over two decades of integration-based, geometric vector field visualization

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Over Two Decades of Integration-Based, Geometric Vector Field Visualization. Part III: Curve based seeding Planar based seeding Ronny Peikert ETH Zurich. Overview. Curve-based seeding objects steady flow stream surfaces unsteady flow "path surfaces" "streak surfaces" - PowerPoint PPT Presentation

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Ronny Peikertpeikert@inf.ethz.ch

Over Two Decades of Integration-Based, Geometric Vector Field Visualization

Part III: Curve based seedingPlanar based seeding

Ronny PeikertETH Zurich

1http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Overview Curve-based seeding objects

steady flow stream surfaces

unsteady flow "path surfaces" "streak surfaces"

Planar-based seeding objects steady flow unsteady flow

Orthogonal surfaces of a vector field Discussion, future research opportunities

2http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Stream surfaces

3http://graphics.ethz.ch/~peikert

Definition A stream surface is the union of the stream lines

seeded at all points of a curve (the seed curve). Motivation

separates (steady) flow, flow cannot cross the surface

surfaces offer more rendering options than lines (perception!)

Ronny Peikertpeikert@inf.ethz.ch

Stream surfaces

4http://graphics.ethz.ch/~peikert

First stream surface computation done before SciVis existed!

Early use in flow visualization (Helman and

Hesselink 1990) for flow separation

Image: Ying et al.

Ronny Peikertpeikert@inf.ethz.ch

Stream surface integration Problem: naïve algorithm fails if streamlines

diverge or grow at largely different speeds. Example of failure: seed curve which extends

to no-slip boundary:

5http://graphics.ethz.ch/~peikert

fixed time steps slightly better: fixed spatial steps

wall (u = 0)

streamlines

streamlines

Ronny Peikertpeikert@inf.ethz.ch

Hultquist's algorithm Hultquist's algorithm (Hultquist 1992) does

optimized triangulation: Of two possible connections choose the one

which is closer to orthogonal to both streamlines.

6http://graphics.ethz.ch/~peikert

systematictriangulation

optimizedtriangulation

stre

amlin

es

stre

amlin

es

Ronny Peikertpeikert@inf.ethz.ch

Hultquist's algorithm (2) The problem of divergence or convergence is

solved by inserting or terminating streamlines.

7http://graphics.ethz.ch/~peikert

inserted streamline terminated streamline

Ronny Peikertpeikert@inf.ethz.ch

Curvature of front curve controlled by limiting the dihedral angle of the mesh (Garth et al. 2004)

Adaptive refinement Intricate structure of vortex

breakdown bubble

Refined Hultquist methods

8http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Refined Hultquist methods (2) Cubic Hermite interpolation along the front

curves. Runge-Kutta used to propagate front and its covariant derivatives (Schneider et al. 2009)

9http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Analytical methods In a tetrahedral cell the vector field

is linearly interpolated: Streamline has equation Stream surface seeded on straight

line (entry curve) is a ruled surface. Exit curve is computed analytically

respecting boundary switch curves

10http://graphics.ethz.ch/~peikert

( ) u x Ax( ) tt e Αx x0

HultquistScheuermann

(Scheuermann et al., 2001).

Ronny Peikertpeikert@inf.ethz.ch

Implicit methods A stream function is a special*) solution of

the PDE[don't confuse with a potential which has PDE ]

11http://graphics.ethz.ch/~peikert

0x u x x

x u x

streamline

stream surfaces

a x b x

d x

c x

*) mass flux = r(b-a)(d-c)

Ronny Peikertpeikert@inf.ethz.ch

Implicit methods (2) Stream functions

exist for divergence-free vector fields (= incompressible flow)

… and for compressible flow, if there are no sinks/sources are computed by solving a PDE (with appropriate

boundary conditions) yield stream surfaces by isosurface extraction

Advantage of stream function method (Kenwright

and Mallinson, 1992, van Wijk, 1993): conservation of mass!

12http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Implicit methods (3) Computational space method, implicit

method per cell, respects conservation of mass (van Gelder, 2001)

13http://graphics.ethz.ch/~peikert

Delta wing. Stream surface close to boundary. Flow separation and attachment.

