In the crossed electric and magnetic fields, the proton experiences a force due to both fields that keeps it moving undeflected. The magnetic force \( F_B \) and electric force \( F_E \) balance each other. The force due to the magnetic field is given by:
\[
F_B = q v B,
\]
where \( q \) is the charge of the proton, \( v \) is the speed, and \( B \) is the magnetic field.
The electric force is:
\[
F_E = q E,
\]
where \( E \) is the electric field.
At equilibrium, \( F_B = F_E \), so:
\[
q v B = q E \quad \Rightarrow \quad v B = E.
\]
The proton moves along a circular path due to the magnetic field, so the centripetal force is:
\[
F_{\text{centripetal}} = \frac{m v^2}{r}.
\]
Equating this with the magnetic force \( F_B \), we get:
\[
\frac{m v^2}{r} = q v B \quad \Rightarrow \quad B = \frac{m v}{q r}.
\]
Using the known values for the mass of the proton \( m = 1.6 \times 10^{-27} \, \text{kg} \), radius \( r = 0.02 \, \text{m} \), and speed \( v = 2 \times 10^5 \, \text{m/s} \), we can find the electric field \( E \) using the relationship \( E = v B \).
Thus, the value of \( x \) is \( \boxed{1} \).