Volume 85, Issue 4, Pages (October 2003)

Slides:



Advertisements
Similar presentations
The Dynamics and Mechanics of Endothelial Cell Spreading Cynthia A. Reinhart-King, Micah Dembo, Daniel A. Hammer Biophysical Journal Volume 89, Issue 1,
Advertisements

Mesoscale Simulation of Blood Flow in Small Vessels Prosenjit Bagchi Biophysical Journal Volume 92, Issue 6, Pages (March 2007) DOI: /biophysj
Membrane Physical Chemistry - II
Volume 101, Issue 8, Pages (October 2011)
Thomas J. English, Daniel A. Hammer  Biophysical Journal 
Geometrical Properties of Gel and Fluid Clusters in DMPC/DSPC Bilayers: Monte Carlo Simulation Approach Using a Two-State Model  István P. Sugár, Ekaterina.
Kejing Chen, Samir K. Ballas, Roy R. Hantgan, Daniel B. Kim-Shapiro 
Ismail M. Hafez, Steven Ansell, Pieter R. Cullis  Biophysical Journal 
Volume 98, Issue 2, Pages (January 2010)
The State Diagram for Cell Adhesion Mediated by Two Receptors
High-Density 3D Single Molecular Analysis Based on Compressed Sensing
Specific Recognition of Macroscopic Objects by the Cell Surface: Evidence for a Receptor Density Threshold Revealed by Micrometric Particle Binding Characteristics 
Anan Abu Ubeid, Longmei Zhao, Ying Wang, Basil M. Hantash 
Precision and Variability in Bacterial Temperature Sensing
Kinetic Studies on Enzyme-Catalyzed Reactions: Oxidation of Glucose, Decomposition of Hydrogen Peroxide and Their Combination  Zhimin Tao, Ryan A. Raffel,
Influence of Chain Length and Unsaturation on Sphingomyelin Bilayers
Regional cell density distribution and oxygen consumption rates in porcine TMJ discs: an explant study  J. Kuo, C. Shi, S. Cisewski, L. Zhang, M.J. Kern,
The Binding Affinity of Ff Gene 5 Protein Depends on the Nearest-Neighbor Composition of the ssDNA Substrate  Tung-Chung Mou, Carla W. Gray, Donald M.
Behavior of Giant Vesicles with Anchored DNA Molecules
Volume 113, Issue 12, Pages (December 2017)
Volume 96, Issue 9, Pages (May 2009)
One-Dimensional Brownian Motion of Charged Nanoparticles along Microtubules: A Model System for Weak Binding Interactions  Itsushi Minoura, Eisaku Katayama,
Joseph M. Johnson, William J. Betz  Biophysical Journal 
Yuhong Xu, Sek-Wen Hui, Peter Frederik, Francis C. Szoka 
Thermal Mechanisms of Millimeter Wave Stimulation of Excitable Cells
Robert W. Walters, Robert R. Jenq, Stephen B. Hall  Biophysical Journal 
Rainer Kurre, Berenike Maier  Biophysical Journal 
Volume 114, Issue 4, Pages (February 2018)
Volume 101, Issue 7, Pages (October 2011)
Volume 85, Issue 4, Pages (October 2003)
Volume 92, Issue 9, Pages (May 2007)
Volume 26, Issue 8, Pages (April 2016)
Volume 74, Issue 5, Pages (May 1998)
Probing Red Blood Cell Morphology Using High-Frequency Photoacoustics
Fiber-Dependent and -Independent Toxicity of Islet Amyloid Polypeptide
Cell Optical Density and Molecular Composition Revealed by Simultaneous Multimodal Label-Free Imaging  Nicolas Pavillon, Alison J. Hobro, Nicholas I.
Yuno Lee, Philip A. Pincus, Changbong Hyeon  Biophysical Journal 
Interplay of Troponin- and Myosin-Based Pathways of Calcium Activation in Skeletal and Cardiac Muscle: The Use of W7 as an Inhibitor of Thin Filament.
