2006
DOI: 10.1002/bip.20483
|View full text |Cite
|
Sign up to set email alerts
|

Investigating the permanent electric dipole moment of β‐lactoglobulin fibrils, using transient electric birefringence

Abstract: Amyloid fibrils, which are polymeric assemblies of protein molecules, have been intensively studied on a structural level, yet due to complications such as the disorder within the molecules, several aspects of their structure remain mysterious. Similarly, the kinetics of assembly are not well understood. Here we investigate the electric dipole moment of beta-lactoglobulin fibrils, a model amyloid fibril system, by applying the technique of transient electric birefringence. This moment appears to be large, and … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

1
21
0

Year Published

2007
2007
2019
2019

Publication Types

Select...
5
2

Relationship

0
7

Authors

Journals

citations
Cited by 27 publications
(22 citation statements)
references
References 47 publications
1
21
0
Order By: Relevance
“…They thus exhibit features associated with conventional charged polymers, with, however, a persistence length remarkably independent of the environmental conditions to which they are exposed; this observation can be rationalised in the light of the fact that the origin of the persistence length of amyloid fibrils is primarily the hydrogen‐bonding network at their core which is less affected by solution conditions than electrostatic repulsion responsible for the persistence length of conventional charged polymers. Furthermore, in contrast to other polymeric systems, they exhibit a combined chirality and polarity along their fibrillar main axis, a characteristic which allows for manipulations through electric fields of very weak intensities, or by adsorption at interfaces as symmetry breaking tool . Thus, a distinctive feature of amyloids at the mesoscale is their intrinsic rigidity, which together with their chiral, polar and charged nature, provides these systems with a rich physical behavior in one, two and three dimensions.…”
Section: Amyloid Fibrils At All Length Scalesmentioning
confidence: 99%
“…They thus exhibit features associated with conventional charged polymers, with, however, a persistence length remarkably independent of the environmental conditions to which they are exposed; this observation can be rationalised in the light of the fact that the origin of the persistence length of amyloid fibrils is primarily the hydrogen‐bonding network at their core which is less affected by solution conditions than electrostatic repulsion responsible for the persistence length of conventional charged polymers. Furthermore, in contrast to other polymeric systems, they exhibit a combined chirality and polarity along their fibrillar main axis, a characteristic which allows for manipulations through electric fields of very weak intensities, or by adsorption at interfaces as symmetry breaking tool . Thus, a distinctive feature of amyloids at the mesoscale is their intrinsic rigidity, which together with their chiral, polar and charged nature, provides these systems with a rich physical behavior in one, two and three dimensions.…”
Section: Amyloid Fibrils At All Length Scalesmentioning
confidence: 99%
“…A polar twisted fibril has an anisotropy that distinguishes 'head' from 'tail' directions along the fibril axis; in F-actin this 'polarization' arises from the orientations required of G-actin monomers to effect self-assembly; 26 in an α-helix the N-C polymerisation breaks the polar symmetry and in cross-β amyloid fibrils such as those studied here the polarity is due to the molecular packing of β-sheets. [27][28][29] The polarity is reflected in variations in molecular structure along the exposed surface of the twisted ribbon. When this structure is placed in a heterogenous environment, as occurs near a solid surface or when immersed within a meniscus between two fluids (or fluid and gas), the inhomogeneity of the environment generally leads to unbalanced torques on the body (see Supplementary Note 2, Fig.…”
Section: Fibril Free Energymentioning
confidence: 99%
“…In the case of the 1 + 1 scheme k rot = 1, because equal spherical particles rotate/orientate themselves with equal velocity. For the 1 + 2 scheme applies: with the rotational diffusion coefficients for monomer particles: where at η is the dynamic viscosity of the solvent, R 1 is the radius of the monomer particle and with l as length of the oligomer, d = 2 R 1 as diameter of the monomer particle and for dimers, trimers and higher chain‐like (‘rod‐like’) oligomers (Rogers et al. , 2006).…”
Section: Model Descriptionmentioning
confidence: 99%
“…for dimers, trimers and higher chain-like ('rod-like') oligomers (Rogers et al, 2006). The interdependence (9) does not apply until l ⁄ d = 5 (Rogers et al, 2006).…”
Section: Collisionsmentioning
confidence: 99%
See 1 more Smart Citation