vacuum pair production/annihilation and cardiac string dynamics · 2019-01-18 · vacuum pair...
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Vacuum Pair Production/Annihilation and Cardiac String Dynamics
John P. Wikswo
Living State Physics Group
Departments of Physics and Astronomy, Molecular Physiology & Biophysics, and Biomedical Engineering
Vanderbilt Institute for Integrative Biosystems Research and Education
Vanderbilt University
Aspen Center for Physics, August 22, 2002 scroll_wave_breakup_fhnplus_high-res.mov
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Acknowledgements
• Rubin Aliev • Mark Bray • Elizabeth Cherry • Deborah Echt • Flavio Fenton • Rick Gray • Peter Hunter • Alain Karma • Mark Lin • Neils Otani • Arkardy Pertsov • Nathalie Virag • Jim Weiss • And many others
textured-heart-spin.mpg
Courtesy of Peter Hunter, Auckland
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Where are the heart strings, and who is pulling
them?
• The normal heart has none
• The presence of one string is serious
• The presence of several for a very few minutes is fatal
flavio_rabbit_vf.avi
Courtesy of Flavio Fenton, Hofstra
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Outline • The heart is a … • Cardiac fibrillation • Spiral waves in the heart
– Two dimensions – Spiral waves – Three dimensions – Scroll waves
• Phase plane analysis • Singularity identification
– Simple reentry – Fibrillation
• Singularity interactions – Attraction vs repulsion versus
oscillation – Annihilation – Creation
• What is needed? – Interaction potential – String creation operator
Β
θ
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The Heart is a…
• Self-assembling, • Biochemically powered, • Electrically activated, • Electrically non-linear, • Pressure- and volume-regulated, • Two-stage, • Tandem, • Mechanical pump • With a mean time-to-failure of
approximately two billion cycles.
s00045
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The heart is ... electrically activated …
Courtesy of Peter Hunter, Auckland
normalbsm.mpg
From: The Ciba Collection of Medical Illustrations: Heart, F. H. Netter, 1978
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7 s00077
The heart is an …
• Electrically activated,
• Mechanical pump
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The Normal Heart Beat
Courtesy of Rick Gray and CRML, U. Alabama Birmingham
SwineSinus.mov
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Outline • The heart is a … • Cardiac fibrillation • Spiral waves in the heart
– Two dimensions – Spiral waves – Three dimensions – Scroll waves
• Phase plane analysis • Singularity identification
– Simple reentry – Fibrillation
• Singularity interactions – Attraction vs repulsion versus
oscillation – Annihilation – Creation
• What is needed? – Interaction potential – String creation operator Courtesy of Flavio Fenton
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Normal Tachycardia Fibrillation Defibrillation
The heart is an electrically activated mechanical pump
…with a mean time-to-failure of approximately two billion cycles….
Courtesy of Debra Echt
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Induction of Fibrillation
Courtesy of Rick Gray and CRML, U. Alabama Birmingham
SwineSinusVF.mov
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Termination of Fibrillation
Courtesy of Rick Gray and CRML, U. Alabama Birmingham
SwineVFShockSinus.mov
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Outline • The heart is a … • Cardiac fibrillation • Spiral waves in the heart
– Two dimensions – Spiral waves – Three dimensions – Scroll waves
• Phase plane analysis • Singularity identification
– Simple reentry – Fibrillation
• Singularity interactions – Attraction vs repulsion versus
oscillation – Annihilation – Creation
• What is needed? – Interaction potential – String creation operator Leon Glass and Physics Today
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Spiral and Scroll Waves in Nature
• A generic property of excitable media • Have been shown to occur in
–Circulating waves of bioelectric activity in cardiac and retinal tissue –Autocatalytic chemical reactions, such as Belousov-Zhabotinsky reaction (BZ) –cAMP waves in slime mold Dictyostelium discoideum –Intracellular calcium release in oocytes –Oxidation of CO on crystal surfaces in ultrahigh vacuum conditions
• Cardiac fibrillation involves multiple scroll waves in 3-D
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Cardiac fibrillation occurs at the spatial scale of the entire heart, and involves multiple, interacting spiral and/or scroll waves!
