Volume 105, Issue 6, Pages (September 2013)

Slides:



Advertisements
Similar presentations
Volume 102, Issue 7, Pages (April 2012)
Advertisements

Volume 105, Issue 4, Pages (August 2013)
Daichi Okuno, Masayoshi Nishiyama, Hiroyuki Noji  Biophysical Journal 
Cholesterol Monohydrate Nucleation in Ultrathin Films on Water
Volume 111, Issue 7, Pages (October 2016)
Volume 93, Issue 7, Pages (October 2007)
Effects of Geometric Parameters on Swimming of Micro Organisms with Single Helical Flagellum in Circular Channels  Alperen Acemoglu, Serhat Yesilyurt 
Volume 105, Issue 3, Pages (August 2013)
Indrajeet Singh, Efrosyni Themistou, Lionel Porcar, Sriram Neelamegham 
Precision and Variability in Bacterial Temperature Sensing
Volume 105, Issue 9, Pages (November 2013)
Ultrafast Photoconversion of the Green Fluorescent Protein Studied by Accumulative Femtosecond Spectroscopy  Florian Langhojer, Frank Dimler, Gregor Jung,
Volume 80, Issue 3, Pages (March 2001)
Volume 2, Issue 5, Pages (May 2017)
Structural Basis for Vertebrate Filamin Dimerization
Volume 113, Issue 12, Pages (December 2017)
Ariel Lubelski, Joseph Klafter  Biophysical Journal 
The N-Terminal Actin-Binding Tandem Calponin-Homology (CH) Domain of Dystrophin Is in a Closed Conformation in Solution and When Bound to F-actin  Surinder M.
Carlos R. Baiz, Andrei Tokmakoff  Biophysical Journal 
MunJu Kim, Katarzyna A. Rejniak  Biophysical Journal 
Marc Jendrny, Thijs J. Aartsma, Jürgen Köhler  Biophysical Journal 
Tamara C. Bidone, Haosu Tang, Dimitrios Vavylonis  Biophysical Journal 
Mechanochemical Symmetry Breaking in Hydra Aggregates
Chirality-Based Signatures of Local Protein Environments in Two-Dimensional Optical Spectroscopy of Two Species Photosynthetic Complexes of Green Sulfur.
Theoretical and Computational Investigation of Flagellin Translocation and Bacterial Flagellum Growth  David E. Tanner, Wen Ma, Zhongzhou Chen, Klaus.
Jérôme Lang, Amandine Maréchal, Manon Couture, Jérôme Santolini 
Christopher B. Stanley, Tatiana Perevozchikova, Valerie Berthelier 
Julia Adolphs, Thomas Renger  Biophysical Journal 
Cecily P. Vaughn, Kojo S.J. Elenitoba-Johnson 
Volume 83, Issue 3, Pages (September 2002)
Cholesterol Depletion Mimics the Effect of Cytoskeletal Destabilization on Membrane Dynamics of the Serotonin1A Receptor: A zFCS Study  Sourav Ganguly,
Shiori Toba, Hiroyuki Iwamoto, Shinji Kamimura, Kazuhiro Oiwa 
