Given two electric field components of plane polarized light:\[E_1 = E_0 \sin(\omega t)\]\[E_2 = E_0 \sin\left( \omega t + \frac{\pi}{3} \right)\]The resultant wave's amplitude is calculated using the formula:\[E_{\text{res}} = \sqrt{E_1^2 + E_2^2 + 2E_1 E_2 \cos(\phi)}\]where \( \phi = \frac{\pi}{3} \) represents the phase difference.Substituting the values yields:\[E_{\text{res}} = \sqrt{E_0^2 + E_0^2 + 2E_0^2 \cos\left( \frac{\pi}{3} \right)}\]As \( \cos\left( \frac{\pi}{3} \right) = \frac{1}{2} \), the equation simplifies to:\[E_{\text{res}} = \sqrt{E_0^2 + E_0^2 + E_0^2} = \sqrt{3E_0^2} = \sqrt{3} E_0\]
Consequently, the amplitude of the resultant wave is \( \sqrt{3} E_0 \approx 1.7 E_0 \).