Physics Today and Leon Glass, Montreal
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Transmural versus intramural scroll waves in reentrant arrhythmias and fibrillation
• Transmural waves can exist in 2-D (thin) or 3-D (thick) • Intramural waves require ~1 cm wall thickness
Courtesy of Arkady Pertsov, Syracuse
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VF VT Normal Rhythm
Transition from Normal Rhythm to Ventricular Tachycardia to
Ventricular Fibrillation
Single spiral wave = Tachycardia Multiple spiral waves = Fibrillation = SCD
SBB.avi Movies courtesy of Flavio Fenton scclong.avi SA.avi
A. Karma, Chaos 4 (3): 461-472, 1994
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Initiation of Spiral
Wave Reentry
S1-S2 crossed- field stimulation
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A “Simple” Spiral Wave
The nature of the spiral is set by the non-linear properties of the excitable medium
– Linear core – Epicycloidal
meander – Circular core
Courtesy of Flavio Fenton tspiralgs.avi
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Nonlinear Properties Determine the Trajectories
• Six Phenotypes – Circular – Epicycloidal – Cycloid – Hypercycloidal – Hypermeander – Linear core
• Winfree, Krinsky,
Barkley, Efimov, Jalife, Pertsov, Gray, Roth, Fenton, Garfinkel, Chen …
Courtesy of Flavio Fenton
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Non-linear dynamics of reentry, fibrillation, and defibrillation
• Reentry -- Self-sustained excitation due to propagating activation wave fronts in the heart that continue to re-excite different regions of tissue rather than terminating after a single excitation
• Anatomical reentry -- activation wave fronts that travel in one direction around an anatomical obstacle
• Functional reentry -- activation circulate around a dynamical phase singularity
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Spiral Wave and
Figure-of-Eight Reentry
• Spiral Wave: – S1 vert line – S2 horiz line
• Figure-of-Eight – S1 vert line – S2 point
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Spiral Wave, Figure-of-Eight, and Quatrefoil Reentry
• Spiral Wave (A) – S1 vertical line – S2 horizontal line – One singularity (plus
boundary) • Figure-of-Eight (B)
– S1 vertical line – S2 point – Two singularities
• Quatrefoil (C & D) – Anisotropic cable – S1 point – S2 point – Cathodal (C) or anodal (D)
have opposite rotations – Four singularities
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Anodal-Break Isochrones
Tim
e
Cathodal-Break Isochrones
S1 S2
A
B
D C
Optical Imaging of Quatrefoil Reentry
SF Lin, BJ Roth, and JP Wikswo. J. Cardiovasc. Electrophysiol. 10(4): 574-586, 1999
M-A Bray, S-F Lin, RR Aliev, BJ Roth, and JP Wikswo, J. Cardiovasc. Electrophysiol. 12(6): 716-722, 2001.
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Outline • The heart is a … • Cardiac fibrillation • Spiral waves in the heart
– Two dimensions – Spiral waves – Three dimensions – Scroll waves
• Phase plane analysis • Singularity identification
– Simple reentry – Fibrillation
• Singularity interactions – Attraction vs repulsion versus
oscillation – Annihilation – Creation
• What is needed? – Interaction potential – String creation operator
Β
θ
Courtesy of Mark Bray
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Β
θ
π
−π
Transmembrane Potential
Time
Time
Vm
Vm (t)
dVm
(t)/d
t
1 ( , , )( , , ) tan( , , ) /m
m
V x y tx y tdV x y t dt
φ − =
Pictures by Mark Bray
Method by RA Gray, AM Pertsov, and J Jalife, Nature 392: 75 (1998)
Phase
Transform into Phase Space
•The problem: a given voltage can either be rising or falling
•The solution: represent the cardiac action potential in terms of “phase” in the cardiac cycle: – 0, 1, 2, 3 … – 1%, 2%, 3%, 3%, 5%, … – 0o, 5o, 10o, 15o, 20o, 25o, …
•One definition of phase (of many):
Pixel
by
Pixel
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From Voltage to Phase Space
Four singularities of indeterminate phase, i.e.,points surrounded by all colors
π
-π
1 2
3 4
Experiment Theory
Phas
e
Frame Difference
M-A Bray, S-F Lin, RR Aliev, BJ Roth, and JP Wikswo, J. Cardiovasc. Electrophysiol. 12(6): 716-722, 2001.
