'Conductance' presentation slideshows

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Vacuum Systems

Vacuum Systems

Vacuum Systems. Lecture 6 G.J. Mankey gmankey@mint.ua.edu. Pumping Speed and Throughput. The mass flow or throughput of a pump is given by the equation Q = SP where S is the pumping speed and P is the pressure. For a conductive element Q = C(P 1 -P 2 )

By amina
(250 views)

IPCMS - DMONS

IPCMS - DMONS

PHYSIQUE MESOSCOPIQUE. IPCMS - DMONS. Rodolfo Jalabert Dietmar Weinmann. Post-docs: Jérôme Roccia (DMONS-DON) Guillaume Weick. Etudiants: Guido Intronati (Strasbourg – Buenos Aires) Wojciech Szewc. Domaines de recherche :.

By jacques
(78 views)

Gauss’s Law

Gauss’s Law

Gauss’s Law. In differential form: When integrated over a volume, we have where Q is the total charge in volume v . Using Gauss’s theorem: We obtain the integral form:. Ulaby Figure 4-8. Gauss’s Law. Applications In some simple cases with high symmetry, solutions may be found directly

By soren
(370 views)

Oracle Labs Graph Analytics Research

Oracle Labs Graph Analytics Research

Oracle Labs Graph Analytics Research. Hassan Chafi Sr. Research Manager Oracle Labs Graph-TA 2/21/2014.

By nayef
(89 views)

Bounding the mixing time via Spectral Gap

Bounding the mixing time via Spectral Gap

Bounding the mixing time via Spectral Gap. Ilan Ben-Bassat Omri Weinstein. Conductance . Properties. Reversible Chains. (*). x>=y. Upper Bound of the Spectral Gap. Path Congestion.

By jalena
(102 views)

Heating and Efficiency

Heating and Efficiency

Heating and Efficiency. AP Env Sci - Home Heating Activity. Heat Needed for a Home or Other “Space”. Heat expressed in Btu - British Thermal Units - heat 1 lb water 1 degree F. H=heat needed in Btu H= K is thermal conductance What are factors that determine K. H = K T t

By zamora
(75 views)

Ion Channels as Nanopores - From Principles to Biosensors

Ion Channels as Nanopores - From Principles to Biosensors

Signal IN. Signal OUT. Sensor. Ion Channels as Nanopores - From Principles to Biosensors. What to detect? Why pores ? Why bio ?. Overview. Today: Principles and proteins. Review of basic properties of channels & pores Single channel measurements – technologies

By missy
(103 views)

IPCMS - DMONS

IPCMS - DMONS

PHYSIQUE MESOSCOPIQUE. IPCMS - DMONS. Rodolfo Jalabert Dietmar Weinmann. Post-docs: Jérôme Roccia (DMONS-DON) Guillaume Weick. Etudiants: Guido Intronati (Strasbourg – Buenos Aires) Wojciech Szewc. Domaines de recherche :.

By selah
(109 views)

A coherent subnanosecond single electron source

A coherent subnanosecond single electron source

A coherent subnanosecond single electron source. Gwendal Fève. Groupe de Physique Mésoscopique Laboratoire Pierre Aigrain ENS. Jean-Marc Berroir Bernard Plaçais Christian Glattli Takis Kontos. Julien Gabelli Adrien Mahé.

By leoma
(98 views)

The Ring Model of Cortical Dynamics: An overview

The Ring Model of Cortical Dynamics: An overview

David Hansel Laboratoire de Neurophysique et Physiologie CNRS-Université René Descartes, Paris, France. The Ring Model of Cortical Dynamics: An overview. Uninet. Leiden 22/05/08. Investigating Brain Dynamical States. Nature of the interactions:

By arva
(112 views)

G. S. Diniz and S. E. Ulloa

G. S. Diniz and S. E. Ulloa

Spin-orbit coupling and electronic transport in carbon nanotubes in external fields. G. S. Diniz and S. E. Ulloa. Department of Physics and Astronomy , Ohio University , Athens -OH. Supported by. G. S. Diniz and S. E. Ulloa. Boston, APS March Meeting 2012. Motivation & Outline.

