ESD
China
 English 繁体 最近信息 静电产品 静电标准 培训服务 ESD专家 静电应用 静电测量 ESD防护 业务产品销售咨询

ESD产品

静电测量

防护用品

售后服务

ESD测试

工厂ESD

设备ESD

元件ESD

ESD问题

业务:产品销售咨询
技术产品技术咨询

English

 

静电信息

静电产品

 

静电驻极,过滤效率不到20提升到95

静电驻极中如何注入更多的电荷,从而提高熔喷布的过滤效率?

 

EST712C静电驻极N95口罩布熔喷布无纺布静电驻极机静电驻极棒 (高效、易安装)

静电驻极N95口罩布熔喷布无纺布静电驻极机静电驻极棒

无锡常州客户使用EST712C静电驻极机的使用效果

静电应用

静电吸附

静电分选

大气静电


静电测试

ESD试验

静电防护

ESD培训

静电标准

劳保世界

ESD试验

 

ESD模型

 

静电标准


ESD问题
 

如何速查
本站

Abstracts from the
Proceedings of the Electrostatics Society of America

June 23 - 25, 1999
Boston University
Boston, Massachusetts

A bound copy of these Proceedings in their entirely can be obtained from Laplacian Press:

Contents

Preface

Charges and Fields
Corona Current in a Wire Cylinder System Revisited by James Q. Feng

Dual Trichel like Emission from Unipolar Corona Points — A Basic DC to AC Conversion
Mechanism by T.S. Lee

Radar Diagnoses of Atmospheric Electricity by M. C. Lee and J. Jastrzebski

Comparative Study of Theoretical Kerr Electro Optic Fringe Patterns in Two Dimensional and
Axisymmetric Electrode Geometries by A. Ustundag and M. Zahn

Electrostatic Aspects of Helicity in Space Physics by P. Robert Kotiuga

Powders and Particles
The Effect of Fluidizing and Transport Air Relative Humidity on Corona and Tribocharging in
the Powder Painting Process by R. A. Sims and M. K. Mazumder

A Method to Determine the Surface Charge Density of a Powder Having an Arbitrary Particle
Size Distribution by Albert E. Seaver

Bipolar Charging Effects in Polydisperse Powders by F. S. Ali, G. S. P. Castle, 1.1. Inculet
and H. Zhao

Electrophoretic and Dielectrophoretic Particle Control and Transport with a New Separation
Apparatus by Jack Macknis

Surface Charge Distribution Analysis by Fluorescent Microsphere Imaging Technique by M. K.
Mazumder, K. Tennal, and D. Lindquist

EHD Atomization of Ceramic Suspensions by W. Balachandran

Sensors and Measurements
Applications of Quasistatic Sensors: From Cure Monitoring to Landmine Imaging and Detection
by Andrew Washabaugh, Yanko Sheiretov, Darrell Schlicker, and Neil Goldfine

Measurements of Moisture Diffusion Dynamics in Transformer Insulation Using Interdigital
Dielectrometry Measurements by Y. Du, S. H. Kang, A. V. Mamishev, B. C. Lesieutre, and
M. Zahn

Forward and Inverse Parameter Estimation Algorithms of Interdigital Dielectrometry Sensors by
B.C. Lesieutre, A. V. Mamishev, Y. Du, E. Keskiner,G.C. Verghese, and M. Zahn

Applied Electrostatics
Ion Beam Contouring to Generate Sub Millimeter Optics by Thomas G. Bifano, Mark N.
Horenstein, Mike Feinberg, and Prahsant Shanbhag

A Micro Scale Electric Induction Machine for a Micro Gas Turbine Generator by Steven F.
Nagle and Jefferey H. Lang

Production of Ions and Nanoparticles from Taylor Cone Jets Of  Highly Conducting Organic
Electrolytes by J. Fernandez de la Mora and M. Gamero Castano

Control of Foodborne Pathogenic Microorganisms Using Electric Discharge Generated Ozone
Enhanced by Ultraviolet Photons by S. Edward Law and Michael E. Diaz

Lumped Element Model for Computing the Equilibrium Charge Distribution Along a Moving
Web by Mark N. Horenstein

Relating Roller Shaft Voltages to Tribocharging During Sheet Transport by Humphrey Wong
Dielectrics and Materials

The Effects of Electric Field Radiated from Electrostatic Discharge on the Electronic Circuit by
Jiu Sheng Huang

A Theoretical Paradox Related to Solid Dielectrics that Cannot be Resolved even after a
Computer Simulation Using Finite Element Analysis by Andreas Trupp

Piezoelectric Effect on Ice by Hasashi Shio

A New Unifed Method for Measurement of Electrical Resistivity of Textile Assemblies by
Pellumb G. Berberi

A Method to Estimate the Area of Contact of a Textile Fabric with a Rigid Flat Surface by
Pellumb G. Berberi, J. Amirbayat, L. Porat

