In an electromagnetic wave:
\[
E = cB, \quad \text{and } \vec{E} \perp \vec{B},\ \vec{E},\vec{B} \perp \text{direction of propagation}
\]
Given:
- \( B_0 = 3 \times 10^{-7}\, \text{T} \)
- \( E_0 = c \cdot B_0 = 3 \times 10^8 \cdot 3 \times 10^{-7} = 90\, \text{Vm}^{-1} \)
Since \( \vec{B} \parallel \hat{j} \), and propagation is along \( \hat{i} \), then \( \vec{E} \parallel \hat{k} \)
\[
\vec{E} = 90 \sin(3 \times 10^4 x + 9 \times 10^{12} t)\, \hat{k}
\]