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![image of Translation of Near-Infrared Fluorescence Imaging Technologies: Emerging Clinical Applications: Supplemental Video 3 image of Translation of Near-Infrared Fluorescence Imaging Technologies: Emerging Clinical Applications: Supplemental Video 3](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.31.131/sevick3.jpg)
Translation of Near-Infrared Fluorescence Imaging Technologies: Emerging Clinical Applications: Supplemental Video 3
A supplemental video from the 2012 review by E.M. Sevick-Muraca "Translation of Near-Infrared Fluorescence Imaging Technologies: Emerging Clinical Applications" from the Annual Review of Medicine.
Investigational NIRF images of the lymphatics in the anteriolateral territory of the right upper arm and left hand in a 67-year-old male with grade I lymphedema presenting approximately six months after carpal tunnel syndrome surgery. Imaging was performed 11 months after onset of symptoms. Lymphatics are contrasted by IGC and show active lymphatic propulsion to the axilla. Analysis of the video demonstrates that the tortuous lymphatic vasculature drains from the edematous regions of the anterior upper arm into the medial lymph bundle. Because the lymphatics cannot be conventionally imaged with the temporal and spatial resolution shown herein it is not known whether tortuous lymphatic vessels are the result or the cause of edema.
![image of A Conversation with P. Roy Vagelos image of A Conversation with P. Roy Vagelos](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.17.75/royvagelos.jpg)
A Conversation with P. Roy Vagelos
![image of Pathogenesis of NUT Midline Carcinoma: Supplemental Video 1 image of Pathogenesis of NUT Midline Carcinoma: Supplemental Video 1](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.28.112/french.jpg)
Pathogenesis of NUT Midline Carcinoma: Supplemental Video 1
A supplemental video from the 2012 review by Christopher A. French "Pathogenesis of NUT Midline Carcinoma" from the Annual Review of Pathology: Mechanisms of Disease.
![image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 1 image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 1](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.17.79/kiger1.jpg)
Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 1
A supplemental video from the 2012 review by Kenneth T. Kiger and James H. Duncan "Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves" from the Annual Review of Fluid Mechanics.
Video corresponds to Figure 5a2 in the review.
![image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 2 image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 2](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.17.80/images_kiger2.jpg)
Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 2
A supplemental video from the 2012 review by Kenneth T. Kiger and James H. Duncan "Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves" from the Annual Review of Fluid Mechanics.
Video corresponds to Figure 5b2 in the review.
![image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 3 image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 3](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.17.81/images_kiger3.jpg)
Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 3
A supplemental video from the 2012 review by Kenneth T. Kiger and James H. Duncan "Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves" from the Annual Review of Fluid Mechanics.
Video corresponds to Figure 5c in the review.
![image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 4 image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 4](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.17.82/kiger5.jpg)
Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 4
A supplemental video from the 2012 review by Kenneth T. Kiger and James H. Duncan "Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves" from the Annual Review of Fluid Mechanics.
Video corresponds to Figure 5d in the review.
![image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 5 image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 5](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.17.83/kiger5.jpg)
Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 5
A supplemental video from the 2012 review by Kenneth T. Kiger and James H. Duncan "Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves" from the Annual Review of Fluid Mechanics.
Video corresponds to Figure 5e in the review.
![image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 6 image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 6](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.17.84/kiger6.jpg)
Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 6
A supplemental video from the 2012 review by Kenneth T. Kiger and James H. Duncan "Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves" from the Annual Review of Fluid Mechanics.
Video corresponds to Figure 5f in the review.
![image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 7 image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 7](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.17.85/kiger7.jpg)
Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 7
A supplemental video from the 2012 review by Kenneth T. Kiger and James H. Duncan "Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves" from the Annual Review of Fluid Mechanics.
Video corresponds to Figure 5g in the review.
![image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 8 image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 8](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.17.86/kiger8.jpg)
Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 8
A supplemental video from the 2012 review by Kenneth T. Kiger and James H. Duncan "Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves" from the Annual Review of Fluid Mechanics.