Preface

At the dawn of the Industrial Revolution, electrostatics was an emerging branch of scientific
discovery. Given what we know today about electrostatics, it's hard to imagine the sense of
mystery and wonder that must have confronted early experimenters such as Franklin, Kelvin,
Coulomb, Faraday, Cavendish, and others. Through basic observation and deductive reasoning,
these scientists developed a deep understanding of electrostatics, paving the way for the
mathematical explanations recounted in Maxwell's Treatise on Electricity and Magnetism.
Although electrostatics retains its status as one of the oldest branches of physics, it continues to
this day to be a vibrant and ever emerging field of study that touches our lives on a daily basis.
We've come to accept copy machines, laser printers, fax machines, flat panel displays,
microphones, high speed printing, digital cameras, and airbag sensors—all electrostatic
devices— as part of everyday life. Although modern electrostatics has its roots in the same
fundamentals discovered by the early experimenters, it has been transformed into an engineering
discipline with strong ties to industry and commercial applications.
In the spirit of modern electrostatics, the papers contained in these proceedings reflect a great
diversity of state of the art topics in science and engineering. Indeed, individuals from other
fields may marvel at the wide range of ideas that fall within the domain of electrostatics. These
proceedings include papers on the use of electrostatics in imaging systems, coating processes,
atmospheric probing, micro electromechanical systems, land mine detection, industrial sensors,
biological pathogen control, and nanoscale particle production. Also, while much of
electrostatics deals with the harnessing of electrostatic charge, a large part of the discipline deals
with eliminating its effects. Several of topics in these proceedings, including papers on
electrostatic discharge (ESD), charge neutralization, and web charging, address this alternative
perspective.

This sixth printing of the ESA Conference Proceedings continues a tradition that started in
1994 with the help of Laplacian Press and Electrostatic Applications. Initially, ESA meetings
consisted of oral presentations only, and no permanent record of the many interesting talks and
presentations was available. Since its inception, the annual ESA Proceedings has become an
oft cited part of the vast body of literature in electrostatics. It also has provided a means for
conveying the content of the annual meeting to those individuals unable to attend. Besides
providing a permanent record of the conference, these proceedings are meant to encourage
further discussions and interactions among the attendees, ESA members, and members of our
counterpart organizations in the United States and in other countries. May the spirit of the ESA,
known by all as "The Friendly Society," continue to permeate our meetings, proceedings, social
events, and technical discussions. On behalf of the Department of Electrical and Computer
Engineering at Boston University, it is with great pleasure that I welcome you to the 1999
Annual ESA Conference.

For the Friendly Society,
Mark N. Horenstein
1999 Conference Chair

Charges and Fields

Corona Current in a Wire Cylinder System Revisited
James Q. Feng
Xerox Corporarion
800 Phillips Road, Webster, NY 14580, USA

Corona current can be generated in air or in other kinds of gas media from a thin wire enclosed
in a concentric cylinder, when the voltage difference applied between the wire and the cylinder
exceeds a threshold value. The threshold voltage difference for corona onset corresponds to the
local electric field strength around the wire becoming aufficiently large to cause localized air
breakdown or, in other words, to ionize some of the gas molecules. In the case of positive
corona, i. e., the electric field is directed outward from the wire, so that negative ions in the
ionization zone are drawn toward the wire whereas positive ions drift along the electric field lines
toward the cylinder. A unipolar charge current is established in the drift zone where ions of one
sign are dominant and those charge carriers are set in motion in response to the electric field.
Although a wire cylinder system represents one of a few simplest system configurations for
corona current generation, some commonly used theoretical formulas in the literature have
lacked rigorous mathematical derivation and analysis [ 1]. In the present work, a quadratic form
of the relationship between corona current and applied voltage is shown to be a very reasonable
approximation to the complicated exact result. However, the form of the coefficient in the
present quadratic formula is quite different from that of Townsend's quadratic formula for small
current [ 1 2]. Experimental data are gathered to compare with the theory.

Radar Diagnoses of Atmospheric Electricity

M. C. Lee and J. Jastrzebski
Department of Electrical and Computer Engineering
Boston University
Boston, Massachusetts 02215
Ph: 617 353 3363, e mail: mclee@enga.bu.edu

In this paper we discuss two phenomena of atmospheric electricity diagnosed by radars.
They are (1) energetic electrons precipitated from radiation belts, and (2) dense and hot
electrons induced by lightning. High energy electrons are trapped by Earth's magnetic field in the
radiation belts. However, whistler waves can interact resonantly with these electrons and
change their pitch angles. As the electrons fall in the loss cone of the Earth's magnetic field, they
move freely and precipitate into the lower atmosphere, causing layers of anomalous ionization.
Controlled study of precipitated electrons from radiation belts was conducted at Arecibo, using
injected VLF waves from the ground. After the ionosphere is heated by high power O mode
HF waves, large scale density irregularity sheets are generated and aligned in parallel with the
meridional plane, forming multi parallel plate waveguides (viz., ionospheric ducts) for ducted
radio wave propagation. VLF waves injected from the ground based transmitter, impinge at the
boundary between the neutral atmosphere and the disturbed ionosphere, and effectively couple
into the ionospheric ducts. When the VLF waves enter the ionosphere, they change from linear
into circular polarization and propagate in the form of whistler waves. These ducted whistler
waves were recorded at the magnetic conjugate point, Trelew, Argentina by a VLF receiver.
Triggered particle precipitation events were monitored by a UHF incoherent radar over
Arecibo. Our results show that electrons with energy exceeding 100 eV can be precipitated into
the atmosphere at the o0 80 km altitudes to produce thin but dense ionization layers, giving rise
to intense radar backscatter echoes.

