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Question

Question: The relation between the volume \( V \) and the mass \( M \) of a nucleus is (A) \( V \propto {M^3...

The relation between the volume VV and the mass MM of a nucleus is
(A) VM3V \propto {M^3}
(B) VM1/3V \propto {M^{1/3}}
(C) VMV \propto M
(D) V1MV \propto \dfrac{1}{M}

Explanation

Solution

To answer this question, we need to use the relationship of the radius of the nucleus with the mass number. Then using the relation of the mass with the volume, i.e. the density, we can get the required proportionality.

Formula used:
R=R0A1/3R = {R_0}{A^{1/3}} , here RR is the radius of the nucleus, AA is the mass number of the nucleus, and R0{R_0} is a constant.
D=MVD = \dfrac{M}{V} , here DD is the density of the nucleus, MM is the mass of the nucleus, and VV is the volume of the nucleus.

Complete step by step solution:
The relationship between the radius and the mass number of a nucleus has been found experimentally to be
R=R0A1/3R = {R_0}{A^{1/3}} .....................(1)
We know that the volume of a nucleus, VR3V \propto {R^3}
From (1), we can say that the volume VAV \propto A
Also, we know that the mass of a nucleus is proportional to the mass number AA .
That is, MAM \propto A
Now, we know that the density D=MVD = \dfrac{M}{V} .....................(2)
As both the mass and the volume are proportional to the mass number AA , the density becomes independent of AA , or it is a constant.
So, from (2) we have
D=MVD = \dfrac{M}{V}
On cross-multiplying we get
V=MDV = \dfrac{M}{D}
As DD is a constant, so 1D\dfrac{1}{D} is also a constant.
VM\therefore V \propto M
So, the volume of a nucleus is proportional to its mass.

Note:
The above proportionality can also be obtained without even considering the relation of the individual quantities with the mass number. As we know that the density of the nuclear matter is a constant ( 2.3×1023kgm3\approx 2.3 \times {10^{23}}kg{m^{ - 3}} ), so the volume of the nucleus will be linearly proportional to its mass.