Video corresponds to Figure 5h in the review.
![image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 9 image of Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 9](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.17.87/kiger9.jpg)
Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves: Supplemental Video 9
A supplemental video from the 2012 review by Kenneth T. Kiger and James H. Duncan "Air-Entrainment Mechanisms in Plunging Jets and Breaking Waves" from the Annual Review of Fluid Mechanics.
Video corresponds to Figure 11 in the review.
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1a image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1a](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.28.113/magnaudet1a.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1a
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental Videos 1a b c and d show a sequence of the first four unsteady bifurcated states in the wake of a short cylinder of aspect ratio χ = 3 held fixed at normal incidence in a uniform stream. From a DNS by Auguste et al. (2010). Supplemental Video 1a: Reflectional symmetry preserving (RSP) state for Re = 182.
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1b image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1b](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.28.114/magnaudet1b.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1b
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental Videos 1a b c and d show a sequence of the first four unsteady bifurcated states in the wake of a short cylinder of aspect ratio χ = 3 held fixed at normal incidence in a uniform stream. From a DNS by Auguste et al. (2010). Supplemental Video 1b: Knit-knot state with two frequencies and no reflectional symmetry for Re = 187.
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1c image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1c](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.28.115/magnaudet1c.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1c
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental videos 1a b c and d show a sequence of the first four unsteady bifurcated states in the wake of a short cylinder of aspect ratio χ = 3 held fixed at normal incidence in a uniform stream. From a DNS by Auguste et al. (2010). Supplemental Video 1c: Reflectional symmetry breaking (or ying-yang) state for Re = 195. Note that the slow pulsation observed in the previous state is not present any more.
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1d image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1d](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.28.116/magnaudet1d.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 1d
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental videos 1a b c and d show a sequence of the first four unsteady bifurcated states in the wake of a short cylinder of aspect ratio χ = 3 held fixed at normal incidence in a uniform stream. From a DNS by Auguste et al. (2010). Supplemental Video 1d: Standing wave (or zigzag) state for Re = 216. Note that the symmetry plane is orthogonal to that of the RSP state.
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 2a image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 2a](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.29.117/magnaudet2a.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 2a
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
An approximately oblate spheroidal air bubble with χ ≈ 2.0 and Re ≈ 760 rising in water (the sphere of same volume would have a diameter of 2.5 mm). The path is close to a planar zigzag. From experiments by Riboux et al. (2010).
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 2b image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 2b](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.29.118/magnaudet2b.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 2b
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Path and wake (illustrated with streamwise vorticity isosurfaces) of an oblate spheroidal bubble with χ = 2.5 and Ar = 138. Note the two transitions first from a straight vertical path to a planar zigzag and much later from this zigzag to a helical path and the associated changes in the wake structure. From a DNS by Mougin & Magnaudet (2002b).
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 3a image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 3a](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.29.119/magnaudet3a.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 3a
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental Videos 3a b and c are of two perpendicular views of the wake past a zigzagging short cylinder (χ = 2 Ar = 90 Re ≈ 250). Supplemental Video 3a: Dye visualizations (Fernandes et al. 2005).
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 3b image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 3b](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.29.120/magnaudet3b.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 3b
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental Video 3a b and c are of two perpendicular views of the wake past a zigzagging short cylinder (χ = 2 Ar = 90 Re ≈ 250). Supplemental Video 3b: Isosurface of the λ2 criterion (Jeong & Hussain 1995) extracted from a DNS by Auguste (2010).
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 3c image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 3c](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.29.121/magnaudet3c.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 3c
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental Video 3a b and c are of two perpendicular views of the wake past a zigzagging short cylinder (χ = 2 Ar = 90 Re ≈ 250). Supplemental Video 3c: Isosurface of the λ2 criterion (Jeong & Hussain 1995) extracted from a DNS by Auguste (2010).
