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Isotopes neutron number

Isotope mass number Abundance, % Thermal neutron cross Contribution to the total cross ... [Pg.439]

Fig. 8. A curve of proton number Z as a function of neutron number N, calculated as described in the text. The horizontal lines show the ranges of stablg isotopes for alternate Z-even elements (for large Z the four most stable isotopes). Fig. 8. A curve of proton number Z as a function of neutron number N, calculated as described in the text. The horizontal lines show the ranges of stablg isotopes for alternate Z-even elements (for large Z the four most stable isotopes).
Note The nucleus of each element may have more than one neutron/proton ratio (different isotopes) in the table are presented the most abundant stable isotopes of some elements and the number before their symbols represents very approximately the mass of that isotope (mass number, A). [Pg.38]

All elements, by definition, have a unique proton number, but some also have a unique number of neutrons (at least, in naturally occurring forms) and therefore a unique atomic weight - examples are gold (Au Z = 79, N = 118, giving A =197), bismuth (Bi Z = 83, N = 126, A = 209), and at the lighter end of the scale, fluorine (F Z = 9, N = 10, A = 19) and sodium (Na Z = 11, N= 12, A = 23). Such behavior is, however, rare in the periodic table, where the vast majority of natural stable elements can exist with two or more different neutron numbers in their nucleus. These are termed isotopes. Isotopes of the same element have the same number of protons in their nucleus (and hence orbital electrons, and hence chemical properties), but... [Pg.231]

Figure 10.2 The radioactive stability of the elements. The x axis is proton number (up to Z = 83, bismuth), the y axis the neutron number (N). Stable isotopes are shown in black and radioactive isotopes in grey, indicating the relative excess of radioactive isotopes over stable isotopes in nature, and the fact that as proton number increases, the neutron number has to increase faster to maintain stability. The basic data for this figure are given in Appendix VI. Figure 10.2 The radioactive stability of the elements. The x axis is proton number (up to Z = 83, bismuth), the y axis the neutron number (N). Stable isotopes are shown in black and radioactive isotopes in grey, indicating the relative excess of radioactive isotopes over stable isotopes in nature, and the fact that as proton number increases, the neutron number has to increase faster to maintain stability. The basic data for this figure are given in Appendix VI.
In this chapter, we introduced the constituents and structure of the atom and showed that elements typically have several isotopes (same number of protons but different numbers of neutrons). Using the Chart of the Nuclides, we briefly discussed the distribution and stability of the isotopes. Radioactive isotopes were introduced, and we mentioned that they can be used for dating of geological and cosmochemical events. We then discussed the periodic... [Pg.51]

Electron, Atom, Atomic Number, Atomic Weight, Electronic Shell, Element, Ion, Isotope, Mass Number, Molecule, Neutron, Proton and Valence. [Pg.714]

Electron, atom, atomic number, atomic wt, electronic shell, element, ion, isotope, mass number, molecule, neutron, proton and valence 5 E71-E72... [Pg.596]

Not all of the atoms in a sample of chlorine, for example, will be identical. Some atoms of the same element can contain different numbers of neutrons and so have different nucleon numbers. Atoms of the same element which have the same proton number but different neutron numbers are called isotopes. The two isotopes of chlorine are shown in Figure 3.4 (p. 36). [Pg.46]

Table 2.1 Isotopes of arsenic (Audi et al., 2003 Holden, 2007 Lindstrom, Blaauw and Fleming, 2003).15As is the only stable arsenic isotope. The possible decay modes include electron capture (EC), electron emission (P ), positron emission (P+), proton decay (p), internal transition (IT), and neutron emission (ne). Superscripts on some of the arsenic isotope mass numbers designate excited-state isomers. The first (lowest energy) excited state is designated with an m and a second excited state is designated with an n. ... Table 2.1 Isotopes of arsenic (Audi et al., 2003 Holden, 2007 Lindstrom, Blaauw and Fleming, 2003).15As is the only stable arsenic isotope. The possible decay modes include electron capture (EC), electron emission (P ), positron emission (P+), proton decay (p), internal transition (IT), and neutron emission (ne). Superscripts on some of the arsenic isotope mass numbers designate excited-state isomers. The first (lowest energy) excited state is designated with an m and a second excited state is designated with an n. ...
The structures of the neutron-rich isotopes 97Y, 98Y and 99Y reflect with special clearness the rapid change of the nuclear shape at neutron number 60. The discovery of a new isomer in 97Y has provided evidence for the shell-model character of this nucleus even at high excitation energies while 99Y shows the properties of a symmetric rotor already in the ground state. The level pattern of the intermediate isotope 98Y indicates shape coexistence. [Pg.206]

Fig. 5. Cranked Shell Model frequency for the proton 1m crossing minus that for the neutron an crossing plotted as a function of neutron number for the Pt isotopes. Fig. 5. Cranked Shell Model frequency for the proton 1m crossing minus that for the neutron an crossing plotted as a function of neutron number for the Pt isotopes.
The experimental work here has shown that the deformation of the isomeric 9/2 states in the light thallium isotopes is increasing with decreasing neutron number while the 1/2 state remains relatively constant. This work shows the fallacy of assuming that a constant moment of inertia infers a constant deformation. Theoretically, this work has demonstrated an interesting aspect of the competition between quadrupole and pairing correlations in near-singly-closed-shell nuclei. [Pg.368]

