Encyclopedia of Renewable Energy. James G. Speight

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0.743 Trans-2-butene -106 1 Isobutylene -141 -7 Cis-2-pentene -151 37 2-Methyl-2-butene -123 39 0.655 2,3-Dimethyl-2-butene -74 73 0.660 Cyclopentene -93 46 0.705 Cyclohexene -104 83 0.774 1,3-Cyclopentadiene -85 42 0.810 1,3-Cyclohexadiene -49 87 0.798 0.847

      Alkenes serve as a feedstock for the petrochemical industry because they can participate in a wide variety of reactions.

      The simplest acyclic alkenes, with only one double bond and no other functional groups, form a homologous series of hydrocarbons with the general formula CnH2n.

      The physical properties of alkene derivatives are comparable with those of alkane derivatives (aliphatic hydrocarbon derivatives). The physical state depends on molecular mass (gases from ethylene to butene and liquids from pentene onwards). The simplest alkenes, ethylene, propylene (propene), and butylene (butene) are gases. Linear alkenes of approximately 5 to 16 carbons are liquids, and higher molecular weight alkenes are waxy solids.

      Alkene derivatives are more reactive than alkane derivatives due to the presence of a carbon-carbon pi-bond (double bond). The majority of the reactions of alkenes involve the rupture of this pi bond, forming new single bonds.

      Alpha decay (α-decay) is the radioactive emission of an α-particle which is the nucleus of helium-4 (4He), consisting of two protons and two neutrons which is a stable nucleus as it is doubly magic. The daughter nucleus has two protons and four nucleons fewer than the parent nucleus. In general, alpha decay leads to the ground state of the daughter nucleus so that the emitted particle carries away as much energy as possible.

      By way of definition, a nucleon is either a proton or a neutron considered in its role as a component of an atomic nucleus. The number of nucleons in a nucleus defines the mass number (the nucleon number) of an isotope. In fact, protons and neutrons are best known in their role as nucleons, i.e., as the components of atomic nuclei, but they also exist as free particles. Free neutrons are unstable, with a half-life of approximately 13 minutes, but they have important applications. Protons not bound to other nucleons are the nuclei of hydrogen atoms when bound with an electron or – if not bound to anything – are ions or cosmic rays. Both the proton and the neutron are composite particles insofar as each is composed of smaller parts and, thus, neither the proton nor the neutron is an elementary particle.

      A pertinent example from the area of nuclear energy is the decay of uranium-238 (238U) to thorium-234 (234Th). An alpha particle (also called alpha rays or alpha radiation) has a charge of +2e, but, as a nuclear equation, describes a nuclear reaction without considering the electrons and consists of two protons and two neutrons bound together into a particle identical to a helium-4 (4He) nucleus and are typically the product of the alpha decay process. The symbol for the alpha particle is α or α2+, and because alpha particles are identical to helium nuclei, they are also sometimes written as He2+ or 42He2+ which indicates a helium ion with a +2 charge (missing two electrons). Once the ion gains electrons from its environment, the alpha particle becomes a normal (electrically neutral) helium atom 42He.

      Alpha decay typically occurs in the heaviest nuclides, and, theoretically, it can occur only in nuclei somewhat heavier (higher atomic number) than nickel atomic (number = element 28), where the overall binding energy per nucleon is no longer a minimum and the nuclides are therefore unstable toward spontaneous fission-type processes. In practice, this mode of decay has only been observed in nuclides considerably heavier than nickel, with the lightest known alpha emitters being the lightest isotopes (mass numbers 104 to 109) of tellurium (atomic number = element 52).

      When an atom emits an alpha particle in alpha decay, the mass number of the atom decreases by four due to the loss of the four nucleons in the alpha particle. The atomic number of the atom decreases by two, as a result of the loss of two protons, and the atom becomes a new element. Also, unlike other types of decay, alpha decay as a process must have a minimum-size atomic nucleus that can support it. The process may leave the nucleus in an excited state after which the emission of a gamma ray then removes the excess energy.

      See also: Beta Decay, Gamma Decay, Nuclear Energy.

      Alpha Particle

      An alpha particle (also termed alpha radiation or alpha rays) is a helium nucleus stripped of its orbital electrons and which is emitted from a radioactive atom with a velocity of about 1/20 that of the speed of light and with energies ranging from 4 to 9 MeV. The alpha particle was the first nuclear radiation to be discovered; beta particles and gamma rays were identified soon thereafter.

      Alpha particles cause ionizations in matter when they are deflected by the positive charge of a nucleus and pull the orbital electrons (attracted by the alpha’s positive charge) along with them. Alpha particles also cause excitation along their path by pulling inner orbital electrons to outer orbits. Energy is then given off by the atom as fluorescent radiation (low energy x-rays) when the electrons drop back down to the inner orbital vacancies.

      Because of its relatively large mass (2 neutrons and 2 protons), high electrical charge (2+) and low velocity, the specific ionization of an alpha particle is high and, as a result, it creates many ion pairs in a very short path length. Because of this, it loses all of its energy in a short distance. The range in air is only several centimeters even for the most energetic alpha particles.

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