The standard model of an atom is of a dense nucleus of charged
protons and electrically-neutral
neutrons, surrounded by an electrically-bound cloud of low mass, negatively charged
electrons. Despite the force of mutual repulsion between the protons, the nucleus is held together by the short-ranged
strong nuclear force between the particles. The
neutron–proton ratio determines the stability of a nucleus, as a proper balance of neutrons counteracts the mutual repulsion of the protons.
Nuclide displaying of the number of protons (Z) versus neutrons (N) for each isotope, with the color showing resulting half life A nuclide, or nuclear species, is a class of atoms characterized by their number of
protons,
Z, their number of
neutrons,
N, and their nuclear
energy state. Atomic nuclei other than , a lone proton, consist of protons and neutrons bound together by the
residual strong force, overcoming electrical repulsion between protons. For that reason, neutrons are required to bind protons together; as the number of protons increases, so does the
neutron–proton ratio necessary for stability. For example, although light elements up through oxygen have stable nuclides with the same number of neutrons as protons, lead requires about 3 neutrons for 2 protons. The
atomic number of an element is equal to the number of protons in each atom, and defines the element. For example, all carbon atoms contain 6 protons in their
atomic nucleus; so the atomic number of carbon is 6. The number of protons in the nucleus determines its
electric charge, which in turn determines the number of bound
electrons of an atom in its
non-ionized state. The electrons occupy
atomic orbitals that determine the atom's
chemical properties. Thus, for example, there are three main isotopes of carbon. All carbon atoms have 6 protons, but they can have either 6, 7, or 8 neutrons. Since the mass numbers of these are 12, 13 and 14 respectively, said three isotopes are known as
carbon-12,
carbon-13, and
carbon-14 (C, C, and C). Natural carbon is a
mixture of C (about 98.9%), C (about 1.1%) and about 1 atom per trillion of C. The number of neutrons in a nucleus usually has very little effect on an element's chemical properties. An exception is hydrogen, for which the
kinetic isotope effect is significant. Thus, all carbon isotopes have nearly identical chemical properties because they all have six electrons, even though they may have 6 to 8 neutrons. That is why atomic number, rather than
mass number or
atomic weight, is considered the identifying characteristic of an element. but many of these radioisotopes are not found in nature due to a low half life. Radioisotopes typically decay into other elements via
alpha decay,
beta decay, or
inverse beta decay; some isotopes of the heaviest elements also undergo
spontaneous fission. Isotopes that are not radioactive, are termed "stable" isotopes. Isotopes with even numbers of protons, even numbers of neutrons, or both, tend to be more stable as like particle can pair up with like. Most (54 of 94) naturally occurring elements have more than one stable isotope. Only 26 elements are
monoisotopic, having exactly one stable isotope; these have an odd atomic number of protons, with the exception of
beryllium-9 which has an odd number of neutrons. The mean number of stable isotopes for the 80 stable elements is 3.1 stable isotopes per element. The largest number of stable isotopes for a single element is 10 (for
tin, element 50). Elements with atomic numbers 1 through 82 each have at least one
stable isotope (except for
technetium, element 43 and
promethium, element 61, which have no stable isotopes). However, observationally stable isotopes of some elements (such as
tungsten and
lead) are predicted to be slightly radioactive with very long half-lives: for example, the half-lives predicted for the observationally stable lead isotopes range from 10 to 10 years. Isotopes are
observationally stable when they are theoretically unstable but no radioactive decay has yet been observed. Out of the over 250 nuclides that are called stable, only 90 are considered theoretically stable, meaning they lack a known decay mode. that make a nucleus more stable Elements with atomic numbers 83 through 94 are
unstable enough that radioactive decay of all isotopes can be detected. Some of these elements, notably
bismuth (atomic number 83),
thorium (atomic number 90), and
uranium (atomic number 92), have one or more isotopes with half-lives long enough to survive from before the
Solar System formed. The remaining longest-lived isotopes have
half lives too short for them to have been present at the beginning of the Solar System, and are therefore "transient elements". Of these 11 transient elements, five (
polonium,
radon,
radium,
actinium, and
