ETH Zürich DLSC: Physics-Informed Neural Networks - Applications

Поделиться
HTML-код
  • Опубликовано: 25 авг 2024

Комментарии • 9

  • @be_happy974
    @be_happy974 5 месяцев назад +2

    it's great, hardly find teach code video of PINN

  • @ramversingh7867
    @ramversingh7867 10 месяцев назад +1

    Awesome 👌. Thanks for sharing valuable knowledge about the topic.

  • @yangluo8317
    @yangluo8317 20 дней назад

    awesome lecture. Since I am new to PINNs, I just want to know what if we could not have access to the PDEs formulation.....

  • @tuo9433
    @tuo9433 11 дней назад

    I wonder if PINNs can solve the three-bodies problem :D

  • @akshays6272
    @akshays6272 Год назад +1

    Why there is no collocation loss term in the second example?

  • @prefachinho
    @prefachinho 6 месяцев назад +2

    Is the Jupyter file of the harmonic oscillator demo available anywhere?

    • @CAMLabETHZurich
      @CAMLabETHZurich  Месяц назад

      All code shown in the lectures is here: github.com/benmoseley/DLSC-2023

  • @user-jf8mm5jn9l
    @user-jf8mm5jn9l 10 месяцев назад +1

    why is the physics loss is 0?

    • @thisisharold9066
      @thisisharold9066 2 месяца назад

      I think that is because the undamped spring mass system can be model with *second order homogeneous ordinary differential equation*, y'' + p(x)*y' + q(x)*y = 0. If you model for forced response, E.g. charging response of resistor-inductor-capacitor circuit with 3.3 volts as input, then physics will not be 0. y'' + p(x)*y' + q(x)*y = -3.3.