We used S band, C band, and UHF radars to investigate the reflectivity of lightning induced
plasmas, by means of radio wave scattering from electron density fluctuations. The lightning
induced hot and dense electrons are modelled as long, perfectly conducting cylinders with
surface density fluctuations on a scale much smaller than the total channel length. The theoretical
wavelength dependence of the radar reflectivity is compared with experimental results. It is
found that the theory of rough surface scattering predicts two types of inverse power law
wavelength dependence for radar reflectivity. They are inversely proportional to the wavelength
and the squared wavelength, which correspond to density fluctuations of lightning plasmas with
a Gaussian type spectrum and a power law type spectrum, respectively. By contrast, the theory
of long, thin conductors predicts a square root of wavelength dependence for radar reflectivity.
The experimental observations on common lightning targets free of precipitation masking effects
show a mean wavelength dependence Iying between the predictions of the two theories. It
means that the wavelength dependence in these observations is bounded by these two theories.
We conclude that the theory for the overdense plasma channels with irregular surfaces and the
theory for long, thin overdense channels bracket the observed wavelength dependence.

Comparative Study of TheoreticalKerr Electro Optic Fringe
Patterns in Two Dimensional and Axisymmetric Electrode Geometries

A. Ustundag and M. Zahn
Department of Electrical Engineering and Computer Science
Laboratory for Electromagnetic and Electronic Systems
Massachusetts Institute of Technology
Cambridge, MA 02139

Kerr electro optic fringe patterns have long been used to study space charge injection and
transport phenomena in highly birefringent materials such as nitrobenzene. The past experimental
work has been limited to one or two dimensional geometries where the electric field magnitude
and direction have been constant along the light path such as two concentric or parallel cylinders
or parallel plate electrodes. For these geometries the light maxima and minima in the fringe
patterns can directly be used to find the electric field magnitude and direction.
In this work we calculate theoretical Kerr electro optic fringe patterns for an axisymmetric
point/plane electrode geometry for which the electric field magnitude and direction vary along
the light path. We compare these patterns to the fringe patterns of the two dimensional analog,
blade/plane geometry. We underline the differences and study how these fringe patterns can be
used to reconstruct the axisymmetric electric field components in practice. It is of interest to
extend the Kerr electro optic measurement technique to point/plane electrode geometry which
is often used in high voltage research to create large electric fields for charge injection at known
location and at reasonable voltages.

Electrostatic Aspects of Helicity in Space Physics

P. Robert Kotiuga
Dept. of Electrical and Computer Engineering
Boston University

In recent decades, magnetic helicity has been identified as a conserved quantity in many
plasmas governed by the equations of magnetohydrodynamics [l]. In particular, many plasmas
relax to a state of minimal energy subject to the constraint that helicity is conserved. This talk
begins by introducing all relevant concepts and illustrates them in the context of space plasmas.
Magnetic helicity is a topological quantity and not like a conventional conserved quantity
such as energy. For example, it changes sign if one considers a "mirror image" problem. For this
reason, it is of great interest to compute its time rate of change in nonideal plasmas and develop
a physical understanding of the result. This leads to the notion of current helicity and other
"electrostatic terms". The purpose of this talk is to identify and give meaning to these
electrostatic terms
.
[1] Invited talks from the Chapmann Conference on "Magnetic Helicity in Space and
Laboratory Plasmas" held in Boulder Colorado, July 28 31, 1998, will soon appear as an
American Geophysical Union (AGU) monograph.

Powders and Particles

The Effect of Fluidizing and Transport Air Relative Humidity on
Corona and Tribocharging in the Powder Painting Process

R. A. Sims and M. K. Mazumder
University of Arkansas at Little Rock
Department of Applied Science
ETAS 575, 2801 S. University
Little Rock, AR 72204
Tel: 501 569 8045, Fax: 501 569 8020
E mail: sims@eivax.ualr.edu

This paper presents the results from experimental studies of the effect of the relative
humidity of the fluidization and transport air on the charging ability of powder paint. These
studies measured the charge to mass ratio of acrylic automotive clear coat powders and
industrial powder paint as the moisture content of the air used for fluidization and transport was
varied from 0 •F to 35 •F dewpoint. Both corona and tribo charging were studied.

