The graph of \( \ln \left( \frac{R}{R_0} \right) \) versus \( \ln A \), where \( R \) is the radius of a nucleus, \( A \) its mass number, and \( R_0 \) a constant, is:
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For nuclear radius \( R = R_0 A^{1/3} \), plotting \( \ln(R/R_0) \) vs \( \ln A \) gives a straight line.
Radius of a nucleus: \( R = R_0 A^{1/3} \Rightarrow \ln R = \ln R_0 + \frac{1}{3} \ln A \)
\[
\Rightarrow \ln \left( \frac{R}{R_0} \right) = \frac{1}{3} \ln A
\]
This is a straight-line equation \( y = mx \) with slope \( \frac{1}{3} \).