For a plane electromagnetic wave, the electric field \(E\) and magnetic field \(B\) are related by \( B = \frac{E}{c} \), where \(c\) is the speed of light in vacuum, approximately \(3 \times 10^8 \text{ m/s}\).
Given the electric field \( E_z = 60 \cos(5x + 1.5 \times 10^{10} t) \, \text{V/m} \), the corresponding magnetic field \(B_y\) is calculated as:
\[ B_y = \frac{E_z}{c} = \frac{60}{3 \times 10^8} \cos(5x + 1.5 \times 10^{10} t) \, \text{T} \]
This simplifies to:
\[ B_y = 2 \times 10^{-7} \cos(5x + 1.5 \times 10^{10} t) \, \text{T} \]
In electromagnetic waves, \(E\), \(B\), and wave propagation are mutually perpendicular and follow the right-hand rule. With \(E\) in the z-direction, \(B\) in the y-direction, and wave propagation in the x-direction, the right-hand rule dictates a negative sign for \(B_y\):
\[ B_y = -2 \times 10^{-7} \cos(5x + 1.5 \times 10^{10} t) \, \text{T} \]