Volume 113, Issue 6, Pages (September 2017)
Volume 99, Issue 8, Pages (October 2010)
Carlos R. Baiz, Andrei Tokmakoff  Biophysical Journal 
Ivan V. Polozov, Klaus Gawrisch  Biophysical Journal 
Dmitry A. Fedosov, Bruce Caswell, George Em Karniadakis 
Histone Octamer Helical Tubes Suggest that an Internucleosomal Four-Helix Bundle Stabilizes the Chromatin Fiber  Timothy D. Frouws, Hugh-G. Patterton,
Structural Basis for Vertebrate Filamin Dimerization
Volume 104, Issue 1, Pages (January 2013)
Volume 113, Issue 6, Pages (September 2017)
Exciton Theory for Supramolecular Chlorosomal Aggregates: 1
Cholesterol Monohydrate Nucleation in Ultrathin Films on Water
Molecular View of Hexagonal Phase Formation in Phospholipid Membranes
Anna M. Popova, Peter Z. Qin  Biophysical Journal 
Mechanical Control of Bacterial Cell Shape
Chang-Chun Lee, Yen Sun, Huey W. Huang  Biophysical Journal 
The Effect of Dye-Dye Interactions on the Spatial Resolution of Single-Molecule FRET Measurements in Nucleic Acids  Nicolas Di Fiori, Amit Meller  Biophysical.
Volume 111, Issue 1, Pages (July 2016)
Volume 96, Issue 8, Pages (April 2009)
Volume 83, Issue 3, Pages (September 2002)
Steven S. Andrews, Adam P. Arkin  Biophysical Journal 
Siyuan Wang, Ned S. Wingreen  Biophysical Journal 
Mechanics of Individual Keratin Bundles in Living Cells
Volume 102, Issue 12, Pages (June 2012)
Volume 93, Issue 10, Pages (November 2007)
Volume 105, Issue 9, Pages (November 2013)
Volume 75, Issue 3, Pages (September 1998)
Mikyung Han, Yuan Mei, Htet Khant, Steven J. Ludtke 
Volume 74, Issue 4, Pages (April 1998)
Modeling of Mitochondrial Donut Formation
Volume 113, Issue 10, Pages (November 2017)
Dependence of Protein Folding Stability and Dynamics on the Density and Composition of Macromolecular Crowders  Jeetain Mittal, Robert B. Best  Biophysical.
The N-Terminal Actin-Binding Tandem Calponin-Homology (CH) Domain of Dystrophin Is in a Closed Conformation in Solution and When Bound to F-actin  Surinder M.
A New Angle on Microscopic Suspension Feeders near Boundaries
Ping-Jung Su, Wei-Liang Chen, Yang-Fang Chen, Chen-Yuan Dong 
Volume 114, Issue 6, Pages (March 2018)
Ai Kia Yip, Pei Huang, Keng-Hwee Chiam  Biophysical Journal 
Cotranslational Folding Increases GFP Folding Yield
Evidence of Cholesterol Accumulated in High Curvature Regions: Implication to the Curvature Elastic Energy for Lipid Mixtures  Wangchen Wang, Lin Yang,
Presentation transcript:

