Step 1: Use magnetic force as centripetal force.
Since the charged particle moves in a circular path inside the magnetic field, the magnetic force provides the centripetal force.
Therefore,
\[
qvB=\frac{mv^2}{r}
\]
So,
\[
B=\frac{mv}{qr}
\]
Step 2: Convert the given quantities into SI units.
Given,
\[
m=2.2\times 10^{-30}\,\text{kg}
\]
\[
q=1.6\times 10^{-19}\,\text{C}
\]
\[
v=10\,\text{km s}^{-1}=10\times 10^3=10^4\,\text{m s}^{-1}
\]
\[
r=2.8\,\text{cm}=2.8\times 10^{-2}\,\text{m}
\]
Step 3: Calculate the magnetic field.
\[
B=\frac{(2.2\times 10^{-30})(10^4)}
{(1.6\times 10^{-19})(2.8\times 10^{-2})}
\]
\[
B=\frac{2.2\times 10^{-26}}
{4.48\times 10^{-21}}
\]
\[
B=4.91\times 10^{-6}\,\text{T}
\]
Step 4: Use magnetic field inside a solenoid.
For a long solenoid,
\[
B=\mu_0 n I
\]
So,
\[
I=\frac{B}{\mu_0 n}
\]
The number of turns per unit length is
\[
n=25\,\text{turns/cm}
\]
Since,
\[
1\,\text{cm}=10^{-2}\,\text{m}
\]
we get
\[
n=25\times 100=2500\,\text{turns/m}
\]
Step 5: Calculate the current.
\[
I=\frac{4.91\times 10^{-6}}
{(4\pi\times 10^{-7})(2500)}
\]
Using
\[
\pi \approx 3.14
\]
\[
I=\frac{4.91\times 10^{-6}}
{3.14\times 10^{-3}}
\]
\[
I=1.56\times 10^{-3}\,\text{A}
\]
\[
I=1.56\,\text{mA}
\]
Step 6: Final conclusion.
Therefore, the current in the solenoid is
\[
\boxed{1.56\,\text{mA}}
\]