Magnetic field produced due to long current carrying wire at point A is
\(B =\frac{\mu_02i}{4\pi r}\)
\(= \frac{10^{-7}\times 2 \times 5}{20 \times 10^{-2}}\)
\(= \frac 12 \times 10^{-5}\)
Direction of magnetic field will be outward to the plane of paper.
Now, force acting on the electron due to this field,
\(\vec F = q(\vec v \times \vec B)\)
\(= 1.6 \times 10^{-19} \times 10^5 \times \frac 12 \times 10^{-5}\)
\(= 0.8 \times 10^{-19}\)
\(\therefore |\vec F| = 8 \times 10^{-20} N\)