.

Each subsequent component differs from old that in his ( its ) nucleus the measure ( sum ) of protons is increased by unit, and the measure ( sum ) of neutrons grows, by and large on some. That is in a nucleus ever there are more than neutrons, than protons ( non including the easiest karyon ) . In the literature this unusual para ( ratio ) of figure of neutrons to figure of protons, for any karyon, nil speaks.

For building of theoretical account of a karyon of atom we shall observe, that at an alpha of a radio-activity of a karyon of He have about equal to energy. Therefore on an external environment of a karyon we shall put all protons with the same measure ( sum ) of neutrons, i.e. at one power degree can be lone bozons with what the karyon placed on an external environment an alpha of a atom and are. Inside a karyon we shall set up the staying neutrons which job ( undertaking ) will be easing electrostatic Fieldss of forcing off of protons. Having assumed a nucleus spherical, and radiuses of a proton and a neutron about indistinguishable, for any component we shall have the theoretical account of a nucleus explicating the attitude ( relation ) of figure of neutrons to figure of protons, following of packing a karyon of atom. ( Discrepancy 0-10 % )

Radioactive decomposition, likely is connected to compaction of a nucleus since with growing of a consecutive figure of an element neutrons in volume of a nucleus all weaken radial forces of forcing off of protons more strongly. If weight of a karyon to accept initial, and chemical

belongingss of atom secondary in the tabular array of elements atomic weight should alter monotonously as across and on a perpendicular. Having constructed the tabular array to these properties we are compelled after Lu and Lr to go forth on four empty topographic points to detect chemical belongingss of elements.

Probably, at opening elements by necessity there is a definition of a charge of a karyon! ( the Charge of a karyon was defined ( determined ) merely for Cu and Pt.

In 1891. James Chadvik has lead ( carried out ) experiences and with the aid of expression Reserford has calculated charges of karyon for Pt – 77,4, for silver – 46,3, for Cu-29,3. These consequences about have coincided with consecutive Numberss of these elements in table Mendeleeva.

But, the last rare earth are radioactive! Harmonizing to our theoretical account of a karyon of atom at the following for lanthanide elements the radio-activity could be removed ( taken off ) debut inside of a karyon of the proton environment dwelling of four protons.

But so, specifying ( finding ) a charge of a karyon of atom of Pt on D.Chadvika ‘s method, we once more would have value 77,4 as alpha-particles would disperse on an external environment of a karyon of atom. Therefore to be put a inquiry on specification of charges of karyon of the elements following for Hf. Can be from here and failures with hit in “ islet of stableness “ .

& # 1057 ; & # 1087 ; & # 1080 ; & # 1089 ; & # 1086 ; & # 1082 ; & # 1083 ; & # 1080 ; & # 1090 ; & # 1077 ; & # 1088 ; & # 1072 ; & # 1090 ; & # 1091 ; & # 1088 ; & # 1099 ;

Henadzi R.Filipenka & # 8221 ; Model of the karyon of atom and the tabular array of elements & # 8221 ; Moscow & # 8220 ; Engineer & # 8221 ; N4 1990, N4 1991.