Ordering of lipid A-monophosphate clusters in aqueous solutions

In this investigation, a study of the self-assembly of electrostatically stabilized aqueous dispersions of nanometric lipid A-monophosphate clusters from Escherichia coli was carried out in three different volume-fraction regimes. The experimental techniques used in the investigation were osmotic pr...

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Veröffentlicht in:The Journal of chemical physics 2007-09, Vol.127 (11), p.115103-115103-22
Hauptverfasser: Faunce, Chester A., Reichelt, Hendrik, Quitschau, Peter, Paradies, Henrich H.
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Reichelt, Hendrik
Quitschau, Peter
Paradies, Henrich H.
description In this investigation, a study of the self-assembly of electrostatically stabilized aqueous dispersions of nanometric lipid A-monophosphate clusters from Escherichia coli was carried out in three different volume-fraction regimes. The experimental techniques used in the investigation were osmotic pressure, static and quasielastic light scattering, scanning electron microscopy and transmission electron microscopy, and small-angle x-ray scattering. Experiments were carried out at low ionic strength ( I = 0.1 - 5.0 mM NaCl) at 25 ° C . At volume fractions between 1.5 × 10 − 4 ⩽ ϕ ⩽ 5.4 × 10 − 4 , the lipid A-monophosphate clusters had an average rms hydrodynamic diameter of d ¯ = 7.5 nm , and a weighted-average molecular weight of ( 1.78 ± 0.23 ) × 10 5 g mol − 1 . Quasielastic light scattering (LS) experiments yield similar values for the particle size and particle size distribution compared to electron microscopy, small-angle x-ray scattering, and LS experiments. When the volume fraction was increased to a higher regime 5.4 × 10 − 4 ⩽ ϕ ⩽ 9.50 × 10 − 4 , much larger clusters of lipid A monophosphate formed. The clusters detected in this volume-fraction range were assembled from between 8 and 52 of the d ¯ = 7.5 nm clusters and the assemblies are densely packed in such a way that colloidal crystals composed of the monodisperse microspheres are in physical contact with their nearest neighbors. Clusters that formed in volume fractions between 10.0 × 10 − 4 ⩽ ϕ ⩽ 40.0 × 10 − 4 revealed a weighted-average molecular weight of ( 10.15 ± 0.17 ) × 10 6 g mol − 1 and a hydrodynamic diameter of ∼ d ¯ = 70.6 nm . The crossover volume fraction between the small and the large clusters appeared at ϕ cr = 5.05 × 10 − 4 . In the intermediate volume-fraction range, the scattered intensity I ( Q ) vs Q curves (light and x rays) showed asymptotic behavior. From the asymptotic curves, the scattered intensity, the relationship between the average mass and radius, and the fractal dimension d f were determined. The d f value, which was evaluated from the expression I ( Q ) ∝ R G d f , was found to be 1.67 ± 0.03 , a value that was virtually independent of the ionic strength ( 0.1 - 5.0 mM NaCl) at 25 ° C . Even at a very low ionic strength ( I = 0.10 mM NaCl), lipid A monophosphate formed a number of differently shaped clusters. Electron microscope images showed that two types of self-assembled clusters existed at the lowest volume-fraction range studied and also dominated the ima
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The experimental techniques used in the investigation were osmotic pressure, static and quasielastic light scattering, scanning electron microscopy and transmission electron microscopy, and small-angle x-ray scattering. Experiments were carried out at low ionic strength ( I = 0.1 - 5.0 mM NaCl) at 25 ° C . At volume fractions between 1.5 × 10 − 4 ⩽ ϕ ⩽ 5.4 × 10 − 4 , the lipid A-monophosphate clusters had an average rms hydrodynamic diameter of d ¯ = 7.5 nm , and a weighted-average molecular weight of ( 1.78 ± 0.23 ) × 10 5 g mol − 1 . Quasielastic light scattering (LS) experiments yield similar values for the particle size and particle size distribution compared to electron microscopy, small-angle x-ray scattering, and LS experiments. When the volume fraction was increased to a higher regime 5.4 × 10 − 4 ⩽ ϕ ⩽ 9.50 × 10 − 4 , much larger clusters of lipid A monophosphate