Stationary Gating of GluN1/GluN2B Receptors in Intact Membrane Patches
Stefan Howorka, Hagan Bayley  Biophysical Journal 
Viscoelasticity as a Biomarker for High-Throughput Flow Cytometry
Probing Red Cell Membrane Cholesterol Movement with Cyclodextrin
Volume 101, Issue 8, Pages (October 2011)
Enhanced Tethered-Particle Motion Analysis Reveals Viscous Effects
Dmitrii V. Vavilin, Esa Tyystjärvi, Eva-Mari Aro  Biophysical Journal 
Volume 103, Issue 5, Pages (September 2012)
Blockers of VacA Provide Insights into the Structure of the Pore
Volume 84, Issue 3, Pages (March 2003)
Kinetics of Surface-Driven Self-Assembly and Fatigue-Induced Disassembly of a Virus- Based Nanocoating  Alejandro Valbuena, Mauricio G. Mateu  Biophysical.
Clustering of Cyclic-Nucleotide-Gated Channels in Olfactory Cilia
Rheological Analysis and Measurement of Neutrophil Indentation
A Kinetic Model for Type I and II IP3R Accounting for Mode Changes
Effects of Temperature on Heteromeric Kv11.1a/1b and Kv11.3 Channels
Volume 97, Issue 8, Pages (October 2009)
Volume 83, Issue 5, Pages (November 2002)
Bacterial Thermotaxis by Speed Modulation
Chien-Jung Lo, Mark C. Leake, Richard M. Berry  Biophysical Journal 
Volume 95, Issue 8, Pages (October 2008)
Ca2+ Regulation of Gelsolin Activity: Binding and Severing of F-actin
Rinat Nahum-Levy, Dafna Lipinski, Sara Shavit, Morris Benveniste 
Volume 102, Issue 6, Pages (March 2012)
Volume 108, Issue 11, Pages (June 2015)
Volume 97, Issue 10, Pages (November 2009)
Polarized Fluorescence Resonance Energy Transfer Microscopy
Role of Ca2+ and Cross-Bridges in Skeletal Muscle Thin Filament Activation Probed with Ca2+ Sensitizers  Philip A. Wahr, Joseph M. Metzger  Biophysical.
Volume 104, Issue 4, Pages (February 2013)
Volume 101, Issue 8, Pages (October 2011)
Probing the Dynamics of Clot-Bound Thrombin at Venous Shear Rates
Ricksen S. Winardhi, Qingnan Tang, Jin Chen, Mingxi Yao, Jie Yan 
Experimental Verification of the Behavioral Foundation of Bacterial Transport Parameters Using Microfluidics  Tanvir Ahmed, Roman Stocker  Biophysical.
Presentation transcript:

Volume 85, Issue 4, Pages 2374-2383 (October 2003) Kinetics of Increased Deformability of Deoxygenated Sickle Cells upon Oxygenation  Zhi Huang, Leigh Hearne, Cynthia E. Irby, S. Bruce King, Samir K. Ballas, Daniel B. Kim-Shapiro  Biophysical Journal  Volume 85, Issue 4, Pages 2374-2383 (October 2003) DOI: 10.1016/S0006-3495(03)74661-X Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 1 The experimental setup. The syringe pump pushed two syringes containing deoxygenated sickle erythrocytes in one and oxygenated or carbon monoxide (CO)-saturated buffer in the other to reach a final flow rate of 20 mL/min through the mixer into the flow channel. The mixer, composed of a homemade mixer followed by a 4.5cm section of an in-line mixer, was used to achieve complete mixing of the two solutions. The time it took from the mixing to the observation point was varied by changing the length of the tubing (d) between the in-line mixer and the flow channel. Longer tubing gave longer times for the deoxygenated erythrocytes to regain their optimal deformability. The deformability was probed by measuring the diffraction pattern from a laser projected onto a screen. Biophysical Journal 2003 85, 2374-2383DOI: (10.1016/S0006-3495(03)74661-X) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 2 Diffraction patterns of sickle and normal erythrocytes: fully deoxygenated, fully oxygenated, and fully CO-saturated. The calculated deformability coefficients (DCs) for the sickle cells are 1.28 for 100% deoxygenated, 1.64 for fully oxygenated, and 1.73 for fully CO-saturated. The calculated DCs for the normal cells are 3.60 for 100% deoxygenated, 3.62 for 100% oxygenated, and 3.60 for fully CO-saturated. Biophysical Journal 2003 85, 2374-2383DOI: (10.1016/S0006-3495(03)74661-X) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 3 Diffraction patterns of sickle and normal erythrocytes of deoxygenated sickle erythrocytes mixed with oxygen (O2, 0.70mM) at various times after mixing. The calculated DCs for the sickle cells are 1.38 for 