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Nucleus mass defect

High-mass resolution is needed to separate mass interferences of molecular and atom ions. Because of the mass defect of the binding energy of the nucleus, atomic ions have a slightly smaller mass than the corresponding molecular ions. To observe this typical mass resolutions between 5000 and 10000 are necessary. [Pg.113]

Nuclear fusion processes derive energy from the formation of low-mass nuclei, which have a different binding energy. Fusion of two nuclear particles produces a new nucleus that is lighter in mass than the masses of the two fusing particles. This mass defect is then interchangeable in energy via Einstein s equation E = me2. Specifically, the formation of an He nucleus from two protons and two neutrons would be expected to have mass ... [Pg.90]

The difference in mass is significant. It would show up on any reasonably precise balance. Thus, the mass of the nucleus of carbon-12 is significantly less than the mass of its component nucleons. The difference in mass between a nucleus and its nucleons is known as the mass defect. What causes this mass defect It is caused by the nuclear binding energy the energy associated with the strong force that holds a nucleus together. [Pg.229]

Main Group Element elements in groups 1, 2, and 13-18, members in each group have the same general electron configuration Mass Defect the change in mass when a nucleus is formed from its constituent nucleons... [Pg.343]

From nuclear physics it is known that the mass of a nucleus is always less than the sum of the masses of its components, the protons and neutrons. This phenomenon - called the mass defect (Am) - seems to be in conflict with the law of conservation of mass. The mass defect Am can be calculated by comparing the atomic weight of the nucleus mk with the sum of the masses of the protons nip and neutrons mn ... [Pg.3]

The mass defect (mass excess) or of a nucleus is equivalent to the binding energy of the nucleons in the nucleus and corresponds to ... [Pg.3]

When a nucleus is formed / v / from protons and neutrons, some mass (mass defect) is converted to energy (binding energy), as related by the Einstein equation, AE = A me2. [Pg.962]

Helium-6 is a radioactive isotope with fj/2 = 0.861 s. Calculate the mass defect (in g/mol) for the formation of a 6He nucleus, and calculate the binding energy in MeV/nucleon. Is a 6He nucleus more stable or less stable than a 4He nucleus (The mass of a 6He atom is 6.018 89 amu.)... [Pg.963]

Find the mass defect by subtracting the mass of the 6He nucleus from the mass of the constituent nucleons, and then use the Einstein equation to find the 6He binding energy. [Pg.963]

In 1931 scientists discovered that the total mass of the components of a nucleus is greater than the mass of the nucleus itself. This difference is called the mass defect. The origin of the mass defect also lies in E = me2. The components of a nucleus, its protons and neutrons, are bound to each other with an enormous amount of energy. When the nucleus comes apart to form individual protons and neutrons, this binding energy is no longer needed and is converted to mass. [Pg.234]

Binding Energy It is the energy equivalent to mass defect and is responsible for holding the nucleus together. It is known as binding energy of the nucleus. [Pg.247]

D) The difference in masses, known as the mass defect, is due to the conversion of mass that accompanies the formation of the nucleus. That is, the energy that is released as the more stable nucleus is formed by a conversion of mass according to the equation... [Pg.108]

For calculating the values of presented in Table VII, we have used the nuclear mass defect evaluated from the experimental data on the atomic defect (Lippmaa et al., 1985). We have taken the recoil energy to have the value 3 eV, which corresponds to the recoil of a free helium nucleus. In our earlier work (Kaplan et al., 1982,1983), for calculating we have used the value of the atomic mass defect measured by Smith et al. (1981). [Pg.336]

As was discussed in Section IV,A, the quantum chemical calculations allow us to compute the end point of the ft spectrum, provided we know the value of the mass defect of the radioactive nucleus. In later experiments of the ITEP group (Boris et al, 1983) the attained energy resolution of 20 eV made it possible to determine the end point of the /i spectrum EfXax (E0 in notations of the ITEP group). The fitting was done within the energy interval 40-50 eV away from the expected edge of the / spectrum. The value obtained was E0 = 18,579 2.1 eV. [Pg.341]

The mass of any atom is less than the combined masses of its separated parts. This difference in mass is known as the mass defect, also called mass loss. Electrons have masses so small that they can be left out of mass defect calculations. For helium, He, the mass of the nucleus is about 99.25% of the total mass of two protons and two neutrons. According to the equation E = mc, energy can be converted into mass, and mass can be converted into energy. So, a small quantity of mass is converted into an enormous quantity of energy when a nucleus forms. [Pg.662]

The mass defect represents the difference in mass between the helium nucleus and the total mass of the separated nucleons. [Pg.662]

As Figure 4 shows, the mass defect for one He nucleus is 0.0304 amu. The equation E = mc can be used to calculate the binding energy for this nucleus. Remember to first convert the mass defect, which has units of... [Pg.662]

The mass that is converted to energy when nucleons form a nucleus is known as the mass defect. [Pg.686]


See other pages where Nucleus mass defect is mentioned: [Pg.295]    [Pg.261]    [Pg.1581]    [Pg.23]    [Pg.91]    [Pg.607]    [Pg.608]    [Pg.246]    [Pg.247]    [Pg.336]    [Pg.3]    [Pg.201]    [Pg.1124]    [Pg.223]    [Pg.962]    [Pg.964]    [Pg.965]    [Pg.978]    [Pg.226]    [Pg.150]    [Pg.102]    [Pg.291]    [Pg.3]    [Pg.994]    [Pg.11]    [Pg.662]    [Pg.822]    [Pg.978]   
See also in sourсe #XX -- [ Pg.887 ]




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