A Method to Determine the Surface Charge Density of a Powder
Having an Arbitrary Particle Size Distribution

Albert E. Seaver
3M Engineering Systems Technology Center
3M Center Bldg. 518 1 01
St. Paul, MN 55144 1000
Ph: (651) 733 8629 email: aeseaver@mmm. com

For safety reasons it is usually desirable to keep the charge on a powder low during
transport and storage. On the other hand it is desirable to obtain a very high charge on a
powder to be used in an electrostatic powder coating process. The surface charge density rTs
on a particle will have an equilibrium value determined by its collisions within its environment,
but this surface charge density can not exceed the Gaussian limit. As a result, the charge on a
powder relative to the Gaussian limit can be used to describe the state of the powder provided
the surface charge density of the powder can be estimated. Although it is relatively easy to
measure the net charge Q and net mass M of a powder sample there is no known method to
relate these measurements to the surface charge density as on the individual particles in the
powder sample if the sample has a particle size distribution. This paper examines the
mathematical relationship between Q, M and as and the results show that the surface charge
density can be determined if a separate measurement of the particle size distribution is also
made. To demonstrate the application of the analysis developed in this paper the theory is
applied to the recent charge measurements on biological particulates discussed by Banerjee and
Law.

Electrophoretic and Dielectrophoretic Particle Control
and Transport with a New Separation Apparatus

Jack Macknis
Lift Feeder, Inc.
Yardley, PA
Phone: 215 321 4776
Fax: 215 321 7003

Principles and applications will be presented for a new separator which diverts selected
components of a fluid stream out of the main stream using electric force fields (electrophoretic
or dielectrophoretic). In operation, a fluid stream is propelled axially through a three dimensional array of field
gradients produced by a repetitive pattern of rods arranged at an angle between parallel and
perpendicular to the initial flow direction into the separator. Those materials which are attracted
or repulsed by electric field forces will move toward the outside walls of the separator because
of the resultant force on them due to the combination of the force propelling them axially through
the separator and the force fields set up inside the separator.

The fluid flows axially through the separator, with the wires or rods disposed within the flow
volume and oriented at a given angle between parallel and perpendicular to the direction of flow
of the fluid stream. The given angle is designed based on the relative magnitude of the force
propelling the fluid stream axially through the separator and the forces on the selected materials
due to the electric field forces between the plurality of small diameter rods. The combination of
those forces and the angle of the rods produces resultant forces on those select molecules or
particles sensitive to the field gradients,
which are different in relation to the particle or molecules location relative to the rods.
When the field gradient force has a component opposite in direction to the propelling force,
the resultant force moves the particle towards the outside wall, and also within a channel formed
by the electric forces and parallel to the rods, because the angle of the rods is the same as the
angle of the resultant force. These particles tend to maintain the same relation relative to the
rods, and remain in the channel moving towards the outside wall. When the field gradient force
has a component in the same direction as the propelling force, the resultant force moves the
particle to a location where the field gradient has a component opposite in direction to the
propelling force or the first case.
Thus, the select molecules or particles will concentrate in the channels parallel to the rods
where the resultant force is towards the outside wall. At the outside walls, partitions or slits to
an outer plenum are located to divert the flow into separate plenum streams, where the select
molecules or particles are removed from the main fluid stream.
Advantages with this process include:

1) It is continuous with minimal contact and build up on the electrodes. The channels are
formed by the force fields with no physical hardware in the flow stream.
2) A highly effective separation volume. Effect is cumulative along the length. Each volume
passes through multiple capture sites.
3) Adaptable to a wide range of particles and molecules. Electric forces are produced
between multiple parallel rods which can be varied in diameter and spacing to produce a wide
range of gradient strength and size. This allows the process to be adaptable to a wide range of
particle sizes.
4) Moves the particles outside the main flow to a separate plenum so certain problems can
be worked on without interrupting the process.
5) Economically adaptable to nanoscale dimensions. Deposition on substrates possible.
6) Low energy and low pressure drop.
Sensors and Measurements

Applications of Quasistatic Sensors: From Cure Monitoring to
Landmine Imaging and Detection

Andrew Washabaugh, Yanko Sheiretov, Darrell Schlicker, and Neil Goldfine
JENTEK Sensors, Inc.
200 Dexter Ave.
Watertown MA 02472
Phone: (617) 926 8422 Fax: (617) 926 8744
email: jentek@shore.net

Electromagnetic sensors that operate in the low frequency, quasistatic regime are well suited
to materials characterization and defect monitoring applications. In this regime the electric and
magnetic fields are decoupled and the sensor choice depends upon the properties of the
materials being tested. For electroquasistatic (EQS) applications, capacitive sensing
dielectrometry provides information for low conductivity materials, such as layer thickness,
porosity, thermal conductivity, cure state, or the presence of defects, through measurements of
the material electrical properties such as dielectric constant, conductivity, loss tangent, or
complex permittivity. For magnetoquasistatic (MQS) applications, inductive sensing
magnetometry provides information for high conductivity and magnetic materials, such as layer
thickness, fatigue state, shot peen intensity, and crack size, through measurements of material
properties such as magnetic susceptibility, electrical conductivity, or complex permeability.
This paper focuses on dielectrometry applications and will describe sensor configurations
and inversion methods for obtaining real time property estimates. Representative applications to
be described include monitoring of epoxies during the curing transient, dielectric coating
thickness measurement, monitoring of moisture concentrations in porous transformer
pressboard insulation, detection of cracks in composite materials, and imaging and detection
of nonmetal and metal objects such as landmines.

