a Nonuniform Rod - Partial Differential Equations | Lecture 24
Sturm-Liouville Theory - Partial Differential Equations | Lecture 23
มุมมอง 1.1K2 หลายเดือนก่อน
Sturm-Liouville Theory - Partial Differential Equations | Lecture 23
Eigenvalues Problems in PDEs - Partial Differential Equations | Lecture 22
มุมมอง 5512 หลายเดือนก่อน
Eigenvalues Problems in PDEs - Partial Differential Equations | Lecture 22
The Wave Equation in Higher Dimensions - Partial Differential Equations | Lecture 21
มุมมอง 5722 หลายเดือนก่อน
The Wave Equation in Higher Dimensions - Partial Differential Equations | Lecture 21
Solving the Wave Equation - Partial Differential Equations | Lecture 20
มุมมอง 5832 หลายเดือนก่อน
Solving the Wave Equation - Partial Differential Equations | Lecture 20
Boundary Conditions of the Wave Equation - Partial Differential Equations | Lecture 19
มุมมอง 3532 หลายเดือนก่อน
Boundary Conditions of the Wave Equation - Partial Differential Equations | Lecture 19
The Wave Equation - Partial Differential Equations | Lecture 18
มุมมอง 7163 หลายเดือนก่อน
The Wave Equation - Partial Differential Equations | Lecture 18
Complex Fourier Series - Partial Differential Equations | Lecture 17
มุมมอง 4943 หลายเดือนก่อน
Complex Fourier Series - Partial Differential Equations | Lecture 17
Integrating Fourier Series - Partial Differential Equations | Lecture 16
มุมมอง 4733 หลายเดือนก่อน
Integrating Fourier Series - Partial Differential Equations | Lecture 16
Differentiating Fourier Series - Partial Differential Equations | Lecture 15
มุมมอง 3723 หลายเดือนก่อน
Differentiating Fourier Series - Partial Differential Equations | Lecture 15
Sine and Cosine Series - Partial Differential Equations | Lecture 14
มุมมอง 7013 หลายเดือนก่อน
Sine and Cosine Series - Partial Differential Equations | Lecture 14
Fourier Series - Partial Differential Equation | Lecture 13
มุมมอง 6063 หลายเดือนก่อน
Fourier Series - Partial Differential Equation | Lecture 13
Qualitative Properties of Laplace's Equation - Partial Differential Equations | Lecture 12
มุมมอง 3133 หลายเดือนก่อน
Qualitative Properties of Laplace's Equation - Partial Differential Equations | Lecture 12

ความคิดเห็น

  • @Mahyawr
    @Mahyawr 20 ชั่วโมงที่ผ่านมา

    Dear Professor Bramburger, Thank you for your thorough explanation. I believe I have found an error in your proof that all eigenfunctions are unique. You plugged in the boundary conditions but then concluded that the expression is zero for all x between [a, b], however, the expression is zero only on the boundaries. Sincerely Mahyar

  • @zeferreira8805
    @zeferreira8805 วันที่ผ่านมา

    I briefly studied Poincaré Maps for my final project of my bachelors. My study was more focused on a computational side of it, where I used Poicare Maps to see the periodicity/quasiperiodicity/chaotic behavious of dynamical systems. I used a little trick to view non autonomous systems on a poincare maps (although this dependeds on the vector being within boundaries for such system). The thing that I found incredible is how quasi periodic and periodic look very different in a poincare map. At first I was expecting some clusters of non converging points for the quasiperiodic, but to my surprise the points for a quasic periodic system follow a closed curve in the poincare section.

  • @drneuropharmacology2496
    @drneuropharmacology2496 วันที่ผ่านมา

    Thanks again! Are you going to more work on dynamical systems theory or a series on neuronal dynamics/mathematical neuroscience

  • @zhuyan2008
    @zhuyan2008 2 วันที่ผ่านมา

    Thank you, Professor. After I left school, I usually learned math by reading books and doing exercises. I have tried several TH-cam videos before. You are the first to make me think that video lectures on Math can be quite helpful.

  • @larrydurante9849
    @larrydurante9849 4 วันที่ผ่านมา

    Dear Jason, so well done, I studied this 40 years ago, now I'm reviewing for research reasons, and I'm so appreciative for your in depth and intuitive approach. Thanks a ton, an Electrical Engineer before simulations ruled :)

    • @jasonbramburger
      @jasonbramburger 4 วันที่ผ่านมา

      Glad I can help and thanks for watching!

  • @NL_PG
    @NL_PG 5 วันที่ผ่านมา

    Thanks, a lot!

  • @정현수-u3c
    @정현수-u3c 6 วันที่ผ่านมา

    Thank you for my engineering mathematics ...