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Outline • The heart is a … • Cardiac fibrillation • Spiral waves in the heart
– Two dimensions – Spiral waves – Three dimensions – Scroll waves
• Phase plane analysis • Singularity identification
– Simple reentry – Fibrillation
• Singularity interactions – Attraction vs repulsion versus
oscillation – Annihilation – Creation
• What is needed? – Interaction potential – String creation operator Mark Bray
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Why look for strings? •Movies of the surface potentials are complicated
•It is not clear how much of the information is needed
•Model based upon –R.R. Aliev and A.V. Panfilov, A. V., Chaos, Solitons, & Fractals, 7(3): 293-301 (1996)
–Gray, R. A. and Jalife, J., Chaos, 8(1): 65-78 (1998)
•Movies by Mark Bray fhnplus_scroll_wave_breakup_surface_fps60.avi
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Wavefronts are Better
• The wavefronts are better
• Require description of the dynamics of the entire system
fhnplus_scroll_wave_breakup_filament_plus_wavefront_fps60.avi Mark Bray
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Strings Alone May Be Best • Surface
singularities are simpler
• Filaments (strings) are the best
• Do they interact in a manner that can allow us to ignore the rest of the problem?
• HOW DO WE FIND THEM??
fhnplus_scroll_wave_breakup_filament_fps60.avi Mark Bray
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Local Phase and the Wave Vector
• The spatial gradient of the phase φ is the wave vector
k
k
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Phase and Topological Charge • Curl k is proportional to the topological charge!
• It can be shown that the differential curl evaluates as exactly zero, except at the singularity, where it is undefined.
• At the singularity, the line integral around the singularity must be used directly to find the topological charge.
“Use of Topological Charge to Determine Filament Location in a Numerical Model of Scroll Wave Activity,” M.-A. Bray and J.P. Wikswo, Jr., IEEE Trans BME, in press
0
1[ ( )] lim ( )ˆ y xS
c
k kz k x k r dx y S∆ →
∂ ∂⋅ ∇× = − = ⋅
∂ ∂ ∆ ∫
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Phase Singularities in Cardiac Reentry
The phase singularities can be identified by computing the curl of the gradient of the phase distribution
Phase (φ) plot Curl k = Curl (∇φ)
Mark Bray
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Topological Charge
• Topological charge nt is zero about any closed path that does not encircle a phase singularity
• nt is +1 or -1 for a path that encircles a singularity with a single arm
• Topological charge is conserved, i.e., singularities are created and destroyed in pairs.
Phase(x,y)
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Singularity Motion During Spiral Wave Breakup
Voltage Curl of Phase
Courtesy of Rick Gray BRDR.avi
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Filaments in Three Dimensions
• Filaments are the 3-D analogue of the 2-D phase singularity
What looks like a figure-of-eight reentrant wave from the surface...
...is actually a 3-D scroll wave in the underlying myocardium with a filament connecting the two singularities
Mark Bray
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Topological charge
• Curl k may be approximated by 1) a differential operator, or 2) as a discretized contour interval that is in
fact a convolution operation of an image with two Nabla windows
Bray, Lin, Aliev, Roth, and Wikswo, J. Cardiovasc. Electrophysiol. 12(6): 716-722, 2001.