The capacitive sensors to be described are designed to provide measurements on a single
side of a material. Electrodes are located in a single plane so that the fringing electric fields
couple to the test material. In one implementation, the electrodes consist of spatially periodic
interdigitated drive and sense electrodes. Since the electric field satisfies Laplace's equation, the
spatial periodicity of the electrode structure or wavelength controls the penetration depth of the
field into the test material and it is possible to generate a profile of the material properties as a
function of depth at a given input frequency. This can be realized with multiple sets of such
interdigitated structures by varying the spatial periodicity of the electrode structure or with novel
electrode structures that provide multiple spatial wavelengths over a fixed sensor footprint. This
approach allows for spatial profile measurements of dispersive media, where the electrical
properties vary with the excitation field frequency and intensity. AISO, arrays of capacitive
sensors can provide quantitative two dimensional imaging of low conductivity materials.
The grid measurement methods to be described provide a real time solution to the inverse
problem relating the material properties to the sensor impedance. These grid measurement
methods use a database of sensor responses to map the measured signals into the desired
properties for the material. The database is derived, prior to the data acquisition, using a
'forward model' of the sensor response based on either a continuum model or a finite element
model for the sensor and the specific problem of interest. The measurement grids can be
visualized as grids that relate measured parameters, such as the magnitude and phase of the
impedance, to the unknown parameters, such as the permittivity and thickness of a dielectric
layer.

Measurements of Moisture Diffusion Dynamics in Transformer Insulation Using
Interdigital Dielectrometry Measurements

Y. Du, S. H. Kang, A. V. Mamishev, B. C. Lesieutre, and M. Zahn
Massachusetts Institute of Technology
Cambridge, MA 02139

The moisture diffusion process in oil free transformer pressboard is monitored using an
interdigital dielectrometry three wavelength sensor in a specially constructed bench top
apparatus. Experiments are performed for five different temperatures at various moisture levels.
The time evolution of the moisture spatial profile in transformer pressboard is non destructively
estimated. Experimental results have a good agreement with theoretical analysis of the moisture
diffusion equation on the effects of pressboard thickness and temperature on the diffusion
process.

The diffusion coefficient for oil free pressboard as a function of temperature and moisture
concentration is estimated. Numerical methods of solving the non linear diffusion equation are
developed. Literature results of the diffusion coefficient for cellulose insulation are compared
and analyzed.

The interdigital sensor setup is also combined in a transformer oil Couette Facility that
simulates the transformer environment for studying temperature and moisture transients in
pressboard. The understanding of moisture related processes in power transformers can be
enhanced with this methodology.

Forward and Inverse Parameter Estimation Algorithms of Interdigital Dielectrometry Sensors

B.C. Lesieutre, A.V. Mamishev, Y. Du, E. Keskiner,
G.C. Verghese, and M. Zahn
Massachusetts Institute of Technology
Cambridge, MA 02139

In this paper we extend the continuum model for interdigital dielectrometry sensors and
propose a new, direct technique for estimating material electrical properties from measurements.
Interdigital sensors consist of alternating parts of long, thin electrodes on a plane. An ideal
model assumes that the periodic structure extends to infinity and the electrodes have no
thickness. We extend the ideal analysis to account for the physical thickness of the electrodes.
We also present the model in a matrix form which is amenable to linear algebraic analysis
techniques. In particular, the "inverse problem" of estimating material properties is formulated as
a generalized eigenvalue problem, which avoids the convergence problems of previously used
iterative algorithms.

Applied Electrostatics

lon Beam Contouring to Generate Sub Millimeter Optics

Thomas G. Bifano, Mark N. Horenstein, Mike Feinberg, Prahsant Shanbhag
Boston University
110 Cummington Street, Boston, MA 02215
Phone: 617 353 5619, Fax: 617 353~659, Pager: 888 377~801
email: bifano@bu.edu

An ion beam microcontouring process has been developed for figuring sub millimeter
diameter optics, characterized by aperture diameters less than 1 um and precision of tens of
nanometers or better. A novel technique was developed to create such optical contours on
suitable optical materials by etching with a narrow ion beam that is rastered across a substrate.
Control of the time history of the rastering can be employed to generate complex aspherical
shapes. The physical setup and procedure are described, as is the mathematical contouring
algorithm and a number of simulations and empirical results.

The algorithm involves a deconvolution process in which the desired removal contour and
ion beam profiles are synthesized as wavelet expansions. The ion beam trajectory is then
computed using a wavelet deconvolution. The ion machining process is to be carried out by
focussed beam sputtering. This involves a 100 um diameter focused ion beam created by a
duoplasmatron ion source. The beam is directed to the target using two orthogonal pairs of
electrostatic plates controlled by a computer guidance system. The ion machining apparatus
comprises an ion source, a positionable sample stage and gauging devices to monitor the
conditions of the chamber and the beam.

