The magnetic field strength \( H \) is given by:
\[
H = \frac{N I}{l}
\]
where \( N = 200 \), \( I = 5 \, \text{mA} = 5 \times 10^{-3} \, \text{A} \), and \( l \) is the length of the magnetic path, which is the average circumference of the toroid. The average radius \( r = \frac{10 + 14}{2} = 12 \, \text{cm} = 0.12 \, \text{m} \), so:
\[
l = 2\pi r = 2\pi \times 0.12 = 0.754 \, \text{m}.
\]
Thus,
\[
H = \frac{200 \times 5 \times 10^{-3}}{0.754} \approx 1.32 \, \text{A/m}.
\]
The flux density \( B \) is given by:
\[
B = \mu_0 \mu_r H = 4\pi \times 10^{-7} \times 3000 \times 1.32 \approx 1.66 \times 10^{-3} \, \text{T} = 1.66 \, \text{mT}.
\]
Thus, the flux density is approximately \( 1.66 \, \text{mT} \).