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Filaments in Three Dimensions
• Filaments are the 3-D analogue of the 2-D phase singularity
bz_scroll_ring_surface.avi bz_scroll_ring_filament_plus_wavefront.avi
Mark Bray
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3-D Filaments
Because curl is a three-dimensional vector operator, this convolution approach can can be extended readily to 3-D in order to visualize scroll wave filaments
Mark Bray
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String Dynamics • Strings with positive line tension
shrink (Paniflov, Rudenko and Krinsky, Biophysics, 31: 926 (1986))
bz_scroll_ring_(filament).avi
bz_scroll_wave_stable_surface_fps60.avi bz_scroll_wave_stable_filament_plus_wavefront_fps60.avi bz_scroll_wave_stable_filament_fps60.avi
Mark Bray
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String Dynamics • Strings with negative
line tension grow and buckle (see V.N. Biktashev, A.V. Holden, and H. Zhang. Phil. Trans. Royal Soc. London, Series A 347: 611-630, 1994)
• If they touch a surface, a pair of singularities is produced
• Topological charge is conserved
Movie Courtesy of Flavio Fenton
T8.avi
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A Little Negative Line Tension
fhnplus_scroll_ring_k8_4panel.avi Mark Bray
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A Lot of Negative Line Tension
fhnplus_scroll_ring_k40_filament_plus_wavefront.avi fhnplus_scroll_ring_k40_filament.avi Mark Bray
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Outline • The heart is a … • Cardiac fibrillation • Spiral waves in the heart
– Two dimensions – Spiral waves – Three dimensions – Scroll waves
• Phase plane analysis • Singularity identification
– Simple reentry – Fibrillation
• Singularity interactions – Attraction vs repulsion versus
oscillation – Annihilation – Creation
• What is needed? – Interaction potential – String creation operator Courtesy of Mark Bray
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Quatrefoil Reentry
• Follows repeated stimuli applied at a single site
• Has been used to demonstrate the importance of unequal bidomain anisotropies in cardiac electrodynamics
• Provides a reproducible, controlled system for study of the interactions of phase singularities and their accompanying filaments
Cathode break
Anode break
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Quatrefoil Reentry Th
eory
E
xper
imen
t
Voltage Singularities(t) Phase Singularities(x,y)
MA Bray, SF Lin, RR Aliev, BJ Roth, and JP Wikswo, J.P., "Experimental and theoretical analysis of phase singularity dynamics in cardiac tissue.," J Cardiovasc Electrophys, vol. 12, no. 6, pp. 716-722, 2001.
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Quatrefoil Reentry • We replicate the experimentally observed
quatrefoil reentry configuration using a simulated pair of adjacent circular filaments (scroll rings) oriented along their symmetry axes with varying initial radii and separation distances Filament
Wavefront Mark Bray
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Reaction-Diffusion System • We use a two-variable model of the Belousov-Zhabotinsky (BZ)
reaction using the Field-Koros-Noyes formulation
where v is the bromous acid concentration, w is the relative ferroin concentration, and δ = Dw/Dv (δ = 1 in this case)
• For δ = 1,
• With this BZ formulation, a single ring shrinks with a relative absence of translational drift; permits us to observe interaction without large single ring dynamics
µα βτ ε µ
α δτ
− = − − + + ∇ − +
= − + ∇−
2
2
1 (1 ) 21
1
dv w vv v q vd w vdw wx wd w
2( ) = -2d R Ddt
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Methodology • Modeled 3-D system using an
axisymmetric cylindrical coordinate system (z,ρ,θ ), such that all results are independent of angle θ → Need only to examine 2-D (z,ρ) plane
• Started rings at initial separation (Z0) and initial radius (R0) and examined life-time (TL) and motion in (z,ρ ) plane
• Simulated cathode and anode break with appropriate initial conditions
R0
Z0
ρ
z
Mark Bray
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Initial Conditions
Cathode break
Anode break
Experimental Numerical Numerical – Wave Fronts