  • @jjyang4469
    @jjyang4469 7 วันที่ผ่านมา

    you are saving lives out here what a great video

  • @drneuropharmacology2496
    @drneuropharmacology2496 7 วันที่ผ่านมา

    Jason you've clearly put so much into this, thank you for your efforts teaching. Would you consider doing an applied series on neuronal dynamics using "Dynamical systems in neuroscience" by izhikevich 2005?

  • @alluwix
    @alluwix 7 วันที่ผ่านมา

    Thanks for this lecture! I'm struggling to work out if/how this relates to action angle coordinates in Hamiltonian mechanics.

  • @JesusSportsNature
    @JesusSportsNature 8 วันที่ผ่านมา

    So interesting! Thank you for explaining.

  • @JesusSportsNature
    @JesusSportsNature 8 วันที่ผ่านมา

    Thank you for these videos!

  • @hrkalita159
    @hrkalita159 8 วันที่ผ่านมา

    one of the best yt channel but yet very under rated .

    • @jasonbramburger
      @jasonbramburger 8 วันที่ผ่านมา

      Thanks for your support!

  • @therealone2418
    @therealone2418 9 วันที่ผ่านมา

    very much helpful

  • @therealone2418
    @therealone2418 10 วันที่ผ่านมา

    damn , these lectures are so helpful . thanks sir

  • @manfredbogner9799
    @manfredbogner9799 12 วันที่ผ่านมา

    Sehr gur

  • @manfredbogner9799
    @manfredbogner9799 12 วันที่ผ่านมา

    Sehr gut

  • @pollenahmed9522
    @pollenahmed9522 13 วันที่ผ่านมา

    my test is this morning and I am cooked.

  • @klausoldie4197
    @klausoldie4197 15 วันที่ผ่านมา

    impressive video. At time 37:25 the coefficients of the sin and cos term are interchanged -> 48/17 sin(t)+12/17 cos(t)

  • @mmesomaemmanuelanukam3722
    @mmesomaemmanuelanukam3722 16 วันที่ผ่านมา

    When we assume v(0) is 0, isn't D = 49 instead of -49? Or is it possible for D to be positive and negative at the same time?

  • @g.sunilnaikg.sunilnai7996
    @g.sunilnaikg.sunilnai7996 17 วันที่ผ่านมา

    i love mathematical modelling and from today im your student im a civil engineering graduate sir

  • @senz3081
    @senz3081 18 วันที่ผ่านมา

    Thank you for doing God’s work, sir.

  • @ankit-jy1oi
    @ankit-jy1oi 19 วันที่ผ่านมา

    I am an electrical engineer...enjoyed your lecture.

  • @hrkalita159
    @hrkalita159 19 วันที่ผ่านมา

    will factor 3 appear in @10:30

  • @Loots1
    @Loots1 20 วันที่ผ่านมา

    excuse me, is this for math364?

    • @jasonbramburger
      @jasonbramburger 20 วันที่ผ่านมา

      Not precisely, but it covers many of the same concepts

    • @Loots1
      @Loots1 20 วันที่ผ่านมา

      @@jasonbramburger ok thanks im a 3rd year CONu student in pure and applied math, hope to run into you one day :) be well and safe!

  • @solomonapuu542
    @solomonapuu542 20 วันที่ผ่านมา

    I passed my PhD Mathematics Qualifying Exams at the first trial last month (August, 2024). Your PDE lecture series were very instrumental to my success. Thank you very much for your great content.

    • @jasonbramburger
      @jasonbramburger 20 วันที่ผ่านมา

      Glad I can help and good job!

  • @crow1999x
    @crow1999x 22 วันที่ผ่านมา

    you saved UAB engineering grad students my man

    • @jasonbramburger
      @jasonbramburger 22 วันที่ผ่านมา

      Love UAB! Visited a couple years ago for a talk

  • @dutonic
    @dutonic 22 วันที่ผ่านมา

    Here to solidify a foundation in D.S. that can help me work with ties between probability theory and fractal geometry for problems in quantum physics. Excited to work through this. Thank you for taking the time to make these!

  • @billworthers1075
    @billworthers1075 25 วันที่ผ่านมา

    How is he writing on the blackboard like that?

  • @jeffreymolony2308
    @jeffreymolony2308 25 วันที่ผ่านมา

    Good Stuff! You are a great man.

  • @veerstar5
    @veerstar5 26 วันที่ผ่านมา

    r u nuts? what's the point of using transparent glass. Get a board idiot.

  • @charlie3k
    @charlie3k 27 วันที่ผ่านมา

    2 years ago I watched your Calculus II video series to help study. This semester I am taking PDEs and am delighted to see you have a new playlist! Keep up the great work :)

    • @jasonbramburger
      @jasonbramburger 26 วันที่ผ่านมา

      Glad I can help and thanks for sticking around for so long!

