Obtain the binding energy of the nuclei \(^{56}_{26}Fe\) and \( ^{209} _{83} Bi\) in units of MeV from the following data: \(m\) (\(^{56}_{26}Fe\)) = 55.934939 u, \(m\) (\( ^{209} _{83} Bi\)) = 208.980388 u
Atomic mass of \(^{56}_{26}Fe\) , \(m1 = 55.934939 u\)
\(^{56}_{26}Fe\) nucleus has 26 protons and (56 − 26) = 30 neutrons
Hence, the mass defect of the nucleus, \(∆m = 26 × m_H + 30 × m_n − m_1 \)
Where,
Mass of a proton, \(m_H = 1.007825 u \)
Mass of a neutron, \(m_n = 1.008665 u \)
∆m = 26 × 1.007825 + 30 × 1.008665 − 55.934939
= 26.20345 + 30.25995 − 55.934939
= 0.528461 u
But 1 u = 931.5 \(\frac{MeV}{c^2 }\)
∆m = 0.528461 × 931.5 \(\frac{MeV}{c^2 }\)
The binding energy of this nucleus is given as:
\(E_{b1} = ∆mc^2 \)
Where, c = Speed of light
\(E_{b1}\) = 0.528461 × 931.5 \((\frac{MeV}{c^2 })\times c^2\)
\(E_{b1}\) = 492.26 MeV
Average binding energy per nucleon = \(\frac{492.26}{56} = 8.79 MeV\)
Atomic mass of \( ^{209} _{83} Bi\), \(m_2 = 208.980388 u\)
\( ^{209} _{83} Bi\) nucleus has 83 protons and (209 − 83) 126 neutrons.
Hence, the mass defect of this nucleus is given as:
\(∆m' = 83 × m_H + 126 × m_n − m_2 \)
Where,
Mass of a proton, \(m_H = 1.007825 u\)
Mass of a neutron, \(m_n = 1.008665 u \)
\(∆m' \)= 83 × 1.007825 + 126 × 1.008665 − 208.980388
\(∆m' = \) 83.649475 + 127.091790 − 208.980388
\(∆m' = 1.760877 u \)
But \(1 u = 931.5 \frac{MeV}{c^2} \)
∆m' = 1.760877 × 931.5\(\frac{MeV}{c^2} \)
Hence, the binding energy of this nucleus is given as:
\(E_{b2} = ∆m'c^2\)
\(E_{b2}\) = 1.760877 × 931.5 \((\frac{MeV}{c^2})c^2\)
\(E_{b2} \)= 1640.26 MeV
Average binding energy per nucleon =\(\frac{1640.26}{209} =\) 7.848 MeV
Obtain the binding energy (in MeV) of a nitrogen nucleus. \((^{14}_{7}N)\) , given m \((^{14}_{7}N)\) = 14.00307 u
A given coin has a mass of 3.0 g. Calculate the nuclear energy that would be required to separate all the neutrons and protons from each other. For simplicity assume that the coin is entirely made of \(^{63}_{ 29}Cu\) atoms (of mass 62.92960 u).
Obtain approximately the ratio of the nuclear radii of the gold isotope \(^{197}_{ 79} Au \) and the silver isotope \(^{107}_{ 47} Ag\).
The Q value of a nuclear reaction A + b → C + d is defined by
Q = [mA+mb–mC–md]c2
where the masses refer to the respective nuclei. Determine from the given data the Q-value of the following reactions and state whether the reactions are exothermic or endothermic.
(i) \(^{1}_{ 1} H + ^{3} _{1}H → ^{2}_{1} H + ^{2}_{1} H\)
(ii) \(^{12}_{6} C + ^{12}_{6} C → ^{12}_{10} Ne + ^{4}_{2} He\)
Atomic masses are given to be
\(m (^{2}_{ 1} H)\) = 2.014102 u
\(m (^{3}_{1} H) \)= 3.016049 u
\(m (^{12}_{ 6} C) \)= 12.000000 u
\(m (^{20}_{10} Ne)\) = 19.992439 u
Suppose we think of fission of a \(^{56}_{26}Fe\) nucleus into two equal fragments, \(^{28}_{13} Al.\) Is the fission energetically possible? Argue by working out Q of the process. Given \(m\)(\(^{56}_{26}Fe\)) = 55.93494 u and \(m\)(\(^{28}_{13} Al\)) = 27.98191 u.
In the year 1911, Rutherford discovered the atomic nucleus along with his associates. It is already known that every atom is manufactured of positive charge and mass in the form of a nucleus that is concentrated at the center of the atom. More than 99.9% of the mass of an atom is located in the nucleus. Additionally, the size of the atom is of the order of 10-10 m and that of the nucleus is of the order of 10-15 m.
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