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ATOMIC MASS NUMBER A

An atom s total number of protons and neutrons is called its atomic mass number and denoted by A. An atom s mass is found in its nucleus and can be calculated as follows  [Pg.57]

Atomic Mass Number = Number of protons + Number of neutrons [Pg.57]

The atomic mass number can sometimes be called nucleon number. [Pg.57]

What is the atomic mass number of molibdenum, which has 42 protons and 54 neutrons  [Pg.57]

By using the following formula, molibdenum s atomic mass number can easily be calculated. [Pg.57]


Work carried out in the Kellogg Laboratory confirmed the existence of a gap at atomic mass number A = 8. Earlier, in the same laboratory, in 1939, the absence of a stable nuclei at A = 5 had been confirmed. Gamow was convinced that all the research relevant to atomic mass 5 was mistaken. [Pg.61]

Let us note the following key point nuclei for which Z and N are even are more abundant than their immediate neighbours. Nuclei with even atomic mass number A are favoured to the detriment of those with odd A. We must move down to the fifteenth position on the list of nuclei in order to find the most abundant one with odd mass number after hydrogen. This is magnesium-25. Note also the sudden drop in abundances in the region of A = 5-11 and around A = 45. [Pg.66]

The Total Bary on Number Remains Constant. A baryon is a nucleon (proton or neutron) or any panicle heavier than those that can he considered to have an atomic mass number A — I. Some mesons have a mass greater than the proton, but they have a mass number. 4 - 0. so they are not barvuns. In computing the number or barvons present in a system, each baryon counts I each ami baryon counts — I and leptons and mesons count 0. [Pg.434]

The most abundant product of the evolution of massive stars is oxygen, in particular—the third most abundant isotope in the Universe and the most abundant metal. Massive stars are also the main source of most heavy elements up to atomic mass number A 80, of some of the rare proton-rich nuclei, and of the r-process nuclei from barium to uranium. In the following, we will briefly review the burning stages and nuclear processes that characterize the evolution of massive stars and the resulting core collapse supemovae. [Pg.11]

Atomic mass number A = N + N = number of protons and neutrons in the nucleus... [Pg.1]

Atoms that have the same atomic number (Z) but different atomic mass numbers (A) are termed isotopes [1]. Isotopes are classified into atoms that are unstable and decay by emission of radiation to stable products (radioisotopes) and those that have never been observed to decay (stable isotopes). Most of the elements associated with organic compounds possess naturally occurring stable isotopic variants. Stable isotopes frequently encountered in the course of pharmacokinetic and drug-metabolism studies and their natural abundances, relative to the most abundant mass, are listed in Table 1 [2,3]. [Pg.337]

Target atoms of atomic mass number A are destroyed. [Pg.479]

Atoms with atomic mass number A. are produced. [Pg.479]

Atomic number (Z) and atomic mass number (A) are both conserved in a radioactive decay. [Pg.692]

Neutrons are scattered by the atomic nucleus. The scattered intensity is spherically symmetrical. The dependence of the scattering cross-section o on the atomic mass number A follows in general an law, but big... [Pg.63]

Free atoms prefer to exist in the neutral (zero charge) state. This results when the number of protons equals the number of electrons within the atom. Note Protons have a unit charge of+1, whereas electrons have a unit charge of -1 (neutrons have no charge). The number of protons within the nucleus of an atom is described by the atom s atomic number (Z). This number appears in the periodic table above the elements symbol (see Appendix A.l). The sum of protons and neutrons within the nucleus of a specific atom, or more specifically, that for a specific isotope of an element is defined by the atomic mass number (A), which is also referred to as the mass number. [Pg.24]

As a result of this electromagnetic repulsion and the fact that all masses are scaled (1 Da equates to l/12th the mass of the isotope), isotopes with masses lesser or greater than display a mass that diverges slightly from the atomic mass number (A). Recall A equates to the sum of protons and neutrons within the... [Pg.25]

Atomic mass is the mass of an atomic particle, i.e. a specific isotope. When expressed in unified atomic mass units, this is called the relative isotopic mass. The word relative is added to denote the fact that all masses are scaled to that of the isotope when set to 12 u. Nominal isotope masses are more commonly used when applying analytical techniques such as Secondary Ion Mass Spectrometry (SIMS) because this significantly simplifies matters without detracting from the information content needed. This represents the number of protons and neutrons within the nucleus, i.e. equal to the atomic mass number (A). Note It was the mass spectrograph constructed by Aston in 1919 (the first mass spectrometer from which SIMS evolved as covered in Section 1.2.1) that confirmed the existence of the isotopes, and allowed for the first time, an accurate means of measuring their relative mass (that relative to H, 0, or more recently C) and distribution. [Pg.26]


See other pages where ATOMIC MASS NUMBER A is mentioned: [Pg.3]    [Pg.3]    [Pg.20]    [Pg.65]    [Pg.31]    [Pg.4]    [Pg.9]    [Pg.3]    [Pg.3]    [Pg.579]    [Pg.856]    [Pg.15]    [Pg.34]   


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