formed. The clusters detected in this volume-fraction range were assembled from between 8 and 52 of the d ¯ = 7.5 nm clusters and the assemblies are densely packed in such a way that colloidal crystals composed of the monodisperse microspheres are in physical contact with their nearest neighbors. Clusters that formed in volume fractions between 10.0 × 10 − 4 ⩽ ϕ ⩽ 40.0 × 10 − 4 revealed a weighted-average molecular weight of ( 10.15 ± 0.17 ) × 10 6 g mol − 1 and a hydrodynamic diameter of ∼ d ¯ = 70.6 nm . The crossover volume fraction between the small and the large clusters appeared at ϕ cr = 5.05 × 10 − 4 . In the intermediate volume-fraction range, the scattered intensity I ( Q ) vs Q curves (light and x rays) showed asymptotic behavior. From the asymptotic curves, the scattered intensity, the relationship between the average mass and radius, and the fractal dimension d f were determined. The d f value, which was evaluated from the expression I ( Q ) ∝ R G d f , was found to be 1.67 ± 0.03 , a value that was virtually independent of the ionic strength ( 0.1 - 5.0 mM NaCl) at 25 ° C . Even at a very low ionic strength ( I = 0.10 mM NaCl), lipid A monophosphate formed a number of differently shaped clusters. Electron microscope images showed that two types of self-assembled clusters existed at the lowest volume-fraction range studied and also dominated the images taken at the higher volume-fraction regimes. One type of cluster showed a cubic morphology and a size variation of 50 - 100 nm , while another type took on the appearance of a quadratic cylinder, with dimensions of 50 × 150 nm 2 . The other clusters appeared in various shapes: dimers, trimers, and distorted tetramers, which were quite different from the ones previously observed for lipid A diphosphate. Small-angle x-ray diffraction experiments on lipid A-monophosphate clusters suspended in water, containing 5 mM NaCl ( 25 ° C ) , indicated the existence of long-range order of d ¯ = 7.5 nm . At low polydispersity, two distinct types of lipid A-monophosphate colloidal clusters were able to form at low polydispersity and were subsequently identified using light scattering, small-angle x-ray scattering, and selected-area electron diffraction. From an analysis of experimental results obtained from these clusters, distinct peaks could be assigned to a body-centered cubic (bcc) lattice, with a = 49.5 ± 1.8 nm . The solution structure found for lipid A diphosphate at volume fractions of 3.75 × 10 − 4 ⩽ ϕ ⩽ 4.15 × 10 − 4 also exhibited a (bcc)-type lattice; however, a = 36.1 nm [ C. A. Faunce J. Phys. Chem. 107 , 2214 ( 2003 ) ]. Using the particle and cluster properties determined from small-angle x-ray scattering, light scattering, and osmotic-pressure measurements as a function of volume fraction, good agreement was found between the directly measured osmotic-pressure values and those calculated from scattering experiments.</description><identifier>ISSN: 0021-9606</identifier><identifier>EISSN: 1089-7690</identifier><identifier>DOI: 10.1063/1.2768524</identifier><identifier>PMID: 17887884</identifier><identifier>CODEN: JCPSA6</identifier><language>eng</language><publisher>United States: American Institute of Physics</publisher><subject>Escherichia coli - metabolism ; Light ; Lipid A - chemistry ; Lipids - chemistry ; Microscopy, Electron, Scanning ; Microscopy, Electron, Transmission ; Microspheres ; Models, Chemical ; Models, Statistical ; Molecular Weight ; Phosphates - chemistry ; Scattering, Radiation ; Spectrometry, Mass, Matrix-Assisted Laser Desorption-Ionization ; Water - chemistry ; X-Rays</subject><ispartof>The Journal of chemical physics, 2007-09, Vol.127 (11), p.115103-115103-22</ispartof><rights>2007 American Institute of Physics</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c337t-4c409c811d016655f55288967baa4f17f2b5a989a89a28cd3a48329ec737bee33</citedby><cites>FETCH-LOGICAL-c337t-4c409c811d016655f55288967baa4f17f2b5a989a89a28cd3a48329ec737bee33</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,794,1559,4512,27924,27925</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/17887884$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Faunce, Chester A.