



To solve this problem, we need to understand the relationship between the radius of a nucleus \( R \) and its mass number \( A \). According to the empirical formula for the radius of a nucleus:
R = R_0 \cdot A^{1/3}
Where \( R_0 \) is a constant approximately equal to 1.2-1.3 fm (femtometers). To investigate the relationship between \( \ln(\frac{R}{R_0}) \) and \( \ln(A) \), we can take the natural logarithm on both sides of the radius equation:
\ln(R) = \ln(R_0 \cdot A^{1/3})
Using the property of logarithms: \ln(xy) = \ln(x) + \ln(y), we can write:
\ln(R) = \ln(R_0) + \ln(A^{1/3})
Again, using the property of logarithms: \ln(x^y) = y \cdot \ln(x), we can express it as:
\ln(R) = \ln(R_0) + \frac{1}{3}\ln(A)
Now, consider the expression \ln(\frac{R}{R_0}):
\ln(\frac{R}{R_0}) = \ln(R) - \ln(R_0)
Substituting the expression we derived:
\ln(\frac{R}{R_0}) = \ln(R_0) + \frac{1}{3}\ln(A) - \ln(R_0)
This simplifies to:
\ln(\frac{R}{R_0}) = \frac{1}{3}\ln(A)
This is a linear relationship where the slope is \(\frac{1}{3}\). Hence, the plot of \ln(\frac{R}{R_0}) vs \ln(A) will be a straight line with a positive slope of \(\frac{1}{3}\).
Therefore, the correct figure is a straight line graph with a positive slope.