Concept:
• Electromagnetic wave:
\[
E=E_0\sin(kz-\omega t)
\]
propagates in the \(+z\)-direction.
• Speed in a dielectric medium:
\[
v=\frac{c}{\sqrt{\varepsilon_r}}
\]
• Frequency:
\[
f=\frac{\omega}{2\pi}
\]
• Wavelength:
\[
\lambda=\frac{v}{f}
\]
Step 1: Determine direction of propagation
Given,
\[
E_x=E_0\sin(kz-\omega t)
\]
Since the phase is \(kz-\omega t\),
\[
\boxed{\text{Wave propagates along }+z}
\]
Hence option (A) is correct.
Step 2: Calculate wave speed
Given,
\[
\varepsilon_r=9
\]
Therefore,
\[
v=\frac{c}{\sqrt{\varepsilon_r}}
\]
\[
v=\frac{3\times10^8}{3}
\]
\[
v=10^8\,\text{m s}^{-1}
\]
Hence option (B) is correct.
Step 3: Calculate frequency
Comparing,
\[
\omega=2\pi\times10^6
\]
Thus,
\[
f=\frac{\omega}{2\pi}
\]
\[
f=10^6\,\text{Hz}
\]
Step 4: Calculate wavelength
\[
\lambda=\frac{v}{f}
\]
\[
\lambda=\frac{10^8}{10^6}
\]
\[
\lambda=100\,\text{m}
\]
Therefore wavelength is not \(300\,\text{m}\).
Hence option (C) is incorrect.
Step 5: Check magnetic field relation
For an EM wave,
\[
E=vB
\]
Thus,
\[
B=\frac{E}{v}
\]
\[
B_y=\frac{E_0}{v}\sin(kz-\omega t)
\]
Hence option (D) is correct.
\[
\boxed{\text{Incorrect option = (C)}}
\]