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 4a image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 4a](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.29.122/magnaudet4a.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 4a
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental Videos 4a and b show planar zigzag paths of short cylinders corresponding to Ar = 90 i.e. Re ≈ 250 (from Fernandes et al. 2005). The red line (Nx) indicates the horizontal projection of a unit vector parallel to the body symmetry axis. The black (Vz') and blue (Vx') lines display the evolution of the fluctuating velocity components along the vertical and horizontal directions respectively. For Supplemental Video 4a χ = 2. Positions of the body center of volume (left panel) are in mm; fluctuating velocities (right panel) are in mm s-1. Note that Nx and Vx' are almost in phase for χ = 2 whereas they are more than 90° out of phase for χ = 10.
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 4b image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 4b](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.30.123/magnaudet4b.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 4b
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental Videos 4a and b show planar zigzag paths of short cylinders corresponding to Ar = 90 i.e. Re ≈ 250 (from Fernandes et al. 2005). The red line (Nx) indicates the horizontal projection of a unit vector parallel to the body symmetry axis. The black (Vz') and blue (Vx') lines display the evolution of the fluctuating velocity components along the vertical and horizontal directions respectively. In Supplemental Video 4b χ = 10. Positions of the body center of volume (left panel) are in mm; fluctuating velocities (right panel) are in mm s-1. Note that Nx and Vx' are almost in phase for χ = 2 whereas they are more than 90° out of phase for χ = 10.
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 5a image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 5a](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.30.124/magnaudet5a.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 5a
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental Videos 5a and b show two perpendicular views of the wake past a short cylinder with χ = 10 and Ar = 80 rising in zigzag [from a DNS by Auguste (2010)]. The wake is visualized with an isosurface of the λ2 criterion (Jeong & Hussain 1995) the color reflecting the sign and magnitude of the streamwise vorticity.
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 5b image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 5b](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.30.125/magnaudet5b.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 5b
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental Videos 5a and b show two perpendicular views of the wake past a short cylinder with χ = 10 and Ar = 80 rising in zigzag [from a DNS by Auguste (2010)]. The wake is visualized with an isosurface of the λ2 criterion (Jeong & Hussain 1995) the color reflecting the sign and magnitude of the streamwise vorticity.
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 6a image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 6a](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.30.126/magnaudet6a.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 6a
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental Videos 6a and b show an infinitely thin disk with I* = 0.06 undergoing (a) a highly nonlinear fluttering motion for Ar = 83 and (b) a tumbling motion for Ar = 156 [from a DNS by Auguste (2010)]. The wake is visualized with an isosurface of the λ2 criterion (Jeong & Hussain 1995) the color reflecting the sign and magnitude of the streamwise vorticity.
![image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 6b image of Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 6b](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.30.127/magnaudet6b.jpg)
Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids: Supplemental Video 6b
A supplemental video from the 2012 review by Patricia Ern Frédéric Risso David Fabre and Jacques Magnaudet "Wake-Induced Oscillatory Paths of Bodies Freely Rising or Falling in Fluids" from the Annual Review of Fluid Mechanics.
Supplemental Videos 6a and b show an infinitely thin disk with I* = 0.06 undergoing (a) a highly nonlinear fluttering motion for Ar = 83 and (b) a tumbling motion for Ar = 156 [from a DNS by Auguste (2010)]. The wake is visualized with an isosurface of the λ2 criterion (Jeong & Hussain 1995) the color reflecting the sign and magnitude of the streamwise vorticity.
![image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 1 image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 1](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.24.104/chang1.jpg)
Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 1
A supplemental video from the 2012 review by Hsueh-Chia Chang Gilad Yossifon and Evgeny A. Demekhin "Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux" from the Annual Review of Fluid Mechanics.
Movie showing the ion-enrichment (cathodic polarity) ion-depletion (anodic polarity) phenomena at different frequencies (0.01 0.1 and 1 Hz) and the same voltage difference of 80 V peak to peak for the nanoslot device of Figure 6.
