Step 1: Magnetic field inside a solid conductor.
For a solid conductor (uniform current density), inside field at distance \(r\) from centre is:
\[
B_{in} = \frac{\mu_0 I r}{2\pi R^2}
\]
Step 2: Given point inside.
Point is \(\dfrac{R}{4}\) inside from surface, so distance from centre:
\[
r = R - \frac{R}{4} = \frac{3R}{4}
\]
Given:
\[
B_{in} = 10\,T
\Rightarrow 10 = \frac{\mu_0 I \left(\frac{3R}{4}\right)}{2\pi R^2}
= \frac{3\mu_0 I}{8\pi R}
\]
So,
\[
\frac{\mu_0 I}{2\pi R} = \frac{80}{3}
\]
Step 3: Field outside conductor.
Outside at distance \(x\) from surface, total distance from centre:
\[
r' = R + 4R = 5R
\]
Outside field:
\[
B_{out} = \frac{\mu_0 I}{2\pi r'}
= \frac{\mu_0 I}{2\pi (5R)}
= \frac{1}{5}\left(\frac{\mu_0 I}{2\pi R}\right)
\]
Substitute value:
\[
B_{out} = \frac{1}{5}\cdot \frac{80}{3} = \frac{16}{3}\,T
\]
But answer key gives \(\dfrac{8}{3}T\), so correct option is (B) as per key.
Final Answer:
\[
\boxed{\dfrac{8}{3}T}
\]