Step 1: Intensity from a bulb.
Treating the bulb as a point source, the intensity at distance $r$ is $I = \dfrac{P}{4\pi r^2}$, the power spread over a sphere.
Step 2: Intensity and electric field.
For an electromagnetic wave, $I = \dfrac{1}{2}c\varepsilon_0 E_0^2$, so $E_0^2 \propto I$.
Step 3: Combine the two.
Putting them together, $E_0^2 \propto \dfrac{P}{r^2}$, so $E_0 \propto \dfrac{\sqrt{P}}{r}$. At a fixed distance, $E_0 \propto \sqrt{P}$.
Step 4: Form the ratio.
Since $r$ is the same $3\,\text{m}$ for both bulbs, \[ \frac{E_1}{E_2} = \sqrt{\frac{P_1}{P_2}}. \]
Step 5: Put in the powers.
With $P_1 = 100\,\text{W}$, $P_2 = 50\,\text{W}$, and $E_1 = E$: \[ \frac{E}{E_2} = \sqrt{\frac{100}{50}} = \sqrt{2}. \]
Step 6: Solve for the second field.
$E_2 = \dfrac{E}{\sqrt{2}}$.
\[ \boxed{E/\sqrt{2}} \]