To find the magnetic field of the electromagnetic wave, we need to utilize the relationship between the electric and magnetic fields in a plane electromagnetic wave. In such a wave, the electric field \( \vec{E} \) and the magnetic field \( \vec{B} \) are related by the speed of light \( c \), and they are perpendicular to each other, as well as to the direction of propagation of the wave.
For an electromagnetic wave traveling along the \( x \)-axis, the electric and magnetic fields are related by the following equation:
\[
\frac{E_z}{B_z} = c
\]
Where:
- \( E_z \) is the electric field,
- \( B_z \) is the magnetic field,
- \( c \) is the speed of light in a vacuum, which is \( 3 \times 10^8 \, \text{m/s} \).
Thus, the magnetic field can be written as:
\[
B_z = \frac{E_z}{c}
\]
Given that the electric field is:
\[
E_z = 60 \sin(500x + 1.5 \times 10^{11} t) \, \text{V/m},
\]
we can substitute this into the equation for \( B_z \):
\[
B_z = \frac{60 \sin(500x + 1.5 \times 10^{11} t)}{3 \times 10^8} \, \text{T}.
\]
Now, simplifying the expression:
\[
B_z = \frac{60}{3 \times 10^8} \sin(500x + 1.5 \times 10^{11} t) \, \text{T}.
\]
We can calculate the constant factor:
\[
\frac{60}{3 \times 10^8} = 2 \times 10^{-7}.
\]
Thus, the equation for the magnetic field becomes:
\[
B_z = 2 \times 10^{-7} \sin(500x + 1.5 \times 10^{11} t) \, \text{T}.
\]
Interpretation of the Result:
- The magnetic field \( B_z \) has the same functional form as the electric field \( E_z \), since they are both sinusoidal waves with the same frequency and wavevector.
- The only difference is the amplitude, which is scaled by a factor of \( 2 \times 10^{-7} \), due to the relationship between the electric and magnetic fields in an electromagnetic wave.
- The phase of the wave, as well as the wavevector \( k \) and angular frequency \( \omega \), remain unchanged.
- The magnetic field oscillates in sync with the electric field but is scaled by the factor related to the speed of light.