Two plane polarized light waves combine at a certain point, whose "E" components are: \[ E_1 = E_0 \sin \omega t, \quad E_2 = E_0 \sin \left( \omega t + \frac{\pi}{3} \right) \] Find the amplitude of the resultant wave.
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When two sinusoidal waves combine, the amplitude of the resultant wave is calculated using the formula \( E_R = \sqrt{E_1^2 + E_2^2 + 2 E_1 E_2 \cos(\phi)} \), where \( \phi \) is the phase difference between the waves.
The two electric fields \( E_1 \) and \( E_2 \) are represented 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 the two waves can be calculated using the formula for the sum of two sinusoidal waves with the same frequency:
\[
E_R = \sqrt{E_1^2 + E_2^2 + 2 E_1 E_2 \cos(\phi)}
\]
where \( \phi \) is the phase difference between the two waves, which in this case is \( \frac{\pi}{3} \).
Substitute the given values:
\[
E_R = \sqrt{E_0^2 + E_0^2 + 2 E_0 \cdot E_0 \cdot \cos \left( \frac{\pi}{3} \right)}
\]
Using \( \cos \left( \frac{\pi}{3} \right) = \frac{1}{2} \):
\[
E_R = \sqrt{E_0^2 + E_0^2 + 2 E_0^2 \cdot \frac{1}{2}} = \sqrt{E_0^2 + E_0^2 + E_0^2} = \sqrt{3 E_0^2}
\]
Thus, the amplitude of the resultant wave is:
\[
E_R = \sqrt{3} E_0 \approx 1.7 E_0
\]
Therefore, the correct answer is (C) \( 1.7 E_0 \).