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Question: The nuclear radius of a certain nucleus is \[7.2fm\] and it has a charge of \[1.28 \times {10^{ - 17...

The nuclear radius of a certain nucleus is 7.2fm7.2fm and it has a charge of 1.28×1017C1.28 \times {10^{ - 17}}C. The number of neutrons inside the nucleus is
\left( {\text{A}} \right)$$$136$$ \left( {\text{B}} \right) 140 \left( {\text{C}} \right) 126 \left( {\text{D}} \right) 142$

Explanation

Solution

Use the equation of relation between the radius of a nucleus, the experimental value of the radius of a proton or neutron, and the atomic mass(=the total number of protons and neutrons in the nucleus).
From the equation, by putting the given values we can get the value of atomic mass.
Calculate the number of the proton from the given charge of the nucleus since neutrons are neutral charged particles of the nucleus. And hence find the number of the neutron by subtracting the proton numbers from the atomic mass or the total number of the protons and neutrons in the nucleus.

Formula used:
R=R0A13R = {R_0}{A^{\dfrac{1}{3}}}
Where RR= The radius of the nucleus,
AA is equal to the total number of protons and neutrons in the nucleus,
R0{R_0}= the radius of a proton or a neutron.
The number of protons, Z = charge of the nucleuscharge of a proton{\text{Z = }}\dfrac{{{\text{charge of the nucleus}}}}{{{\text{charge of a proton}}}}.
The number of neutrons = AZA - Z.

Complete step by step answer:
The radius of the nucleus isRR, the atomic mass=the total number of protons and neutrons in the nucleus=AA and the radius of a proton or a neutron is R0{R_0}.
So, the volume of the nucleus, V=43πR3V = \dfrac{4}{3}\pi R_{}^3
And, the volume of a proton or a neutron, V=43πR03V' = \dfrac{4}{3}\pi R_0^3
So, V=V×AV = V' \times A

43πR03=43πR3×A \Rightarrow \dfrac{4}{3}\pi R_0^3 = \dfrac{4}{3}\pi R_{}^3 \times A
R03=R3A\Rightarrow R_0^3 = {R^3}A
A=(RR0)3\Rightarrow A = {\left( {\dfrac{R}{{{R_0}}}} \right)^3}
Since, the experimental value of the radius of a proton or a neutron is R0=1.2fm{R_0} = 1.2fm
A=(7.21.2)3\Rightarrow A = {\left( {\dfrac{{7.2}}{{1.2}}} \right)^3}
A=63\Rightarrow A = {6^3}
A=216\Rightarrow A = 216
The number of proton in the nucleus,
Z = charge of the nucleuscharge of a proton{\text{Z = }}\dfrac{{{\text{charge of the nucleus}}}}{{{\text{charge of a proton}}}}
Z=1.28×10171.6×1019Z = \dfrac{{1.28 \times {{10}^{ - 17}}}}{{1.6 \times {{10}^{ - 19}}}}
Z=0.8×100\Rightarrow Z = 0.8 \times 100
Z=80\Rightarrow Z = 80
The number of neutrons in the nucleus,
AZ=21680A - Z = 216 - 80
AZ=136\Rightarrow A - Z = 136

Hence the right answer is in option (A)\left( {\text{A}} \right). $$$$

Notes:
From the experimental value of the radius of a proton or a neutron we can get the nuclear density by the following steps,
Nuclear density, ρN=MV{\rho _N} = \dfrac{M}{V}, where M=M = Au=A×1.66×1024gmAu = A \times 1.66 \times {10^{ - 24}}gm
ρN=A×1.66×102443πR03A\therefore {\rho _N} = \dfrac{{A \times 1.66 \times {{10}^{ - 24}}}}{{\dfrac{4}{3}\pi R_0^3A}}, where R0=1.2fm=1.2×1013cm{R_0} = 1.2fm = 1.2 \times {10^{ - 13}}cm
ρN=1.66×102443π(1.2×1013)3\Rightarrow {\rho _N} = \dfrac{{1.66 \times {{10}^{ - 24}}}}{{\dfrac{4}{3}\pi {{(1.2 \times {{10}^{ - 13}})}^3}}}
On simplification we get,
ρN=2.3×1014g/cm3\Rightarrow {\rho _N} = 2.3 \times {10^{14}}g/c{m^3}
This value implies that the density of a nucleus is very high and hence a large number of objects remain concentrated in a very small space.