Step 1: Understanding the Concept
Convert the cosine wave into a sine wave so that the phases can be compared.
Step 2: Convert
\[ \cos\theta=\sin\left(\theta+\frac\pi2\right) \]
\[ y_2=a_2\sin\left(\omega t-\frac{2\pi x}{\lambda}+\frac\pi6+\frac\pi2\right)=a_2\sin\left(\omega t-\frac{2\pi x}{\lambda}+\frac{2\pi}{3}\right) \]
Step 3: Phase difference
Compared with \(y_1\), the extra phase is \(\phi=\dfrac{2\pi}{3}\).
Step 4: Path difference
\[ \Delta x=\frac\lambda{2\pi}\phi=\frac{\lambda}{2\pi}\cdot\frac{2\pi}{3}=\frac\lambda3 \]
This is option (C).
Final Answer:
The phase difference is 2 pi over 3, which corresponds to a path difference of lambda over 3, option (C).
\[ \boxed{\frac{\lambda}{3}} \]