Complex three dimensional shapes were machined in single crystal silicon and in nickel.
Results characterizing ion beam behavior, system performance and contouring results are
presented.

A Micro Scale Electric lnduction Machine for a Micro Gas Turbine
Generator

Steven F. Nagle and Jefferey H. Lang
Room 10 007, EECS Department
Massachusetts Institute of Technology
Cambridge, MA 02139

This paper describes a micro scale electric induction machine that is designed to serve as
the starter and generator in a micro gas turbine generator. Its development is part of the MIT
Micro Gas Turbine Generator project, which has the ambitious goal of using MEMS fabrication
technologies to construct compact electric power systems from a gas turbine generator
comprising a compressor, combustor, turbine and electric generator. This system could exhibit a
power density 20 30 times more powerful than the most powerful Lithium batteries today,
based on the energy density of hydrocarbon fuel sources [Epstein et al., 1997]. It is possible
that the technology could be used to create compact, portable power supplies.

This research has been aided by several previous research efforts concerning micro motors.
Various types of micro motors have been given a great deal of attention in the past ten years
[Tai, 1989; Lober and Howe, 1988; Bart, 1988; Mehregany, 1990]; and several types of
variable capacitance micro motors have been fabricated and tested extensively at MIT
[Mehregany et al., 1990; Bart et al., 1992; Tavrow et al, 1992]. We have considered all
possible electric motor arrangements and chosen an electric induction machine, as shown in
Figure I . At the outset, magnetic machines were ruled out due to issues of incompatibility with
their fabrication processes. Also, permanent electret machines were
ruled out for lack of a suitable material. And any machine which would require contact to the
rotor was ruled because of fabrication and friction concerns. Only electric induction and
variable capacitance remained; and variable capacitance was ruled out because of poor
performance and a more difficult fabrication sequence. Like their variable capacitance counter
parts, electric induction micro motors have been studied in the past [Bart and Lang, 1989];
however the research was meant only as a detailed introduction to the subject. Our efforts to
date have treated the analysis and design of electric induction machines from the ground up. The
goal of this research has been to develop an electric induction machine exhibiting the highest
possible power density, with the highest efficiency possible, within the severe design constraints
of its CMOSMEMS fabrication process and within the confines of its host turbomachinery.

Production of Ions and Nanoparticles from Taylor Cone Jets of
Highly Conducting Organic Electrolytes

J. Fernandez de la Mora and M. Gamero Castano
Mechanical Engineering Department
Yale University
New Haven, CT06520 8286, USA
delamora @torus.eng.yale.edu

Following the early studies by Zeleny [1] and Taylor [2] on electrified liquid cones, their
richness of regimes was greatly clarified by Cloupeau and Prunet Foch, who introduced the
more precise term 'conejet' [3, 4]. Research on the subject received a formidable stimulus after
Fenn's discovery of multiply charged species in electrospray ionization mass spectrometry [5].
In the following decade, a number of articles have investigated the scaling laws determining the
diameter [6 10] and charge [11] carried by the drops formed after breakup of these conejets.
Although a number of subtle disagreements remain, there is an approximate consensus on the
nature of these laws in the limit of liquids with electrical conductivities K above 10S/m, which
tend to produce micron or submicron jets. This is the most interesting range for many
application, since no alternative process able to atomize a liquid into such small drops is known.
In this limit, the jet current l is essentially independent of liquid viscosity and meniscus voltage
(within the finite voltage range where the conejet is stable), depending only on the flow rate Q of
liquid pushed through the jet as well as three physical properties of the liquid: its surface tension
coefficient y, electrical conductivity K, and dielectric constant.

Control of Foodborne Pathogenic
Microorganisms Using Electric
Discharge Generated Ozone
Enhanced by Ultraviolet Photon

S. Edward Law and Michael E. Diaz
Department of Biological and Agricultural Engineering
Driftmier Engineering Center
University of Georgia
Athens, GA 30602 4435, USA
Email: edlaw@bae.uga.edu

A fundamental need of all societies worldwide is an adequate and safe source of food.
Consumer conf~dence in food safety has become of paramount importance, while at the same
time to remain competitive and environmentally sound, the US food processing industry must
conserve input resources and more effectively treat process wastewaters. Over the past ~8
years the use of chlorine based treatment of certain process waters has raised concerns
regarding inadvertent formation of carcinogenic chlorinated hydrocarbon compounds (e. g.,
trihalomethanes) in the water. Consequently, major water users such as the pulp and paper
industry are relying less on chlorination and are phasing in alternative treatments—principally
ozonation

Lumped Element Model for
Computing the Equilibrium
Charge Distribution Along a
Moving Web

Mark N. Horenstein
Dept. of Electrical and Computer Engineering
Boston University
8 Saint Mary's St.
Boston, MA 02215 USA
Ph: 617 353 9052 Fax: 617 353 6440 email: mnh@bu.edu

A lumped element model has been used to explain charge conduction and convection in
stationary and moving web systems. Incremental sectors of the web are assigned conductance
and their individual potentials are computed. Ordinary circuit equations are used to determine
the evolution of the charge distribution. Results compare favorably with the analytical solutions
of other authors.

