Step 1: Use the condition for circular motion of the charged particle.
The magnetic force provides centripetal force inside the solenoid: \[ qvB = \frac{mv^2}{r} \implies B = \frac{mv}{qr} \]
Step 2: Convert all quantities to SI units.
$m = 2.2 \times 10^{-30}\,\text{kg}$, $q = 1.6 \times 10^{-19}\,\text{C}$, $v = 10\,\text{km/s} = 10^4\,\text{m/s}$, $r = 2.8\,\text{cm} = 2.8 \times 10^{-2}\,\text{m}$.
Step 3: Calculate the magnetic field inside the solenoid.
\[ B = \frac{mv}{qr} = \frac{2.2 \times 10^{-30} \times 10^4}{1.6 \times 10^{-19} \times 2.8 \times 10^{-2}} \] \[ B = \frac{2.2 \times 10^{-26}}{4.48 \times 10^{-21}} = \frac{2.2}{4.48} \times 10^{-5} \approx 4.91 \times 10^{-6}\,\text{T} \]
Step 4: Apply Ampere's circuital law for a solenoid.
The magnetic field inside a solenoid is: \[ B = \mu_0 n I \] where $n$ is the number of turns per unit length and $I$ is the current. Given $n = 25\,\text{turns/cm} = 2500\,\text{turns/m}$ and $\mu_0 = 4\pi \times 10^{-7}\,\text{H/m}$.
Step 5: Solve for the current $I$.
\[ I = \frac{B}{\mu_0 n} = \frac{4.91 \times 10^{-6}}{4\pi \times 10^{-7} \times 2500} \] \[ I = \frac{4.91 \times 10^{-6}}{\pi \times 10^{-3}} = \frac{4.91}{\pi} \times 10^{-3}\,\text{A} \approx 1.56\,\text{mA} \]
Step 6: State the final answer.
The current in the solenoid required to maintain the circular orbit is: \[ \boxed{I \approx 1.56\,\text{mA}} \]