protactinium) are relatively common
decay products of
thorium and
uranium. The remaining six transient elements (technetium, promethium, astatine,
francium,
neptunium, and
plutonium) occur only rarely, as products of rare decay modes or nuclear reaction processes involving uranium or other heavy elements. The remaining 24 heaviest elements (
those beyond plutonium, element 94) are radioactive, with
half-lives so short that they are not found on Earth and must be
synthesized. Five have been discovered in the spectrum of
Przybylski's star, from element 95 (
americium) to 99 (
einsteinium). These are thought to be
neutron capture products of uranium and thorium. All 24 heavier elements are radioactive, with short half-lives; if any of these elements were present when the Earth formed, they are certain to have completely decayed, and if present in novae, are in quantities too small to have been noted. Technetium was the first purportedly non-naturally occurring element synthesized, in 1937, though traces of technetium have since been found in nature (and also the element may have been discovered naturally in 1925). This pattern of artificial production and later natural discovery has been repeated with several other radioactive naturally occurring rare elements. The lightest radioactive isotope is
tritium, which undergoes
Beta decay with a half-life of 12.3 years. At 2 years, over 10 times the estimated age of the universe,
bismuth-209 has the longest known alpha decay half-life of any nuclide, and is almost always considered on par with the 80 stable elements. The isotope
tellurium-128 transmutes through double beta decay with a half life of 2.25 years, over 100,000 times longer than bismuth-209. The primary source of radiation exposure from isotope decays in the human body come from
carbon-14 and
potassium-40 intake, which produce an annual effective dose of .
Isotopic mass and atomic mass The
mass number of an element,
A, is the number of
nucleons (protons and neutrons) in the atomic nucleus. Different isotopes of a given element are distinguished by their mass number, which is written as a superscript on the left hand side of the chemical symbol (e.g., U). The mass number is always an integer and has units of "nucleons". Thus,
magnesium-24 (24 is the mass number) is an atom with 24 nucleons (12 protons and 12 neutrons). Whereas the mass number simply counts the total number of neutrons and protons and is thus an integer, the
atomic mass of a particular isotope (or "nuclide") of the element is the mass of a single atom of that isotope, and is typically expressed in
daltons (symbol: Da), aka universal atomic mass units (symbol: u). Its
relative atomic mass is a dimensionless number equal to the atomic mass divided by the
atomic mass constant, which equals 1 Da. However, the relative atomic mass of each isotope is quite close to its mass number (always within 1%). The only isotope whose atomic mass is exactly a
natural number is C, which has a mass of 12 Da; because the dalton is defined as 1/12 of the mass of a free neutral carbon-12 atom in the ground state. During the
nuclear fusion of lower mass atoms such as hydrogen, the net change in mass deficit is released as energy, as determined by the
mass–energy equivalence relationship. This process of fusing hydrogen atoms into helium is what drives the energy output of the Sun. Over time, the result is an increasing concentration of helium at the
stellar core. During the
evolution of stars much more massive than the Sun, increasingly massive nuclei are then formed through a type of fusion called the
alpha process, until
iron-52 is reached. In the
nuclear fission process, the resulting particles have a higher net binding energy. This change in the net mass deficit again results in a release of energy. Hence, highly radioactive elements such as
uranium-235 can be useful sources of energy production. The
standard atomic weight (commonly called "atomic weight") of an element is the
average of the atomic masses of all the chemical element's isotopes as found in a particular environment, weighted by isotopic abundance, relative to the atomic mass unit. This number may be a fraction that is
not close to a whole number. For example, the relative atomic mass of chlorine is 35.453 u, which differs greatly from a whole number as it is an average of about 76% chlorine-35 and 24% chlorine-37. For example, a
copper wire is 99.99% chemically pure if 99.99% of its atoms are copper, with 29 protons each. However it is not isotopically pure since natural copper consists of two stable isotopes, 69% Cu and 31% Cu, with different numbers of neutrons . However, pure gold would be both chemically and isotopically pure, since ordinary gold consists only of one isotope, Au. == Chemical and physical properties ==