</creatorcontrib><creatorcontrib>Reichelt, Hendrik</creatorcontrib><creatorcontrib>Quitschau, Peter</creatorcontrib><creatorcontrib>Paradies, Henrich H.</creatorcontrib><title>Ordering of lipid A-monophosphate clusters in aqueous solutions</title><title>The Journal of chemical physics</title><addtitle>J Chem Phys</addtitle><description>In this investigation, a study of the self-assembly of electrostatically stabilized aqueous dispersions of nanometric lipid A-monophosphate clusters from Escherichia coli was carried out in three different volume-fraction regimes. The experimental techniques used in the investigation were osmotic pressure, static and quasielastic light scattering, scanning electron microscopy and transmission electron microscopy, and small-angle x-ray scattering. Experiments were carried out at low ionic strength ( I = 0.1 - 5.0 mM NaCl) at 25 ° C . At volume fractions between 1.5 × 10 − 4 ⩽ ϕ ⩽ 5.4 × 10 − 4 , the lipid A-monophosphate clusters had an average rms hydrodynamic diameter of d ¯ = 7.5 nm , and a weighted-average molecular weight of ( 1.78 ± 0.23 ) × 10 5 g mol − 1 . Quasielastic light scattering (LS) experiments yield similar values for the particle size and particle size distribution compared to electron microscopy, small-angle x-ray scattering, and LS experiments. When the volume fraction was increased to a higher regime 5.4 × 10 − 4 ⩽ ϕ ⩽ 9.50 × 10 − 4 , much larger clusters of lipid A monophosphate formed. The clusters detected in this volume-fraction range were assembled from between 8 and 52 of the d ¯ = 7.5 nm clusters and the assemblies are densely packed in such a way that colloidal crystals composed of the monodisperse microspheres are in physical contact with their nearest neighbors. Clusters that formed in volume fractions between 10.0 × 10 − 4 ⩽ ϕ ⩽ 40.0 × 10 − 4 revealed a weighted-average molecular weight of ( 10.15 ± 0.17 ) × 10 6 g mol − 1 and a hydrodynamic diameter of ∼ d ¯ = 70.6 nm . The crossover volume fraction between the small and the large clusters appeared at ϕ cr = 5.05 × 10 − 4 . In the intermediate volume-fraction range, the scattered intensity I ( Q ) vs Q curves (light and x rays) showed asymptotic behavior. From the asymptotic curves, the scattered intensity, the relationship between the average mass and radius, and the fractal dimension d f were determined. The d f value, which was evaluated from the expression I ( Q ) ∝ R G d f , was found to be 1.67 ± 0.03 , a value that was virtually independent of the ionic strength ( 0.1 - 5.0 mM NaCl) at 25 ° C . Even at a very low ionic strength ( I = 0.10 mM NaCl), lipid A monophosphate formed a number of differently shaped clusters. Electron microscope images showed that two types of self-assembled clusters existed at the lowest volume-fraction range studied and also dominated the images taken at the higher volume-fraction regimes. One type of cluster showed a cubic morphology and a size variation of 50 - 100 nm , while another type took on the appearance of a quadratic cylinder, with dimensions of 50 × 150 nm 2 . The other clusters appeared in various shapes: dimers, trimers, and distorted tetramers, which were quite different from the ones previously observed for lipid A diphosphate. Small-angle x-ray diffraction experiments on lipid A-monophosphate clusters suspended in water, containing 5 mM NaCl ( 25 ° C ) , indicated the existence of long-range order of d ¯ = 7.5 nm . At low polydispersity, two distinct types of lipid A-monophosphate colloidal clusters were able to form at low polydispersity and were subsequently identified using light scattering, small-angle x-ray scattering, and selected-area electron diffraction. From an analysis of experimental results obtained from these clusters, distinct peaks could be assigned to a body-centered cubic (bcc) lattice, with a = 49.5 ± 1.8 nm . The solution structure found for lipid A diphosphate at volume fractions of 3.75 × 10 − 4 ⩽ ϕ ⩽ 4.15 × 10 − 4 also exhibited a (bcc)-type lattice; however, a = 36.1 nm [ C. A. Faunce J. Phys. Chem. 107 , 2214 ( 2003 ) ]. Using the particle and cluster properties determined from small-angle x-ray scattering, light scattering, and osmotic-pressure measurements as a function of volume fraction, good agreement was found between the directly measured osmotic-pressure values and those calculated from scattering experiments.