Step 1: Use magnetic force as centripetal force.
For an electron moving in a circular path in a magnetic field,
\[
qvB=\frac{mv^2}{r}
\]
Therefore,
\[
B=\frac{mv}{qr}
\]
Since,
\[
p=mv,
\]
we can write
\[
B=\frac{p}{qr}
\]
Step 2: Find momentum using kinetic energy.
For non-relativistic motion,
\[
K=\frac{p^2}{2m}
\]
So,
\[
p=\sqrt{2mK}
\]
Multiplying by \(c\),
\[
pc=\sqrt{2mc^2K}
\]
Given,
\[
mc^2=0.5\,\text{MeV}=5\times10^5\,\text{eV}
\]
and
\[
K=100\,\text{eV}
\]
Thus,
\[
pc=\sqrt{2\times 5\times10^5\times 100}
\]
\[
pc=\sqrt{10^8}
\]
\[
pc=10^4\,\text{eV}
\]
Hence,
\[
p=\frac{10^4\,\text{eV}}{c}
\]
Step 3: Convert momentum into SI units.
\[
p=\frac{10^4\times 1.6\times10^{-19}}{3\times10^8}
\]
\[
p=5.33\times10^{-24}\,\text{kg m s}^{-1}
\]
Step 4: Calculate magnetic field.
Given,
\[
q=1.6\times10^{-19}\,\text{C}
\]
and
\[
r=10\,\text{cm}=0.1\,\text{m}
\]
Using
\[
B=\frac{p}{qr}
\]
\[
B=\frac{5.33\times10^{-24}}{1.6\times10^{-19}\times0.1}
\]
\[
B=3.33\times10^{-4}\,\text{T}
\]
Step 5: Final conclusion.
Hence, the magnetic field is approximately
\[
\boxed{3.3\times10^{-4}\,\text{T}}
\]