Step 1: Identify the direction of magnetic field.
The electromagnetic wave is propagating along \(x\)-direction.
The electric field is along \(y\)-direction.
For an electromagnetic wave, the electric field, magnetic field, and direction of propagation are mutually perpendicular.
Also,
\[
\vec{E}\times \vec{B}
\]
gives the direction of propagation.
Since propagation is along \(\hat{i}\) and electric field is along \(\hat{j}\), magnetic field must be along \(\hat{k}\), because
\[
\hat{j}\times \hat{k}=\hat{i}
\]
Thus, magnetic field is along
\[
\hat{k}
\]
Step 2: Find the maximum magnetic field.
For an electromagnetic wave,
\[
E_0=cB_0
\]
Therefore,
\[
B_0=\frac{E_0}{c}
\]
Given,
\[
E_0=60\,\text{V m}^{-1}
\]
and
\[
c=3\times 10^8\,\text{m s}^{-1}
\]
So,
\[
B_0=\frac{60}{3\times 10^8}
\]
\[
B_0=20\times 10^{-8}
\]
\[
B_0=2\times 10^{-7}\,\text{T}
\]
Step 3: Find the wave number.
Given wavelength is
\[
\lambda=10\,\text{mm}
\]
Since,
\[
1\,\text{mm}=10^{-3}\,\text{m}
\]
Therefore,
\[
\lambda=10\times 10^{-3}\,\text{m}
\]
\[
\lambda=10^{-2}\,\text{m}
\]
Wave number is
\[
k=\frac{2\pi}{\lambda}
\]
\[
k=\frac{2\pi}{10^{-2}}
\]
\[
k=200\pi\,\text{m}^{-1}
\]
Step 4: Write the magnetic field equation.
For a wave travelling along positive \(x\)-direction, the phase can be written as
\[
k(ct-x)
\]
Therefore,
\[
\vec{B}=B_0\sin[k(ct-x)]\hat{k}
\]
Substituting the values,
\[
\vec{B}=(2\times 10^{-7})\sin[200\pi(ct-x)]\hat{k}\,\text{tesla}
\]
Step 5: Final conclusion.
Therefore, the required magnetic field equation is
\[
\boxed{(2\times 10^{-7})\sin[200\pi(ct-x)]\hat{k}\,\text{tesla}}
\]