</description><subject>Escherichia coli - metabolism</subject><subject>Light</subject><subject>Lipid A - chemistry</subject><subject>Lipids - chemistry</subject><subject>Microscopy, Electron, Scanning</subject><subject>Microscopy, Electron, Transmission</subject><subject>Microspheres</subject><subject>Models, Chemical</subject><subject>Models, Statistical</subject><subject>Molecular Weight</subject><subject>Phosphates - chemistry</subject><subject>Scattering, Radiation</subject><subject>Spectrometry, Mass, Matrix-Assisted Laser Desorption-Ionization</subject><subject>Water - chemistry</subject><subject>X-Rays</subject><issn>0021-9606</issn><issn>1089-7690</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2007</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNp1kEtLxDAUhYMozji68A9IV4KLjjdJm8dCZBh8wcBsdB3SNHUibVOTduG_t-NUXAkH7ubjcO6H0CWGJQZGb_GScCZykh2hOQYhU84kHKM5AMGpZMBm6CzGDwDAnGSnaIa5EGOyObrfhtIG174nvkpq17kyWaWNb32387Hb6d4mph5ib0NMXJvoz8H6ISbR10PvfBvP0Uml62gvprtAb48Pr-vndLN9elmvNqmhlPdpZjKQRmBcAmYsz6s8J0JIxgutswrzihS5lkLqMUSYkupMUCKt4ZQX1lK6QNeH3i74cUPsVeOisXWt2_0gxQQFDiBG8OYAmuBjDLZSXXCNDl8Kg9rbUlhNtkb2aiodisaWf-SkZwTuDkA0rtf7h_9v-xWpfKV-RKoV_QbqxHin</recordid><startdate>20070921</startdate><enddate>20070921</enddate><creator>Faunce, Chester A.</creator><creator>Reichelt, Hendrik</creator><creator>Quitschau, Peter</creator><creator>Paradies, Henrich H.</creator><general>American Institute of Physics</general><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope></search><sort><creationdate>20070921</creationdate><title>Ordering of lipid A-monophosphate clusters in aqueous solutions</title><author>Faunce, Chester A. ; Reichelt, Hendrik ; Quitschau, Peter ; Paradies, Henrich H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c337t-4c409c811d016655f55288967baa4f17f2b5a989a89a28cd3a48329ec737bee33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2007</creationdate><topic>Escherichia coli - metabolism</topic><topic>Light</topic><topic>Lipid A - chemistry</topic><topic>Lipids - chemistry</topic><topic>Microscopy, Electron, Scanning</topic><topic>Microscopy, Electron, Transmission</topic><topic>Microspheres</topic><topic>Models, Chemical</topic><topic>Models, Statistical</topic><topic>Molecular Weight</topic><topic>Phosphates - chemistry</topic><topic>Scattering, Radiation</topic><topic>Spectrometry, Mass, Matrix-Assisted Laser Desorption-Ionization</topic><topic>Water - chemistry</topic><topic>X-Rays</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Faunce, Chester A.</creatorcontrib><creatorcontrib>Reichelt, Hendrik</creatorcontrib><creatorcontrib>Quitschau, Peter</creatorcontrib><creatorcontrib>Paradies, Henrich H.</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>The Journal of chemical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Faunce, Chester A.</au><au>Reichelt, Hendrik</au><au>Quitschau, Peter</au><au>Paradies, Henrich H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Ordering of lipid A-monophosphate clusters in aqueous solutions</atitle><jtitle>The Journal of chemical physics</jtitle><addtitle>J Chem Phys</addtitle><date>2007-09-21</date><risdate>2007</risdate><volume>127</volume><issue>11</issue><spage>115103</spage><epage>115103-22</epage><pages>115103-115103-22</pages><issn>0021-9606</issn><eissn>1089-7690</eissn><coden>JCPSA6</coden><abstract>In this investigation, a study of the self-assembly of electrostatically stabilized aqueous dispersions of nanometric lipid A-monophosphate clusters from Escherichia coli was carried out in three different volume-fraction regimes. The experimental techniques used in the investigation were osmotic pressure, static and quasielastic light scattering, scanning electron microscopy and transmission electron microscopy, and small-angle x-ray scattering. Experiments were carried out at low ionic strength ( I = 0.1 - 5.0 mM NaCl) at 25 ° C . At volume fractions between 