Electrons flow from the negative terminal of the power supply up the negative rail, across the projectile, and down the positive rail, back to the power supply.

Electrons will move to the left side ( uncovering positive ions on the right side ) until they cancel the field inside the metal.

Electrons can only reach ( and " illuminate ") a given plate element if both the grid and the plate are at a positive potential with respect to the cathode.

Electrons flow through that digit's grid and strike those plates that are at a positive potential.

Electrons ( negative charges ) and holes ( positive charges ) both contribute to the induced thermoelectric voltage thus canceling each other's contribution to that voltage and making it small.

: Electrons are repelled from the negative electrode while positive ions are drawn towards it.

Electrons are reflected from the outside surface of the sheath while all positive ions which reach the sheath are attracted to the electrode.

Electrons in the conduction band can respond to the electric field in the detector, and therefore move to the positive contact that is creating the electrical field.

Electrons are the charge carriers in metals and they follow an erratic path, bouncing from atom to atom, but generally drifting in the opposite direction of the electric field.

Electrons in the emitters, or the " holes " in the collectors, would cluster at the surface of the crystal where they could find their opposite charge " floating around " in the air ( or water ).

Electrons within the conduction band are mobile charge carriers in solids, responsible for conduction of electric currents in metals and other good electrical conductors.

For instance, " Electrons attract protons " and " Electrons have negative charge " employ the terms " protons " and " negative charge " ( with the latter also implicitly using the concept of " charge ").

Electrons ( things that have P1 ) have charge ( P2 ).

Electrons and holes are the charge carriers in semiconductors.

Electrons from the metal are used to bond to the ligand, in the process relieving the metal of excess negative charge.

Electrons were ideal for the role, as they are abundant and easily accelerated to high energies due to their electric charge.

Electrons which diffuse from the cathode into the P-doped layer, or anode, become what is termed " minority carriers " and tend to recombine there with the majority carriers, which are holes, on a timescale characteristic of the material which is the p-type minority carrier lifetime.

They ’ ll carry it with them in their future life …. And this future life in the body of eons will be very long, almost as long as the Universe itself .” Suggests Charon, “ the electrons which form my body are not only carriers of what I call ‘ my ’ spirit, but, in fact constitute my spirit itself .” Electrons are sent individually into the Universe to learn and to increase the order of the Universe ; “ the psychic level of the whole Universe progressively elevates itself … during the ‘ successively lived experiences ’ of elemental matter .” The goal of each electron is to increase its energy to the highest level of sustainable excitement ; that is, to contain the most information within the largest stable system of organization possible.

These he interpreted as " negative-energy electrons " and attempted to identify them with protons in his 1930 paper A Theory of Electrons and Protons However, these " negative-energy electrons " turned out to be positrons, and not protons.

Electrons and how they interact with electromagnetic fields are important in our understanding of chemistry and physics.

Electrons are fermions with S = 1 / 2 ; quanta of light are bosons with S = 1.

Electrons and how they interact with electromagnetic fields are important in our understanding of chemistry and physics.

Electrons from ionized atoms interact mainly with neutral atoms, causing thermal bremsstrahlung radiation.

Electrons can be exchanged between materials on contact ; materials with weakly bound electrons tend to lose them, while materials with sparsely filled outer shells tend to gain them.

Electrons in this system are not conserved, but are rather continually entering from oxidized 2H < sub > 2 </ sub > O ( O < sub > 2 </ sub > + 4 H < sup >+</ sup > + 4 e < sup >-</ sup >) and exiting with NADP < sup >+</ sup > when it is finally reduced to NADPH.

* Bhees: Beams of High Energy Electrons, these are beams of focused and accelerated electrons with considerable penetrating power.

This project was continued with the launch of From Electrons to Elections, a science and technology policy guide to the 2008 elections.

From Electrons to Elections is a non-partisan resource designed to educate young voters on science, technology, and health issues and provide them with the platforms of the leading political candidates on these subjects.

Electrons in non-bonding orbitals tend to be in deep orbitals ( nearly atomic orbitals ) associated almost entirely with one nucleus or the other, and thus they spend equal time between and not between nuclei.

Electrons are delocalized along the conjugated backbones of conducting polymers, usually through overlap of π-orbitals, resulting in an extended π-system with a filled valence band.

Electrons from the cathode collide with the anode material, usually tungsten, molybdenum or copper, and accelerate other electrons, ions and nuclei within the anode material.

* Gover, " Collective and Single Electron Interactions of Electron Beams with Electromagnetic Waves and Free Electrons Lasers ".

Electrons for the reduction of nitrogen are supplied to nitrogenase when it associates with the reduced, nucleotide-bound homodimeric Fe protein.

In 1936, the two published a paper, " The Passage of Fast Electrons and the Theory of Cosmic Showers " in the Proceedings of the Royal Society, Series A, in which they used their theory to describe how primary cosmic rays from outer space interact with the upper atmosphere to produce particles observed at the ground level.

* Brode, R. B., The Quantitative Study of the Collisions of Electrons with Atoms, Rev.

Electrons can be used in these situations, whereas X-rays cannot, because electrons interact more strongly with atoms than X-rays do.

Electrons will be accelerated in the opposite direction to the electric field by the average electric field at their location.

Electrons scatter from all of these, resulting in resistance to their flow.

Electrons in the closer orbitals experience greater forces of electrostatic attraction ; thus, their removal requires increasingly more energy.

Electrons do not penetrate as deeply into matter as X-rays, hence electron diffraction reveals structure near the surface ; neutrons do penetrate easily and have an advantage that they possess an intrinsic magnetic moment that causes them to interact differently with atoms having different alignments of their magnetic moments.

Electrons also have a long ballistic length at this temperature ; their mean free path can be several micrometres.

Electrons appear as a track in the inner detector and deposit all their energy in the electromagnetic calorimeter.

Electrons in such orbitals are strongly localized and therefore easily retain their magnetic moments and function as paramagnetic centers.

# Electrons ( negatively charged ) are knocked loose from their atoms, causing an electric potential difference.