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Single-Particle Electrophoresis in Nanochannels

[Image: see text] Electrophoretic mobilities and particle sizes of individual Hepatitis B Virus (HBV) capsids were measured in nanofluidic channels with two nanopores in series. The channels and pores had three-dimensional topography and were milled directly in glass substrates with a focused ion be...

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Autores principales: Harms, Zachary D., Haywood, Daniel G., Kneller, Andrew R., Selzer, Lisa, Zlotnick, Adam, Jacobson, Stephen C.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2014
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4287839/
https://www.ncbi.nlm.nih.gov/pubmed/25489919
http://dx.doi.org/10.1021/ac503527d
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author Harms, Zachary D.
Haywood, Daniel G.
Kneller, Andrew R.
Selzer, Lisa
Zlotnick, Adam
Jacobson, Stephen C.
author_facet Harms, Zachary D.
Haywood, Daniel G.
Kneller, Andrew R.
Selzer, Lisa
Zlotnick, Adam
Jacobson, Stephen C.
author_sort Harms, Zachary D.
collection PubMed
description [Image: see text] Electrophoretic mobilities and particle sizes of individual Hepatitis B Virus (HBV) capsids were measured in nanofluidic channels with two nanopores in series. The channels and pores had three-dimensional topography and were milled directly in glass substrates with a focused ion beam instrument assisted by an electron flood gun. The nanochannel between the two pores was 300 nm wide, 100 nm deep, and 2.5 μm long, and the nanopores at each end had dimensions 45 nm wide, 45 nm deep, and 400 nm long. With resistive-pulse sensing, the nanopores fully resolved pulse amplitude distributions of T = 3 HBV capsids (32 nm outer diameter) and T = 4 HBV capsids (35 nm outer diameter) and had sufficient peak capacity to discriminate intermediate species from the T = 3 and T = 4 capsid distributions in an assembly reaction. Because the T = 3 and T = 4 capsids have a wiffle-ball geometry with a hollow core, the observed change in current due to the capsid transiting the nanopore is proportional to the volume of electrolyte displaced by the volume of capsid protein, not the volume of the entire capsid. Both the signal-to-noise ratio of the pulse amplitude and resolution between the T = 3 and T = 4 distributions of the pulse amplitudes increase as the electric field strength is increased. At low field strengths, transport of the larger T = 4 capsid through the nanopores is hindered relative to the smaller T = 3 capsid due to interaction with the pores, but at sufficiently high field strengths, the T = 3 and T = 4 capsids had the same electrophoretic mobilities (7.4 × 10(–5) cm(2) V(–1) s(–1)) in the nanopores and in the nanochannel with the larger cross-sectional area.
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spelling pubmed-42878392015-11-28 Single-Particle Electrophoresis in Nanochannels Harms, Zachary D. Haywood, Daniel G. Kneller, Andrew R. Selzer, Lisa Zlotnick, Adam Jacobson, Stephen C. Anal Chem [Image: see text] Electrophoretic mobilities and particle sizes of individual Hepatitis B Virus (HBV) capsids were measured in nanofluidic channels with two nanopores in series. The channels and pores had three-dimensional topography and were milled directly in glass substrates with a focused ion beam instrument assisted by an electron flood gun. The nanochannel between the two pores was 300 nm wide, 100 nm deep, and 2.5 μm long, and the nanopores at each end had dimensions 45 nm wide, 45 nm deep, and 400 nm long. With resistive-pulse sensing, the nanopores fully resolved pulse amplitude distributions of T = 3 HBV capsids (32 nm outer diameter) and T = 4 HBV capsids (35 nm outer diameter) and had sufficient peak capacity to discriminate intermediate species from the T = 3 and T = 4 capsid distributions in an assembly reaction. Because the T = 3 and T = 4 capsids have a wiffle-ball geometry with a hollow core, the observed change in current due to the capsid transiting the nanopore is proportional to the volume of electrolyte displaced by the volume of capsid protein, not the volume of the entire capsid. Both the signal-to-noise ratio of the pulse amplitude and resolution between the T = 3 and T = 4 distributions of the pulse amplitudes increase as the electric field strength is increased. At low field strengths, transport of the larger T = 4 capsid through the nanopores is hindered relative to the smaller T = 3 capsid due to interaction with the pores, but at sufficiently high field strengths, the T = 3 and T = 4 capsids had the same electrophoretic mobilities (7.4 × 10(–5) cm(2) V(–1) s(–1)) in the nanopores and in the nanochannel with the larger cross-sectional area. American Chemical Society 2014-11-28 2015-01-06 /pmc/articles/PMC4287839/ /pubmed/25489919 http://dx.doi.org/10.1021/ac503527d Text en Copyright © 2014 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes.
spellingShingle Harms, Zachary D.
Haywood, Daniel G.
Kneller, Andrew R.
Selzer, Lisa
Zlotnick, Adam
Jacobson, Stephen C.
Single-Particle Electrophoresis in Nanochannels
title Single-Particle Electrophoresis in Nanochannels
title_full Single-Particle Electrophoresis in Nanochannels
title_fullStr Single-Particle Electrophoresis in Nanochannels
title_full_unstemmed Single-Particle Electrophoresis in Nanochannels
title_short Single-Particle Electrophoresis in Nanochannels
title_sort single-particle electrophoresis in nanochannels
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4287839/
https://www.ncbi.nlm.nih.gov/pubmed/25489919
http://dx.doi.org/10.1021/ac503527d
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