Electrostatics plays an important role in the processing of textiles, polymers, plastics, and
other insulators. Large sheets of these materials are commonly called "webs." When a thin web
of insulating material is drawn over metal rollers or similar guiding structures, contact
electrification can cause excess charge to build up, leading to arcing, electrostatic discharge
(ESD), unwanted electrostatic forces, or undesirable dust precipitation. The electrostatics of a
moving web system is a dynamic problem affected by surface conductivity, surface layer
capacitance, geometry, and material motion. An analysis method that predicts the charge distribution and
surface potential on a moving web can be a valuable tool when designing web based
manufacturing systems, but direct mathematical analysis becomes difficult in the complex
geometries found in many practical industrial situations. This paper describes an analysis method
based on a discretized, lumped element representation of moving webs. Charge conduction is
modeled using fixed value resistors, and charge convection is modeled by direct material
transport over time. The analysis method can be applied to a wide variety of geometries and
industrial situations and provides physical insight into the fundamental electrostatic processes at
work in moving web systems. It also should be useful in predicting the behavior of web systems
in which surface conductivity is non ohmic (i. e., nonlinear.)

Relating Roller Shaft \/oltages to
Tribocharging During Sheet
Transport

Humphrey Wong
Surface Modification ar1d Electrostatics Unit, MR&E, IMMPC
Eastman Kodak Company
Rochester, NY 14652

Printers often employ pinch rollers in order to convey sheets of material from storage
cassettes, through a printing operation, and sometimes through a development station before
finally depositing the sheets into a receiving area. Transport of sheets through pairs of pinch
rollers can result in tribocharging both the rollers and the sheets. By monitoring the end shafts of
certain types of pinch rollers with voltmeters, it is possible to relate the voltage vs. time behavior
to the tribocharging taking place during passage of the sheets through the pinch rollers. In this
paper, we will present an interpretation of various voltage signals in terms of the charging and
discharging characteristics of the roller and sheet surfaces.

The Effects of Electric Field Radiated from Electrostatic
Discharge on the Electronic Circuit

Jiu sheng Huang
9th Department
Beijing Research Institute of Special Electromechanical Technologies
No. 1, Bei yuan Da Yan, An Ding Men Wai
Beijing, China, 100012
Tel: 86 1~66749396~5
E mail: jiushuang@263.net

This transient electric field radiated from charged human body discharging to the ground and
from the ESD simulator are studied. Many waveforms and spectrums of the field from the ESD
are analyzed. The effects of the field to typical electronic circuits are studied.

A Theoretical Paradox Related to
Solid Dielectrics that Cannot be
Resolved Even After a Computer
Simulation Using Finite Element Analysis

Andreas Trupp
atrupp@hotmail.com

It is demonstrated that two common methods of determining the mechanical force acting
between two electrified bodies, that is Coulomb's law on the one hand, and the method of
virtual work on the other hand, yield results that differ from each other if dielectrics are involved.

Piezoelectric Effects in Ice

Hasashi Shio
Department of Physics, Hokkaido University, Japan
Fax: 81 11884 6184

Charging mechanisms of ice are generally based on the temperature gradient theory in which
the electric potential is formulated as V = 2~1T (mV), where V is a electric potential difference
between two specimens, and T is the temperature difference between them. If the temperature
difference is 30 •C, the electric potential difference becomes only 60 mV. On the other hand,
when two ice specimens are asymmetrically rubbed together the electric potential difference
reaches to above I V. As a result, it is suggested that the charging mechanism is based on a
different origin from the temperature gradient. In order to research this new origin of the
charging mechanism of ice, the dependence of the charging phenomena of ice on stress of the
specimens is investigated.

A New Unified Method for
Measurement of Electrical
Resistivity of Textile Assemblies

Pellumb G. Berberi
Department of Physics
Polytechnic University of Tirana
Tirana, Albania

A new multiple step method for measuring electrical resistivity of textile assemblies is
proposed that takes compressional properties of the assembly into consideration. A new
parameter is introduced to describe electrical resistivity of textile materials as the limit resistivity
of a compressed fiber assembly. This new definition approaches the measured resistance of the
textile assembly as something similar to the volume resistivity of a rigid homogeneous material.
Experiments carried out with different kinds of fiber assemblies clearly show that the electrical
resistivity so defined is an inherent characteristic reflecting the. and is independent of sample form
(fabric, yarn, fiber).electrical properties of fiber material.

A Method to Estimate the Area of Contact of a Textile Fabric
with a Rigid Flat Surface

Pellumb G. Berberi, J. Amirbayatt, I. Poratt
Department of Physics
The Polytechnic University of Tirana
Tirana, Albania
TDepartment of Textiles, UMIST
Manchester, UK

The true area of contact of two surfaces is an important parameter to be estimated when electrostatic propensity,
surface resistivity, frictional resistance, or any other property of the surfaces are to be measured [1, 2, 7]. Some
methods for testing of electrostatic properties of textiles as 'decay time,' 'frictional charge' or 'electrical surface
resistance' are known, among others, for their low reproducibility due to the uncontrolled alteration of 'true area of
contact' [3, 6].

