Step 1: Use the relation between electric and magnetic fields.
For an electromagnetic wave,
\[
E_0=cB_0
\]
where,
\[
c=3\times10^8\,\text{m s}^{-1}
\]
is the speed of light.
Given magnetic field amplitude,
\[
B_0=3\times10^{-7}\,\text{T}
\]
Therefore,
\[
E_0=(3\times10^8)(3\times10^{-7})
\]
\[
E_0=9\times10^1
\]
\[
E_0=90\,\text{V m}^{-1}
\]
Step 2: Determine the direction of propagation.
The wave equation is
\[
\sin(kx+\omega t)
\]
This represents propagation along the negative \(x\)-direction.
Thus, direction of propagation is
\[
-\hat{i}
\]
Step 3: Determine the direction of electric field.
For electromagnetic waves,
\[
\vec{E}\times\vec{B}
\]
gives the direction of propagation.
Given,
\[
\vec{B}\parallel \hat{j}
\]
We require
\[
\vec{E}\times\hat{j}=-\hat{i}
\]
Using vector products,
\[
\hat{k}\times\hat{j}=-\hat{i}
\]
Hence,
\[
\vec{E}\parallel \hat{k}
\]
Step 4: Write the electric field expression.
Therefore,
\[
\vec{E}=90\sin(3\times10^4x+9\times10^{12}t)\,\hat{k}\ \text{V m}^{-1}
\]
Step 5: Final conclusion.
Hence, the electric field is
\[
\boxed{
90\sin(3\times10^4x+9\times10^{12}t)\,\hat{k}\ \text{V m}^{-1}
}
\]