Step 1: The given electric field is:
\[
\vec{E} = 69 \sin(\omega t - kx)\,\hat{j}
\]
which shows that the electric field oscillates along the \(+\hat{j}\) (y-axis).
Step 2: The phase \((\omega t - kx)\) indicates that the wave is propagating in the \(+\hat{i}\) (x-axis) direction.
Step 3: For an electromagnetic wave:
\[
\vec{E} \perp \vec{B} \perp \vec{k}
\]
and the direction of propagation is given by:
\[
\vec{k} = \vec{E} \times \vec{B}
\]
Step 4: Since
\[
\vec{E} \parallel \hat{j}, \vec{k} \parallel \hat{i},
\]
we must have:
\[
\hat{j} \times \vec{B} = \hat{i}
\]
This is satisfied when:
\[
\vec{B} \parallel \hat{k}
\]