Several attempts have been reported by different authors for the estimation of the area of apparent contact
between metal and a flat polymer sheet by measuring the imprint made on the polymer surface by a travelling
microscope [4, 5]. Naturally, this method can not be used to estimate the area of contact of a textile fabric with a flat
rigid surface because of relatively high surface asperities.
To the best of authors' knowledge, there is no work published which describes the objective measurement of
contact area of a textile material with a flat rigid surface.

最近信息   更多>>

最近ESD培训计划
美国第36届ESD 年会

美国EsdEmc公司热烈庆祝EMC2014 6月17-19日在北京国际会议中心召开

 

 

静电产品   更多>>

系统、整机ESD测试

±20kV静电放电发生器

±30kV静电放电发生器

 

电子元器件ESD测试

电子元器件ESD敏感度分类

HBM人体模型ESD模拟

HBM/MM静电放电模拟器 (0~±20kV)(通用)
HBM/MM/CDM静电放电模拟器 (0~±20kV)
CDM静电放电模拟器 (0~±20kV)

 

工厂级ESD测试

离子风机测试仪(±1kV±5kV)

 

静电电压测量类

防爆静电电压表(低价格通用)

静电动态计算机监测(多通道电脑存储)

静电电荷量测量类

数字电荷量仪(推荐 通用型)
数字电荷皮库表(极灵敏型)
数字电量表(低价格)
数字电量表(大电量)

高电阻或超高阻测量类

数字高阻计(低价格)
超高阻微电流测量仪(推荐)
人体综合电阻测试仪
防静电鞋、导电鞋测量仪
导电和防静电材料电阻率测量(宽范围)

微电流或超微弱电流测量类

皮安飞安电流表
数字超高阻、微电流测量仪 推荐

 

静电发生器、高压直流电源

袖珍正负静电发生器

EST801静电发生器(0 ~ +8kV)
静电发生器 (0-20kV)
价格静电发生器(0 ~80kV)
大电流静电发生器(5mA以上)
高精度静电发生器(EST705)

双极性高精度电发生器(0~±20kV、±30kV、±50kV)

 

 

 

静电应用   更多>>

静电吸纸覆纸设备
节能环保型静电分选机
静电放电棒

人体静电表演装置

静电放电(ESD)发生器(模拟器、放电枪)校对装置

静电电压表计量装置
多通道大气静电场强测试仪

静电吸附  静电分选

 

劳保世界>>

 

技术支持与服务

国际认证ESD工程师来了,您准备好了吗?

美国、日本ESD专家授课,高水平ESD培训课程。

您能理解和区分两个最常用ESD标志吗?

导电、防静电塑料、橡胶体积电阻率测试 EST991

定做特殊专用静电产品

培训&认证  更多>>

ESD-china 课程特点IEC61340-5-1静电防护体系认证咨询培训辅导
高水平授课方式的ESD培训ANSI/ESD S20.20认证咨询

充分理解S20.20标准的要求

AC电阻测试

认证咨询辅导的有关问题 FAQ

往期培训回顾

 

ESD-china优

 

联系我们更多>>

 

业务电话:

010-⑥③⑤②,⑧②⑤④

010-⑥③⑤②,⑧②⑥④

010-
⑥③⑤①,②⑥⑦⑧

北京时间:周一至周五:
8:30~12:00, 13:30~17:30

传真1:⑥③⑤②,④⑦⑨⑧

传真2:⑥③⑤①,②⑥⑦⑧
 

投诉与建议:010-6358.0337

销售咨询1:产品销售咨询

销售咨询2:产品销售咨询

技术咨询产品技术咨询


   

 

静电驻极,过滤效率不到20提升到95

静电驻极中如何注入更多的电荷,从而提高熔喷布的过滤效率?

 

EST712C静电驻极N95口罩布熔喷布无纺布静电驻极机静电驻极棒 (高效、易安装)

静电驻极N95口罩布熔喷布无纺布静电驻极机静电驻极棒

无锡常州客户使用EST712C静电驻极机的使用效果

ESD-china静电信息网   亿艾迪(ESD)(产品)  华晶汇(HJH)(技术)  主要客户  汇款帐号
联系我们010-6358.0337  6352.8264,  6352.8254   6351.2678  (周一至周五:8:30-12:00, 13:30-17:30)
 业务联系::产品销售咨询       :产品销售咨询     技术支持:产品技术咨询
地址:北京市西城区亚泰中心,传真1:⑥③⑤②.④⑦⑨⑧,  传真2:⑥③⑤①,②⑥⑦⑧ 
  最近更新:2020-05-29 有问必答电子邮  版权所有©复制必究1997-2019
 
关于或联系我们:email:   About ESD-china  网站地图