![image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 2 image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 2](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.24.105/chang2.jpg)
Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 2
A supplemental video from the 2012 review by Hsueh-Chia Chang Gilad Yossifon and Evgeny A. Demekhin "Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux" from the Annual Review of Fluid Mechanics.
Movie showing the depletion-layer pattern evolution as a response to a step input of 40 V. In particular we clearly see the complex process of wavelength selection by small vortices breaking up through fusion and transformation into still larger vortices until a quasi-steady like pattern is formed in the case of the deep (122-µm) microchamber.
![image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 3 image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 3](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.25.106/chang3.jpg)
Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 3
A supplemental video from the 2012 review by Hsueh-Chia Chang Gilad Yossifon and Evgeny A. Demekhin "Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux" from the Annual Review of Fluid Mechanics.
In contrast to the case of the deep (122-µm) microchamber these patterns do not occur for the shallow (2-µm) microchamber. Instead a relatively uniform propagating concentration polarization layer front is observed.
![image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 4 image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 4](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.28.107/chang4.jpg)
Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 4
A supplemental video from the 2012 review by Hsueh-Chia Chang Gilad Yossifon and Evgeny A. Demekhin "Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux" from the Annual Review of Fluid Mechanics.
Movie showing the depletion layer and its associated vortex dependence (using 1.2-µm fluorescent microbeads) on the voltage for the widest (2.5-mm) nanoslot.
![image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 5 image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 5](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.28.108/chang5.jpg)
Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 5
A supplemental video from the 2012 review by Hsueh-Chia Chang Gilad Yossifon and Evgeny A. Demekhin "Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux" from the Annual Review of Fluid Mechanics.
Movie showing the depletion layer and its associated vortex dependence (using 1.2-µm fluorescent microbeads) on the voltage for the narrowest (50-µm) nanoslot.
![image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 7 image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 7](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.28.110/images_chang7.jpg)
Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 7
A supplemental video from the 2012 review by Hsueh-Chia Chang Gilad Yossifon and Evgeny A. Demekhin "Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux" from the Annual Review of Fluid Mechanics.
Movie showing the evolution of the depletion-enrichment phenomenon under reverse 40-V DC bias for a single nanochannel.
![image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 6 image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 6](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.28.109/chang6.jpg)
Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 6
A supplemental video from the 2012 review by Hsueh-Chia Chang Gilad Yossifon and Evgeny A. Demekhin "Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux" from the Annual Review of Fluid Mechanics.
Movie showing the evolution of the depletion-enrichment phenomenon under forward and reverse 30-V DC bias for a nanochannel array (consisting of seven channels) with asymmetric channel separation at the entrances.
![image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 8 image of Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 8](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.28.111/chang8.jpg)
Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux: Supplemental Video 8
A supplemental video from the 2012 review by Hsueh-Chia Chang Gilad Yossifon and Evgeny A. Demekhin "Nanoscale Electrokinetics and Microvortices: How Microhydrodynamics Affects Nanofluidic Ion Flux" from the Annual Review of Fluid Mechanics.
Movie showing the colloid dynamics for different applied voltages in the case of weak electrolyte (0.1 mM) and 1.2-µm beads without fluorescent dye molecules in the background electrolyte solution.
![image of Liquid Rope Coiling: Supplemental Video 1 image of Liquid Rope Coiling: Supplemental Video 1](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.17.78/ribe1.jpg)
Liquid Rope Coiling: Supplemental Video 1
A supplemental video from the 2012 review by Neil M. Ribe Mehdi Habibi and Daniel Bonn "Liquid Rope Coiling" from the Annual Review of Fluid Mechanics.
Each frame is 1 cm wide and the playback rate is 1/20 real time.
![image of A Conversation with Olle Björkman image of A Conversation with Olle Björkman](/docserver/fulltext//multimedia/10.1146/do.multimedia.2012.12.06.46/ollebjorkman.jpg)
A Conversation with Olle Björkman
The Annual Review of Plant Biology presents a conversation with Dr.Olle Björkman. In this interview Dr. Björkman talks about his research and career in plant biology.