Ronny Peikertpeikert@inf.ethz.ch

Rendering of stream surfaces Stream arrows

(Löffelmann et al. 1997) Texture advection on stream

surfaces (Laramee et al. 2006)

14http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Rendering of stream surfaces (2)

15http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Invariant 2D manifolds Critical points of types saddle and focus saddle (spiral

saddle) have a stream surface converging to them.

And so do periodic orbits of types saddle and twisted saddle.

16http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Invariant 2D manifolds Saddle connectors (Theisel et al, 2003)

Visualization of topological skeleton of 3D vector fields

Intersection of 2D manifolds of (focus) saddles

17http://graphics.ethz.ch/~peikert

Flow past a cylinder

saddle-connector of a pair of focus saddle crit. points

Ronny Peikertpeikert@inf.ethz.ch

Geodesic circles stream surface algorithm (Krauskopf and Osinga 1999) Front grows radially (not along stream lines) by solving a boundary value problem "immune" against spiraling

Invariant 2D manifolds (2)

18http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Invariant 2D manifolds (3) Topology-aware stream surface method

(Peikert and Sadlo, 2009) starts at critical point, periodic

orbit, or given seed curve handles convergence to saddle

or sink

19http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Path surfaces Particle based path surfaces

(Schafhitzel et al. 2007) Density control a la Hultquist Point splatting 1st order Euler integration GPU implementation

interactive seeding!

20http://graphics.ethz.ch/~peikert

Path surface of unsteady flow past a cylinder

Ronny Peikertpeikert@inf.ethz.ch

Streak surfaces Smoke surfaces are a technique based on

streak surfaces (von Funck et al. 2008) advected mesh is not

retriangulated, but size/shape of triangles is

mapped to opacity simplified optical model

for smoke

21http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Planar based seeding Planar-based seeding for steady flow

Stream polygons (Schroeder et al. 1991)

Flow volumes (Max et al. 1993)

Implicit flow volumes(Xue et al. 2004)

22http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

Planar based seeding (2) Planar-based seeding for unsteady flow

Extension of flow volume technique to unsteady vector fields(Becker et at. 1995).

23http://graphics.ethz.ch/~peikert

Image: Crawfis, Shen, MaxUnsteady flow volume

Ronny Peikertpeikert@inf.ethz.ch

Orthogonal surfaces Surfaces (approximately) orthogonal to a vector (or eigen-

vector) field as a visualization technique (Zhang et al. 2003). If a vector field is conservative, , its potential can be

visualized with a scalar field visualization technique, such as isosurfaces.

Orthogonal surfaces exist also in the slightly more general case of helicity-free vector fields .

However, 3D flow fields usually have helicity. Also eigenvector fields of symmetric 3D tensors.

Consequence: For many applications, orthogonal surfaces are less suitable (discussed by Schultz et al. 2009).

24http://graphics.ethz.ch/~peikert

u 0

u u 0

Ronny Peikertpeikert@inf.ethz.ch

Discussion, future research There is no single best flow vis technique! Most effort spent so far on streamlines

Extension to unsteady flow somewhat lacking behind Also extension to stream surfaces (and unsteady variants)

Other areas needing more research: Uncertainty visualization tools for geometric techniques Comparative visualization tools for geometric techniques Improved surface and volume construction methods Automatic seeding for surfaces and volumes

25http://graphics.ethz.ch/~peikert

Ronny Peikertpeikert@inf.ethz.ch

The End

26http://graphics.ethz.ch/~peikert

Thank you for your attention! Any questions?

We would like to thank the following:R. Crawfis, W. v. Funck, C. Garth, J.L. Helman, J. Hultquist, H. Loeffelmann, N. Max, H. Osinga, T. Schafhitzel, G. Scheuermann, D. Schneider, W. Schroeder, H.W. Shen, H. Theisel, T. Weinkauf, S.X. Ying, D. Xue

PDF versions of STAR and MPEG movies available at:http://cs.swan.ac.uk/~csbob

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