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BZ: Anode break BZ: Cathode break
Ro
Zo
Ro
Zo
Simulated Singularity Interactions • Start with a pair of vortex
rings of fixed diameter and positive line tension
• Measure decay time as a function of separation and initial size
Mark Bray
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Cathodal Break
5: Free decay and self-annihilation per Paniflov, Rudenko and Krinsky, Biophysics, 31: 926 (1986)
4: Repulsion per Elphick and Meron, Physica D, 53: 385 (1991)
1: Enhanced decay, attraction, and mutual annihilation per Elphick and Meron, Physica D, 53: 385 (1991)
Ro
Zo
M Bray and J. Wikswo, in preparation Self-annihilation by shrinkage
Mut
ual a
nnih
ilatio
n by
col
lisio
n
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Cathode break movie
ρ
z t =195
t =2025
t =1410 t =990
t =600
R0 = 128, Z0 = 52
t =225
t =3840 t =1800
t =1410
t =600
R0 = 128, Z0 = 60
Filament annihilation by collision Self-annihilation by shrinkage
t =990
t =1800
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Cathodal Break Trajectories
Mark Bray
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Anodal Break
4: Free decay and self-annihilation Paniflov, Rudenko and Krinsky, Biophysics, 31: 926 (1986)
1: Enhanced decay, attraction, and mutual annihilation per per Elphick and Meron, Physica D, 53: 385 (1991)
2: Extended lifetime 3: Repulsion per per Elphick
and Meron, Physica D, 53: 385 (1991)
Ro
Zo
Mark Bray
Mut
ual a
nnih
ilatio
n by
col
lisio
n
Self-annihilation by shrinkagec
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Anode break movie
t = 105 t = 5810
t = 6920
t = 11390 t =1635 t =1515
t =1320 t =930
t =735 t =105
ρ
z
R0 = 128, Z0 = 60 R0 = 128, Z0 = 52
t = 9160
t = 8040
Filament annihilation by collision Delayed self-annihilation by shrinkage
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Anodal Break Trajectories
Mark Bray
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Initial Velocity = Force
Mark Bray
Attr
activ
e
R
epul
sive
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Outline • The heart is a … • Cardiac fibrillation • Spiral waves in the heart
– Two dimensions – Spiral waves – Three dimensions – Scroll waves
• Phase plane analysis • Singularity identification
– Simple reentry – Fibrillation
• Singularity interactions – Attraction vs repulsion versus
oscillation – Annihilation – Creation
• What is needed? – Interaction potential – String creation operator Courtesy of Jim Weiss
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String Creation and Annihilation:
Positive Line Tension with Fiber
Rotation
Loop pinch-off Vacuum loop creation
and coupling Vacuum loop
creation/annihilation
Movies Courtesy of Flavio Fenton
F. Fenton and A. Karma Chaos 8 (1):20-47, 1998
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70 Jim Weiss, The Wedge, Newport Beach, CA
1.6 1.8 2 2.2 2.4 2.6 2.8 3
Pos
ition
Block Reentry
Time [s]
Wavebreak = Vacuum Creation
• Wave break occurs when the leading edge of a wave runs into the tail of a preceding wave
• Wavebreaks create filaments which create reentrant activation
Nor
mal
P
ropa
gatio
n
Courtesy of Nathalie Virag,
Medtronic
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Future Questions • For both cases, what parameters determine
attractive versus repulsive behavior? Parameter gradients?
• Can a kinematic relationship be derived for the scroll ring interactions? – Is the effective mass constant or not, since it is a
dissipative system? – Can the ring interaction be described by a point-to-
point potential, and if so, are there obvious centers of action?
• In a field model, how do you introduce string creation from the vacuum?
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Acknowledgements
• Rubin Aliev • Mark Bray • Elizabeth Cherry • Deborah Echt • Flavio Fenton • Rick Gray • Peter Hunter • Alain Karma • Mark Lin • Neils Otani • Arkardy Pertsov • Nathalie Virag • Jim Weiss • And many others
textured-heart-spin.mpg
Courtesy of Peter Hunter, Auckland fhnplus_scroll_wave_break_4panel.avi
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The End
fhnplus_scroll_wave_break_4panel.avi