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Page "Video camera tube" ¶ 15
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electron and image
Transmission secondary electron multiplication image intensifiers ( TSEM tubes ), ( E )
The electron beam could be swept across the screen much faster than any mechanical disc system, allowing for more closely spaced scan lines and much higher image resolution, while slow-fade phosphors removed image flicker effects.
Whilst providing a projected image, the technique has limited resolution ( 2-2. 5 nm ), due to both quantum mechanical effects and lateral variation in electron velocity.
A scanning electron microscope ( SEM ) image of a normal red blood cell, a platelet, and a white blood cell.
A transmission electron microscopy image of a single-walled carbon nanotube
A scanning electron microscopy image of carbon nanotubes bundles
Transmission electron microscopy | TEM image of a chloroplast
These capacitors are biased above the threshold for inversion when image acquisition begins, allowing the conversion of incoming photons into electron charges at the semiconductor-oxide interface ; the CCD is then used to read out these charges.
Transmission electron microscopy | TEM image of collagen fibres.
By recording these changes in the electron beam, microscopists can produce atomically resolved image of the material.
In scanning electron microscopes, the image is produced by rastering a finely focused electron beam, as in a TV set, across the studied sample.
An electron microscope uses a beam of electrons to illuminate a specimen and produce a magnified image.
The electron microscope uses electrostatic and electromagnetic " lenses " to control the electron beam and focus it to form an image.
Modern electron microscopes produce electron micrographs, using specialised digital cameras or frame grabbers to capture the image.
The original form of electron microscope, the transmission electron microscope ( TEM ) uses a high voltage electron beam to create an image.
The spatial variation in this information ( the " image ") may be viewed by projecting the magnified electron image onto a fluorescent viewing screen coated with a phosphor or scintillator material such as zinc sulfide.
Alternatively, the image can be photographically recorded by exposing a photographic film or plate directly to the electron beam, or a high-resolution phosphor may be coupled by means of a lens optical system or a fibre optic light-guide to the sensor of a CCD ( charge-coupled device ) camera.
An image of an ant in a scanning electron microscope

electron and is
Af is paramagnetic, and electron paramagnetic dipole as well as nuclear dipole effects lead to line broadening.
Indeed it is possible to separate electron paramagnetic from nuclear effects.
The information provided by the electron paramagnetic effects is then discussed, and finally the nuclear effects are interpreted in terms of various motional-modified models of the Af bond in Af.
The approximate equation is Af, where N is the number of Af with electron line-density greater than or equal to Af, and Q is proportional to the mass of the meteorite.
Radiopasteurization by either the electron accelerator or cesium-137 source is in the range of freezing costs.
Irradiation using the nuclide source is more expensive than use of an electron accelerator.
It should be noted, however, that the paraxial resolution is quite similar for both electron optical systems.
The electron optical system ( see fig. 14-1 ) is based in principle on the focusing action of concentric spherical cathode and anode surfaces.
The charges of the electron and proton are believed to be exactly equal and opposite, but Dr. Lyttleton is not so sure.
Suppose, says Dr. Lyttleton, the proton has a slightly greater charge than the electron ( so slight it is presently immeasurable ).
A Lewis acid is a species that accepts a pair of electrons from another species ; in other words, it is an electron pair acceptor.
BF < sub > 3 </ sub > is a Lewis acid because it accepts the electron pair from fluoride.
The species that gains the electron pair is the Lewis acid ; for example, the oxygen atom in H < sub > 3 </ sub > O < sup >+</ sup > gains a pair of electrons when one of the H — O bonds is broken and the electrons shared in the bond become localized on oxygen.
The number of electrons in each element's electron shells, particularly the outermost valence shell, is the primary factor in determining its chemical bonding behavior.
An atom containing an equal number of protons and electrons is electrically neutral, otherwise it has a positive charge if there are fewer electrons ( electron deficiency ) or negative charge if there are more electrons ( electron excess ).
Over 99. 94 % of an atom's mass is concentrated in the nucleus ,< ref group = note > In the case of hydrogen-1, with a single electron and nucleon, the proton is, or 99. 95 % of the total atomic mass.
Thus, the planetary model of the atom was discarded in favor of one that described atomic orbital zones around the nucleus where a given electron is most likely to be observed.
The electron is by far the least massive of these particles at, with a negative electrical charge and a size that is too small to be measured using available techniques.

electron and periodically
An electron beam periodically sweeps across the plate, effectively scanning the stored image and discharging each capacitor in turn such that the electrical output from each capacitor is proportional to the average intensity of the light striking it between each discharge event.
Finally, an electron beam periodically sweeps across the target, effectively scanning the stored image, discharging each granule, and producing an electronic signal like in the iconoscope.
Finally, an electron beam periodically sweeps across the target, effectively scanning the stored image and discharging each capacitor in turn such that the electrical output from each capacitor is proportional to the average intensity of the scene light between each discharge event ( as in the iconoscope ).
* Madey, John, Stimulated emission of radiation in periodically deflected electron beam, US Patent 38 22 410, 1974
Electrostatic deflecting plates or magnetic fields then periodically manipulate the resulting electron image horizontally and vertically before an electron multiplier, or a small aperture leading to a positively-charged detector or " anode " in the case of the earliest dissector tubes.

0.734 seconds.