Concept:
The magnetic field on the axis of a circular current carrying coil is
\[
B=\frac{\mu_0 I R^2}{2(R^2+x^2)^{3/2}}
\]
where
\[
R=\text{radius of coil}
\]
\[
x=\text{distance of the point from the centre}
\]
The magnetic field varies inversely as
\[
(R^2+x^2)^{3/2}
\]
for a given current and radius.
Step 1: Write the magnetic field at point P.
Given,
\[
x_P=R\sqrt{15}
\]
Hence,
\[
B_P=
\frac{\mu_0IR^2}
{2(R^2+15R^2)^{3/2}}
\]
\[
B_P=
\frac{\mu_0IR^2}
{2(16R^2)^{3/2}}
\]
\[
B_P=
\frac{\mu_0IR^2}
{2(4R)^3}
\]
\[
B_P=
\frac{\mu_0IR^2}
{128R^3}
\]
Given that this magnetic field is equal to \(B\).
\[
B_P=B
\]
Step 2: Write the magnetic field at point Q.
Given,
\[
x_Q=R\sqrt3
\]
Therefore,
\[
B_Q=
\frac{\mu_0IR^2}
{2(R^2+3R^2)^{3/2}}
\]
\[
B_Q=
\frac{\mu_0IR^2}
{2(4R^2)^{3/2}}
\]
\[
B_Q=
\frac{\mu_0IR^2}
{2(2R)^3}
\]
\[
B_Q=
\frac{\mu_0IR^2}
{16R^3}
\]
Step 3: Find the ratio of the two magnetic fields.
\[
\frac{B_Q}{B_P}
=
\frac{\dfrac{\mu_0IR^2}{16R^3}}
{\dfrac{\mu_0IR^2}{128R^3}}
\]
\[
\frac{B_Q}{B_P}
=
\frac{128}{16}
\]
\[
\frac{B_Q}{B_P}=8
\]
Thus,
\[
B_Q=8B
\]
However, simplifying directly using the standard relation:
\[
B \propto \frac{1}{(R^2+x^2)^{3/2}}
\]
\[
\frac{B_Q}{B_P}
=
\left(
\frac{16R^2}{4R^2}
\right)^{3/2}
\]
\[
=
4^{3/2}
\]
\[
=8
\]
Therefore,
\[
\boxed{B_Q=8B}
\]
Step 4: State the answer.
\[
\boxed{8B}
\]
Hence the correct option is
\[
\boxed{(D)}
\]