By blithe
(120 views)

G. S. Diniz and S. E. Ulloa

G. S. Diniz and S. E. Ulloa

Spin-orbit coupling and electronic transport in carbon nanotubes in external fields. G. S. Diniz and S. E. Ulloa. Department of Physics and Astronomy , Ohio University , Athens -OH. Supported by. G. S. Diniz and S. E. Ulloa. Boston, APS March Meeting 2012. Motivation & Outline.

By nhi
(119 views)

Rf-set and rf QPC 超灵敏静电计

Rf-set and rf QPC 超灵敏静电计

Rf-set and rf QPC 超灵敏静电计. LQCC-QT. SET 工作原理. SET 中的噪声. SET 的极限灵敏度. RF-SET. 反射型 RF-SET.

By duena
(81 views)

Probing the conductance superposition law in single-molecule circuits with parallel paths

Probing the conductance superposition law in single-molecule circuits with parallel paths

Probing the conductance superposition law in single-molecule circuits with parallel paths. Probing the conductance superposition law in single-molecule circuits with parallel paths. 1,4-bis(methyl(thio)methyl)–benzene (1). sulphur groups bind to the gold leads.

By amma
(185 views)

Congresso del Dipartimento di Fisica Highlights in Physics 2005

Congresso del Dipartimento di Fisica Highlights in Physics 2005

A. Figure 4 : Experimental setup: (1) DSO (2) Computer (3) Relay (4) Contacts (5) AC Voltage Supplier. Figure 3. (a) Energy dispersion of graphene p -band, (b) Electronic band structure of a (4,2) nanotube, (c) Density of states of the electronic band diagram.

By waseem
(119 views)

Transport through junctions of interacting quantum wires and nanotubes

Transport through junctions of interacting quantum wires and nanotubes

Transport through junctions of interacting quantum wires and nanotubes. R. Egger Institut für Theoretische Physik Heinrich-Heine Universität Düsseldorf S. Chen, S. Gogolin, H. Grabert, A. Komnik, H. Saleur, F. Siano, B. Trauzettel. Overview.

By byrd
(151 views)

Experimental characterization of simple single-molecule junctions

Experimental characterization of simple single-molecule junctions

Experimental characterization of simple single-molecule junctions. In collaboration with. Kamerlingh Onnes Laboratory, Leiden University. Leiden: Marc van Hemert IBM Yorktown Heights: Norton Lang Technical University of Denmark: Kristian Thygesen, Karsten Jacobsen.

By ganit
(107 views)

Ballistic conductance of suspended nanowires: An ab initio description

Ballistic conductance of suspended nanowires: An ab initio description

Ballistic conductance of suspended nanowires: An ab initio description. M. Czerner 1 , A. Bagrets 1 , N. Papanikolaou 2 , V.S. Stepanyuk 3 and I. Mertig 1 1 Martin-Luther-Universit ät Halle, Germany

By duke
(104 views)

Ballistic transport under Quantum Hall effect conditions

Ballistic transport under Quantum Hall effect conditions

Ballistic transport under Quantum Hall effect conditions. S.Nazin, V.Shikin, ISSP RAS. Outline. 1. 1-D ballistic conductance definition 2. Hall-effect, Quantum Hall-effect (QHE) definitions 3. Edge (ballistic) scenario for QHE realization (Halperin, 1982; Buttiker, 1986)

By dillon-mcconnell
(292 views)

Cable Model Voltage Clamp Propagation of an Action Potential

Cable Model Voltage Clamp Propagation of an Action Potential

Cable Model Voltage Clamp Propagation of an Action Potential. Illustrations are taken from: J. Malmivuo, R. Plonsey, Bioelectromagnetism, Oxford Press, 1995 http://butler.cc.tut.fi/~malmivuo/bem/book/. Cable Model of Axon. Steady-State Response. Propagation of Activation.

By rinah-jones
(269 views)

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