Paul,

Sorry to have given such an off target answer! Your idea about checking the dot product as you progress makes sense. That's how VTK's a hyper stream tracer handles the issue. I wonder if you can make use of it? Bringing VTK classes into PV isn't too hard but parallelizing them can be challenging.

Burlen

On 08/24/2013 12:27 PM, Burlen Loring wrote:
in the case of the glyphing algorithm it's the surface normals of the transformed glyph that have the relation to the sign determinant of the transform matrix. this transformation matrix is constructed from the eigenvectors directly. at any rate, good luck.

On 08/23/2013 06:35 PM, pwhiteho wrote:
Burlen, you had me hoping, but alas ... there is no direct correlation between the determinant ( a.k.a. the 3rd tensor invariant ) and the orientation of the computed eigenvectors. You did get me thinking there may be other possibilities. I'm sure I can use the dot product in a marching cube scheme to enforce a consistent orientation progression and generate a "vector" field ParaView will handle well. It'll just have to be robust enough to handle a true change near some sharp topological feature.

Thanks,
Paul

------------------------------------------------------------------------
*From:* Burlen Loring [[email protected]]
*Sent:* Friday, August 23, 2013 4:31 PM
*To:* Andy Bauer; pwhiteho
*Cc:* [email protected]
*Subject:* Re: [Paraview] Stream Tracer in eigenvector field

Eigenvectors are unique up to a constantso if you took any eigenvector and multiplied it by -1 it's still an eigenvector. You could see it in the definition,

M x=\lambda x

eigenvector x appears in both sides of the eqn.

I had a similar problem with tensor glyphs in ParaView. In that case I was able to solve by looking at the sign of the determinant of the transformation matrix (see bug report, patch and mail list posts below). I wonder if you could adapt/build on this solution there to solve your issue here?

http://vtk.org/Bug/view.php?id=12179
http://vtk.1045678.n5.nabble.com/tensor-glyph-inward-pointing-surface-normals-td4388361.html

Burlen


On 08/23/2013 01:10 PM, Andy Bauer wrote:
Hi Paul,

Apologies as my math is a bit rusty but isn't the sign of the eigenvector related to the sign of its corresponding eigenvalue? In that case if you make sure that all of the eigenvalues are positive then all of their corresponding eigenvectors should be aligned properly. If that's the case and you have access to the eigenvalues of the eigenvectors you could use the calculator or python calculator to properly orient the eigenvectors.

In any case, if you can come up with an algorithm that properly orients the eigenvectors you should be able to do that in the python calculator or calculator filters. If not, then things could get a bit hairy as far as computationally figuring out which is the "proper" direction your eigenvalues should have.

Regards,
Andy


On Fri, Aug 23, 2013 at 3:38 PM, pwhiteho <[email protected] <mailto:[email protected]>> wrote:

    The term "eigenvector", used to describe the principal
    directions of a tensor, is a bit of a misnomer since it's not a
    "vector" as interpreted by the Stream Tracer filter - it's more
    accurately bi-directional like tension/compression and could be
    termed "eigenaxis/eigenaxes". When interpreted as a vector,
    there is an inherent sign ambiguity in each eigenvector - the
    sign is indeterminate and one is free to choose + or -, and that
    is exactly what Mathematica does ( likely true for other
    routines also ).

    I've been using Mathematica to prototype computations for the
    investigation of tensor topology which I then visualize in
    ParaView. Eigen-decomposition of a tensor field at each grid
    point returns an orthonormal set of eigenvectors, uncorrelated
    with any neighbors. Taken separately, each eigenvector field
    exhibits large regions of smoothly varying orientation, but
    there are systematic and random reversals of orientation that
    confound the Stream Tracer filter, sending streamlines wandering
    around the field. What is needed is a true tangent curve (
    tensor line ) integrator that would avoid "doubling back" as the
    "streamline" propagates, similar to the scheme of Weinstein, et.
    al., ( IEEE VIS'99 ) which computes the dot product of the
    incoming propagation vector with the eigenvector; and if near
    -1, negate the outgoing propagation vector. This can also be
    fancied-up to accommodate noisy initial tensor data as in Weinstein.

    I think I would be taking on too much at this point in learning
    to write my own filter so have been exploring ways to
    pre-process the eigenvector fields before visualizing in
    Paraview, but I ask:
    1. Have I missed something in existing filters that would handle
    this?
    2. Can the existing Stream Tracer be modified?
    3. Does the eigenvector routine in ParaView yield the same sign
    ambiguity among uncorrelated computations?

    Thanks,
    Paul W


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