Evidence map›Paper›PMID 25758637›Full record

ArticlePhysical chemistry chemical physics : PCCP2015

Structural insights into the cubic-hexagonal phase transition kinetics of monoolein modulated by sucrose solutions.

Caleb W Reese, Zachariah I Strango, Zachary R Dell, Stephanie Tristram-Nagle, Paul E Harper

Abstract read
In one paragraph

Article in Physical chemistry chemical physics : PCCP, 2015. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 3 papers.

0numbers the graph read from it
0cells of the map it votes in
3citing papers in PubMed
–field-weighted citation impact
1 · What the graph read from it

What it found

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The abstract states no effect estimate the extractor could read, or names no intervention and outcome on the map, so this paper lights no cell and moves no belief. It is still indexed, cited and linked below.

2 · The registry

The trial behind it

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3 · Its place in the literature

Who cites it

3 citing papers in PubMed.

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4 · The record

Corrections and comments

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5 · Who and what money

Authors and funding

5 authors.

Caleb W ReeseDepartment of Physics and Astronomy, Calvin College, 1734 Knollcrest Circle SE, Grand Rapids, MI, USA. pharper@calvin.edu.
Zachariah I Strango
Zachary R Dell
Stephanie Tristram-Nagle
Paul E Harper

Funding

STRUCTURE OF LIPID BILAYERSR01GM044976 · NIGMS · CARNEGIE-MELLON UNIVERSITY · PI NAGLE, JOHN F, TRISTRAM-NAGLE, STEPHANIE · 1990 to 2014
$3.1M
Howard Hughes Medical InstituteNIGMS NIH HHS GM44976NIGMS NIH HHS R01 GM044976
6 · The paper itself

Abstract

Using DSC (differential scanning calorimetry), we measure the kinetics of the cubic-HII phase transition of monoolein in bulk sucrose solutions. We find that the transition temperature is dramatically lowered, with each 1 mol kg(-1) of sucrose concentration dropping the transition by 20 °C. The kinetics of this transition also slow greatly with increasing sucrose concentration. For low sucrose concentrations, the kinetics are asymmetric, with the cooling (HII-cubic) transition taking twice as long as the heating (cubic-HII) transition. This asymmetry in transition times is reduced for higher sucrose concentrations. The cooling transition exhibits Avrami exponents in the range of 2 to 2.5 and the heating transition shows Avrami exponents ranging from 1 to 3. A classical Avrami interpretation would be that these processes occur via a one or two dimensional pathway with variable nucleation rates. A non-classical perspective would suggest that these exponents reflect the time dependence of pore formation (cooling) and destruction (heating). New density measurements of monoolein show that the currently accepted value is about 5% too low; this has substantial implications for electron density modeling. Structural calculations indicate that the head group area and lipid length in the cubic-HII transition shrink by about 12% and 4% respectively; this reduction is practically the same as that seen in a lipid with a very different molecular structure (rac-di-12:0 β-GlcDAG) that makes the same transition. Thermodynamic considerations suggest there is a hydration shell about one water molecule thick in front of the lipid head groups in both the cubic and HII phases.

Indexed as

Phase TransitionCalorimetry, Differential ScanningGlyceridesKineticsMolecular StructurePhosphatidylethanolaminesSucroseThermodynamicsTransition TemperatureWaterX-Ray DiffractionGlyceridesmonooleinPhosphatidylethanolaminesSucroseWater

Identifiers

PMID25758637
PMCPMC4381959

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Read under generation 80e0d062 · epoch 390. Bibliography from PubMed, PubMed Central and OpenAlex; grants from NIH RePORTER; trial links from ClinicalTrials.gov; estimates, votes and beliefs from the OpenQuestion graph.