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.
The fission of \( ^{56}_ {26}Fe \) can be given as:
\(^{56}_{13} Fe → 2\space ^{28}_{13} Al\)
It is given that:
Atomic mass of \(m(^{56}_ {26}Fe) = 55.93494 u\)
Atomic mass of \(m ( ^{28}_{13} Al ) = 27.98191 u\)
The Q-value of this nuclear reaction is given as:
Q = \([m(^{56}_{26}Fe) - 2m(^{28}_{13} Al)]c^2\)
\(Q = [55.93494 - 2 \times 27.98191]c^2\)
\(Q = (-0.02888 \space c^2)u\)
But 1u = 931.5 \(\frac{MeV}{c^{2}}\)
Q = -0.02888 x 931.5
Q = -26.902 MeV
The Q-value of the fission is negative. Therefore, the fission is not possible energetically. For an energetically possible fission reaction, the Q-value must be positive.
Obtain the binding energy (in MeV) of a nitrogen nucleus. \((^{14}_{7}N)\) , given m \((^{14}_{7}N)\) = 14.00307 u
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
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
Nuclear physics is the field of physics that studies atomic nuclei and their constituents and interactions, in addition to the study of other forms of nuclear matter. Nuclear physics should not be confused with atomic physics, which studies the atom as a whole, including its electrons
‘R’ represents the radius of the nucleus. R = RoA1/3
Where,
The mass number (A), also known as the nucleon number, is the total number of neutrons and protons in a nucleus.
A = Z + N
Where, N is the neutron number, A is the mass number, Z is the proton number
Mass defect is the difference between the sum of masses of the nucleons (neutrons + protons) constituting a nucleus and the rest mass of the nucleus and is given as:
Δm = Zmp + (A - Z) mn - M
Where Z = atomic number, A = mass number, mp = mass of 1 proton, mn = mass of 1 neutron and M = mass of nucleus.