![image of A Conversation with Haldor Topsøe image of A Conversation with Haldor Topsøe](/docserver/fulltext//multimedia/10.1146/do.multimedia.2012.12.20.51/haldortopsoe.jpg)
A Conversation with Haldor Topsøe
The Annual Review of Chemical and Biomolecular Engineering presents a conversation with Dr. Haldor Topsøe chairman of Haldor Topsøe. In this interview Dr. Topsøe talks about his career in industry as well as his corporation's work with academic scientists.
![image of A Conversation with Robert M. Solow image of A Conversation with Robert M. Solow](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.16.68/robertsolow.jpg)
A Conversation with Robert M. Solow
Dr. Robert Solow Professor Emeritus of Economics at the Massachusetts Institute of Technology talks about his life and career with Dr. Peter Berck SJ Hall Professor of Agricultural and Resource Economics and Policy at the University of California at Berkeley. In this conversation Dr. Solow discusses growing up in an immigrant family in 1930s Brooklyn being introduced to literature and ideas at James Madison High School attending Harvard University on scholarship and receiving the 1987 Nobel Prize in Economics Laureate.
![image of In Vitro Models of Traumatic Brain Injury: Supplemental Video 1 image of In Vitro Models of Traumatic Brain Injury: Supplemental Video 1](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.02.01.137/morrison1.jpg)
In Vitro Models of Traumatic Brain Injury: Supplemental Video 1
A supplemental video from the 2011 review by Barclay Morrison III Benjamin S. Elkin Jean-Pierre Dollé and Martin L. Yarmush "In Vitro Models of Traumatic Brain Injury" from the Annual Review of Biomedical Engineering.
Equibiaxial stretch of cultures is achieved through deformation of the culture substrate by pulling the clamped membrane over a hollow cylinder. This video shows the dynamic deformation of a culture being injured with this model.
![image of In Vitro Models of Traumatic Brain Injury: Supplemental Video 2 image of In Vitro Models of Traumatic Brain Injury: Supplemental Video 2](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.02.01.138/morrison2.jpg)
In Vitro Models of Traumatic Brain Injury: Supplemental Video 2
A supplemental video from the 2011 review by Barclay Morrison III Benjamin S. Elkin Jean-Pierre Dollé and Martin L. Yarmush "In Vitro Models of Traumatic Brain Injury" from the Annual Review of Biomedical Engineering.
Propagation of evoked activity through the neural circuitry.
![image of A Conversation with Karl K. Turekian image of A Conversation with Karl K. Turekian](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.02.13.143/turekian_video_still.jpg)
A Conversation with Karl K. Turekian
The Annual Review of Marine Science presents an interview with Dr. Karl K. Turekian Sterling Professor of Geology and Geophysics at Yale University in conversation with Dr. Kirk Cochran Professor of Marine Science at Stony Brook University.
![image of An Interview with Jeremy Thorner image of An Interview with Jeremy Thorner](/docserver/fulltext/images_thumb_audio.png)
An Interview with Jeremy Thorner
![image of The Structure of the Nuclear Pore Complex: Supplemental Video 1 image of The Structure of the Nuclear Pore Complex: Supplemental Video 1](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.31.133/hoelz1.jpg)
The Structure of the Nuclear Pore Complex: Supplemental Video 1
A supplemental video from the 2011 review by André Hoelz Erik W. Debler and Günter Blobel "The Structure of the Nuclear Pore Complex" from the Annual Review of Biochemistry.
Overall the nuclear pore complex (NPC) consists of a cylindrical symmetric core which is asymmetrically decorated with filaments and a nuclear basket structure on the cytoplasmic and nucleoplasmic sides respectively. Molecules smaller than ∼40 kDa (small spheres) freely diffuse through the NPC whereas larger noncargo molecules (large spheres) are prevented from crossing the nuclear envelope. Artwork by Joseph Alexander Erik W. Debler and André Hoelz.
