The two electric fields, \( E_1 \) and \( E_2 \), are defined as:
\[
E_1 = E_0 \sin \omega t, \quad E_2 = E_0 \sin \left( \omega t + \frac{\pi}{3} \right)
\]
The resultant amplitude, \( E_R \), of these two waves with identical frequencies is determined by the formula:
\[
E_R = \sqrt{E_1^2 + E_2^2 + 2 E_1 E_2 \cos(\phi)}
\]
In this context, \( \phi \), the phase difference between the waves, is \( \frac{\pi}{3} \).
Substituting the given values:
\[
E_R = \sqrt{E_0^2 + E_0^2 + 2 E_0 \cdot E_0 \cdot \cos \left( \frac{\pi}{3} \right)}
\]
Given that \( \cos \left( \frac{\pi}{3} \right) = \frac{1}{2} \):
\[
E_R = \sqrt{E_0^2 + E_0^2 + 2 E_0^2 \cdot \frac{1}{2}} = \sqrt{E_0^2 + E_0^2 + E_0^2} = \sqrt{3 E_0^2}
\]
Consequently, the amplitude of the resultant wave is:
\[
E_R = \sqrt{3} E_0 \approx 1.7 E_0
\]
The determined amplitude for the resultant wave is \( 1.7 E_0 \).