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Posts tagged 'electrons'

Potential Difference

by @ Friday, April 18th, 2008. Filed under Electrical Science

Potential Difference Potential difference is the term used to describe how large the electrostatic force is between two charged objects. If a charged body is placed between two objects with a potential difference, the charged body will try to move in one direction, depending upon the polarity of the object. If an electron is placed [...]

Electrostatic Forces

by @ Friday, April 18th, 2008. Filed under Electrical Science

Electrostatic Forces  One of the mysteries of the atom is that the electron and the nucleus attract each other. This attraction is called electrostatic force, the force that holds the electron in orbit. This force may be illustrated with lines as shown in Figure 3. Without this electrostatic force, the electron, which is traveling at [...]

The Atom

by @ Friday, April 11th, 2008. Filed under Electrical Science

The Atom Elements are the basic building blocks of all matter. The atom is the smallest particle to which an element can be reduced while still keeping the properties of that element. An atom consists of a positively charged nucleus surrounded by negatively charged electrons, so that the atom as a whole is electrically neutral. [...]

RADIATION TYPES – Gamma Ray

by @ Monday, November 19th, 2007. Filed under Instrumentation and Control

Gamma Ray The gamma ray is a photon of electromagnetic radiation with a very short wavelength and high energy. It is emitted from an unstable atomic nucleus and has high penetrating power. There are three methods of attenuating (reducing the energy level of) gamma-rays: photoelectric effect, compton scattering, and pair production. The photoelectric effect occurs [...]

RADIATION TYPES – Alpha Particle

by @ Monday, November 19th, 2007. Filed under Instrumentation and Control

Alpha Particle The alpha particle is a helium nucleus produced from the radioactive decay of heavy metals and some nuclear reactions. Alpha decay often occurs among nuclei that have a favorable neutron/proton ratio, but contain too many nucleons for stability. The alpha particle is a massive particle consisting of an assembly of two protons and [...]

GAS-FILLED DETECTOR

by @ Monday, November 19th, 2007. Filed under Instrumentation and Control

The pulsed operation of the gas-filled detector illustrates the principles of basic radiation detection. Gases are used in radiation detectors since their ionized particles can travel more freely than those of a liquid or a solid. Typical gases used in detectors are argon and helium, although boron-triflouride is utilized when the detector is to be [...]

PROPORTIONAL COUNTER

by @ Monday, November 19th, 2007. Filed under Instrumentation and Control

A proportional counter is a detector which operates in the proportional region, as shown in Figure 6. Figure 7 illustrates a simplified proportional counter circuit. To be able to detect a single particle, the number of ions produced must be increased. As voltage is increased into the proportional region, the primary ions acquire enough energy [...]

PROPORTIONAL COUNTER CIRCUITRY

by @ Monday, November 19th, 2007. Filed under Instrumentation and Control

Proportional counters measure the charge produced by each particle of radiation. To make full use of the counter’s capabilities, it is necessary to measure the number of pulses and the charge in each pulse. Figure 9 shows a typical circuit used to make such measurements. The capacitor converts the charge pulse to a voltage pulse. [...]

IONIZATION CHAMBER

by @ Monday, November 19th, 2007. Filed under Instrumentation and Control

Ionization chambers are electrical devices that detect radiation when the voltage is adjusted so that the conditions correspond to the ionization region (refer to Region II of Figure 6). The charge obtained is the result of collecting the ions produced by radiation. This charge will depend on the type of radiation being detected. Ionization chambers [...]

GEIGER-MÜLLER DETECTOR

by @ Sunday, November 18th, 2007. Filed under Instrumentation and Control

The Geiger-Müller or G-M detector is a radiation detector that operates in Region V, or G-M region, as shown on Figure 23. G-M detectors produce larger pulses than other types of detectors. However, discrimination is not possible, since the pulse height is independent of the type of radiation. Counting systems that use G-M detectors are [...]

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