Concept:
The total radiant power emitted by a star is given by the Stefan–Boltzmann law:
\[
P = \sigma A T^4
\]
where
\(P\) = radiant power,
\(\sigma\) = Stefan–Boltzmann constant,
\(A = 4\pi R^2\) = surface area of the star,
\(T\) = absolute temperature.
Substituting the surface area:
\[
P = 4\pi \sigma R^2 T^4
\]
Thus,
\[
P \propto R^2 T^4
\]
Step 1: Write the ratio of powers.
\[
\frac{P_A}{P_{Sun}} =
\frac{R_A^2 T_A^4}{R_{Sun}^2 T_{Sun}^4}
\]
Given:
\[
\frac{P_A}{P_{Sun}} = 3
\]
\[
T_A = 6000K, \quad T_{Sun} = 2000K
\]
Step 2: Calculate the temperature ratio.
\[
\left(\frac{T_A}{T_{Sun}}\right)^4 =
\left(\frac{6000}{2000}\right)^4
\]
\[
= 3^4 = 81
\]
Step 3: Substitute into the power relation.
\[
3 = \frac{R_A^2}{R_{Sun}^2} \times 81
\]
\[
\frac{R_A^2}{R_{Sun}^2} = \frac{3}{81}
\]
\[
\frac{R_A^2}{R_{Sun}^2} = \frac{1}{27}
\]
Step 4: Take square root to obtain radius ratio.
\[
\frac{R_A}{R_{Sun}} = \sqrt{\frac{1}{27}}
\]
\[
\frac{R_A}{R_{Sun}} = \frac{1}{\sqrt{27}}
\]
Step 5: Final result.
\[
R_A : R_{Sun} = 1 : \sqrt{27}
\]