1.5 × 10 − 4 ⩽ ϕ ⩽ 5.4 × 10 − 4 , the lipid A-monophosphate clusters had an average rms hydrodynamic diameter of d ¯ = 7.5 nm , and a weighted-average molecular weight of ( 1.78 ± 0.23 ) × 10 5 g mol − 1 . Quasielastic light scattering (LS) experiments yield similar values for the particle size and particle size distribution compared to electron microscopy, small-angle x-ray scattering, and LS experiments. When the volume fraction was increased to a higher regime 5.4 × 10 − 4 ⩽ ϕ ⩽ 9.50 × 10 − 4 , much larger clusters of lipid A monophosphate formed. The clusters detected in this volume-fraction range were assembled from between 8 and 52 of the d ¯ = 7.5 nm clusters and the assemblies are densely packed in such a way that colloidal crystals composed of the monodisperse microspheres are in physical contact with their nearest neighbors. Clusters that formed in volume fractions between 10.0 × 10 − 4 ⩽ ϕ ⩽ 40.0 × 10 − 4 revealed a weighted-average molecular weight of ( 10.15 ± 0.17 ) × 10 6 g mol − 1 and a hydrodynamic diameter of ∼ d ¯ = 70.6 nm . The crossover volume fraction between the small and the large clusters appeared at ϕ cr = 5.05 × 10 − 4 . In the intermediate volume-fraction range, the scattered intensity I ( Q ) vs Q curves (light and x rays) showed asymptotic behavior. From the asymptotic curves, the scattered intensity, the relationship between the average mass and radius, and the fractal dimension d f were determined. The d f value, which was evaluated from the expression I ( Q ) ∝ R G d f , was found to be 1.67 ± 0.03 , a value that was virtually independent of the ionic strength ( 0.1 - 5.0 mM NaCl) at 25 ° C . Even at a very low ionic strength ( I = 0.10 mM NaCl), lipid A monophosphate formed a number of differently shaped clusters. Electron microscope images showed that two types of self-assembled clusters existed at the lowest volume-fraction range studied and also dominated the images taken at the higher volume-fraction regimes. One type of cluster showed a cubic morphology and a size variation of 50 - 100 nm , while another type took on the appearance of a quadratic cylinder, with dimensions of 50 × 150 nm 2 . The other clusters appeared in various shapes: dimers, trimers, and distorted tetramers, which were quite different from the ones previously observed for lipid A diphosphate. Small-angle x-ray diffraction experiments on lipid A-monophosphate clusters suspended in water, containing 5 mM NaCl ( 25 ° C ) , indicated the existence of long-range order of d ¯ = 7.5 nm . At low polydispersity, two distinct types of lipid A-monophosphate colloidal clusters were able to form at low polydispersity and were subsequently identified using light scattering, small-angle x-ray scattering, and selected-area electron diffraction. From an analysis of experimental results obtained from these clusters, distinct peaks could be assigned to a body-centered cubic (bcc) lattice, with a = 49.5 ± 1.8 nm . The solution structure found for lipid A diphosphate at volume fractions of 3.75 × 10 − 4 ⩽ ϕ ⩽ 4.15 × 10 − 4 also exhibited a (bcc)-type lattice; however, a = 36.1 nm [ C. A. Faunce J. Phys. Chem. 107 , 2214 ( 2003 ) ]. Using the particle and cluster properties determined from small-angle x-ray scattering, light scattering, and osmotic-pressure measurements as a function of volume fraction, good agreement was found between the directly measured osmotic-pressure values and those calculated from scattering experiments.</abstract><cop>United States</cop><pub>American Institute of Physics</pub><pmid>17887884</pmid><doi>10.1063/1.2768524</doi><tpages>1</tpages></addata></record>
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subjects Escherichia coli - metabolism
Light
Lipid A - chemistry
Lipids - chemistry
Microscopy, Electron, Scanning
Microscopy, Electron, Transmission
Microspheres
Models, Chemical
Models, Statistical
Molecular Weight
Phosphates - chemistry
Scattering, Radiation
Spectrometry, Mass, Matrix-Assisted Laser Desorption-Ionization
Water - chemistry
X-Rays
title Ordering of lipid A-monophosphate clusters in aqueous solutions
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