Volume 105, Issue 6, Pages 1346-1356 (September 2013) Temperature and Carbon Assimilation Regulate the Chlorosome Biogenesis in Green Sulfur Bacteria  Joseph Kuo-Hsiang Tang, Semion K. Saikin, Sai Venkatesh Pingali, Miriam M. Enriquez, Joonsuk Huh, Harry A. Frank, Volker S. Urban, Alán Aspuru-Guzik  Biophysical Journal  Volume 105, Issue 6, Pages 1346-1356 (September 2013) DOI: 10.1016/j.bpj.2013.07.027 Copyright © 2013 Biophysical Society Terms and Conditions

Figure 1 (A) High-performance liquid chromatography chromatogram of BChl c homologs in the chlorosome from Cultures 1, 3, 4, 6, 7, and 9 with detection wavelength at 640 nm and the elution pattern of each BChl c homolog. (B) Percentage of BChl c homologs in the chlorosome determined by mass peak area. Biophysical Journal 2013 105, 1346-1356DOI: (10.1016/j.bpj.2013.07.027) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 2 (A) SANS profiles of the chlorosome isolated from constant temperature cultures at 50°C (Culture 1 and Culture 3), temperature down-shifted to 30°C cultures (Culture 4 and Culture 6), and constant temperature cultures at 30°C (Culture 7 and Culture 9). SANS data fitted with modified (B) Guinier’s model and (C) biaxial ellipsoid of rotation. Biophysical Journal 2013 105, 1346-1356DOI: (10.1016/j.bpj.2013.07.027) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 3 (A) UV-visible spectra of temperature down-shifted cultures grown on acetate/HCO3− (Culture 4) and pyruvate/HCO3− (Culture 6), (B) the chlorosome from Culture 4 and Culture 6, and (C) the chlorosome from Culture 6 and C. aurantiacus. Biophysical Journal 2013 105, 1346-1356DOI: (10.1016/j.bpj.2013.07.027) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 4 CD spectra of the chlorosome. (A) CD spectra of the chlorosome from Culture 4 and the chlorosome from Culture 6, and (B) the chlorosome from Culture 6 and the chlorosome from C. aurantiacus. The chlorosome with an OD of 1.0 for the BChl c Qy transition was used for the measurements. Biophysical Journal 2013 105, 1346-1356DOI: (10.1016/j.bpj.2013.07.027) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 5 77-K fluorescence spectra of (A) the chlorosome from Culture 4 and Culture 6 (A) and (B) the whole cells from the same cultures. Spectra were normalized at the maxima of the chlorosome. Biophysical Journal 2013 105, 1346-1356DOI: (10.1016/j.bpj.2013.07.027) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 6 Schematic illustration of BChl packing in the chlorosome. The chlorosome is considered as an ellipsoidal body with semi-axes L1−3. Two-dimensional aggregates of BChls are packed in a form of concentric rolls and curved lamellae. Biophysical Journal 2013 105, 1346-1356DOI: (10.1016/j.bpj.2013.07.027) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 7 Model of BChl aggregation. (A) BChl pigments form two-dimensional lattice (35) with the lattice parameters a=6.25 Å, b=9.79 Å, θ=122°, and α=35°. Binding of BChls is schematically illustrated. Arrows show the orientation of molecular Qy transition dipoles. (B) and (C) represent two suggested ways for aggregate folding in rolls. (B) Structure I suggested for a mutant chlorosome with BChl stacks forming concentric rings (41). (C) Structure II proposed for a wild-type of bacteria (41), in which BChl stacks are parallel to the roll symmetry axis of the roll. Biophysical Journal 2013 105, 1346-1356DOI: (10.1016/j.bpj.2013.07.027) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 8 Structure II: Length/radius dependence of CD spectra. (A) The characteristic length of a roll that corresponds to the transition between the mixed (–/+/–) and Type II (–/+) CD spectra is shown as a function of a roll radius. (B) Two types of CD spectra are shown for rolls of the radius R=7 nm and the lengths L=100 nm and L=60 nm marked by black and grey stars in (A). The relative intensities are normalized to the number of molecules. The wavenumber scale shows the frequency red shift from the monomer transition due to BChl aggregation. Biophysical Journal 2013 105, 1346-1356DOI: (10.1016/j.bpj.2013.07.027) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 9 Structure I: Length dependence of CD spectra. Two types of CD spectra are shown for rolls of the radius R=7 nm and the lengths L=100 nm and L=20 nm. The transition between the mixed-type and Type I spectra occurs independently of the roll radius at about L=20 nm. Biophysical Journal 2013 105, 1346-1356DOI: (10.1016/j.bpj.2013.07.027) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 10 CD spectra: Roll to lamella transition. CD spectra of single rolls (radius R = 7 nm and length is L = 100 nm) as compared with the spectra of curved lamellae of the same curvature radius and length. The curved lamellae are represented by halves of the rolls cut along the symmetry axis. The relative intensities are normalized to the number of molecules. (A) Structure I shows transition between the mixed-type and Type II spectra. (B) Structure II shows transition between the mixed-type and Type II spectra. Biophysical Journal 2013 105, 1346-1356DOI: (10.1016/j.bpj.2013.07.027) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 11 Computed Qy transition frequencies of BChl homologs. The transition frequencies are computed using time-dependent density functional theory. The following homologs are shown: m/z = 793.5 (8-ethyl, 12-methyl), m/z = 807.5 (8-ethyl, 12-ethyl), m/z = 823.5 (8-propyl, 12-ethyl), m/z = 839.5 (8-isobutyl, 12-ethyl), and m/z = 853.5 (8-neopentyl, 12- ethyl). Biophysical Journal 2013 105, 1346-1356DOI: (10.1016/j.bpj.2013.07.027) Copyright © 2013 Biophysical Society Terms and Conditions