Step 1: Determine the magnetic field amplitude and wave vector.
\( B_0 = E_0/c = 60/(3\times10^8) = 2\times10^{-7}\,\text{T} \). Wave propagates along x, so \( k = 2\pi/\lambda = 2\pi/(10^{-2}) = 200\pi\,\text{m}^{-1} \).
Step 2: Determine the direction of B and write the equation.
Wave along \( +x \), E along \( +y \), so B must be along \( +z \) (i.e., \( \hat{k} \)) by \( \vec{E}\times\vec{B} \parallel \hat{x} \). \[ \vec{B} = (2\times10^{-7})\sin[200\pi(ct-x)]\hat{k}\,\text{T} \] \[ \boxed{(2\times10^{-7})\sin[200\pi(ct-x)]\hat{k}\,\text{tesla}} \]