  • @nonato7853
    @nonato7853 27 วันที่ผ่านมา

    OMG! That's all I wanted right now!!!!!!!!!!!!!!!!!!! Thnks!!!!!!!

  • @gt6139a
    @gt6139a 27 วันที่ผ่านมา

    Thank you for your lectures. It is a well explained series so far and I am really enjoying it. Thank you. However, I do have 1 question: why can't growth and decay happen in a second order linear system? The spring mass damper system has oscillations as well as decay and it is a second order system.

  • @jeffreymolony2308
    @jeffreymolony2308 หลายเดือนก่อน

    After taking your Dynamical Systems course, it seems that dynamical systems can run forward and backward in time. But the forward (in time) Heat Equation and the backward (in time) Heat Equation are different. Is this true?

    • @jasonbramburger
      @jasonbramburger 28 วันที่ผ่านมา

      Yes, running PDEs backward in time is very problematic. For ODEs the standard existence and uniqueness theorems guarantee that solutions can be flowed both forward and backward (locally) in time. However, PDEs don't have these properties usually. One way to think of this is the fundamental solution of the heat equation that starts with a Dirac delta function at t = 0 and becomes a Gaussian for all t > 0. Try to imagine what would this solution would look like if we took t < 0, though. I can't... This is just a simple example, but it illuminates some technicalities without getting into the actual math.

    • @jeffreymolony2308
      @jeffreymolony2308 28 วันที่ผ่านมา

      @@jasonbramburger Thank you for your reply. I've heard it said that the only known law of physics that is NOT reversable in time is the 2nd Law of Thermodynamics, and from this we can relate the Arrow of Time with Entropy. BUT... your example contradicts this...Maybe??????

    • @jasonbramburger
      @jasonbramburger 28 วันที่ผ่านมา

      @@jeffreymolony2308 No my example does not contradict this. These things are not related to my knowledge.

  • @dnaviap
    @dnaviap หลายเดือนก่อน

    Amazing lecture, thanks a lot!

  • @nicholasseifert4072
    @nicholasseifert4072 หลายเดือนก่อน

    Really cool. Thanks from Brazil

    • @jasonbramburger
      @jasonbramburger หลายเดือนก่อน

      Thanks for watching! (from Canada)

  • @Stefabro
    @Stefabro หลายเดือนก่อน

    thank you for this! I was looking for this proof for my numerical analysis course but couldn't find a video that made sense to me, until now

  • @jeffreymolony2308
    @jeffreymolony2308 หลายเดือนก่อน

    Great Series! Fantastic! Thank You for your time, effort, and expertise!

  • @graemelawson1327
    @graemelawson1327 หลายเดือนก่อน

    Great job. I jumped into the lecture on poincare maps, as a refresher. Have also watched a few others as well. You are an excellent communicator, and the content is spot on.

    • @jasonbramburger
      @jasonbramburger หลายเดือนก่อน

      Thanks for watching! I'm glad I can help!

  • @DebarghaRay-r8k
    @DebarghaRay-r8k หลายเดือนก่อน

    Bro you're MY Genie ❤❤

  • @abhisheksingh-li6zo
    @abhisheksingh-li6zo หลายเดือนก่อน

    Which book would you recommend , very nice video

    • @jasonbramburger
      @jasonbramburger หลายเดือนก่อน

      In the intro video I mention Strogatz's book

  • @jeffreymolony2308
    @jeffreymolony2308 หลายเดือนก่อน

    I'm up to Lecture 23 and I have to say Fantastic Lecture Series and Thank You!!!

  • @vootanical5512
    @vootanical5512 หลายเดือนก่อน

    is this direction promising now?

  • @JPRL
    @JPRL หลายเดือนก่อน

    This is gold, thank you for these videos

  • @ansonpang8468
    @ansonpang8468 หลายเดือนก่อน

    Gonna do a Linear Algebra series in the future?

    • @jasonbramburger
      @jasonbramburger หลายเดือนก่อน

      Not anytime soon. There are plenty of other resources on YT that do linear algebra quite well and I don't want to compete with them.

  • @DebarghaRay-r8k
    @DebarghaRay-r8k หลายเดือนก่อน

    17:18 doesn't that sign from 0 to -infinity say y is increasing?

    • @jasonbramburger
      @jasonbramburger หลายเดือนก่อน

      Yes, that is what is drawn in the figure

  • @antonioe.2396
    @antonioe.2396 หลายเดือนก่อน

    As an electrical engineer I am fascinated by this equation and know for a fact the utility of it. Do you know if there's any material that explains the relationship of this equation properties with the electromagnetic fields?

  • @LaureanoLuna
    @LaureanoLuna หลายเดือนก่อน

    No precise definition of linearity for DEs is given...

  • @DebarghaRay-r8k
    @DebarghaRay-r8k หลายเดือนก่อน

    My brain is hamburgered.Amzing job btw