Chart of nuclei. The stable isotopes are represented by black squares. The known isotopes are indicated in addition to the magic proton and neutron numbers. The smooth lines enclose regions with a nuclear deformation B 0.2. Those isotopes are marked by open bars where optical spectroscopy yielded information on nuclear ground state properties in long isotopic chains. This picture gives the status as of September 1985. [Pg.371]

The IS s of nuclei far from stability turned out to be the most informative data obtained by optical spectroscopy. This is because the nuclear charge radius depends on collective as well as on single-particle effects. The integral IS s (6 with A being a reference isotope) exhibit the gross behaviour of nuclear matter as a function of varying neutron number. These can be compared with predictions of macroscopic models like the Droplet Model [MEY83], which describes the overall trend quite well. [Pg.375]

Many well-deformed nuclei have been found in rare earth and actinide regions. In those nuclei the ratio of the excitation energies of the 4+ to the 2+ states E /E2 are almost equal to the rotational limit 10/3. The lowest values of the E2 are about 72 keV and 43 keV, respectively. Can we find such well-deformed nuclei in the region of the proton and neutron numbers ranging from 50 to 82 What the minimum E2 there these questions have not been answered yet because well-deformed nuclei, if any, are too proton-rich and have too poor yields to observe by conventional in-beam spectroscopic methods. The present studies on light isotopes of Sm, Nd and Ce aim at finding a clue to the questions. [Pg.493]

Isotopes have the same atomic number but different neutron numbers. [Pg.389]

Mass number is equal to the proton number plus the neutron number. The average atomic mass appears on the periodic table and is the mass of each naturally occurring isotope of an element weighted by the fractional abundance of the isotope. [Pg.389]

Element abundance data were useful not only in astrophysics and cosmology but also in the attempts to understand the structure of the atomic nucleus. [74] As mentioned, this line of reasoning was adopted by Harkins as early as 1917, of course based on a highly inadequate picture of the nucleus. It was only after 1932, with the discovery of the neutron as a nuclear component, that it was realized that not only is the atomic mass number related to isotopic abundance, but so are the proton and neutron numbers individually. Cosmochemical data played an important part in the development of the shell model, first proposed by Walter Elsasser and Kurt Guggenheimer in 1933-34 but only turned into a precise quantitative theory in the late 1940s. [75] Guggenheimer, a physical chemist, used isotopic abundance data as evidence of closed nuclear shells with nucleon numbers 50 and 82. [Pg.175]

W. Harkins, The constitution and stability of atom nuclei, Philosophical Magazine 42 (1921) 305-339, on 310. See also W. Harkins, Isotopes Their number and classification," Nature 107 (1921) 202-203, which includes what is probably the first diagram of the abundance of isotopes as a function of the atomic number. Like all other physicists at the time, Harkins believed that atomic nuclei consisted of protons and electrons. The number of electrons corresponds to the quantity A-Z, later identified with the neutron number. [Pg.186]

Isotope Number of Protons Number of Neutrons Number of Electrons Mass Number Atomic Number... [Pg.226]

Problem 1.5 By definition, isotopes have the same proton number but a different neutron number. However, Ps and H have a different proton number but the same neutron number (zero). In chemistry, isotopes always have similar chemical reactivities. However, Ps reacts with molecules very differently from H. In physics, although their atomic size is the same, their energy levels are distinctly different from each other. Therefore, it is inappropriate to consider Ps a light isotope of H. It should stay at its own location Period 0 and Group 1, or 1A as proposed in the revised Periodic Table of the Elements as revised and shown in Figure 1.6. Ps has its own new chemistry. [Pg.13]

ISOTOPE SYMBOL NAME PROTONS ELECTRONS NEUTRONS NUMBER... [Pg.25]

I Atomic mass and mass number are not the same. Atomic mass refers to the naturally occurring mixture of isotopes mass number refers to an individual isotope. Atomic mass is an average and is never an exact integer mass number is a sum (of the number of protons plus the number of neutrons) and is always an integer. Except for the artificial elements, mass numbers are not given in the periodic table. [Pg.104]

The sum of the number of protons and the number of neutrons in the isotope is called the mass number of the isotope. Mass number is symbolized A. Isotopes are usually distinguished from one another by their mass numbers, given as a superscript before the chemical symbol for the element. Carbon-12 is an isotope of carbon with a symbol C. [Pg.41]


See other pages where Isotopes neutron number is mentioned: [Pg.149]    [Pg.20]    [Pg.51]    [Pg.421]    [Pg.707]    [Pg.243]    [Pg.310]    [Pg.353]    [Pg.431]    [Pg.136]    [Pg.136]    [Pg.206]    [Pg.231]    [Pg.328]    [Pg.356]    [Pg.363]    [Pg.363]    [Pg.173]    [Pg.176]    [Pg.177]    [Pg.153]    [Pg.9]    [Pg.296]    [Pg.115]    [Pg.56]   
See also in sourсe #XX -- [ Pg.111 ]




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