![image of The Structure of the Nuclear Pore Complex: Supplemental Video 2 image of The Structure of the Nuclear Pore Complex: Supplemental Video 2](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.31.134/hoelz2.jpg)
The Structure of the Nuclear Pore Complex: Supplemental Video 2
A supplemental video from the 2011 review by André Hoelz Erik W. Debler and Günter Blobel "The Structure of the Nuclear Pore Complex" from the Annual Review of Biochemistry.
Active import and export of cargoes are facilitated by nuclear localization and nuclear export sequences (NLS and NES respectively) that are recognized by transport factors collectively termed karyopherins (Kaps). The NLS of import cargoes (blue) is recognized either directly by an import karyopherin-β (Kap-β; salmon) or via an adapter karyopherin (Kap-α; light green). RanGTP (red) binding inside the nucleus leads to dissociation of the import complex. By contrast the assembly of a NES-cargo Kap-β export complex requires RanGTP binding (represented in blue yellow and red respectively). In the cytosol this export complex is dissociated by GTP hydrolysis which is catalyzed by Ran GTPase-activating protein (RanGAP; dark green) or Ran-binding protein 1 (RanBP1). Artwork by Joseph Alexander Erik W. Debler and André Hoelz.
![image of The Structure of the Nuclear Pore Complex: Supplemental Video 3 image of The Structure of the Nuclear Pore Complex: Supplemental Video 3](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.31.135/hoelz3.jpg)
The Structure of the Nuclear Pore Complex: Supplemental Video 3
A supplemental video from the 2011 review by André Hoelz Erik W. Debler and Günter Blobel "The Structure of the Nuclear Pore Complex" from the Annual Review of Biochemistry.
The transport of large cargoes (blue) is thought to require the dilation of the central channel of the NPC. Artwork by Joseph Alexander Erik W. Debler and André Hoelz.
![image of The Structure of the Nuclear Pore Complex: Supplemental Video 4 image of The Structure of the Nuclear Pore Complex: Supplemental Video 4](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.01.31.136/hoelz4.jpg)
The Structure of the Nuclear Pore Complex: Supplemental Video 4
A supplemental video from the 2011 review by André Hoelz Erik W. Debler and Günter Blobel "The Structure of the Nuclear Pore Complex" from the Annual Review of Biochemistry.
Inner nuclear membrane (INM) proteins are cotranslationally integrated into the endoplasmic reticulum membrane which is continuous with the outer nuclear membrane and then imported to the INM. Similar to the karyopherin-mediated transport in Movie 2 the transport of INM proteins is also dependent on the Ran cycle and karyopherins that likely travel through the central channel whereas the cargo protein is anchored in the membrane. INM proteins Kap-α Kap-β and RanGTP are illustrated in light purple light green brown and red respectively. Substantial structural changes within the NPC would be necessary to facilitate this transport event. Artwork by Joseph Alexander Erik W. Debler and André Hoelz.
![image of The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates: Supplemental Video 1 image of The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates: Supplemental Video 1](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.04.15.160/orban1.jpg)
The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates: Supplemental Video 1
A supplemental video from the 2011 review by Guy A. Orban "The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates" from the Annual Review of Neuroscience. Second order speed gradient portraying a ridge.
![image of The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates: Supplemental Video 2 image of The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates: Supplemental Video 2](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.04.15.161/orban2.jpg)
The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates: Supplemental Video 2
A supplemental video from the 2011 review by Guy A. Orban "The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates" from the Annual Review of Neuroscience. Second order speed gradient portraying a saddle.
![image of The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates: Supplemental Video 3 image of The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates: Supplemental Video 3](/docserver/fulltext//multimedia/10.1146/do.multimedia.2013.04.15.162/orban3.jpg)
The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates: Supplemental Video 3
A supplemental video from the 2011 review by Guy A. Orban "The Extraction of 3D Shape in the Visual System of Human and Nonhuman Primates" from the Annual Review of Neuroscience. Rotating random lines portraying a 3D wire figure.