This lecture provides an overview of the algorithm (exact DMD) for computing DMD modes and eigenvalues. Several examples are demonstrated where the DMD provides interpretable and low-rank decompositions of the data.
Пікірлер: 18
@muhammadahsanzamee43853 жыл бұрын
literally, i can listen to professor Kutz for hours and not get bored. He is a genius.
@erenkeskus61326 жыл бұрын
I can't wait to try this on multivariate time series data. (namely security prices) . I appreciated this class, it was very explanatory. I've read an article by you about an DMD application and for me now everything is put in place. Thank you for the upload.
@casusbelli4905 Жыл бұрын
Brilliant lecture. Thank you Professor!
@dr.alikhudhair9414 Жыл бұрын
Wonderful Lec .. thank you professor
@mohammadkhezri68775 ай бұрын
Thank you, it was very helpful🌹
@shutaoshen81153 жыл бұрын
easy to understand, as a supplement of the paper of "A KERNEL-BASED METHOD FOR DATA-DRIVEN KOOPMAN SPECTRAL ANALYSIS"
@a3igner2 жыл бұрын
@NathanKutz what’s the optimal length of the time window to use? How do you determine this? One will cutoff any long wavelength modes that are greater than the length of the time window (or T/2)
@blchen13 жыл бұрын
At 28:09, if we use svds(X1,r) to get the truncated singular vectors, they differ by a constant complex phase compared with those obtained by svd(X1,'econ'). But somehow that affects the eigen-modes Phi. Should I stick with svd when doing DMD or am I missing something? Thanks!
@theohlong3074 жыл бұрын
this is something really cool, omg !!!
@nurulashikin49302 жыл бұрын
Hi, Prof. May I know how to plot the true mode to compare with the DMD modes and PCA signal, in addition, I would like to know how to plot the time dynamics to be compared with singular vector V. Thank you 🙏
@shabyshaby1235 жыл бұрын
Is it correct to call Atilde a similarity transform? It's clear that eigenvalues of A and Atilde are the same, but is Ur'*A*Ur a similarity transform when Ur is not square?
@PABITRABADHUK4 жыл бұрын
The operation is a similarity transformation from an n*n dimensional space to an r*r dimensional space.
@JeffMTX6 жыл бұрын
Try setting f1 and f2 equal to their real parts only, before doing the POD or otherwise. It doesn't work very well. It would be really awesome to see an example that used real-valued example data!
@nikhileshnatraj3316 жыл бұрын
J M I tried this. Setting real values f1 and f2 roughly translates to the dynamics of a standing wave (no oscillations through time for the sech and tanh functions). The X matrix then has to be transformed into a Hankel matrix ... this models the dynamics and solves the problem. Hankel matrix: take X from 1 up to n-m where n is no of time points and m is number of stacks , say 20 for n=1000. Right below X, append X from 2 to n-m+1. Below this new X, append from 3 to n-m+2 and so on... essentially you are inflating X in its height stacking on top o each other. Notice this construction introduces time dynamics and solves the problem
@goharshoukat37824 жыл бұрын
At 30:28, you divide by Sr. Shouldnt you multiply it with inv(Sr)? Or am I missing something?
@matthewjames75133 жыл бұрын
"/" is the matrix divide. It's the same thing as multiplying by the inverse.au.mathworks.com/help/fixedpoint/ref/embedded.fi.mrdivide.html
@pradnyajagtap36382 жыл бұрын
how x is given as summation of bj*phij*e^wjt ?
@user-rs9cg2zg2n2 жыл бұрын
In dx/dt = Ax vector x is a set of variables and A is a transform matrix and in term of system of linear equations A has coefficients of system and x has unknown functions so Euler's method can be applied. According to it solution is x_i(t)=b_i*phi_i*e^lambda_i*t where lambda_i is eigenvalue, phi_i is eigenvector corresponding to lambda_i and b_i is initial solution when t=0