0.7s, 1.58 for 2.4s, and 1.64 for 5.3s. The calculated DCs for the normal cells are 3.62 for 0.7s, 3.58 for 2.4s, and 3.59 for 5.3s. Biophysical Journal 2003 85, 2374-2383DOI: (10.1016/S0006-3495(03)74661-X) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 4 The DC of deoxygenated sickle erythrocytes mixed with oxygenated or CO-saturated buffer plotted against time after mixing. (A) Deoxygenated sickle erythrocytes were mixed with 0.56mM oxygenated buffer to achieve a final O2 concentration of 0.28mM. The difference between the trials was due to different blood source, the freshness of the erythrocytes, and the storage time after deoxygenation. The error bars on trial 6 represent the standard deviation from two measurements on the same blood sample taken ∼30min apart. (B) Deoxygenated sickle erythrocytes were mixed with 50% CO-saturated buffer to reach a final concentration of dissolved CO of 25% (250μM). The error bars on trial 6 represent the standard deviation from two measurements on the same blood sample taken ∼30min apart. (C) Deoxygenated sickle erythrocytes were mixed with 1.4mM oxygenated (fully saturated) buffer to achieve a final O2 concentration of 0.70mM. (D) Deoxygenated sickle erythrocytes were mixed with 100% CO-saturated buffer to reach a final concentration of dissolved CO of 50% or 0.5mM. Biophysical Journal 2003 85, 2374-2383DOI: (10.1016/S0006-3495(03)74661-X) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 5 Normalized average DC of deoxygenated density-fractionated sickle erythrocytes mixed with partially O2-saturated buffer plotted against time after mixing. Measurements were taken on five different blood samples and the normalized average deformability, DC¯norm(t), was calculated as described in the Materials and Methods section. The deformability at each time after mixing was divided by the maximum deformability for that particular blood sample fraction obtained by equilibration with 100% O2. This ratio is then multiplied by the average maximum deformability of all the blood samples for the particular fraction (light, medium, or dense). The average of these normalized deformabilities from five different blood samples are plotted with ±SD. Light, medium, and dense indicate the increase in density of the three density fractions of sickle erythrocytes. Each fraction of erythrocytes was deoxygenated and then mixed with 0.56mM oxygenated buffer to achieve a final O2 concentration of 0.28mM. Biophysical Journal 2003 85, 2374-2383DOI: (10.1016/S0006-3495(03)74661-X) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 6 Average DC of deoxygenated density-fractionated sickle erythrocytes 6.5s after mixing with partially O2-saturated buffer compared with that of fully oxygenated erythrocytes for the same density fractions. The average and standard deviations were calculated from the original un-normalized data for five different blood samples. p-values were derived from a paired t-test. Biophysical Journal 2003 85, 2374-2383DOI: (10.1016/S0006-3495(03)74661-X) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 7 Average temperature effect on the DC of deoxygenated sickle erythrocytes mixed with partially O2-saturated buffer plotted against time after mixing. The un-normalized average DC and standard deviations were calculated from three paired measurements, at 20°C and 37°C, and each measurement was conducted using a different blood sample. For the DC measurements at 37°C, the blood samples were incubated at 37°C for 30min before use. The deformability of the samples after equilibration with 100% O2-saturated buffer was the same at both temperatures; for example, on one blood sample, we measured DC=2.16 at 37°C and 2.22 at 20°C. The average DC for samples equilibrated with 100% O2 at 37°C DC was 2.09±0.14. Further measurements at 37°C at 6.5s after mixing gave a value of 1.74±0.05, confirming that the deformability of the cells was still changing at 5.3s where the DC was 1.71±0.21 after mixing at this temperature. Biophysical Journal 2003 85, 2374-2383DOI: (10.1016/S0006-3495(03)74661-X) Copyright © 2003 The Biophysical Society Terms and Conditions