Atomic Radii

An atomic radii is difficult to quantify because electrons move towards and away from the nucleus (in electron clouds). The nucleus also does not have a defined boundary, but the radius can be approximated by the following value:

\(R = 1.25 \cdot A^{1/3} \; [\text{fm}]\)

\(1\) femtometer is equivalent to \(10^{-15}\) meters.

Thus, the volume of the sphere increases proportionally to the atomic mass. The ratio \( V/A\) is also constant suggesting the density is uniform like a liquid drop (i.e. the liquid-drop model).


The radius of an unknown nucleus is determined to be twice a large as another. What is the ratio of their masses?

The first element can be expressed as:

\(R_1 = 1.25 \cdot A^{1/3}_1\)

The second element can be expressed as:

\(R_2 = 1.25 \cdot A^{1/3}_2\)

The second radius is twice the first:

\(R_2 = 2 \cdot R_1\)

We can substitute the respective values to determine the ratio of the masses:

\(1.25 \cdot A^{1/3}_2 = 2 \cdot 1.25 \cdot A^{1/3}_1\)

\(A^{\frac{1}{3}}_2 = 2 \cdot A^{1/3}_1\)

\(A_2 = 8 \cdot A_1\)

\(\cfrac{A_2}{A_1} = 8\)

Thus, the mass of the unknown element is \(\boldsymbol{8}\) times larger than the known element.


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