The graph of
\[
\ln\left(\frac{R}{R_0}\right)\ \text{versus}\ \ln A
\]
is
where \(R\) is the radius of a nucleus, \(A\) is its mass number, and \(R_0\) is constant.
Show Hint
The nuclear radius relation \(R=R_0A^{1/3}\) becomes linear when logarithms are taken on both sides.
Step 1: Recall the nuclear radius law. The radius of a nucleus depends on its mass number $A$ as \[ R = R_0 A^{1/3}, \] where $R_0$ is a constant. Step 2: Isolate the ratio. Dividing by $R_0$, \[ \frac{R}{R_0} = A^{1/3}. \] Step 3: Take logarithms. \[ \ln\!\left(\frac{R}{R_0}\right) = \ln\!\left(A^{1/3}\right). \] Step 4: Use the power rule of logs. \[ \ln\!\left(\frac{R}{R_0}\right) = \frac{1}{3}\ln A. \] Step 5: Compare with a line. Writing $y = \ln(R/R_0)$ and $x = \ln A$ gives $y = \dfrac{1}{3}x$, which is of the form $y = mx$, a straight line through the origin with slope $\dfrac13$. Step 6: Conclude. Therefore the graph is a straight line. \[ \boxed{\text{A straight line}} \]